# DISCRETE 2014: Fourth Symposium on Prospects in the Physics of Discrete Symmetries

Europe/London
Great Hall and several lecture theatres (King's College London, Strand Campus)

### Great Hall and several lecture theatres

#### King's College London, Strand Campus

Strand London WC2R 2LS UK
Description

This is the Fourth Symposium on Prospects in the Physics of Discrete Symmetries, DISCRETE 2014, the latest of the DISCRETE conference series (for information on previous ones see:  Discrete'08, Discrete2010, Discrete2012), which this year will take place at King's College London, Strand Campus, London WC2R 2LS, from: Tuesday, December 2 2014 till Saturday, December 6 2014. The topics covered at the DISCRETE series of conferences are: T, C, P, CP symmetries; accidental symmetries (B, L conservation); CPT symmetry, decoherence and entangled states, Lorentz symmetry breaking (phenomenology and current bounds); neutrino mass and mixing; implications for cosmology and astroparticle physics, dark matter searches; experimental prospects at LHC, new facilities. In this coming DISCRETE we shall also introduce two new topics: cosmological aspects of non-commutative space-times as well as PT symmetric Hamiltonians (non-Hermitian but with real eigenvalues), a topic that has wide applications in particle physics and beyond.

This year at King's College London we also celebrate the 150th anniversary of the publication of Maxwell’s equations, while James Clerk Maxwell was the Professor of Natural Philosophy here. Moreover it is the 60th Anniversary of the discovery of Yang-Mills Gauge theories, the 50th anniversary of the discovery of CP Violation and the 50th anniversary of the proposal of Bell's Inequalities in Quantum Physics. Hence DISCRETE 2014 can be combined with the celebration of the above anniversaries.

The format of the talks will be: Plenary (40+5 min), invited research talks (30 + 5 min) and shorter presentations (25 + 5 min), selected (by the conveners of each session in consultation with the organisers) from the submitted abstracts. The conference fee for registered participants is £400, which covers lunches, proceedings and participation in the conference dinner that is going to take place at the historic Royal Society in Carlton House Terrace. PhD students and non-tenured postdoctoral fellows will be allowed to register for Discrete 2014 with a reduced registration fee of £250. This reduced-fee registration period will extend to November 28 2014.

Participants
• Aielet Efrati
• Aleksander Gajos
• Alessandro Pilloni
• Alfredo Aranda
• Alon Faraggi
• Andrea Longhin
• Antonio Di Domenico
• Antonio Marrone
• António Figueiredo
• Apostolos Pilaftsis
• Arlene Cristina Aguilar
• Arttu Rajantie
• Beatrix Hiesmayr
• Bhupal Dev
• Biagio Lucini
• Carl Bender
• Catalina Oana Curceanu
• Catarina Simoes
• Caterina Bloise
• cecilia jarlskog
• Chakrit Pongkitivanichkul
• Christoph Luhn
• Claudia Hagedorn
• Daniele Binosi
• Daniele Teresi
• Daria Kaminska
• David Evans
• David G. Cerdeno
• Denise Vicino
• Dimitris Skliros
• Eberhard Widmann
• Ed Daw
• Emmanuel Moulin
• Enrico Graziani
• Fabio Siringo
• Fairouz Malek
• Fatima Soomro
• Ferdinand Hahn
• Fotis Farakos
• Francisco J. de Anda
• Francisco Jose Botella Olcina
• Franklin Potter
• Fredrik Björkeroth
• Gabriele Honecker
• Gaetano Lambiase
• Georgios Leontaris
• Gerald Eigen
• Giovanni F. Tassielli
• Giulio D'Agostini
• Giuseppe Vitiello
• Gustavo C. Branco
• Gustavo Da Fonseca Castelo Branco
• Hans-Thomas Elze
• Hasan Sonmez
• Hèlios Sanchis Alepuz
• Ioannis Florakis
• Isabella Garzia
• Ivan Girardi
• Ivo de Medeiros Varzielas
• James Brister
• James Pinfold
• Jared Yamaoka
• Javier Fuentes-Martin
• Javier Rubio
• Jean Alexandre
• Jean-Pierre Derendinger
• Jim Talbert
• Joannis Papavassiliou
• Joaquim Matias
• Johann Marton
• John Heal
• Jonathan Ellis
• Jorge Casaus
• Jorge S. Diaz
• Jose Bernabeu
• José Rodriguez Quintero
• JUAN CARLOS D'OLIVO
• Julio Leite
• Karim Benakli
• Karim Massri
• Katy Clough
• Kevin Hickerson
• Krzysztof Bozek
• Kurt Langfeld
• Kyriakos Tamvakis
• Lee Barnby
• Luka Santelj
• Lukas Nellen
• Manuel Walter
• Marco de Cesare
• MARCO LAVEDER
• Margarida Nesbitt Rebelo
• Margarida Nesbitt Rebelo
• Maria Dimou
• Maria Krawczyk
• Maria Vittoria Gargiulo
• Mark Lancaster
• Martin Flechl
• Masaki Hori
• Masoud Ghezelbash
• Massimo Blasone
• Massimo Lenti
• Matthew Tamsett
• Melanie Day
• Melina Gomez
• Michael Christian Rammensee
• Michael Duerr
• Michael Franke
• Miguel Crispim Romao
• Miguel Nebot Gomez
• Mikael Chala
• Mike Hewitt
• Mitsuhiro Kimura
• Monica F Ramirez
• Monika Blanke
• Mu-Chun Chen
• Myriam Mondragon
• Myriam Mondragon
• Neville Harnew
• Nick Houston
• Nikos Mavromatos
• Nuno Leonardo
• Nuria Rius
• Owe Philipsen
• Panos Athanasopoulos
• Peter Millington
• Philip Mannheim
• Rabindra Mohapatra
• sarben sarkar
• Sergey Sukhoruchkin
• Sergio Palomares-Ruiz
• Stefan Olejnik
• Stefano Liberati
• Stephen King
• Subir Sarkar
• Sukhdev Sharma
• Sven Krippendorf
• Tevong You
• Thomas Latham
• Thomas Neder
• Vasiliki Mitsou
• Vincenzo Branchina
• Viraf Mehta
• Volpe Cristina
• William Alan Bertsche
• Yevgeniy Petrov
• Tuesday, 2 December
• 08:55 09:00
Registration: Desk (Great Hall) 8:30 - 17:00 5m
• 09:00 13:30
PLENARY 1 Great Hall

#### Great Hall

• 09:00
• 09:15
Discrete Glimpses of the Physics Landscape after the Higgs Discovery 45m
The discovery of a Higgs boson at the LHC raises (almost) as many questions as it answers. Is it an elementary particle, or composite? Are there other Higgs bosons? Is the vacuum stable? Are there other particles at the TeV scale waiting to be discovered at the LHC or in dark matter experiments? This talk will answer none of these questions.
Speaker: Jonathan R. Ellis (CERN)
• 10:00
Experimental particle physics in light of results from the LHC 45m
I will concentrate on hadron colliders, although I will also discuss (briefly) neutrino physics, e+e- colliders etc
Speaker: Jim Virdee (Imperial College Sci., Tech. & Med. (GB))
• 10:45
Coffee break 30m Great Hall and River Room

#### Great Hall and River Room

• 11:15
News from the Universe 45m
I will review recent observational results in particle astrophysics/cosmology, focussing on new data from Planck and from AMS-02 & IceCube, and discuss how the universe can be used as a laboratory for probing fundamental physics.
Speaker: Prof. S Sarkar (University of Oxford (GB))
• 12:00
PT-symmetric quantum theory 45m
The average quantum physicist on the street would say that a quantum-mechanical Hamiltonian must be Dirac Hermitian (invariant under combined matrix transposition and complex conjugation) in order to guarantee that the energy eigenvalues are real and that time evolution is unitary. However, the Hamiltonian $H=p^2+ix^3$, which is obviously not Dirac Hermitian, has a positive real discrete spectrum and generates unitary time evolution, and thus it defines a fully consistent and physical quantum theory! Evidently, the axiom of Dirac Hermiticity is too restrictive. While $H=p^2+ix^3$ is not Dirac Hermitian, it is PT symmetric; that is, invariant under combined parity P (space reflection) and time reversal T. The quantum mechanics defined by a PT-symmetric Hamiltonian is a complex generalization of ordinary quantum mechanics. When quantum mechanics is extended into the complex domain, new kinds of theories having strange and remarkable properties emerge. In the past few years, some of these properties have been verified in laboratory experiments. A particularly interesting PT-symmetric Hamiltonian is $H=p^2-x^4$, which contains an upside-down potential. We will discuss this potential in detail, and explain in intuitive as well as in rigorous terms why the energy levels of this potential are real, positive, and discrete. Applications of PT-symmetry in quantum field theory will be discussed.
Speaker: Prof. Carl Bender (Washington University in St Louis)
• 12:45
Experimental prospects for C, P, T, CP and CPT tests 45m
The prospects for tests of C, P, and CP using triple product asymmetries in quark, charged lepton, and boson decay are discussed, and possibilities of testing CP, T and CPT with entangled pairs of neutral mesons will be reviewed.
Speaker: Adrian Bevan (University of London (GB))
• 13:30 14:45
Lunch Break 1h 15m Great Hall and River Room

#### Great Hall and River Room

• 14:45 16:20
Parallel 1: Discrete symmetries (T, C, P), flavour, accidental symmetries River Room

#### River Room

• 14:45
Subtleties in the BaBar measurement of time-reversal violation 30m
A first measurement of T asymmetries that are not also CP asymmetries has been recently achieved by the BaBar collaboration. We analyze the measured asymmetries in the presence of direct CP violation, CPT violation, wrong strangeness decays and wrong sign semileptonic decays. We introduce parameters that have well-defined transformation properties under CP, T and CPT, and identify contributions to the measured asymmetries that are T conserving. We explain why, in order that the measured asymmetries would be purely odd under time-reversal, there is no need to assume the absence of direct CP violation. Instead, one needs to assume (i) the absence of CPT violation in strangeness changing decays, and (ii) the absence of wrong sign decays.
Speaker: Aielet Efrati (W)
• 15:15
NOVEL T-VIOLATION OBSERVABLE OPEN TO ANY DECAY CHANNEL AT MESON FACTORIES 35m
Quantum Entanglement between the two neutral mesons produced in meson factories has allowed the first direct observation of Time-Reversal-Violation in the time evolution of the B neutral meson system between the two decays. The exceptional meson transitions are directly connected to semileptonic and CP-eigenstate decay channels. The possibility of extending the observable asymmetries to more decay channels confronts the problem of the "orthogonality condition", which can be stated with this tongue-twister: Given a decay channel f, which is the decay channel f' such that the meson state not going to f' is orthogonal to the meson state not going to f ? We propose an alternative T-Violation Asymmetry in the meson factories which allows its opening to any pair of decay channels
Speaker: francisco j. botella (University of Valencia)
• 15:50
A direct test of T symmetry in the neutral K meson system at KLOE-2 30m
This work presents prospects for conducting a novel direct test of time- reversal symmetry at the KLOE-2 experiment. Quantum entanglement of neutral K meson pairs uniquely available at KLOE-2 allows to probe the T symmetry directly and independently of CP violation. This is achieved by a comparison of probabilities for a transition and its inverse obtained through exchange of initial and final states. Such transitions between flavor and CP- definite states of the neutral kaons are only connected by the T conjugation which ensures the CP-independence of the test. While a similar measurement was performed by the BaBar experiment with neutral B mesons, the KLOE-2 detector can test T -violation in the neutral kaons system. Such a test requires i.a. reconstruction of the KL → 3π0 decay accompanied by KS → π±l∓ν with good timing information. Therefore a new reconstruction method for this process is also presented which is capable of reconstructing the KL → 3π0 decay with decay time resolution of O(1τS).
Speaker: Aleksander Gajos (Jagiellonian University)
• 14:45 16:30
Parallel 2: Neutrinos mass and mixing, implications for astroparticle physics, dark matter searches S 7.06 (7th floor Strand Bldg)

#### S 7.06 (7th floor Strand Bldg)

• 14:45
Neutrino Astrophysics : recent advances and open issues 35m
Neutrinos of astrophysical origin are messengers produced in stars, in explosive phenomena like core-collapse supernovae, in the accretion disks around black holes, or in the Earth's atmosphere. Their fluxes and spectra encode information on the environments that produce them. Such fluxes are modified in characteristic ways when neutrinos traverse a medium, also depending on key unknown neutrino properties. We will summarize recent advances in this domain, the open questions and their importance for observations.
Speaker: Dr CRISTINA VOLPE (ASTROPARTICULE ET COSMOLOGIE (APC))
• 15:20
Dynamical generation of fermion mixing 35m
We present a dynamical mechanism à la Nambu-Jona-Lasinio for the generation of masses and mixing for two interacting fermion fields. The analysis is carried out in a framework in which mass generation is achieved via inequivalent representations, and that we generalize to the case of two generations. The method allows a clear identification of the vacuum structure for each physical phase, confirming previous results about the distinct physical nature of the vacuum for fields with definite mass and fields with definite flavor.
Speaker: Massimo Blasone (Università di Salerno)
• 15:55
Time-reversal invariance and neutrino oscillations in a medium with a symmetric density 30m
We consider the evolution operator of a quantum system described by a time-dependent Hamiltonian that is invariant under time reversal. As an illustration we examine the three-neutrino oscillations in a medium with a density profile which is symmetrical about the midpoint of the of the neutrino trajectory. The evolution operator is written as the product of factors corresponding to effective two-neutrino problems for a low and a high energy regime and each factor determined by means of the Magnus approximation up to second order. Oscillation probabilities calculated in this manner for the case of atmospheric neutrinos traversing Earth show good agreement with numerical calculations.
Speaker: Dr Juan Carlos D'Olivo (Depto. de Física Teórica, Universidad de Valencia)
• 14:45 16:30
Parallel 4: Experiments-discrete-symmetries Great Hall

#### Great Hall

• 14:45
Status and prospects for the Mu2e experiment at Fermilab 30m
The Mu2e Experiment at Fermilab will search for coherent, neutrino-less conversion of muons into electrons in the field of a nucleus with a sensitivity improvement of a factor of 10,000 over existing limits. Such a lepton flavor-violating reaction probes new physics at a scale inaccessible with direct searches at either present or planned high energy colliders. The experiment both complements and extends the current search for muon decay to electron+gamma at MEG and searches for new physics at the LHC. We will present the physics motivation for Mu2e, the design of the muon beamline and the detector, and the current status of the experiment.
Speaker: Dr Giovanni F. Tassielli (INFN Lecce / Università del Salento)
• 15:15
New Measurements of the ${\pi}^+{\rightarrow}e^+{\nu}_e$ Branching Ratio 30m
Study of rare decays is an important approach to search for new physics beyond the Standard Model. The branching ratio of charged pion decays, $R={\Gamma}({\pi}^+{\rightarrow}e^{+}{\nu}_{e}({\gamma}))$/${\Gamma}({\pi}^+{\rightarrow}{\mu}^+{\nu}_{\mu}({\gamma}))$ is one of the most precisely calculated processes involving quarks with $R_{SM}=(1.2352{\pm}0.0001)$ ${\times}10^{-4}$. Precise measurement of $R$ provides one of the most stringent tests of the hypothesis of electron-muon universality in weak interactions. The current experimental values of the branching ratio are $R_{EXP}=(1.2265{\pm}0.0034(stat){\pm}0.0044(syst)){\times}10^{-4}$ (TRIUMF, 1992) and $R_{EXP}=(1.2346{\pm}0.0035(stat){\pm}0.0036(syst)){\times}10^{-4}$ (PSI, 1993), which indicate that there is a room for improvement by two orders of magnitude in precision. The goal of PIENU experiment at TRIUMF is to improve the accuracy of the branching ratio measurement by a factor of 5, to $<0.1\%$. This precision allows potential access to new physics up to the mass scale of 1000 TeV for pseudoscalar interactions. Examples of the new physics probed include R-parity violating SUSY, heavy neutrino mixing, excited gauge bosons, leptoquarks, compositeness, and the effects of charged Higgs bosons. The PIENU experiment collected about $4.5{\times}10^5~{\pi}^+{\rightarrow}e^+{\nu}_e$ events, which corresponds to about 30 times higher statistics than in the previous TRIUMF experiment. The time and energy of decay positrons from decays of pions at rest were measured in a spectrometer employing plastic scintillators, tracking detectors, and NaI(Tl) and pure CsI crystals. The branching ratio is obtained from the ratio of the positron yields from ${\pi}^+{\rightarrow}e^+{\nu}_e$ decays $(E_e=69.8 ~{\rm MeV})$ and ${\pi}^+{\rightarrow}{\mu}^+{\nu}_{\mu}$ decays followed by ${\mu}^+{\rightarrow}e^+{\nu}_e\overline{{\nu}_{\mu}}$ decays (${\pi}^+{\rightarrow}{\mu}^+{\rightarrow}e^+, E_e=0.5$ to 52.8 MeV). Two energy regions, above and below the ${\pi}^+{\rightarrow}{\mu}^+{\rightarrow}e^+$ distribution were used to determine the time spectra of decay positrons. Data in the two regions are fitted simultaneously to extract the branching ratio to which corrections are applied. The most important corrections resulting in systemmatic uncertainties include the ${\pi}^+{\rightarrow}e^+{\nu}_e$ low energy distribution in the calorimeter due to shower leakage and the difference of positron acceptances between ${\pi}^+{\rightarrow}e^+{\nu}_e$ and ${\pi}^+{\rightarrow}{\mu}^+{\rightarrow}e^+$ events. The current analysis corresponds to approximately $10\%$ of the statistics of the full data. Results will be presented.
Speaker: Shintaro Ito (Osaka University, Toyonaka, Osaka, 560-0043, Japan)
• 16:30 17:00
Coffee Break 30m River and parallel session rooms

#### River and parallel session rooms

• 17:00 19:35
Parallel 1: g-2 & discrete symmetries (T, C, P), flavour, accidental symmetries River Room

#### River Room

• 17:00
The Fermilab Muon g-2 Experiment 30m
The Fermilab Muon g-2 experiment, E989, is presently being constructed and is seeking to measure the anomalous magnetic moment of the muon to a precision of 0.14ppm: a factor of four better than the previous Brookhaven measurement which has a long-standing discrepancy with respect to the SM prediction of approximately 3.5 standard deviations. I will review the status of the Fermilab experiment and describe how the reduction in the experimental uncertainty will be achieved.
Speaker: Mark Lancaster (University College London (UK))
• 17:30
Phenomenology of scenarios with flavor and CP symmetries 30m
I discuss a scenario for leptons with a flavor and a CP symmetry. If these symmetries are broken in a particular way, lepton mixing angles as well as the Dirac and the Majorana phases can be predicted in terms of quantities determined by the symmetries of the theory and only one continuous parameter. I present results for a large class of flavor and CP symmetries. Furthermore, I study leptogenesis and neutrinoless double beta decay in such a scenario.
Speaker: Claudia Hagedorn (Excellence Cluster 'Universe', TU Munich)
• 18:00
Gauge Theories for Baryon and Lepton Numbers with Lepto-Baryons 30m
I present extensions of the Standard Model, where the global symmetries baryon and lepton number are gauged and subsequently spontaneously broken. These theories are consistent with collider bounds and cosmology, and have intriguing consequences due to the requirement of anomaly cancellation: lepto-baryon fields that have to be introduced can be a dark matter candidate and/or generate neutrino masses. I discuss symmetric and asymmetric dark matter, the generation of neutrino masses, as well as collider signatures in these extensions.
Speaker: Michael Duerr (MPIK Heidelberg)
• 18:30
Break (5min) 5m
• 18:35
Extra dimensions with flavor. 30m
The use of discrete symmetries to explain fermion masses and mixings has been a popular and profitable tool in particle physics. Some of the most interesting features shown in both the quark and lepton sectors, specially with regards to their mixing patterns, strongly hint at the presence of some underlying "flavor" symmetry. On the other hand, the puzzling wide spread in the mass spectrum of fundamental particles, specially when neutrinos are included in the discussion, cannot so clearly nor directly be associated to a symmetry. Instead, several mechanisms have been concocted that, most of the time in collaboration with flavor symmetries, try to explain such observed richness. In this talk we will discuss how some simple and economical models with cyclic symmetry, that reproduce all mixing angles, when constructed in extra dimensions, can also lead to a reproduction of the fermion mass spectrum through the process of localization.
Speaker: Alfredo Aranda (Universidad de Colima)
• 19:05
Predicting Lepton Mixing Parameters including Majorana Phases from Δ(6n2) Flavour Symmetry and Generalised CP 30m
An important class of flavour groups that are subgroups of U(3) and that predict experimentally viable lepton mixing parameters including Majorana phases, is the Delta(6n^2) series. The most well-known member is Delta(24)=S_4. I present results of several extensive studies of lepton mixing predictions obtained in models with a Delta(6n^2) flavour group that preserve either the full Klein symmetry or a Z_2 subgroup for neutrinos and can include a generalised CP symmetry. Predictions include mixing angles and Dirac CP phase generally; and if invariance under a generalised CP symmetry is included, also Majorana phases. For this, the interplay of flavour group and generalised CP symmetry has to be studied carefully. Furthermore, I present results for neutrinoless double-beta decay.
Speaker: Mr Thomas Neder (University of Southampton)
• 17:00 19:40
Parallel 2: Neutrino mass and mixing, implications for astroparticle physics, dark matter searches S7.06 7th floor Strand Bldg.

#### S7.06 7th floor Strand Bldg.

• 17:00
Neutrino Oscillations and Dark Matter in IceCube 30m
The IceCube detector is the world's largest neutrino observatory, a 1 km$^{3}$ array of photomultipliers buried in the ice at the geographic South Pole. With the addition of the DeepCore in-fill, IceCube is sensitive to physics down the the ~10 GeV range. Current studies of neutrino oscillations and dark matter in DeepCore will be discussed. Also I will discuss the proposed in-fill extension, PINGU, with potential to probe low mass dark matter, further constrain neutrino oscillation parameters and determine the neutrino mass hierarchy.
Speaker: Melanie Day (IceCube)
• 17:30
On the flavor composition of the high-energy neutrinos in IceCube 35m
The IceCube experiment has recently released 3 years of data of the first ever detected high-energy ($> 30$ TeV) neutrinos, which are consistent with an extraterrestrial origin. In this talk, I will discuss the compatibility of the observed track-to-shower ratio with possible combinations of neutrino flavors and its implications.
Speaker: Sergio Palomares-Ruiz (IFIC-Valencia)
• 18:05
Break (5 min) 5m
• 18:10
Neutrino mass hierarchy determination with PINGU 30m
This work is being performed in collaboration with E. Lisi (INFN, Bari, Italy) and F. Capozzi (U. of Bari, Italy). The proposed PINGU experiment (Precision IceCube Next Generation Upgrade) will study low energy atmospheric neutrinos and it will allow to probe the neutrino mass hierarchy, after 3-5 years of data taking. It will also be sensitive to the theta_23 octant and it will help to resolve some degeneracies between neutrino oscillation parameters. We study the robustness of PINGU predictions with respect to a large variety of systematic uncertainties, including energy and angle resolution systematic errors and spectrum shape uncertainties, and we quantitatively determine the impact of such uncertainties on the hierarchy discrimination.
Speaker: Antonio Marrone (Univ. of Bari)
• 18:40
Measurement of the neutrino mixing angle $\theta_{13}$ with the Double Chooz detector 30m
The $\theta_{13}$ parameter of the PMNS mixing matrix remained unknown until first hints and estimates by both Double Chooz and beam experiments in 2011. The Double Chooz reactor antineutrino experiment aims for a precise measurement of this parameter. Located at the Chooz nuclear power plant in France, it relies on a two identical detector measurement, canceling most of systematic uncertainties related to neutrino flux emission and detection. The near detector, located at a few hundred meters from the two reactor cores, aims to monitor the $\bar\nu_e$ flux from the cores. The far detector, located at a distance of about one kilometer from the reactor cores near the expected first maximum of the oscillation, measures an energy dependent deficit in the electron antineutrino spectrum. Different approaches are used to extract $\theta_{13}$: A combined rate and spectral shape analysis as well as a background-model-independent analysis based on reactor power variations. A unique feature of the Double Chooz experiment is, that it was the only one of the currently running $\theta_{13}$ reactor experiments observing a phase with both reactors off. This provides access to the background only measurement, allowing to crosscheck the background modes used in the oscillation analysis. New analysis enhancements resulted in the latest results of the experiment, based on far detector only measurement, published in summer 2014. In total 467.90 live days with 66.5 GW-ton-years of exposure, twice as much data compared to the last publication, the value of $\theta_{13}$ is measured to be $\sin^2 2 \theta_{13} = 0.090^{+0.032}_{-0.029}$. Data taking in the near detector is about to start, enabling a significant reduction of both reactor and detector related systematics uncertainties in a near future.
Speaker: Michael Franke
• 19:10
On the origin of neutrino oscillations through Lorentz violation 30m
We propose Lorentz invariance violating models to study the possibility of dynamical generation of neutrino masses and oscillations. We show that such models are consistent with both Majorana and Dirac neutrinos and that the only observable effects are the dynamical generation of neutrino masses and oscillations.
Speaker: Julio Leite
• 17:00 19:20
Parallel 3: PT symmetric quantum theory K0.31

#### K0.31

• 17:00
Solitons, soliton vortices and PT-symmetry in spin-orbit coupled Bose-Einstein condensates. 35m
Spin-orbit coupled Bose-Einstein condensates (SO-BECs), which in the meanfield approximation are governed by two linearly coupled Gross-Pitaevskii equations, allow for the existence of many types of localized nonlinear excitations: fundamental and multipole solitons, soliton half-vortices, etc. In the first part of the talk, such excitations will be considered in the presence of so-called Zeeman lattice (i.e. periodic potential which is pi-shifted in both components). I will discuss classification of the solutions with respect to the parity, time, pseudo-charge, and lattice symmetries. In the second part of the talk, a homogeneous SO-BEC will be considered in the presence of mechanisms of loading and loosing atoms. Spontaneous PT-symmetry breaking scenarios, as well as nonlinear modes in such SO-BECs will be described.
• 17:35
PT-Symmetric $\phi^3$ and $\phi^4$ theories: properties and intriguing results. 35m
The renormalization group properties of a PT-symmetric $\phi^3$ theory are discussed and compared to the corresponding properties of the conventional theory. In d=6 dimensions, the theory turns out to be energetically stable, perturbatively renormalizable, and trivial (the conventional one being asymptotically free and unstable). Moreover, in $d =6-\epsilon$ dimensions, the theory has a non-trivial fixed point. The critical behaviour around this point is discussed. Finally, it is shown that, due to its stability properties, the PT-symmetric theory has a predictive power higher than the conventional one. As for the PT-symmetric $\phi^4$ theory, the $d=0$ dimension case is studied. Unexpected and intriguing results arise.
Speaker: Prof. Vincenzo Branchina (University of Catania)
• 18:10
Break (5 min) 5m
• 18:15
PT Symmetry, Quantum Gravity, and the Metrication of the Fundamental Forces 35m
We discuss some recent applications of PT symmetry to fundamental physics. We show that the recognition (Bender and Mannheim) that fourth-order derivative theories are PT symmetric theories rather than Hermitian ones enables one to show that such theories are ghost free and unitary. This then permits the fourth-order derivative conformal gravity theory to be a consistent quantum theory of gravity. We show that the conformal gravity theory provides for a universal departure from Newtonian gravity on large distance scales, which enables us to universally fit (Mannheim and O'Brien) the galactic rotation curves of 141 galaxies without the need for any dark matter, and without the 282 free parameters (two per galactic halo) present in standard dark matter fits to the same set of galaxies. Finally we show that through the use of generalized geometric connections that are PT symmetric we are able to metricate the fundamental forces, to thus both complete and generalize Weyl's original attempt to provide a geometric origin to electromagnetism based on utilizing and extending to gravity the underlying conformal structure that electromagnetism possesses. C. M. Bender and P. D. Mannheim, Physical Review Letters 100, 110402 (2008). P. D. Mannheim and J. G. O’Brien, Physical Review Letters 106, 121101 (2011). P. D. Mannheim, PT Symmetry, Conformal Symmetry, and the Metrication of Electromagnetism, arXiv:1407.1820 [hep-th].
Speaker: Prof. Philip Mannheim (University of Connecticut)
• 18:50
Foldy-Wouthuysen transformation for a non-Hermitian Hamiltonian 30m
I will show the consistency of a non-Hermitian Lagrangian describing free fermions, and perform the Foldy-Wouthuysen transformation in order to map the Hamiltonian on a Hermitian one.
Speaker: Jean Alexandre (King's College London)
• 17:00 19:30
Parallel 4: Experiments-discrete-symmetries Great Hall

#### Great Hall

• 17:00
Recent BaBar results 30m
We present a selection of recent results obtained by using the data collected with the BaBar detector at the PEP-II e+e- B-factory, with particular emphasis on measurements probing the discrete symmetries in beauty and charm decays. These include the measurements of partial decay rates and CP asymmetries of the inclusive decays B -> Xs l+ l- and B -> Xs gamma; searches for lepton number violation in several B+ -> X-l+l+ decays (where l = e, mu and X- is a charged hadron); and studies of semi-leptonic decays to measure the sides of the Unitarity Triangle.
Speaker: Gerald Eigen (University of Bergen (NO))
• 17:30
Direct searches for New Physics particles at BABAR 25m
We report on the latest searches for low mass states predicted in several New Physics models performed with the data collected by the BABAR detector. These include: searches for the so-called dark photons in e+e- annihilations (e+e- -> gamma A’, A’ -> e+e-, mu+mu-), and for long-lived particles motivated by recent astrophysical observations; searches for non-standard pi0-like particle production in e+e- -> tau+tau- events; and searches for a low mass CP-odd Higgs boson predicted in non-minimal supersymmetric extensions of the Standard Model.
Speaker: Gerald Eigen (University of Bergen (NO))
• 17:55
The Belle II Experiment 30m
The Belle II experiment is now being constructed at the KEK laboratory in Japan. This project represents a substantial upgrade to both the Belle detector and the KEKB accelerator. The Belle II experiment will record 50~ab$^{-1}$ of data, a factor of 50 more than that recorded by the Belle experiment. This large data set, combined with the low backgrounds and high trigger efficiencies characteristic of an $e^+e^-$ experiment, should provide unprecedented sensitivity to new physics signatures in $B$ and $D$ meson decays, and in $\tau$ lepton decays. The experiment is scheduled to begin taking data in 2016. This talk will review the capabilities of the experiment, the expected sensitivity to new physics, and the current status of detector construction.
Speaker: Dr Jared Yamaoka (Pacific Northwest National Lab)
• 18:25
Break (5 min) 5m
• 18:30
Measurements of exclusive and inclusive b->X_s l+ l- and b->s gamma radiative decays at Belle 25m
Recent measurements of exclusive and inclusive b->X_s l+ l- and b->s gamma decays are reported from Belle.
Speaker: Dr Jared Yamaoka (Pacific Northwest National Lab)
• 18:55
Exclusive $b\rightarrow s \gamma$ decays at Belle. 30m
We search for the decay $B_{s}\rightarrow\gamma\gamma$ and measure the branching fraction for $B_{s}\rightarrow\phi\gamma$ using 121.4~$\textrm{fb}^{-1}$ of data collected at the $\Upsilon(\mathrm{5}S)$ resonance with the Belle detector at the KEKB asymmetric energy B-factory located at the High Energy Accelerator Research Organization (KEK), Japan. These are flavor changing neutral current processes involving the transition of a \textit{b} to \textit{s} quark which are extremely sensitive to new physics beyond the Standard Model. We measure the branching fraction of $B_{s}\rightarrow\phi\gamma$ to be $(3.6 \pm 0.5 \rm{(stat.)}\pm 0.3 \rm{(syst.)} \pm 0.6 \rm{(f_{s})}) \times 10^{-5}$, which is in a good agreement with the theoretical predictions as well as a recent measurement from LHCb. We observe no statistically significant signal for the $B_{s}\rightarrow\gamma\gamma$ decay and set an upper limit at $3.1\times10^{-6}$ at 90$\%$ C.L. Recent results on these decays will be presented in this talk.
Speaker: Ms Deepanwita Dutta (IIT Guwahati)
• 20:15 21:30
Welcome Reception 1h 15m 7th floor Strand Bldg.

#### 7th floor Strand Bldg.

• Wednesday, 3 December
• 08:55 09:00
Registration: Desk (Great Hall) 8:30 - 17:00 5m
• 09:00 13:15
PLENARY 2 Great Hall

#### Great Hall

• 09:00
Half a Century with CP Violation 45m
The speaker intends to present a "historical" talk on CP violation discussing what have been the most important lessons learned so far and what can be said about the future prospects in this field.
Speaker: Prof. cecilia jarlskog (lund university)
• 09:45
Some Open Questions on CP Violation and Flavour 45m
We address some open questions on CP Violation and Flavour, including the nature and scale of New Physics and the origin of CP Violation. In the lepton sector, we conjecture that the observed pattern of leptonic mixing may just reflect a quasi-degeneracy of Majorana Neutrino Masses.
Speaker: Gustavo Branco (Instituto Superior Tecnico)
• 10:30
Coffee Break 30m Great Hall and River Room

#### Great Hall and River Room

• 11:00
Tests of Discrete Symmetries in K systems 45m
The status of present experiments and future projects with kaons is reviewed, focusing on prospects for discrete symmetries tests.
Speaker: Prof. Antonio Di Domenico (Universita Sapienza e INFN, Roma I (IT))
• 11:45
Discrete symmetries and models of flavour mixing 45m
In this talk we shall give an overview of the role of discrete symmetries, including both CP and family symmetry, in constructing unified models of quark and lepton (including especially neutrino) masses and mixing. Various different approaches to model building will be described, denoted as direct, semi-direct and indirect, and the pros and cons of each approach discussed. Particular examples based on Delta(6n^2) will be discussed and an A to Z of Flavour with Pati-Salam will be presented.
Speaker: Prof. Stephen King (University of Southampton)
• 12:30
Unraveling the organization of the QCD tapestry 45m
I will review recent progress in our understanding of the infrared dynamics of the QCD Green's functions, derived from the close synergy between lattice simulations and Schwinger-Dyson equations. Particular attention will be devoted to the elaborate nonperturbative mechanisms that endow the fundamental degrees of freedom (quarks and gluons) with dynamical masses.
Speaker: Joannis Papavassiliou (University of Valencia)
• 13:15 14:30
Lunch Break 1h 15m Great Hall and River Room

#### Great Hall and River Room

• 14:30 16:10
Parallel 1: Discrete symmetries (T, C, P), flavour, accidental symmetries Great Hall

#### Great Hall

• 14:30
Adding CP to Flavour Symmetries 30m
Topics on addding CP to flavour symmetries.
Speaker: Ivo de Medeiros Varzielas (University of Southampton)
• 15:00
Tests of Lorentz and CPT invariance with neutrinos and photons 30m
Lorentz symmetry is a cornerstone of modern physics. As the spacetime symmetry of special relativity, Lorentz invariance is a basic component of the standard model of particle physics and general relativity, which to date constitute our most successful descriptions of nature. Deviations from exact symmetry would radically change our view of the universe and current experiments allow us to test the validity of this assumption. In this talk, I will describe how we can use neutrinos and photons to search for deviations from exact Lorentz and CPT invariance.
Speaker: Jorge S. Diaz
• 15:30
Non-minimally flavour violating dark matter 30m
Flavour symmetries provide an appealing mechanism to stabilize the dark matter particle. I present a simple model of quark flavoured dark matter that goes beyond the framework of minimal flavour violation. I discuss the phenomenological implications for direct and indirect dark matter detection experiments, high energy collider searches as well as flavour violating precision data.
Speaker: Monika Blanke (CERN)
• 14:30 16:10
Parallel 2: Neutrinos mass and mixing, implications for astroparticle physics, dark matter searches K-1.56

#### K-1.56

• 14:30
Predictions for the Dirac Phase in the Neutrino Mixing Matrix 30m
Using the fact that the neutrino mixing matrix $U = U^\dagger_{e}U_{\nu}$, where $U_{e}$ and $U_{\nu}$ result from the diagonalisation of the charged lepton and neutrino mass matrices, and assuming 3-neutrino mixing, we consider a number of forms of $U_{\nu}$ associated with a variety of flavour symmetries: i) tri-bimaximal (TBM) and ii) bimaximal BM) forms , the forms corresponding iii) to the conservation of the lepton charge $L' = L_e - L_\mu - L_{\tau}$ (LC), iv) to golden ratio type A (GRA) mixing, v) golden ratio type B (GRB) mixing, and vi) to hexagonal (HG) mixing. In this approach to neutrino mixing one obtains exact predictions for the Dirac phase $\delta$ in the neutrino mixing matrix if the matrix $U_e$ has a minimal form in terms of angles and phases it contains that can provide the requisite corrections to $U_{\nu}$ so that the reactor, atmospheric and solar neutrino mixing angles $\theta_{13}$, $\theta_{23}$ and $\theta_{12}$ have values compatible with the current data. The predictions for $\delta$ depend on the angles $\theta_{13}$, $\theta_{23}$ and $\theta_{12}$ and have also simple "leading order" and "next-to-leading order" approximate forms. We compare the exact predictions for $\delta$ with those obtained in the "leading order" approximation. We investigate also the variation of the predictions of $\delta$ with the variation of the values of the neutrino mixing angles $\theta_{13}$, $\theta_{23}$ and $\theta_{12}$ in their 3$\sigma$ experimentally allowed ranges. Finally, we discuss other forms for the matrices $U_e$ and $U_{\nu}$ which allow us to derive exact predictions for the CP violation phase $\delta$. A measurement of $\cos\delta$ can allow to descriminate between the different forms of $U_{e}$ and $U_{\nu}$ considered in our study.
Speaker: Mr Ivan Girardi (SISSA)
• 15:00
Phenomenology of Light Sterile Neutrinos 30m
I review the experimental indications in favor of short-baseline neutrino oscillations. I discuss their interpretation in the framework of neutrino mixing schemes with one or more sterile neutrinos which have masses around the eV scale. Taking into account also cosmological constraints, I present arguments in favor of 3+1 neutrino mixing with one sterile neutrino at the eV scale. I discuss the implications for neutrinoless double-beta decay and cosmology.
Speaker: Marco Laveder (Dipartimento di Fisica Galileo Galilei)
• 15:30
The NOvA long-baseline neutrino oscillation experiment 30m
The recently completed NuMI Off-Axis Nu_e Appearance (NOvA) long-baseline neutrino oscillation experiment, will use an upgraded NuMI neutrino source at Fermilab in conjunction with a 300-ton near-detector and a 14-kton far-detector to explore the neutrino sector. NOvA uses a fully active, finely segmented detector design that offers superb event identification capability, allowing precision measurements of electron (anti-)neutrino appearance and muon (anti-)neutrino disappearance. Through these NOvA will provide constraints on theta_13, theta_23, the atmospheric mass splitting, the neutrino mass hierarchy, and the CP-violating phase. This talk reviews NOvA's uniquely broad physics scope, including sensitivity updates, presents some early measures of the detector performance and discusses the experiment's construction and operation timeline.
Speaker: Matthew Tamsett (University of Sussex)
• 14:30 16:10
Parallel 5: Strongly Coupled gauge Theories River Room

#### River Room

• 14:30
The Yang-Mills vacuum wave-functional thirty-five years later 35m
Beside anniversaries of the important discoveries celebrated at this workshop, there is another worth to mention: The first paper attempting direct calculation of the Yang-Mills vacuum wave-functional was published in 1979 [J. Greensite, Nucl. Phys. **B158** (1979) 469]. I will review some recent results of the determination of the vacuum wave-functional in Monte Carlo simulations of SU(2) lattice gauge theory.
Speaker: Stefan Olejnik (Institute of Physics, Slovak Acad. Sci., Bratislava)
• 15:05
A new method for computing the quark-gluon vertex 35m
In this talk we present a new method for determining the nonperturbative quark-gluon vertex, which constitutes a crucial ingredient for a variety of theoretical and phenomenological studies. This new method relies heavily on the exact all-order relation connecting the conventional quark-gluon vertex with the corresponding vertex of the background field method, which is Abelian-like. The longitudinal part of this latter quantity is fixed using the standard gauge technique, whereas the transverse is estimated with the help of the so-called transverse Ward identities. This method allows the approximate determination of the nonperturbative behavior of all twelve form factors comprising the quark-gluon vertex, for arbitrary values of the momenta. Numerical results will be presented for the form factors in three special kinematical configurations (soft gluon and quark symmetric limit, zero quark momentum) and compared with the corresponding lattice data.
Speaker: Arlene Cristina Aguilar (University of Campinas)
• 15:40
Negative-Frequency Modes in Quantum Field Theory 30m River room

#### River room

We illustrate a number of interesting features of a nominal departure from standard quantum field theory, constructed so as to permit momentum eigenstates of both positive and negative energy. Postulating an additional discrete symmetry of the free field theory under the interchange of positive- and negative-frequency modes, we show that one can obtain tree-level source-to-source amplitudes that are manifestly causal, whilst being consistent with the standard S-matrix results. In addition, we highlight intriguing possibilities for both the naturalness and cosmological constant problems. Finally, we draw attention to potential issues with perturbative unitarity and Bloch-Nordsieck cancellation, commenting on a possible solution provided by resonance phenomena and the breakdown of naive perturbation theory. As a non-trivial example, we recover the Peskin-Takeuchi parametrization of the oblique corrections of the standard electroweak theory.
Speaker: Dr Peter Millington (Technische Universität München (TUM))
• 14:30 16:00
Parallel 7: Supersymmetry, Supergravity, Strings and Branes S7.06 7th floor Strand Bldg.

#### S7.06 7th floor Strand Bldg.

• 14:30
Convoluted Solutions in Supergravity 30m
Inspired by the convoluted solutions for two intersecting M2 branes in eleven-dimesnional supergravity, in which one brane in the system is completely localized along the overall and relative transverse coordinates while the other brane in the system is localized only along the overall transverse coordinates, we construct two classes of exact solutions to Einstein-Maxwell theory in six and higher dimensions. We show that the membrane configuration preserves four supersymmetries and upon dimensional reduction, the solutions provide intersecting configurations of three D-branes in type IIA supergravity. Moreover, we show that the metric functions in six and higher dimensions can be written as convolution-like integrals of two special functions. The solutions are regular everywhere and show a bolt structure on a single point in any dimensionality. Also, we find the exact nonstationary solutions to the Einstein-Maxwell theory with positive cosmological constant. We show that the cosmological solutions are expanding patches in asymptotically de Sitter spacetime.
Speaker: Masoud Ghezelbash (University of saskatchewan)
• 15:00
Sequestered de Sitter String Scenarios 30m
We present soft supersymmetry breaking terms in type IIB de Sitter string vacua after moduli stabilisation. We focus on models in which the Standard Model is sequestered from the supersymmetry breaking sources and the spectrum of soft-terms is hierarchically smaller than the gravitino mass.
Speaker: Dr Sven Krippendorf (University of Oxford)
• 15:30
Thermal Duality and Gravitational Collapse 30m
Thermal duality is a relationship between the behaviour of heterotic string models of the E(8)xE(8) or SO(32) types at inversely related temperatures, a variant of T duality in the Euclidean regime. This duality would have consequences for the nature of the Hagedon transition in these string models. We propose that the vacuum admits a family of deformations in situations where there are closed surfaces of constant area but high radial acceleration (a ‘string regularized’ version of a Penrose trapped surface), such as would be formed in situations of extreme gravitational collapse. This would allow a radical resolution of the ‘firewall paradox’ by allowing quantum effects to significantly modify the spacetime geometry around a collapsed object. A ‘string bremsstrahlung’ process would convert the kinetic energy of infalling matter in extreme gravitational collapse to form a region of the deformed vacuum, which would be equivalent to forming a high temperature string phase. A notable feature of this scenario is that the spectrum of final states would respect time reversal (T) symmetry, unlike conventional black holes.This process might have observable consequences for charged particles falling into a rotating collapsed object by producing high energy particles via a variant of the Penrose process.
Speaker: Mike Hewitt (Canterbury Christ Church University)
• 16:10 16:35
Coffee Break 25m River and parallel session rooms

#### River and parallel session rooms

• 16:35 19:45
Parallel 14: Discrete Symmetries in Strings and in GUT theories S7.06 7th floor Strand Bldg.

#### S7.06 7th floor Strand Bldg.

• 16:35
The origin of discrete symmetries in F-theory models and their role in particle physics 35m
We discuss the origin of discrete symmetries in F-theory models. Motivated by the neutrino sector, we focus on non-abelian discrete family symmetries associated to monodromies. We combine them with SU(5) GUT and examine their low energy implications.
Speaker: Prof. George Leontaris (Ioannina University)
• 17:10
Discrete Symmetries in F-theory Model Building 30m
F-theory is known to admit a number of discrete symmetries, such as $A_4$, $D_4$ and $Z_N$ symmetries. An introduction to the methods involved will be provided, with a view to discussing current work in the field.
Speaker: Andrew Meadowcroft (University of Southampton)
• 17:40
Discrete symmetries in the heterotic-string landscape 30m
We describe a new type of discrete symmetry that relates heterotic-string models. It is based on the spectral flow operator which is normally acting within a general $\cal N=(2,2)$ model. We use this operator to construct a map between $\cal N=(2,0)$ models. The landscape of $\cal N=(2,0)$ models is of particular interest among all heterotic-string models for two important reasons: 1. $N=1$ spacetime SUSY requires $(2,0)$ superconformal invariance and 2. models with the minimal $SO(10)$ unification structure, which is well motivated by the Standard Model of particle physics data, are of this type. This idea was inspired by a new discrete symmetry in the space of fermionic $Z_2\times Z_2$ heterotic-string models that exchanges the spinors and vectors of the $SO(10)$ GUT group, dubbed spinor-vector duality. We will describe how to generalize this to arbitrary internal Rational Conformal Field Theories (RCFTs).
Speaker: Panos Athanasopoulos
• 18:10
Break (5 min) 5m S7.06 7th floor Strand Bldg.

#### S7.06 7th floor Strand Bldg.

• 18:15
Mass insertion parameters from an SU(5)xS4xU(1) family summetry model. 30m
The aim of this work is to provide an explanation for the masses and mixings of the Standard Model fermionic content as well as for its supersymmetric extensions, using an S4xU(1) family symmetry in an SU(5) background. The results are given in terms of mass insertion parameters and are compared to the latest experimental limits.
Speaker: Maria Dimou (Southampton University)
• 18:45
Anomaly-free chiral fermion sets and gauge coupling unification 30m
We look for minimal chiral sets of fermions beyond the Standard Model that are anomaly-free and, simultaneously, vector-like particles with respect to color SU(3) and electromagnetic U(1). We then study whether the addition of such particles to the Standard Model particle content allows for the unification of gauge couplings at a high energy scale, above 5.0x10^15 GeV so as to be safely consistent with proton decay bounds. The possibility to have unifcation at the string scale is also considered. Inspired in grand unified theories, we also search for minimal chiral fermion sets that belong to SU(5) multiplets, restricted to representations up to dimension 50. It is shown that, in various cases, it is possible to achieve gauge unifcation provided that some of the extra fermions decouple at relatively high intermediate scales.
Speaker: Catarina Simões (IFPA, University of Liège)
• 19:15
SO(10) Grand Unification from M-theory on a G2-manifold 30m
We consider Grand Unified Theories based on $SO(10)$ which originate from $M$-theory on $G_2$-manifolds. In this framework we are naturally led to a novel solution of the doublet-triplet splitting problem involving an extra ${\bf 16}_X,{\bf {\overline{16}}}_X$ vector-like pair by considering discrete symmetries of the extra dimensions and preserving unification. Since Wilson line breaking preserves the rank of the gauge group, the necessary $U(1)$ gauge breaking is generated from extra multiplets. The main prediction of the approach is the existence of light states with the quantum numbers of a ${\bf 16}_X,{\bf {\overline{16}}}_X$ vector-like pair which could show up in future LHC searches.
Speaker: Miguel Crispim Romao (University of Southampton)
• 16:35 19:50
Parallel 1: Discrete symmetries (T, C, P), flavour, accidental symmetries Great Hall

#### Great Hall

• 16:35
TIME-REVERSAL, LOOP-ANTILOOP SYMMETRY AND THE BESSEL EQUATION 35m
TIME-REVERSAL, LOOP-ANTILOOP SYMMETRY AND THE BESSEL EQUATION GIUSEPPE VITIELLO Dipartimento di Fisica “E. R. Caianiello” Università di Salerno, 84080 Salerno, Italy and INFN, Gruppo Collegato di Salerno, Italy vitiello@sa.infn.it The Bessel equation is shown to be equivalent, under suitable transformations, to a system of two damped/amplified parametric oscillator equations, which have been used in the study of inflationary models of the Universe, thermal field theories and Chern-Simons gauge theories. The breakdown of loop-antiloop symmetry due to group contraction manifests itself as breaking of time-reversal symmetry. The relation between some infinite dimensional loop-algebras, such as the Virasoro-like algebra, and the Euclidean algebras e(2) and e(3) is also discussed.
Speaker: Giuseppe Vitiello (University of Salerno, Italy)
• 17:10
[Re]constructing Finite Flavour Groups: Horizontal Symmetry Scans from the Bottom-Up 30m
We present a novel procedure for identifying discrete, leptonic flavour symmetries, given a class of unitary mixing matrices. By creating explicit 3D representations for generators of residual symmetries in both the charged lepton and neutrino sector, we reconstruct large(r) non-abelian flavour groups using the GAP language for computational finite algebra. We use experimental data to construct only those generators that yield acceptable (or preferable) mixing patterns. Such an approach is advantageous because it 1) can reproduce known groups from other 'top-down' scans while elucidating their origins from residuals, 2) find new previously unconsidered groups, and 3) serve as a powerful model building tool for theorists wishing to explore exotic flavour scenarios. We test our procedure on a generalization of the canonical tri-bimaximal (TBM) form and discuss further work that is ongoing.
Speaker: Jim Talbert (University of Oxford)
• 17:40
Break (5 min) 5m
• 17:45
Discrete Flavor Symmetries and Origin of CP Violation 35m
We discuss the origin of CP violation in settings with a discrete (flavor) symmetry G. We show that physical CP transformations always have to be class-inverting automorphisms of G. This allows us to categorize finite groups into three types: (i) Groups that do not exhibit such an automorphism and, therefore, in generic settings, explicitly violate CP. In settings based on such groups, CP violation can have pure group-theoretic origin and can be related to the complexity of some Clebsch-Gordan coefficients. (ii) Groups for which one can find a CP basis in which all the Clebsch-Gordan coefficients are real. For such groups, imposing CP invariance restricts the phases of coupling coefficients. (iii) Groups that do not admit real Clebsch-Gordan coefficients but possess a class-inverting automorphism that can be used to define a proper (generalized) CP transformation. For such groups, imposing CP invariance can lead to an additional symmetry that forbids certain couplings. We make use of the so-called twisted Frobenius-Schur indicator to distinguish between the three types of discrete groups. We present one explicit example for each type of group, thereby illustrating the CP properties of models based on them. We also show that certain operations that have been dubbed generalized CP transformations in the recent literature do not lead to physical CP conservation.
Speaker: Mu-Chun Chen (University of California at Irvine)
• 18:20
Two invisible axion models with a non-minimal flavor structure 30m
In this talk I will present two invisible axion model implementations. The first one consists in an ultraviolet completion of the so-called aligned two-Higgs-doublet model that solves the strong CP problem. I will show that, for certain decoupling scenarios, mixing effects among the scalar fields allow for the possibility to obtain a rich scalar sector at the weak scale. The second model implementation is given by a class of invisible axion models with Flavour Changing Neutral Currents at tree-level controlled by the fermion mixing matrices. In this model, the PQ symmetry is constructed as a horizontal symmetry which provides a solution to the Strong CP problem and gives rise to a rich phenomenology. The presence of Flavour Changing Axion Interaction and the possibility to avoid the domain wall problem stand as the main features of this class of models. Right-handed neutrinos are also introduced to account for the smallness of active neutrinos masses via a Type I see-saw mechanism that relates the PQ symmetry breaking and the see-saw scales. Experimental limits on the axion couplings will also be discussed.
Speaker: Javier Fuentes-Martín (IFIC University of Valencia-CSIC)
• 18:50
CKM and PMNS Mixing Matrices from Discrete Subgroups of SU(2) 30m
I have the only first principles derivation of the PMNS and CKM matrices within the realm of the Standard Model lagrangian. The mixings originate from the generators of three discrete (i.e., finite) binary rotational subgroups of the EW local gauge group SU(2) x U(1) for three lepton families in R
$^3$ and four related discrete binary rotation subgroups for four quark families in R$^4$. For each group two of its three generators match the Pauli generators for SU(2), but the different third generators must act together in a linear superposition to match the third Pauli generator. The results dictate the angles for the PMNS and CKM4 matrices. The CKM matrix can be extracted from CKM4 and assuming unitarity. Consequently, one can predict three lepton families and four quark families. However, a sterile neutrino cannot be eliminated. If the two new quarks in the predicted fourth quark family exist, the SM lagrangian may be an excellent approximation all the way down to the Planck scale. In addition, putting the fourth quark family mass values in the Jarlskog expression increases the CPV by more than 10$^{13}$, thereby providing a possible explanation of the BAU. The mathematical details are in the online peer reviewed paper at http://www.ptep-online.com/index_files/2014/PP-38-03.PDF
Speaker: Franklin Potter (S)
• 16:35 18:20
Parallel 5: Strongly coupled gauge theories River Room

#### River Room

• 16:35
A 3d effective lattice theory for Yang-Mills and QCD thermodynamics 35m
QCD thermodynamics is crucial for the physics of the early universe, heavy ion collisions and compact stars. However, predictions by lattice simulations are very costly or, in the case of finite baryon density, even impossible because of a sign problem. Starting from Yang-Mills theory, it is shown how to use strong coupling methods to construct a 3d effective theory which accurately reproduces the deconfinement phase transition. The generalisation to QCD, which is valid for heavy quarks, has only a mild sign problem in the case of finite density and can be simulated efficiently.
Speaker: Owe Philipsen (Goethe-University Frankfurt)
• 17:10
Variationl Study of SU(3) Gauge Theory by Stationary Variance 35m
> The principle of stationary variance is advocated as a viable variational approach to gauge theories where the simple Gaussian Effective Potential (GEP) is known to be useless. The method can be regarded as a second-order extension of the GEP and seems to be suited for describing the strong coupling limit of non-Abelian gauge theories. The single variational parameter of the GEP is replaced by trial unknown two-point functions, with infinite variational parameters to be optimized by the solution of a set of integral equations. The stationary conditions can be easily derived by the self-energy, without having to write the effective potential, making use of a general relation between self-energy and functional derivatives that has been proven to any order. By that method, the low-energy limit of pure Yang-Mills $SU(3)$ gauge theory has been studied in Feynman gauge. In terms of standard irreducible graphs, the stationary equations are written as a set of coupled non-linear integral equations for the gluon and ghost propagators. A physically sensible solution is found for any strength of the coupling. The gluon propagator is finite in the infrared, with a dynamical mass that decreases as a power at high energies. At variance with some recent findings in Feynman gauge, the ghost dressing function does not vanish in the infrared limit and a decoupling scenario emerges as recently reported for the Landau gauge. ##INTRODUCTION ## There is a growing consensus on the utility of variational methods as analytical tools for a deeper understanding of the infrared (IR) limit of non-Abelian gauge theories. The IR slavery of these theories makes the standard perturbation theory useless below some energy scale, and our theoretical knowledge of the IR limit relies on lattice simulation and on non-perturbative techniques like functional renormalization group and Dyson-Schwinger equations. Variational methods have been developed[1-7] as a complement to these analytical approaches and quite recently the method of stationary variance[8, 9] has been advocated as a powerful second order extension of the Gaaussian Effective Potential (GEP)[10–13]. The GEP is a genuine variational method and has been successfully applied to many physical problems in field theory, from scalar and electroweak theories[14–20] to superconductivity[21–23] and antiferromagnetism[24], but turns out to be useless for gauge interacting fermions[25-26]. Actually, since the GEP only contains first order terms, it is not suited for describing the minimal coupling of gauge theories that has no first-order effects. Several methods have been explored for including fermions[20] and higher order corrections[25,26], sometimes spoiling the genuine variational character of the method. By a formal higher order extension of the GEP[27] the method of stationary variance has been developed as a genuine variational method that keeps in due account second order effects and seems to be suited to deal with the minimal coupling of gauge theories. While the method has been shown to be viable for the simple Abelian case of QED[28], its full potentialities have not been explored yet. As a non-perturbative tool that can deal with fermions in gauge theories, the method seems to be very useful for exploring the IR limit of QCD, and its natural application field is the non-Abelian SU(3) gauge theory[29]. ## YANG-MILLS $SU(3)$ BY STATIONARY VARIANCE ## A full study of QCD by the method of stationary variance is still far away. As a first step, in Ref.[29] we explored the solution of the stationary equations for pure Yang-Mills SU(3) theory. While the method is a genuine variational tool that does not require any small parameter, the technique is based on standard Feynman rules of perturbation theory. The single variational parameter of the GEP is replaced by trial unknown two-point functions, with infinite variational parameters to be optimized by the solution of a set of integral equations, the stationary equations. However, these equations can be easily derived by the self-energy, without having to write the effective potential, making use of a general relation between self-energy and functional derivatives that has been proven to any order[27]. For pure Yang-Mills theory the method of stationary variance provides a set of non-linear coupled integral equations whose solutions are the propagators for gluons and ghosts. Therefore the work has a double motivation: the technical aim of showing that the method is viable and a solution does exist (which was not obvious nor proven in general), and the physical interest on the gluon propagator in the IR limit, where its properties seem to be related to the important issue of confinement. On the technical side, having shown that a sensible untrivial solution does exist is a major achievement that opens the way to a broader study of QCD by the same method. Inclusion of quarks would be straightforward as some fermions, the ghosts, are already present in the simple Yang-Mills theory, and they already seem to play well their role of canceling the unphysical degrees of freedom. Other important technical issues are gauge invariance, renormalization and the choice of a physical scale. The method is not gauge invariant, and no effort has been made to restore gauge invariance at this first stage. While there are several ways to attempt it[1,30], in this first step a fixed gauge has been used, namely the Feynman gauge where the calculation is easier. In this gauge, the properties of the solution are explored in order to see if any unphysical feature emerges for the propagator and the polarization function. Actually the polarization function is found approximately transverse up to a constant mass shift due to the dynamical mass generation. As far as the solution satisfies, even approximately, the constraints imposed by gauge invariance, the method is acceptable on the physical ground. On the other hand the gluon propagator is not a physical observable and is known to be a gauge-dependent quantity. Of course, since the solution depends on the gauge, the choice of working in Feynman gauge could be non-optimal, and the method could be improved by exploring other gauge choices, like Landau gauge. Besides being easier, working in Feynman gauge is also interesting from the physical point of view, as there are very few data available on the gluon propagator in this gauge. Since lattice simulations are the most natural benchmark for any variational calculation in the IR limit, the regulating scheme is borrowed from lattice simulation, with an energy cutoff and a bare coupling that depends on it. Renormalization Group (RG) invariance requires that the physical observables are left invariant by a change of the cutoff that is followed by the corresponding change of the bare coupling. Then, renormalized physical quantities can be defined that do not depend on the cutoff. The only free parameter of the theory is the energy scale, that must be fixed by a comparison with the experimental data or lattice simulations. No other fit parameter has been introduced in the method, especially mass counterterms that are forbidden by the gauge invariance of the Lagrangian. On the physical side, the properties of the gluon propagator in Feynman gauge are basically unexplored. In Coulomb gauge[2–5, 7] and in Landau gauge[6, 31–38] there has been an intense theoretical work in the last years. In Landau gauge theoretical and lattice data are generally explained in terms of a decoupling regime, with a finite ghost dressing function and a finite massive gluon propagator. The more recent findings confirm the original prediction[39] of a dynamical mass generation for the gluon. In Feynman gauge we do not expect a very different scenario. A finite ghost propagator has been recently proposed[40], but there are no lattice data available that could confirm it. That makes the study of the Feynman gauge more interesting. As discussed in Ref.[29], in the present work no important differences are found with respect to the Landau gauge. A decoupling scenario emerges, with very flat ghost dressing functions, flatter than expected, and a ghost propagator that diverges in the IR limit where the ghost behaves like a free zero-mass particle. A finite gluon propagator is found in the IR limit, with a dynamical mass that saturates at about 0.5-0.8 GeV and decreases as a power in the high energy limit. Unfortunately the quantitative predictions are biased by an approximate estimate of the energy scale due to the lack of lattice data in Feynman gauge. Any quantitative estimate of the gluon mass requires that an accurate energy scale should be fixed first. We can only say that a qualitative agreement is found with other predictions in Feynman gauge. ## CONCLUDING REMARKS ## In summary, one of the major achievements of the present work is the proof that a physically consistent solution does exist for the coupled set of non-linear integral equations that arise from the condition of stationary variance. Since pure Yang-Mills theory already contains fermions (the ghosts), inclusion of quarks in the formalism is straightforward, and would open the way to a broader study of QCD by the same technique. The method can be improved in many way. We did not bother about gauge invariance in this first approach, but the properties of the polarization function, namely the correct cancellations of the unphysical degrees of freedom by the ghosts, show that the constraints of gauge invariance can be satisfied, at least approximately, by the variational solution. While some attempts could be made for enforcing gauge invariance[1,30], a physically motivated choice for the gauge would probably improve the approximation. Landau gauge would be a good candidate, as it would enforce the transversality in the polarization function from the beginning. An other interesting further development would come from the extension of the formalism to the general case of a finite external background field. For a scalar theory that kind of approach allows a consistent definition of approximate vertex functions by the functional derivative of the effective action. For the GEP these functions can be shown to be the sum of an infinite set of bubble graphs[16]. A similar approach would give a more consistent approximation for the gluon propagator in the present variational framework. Eventually, the inclusion of quarks would lead to a direct comparison with the low energy phenomenology of QCD. ## REFERENCES ## 1. I.L. Kogan and A. Kovner, Phys. Rev. D 52, 3719 (1995). 2. C. Feuchter and H. Reinhardt, Phys. Rev. D 70, 105021 (2004). 3. H. Reinhardt and C. Feuchter, Phys.Rev. D 71, 105002, (2005). 4. D. Epple, H. Reinhardt, W. Schleifenbaum, A.P. Szczepaniak, Phys. Rev. D77, 085007,(2008), arXiv:0712.3694 5. H. Reinhardt, D. R. Campagnari, A. P. Szczepaniak, Phys. Rev. D84, 045006 (2011), arXiv:1107.3389. 6. M. Quandt, H. Reinhardt, J. Heffner, Phys. Rev. D 89, 065037 (2014). 7. A. P. Szczepaniak, Phys.Rev. D 69, 074031 (2004). 8. F. Siringo and L. Marotta, Eur. Phys. J. C {\bf 44}, 293 (2005). 9. F. Siringo, Mod. Phys. Lett. A, Vol. 29, No. 5 (2014) 1450026, arXiv:1308.4037. 10. L.I. Schiff, Phys. Rev. 130, 458 (1963). 11. G. Rosen, Phys. Rev. 172, 1632 (1968). 12. T. Barnes and G. I. Ghandour, Phys. Rev. D 22, 924 (1980). 13. P.M. Stevenson, Phys. Rev. D 32, 1389 (1985). 14. F. Siringo, Phys. Rev. D 62, 116009 (2000). 15. F. Siringo, Europhys. Lett. 59, 820 (2002). 16. F. Siringo and L. Marotta, Int. J. Mod. Phys. A25, 5865 (2010), arXiv:0901.2418v2. 17. R. Ibanez-Meier, I. Stancu, P.M. Stevenson, Z. Phys. C 70, 307 (1996). 18. F. Siringo, L. Marotta, Phys. Rev. D 78, 016003 (2008). 19. F. Siringo and L. Marotta, Phys. Rev. D 74, 115001 (2006). 20. F. Siringo, Phys. Rev. D 86, 076016 (2012), arXiv: 1208.3592v2. 21. M. Camarda, G.G.N. Angilella, R. Pucci, F. Siringo, Eur. Phys. J. B 33, 273 (2003). 22. L. Marotta, M. Camarda, G.G.N. Angilella and F. Siringo, Phys. Rev. B 73, 104517 (2006). 23. C. K. Kim, A, Rakhimow, Jae Hyung Hee, Eur. Phys. Jour. B 39, 301 (2004). 24. L. Marotta and F. Siringo, Mod. Phys. Lett. B 26, 1250130 (2012), arXiv:0806.4569v3. 25. I. Stancu and P. M. Stevenson, Phys. Rev. D 42, 2710 (1990). 26. I. Stancu, Phys. Rev. D 43, 1283 (1991). 27. F. Siringo, Phys. Rev. D 88, 056020 (2013), arXiv:1308.1836. 28. F. Siringo, Phys. Rev. D 89, 025005 (2014), arXiv:1308.2913. 29. F. Siringo, arXiv:1408.5313. 30. A. C. Aguilar, J. Papavassiliou, Phys. Rev. D81, 034003 (2010), arXiv:0910.4142. 31. A. C. Aguilar, D. Binosi, J. Papavassiliou, Phys. Rev. D78, 025010 (2008), arXiv:0802.1870. 32. A. C. Aguilar, D. Binosi, J. Papavassiliou, J. Rodriguez-Quintero, Phys. Rev. D80, 085018 (2009), arXiv:0906.2633. 33. A. C. Aguilar, D. Ibanez, J. Papavassiliou, Phys. Rev. D 87, 114020 (2013), arXiv:1303.3609. 34. A. C. Aguilar, D. Binosi, J. Papavassiliou, Phys. Rev. D 89, 085032 (2014), arXiv:1401.3631. 35. A. C. Aguilar, D. Binosi, D. Ibanez, J. Papavassiliou, arXiv:1405.3506. 36. I.L. Bogolubsky, E.M. Ilgenfritz, M. Muller-Preussker, A. Sternbeckc, Phys. Lett. B 676, 69 (2009), arXiv:0901.0736v3. 37. A. Cucchieri and T. Mendes, Phys. Rev. D 71, 051902(R) (2005). 38. A. Cucchieri and T. Mendes, arXiv:0710.0412v1. 39. J. M. Cornwall, Phys. Rev. D 26, 1453 (1982). 40. A. C. Aguilar, J. Papavassiliou, Phys.Rev. D 77, 125022 (2008), arXiv:0712.0780v1.
Speaker: Fabio Siringo (Università degli Studi di Catania)
• 17:45
DSE-isnpired model for the Pion GPD 35m
We sketch an approach to a computation of the pion's valence dressed-quark GPD based upon a Rainbow-Ladder truncation of the QCD Dyson-Schwinger equations. In particular, our starting point is the appropriate recasting of the computed GPD as the well-known double distribution ansatz, which automatically fulfils all the constraints required by the observing of discrete and Lorentz symmetries.
Speaker: José Rodriguez Quintero (University of Huelva)
• 16:35 17:45
Parallel 6: Foundations of Quantum Theory, 50 years Bell’s Inequalities K-1.56

#### K-1.56

• 16:35
50 years of Bell's theorem and Weak Interaction Processes 35m
John St. Bell was known and hired as a "particle physicist" when he came up with his work on hidden parameters. The aim of this talk is to discuss whether his theorem can be brought back to those systems that do not build up ordinary matter and light. Indeed, entanglement can be witnessed in decay processes governed by the weak interaction, e.g., in flavour oscillating systems or hyperon systems, BUT: Can an experimentally conclusive test be found proving the existence of correlations that are stronger than those allowed by classical physics? It is not straightforwardly to apply Bell's theorem to unstable systems. For neutral entangled K-mesons finally Bell’s theorem could be generalized without spoiling the conclusiveness [1] and allows for an experimental test, however, for the entangled Lambda-Antilambda system such a solution has not yet been found [2]. The findings [1] turned out to be also surprising from the theoretical point of view since a connection between the violation of Bell's theorem and the tiny violation of the CP symmetry (C..charge conjugation, P...parity) has been found. Herewith, e.g. the security of quantum cryptography protocols gets related to the small difference between a world of matter and antimatter that itself can be attributed to the unsolved problem why we live in a universe dominated by matter. In the last part of the talk I point out, why weakly decaying systems are a unique laboratory to study foundations of quantum mechanics, e.g. for testing decoherence models or collapse models [3] or for quantum information theoretic tasks [2]. [1] Hiesmayr et al., "Revealing Bell's Nonlocality for Unstable Systems in High Energy Physics", EPJ C , Vol. 72, 1856 (2012). [2] Hiesmayr, “Weak Interaction Processes: Which Quantum Information is revealed?”, arXiv:1410.1707 [3] Brahami et al., "Are collapse models testable with quantum oscillating systems? The case of neutrinos, mesons, chiral molecules", Nature:Scientific Reports 3, 1952 (2013).
Speaker: Beatrix Hiesmayr (University of Vienna)
• 17:10
Whispers from the collapse of the w.f: spontaneously emitted radiation 35m
The “measurement problem” in quantum mechanics continues to remain a problem which needs an explanation. A possible solution to this problem is the modification of the Schrodinger equation within the so-called dynamical reduction models. The dynamical reduction models were put forward alternatively to the "standard" quantum mechanics' Schrodinger equation, followed by a "alla von Neumann" collapse of the wave-function, implementing a (nonrelativistic) dynamical reduction/collapse models, by adding a non-linear and stochastic terms to the Schrodinger equation. Considering the relevance of this conceptually new model(s), it is of utmost importance to study its experimental consequences, where the predictions are diverging from the standard equations, and to perform dedicated experiments to check it. We discuss various ideas to find experimental signatures for the collapse of the wave function within the dynamical reduction models, starting with the measurement of the spontaneously emitted X rays predicted in the framework the new theory – whispers of the collapse – which is the most promising method to put the strongest limits of the collapse model parameter lambda.
Speaker: Catalina Curceanu (LNF-INFN)
• 17:45 18:30
Break - Change of Room 45m
• 18:30 19:35
Parallel 6b: Foundations of Quantum Theory, Pauli Principle Tests River Room

#### River Room

• 18:30
Quantum mechanical models, conservation laws and a discrete action principle 35m
It has been shown that the dynamics of discrete (integer-valued) Hamiltonian cellular automata can only be defined consistently, if it is linear in analogy to the linearity of unitary evolution in quantum mechanics. This suggests to look for an invertible map between such automata and continuous quantum mechanical models. Based on sampling theory, such a map can indeed be constructed and leads to quantum mechanical models which incorporate a fundamental scale. The admissible observables, the one-to-one correspondence of the respective conservation laws, and the existence of solutions of the modified dispersion relation for stationary states are discussed. References: H.-T. Elze, Action principle for cellular automata and the linearity of quantum mechanics, Phys. Rev. A 89, 012111 (2014) [arXiv:1312.1615]; H.-T. Elze, JPCS 504 (2014) 012004 [arXiv:1403.2646]; H.-T. Elze, EPJ WoC 78, 02005 (2014) [arXiv:1407.2160].
Speaker: Hans-Thomas Elze (Universita di Pisa)
• 19:05
High sensitivity tests of the Pauli Exclusion Principle with VIP2 30m
The Pauli Exclusion Principle (PEP) is one of the most fundamental rules of nature and thus a major pillar of modern physics. According to many observations PEP must be extremely well fulfilled. Nevertheless numerous experimental investigations were performed to search for a small PEP violation. The experiment VIP2 at the Gran Sasso underground laboratory is designed to test the Pauli Exclusion Principle for electrons with high sensitivity by searching for forbidden X-ray transitions in copper atoms. VIP2 aims to improve the PEP violation limit obtained with our preceding experiment VIP by orders of magnitude. The experimental method, comparison of different PEP tests based on different assumptions and the developments for VIP2 will be presented.
Speaker: Dr Johann Marton (Oesterreichische Akademie der Wissenschaften)
• Thursday, 4 December
• 08:55 09:00
Registration: Desk (Great Hall) 8:30 - 17:00 5m
• 09:00 13:15
PLENARY 3 Great Hall

#### Great Hall

• 09:00
TeV Scale Lepton number Violation and Baryogenesis 45m
I will discuss the possibility that physics of neutrino mass is a TeV scale phenomenon which can be probed at the LHC via the searches for right handed W-bosons and the heavy right handed neutrinos and other low energy experiments.The same TeV scale model also leads to successful leptogenesis as a way to understand the origin of matter in the universe. Thus, the Large Hadron Collider can provide information not only on supersymmetry, extra space dimensions as well as the nature of dark matter but also on the physics behind the neutrino masses and the mechanism behind the origin of matter.
Speaker: Rabindra Mohapatra (University of Maryland, College Park)
• 09:45
Symmetry Improved CJT Effective Potential 45m
The formalism introduced by Cornwall, Jackiw and Tomboulis (CJT) provides a systematic analytic approach to consistently describing non-perturbative effects in Quantum Thermal Field Theory. One major limitation of the CJT effective action is that its loopwise expansion introduces residual violations of possible global symmetries, thus giving rise to massive Goldstone bosons in the spontaneously broken phase of the theory. In my talk I will present a novel symmetry-improved CJT formalism which consistently encodes global symmetries in a loopwise expansion. Unlike other methods, I will illustrate how the symmetry-improved CJT effective action satisfies a number of important field-theoretic properties, such as the masslessness of the Goldstone boson and the fact that the phase transition is of second order in O(N) theories, already in the Hartree-Fock approximation. After taking the sunset diagrams into account, I show how the symmetry-improved CJT approach properly describes the threshold properties of the massless Goldstone boson and the Higgs particle within quantum loops. Finally, I will briefly outline the derivation of a symmetry-improved CJT effective potential, in which new topologies of infinite class of graphs can be resummed that go well beyond the standard Coleman--Weinberg effective potential. [This presentation is based on my paper with Daniele Teresi, Nucl. Phys. B874 (2013) 594.]
Speaker: Apostolos Pilaftsis (University of Manchester (GB))
• 10:30
Coffee Break 30m Great Hall and River Room

#### Great Hall and River Room

• 11:00
Results from the Heavy-Ion Programme at the CERN LHC 45m
At extreme energy densities, hadronic matter undergoes a phase transition into a deconfined system of quarks and gluons, known as a Quark-Gluon Plasma (QGP). Such a state of matter may be formed by colliding ultra-relativistic heavy-ions together, which reproduce the high temperatures and densities thought to have existed about ten microseconds after the Big Bang. Lead ions have been accelerated and collided in the Large Hadron Collider (LHC) at CERN in order to allow experiments to study of the properties of the QGP. Data from proton-proton and proton-lead collisions, where no QGP formation is expected, have also been collected and analysed as a comparison to the lead-lead data. A brief summary of some of the main results from lead-lead collisions, at the LHC, will be presented together with relevant results from proton-proton and proton-lead collisions.
Speaker: David Evans (University of Birmingham (GB))
• 11:45
Testing Non-minimal Higgs sector at Colldiers 45m
Testing models with Higgs doublets at LHC will be discussed. I will focus on the Inert Doublet Model, with the exact Z2 symmetry, which offers viable Dark Matter candidates. LHC data together with Planck results on relic density provide very strong constraints on DM mass and its coupling to the Higgs boson. Some results on the potential of ILC in testing such models will be shown as well.
Speaker: Prof. Maria Krawczyk (Institute of Theoretical Physics, Warsaw University)
• 12:30
History of Electroweak Symmetry Breaking 45m
In this talk, I will recall the history of the development of the unified electroweak theory, incorporating the symmetry-breaking Higgs mechanism, as I saw it from my standpoint as a member of Abdus Salam's group at Imperial College. I will start by describing the state of physics in the years after the Second World War, explain how the goal of a unified gauge theory of weak and electromagnetic interactions emerged, the obstacles encountered, in particular the Goldstone theorem, and how they were overcome, followed by a brief account of more recent history, culminating in the historic discovery of the Higgs boson in 2012.
Speaker: Prof. Tom W.B. Kibble (Imperial College London)
• 13:15 14:30
Lunch Break 1h 15m Great Hall and River Room

#### Great Hall and River Room

• 14:30 16:05
Parallel 1: Discrete symmetries (T, C, P), flavour, accidental symmetries S7.06 7th floor Strand Bldg.

#### S7.06 7th floor Strand Bldg.

• 14:30
Hunting for New Physics with vector-like quarks 30m
Extending the Standard Model through the inclusion of additional vector-like quarks provides a rich playground for New Physics searches both in the Flavour sector and at the LHC. A detailed analysis of present constraints and future prospects with special emphasis on potential deviations from the Standard Model expectations in selected observables is presented.
Speaker: Dr Miguel Nebot Gómez (CFTP - Lisbon)
• 15:00
Order and Anarchy hand in hand in 5D SO(10) 30m
A mechanism to generate flavour hierarchy via 5D wave-function localization is revisited in the context of SO(10) grand unified theory. In an extra-dimension compactified on an orbifold, fermions (living in the same 16 representation of SO(10) ) result having exponential zero-modes profiles. The breaking of SO(10) down to SU(5) \times U(1)_X provides the key parameter that distinguishes the profiles of the different SU(5) components inside the same 16 representation. Utilizing suitable scalar fields, a predictive model for fermion masses and mixing is constructed and shown to be viable with the current data through a detailed numerical analysis. All the Yukawa couplings in the model are anarchical and of order unity, while the hierarchies among different fermions result only from zero-mode profiles. The naturalness of anarchical Yukawa couplings is studied, showing a preference for a normal ordered neutrino spectrum; predictions for various observables in the lepton sector are also derived. The scalar field content of the model is also suitable to solve the doublet-triplet splitting problem through the "missing partner" mechanism.
Speaker: Denise Vicino (INFN University of Padova)
• 15:30
Theoretical status of B->K(*)mumu and New Physics. 35m
..
Speaker: Prof. Matias Joaquim (Universitat Autonoma Barcelona)
• 14:30 16:05
Parallel 4: Experiments-discrete-symmetries Anatomy Museum

#### Anatomy Museum

• 14:30
Study of CP asymmetry in B0 - antiB0 mixing using inclusive dilepton samples in BaBar 35m
The asymmetry between same sign inclusive dilepton samples l+ l+ and l- l- from semileptonic B decays in Upsilon(4S) -> B0 antiB0 events allows us to compare B mixing probabilities P(antiB0 -> B0) and P(B0 -> antiB0), and therefore to test the T and CP invariance. We present the measurement of CP asymmetry in inclusive dilepton samples with the full BaBar dataset near Upsilon(4S) resonance, corresponding to 471 million B-antiB pairs.
Speaker: Isabella Garzia (INFN)
• 15:05
ChiPT tests at NA48 and NA62 experiments at CERN 30m
New final results from an analysis of about 400 K+- --> pi+- gamma gamma rare decay candidates collected by the NA48/2 and NA62 experiments at CERN during low intensity runs with minimum bias trigger configurations are presented. The results include a model-independent decay rate measurement and fits to Chiral Perturbation Theory (ChPT) description. The data support the ChPT prediction for a cusp in the di-photon invariant mass spectrum at the two pion threshold.
Speaker: Massimo Lenti (Universita e INFN (IT))
• 15:35
Rare decays at LHCb 30m
LHCb is a forward spectrometer covering a unique rapidity range at the LHC and with excellent capability to detect decays of heavy flavour mesons. LHCb has recoreded an integrated luminosity of 3fb-1 of proton-proton collisions during 2011 and 2012. Recent results from the LHCb in rare decays of beauty and charm mesons are shown.
Speaker: Fatima Soomro (Ecole Polytechnique Federale de Lausanne (CH))
• 14:30 16:15
Parallel 5: Strongly coupled gauge theories River Room

#### River Room

• 14:30
The density of states approach for the simulation of finite density quantum field theories 35m
Finite density quantum field theories have evaded first principle Monte-Carlo simulations due to the notorious sign-problem. The partition function of such theories appears as the Fourier transform of the generalised density-of-states, which is the probability distribution of the imaginary part of the action. With the advent of Wang-Landau type simulation techniques and recent advances [1], the density-of-states can be calculated over many hundreds of orders of magnitude. Current research addresses the question whether the achieved precision is high enough to reliably extract the finite density partition function, which is exponentially suppressed with the volume. In my talk, I review the state-of-play for the high precision calculations of the density-of-states as well as the recent progress for obtaining reliable results from highly oscillating integrals. I will review recent progress for Z3 and phi^4 quantum field theories for which results can be obtained from the simulation of the dual theory, which appears to free of a sign problem. [1] K Langfeld, B Lucini, A Rago, Phys .Rev. Lett. 109 (2012) 111601.
Speaker: Kurt Langfeld (Plymouth University)
• 15:05
Hadron properties using Dyson-Schwinger and Bethe-Salpeter equations 35m
The combination of Dyson-Schwinger and Bethe-Salpeter equations allows, in principle, for an *ab-initio* continuum-QCD study of hadrons and their properties. Glueballs, mesons, baryons, etc. are all treated in a unified framework. Moreover it has the advantage that that it gives access to all momentum regimes and all quark masses, connecting the deep infrared to perturbative QCD and light- and heavy-quark physics. The major downside is, however, the necessity of truncationg both Dyson-Schwinger and Bethe-Salpeter equations to make the problem tractable. However, guided by symmetries such as Poincare invariance, chiral symmetry, etc. one can define a systematic procedure to successively incorporate interaction terms in the calculations. The purpose of the presentation is to discuss this procedure as well as to illustrate it with some selected results.
Speaker: Dr Hèlios Sanchis Alepuz (Justus-Liebig University Giessen)
• 15:40
Quantum Field Theory of Magnetic Monopoles 35m
In spite of a vast amount research over several decades, the behaviour of magnetic monopoles in quantum field theory is still poorly understood. Quantum field theory formulation of elementary magnetic monopoles is plagued by lack of manifest locality and Lorentz invariance, which makes calculations very cumbersome. Solitonic 't Hooft-Polyakov monopoles avoid this problem, but even in their case calculating genuine quantum effects is difficult, and very few results exist. Even basic observables such as the pair production of rate of monopoles in particle collisions cannot currently be calculated. I will describe a non-perturbative lattice field theory approach to this problem, and present results for both 't Hooft-Polyakov and elementary magnetic monopoles.
Speaker: Prof. Arttu Rajantie (Imperial College Sci., Tech. & Med. (GB))
• 14:30 16:05
Parallel 9: Higgs physics @ LHC, discrete symmetries @ LHC, new facilities Great Hall

#### Great Hall

• 14:30
Higgs Physics: Review of recent results and prospects from ATLAS and CMS 30m
We present an overview of recent results in Higgs boson physics obtained with the ATLAS and CMS experiments at the Large Hadron Collider (LHC) located at CERN, Geneva. The focus is on measurements of the properties of the recently discovered Higgs boson with a mass of about 125 GeV. We will then present a brief selection of results in searches for Higgs bosons beyond the Standard Model. We will close by discussing prospects of future Higgs boson measurements and searches at the LHC.
Speaker: Martin Flechl (Austrian Academy of Sciences (AT))
• 15:00
How effective is the Standard Model effective field theory? 30m
The discovery of the Higgs boson closes the last remaining degree of freedom in the space of Standard Model physics, thus allowing unprecedented model-independent sensitivity to BSM physics. We may use this sensitivity by formally treating the Standard Model the way it has always been thought of: as an effective field theory supplemented by higher-dimensional operators. This approach parametrizes all possible ways decoupled new physics may enter in experimental observables. In this talk we place limits on a complete basis of dimension-6 operators from electroweak precision tests at LEP, as well as triple-gauge couplings and Higgs measurements at the Tevatron and LHC.
Speaker: Tevong You (King's College London)
• 15:30
Natural Standard Model Alignment in the Two Higgs Doublet Model 30m
In order to satisfy the current LHC Higgs data, which require the couplings of the observed 125 GeV Higgs boson to be close to the Standard Model (SM) expectations, any extended Higgs sector must lead to the so-called SM 'alignment limit'. In the context of the Two Higgs Doublet Model (2HDM), this alignment is often associated with either decoupling of the heavy Higgs sector or accidental cancellations in the 2HDM potential. In this talk, we present a symmetry justification for 'natural' alignment without decoupling or fine-tuning. We show that there exist only three different symmetry realizations which could lead to a natural alignment. We discuss some phenomenological implications of the Maximally-Symmetric 2HDM and propose new collider signals for the heavy Higgs sector, which could be searched for during the Run-II phase of the LHC.
Speaker: Bhupal Dev (University of Manchester)
• 16:15 16:35
Coffee Break 20m River Room, parallel session rooms

#### River Room, parallel session rooms

• 16:35 19:40
Parallel 10: LHC and dark matter experiments S7.06 7th floor Strand Bldg.

#### S7.06 7th floor Strand Bldg.

• 16:35
SuperCDMS: Results on low mass WIMPs and future perspectives 30m
The SuperCDMS experiment attempts to detect WIMP dark matter particles through their elastic scattering off Ge nuclei. The simultaneous measurement of the energy deposited in ionization and phonons allows for an excellent discrimination of nuclear recoils (expected from WIMP interactions) versus electron recoils (due to background events). The current experimental setup features new detectors (iZIPs) which are instrumented on both sides with interleaved ionization and phonon sensors and allow to separate surface and bulk events, thereby eliminating the main source of background of the previous CDMS II phase. Using this full background rejection capability, and operating at a very low analysis threshold ($1.6-10$ keV$_{nr}$) we have carried out a search for low-mass WIMPs. An exposure of 577 kg days was analysed for WIMPs with mass below 30 GeV, with the signal region blinded. An upper bound was extracted on the WIMP-nucleon scattering cross-section, which probes new parameter space for WIMP masses below 6 GeV and is in tension with the dark matter interpretation of previous experimental results.
Speaker: David G. Cerdeno (University of Durham)
• 17:05
ADMX Results on Axion Searches 25m
I present a progress report on the direct search for dark matter axions with ADMX upgraded with low noise RF SQUID amplifiers and cryogenics. Axions are a well motivated candidate to explain the discrepancy between the observed baryonic matter density and that inferred from precision measurements of the microwave background anisotropy, gravitational lensing, and the dynamics of spiral galaxies. As a pseudo-Goldstone boson associated with spontaneous breaking of the PQ symmetry, axions gain further credibility from the Higgs discovery. The ADMX experiment utilises a cryogenic tuneable electromagnetic resonator immersed in a static magnetic field to search for axions at micro electron volt scales. The axion field undergoes Primakov  conversion into microwave photons when the frequency of a TM resonance of the cavity corresponds to the energy per axion. Background originates from the physical cavity temperature added to the effective noise temperature of the receiver electronics. By reducing the temperature of the axion receiver, we aim for an improved rate of search of the allowed window of axion masses.
Speaker: Edward Daw (The University of Sheffield)
• 17:30
Recent results from ALICE and future prospects 30m
During the first LHC run the ALICE experiment collected data from pp, p-Pb and Pb-Pb collision systems. A selection of recent results will be presented, including those which focus on characterisation of the deconfined system formed in heavy-ion collisions. The future prospects for Run 2 and for the upgrade of ALICE beyond that will also be discussed.
Speaker: Lee Barnby (University of Birmingham (GB))
• 18:00
Break (5 min) 5m S7.06 7th floor Strand Bldg.

#### S7.06 7th floor Strand Bldg.

• 18:05
Latest results from CUORE-0 and status of CUORE 30m
Aiming to discover neutrinoless double beta decay from $^{130}$Te, the CUORE experiment continues to make progress at Laboratori Nazionali del Gran Sasso (LNGS). CUORE-0, a 1/19 mass replica of CUORE, is a 52 bolometer array that continues to take data providing validation for the methods and strategies undertaken for CUORE. We will present the latest results from CUORE-0 and milestones achieved by the ongoing commissioning of CUORE. Furthermore, we will summarize R&D with bolometers for future generation double-beta decay experiments.​
Speaker: Kevin Hickerson (UCLA)
• 18:35
Non-SUSY BSM Searches: Recent Results from ATLAS & CMS 30m
The Standard Model of particle physics is a sensational success, especially since the discovery the 125 GeV Higgs boson. However, there are still numerous unanswered questions… Why is the Higgs so light? Do the interactions couplings unify and how can gravity be included? Why three fermion generations? What is dark matter? Theories Beyond the Standard Model (BSM), such as Grand Unified Theories, Extra Dimensions or Technicolour are trying to answer these questions. In this talk, we will focus on the most recent results obtained by the ATLAS and CMS experiments at the LHC for BSM searches, excluding Higgs and supersymmetry searches. New results in Dark matter, heavy narrow bosons, new heavy quarks and 3rd generation lepto-quarks will be presented. A brief summary of the perspectives at 14 TeV and at HL-LHC will be shown.
Speaker: Fairouz Malek (LPSC-Grenoble , CNRS-IN2P3 (FR))
• 19:05
String theory suggests that cosmology is populated by many light pseudoscalar axions (an Axiverse" scenario). Their presence in early universe give rise to dark radiation, non-standard model contribution to radiation imprinted onto Cosmic Microwave Background (CMB). Due to complexity of string compactification, it is natural to expect number of axions to be several hundreds up to thousands. Although there have been hints of dark radiation from Planck satellite and WMAP experiment, we show in this talk that large number of axions in typical axiverse scenario produces dark radiation much larger than observable value. Motivated by this problem, we study moduli space of compactified manifolds allowing by this constraint. We show that G2 manifold can relax strong dependency between number of axions and dark radiation. In addition, under plausible condition on moduli mass matrix, a compactified manifold with sufficiently large number of axions gives a phenomenologically acceptable value of dark radiation. The application on G2 compactified M-theory is also presented in great detail.
Speaker: Chakrit Pongkitivanichkul (King's College London)
• 16:35 19:20
Parallel 4: Experiments-discrete-symmetries Anatomy Museum

#### Anatomy Museum

• 16:35
Prospects for K+ ->pi+ nu nu observation at CERN in NA62 30m
The rare decays K+ ->pi+ nu nu are excellent processes to make tests of new physics at the highest scale complementary to LHC thanks to their theoretically cleaness. The NA62 experiment at CERN SPS aims to collect of the order of 100 events in two years of data taking, keeping the background at the level of 10%. Part of the experimental apparatus has been commissioned during a technical run in 2012. The physics prospects and the status of the experiment will be reviewed in light of the first physics run in October-December 2014.
Speaker: Ferdinand Hahn (CERN)
• 17:05
Study of B -> K pi pi gamma decays 25m
In b -> s gamma transitions, the standard model predicts that B0 (antiB0) decays are related predominantly to the presence of right (left) handed photons in the final state. Therefore, the mixing-induced CP asymmetry in B -> fCP decays, where fCP is a CP eigenstate, is expected to be small. This prediction may be altered by new-physics (NP) processes in which opposite helicity photons are involved. Independently, decays to K pi pi gamma can display an interesting hadronic structure: they have contributions from several kaonic resonances decaying to Kpipi. The decays of these resonances themselves exhibits a resonant structure, with contributions from K*pi, Krho and a (Kpi) S-wave. In the present analysis, we extract information about the Kpipi resonant structure by means of an amplitude analysis of the Kpipi and Kpi invariant mass distributions in B+ -> K+pi-pi+ gamma decays. The results are used, assuming isospin symmetry, to extract the mixing-induced CP parameters of the process B0 -> K0S rho0 gamma from the time-independent analysis of B0 -> K0S pi+ pi- gamma.
Speaker: Alessandro Pilloni (Sapienza U.)
• 17:30
B-physics with ATLAS and CMS 30m
The large production rates of heavy flavoured particles at the LHC provide excellent opportunities to test the standard model and probe for new physics effects. A review of selected recent measurements by ATLAS and CMS based on LHC Run I data is presented, along with prospects for coming LHC runs.
Speaker: Nuno Viegas Guerreiro Leonardo (Purdue University (US))
• 18:00
Break (5 min) 5m
• 18:05
Study of CP violation effects in the charmless hadronic decay B -> Ks pi+ pi0 25m
We report a Dalitz plot analysis of the charmless hadronic decays of charged B mesons to the final state Ks pi+ pi0 using the full BaBar dataset of 471 million BBbar events collected at the Upsilon(4S) resonance. We observe an excess of signal events and measure the branching fractions and CP asymmetries, for the different resonant decay modes and inclusively.
Speaker: Dr Thomas Edward Latham (University of Warwick (GB))
• 18:30
Study of KS semileptonic decays and CPT tests with the KLOE detector 25m
Study of semileptonic decays of neutral kaons allows to perform a test of discrete symmetries, as well as basic principles of the Standard Model. In this presentation a general review on dependency between charge asymmetry constructed for semileptonic decays of short- and long-lived kaons and CPT symmetry is given. The current status of determination of charge asymmetry for short-lived kaon, obtained by registering of about 1.7 billion KSKL meson pairs collected at DAΦNE with the KLOE detector is also reviewed.
Speaker: Daria Kaminska
• 18:55
Precision tests of the Standard Model with kaon decays at CERN 25m
Recent results and prospects for precision tests of the Standard Model in kaon decay in flight experiments at CERN are presented. A measurement of the ratio of leptonic decay rates of the charged kaon at a 0.4% precision constrains the parameter space of new physics models with extended Higgs sector, a fourth generation of quarks and leptons or sterile neutrinos. Searches for heavy neutrino mass states and the dark photon in the ~100 MeV/c$^2$ mass range based on samples collected in 2003-2007 are in progress and prospects will be discussed. The NA62 experiment starting in 2014 will search for a range of lepton number and lepton flavour violating decays of the charged kaon and the neutral pion at improved sensitivities down to ~$10^{-12}$, which will probe new physics scenarios involving heavy Majorana neutrinos or R-parity violating SUSY.
Speaker: Karim Massri (University of Birmingham (GB))
• 16:35 18:55
Parallel 5: Strongly coupled gauge theories River Room

#### River Room

• 16:35
Symmetry-improved 2PI Approach to the Infrared Divergences of the Standard Model Effective Potential 35m
The 3-loop Standard Model (SM) effective potential suffers from infrared (IR) divergences due to the Goldstone bosons. These IR problems start at lower loop-orders for the derivatives of the potential. We study these issues by means of the recently developed *symmetry-improved CJT effective action*. Our formalism, as opposed to other existing approaches, is particularly appropriate for studying this problem, since the thresholds of the particles are correctly described within quantum loops. By considering the Higgs and top-quark sectors of the SM we show that, in agreement with other recent approaches, the IR divergences are actually absent, being an artifact of perturbation theory. Moreover, we give preliminary quantitative comparisons with the existing treatments, which are based on partial resummations of perturbation-theory contributions. These IR issues can potentially have an important quantitative impact on the stability analyses of the SM effective potential extrapolated at very high energies, since this is known to be particularly sensitive to the matching conditions at the electroweak scale.
Speaker: Daniele Teresi (University of Manchester)
• 17:10
Numerical results for gauge theories near the conformal window 35m
A novel strong interaction beyond the standard model could provide a dynamical explanation of electroweak symmetry breaking. Experimental results strongly constrain properties of models that realise this mechanism. Whether these constraints are obeyed by any strongly interacting quantum field theory is a non-perturbative problem that needs to be addressed by first-principle calculations. Monte Carlo simulations of lattice regularised gauge theories is a powerful tool that enables us to address this question. Recently various lattice investigations have appeared that have studied candidate models of strongly interacting dynamics beyond the standard model. After a brief review of the main methods and of some recent results, we focus on the analysis of SU(2) gauge theory with one adjoint Dirac fermion flavour, which is shown to have a near-conformal behaviour with an anomalous dimension of order one. The implications of our findings are also discussed.
Speaker: Biagio Lucini (Swansea University)
• 17:45
Break (5 min) 5m
• 17:50
Effects of divergent ghost loops on the Green's functions of QCD 35m
I discuss certain characteristic features encoded in some of the fundamental QCD Green's functions, whose origin can be traced back to the (Landau gauge) nonperturbative masslessness of the ghost field. Specifically, the ghost loops that contribute to these Green's functions display infrared divergences, akin to those encountered in the perturbative treatment, in contradistinction to the gluonic loops, whose perturbative divergences are tamed by the dynamical generation of an effective gluon mass. In d=4, the aforementioned divergences are logarithmic, thus causing a relatively mild impact, whereas in d=3 they are linear, giving rise to enhanced effects. In the case of the gluon propagator, these effects do not interfere with its finiteness, but make its first derivative diverge at the origin, and introduce a maximum in the region of infrared momenta. The three-gluon vertex is also affected, and the induced divergent behavior is clearly exposed in certain special kinematic configurations, usually considered in lattice simulations; the sign of the corresponding divergence is unambiguously determined. The picture that emerges is finally compared to the available lattice data.
Speaker: Daniele Binosi (ECT* Fondazione Bruno Kessler)
• 16:35 19:35
Parallel 9: Higgs Physics @ LHC, discrete symmetries @LHC, new facilities Great Hall

#### Great Hall

• 16:35
Lepton number violation in non-standard Higgs sectors 30m
We consider the phenomenology of extended Higgs sectors that allow the neutrino masses to be Majorana. This means that the extra scalars do violate lepton number. For that purpose, we classify them using an effective field theory approach. Then, using appropriate current ATLAS and CMS analyses we set the first bounds on lepton number violation in the scalar sector. We also describe how to measure the quantum numbers of the corresponding scalar fields if they were detected in a second phase of the LHC running.
Speaker: Dr Mikael Chala (DESY)
• 17:05
Implications of Higgs mediated Flavour Changing Neutral Currents with Minimal Flavour Violation. 30m
We poropose an extension of the hypothesis of Minimal Flavour Violation to two Higgs doublet Models without the assumption of Natural Flavour Conservation in the Higgs sector. The potentially dangerous flavour changing neutral currents are suppressed by small entries of the CKM matrix as a result of a discrete symmetry imposed to the Lagrangian. This discrete symmetry is also extended to the leptonic sector. We analyse the constraints and some of the phenomenological implication of this class of models.
Speaker: Margarida Nesbitt Rebelo (Instituto Superior Tecnico (IST))
• 17:35
Higgs-Dilaton Cosmology: Universality vs. Criticality 30m
The Higgs-Dilaton model is able to produce an early inflationary expansion followed by a dark energy dominated era responsible for the late time acceleration of the Universe. At tree-level, the model predicts a small tensor-to-scalar ratio, a tiny negative running of the spectral tilt and a non-trivial consistency relation between the spectral tilt of scalar perturbations and the dark energy equation of state. We will reconsider the validity of these predictions in the presence of radiative corrections and their connection to low energy Higgs and top masses.
Speaker: Dr Javier Rubio (EPFL)
• 18:05
Break (5 min) 5m
• 18:10
Electroweak vacuum stability, Higgs and top masses, and new physics 25m
According to the usual analysis, if the Standard Model (SM) is valid up to the Planck scale $M_P$, the stability condition of the electroweak (EW) vacuum (stable, metastable or unstable) mainly depends on the Higgs and top masses, $M_H$ and $M_t$. The analysis is performed by considering SM interactions only, as it is argued that new physics at $M_P$, although present, has no impact on it, and the results are presented with the help of a stability diagram in the ($M_H$, $M_t$) plane. For the current experimental values of $M_H$ and $M_t$, in particular, the EW vacuum turns out to be metastable, with a lifetime much longer than the age of the universe. I this talk I present some recent work showing that new physics can have a great impact on the stability phase diagram, a result that has quite interesting phenomenological consequences. Candidates for beyond SM physics can be "tested" against this stability analysis. Moreover, contrary to some recent claims, higher precision measurements of the top and Higgs masses cannot provide any definite indication on whether we live in a stable or metastable universe, the answer to this question strongly depends on new physics. Finally, these results cast serious doubts on the Higgs inflation scenario, the latter being highly based on a crucial fine tuning of the EW vacuum stability condition.
Speaker: Vincenzo Branchina (University of Catania)
• 18:35
Degeneracy on a multiHiggs CP non invariant sector. 30m
The Higgs sector with more than one Higgs doublet may have de\-ge\-ne\-ra\-cy in its physical states. Considering also $CP$ symmetry is not conserved in the Higgs sector, then the neutral Higgs states would not have a defined $CP$ charge,{\it i.e.} there is a mixing within scalar and pseudoscalar components of the Higgs doublets. This situation will occur for the cMSSM, {\it i.e.} with complex soft couplings, and will be manifest through one-loop corrections. This possibility has consequences on the phenomenology and in the type of expected signatures for the nearly and exact Higgs de\-ge\-ne\-ra\-cy, as for example the line-shape will present very different behaviour than expected for the fermion scattering amplitude via $non-CP$ defined Higgs, $\sigma(f \bar{f} \to H_{i}^{non CP} \to f'\bar{f'})$.
Speaker: Dr Melina Gomez Bock (Universidad de las Americas Puebla)
• 19:05
S3 and Q6 as flavour symmetries in multi-Higgs models 30m
We present an overview of the flavour groups S3 and Q6 in models with an extended Higgs sector. We extend the S3 results to SU(5) Grand Unified theories with Q6 as flavour group. We find the generic form of the mass matrices both in the quark and lepton sectors, which are consistent with experimental data. We reproduce, according to current data, the mixing in the CKM matrix. In the leptonic sector, the neutrino mixing angles are also found, in good agreement with experimental data.
• 20:00 21:00
CULTURAL EVENT (Kateřina Fűrstová (soprano) and Massimo Blasone (piano)) 1h Great Hall

#### Great Hall

Kateřina Fűrstová, soprano
M Blasone (piano)

• Friday, 5 December
• 08:55 09:00
Registration: Desk (Great Hall) 8:30 - 17:00 5m
• 09:00 13:15
PLENARY 4 Great Hall

#### Great Hall

• 09:00
Supergravity: status and prospects 45m
I give a review of Supergravity theories with emphasis on recent developments and prospects.
Speaker: Jean-Pierre Derendinger (Universitaet Bern (CH))
• 09:45
The Moebius symmetry of quantum mechanics 45m
Adaptation of the Hamilton-Jacobi formalism to quantum mechanics yields a cocycle condition which is invariant under D-dimensional Mobious transformations. The invariance under Mobious transformations can only be implemented consistently if space is compact and implies energy quantisation and undefinability of quantum trajectories. It implies the existence of a fundamental length scale that may be identified with the Planck length. Consistency of phase space duality is a complementary facet of the formalism and may serve as the fundamental physical principle underlying quantum mechanics. Evidence for the compactness of space may exist in the cosmic microwave background radiation.
Speaker: Alon Faraggi (U)
• 10:30
Coffee Break 30m Great Hall and River Room

#### Great Hall and River Room

• 11:00
Discrete Symmetries in String/M theory and Grand Unification 45m
After reviewing the origin of discrete symmetries like B and L and CP in string/M theory we go on to address the origin and fate of such symmetries in phenomenological Grand Unified models which derive from string/M theory. The impact on the nature of dark matter and other phenomenological consequences is discussed.
Speaker: Bobby Samir Acharya (Abdus Salam Int. Cent. Theor. Phys. (IT))
• 11:45
Lorentz symmetry breaking: phenomenology and constraints 45m
In this talk I shall review several motivations for considering departures from exact Lorentz invariance and the different theoretical frameworks adopted to describe these departures. Among these, I shall focus on an effective field theory approach and discuss the phenomenology and constraints of Lorentz symmetry breaking in the Standard Model as well as in Gravity. In particular I will focus on current constraints on UV breaking inspired by quantum gravity scenarios and briefly discuss the open issues and future perspectives for this field of research.
Speaker: Stefano Liberati (SISSA)
• 12:30
Summary and prospects of the LHCb Experiment 45m
The physics highlights of the LHCb experiment will be reviewed, based on results from up to 3 fb^-1 of pp-collision data. Measurements of the angles of the unitary triangle will be highlighted, together with limits on new physics from rare b-decays, plus the observation of new baryonic states. Physics prospects for the upcoming Run-2 and the LHCb upgrade will also be summarized.
Speaker: Prof. Neville Harnew (University of Oxford (GB))
• 13:15 14:30
Lunch Break 1h 15m Great Hall and River Room

#### Great Hall and River Room

• 14:30 16:00
Parallel 11: Astroparticle Physics Experiments River Room

#### River Room

• 14:30
Recent Results of the AMS-02 Experiment on the ISS 30m
AMS-02 is a general purpose cosmic ray detector operating on the International Space Station since 19 May 2011. Results based on the data collected during the first 2.5 years of the mission include high precision measurements of the proton, helium, electron and positron fluxes, and the boron to carbon ratio in the energy range from ~1GeV/n to ~1TeV/n. The positron fraction is determined in the energy range from 0.5 to 500GeV and its energy spectrum shows an steadily increasing fraction from 10 to 200GeV with no fine structure. Individual electron and positron fluxes require a description beyond a single power-law spectrum.
Speaker: Jorge Casaus (Centro de Investigaciones Energ. Medioambientales y Tecn. - (ES)
• 15:00
Results from the Pierre Auger Observatory 30m

We will present highlights from the Pierre Auger Observatory. We will also present the current status
and plans for upgrades of the Observatory. We will mention briefly
the programme of the Observatory to search for new, exotic physics.

Speaker: Dr Lukas Nellen (I. DE CIENCIAS NUCLEARES, UNAM)
• 15:30
The Cherenkov Telescope Array : status and science goals for fundamental physics 30m
The Cherenkov Telescope Array (CTA) is a worldwide project aiming at building the next ground-based gamma-ray observatory with a sensitivity ten times better than current experiments like H.E.S.S., MAGIC and VERITAS. CTA will be composed of several tens of telescopes with two-to-three different sizes distributed on two sites located in the Northern and Southern Hemispheres. CTA will also have a much wider energy lever arm and improved angular resolution. Important steps for the CTA project are currently underway: the decision about the site locations and the shaping of the key science projects. The science program will be presented with specific emphasis on the plans for indirect searches for dark matter.
Speaker: Emmanuel Moulin (CEA)
• 14:30 16:05
Parallel 4: Experiments-discrete-symmetries Great Hall

#### Great Hall

• 14:30
Recent results, status and prospects for the BESIII experiment 35m
We report the measurement of the asymmetry $A_{CP}$ of the branching fractions of $D^0\rightarrow K^-\pi^+$ in the CP-odd and CP-even eigenstates using a data sample of $2.92$ fb$^{-1}$ collected with the BESIII detector at the center-of-mass energy $\sqrt{s}=3.773$ GeV. With the measured $A_{CP}$ the strong phase difference $\delta_{K\pi}$ between the doubly Cabibbo-suppressed process $\bar{D}^0\rightarrow K^-\pi^+$ and the Cabibbo-favored process $D^0\rightarrow K^-\pi^+$ is extracted. Using world-average values of external parameters, we obtain the most precise measurement of $\delta_{K\pi}$ to date: $\cos\delta_{K\pi}=1.02\pm0.11\pm0.06\pm0.01$. The first and second uncertainties are statistical and systematic, respectively, while the third arises from external input. Based on the same data sample a preliminary results of the parameter $y_{CP}$ in $D^0-\bar{D}^0$ oscillation is obtained. Finally, a summary of the recent results from charmonium spectroscopy is reported. The high statistics accumulated at the $Y(4260)$ and $Y(4360)$ energies help us to understand the nature and the proprieties of the XYZ states.
Speaker: Isabella Garzia (INFN)
• 15:05
Searches for dark forces with KLOE 30m
Recent astrophysical observations are consistent with the existence of a secluded dark gauge sector weakly interacting with the Standard Model. The mass of the mediator, the so called dark photon, or U boson, is predicted to be at the GeV scale. Possible extensions of the minimal model lead to the introduction of a dark Higgs boson which, analogously to its Standard Model counterpart, breaks the gauge symmetry. These new particles can be observed as sharp resonances in the invariant mass distribution of charged lepton or pion pairs in reactions of the type e+e- --> l(pi)+l(pi)- gamma, in pseudoscalar meson decays or in associate production with a dark Higgs scalar. KLOE searched for U boson production in phi meson dalitz decays and in e+e- --> mu+mu- gamma reaction,while preliminary results are available for electron positron final state and for the higgstrahlung channel. No evidence of the process was found and tight upper limits were set to the relevant parameters.
Speaker: Dr enrico graziani (INFN)
• 15:35
Measurements of CP violation at Belle 30m
We present some of the recent measurements of $CP$ violation in $B$ decays based on the full data sample containing 772 million $B$ meson pairs collected at the $\Upsilon(4S)$ resonance using the Belle detector at the KEKB asymmetric-energy $e^+e^-$ collider. In particular, we present measurements of time-dependent $CP$ violation parameters in $B^0 \to \eta'K^0$, $B^0 \to \omega K^0_S$ and $B^0\to K^0_S \eta \gamma$ decays. In the Standard Model these decays only proceed through the $b\to s$ quark transition penguin diagrams and are as such very sensitive to new CP violating phases carried by potential new heavy particles in the loops. In addition we also present measurement of direct $CP$ violation in $B^0 \to \eta' K^{\ast 0}$, and measurement of branching fraction of $B^0\to \pi^0\pi^0$ decay. The latter result plays an important role in determinations of $\phi_2$ angle of the unitarity triangle.
Speaker: Luka Santelj (KEK, Japan)
• 14:30 16:00
Parallel 7: Supersymmetry, Supergravity, Strings, Branes S7.06 7th floor Strand Bldg.

#### S7.06 7th floor Strand Bldg.

• 14:30
SUSY Searches: Recent Results from ATLAS & CMS 30m
Despite the absence of experimental evidence, weak scale supersymmetry remains one of the best motivated and studied Standard Model extensions. This talk summarises recent ATLAS and CMS results for searches for supersymmetric (SUSY) particles. Weak and strong production in both R-Parity conserving and R-Parity violating SUSY scenarios are considered. The searches involved final states including jets, missing transverse momentum, light leptons, taus or photons, as well as long-lived particle signatures.
Speaker: Michael Christian Rammensee (CERN)
• 15:00
Neutrino masses from SUSY breaking in radiative seesaw models 30m
$\require{cancel}$ $\def\SUSY{\text{SUSY}}$ $\def\nSUSY{\cancel{\text{SUSY}}}$ $\def\Msoft{m_\text{soft}}$ $\def\nSUSYEWSB{\nSUSY_{\text{EWSB}}}$ $\def\nSUSYEWS{{\nSUSY}_{\text{EWS}}}$ Radiatively generated neutrino masses ($m_\nu$) are proportional to supersymmetry (SUSY) breaking, as a result of the SUSY non-renormalisation theorem. In this work, we investigate the space of SUSY radiative seesaw models with regard to their dependence on SUSY breaking ($\require{cancel}\cancel{\text{SUSY}}$). In addition to contributions from sources of $\nSUSY$ that are involved in electroweak symmetry breaking ($\nSUSYEWSB$ contributions), and which are manifest from $\langle F^\dagger_H \rangle = \mu \langle \bar H \rangle \neq 0$ and $\langle D \rangle = g \sum_H \langle H^\dagger \otimes_H H \rangle \neq 0$, radiatively generated $m_\nu$ can also receive contributions from $\nSUSY$ sources that are unrelated to EWSB ($\nSUSYEWS$ contributions). We point out that recent literature overlooks pure-$\nSUSYEWSB$ contributions ($\propto \mu / M$) that can arise at the same order of perturbation theory as the leading order contribution from $\nSUSYEWS$. We show that there exist realistic radiative seesaw models in which the leading order contribution to $m_\nu$ is proportional to $\nSUSYEWS$. To our knowledge no model with such a feature exists in the literature. We give a complete description of the simplest model-topologies and their leading dependence on $\nSUSY$. We show that in one-loop realisations $L L H H$ operators are suppressed by at least $\mu \, \Msoft / M^3$ or $\Msoft^2 / M^3$. We construct a model example based on a one-loop type-II seesaw. An interesting aspect of these models lies in the fact that the scale of soft-$\nSUSY$ effects generating the leading order $m_\nu$ can be quite small without conflicting with lower limits on the mass of new particles.
Speaker: Antonio Figueiredo (CFTP / IST - U. Lisbon)
• 15:30
Exploring neutrino physics at LHC via R-parity violating SUSY 30m
$R$-parity violating supersymmetric models (RPV SUSY) are becoming increasingly more appealing than its $R$-parity conserving counterpart in view of the hitherto non-observation of SUSY signals at the LHC. In this talk, RPV scenarios where neutrino masses are naturally generated will be discussed, namely RPV through bilinear terms (bRPV) and the "$\mu$-from-$\nu$" supersymmetric standard model ($\mu\nu$SSM). The latter is characterised by a rich Higgs sector that easily accommodates a 125-GeV Higgs boson. The phenomenology of such models at the LHC is reviewed, giving emphasis on final states with displaced objects, and relevant results obtained by LHC experiments are presented. The implications for dark matter for these theoretical proposals is also addressed.
Speaker: Dr Vasiliki Mitsou (IFIC Valencia (ES))
• 16:05 16:30
Coffee Break 25m River room and parallel session rooms

#### River room and parallel session rooms

• 16:30 18:35
Parallel 12: Neutrino Experiments Great Hall

#### Great Hall

• 16:30
SUMMARY OF THE LATEST RESULTS AND FUTURE PROSPECTS FROM THE T2K EXPERIMENT 30m
The T2K long-baseline experiment is located in Japan and is designed to study oscillations of muon neutrinos. T2K receives a beam of muon neutrinos peaked at 0.6 GeV that are produced at J-PARC accelerator complex by converting a beam of 30-GeV protons hitting a graphite target. Upon travelling 295 km, neutrinos are detected by the Super-Kamiokande water Cherenkov detector. Located at 280 m from the target, the near detector complex (ND280) provides information about un-oscillated neutrino flux, direction and interaction cross-sections. The T2K experiment observed electron neutrino appearance at Super-K with the significance of 7.3σ and measured the associated oscillation parameter θ13 for both normal and inverted mass hierarchies. In addition, by looking at muon neutrino disappearance T2K provided improved measurements of the θ23 and Δm232 parameters. The results of these measurements are presented as well as a brief summary of the neutrino cross section measurements. Future prospects of the T2K experiment are discussed.
Speaker: Dr Yevgeniy Petrov (University of British Columbia, for the T2K collaboration)
• 17:00
Recent results from the OPERA experiment at the CNGS beam 30m
The OPERA experiment at the Gran Sasso underground laboratory is searching for nu_mu -> nu_tau oscillations in appearance mode in the CNGS neutrino beam. Four nu_tau candidate events have been found so far, using a sub-sample of data from the 2008-2012 runs. Given the number of analysed events and the low background, nu_mu -> nu_tau oscillations are established with a significance of 4.2 sigma. In the talk the data analysis will be discussed, with emphasis on the background constraints obtained by using dedicated data-driven control samples. We will also present an analysis of the present tau neutrino and electron neutrino sample in the framework of the 3+1 sterile model. The analysis of the muon charge ratio in the cosmic ray sample will be also covered.
Speaker: Dr Andrea (on behalf of the OPERA Coll.) Longhin (INFN Laboratori Nazionali di Frascati)
• 17:30
The GERDA Experiment for the Search of Neutrinoless Double Beta Decay 30m
{\sc Gerda} is designed to search for the neutrinoless double beta (0$\nu\beta\beta$) decay, a lepton number violating process. It employs bare high-purity germanium diodes enriched to 86\,\% in $^{76}$Ge directly immersed in liquid argon. Phase~I operated till May 2013 with a mean background of 1$\cdot10^{-2}$\,cts/(keV$\cdot$kg$\cdot$yr) near the Q-value. GERDA sets a new lower limit of T$_{1/2}$\textgreater 2.1$\cdot10^{25}$\,yr (90\% C.L.) strongly disfavouring the long-standing claim of signal observation. For Phase~II, exploring half-lives up to 1.5$\cdot10^{26}$\,yr, additional 20\,kg of broad-energy Ge detectors will be installed in late 2014. An order of magnitude lower background will be achieved with an active liquid Ar veto and pulse shape analysis. The liquid Ar veto is a hybrid system of wavelength shifting fibres read out by silicon photomultipliers on the one hand and wavelength shifting reflector foils with (vacuum) PMTs on the other hand.
Speaker: Manuel Walter (University of Zurich)
• 16:30 19:20
Parallel 7: Supersymmetry, Supergravity, Strings, Branes S7.06 7th floor Strand Bldg.

#### S7.06 7th floor Strand Bldg.

• 16:30
Non-supersymmetric heterotic model building 30m
We investigate orbifold and smooth Calabi-Yau compactifications of the non- supersymmetric heterotic SO(16)×SO(16) string. We focus on such Calabi-Yau backgrounds in order to recycle commonly employed techniques, like index theorems and cohomology theory, to determine both the fermionic and bosonic 4D spectra. We argue that the N=0 theory never leads to tachyons on smooth Calabi-Yaus in the large volume approximation. As twisted tachyons may arise on certain singular orbifolds, we conjecture that such tachyonic states are lifted in the full blow-up. We perform model searches on selected orbifold geometries. In particular, we construct an explicit example of a Standard Model-like theory with three generations and a single Higgs field.
• 17:00
Light U(1)s in Heterotic String Models 25m
Although additional low scale U(1)s have been discussed extensively in SUSY GUTs and superstring models, having a viable light, extra U(1) in worldsheet heterotic string constructions has proven to be a challenge. Here, we present the construction of heterotic string models using the free fermionic formulation and focus on how viable U(1)s may arise. We motivate an example as an appealing proposition to explain the suppression of proton decay mediating operators, induced in supersymmetric models. The additional symmetry forbids the undesired operators, and therefore must be light to accommodate proton lifetime constraints. We discuss and contrast two classes of superstring models with a desirable additional U(1): those with charges embedded in E6 and those without embedding. We show that the gauge coupling data at the electroweak scale necessitate that the Z' charges are embeddable in E6 but that anomaly free U(1) combinations require no such embedding. We present a recipe of how enhancement may circumvent this conundrum and construct a standardlike model with desirable properties.
Speaker: Viraf Mehta (Ruprecht-Karls Universität Heidelberg)
• 17:25
Universality of radiative corrections to gauge couplings for strings with spontaneously broken supersymmetry 30m
I will present recent work on computing radiative corrections to non-abelian gauge couplings in four-dimensional heterotic vacua with spontaneously broken supersymmetry. They may be considered as K3 surfaces with additional Scherk-Schwarz fluxes responsible for the spontaneous N=4 ---> N=0 breaking. Remarkably, although the gauge thresholds are no longer BPS protected and receive contributions also from the excitations of the RNS sector, we find that their difference is still BPS saturated and exhibits a universal behaviour. Contrary to the case of unbroken supersymmetry, the non-abelian gauge thresholds develop infrared logarithmic singularities due to charged BPS-like states originating from the twisted RNS sector becoming massless at special points of the classical moduli space.
Speaker: Ioannis Florakis (CERN)
• 17:55
Break (5 min) 5m
• 18:00
Discrete Abelian Gauge Symmetries and Axions 30m
As recently observed, discrete Abelian symmetries can remain as remnants in the low-energy effective action of string compactifications with massive U(1) symmetries. As I will discuss in this talk, the Peccei-Quinn symmetry arises naturally in this way in D-brane models with the QCD axion as an open string excitation and several other (invisible) axions from both the open and closed string sectors.
Speaker: Gabriele Honecker (Johannes Gutenberg University Mainz)
• 18:30
Phenomenology of discrete symmetries 25m
Discrete symmetries play a crucial role in physics beyond the Standard Model. Focusing on supersymmetric models which aim at explaining the family structure of quarks and leptons, I first discuss how Abelian discrete symmetries such as e.g. R-parity can emerge from an underlying U(1) family symmetry. Non-Abelian discrete family symmetries are motivated by the observation of large and very peculiar mixing angles in the neutrino sector. I review their implementation in supersymmetric models and briefly comment on the implications arising from the measurement of a non-zero reactor neutrino mixing angle.
Speaker: Christoph Luhn (University of Siegen)
• 18:55
Exotica and discreteness in the classification of string spectra 25m
I discuss the existence of discrete symmetries in the landscape of free fermionic heterotic–string vacua that were discovered via their classification by SO(10) GUT models and its subgroups such as the Pati-Salam, Flipped SU(5) and Standard-Like models. The classification is carried out by fixing a set of basis vectors and varying the GGSO projection coefficients entering the one–loop partition function. The analysis of the models is facilitated by deriving algebraic expressions for the GSO projections that enable a computerised analysis of the entire string spectrum and the scanning of large spaces of vacua. The analysis reveals discrete symmetries like the spinor-vector duality observed at the SO(10) level and the existence of exophobic Pati-Salam vacua. Contrary to the Pati–Salam case the classification shows that there are no exophobic flipped SU(5) vacua with an odd number of generations. It is observed that the standard-like models are substantially more constrained.
Speaker: Hasan Sonmez (University Of Liverpool)
• 16:30 19:10
Parallel 8: Early universe Physics (Inflation, Lepto(Baryo)genesis) River Room

#### River Room

• 16:30
WIMPy baryogenesis with sterile neutrinos 30m
We propose a mechanism for baryogenesis from particle decays or annihilations that can work at the TeV scale. Some heavy particles annihilate or decay into a heavy sterile neutrino $N$ (with $M \gtrsim 0.5$~TeV) and a light'' one $\nu$ (with $m \ll 100$~GeV), generating an asymmetry among the two helicity degrees of freedom of $\nu$. This asymmetry is partially transferred to Standard Model leptons via fast Yukawa interactions and reprocessed into a baryon asymmetry by the electroweak sphalerons. We illustrate this mechanism in a WIMPy baryogenesis model where the helicity asymmetry is generated in the annihilation of dark matter. This model connects the baryon asymmetry, dark matter, and neutrino masses.
Speaker: Mrs Nuria Rius (IFIC, Valencia University-CSIC)
• 17:00
Flavour Effects in Resonant Leptogenesis from Semi-classical and Kadanoff-Baym Approaches 25m
Flavour effects play an important role in the statistical evolution of particle number densities in several particle physics phenomena. We present a fully flavour-covariant formalism for transport phenomena, in order to consistently capure all flavour effects in the system. We explicitly study a Resonant Leptogenesis (RL) scenario, and show that flavour covariance requires one to consider generically off-diagonal number densities, rank-4 rate tensors in flavour space, and non-trivial generalization of the discrete symmetries $C$, $P$ and $T$. The flavour-covariant transport equations, obtained in our semi-classical framework, describe the effect of three relevant physical phenomena: coherent heavy-neutrino oscillations, quantum decoherence in the charged-lepton sector, and the standard resonant $CP$ violation due to heavy-neutrino mixing. We show quantitatively that the final asymmetry is enhanced by up to an order of magnitude, for electroweak-scale heavy neutrinos, as compared to that obtained from flavour-diagonal or partially flavour off-diagonal equations. A full field-theoretical treatment in the weakly-resonant regime, based on the so-called Kadanoff-Baym (KB) equations, confirms that heavy-neutrino oscillations and mixing are two *distinct* phenomena, and reproduces the results obtained in our semi-classical framework. Finally, we show that the quasi-particle ansaetze, often employed in KB approaches to RL, discard the phenomenon of mixing, capturing only oscillations and leading to an underestimate of the final asymmetry by a factor of order 2.
Speaker: Daniele Teresi (University of Manchester)
• 17:25
Tree level Baryogenesis through Leptogenesis from Kalb-Ramond Torsion Background 30m
We consider a model of an expanding Universe in string theory that yields CPT violation for fermions, in the sense of different dispersion relations for fermions and antifermions. These are induced by a cosmological background with constant torsion provided by the Kalb–Ramond antisymmetric tensor field (axion) of the string gravitational multiplet. This effect induces different densities of neutrinos and antineutrinos while in chemical equilibrium, offering new scenarios for leptogenesis and baryogenesis even in the absence of CP violation. Leptogenesis effects are visible at tree level and are discussed.
Speaker: sarben sarkar (King's College London)
• 17:55
Break (5 min) 5m
• 18:00
Inflation in supergravity from massive vector multiplets 30m
In a supergravity framework we present single field inflationary models built from massive vector multiplets. This property is due to an underlying stueckelberg mechanism where the second scalar partner of the inflaton is eaten by the massive vector. This mechanism can be used to built Starobinsky as well as chaotic models of inflation.
Speaker: Fotis Farakos
• 18:30
Gravitino condensation, supersymmetry breaking and inflation 30m
Supersymmetry is a well motivated theoretical paradigm, which, if it exists, must be broken at low energies. As such, understanding the origin of this breaking is key in order to make contact with known phenomenology. To this end we detail a non-pertubative breaking mechanism for local supersymmetry in gravitino condensation, an approach which we demonstrate also provides a UV motivated, phenomenologically viable inflationary mechanism at no added cost. We present results establishing contact between this scenario and known phenomenology, and discuss future avenues for research.
Speaker: Nick Houston (KCL)
• 16:59 19:05
Parallel 13: Antimatter Experiments K6.29 (Anatomy Lecture Theater)

#### K6.29 (Anatomy Lecture Theater)

• 16:59
Testing the Weak Equivalence Principle with antimatter at CERN 30m
The AEgIS collaboration is planning to measure the gravitational acceleration of antihydrogen, the simplest atom consisting entirely of antimatter, with a precision of 1% as a first achievement. The experiment, based at the Antiproton Decelerator of CERN, provides important information for the development of a quantum theory of gravity. The experimental setup consists of a nested penning trap and a Stark accelerator, which are used to form and accelerate a pulsed beam of antihydrogen atoms towards a gravity free-fall detector. In this region the beam passes through a moiré deflectometer, which allows the measurement of its vertical displacement, due to the gravitational force, by means of a hybrid position and time sensitive detector (less than 10 um spatial resolution, and 50 ns time resolution), registering the impact point of the anti-atoms and their time of flight. Recently, a proof of principle study of the AEgIS detection system has been successfully conducted using a miniature copy of the moiré deflectometer coupled to an emulsion film detector. The displacement of the moiré pattern of an antiproton beam due to an electromagnetic field was measured, confirming the detection principle for the gravity measurement in the AEgIS experiment. The talk will discuss the theoretical background, present the latest developments of the experimental setup and outline the AEgIS plans to achieve the above-mentioned precision.
Speaker: Dr Mitsuhiro Kimura (Universitaet Bern (CH))
• 17:29
Towards precision measurements with trapped Antihydrogen 30m
Precise low-energy measurements of antimatter and subsequent comparison with equivalent matter measurements offer an experimental approach to address the question of why the Universe appears to be largely composed of matter. The observed abundance of matter relative to antimatter is not adequately explained by our present theories which would suggest that largely equal quantities should have been present from the beginning. Antihydrogen, as the antimatter equivalent of hydrogen, allows a unique opportunity to make precise comparison with matter spectra to test CPT and Lorentz invariance as well as to make direct tests of antimatter gravitation. Measured quantities in the anti-atomic system are expected to be exactly the same as the supremely well-measured and –calculated values for the atomic system, therefore any slight deviation would shed light on the problem of baryon asymmetry. The ALPHA collaboration at CERN was the first group to demonstrate trapping of antihydrogen and make preliminary measurements on this exotic bound state. We have demonstrated the first resonant quantum interaction with a pure antimatter system by driving and detecting magnetic resonance transitions between hyperfine states in trapped antihydrogen atoms [1], the first application of a method for measuring the gravitational mass of trapped antihydrogen [2], and made initial precision measurements of the antihydrogen charge anomaly [3]. These measurements are significant milestones towards sensitive tests of CPT and antimatter gravitation. ALPHA is commissioning a major upgrade to improve these measurements and begin investigating optical transitions in antihydrogen. [1] C. Amole, et al. (ALPHA), Nature 483, 439 (2012) [2] C. Amole, et al. (ALPHA). Nature Communications, 4, 1785 (2013) [3] C. Amole, et al. (ALPHA). Nature Communications, 5, 3955 (2014)
Speaker: William Alan Bertsche (University of Manchester (GB))
• 17:59
Break (5 min) 5m
• 18:04
Progress towards in-beam hyperfine spectroscopy of antihydrogen 30m
Antihydrogen is the simplest atom consisting purely of antimatter. Its matter counterpart, hydrogen, is one of the best studied atomic systems in physics. Thus comparing the spectra of hydrogen and antihydrogen offers some of the most sensitive tests of matter-antimatter symmetry. The ASACUSA collaboration is pursuing an experiment to measure the ground-state hyperfine splitting of antihydrogen in a polarized beam [1,2], a quantity which was measured in hydrogen in a beam to a relative precision of $4\times10^{-8}$ [3] and in a maser to better than $10^{-12}$ [5,6] . After recently reporting the first observation of a beam of antihydrogen atoms 2.7 m downstream of the formation region in a field-free environment [4], the atomic resonance beam apparatus to perform a hyperfine measurement was completed. During the shutdown of CERN, a source of cold polarized hydrogen atoms was built and experiments were performed to characterize the apparatus with a hydrogen beam of similar properties as compared to the expected antihydrogen beam. Scans of the hyperfine structure of hydrogen showing encouraging results for the achievable precision for a measurement with antihydrogen will be reported. [1] E. Widmann et al., in The Hydrogen Atom: Precision Physics of Simple Atomic Systems} (ed. S. Kahrshenboim) pp. 528--542 (Lecture Notes in Physics vol. 570), Springer (2001). [2] E. Widmann et al. Hyperfine Interact. 215, 1–8 (2013). [3] A. G Prodell & P. Kusch, Physical Review, 88 184 (1952). [4] N. Kuroda et al., Nature Communications 5, 3089 (2014). [5] H. Hellwig et al., IEEE Trans. Instr. Meas. IM 19 ( 200 1970), [6] L. Essen, R.W. Donaldson et al., Nature 229 110 (1971).
Speaker: Eberhard Widmann (Austrian Academy of Sciences (AT))
• 18:34
Laser spectroscopy of metastable antiprotonic and pionic helium atoms 30m
The ASACUSA collaboration at CERN carries out two-photon laser spectroscopy of metastable antiprotonic helium atoms, which are three-body systems composed of a helium nucleus, an antiproton, and an electron. By measuring the transition frequencies of this atom and comparing the results with three-body QED calculations, the antiproton-to-electron mass ratio was determined to a precision of 1.4 parts per billion. We also describe the PiHe collaboration, which aims to measure the transition frequencies of pionic helium atoms using the 590-MeV ring cyclotron of the Paul Scherrer Institute.
Speaker: Masaki Hori (Max-Planck Institute of Quantum Optics (DE))
• 20:00 23:00
CONFERENCE DINNER (ROYAL SOCIETY, Trafalgar Sq.) 3h Royal Society, Carlton House Terrace ()

### Royal Society, Carlton House Terrace

• Saturday, 6 December
• 09:50 14:05
PLENARY 5 Great Hall

#### Great Hall

• 09:50
Particle Physics and Cosmology from Almost-Commutative Manifolds 45m
I will review almost-commutative manifolds, a light version of noncommutative geometry, proposed by Connes in order to explain the Standard Model of electroweak and strong interactions and eventually unify the Standard Model with Einstein's geometrical theory of gravity. I will briefly discuss the spectral action principle and the choice of the algebra. After a short presentation of the phenomenological successes of the model, I will address cosmological issues by considering the gravitational sector of the theory.
Speaker: Prof. Mairi Sakellariadou (King's College London)
• 10:35
Galileons and their Generalizations 45m
A new class of effective scalar field theories, with properties potentially interesting for cosmology, have emerged from attempts to modify gravity. I will discuss these "Galileon" field theories, emphasizing how they may be derived from the probe brane construction, and using this to generalize them to their associated curved-background and multi-field incarnations. I will comment on issues of stability, non-renormalization, coupling to gravity, and cosmological applications, and conclude by sketching how such terms can be constructed as Wess-Zumino terms of a particular type.
Speaker: Mark Trodden (University of Pennsylvania)
• 11:20
Coffee Break 30m Great Hall

#### Great Hall

• 11:50
Neutrinos and Leptogenesis in the Early Universe 45m
Neutrino mass models can explain the origin of the baryon asymmetry in the Universe, via the leptogenesis mechanism. A review of its main features and of the possible connection between low energy leptonic CP-violation and the one responsible for the baryon asymmetry will be presented.
Speaker: Silvia Pascoli (University of Durham (GB))
• 12:35
The MoEDAL Experiment at the LHC - a New Light on the Terascale Frontier 45m
In 2010 the MoEDAL experiment at the Large Hadron Collider (LHC) was unanimously approved by CERN's Research Board to start data taking in 2015. MoEDAL is a pioneering experiment designed to search for highly ionizing avatars of new physics such as magnetic monopoles or massive (pseudo-)stable charged particles. Its groundbreaking physics program defines over 30 scenarios that yield potentially revolutionary insights into such foundational questions as: are there extra dimensions or new symmetries; what is the mechanism for the generation of mass; does magnetic charge exist; what is the nature of dark matter; and, how did the big-bang develop. MoEDAL's purpose is to meet such far-reaching challenges at the frontier of the field. The innovative MoEDAL detector employs unconventional methodologies tuned to the prospect of discovery physics. The largely passive MoEDAL detector, deployed at Point 8 on the LHC ring, has a dual nature. First, it acts like a giant camera, comprised of nuclear track detectors - analyzed offline by ultra fast scanning microscopes - sensitive only to new physics. Second, it is uniquely able to trap the particle messengers of physics beyond the Standard Model for further study. MoEDAL's radiation environment is monitored by a state-of-the-art real-time TimePix pixel detector array.
Speaker: James Pinfold (University of Alberta (CA))
• 13:20
DISCRETE SYMMETRIES CP, T, CPT 45m
We are cellebrating the 50 anniversary of the discovery of CP- Violation. The direct evidence of separate genuine Time-Reversal- Violating Asymmetries, independent of CP-Violation and CPT-Invariance, came recently in the transitions filtered by time-ordered decays of Entangled Neutral B-mesons. These Symmetry Breakings are understood in the quantum field theory of ElectroWeak Interactions in terms of the particle content. Quantum Mechanics does not preclude the possible Violation of the CPT-Theorem, but it needs a more subtle mechanism.
Speaker: Jose Bernabeu (IFIC)
• 14:05 14:25
Closing of the Symposium-Announcement of next Discrete 2016 20m Great Hall

#### Great Hall

• 14:25 15:40
Lunch 1h 15m Great Hall

#### Great Hall

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