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Georgi Dvali (NYU and LMU)10/04/2016, 20:00
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Martin Flechl (Austrian Academy of Sciences (AT))11/04/2016, 08:20Invited Talk
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Veronica Sanz Gonzalez (University of Sussex)11/04/2016, 09:00Invited Talk
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Francesco Sannino (CP3-Origins)11/04/2016, 10:10Invited Talk
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Brian Thomas Batell11/04/2016, 10:50Invited Talk
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Nicola Venturi (University of Toronto (CA))11/04/2016, 17:00This talk will summarize the most important properties of the h(125) boson measured at the LHC run-1 by the ATLAS collaboration. It will also present early measurements made with the first data taken at 13 TeV in 2015.Go to contribution page
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Alexei Safonov (Texas A & M University (US))11/04/2016, 17:20This talk will review the status of what we know about the observed Higgs boson decaying to bosons, together with the search for Physics beyond the standard model in cases with bosons in the final state.Go to contribution page
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Daniel Salerno (Universitaet Zuerich (CH))11/04/2016, 17:40This talk will review the status of what we know about the observed Higgs boson decaying to fermions, together with the search for Physics beyond the standard model in cases with fermions in the final state. The presentation will cover the couplings from the analyses of final states and initial states like production in association with top quark pairs or single top quarks.Go to contribution page
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Dr Kiel Howe (Fermi National Accelerator Laboratory)11/04/2016, 18:20TalkInduced electroweak symmetry breaking is an alternative to the Standard Model mechanism for triggering the Higgs vev which can preserve a Standard-Model-like Higgs decoupled from additional states. In composite Higgs models, this provides a natural mechanism to explain a hierarchy $v \ll f$ between the EWSB scale and the global symmetry breaking scale. In particular, we describe how composite...Go to contribution page
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Dr Emiliano Molinaro (CP3-Origins, University of Southern Denmark)11/04/2016, 18:40ATLAS and CMS observe deviations from the expected background in the diphoton invariant mass searches of new resonances around 750 GeV. We show that a simple realization in terms of a new pseudoscalar state can accommodate the observations. The model leads to further footprints that can be soon observed. The new state can be interpreted both as an axion or as a highly natural composite state...Go to contribution page
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Suchita Kulkarni (Austrian Academy of Sciences (AT))11/04/2016, 19:00Towards the end of Run-1 data taking, an excess in the diboson as well as eejj channel was announced. During the first round of Run-2 data taking, an excess in diphoton channel has been announced. I consider possible explanations of these excesses in two different BSM scenarios. I demonstrate the feasibility of accommodating the diboson and eejj excess in a Left-Right Symmetric Standard Model....Go to contribution page
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Sezen Sekmen (Kyungpook National University (KR))12/04/2016, 08:20Invited Talk
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Maurizio Pierini (CERN)12/04/2016, 09:00Invited Talk
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Tetiana Hryn'ova (Centre National de la Recherche Scientifique (FR))12/04/2016, 10:10Invited Talk
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Christian Schwanenberger (Deutsches Elektronen-Synchrotron (DE))12/04/2016, 10:50Invited Talk
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Zinonas Zinonos (Georg-August-Universitaet Goettingen (DE))12/04/2016, 17:00This talk will briefly summarize the searches for BSM Higgs Bosons performed at the LHC run-1 by the ATLAS collaboration. Then it will present the searches for high mass Higgses in several channels, made at 13 TeV with the 2015 data.Go to contribution page
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Nikoloz Skhirtladze (Kansas State University (US))12/04/2016, 17:20The Large Hadron Collider has restarted pp collisions at 13 TeV center of mass energy in June 2015. The CMS experiments have taken data at this new energy which allows greater reach in probing for physics beyond the Standard Model. Several results on searches for physics not associated with supersymmetric extensions of the Standard Model are presented. To give few examples, these extensions...Go to contribution page
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Charles Vincent Welke (Univ. of California San Diego (US))12/04/2016, 17:40The CMS SUSY program is very active in performing searches with the 13 TeV data including multiple analyses done in regions with leptonic final states. The results of these analyses are used to expand the reach of the searches done by CMS at 8 TeV and additionally to investigate two excesses seen in run I, namely a 2.6 sigma excess seen by CMS and a 3.0 sigma excess seen by ATLAS. These...Go to contribution page
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Jeff Dandoy (University of Chicago (US))12/04/2016, 18:20Many extensions of the Standard Model of particle physics predict heavy new particles and new phenomena, leading to characteristic signatures such as a narrow peak or excess in the tail of distributions. This talk highlights results on searches with fermionic signatures, mainly with high-pT jets and leptons, using 2015 data collected at 13 TeV.Go to contribution page
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Kalliopi Iordanidou (Columbia University (US))12/04/2016, 18:40Searches for new physics beyond the Standard Model with bosonic signatures in LHC Run 2 are presented. These include searches for resonant production of two massive bosons (VV, VH and HH) and (non)resonant production of photons in high-mass region.Go to contribution page
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Michael Brodski (Rheinisch-Westfaelische Tech. Hoch. (DE))12/04/2016, 19:00Young Scientists ForumDespite the great understanding of particle interactions in terms of the Standard Model and the recent discovery of the Higgs boson at the LHC, the Standard Model of particle physics can not yet explain various phenomena, such as neutrino masses or the Dark Matter halo in the galaxies. This talk presents new LHC Run II results of a search for New Physics in Z+MET channel, discussing the main...Go to contribution page
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Brian Thomas Amadio (Lawrence Berkeley National Lab. (US))12/04/2016, 19:10Significant increase of the center-of-mass energy from 8 to 13 TeV at LHC Run II offers a great discovery potential for new physics at high mass, especially for strongly produced high-mass resources, contact interactions and TeV-gravity phenomena with high-pT jets. This talk presents most recent Run II results from ATLAS on new physics searches in the jet final states.Go to contribution page
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Muhammad Bilal Kiani (Universita e INFN Torino (IT))12/04/2016, 19:20Young Scientists ForumThis talk will present the H->4l analysis with 13 TeV data, and the corresponding results.Go to contribution page
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Peter Stangl (Excellence Cluster Universe, Munich)12/04/2016, 19:30Direct searches for fermion and vector boson resonances, as well as indirect constraints from precision measurements are both important tools to test the predictions of composite Higgs models. A novel numerical technique allows us to take into account many direct and indirect constraints in a single framework. This talk present results from applying our method to a class of four-dimensional...Go to contribution page
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Marc Schumann (University of Bern)13/04/2016, 08:20Invited Talk
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Tomer Volansky (Tel Aviv University (IL))13/04/2016, 09:00
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Maxim Pospelov13/04/2016, 10:10Invited Talk
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David Salek (Nikhef National institute for subatomic physics (NL))13/04/2016, 10:50
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Olaf Reimer13/04/2016, 11:30
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Joachim Kopp (Johannes-Gutenberg-Universitaet Mainz (DE))13/04/2016, 17:00
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Dr Felix Kahlhoefer (DESY)13/04/2016, 17:40I will discuss the motivation, the advantages and the problems of using simplified models as a tool to interpret LHC searches for dark matter. I will present a few examples for how this approach can be used to understand the complementarity of different dark matter search strategies. Finally, I will focus on various consistency conditions that should be imposed even on the most simplified...Go to contribution page
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Michael Duerr (DESY)13/04/2016, 18:20I present an extension of the Standard Model where baryon number is a local gauge symmetry that is spontaneously broken. In such a setup, anomaly cancellation requires the introduction of new fermion fields, the lightest of which is an attractive dark matter candidate. Dark matter stability is an automatic consequence of the gauge symmetry, and proton decay never occurs even if baryon number...Go to contribution page
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Dan Levin (University of Michigan (US))13/04/2016, 18:40Signatures of large missing transverse momentum recoiling against jets at the LHC provide powerful probe to strongly produced dark matter (DM), complementary to direct and indirect DM detection experiments. This talk presents recent results on dark matter searches with the ATLAS detector in LHC Run 2, focusing on signatures with jets, photons or hadronically decaying bosons.Go to contribution page
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Manfred Jeitler (Austrian Academy of Sciences (AT))13/04/2016, 19:00The existence of dark matter, indicated by astronomical observations, is one of the main proofs of physics beyond the standard model. Despite its abundance, dark matter has not been directly observed yet. This talk presents several searches for dark matter production in proton-proton collisions at 7, 8, and 13 TeV at the LHC, performed by the CMS collaboration. They are interpreted in terms of...Go to contribution page
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Jenny List (Deutsches Elektronen-Synchrotron Hamburg and Zeuthen (DE))14/04/2016, 08:20Invited Talk
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Jernej F. Kamenik (Jozef Stefan Institute)14/04/2016, 09:00Invited Talk
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Timothy Gershon (University of Warwick (GB))14/04/2016, 10:10Invited Talk
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Andreas Crivellin (CERN)14/04/2016, 10:50Invited Talk
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Florian Urs Bernlochner (Universitaet Bonn (DE))14/04/2016, 11:30Invited Talk
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Alejandro Celis (Ludwig Maximilian University of Munich)14/04/2016, 17:00TalkRecent anomalies in B meson decays observed by the LHCb collaboration have motivated the construction of extensions of the Standard Model with a gauged family non-universal U(1) factor. I will present a large class of family non-universal U(1) gauge models for which flavor changing neutral currents are completely controlled by CKM matrix elements. I will discuss then phenomenological...Go to contribution page
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Eung Jin Chun (Korea Institute for Advanced Study)14/04/2016, 17:20Updating various theoretical and experimental constraints on the four different types of two-Higgs-doublet models (2HDMs), we find that only the ``lepton-specific" (or ``type X") 2HDM can explain the present muon g−2 anomaly in the parameter region of large tanβ, a light CP-odd boson, and heavier CP-even and charged bosons which are almost degenerate. The severe constraints on the models come...Go to contribution page
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Mr Antonio Augusto Alves Junior (University of Cincinnati (US))14/04/2016, 17:40The analysis of the full LHC Run I data set of proton-proton collision events collected with the LHCb detector, corresponding to an integrated luminosity of 3.0 fb-1, is yielding several improved results on exotic hadron candidates, such as $X(3872)$ and $Z(4430)^+$, as well as the first observation of two new states compatible with the pentaquark hypothesis. Run II data allow LHCb to further...Go to contribution page
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Luigi Li Gioi (Max-Planck-Institut fuer Physik (Werner-Heisenberg-Institut) (D)14/04/2016, 18:20The Belle II experiment at the SuperKEKB collider is a major upgrade of the KEK B factory in Tsukuba, Japan. The machine is designed for an instantaneous luminosity of $8\times 10^{35}$ cm$^{-2}$s$^{-1}$ and the experiment is expected to accumulate a data sample of about 50 ab$^{-1}$ in 5 years running. With this amount of data, decays sensitive to physics beyond the Standard Model can be...Go to contribution page
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Barbara Storaci (Universitaet Zuerich (CH))14/04/2016, 18:40By using the very first proton-proton collision data of the LHC Run II, LHCb performed a series of measurements, notably including the cross-sections for quarkonia, beauty and charm productions. The results have been carried out by exploiting a new scheme for the LHCb software trigger, where the algorithm has been split in two stages to allowing for a delayed trigger decision. This enables the...Go to contribution page
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Sebastian Ohmer (Max-Planck-Institut fuer Kernphysik (MPIK), Heidelberg)14/04/2016, 19:00Young Scientists ForumThe Talk is based on - P. Fileviez Perez, S. Ohmer and H. H. Patel, "Minimal Theory for Lepto-Baryons", Phys.Lett. B735 (2014) 283-287, [arXiv: 1403.8029] - P. Fileviez Perez and S. Ohmer, "Low Scale Unification of Gauge Interactions", Phys.Rev. D90 (2014) 3, 037701, [arXiv: 1405.1199] - S. Ohmer and H. H. Patel, "Leptobaryons as Majorana...Go to contribution page
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Simon Wehle (DESY Hamburg)14/04/2016, 19:10We present the measurement of angular observables in the decay $B^0\to K^{∗0}(892)\ell^+\ell^−$, where $\ell^+\ell^−$ is either $e^+e^−$ or $\mu^+\mu^−$. The analysis is performed on a data sample corre- sponding to 711 fb$^{−1}$ containing $772 × 10^6$ $B\bar B$ pairs, collected at the $\Upsilon(4S)$ resonance with the Belle detector at the asymmetric-energy $e^+e^−$ collider KEKB. Four...Go to contribution page
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Zoltán Tulpiánt (University of Debrecen)14/04/2016, 19:20Young Scientists ForumVetoing undesired jets is essential in many analyses aiming at searches for new particles. A new jet function, called N-jettiness has been introduced with the purpose of using an inclusive event shape variable for vetoing jets. The logarithms from the phase space restriction, are simple enough to allow their systematic summation to all orders, which allows for providing high precision...Go to contribution page
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Hartger Weits (NIKHEF (NL))14/04/2016, 19:30Direct searches for lepton–flavour–violation (LFV) in decays of the Z and recently discovered Higgs boson with the ATLAS detector at the LHC are presented. Three LFV decays are considered: H → eτ, H → µτ, and Z → µτ. The searches are based on the data sample of proton–proton collisions collected by the ATLAS detector corresponding to an integrated luminosity of 20.3 fb−1 at a center–of–mass...Go to contribution page
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Valentin V Khoze (Durham University)15/04/2016, 08:20Invited Talk
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Christian Kiesling (Werner-Heisenberg-Institut)15/04/2016, 09:00Invited Talk
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Tilman Plehn (Heidelberg University)15/04/2016, 10:10Invited Talk
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Belle II speakerFlavor PhysicsTalkThe Belle II experiment at the SuperKEKB collider is a major upgrade of KEK B factory facility in Tsukuba, Japan. First beams are planned for early 2016 and first physics data will be recorded in the middle of 2017 during phase 2 commissioning, while the Belle II detector is still missing its vertex detector system. In this talk, we will describe the physics program for this early data, which...Go to contribution page
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Carlos Tamarit (IPPP Durham)Scalar SectorTalkThe experimental data point towards the fact that the Standard Model, when assumed to be valid up to very high energies, might be metastable. The stability properties of the theory strongly depend on the Higgs and top masses, so that it becomes important to perform precise, unambiguous computations. Traditionally, these rely on calculating the effective potential and checking for an...Go to contribution page
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Giorgio BusoniTalkThe Sun may act as a gravitational well and capture Dark Matter at a constant rate: DM would therefore accrete inside the Sun. In absence of Annihilation (for example, for Asymmetric Dark Matter) the total number of captured DM particles at $t=t_{sun}$ may have stabilised to a constant number only if capture goes in equilibrium with evaporation, for DM masses below 5-10 GeV, while for higher...Go to contribution page
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Joachim Kopp (Johannes-Gutenberg-Universitaet Mainz (DE))
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