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The 15th International Workshop on Tau Lepton Physics

24–28 Sept 2018
Vondelkerk, Amsterdam
Europe/Amsterdam timezone

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Session

Session

24 Sept 2018, 13:00
Vondelkerk, Amsterdam

Vondelkerk, Amsterdam

Vondelstraat 120, 1054 GS Amsterdam, The Netherlands

Conveners

Session: Welcome

  • There are no conveners in this block

Session: Tau properties - I

  • Yuping Guo

Session: Tau properties - II

  • Matthias Jamin

Session: Flavor puzzles

  • Gregory Max Ciezarek (CERN)

Session: Lepton Flavor Violation with taus and muons

  • Robert Fleischer (Vrije Universiteit Amsterdam)

Session: Standard Model measurements with taus at the LHC

  • Keti Kaadze (Kansas State University (US))

Session: Beyond Standard Model measurements with taus at LHC - I

  • Luca Fiorini (Univ. of Valencia and CSIC (ES))

Session: Beyond Standard Model measurements at the LHC - II

  • Cristina Galea (Nikhef National institute for subatomic physics (NL))

Session: Neutrino - I

  • Vittorio Paolone (University of Pittsburgh)

Session: Neutrino - II

  • Paul De Jong (Nikhef National institute for subatomic physics (NL))

Session: g-2 theory

  • Mattia Bruno (BNL)

Session: g-2 experiments

  • Charles Timmermans

Session: QCD

  • Elisabetta Pallante

Session: Muon experiments

  • Nicolo De Groot (Department of Experimental High Energy Physics)

Session: Future detectors - I

  • Kenji Inami (Nagoya university)

Session: Future detectors - II

  • Marcus Matthias Morgenstern (Nikhef National institute for subatomic physics (NL))

Session: Poster presentations and summary talk

  • Olga Igonkina (Nikhef National institute for subatomic physics (NL))

Presentation materials

There are no materials yet.

  1. 89. Welcome
    Stan Bentvelsen (Nikhef National institute for subatomic physics (NL))
    24/09/2018, 13:00
  2. 90. Organisation issues
    Olga Igonkina (Nikhef National institute for subatomic physics (NL))
    24/09/2018, 13:20
  3. 91. Report from the HFLAV group
    Alberto Lusiani (INFN)
    24/09/2018, 13:30
    Talk
  4. 92. Latest Belle results on tau decays
    Yifan Jin (The University of Tokyo)
    24/09/2018, 14:00

    We firstly measure the branching fraction for tau -> pi e+e- nu and pi
    mu+mu- nu. Though these decays are allowed by the standard model, they
    have never been measured because they are expected to have a small
    branching fraction. Belle's largest tau data sample makes us to expect
    to measure these decays with a high sensitivity. In this presentation,
    we show the result of measurement of...

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  5. 94. Measurement of the branching fractions B(tau -> K npi0 nu), n=0,1,2,3, and B(tau -> pi npi0 nu), n=3,4
    Thomas Lueck (University of Pisa)
    24/09/2018, 14:20
    Talk

    We report the measurements of the branching fractions of the decay B(tau -> K npi0 nu), n=0,1,2,3, and B(tau -> pi npi0 nu), n=3,4 excluding the contributions that proceed through the decay of intermediate K0 and \eta mesons. The measurements are based on a data sample of 435 million tau pairs produced in e+e- collisions at and near the Y(4s) peak and collected with the BaBar detector in...

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  6. 93. Prospects for τ lepton physics at Belle II
    Michel Hernandez Villanueva (Cinvestav)
    24/09/2018, 14:40

    The Belle II experiment is a substantial upgrade of the Belle detector and will operate at the SuperKEKB energy-asymmetric e+e− collider. The accelerator has already successfully completed the first phase of commissioning in 2016 and first electron positron collisions in Belle II are expected for April 2018. The design luminosity of SuperKEKB is 8×1035 cm−2s−1 and the Belle II experiment aims...

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  7. 98. Tau mass measurement at BESIII
    Jianyong Zhang (IHEP, CAS)
    24/09/2018, 15:30
    Talk

    In order to obtain the most accurate mass of tau lepton using a limited amount of data at BESIII, we optimized the position and luminosity distribution of each energy point. Beam energy measurement system was built at BEPCII for minimizing the system error caused by energy uncertainty. About 140 pb-1 tau mass scan data was acquired in April this year, and preliminary measurement results is...

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  8. 95. Implications of tau data for CP violation in K decays
    Antonio Rodríguez-Sánchez
    24/09/2018, 15:50
    Talk

    In the chiral limit, the D = 6 contribution of the Operator Product Expansion (OPE) of the V-A correlator of quark currents only depends on two vacuum condensates, which can be related with the electroweak penguin contributions of K->pipi processes, keys for a better understanding of CP violation in kaons. We use those relations to obtain those matrix elements between hadrons using the ALEPH...

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  9. 97. The status of the inclusive tau determination of V_us
    Kim Maltman (York University)
    24/09/2018, 16:10
    Talk

    I review the current status of determinations of V_us using inclusive hadronic tau decay data, focusing on (1) recent work establishing theoretical systematic issues with the conventional determination based on flavor-breaking finite-energy sum rule analyses employing only inclusive strange and non-strange branching fractions as experimental input, (2) an alternate flavor-breaking sum rule...

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  10. 170. A no-go theorem for non-standard explanations of the τ→KSπντ CP asymmetry
    Martin Hoferichter (University of Washington)
    24/09/2018, 16:30
    Talk
  11. 100. Non-standard interactions in tau- -> (pi-pi0,pi-eta)nu_tau
    Gabriel Lopez Castro (Cinvestav-IPN)
    24/09/2018, 16:50
    Talk

    Being G-parity suppressed in the SM, tau to eta/eta' pi nu_tau decays can set competitive bounds on non-standard scalar charged current interactions. This question is addressed within an EFT framework, including the most general interactions between SM fields up to dimension six, assuming massless neutrinos (based on JHEP 1712 (2017) 027).

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  12. 101. New Physics bounds from Hadronic Tau decays
    Martin Gonzalez-Alonso (CERN)
    24/09/2018, 17:10
    Talk

    I'll discuss the information about New Physics that can be extracted from Hadronic Tau decays, and its interplay with other Electroweak Precision Observables and the complementarity with searches at the LHC.

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  13. 99. NLO prediction for the decays τ→ℓℓ′ℓ′νν¯ and μ→eeeνν¯
    Matteo Fael (University of Siegen)
    24/09/2018, 17:30
    Talk

    We present the differential decay rates and the branching ratios of the tau and muon decays with internal conversion, τ→ℓℓ′ℓ′νν¯ and μ→eeeνν¯, in the Standard Model at NLO in the on-shell scheme.

    These five-body leptonic decays are a tool to study the Lorentz structure of the weak interactions and to test lepton flavor universality. They are also a source of SM background for...

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  14. 96. BSM b->s tau+ tau-
    Bernat Capdevila (IFAE)
    24/09/2018, 17:50
    Talk
  15. 121. Theory status
    Svjetlana Fajfer (Univ. of Ljubljana and Inst. J. Stefan)
    25/09/2018, 08:30
    Talk
  16. 124. LFU tests with semitauonic decays at LHCb
    Sean Benson (Nikhef National institute for subatomic physics (NL))
    25/09/2018, 09:00
    Talk

    In the Standard Model, the three charged leptons are identical copies of each other, apart from mass differences. Experimental tests of this feature in semileptonic decays of b-hadrons are highly sensitive to New Physics particles which preferentially couple to the 2nd and 3rd generations of leptons. This talk will review the latest lepton universality tests in semileptonic b->c transitions at LHCb.

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  17. 123. Exploiting tau polarisation in B -> D* tau nu
    Susanne Westhoff (Heidelberg University)
    25/09/2018, 09:20
    Talk
  18. 122. Probing LNU with (semi)leptonic B decays
    Gilberto Tetlalmatzi-Xolocotzi (Nikhef)
    25/09/2018, 09:40
    Talk
  19. 125. LNU, LNV and LFV at Belle II
    Ami Rostomyan (DESY)
    25/09/2018, 10:00
    Talk
  20. 115. Leptonic LFV theory
    Adrian Signer (Durham University)
    25/09/2018, 10:40
    Talk
  21. 119. LFV and neutrino mass
    Ana M. Teixeira (LPC Clermont)
    25/09/2018, 11:10
    Talk
  22. 117. Meson LFV decays (X->e+mu) in LHCb
    Maarten Van Veghel (Nikhef National institute for subatomic physics (NL))
    25/09/2018, 11:40
    Talk
  23. 118. Test lepton flavor universality with (semi)leptonic D decays at BESIII
    Sifan Zhang (Institute of High Energy Physics Chinese Academy of Sciences)
    25/09/2018, 12:00
    Talk

    Using 2.93 fb−1 data taken at s√=3.773 GeV and 3.19~fb−1 data taken at s√=4.178 GeV with the BESIII detector, precision measurements of the branching fractions of D0→K−μ+νμ, D+→K¯0μ+νμ, D0→π−μ+νμ, D+→π0μ+νμ and D+s→μ+νμ are performed.
    Combining the known branching fractions of D→K¯e+νe, D→πe+νe and D+s→τ+ντ,
    we have tested the lepton flavor universality with D→K¯ℓ+νℓ, D→πℓ+νℓ and D+s→ℓ+νℓ...

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  24. 193. L to l(') l+ l- LFV decays in the SM with massive neutrinos
    Dr Gerardo Hernández Tomé (Cinvestav)
    25/09/2018, 12:20
    Talk
  25. 102. Hadronic Tau reconstruction and identification performance in ATLAS and CMS
    Anne-Catherine Le Bihan (Centre National de la Recherche Scientifique (FR))
    25/09/2018, 14:00
    Talk

    Tau leptons play an important role in many Standard Model and Beyond the Standard Model physics processes that are being investigated at the LHC. This talk details measurements of the performance of the reconstruction and identification of hadronic tau lepton decays by the ATLAS and CMS detectors. The measurements include the performance of the identification, trigger, energy calibration and...

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  26. 106. Monte Carlo, fitting, Machine Learning for Tau leptons
    Zbigniew Andrzej Was (Polish Academy of Sciences (PL))
    25/09/2018, 14:25
    Talk

    Over the last few years, progress in analysis of massively multidimensional distribution was achieved for the broad range of applications in Industry, Science and in particular in domain of High Energy physics. In the talk use of such techniques for Higgs boson parity measurement using its cascade decay into tau leptons and later into 3pi decay modes will be used as an example. The use of...

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  27. 103. Tau polarization measurement in Z->tautau at LHC
    Benedict Tobias Winter (Albert Ludwigs Universitaet Freiburg (DE))
    25/09/2018, 14:45
    Talk

    Parity violation in decays of Z bosons leads to tau lepton polarisation. The measurement of the polarisation offers a unique possibility to measure tau lepton couplings and to translate them into a measurement of the effective electroweak mixing angle. Data taken by the CMS experiment are used to perform a measurement of the tau lepton polarisation in the most promising hadronic decay modes....

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  28. 104. Measurements of Higgs boson decays to leptons with the ATLAS detector
    Lara Katharina Schildgen (University of Bonn (DE))
    25/09/2018, 15:05
    Talk

    The Higgs boson decays to di-leptons has been studied by the ATLAS Collaboration using pp collisions at the LHC. Recent results on the H-> tau tau final state based on 36fb-1 of data collected at 13 TeV will be shown. In addition searches for the Lepton Flavour Violating Higgs boson decays and for the H-> mu mu final state will also be reported.

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  29. 105. Measurements of Higgs properties with the H->tautau decay at CMS
    Somnath Choudhury (Indian Institute of Science (IN))
    25/09/2018, 15:30
    Talk

    The latest results on the Higgs boson decaying into a tau pair using data from the CMS experiment are reported. The talk will include the observation of the Higgs boson into a tau pair decays with the Run 2 and Run 1 data, and the more recent analyses targeting the VH and ttH production modes. The decay channel into taus allows also constraining the CP properties of the Higgs boson and first...

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  30. 112. Higgs LFV involving taus (theory)
    Cedric Weiland (IPPP Durham)
    25/09/2018, 16:20
  31. 113. Search for lepton flavour violation with the ATLAS detector
    Brian Le (University of Melbourne (AU))
    25/09/2018, 16:40
    Talk

    Lepton flavor violation (LVF) is a striking signature of potential beyond the Standard Model physics. The search for LFV with the ATLAS detector is reported in searches focusing on the decay of the Higgs boson, the Z boson and of a heavy neutral gauge boson, Z', using pp collisions data with a center of mass energy of 8 TeV and 13 TeV.

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  32. 116. Search for lepton flavour violation with the CMS detector
    Jian Wang (University of Florida (US))
    25/09/2018, 17:00
    Talk

    The experimental observation of neutrino oscillations proves that neutrinos have mass and Lepton Flavour is not conserved in the neutral sector. This implies that Lepton Flavour non-conservation occurs also in the charged sector through neutrino loops, which, however, are extremely suppressed, well beyond the foreseeable experimental reach. On the other hand, several Beyond the Standard Model...

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  33. 120. LHC searches motivated by recent B-anomalies
    Darius Faroughy (Jozef Stefan Institute)
    25/09/2018, 17:20
    Talk
  34. 107. Leptoquark searches and high mass phenomena with taus at CMS
    Klaas Padeken (Vanderbilt University (US))
    25/09/2018, 17:40
    Talk

    Several searches for new particles with taus are presented. Leptoquarks that couple strongly to the third generation may explain long-standing anomalies observed in B physics. Searches for both singly and doubly produced leptoquarks have been carried out with LHC run 2 data. In addition, searches for scalar partners of the tau, as predicted in supersymmetric models, for new gauge bosons (W' to...

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  35. 108. Searches for new phenomena with tau leptons in the final state using the ATLAS detector
    Masahiro Kuze (Tokyo Institute of Technology (JP))
    25/09/2018, 18:00
    Talk

    Many theories beyond the Standard Model predict new phenomena which decay to well isolated, high-pT tau leptons. Searches for new physics models with these signatures are performed using the ATLAS experiment at the LHC. The results reported here use the pp collision data sample collected in 2015 and 2016 by the ATLAS detector at the LHC with a centre-of-mass energy of 13 TeV.

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  36. 165. New physics opportunities in the tau sector
    AMARJIT Soni (BNL)
    25/09/2018, 18:20
    Talk
  37. 109. Di-Higgs searches in final states with tau leptons at the LHC
    Petar Bokan (Uppsala University (SE), Georg-August-Universitaet Goettingen (DE))
    26/09/2018, 08:30
    Talk

    Di-Higgs final states can arise through non-resonant production of two Higgs
    bosons and through potential heavy states decaying to two Higgs boson. This
    talk presents searches for di-Higgs decays in final states containing two tau
    leptons and two b-quarks at the ATLAS and CMS experiments using 13 TeV
    collision data from the LHC.

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  38. 110. Searches for additional Higgs bosons decaying to tau leptons at the LHC
    Claudio Caputo (Universite Catholique de Louvain (UCL) (BE))
    26/09/2018, 08:50
    Talk

    The searches for additional Higgs bosons decaying to tau leptons in scenarios beyond the standard model will be summarised, from the pp collision data collected by the ATLAS and CMS experiments at LHC Run-2.

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  39. 111. SUSY searches with taus at the LHC
    Feng Lyu (Chinese Academy of Sciences (CN))
    26/09/2018, 09:10
    Talk

    The supersymmetric partner of the tau lepton, the stau, is predicted to be relatively light in a range of SUSY models, and may be a key for dark matter.
    This talk presents recent CMS and ATLAS results from searches for chargino and neutralino mediated stau, and direct stau pair production.

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  40. 126. Neutrinoless Double Beta Decay Overview
    Laura Cardani (INFN - National Institute for Nuclear Physics)
    26/09/2018, 09:50
    Talk
  41. 127. Neutrinoless Double Beta Decay - Theory and Connection to Tau
    Vincenzo Cirigliano (Los Alamos National Laboratory)
    26/09/2018, 10:20
    Talk
  42. 128. Solar Neutrino Physics with Borexino
    Andrea Pocar (University of Massachusetts, Amherst)
    26/09/2018, 10:50
    Talk

    Borexino is a large solar neutrino detector running at the Laboratori Nazionali del Gran Sasso since 2007. Neutrinos are detected via their interaction with a 300-ton liquid scintillator target, purified to achieve unprecedented levels of radio-purity. Borexino has detected most of the expected solar neutrino spectrum, as well as anti-neutrinos from Earth’s radioactivity and from nuclear...

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  43. 129. KATRIN First Tritium
    Volker Hannen (University of Münster)
    26/09/2018, 11:10
    Talk
  44. 133. Sterile neutrinos (including SBND program)
    Ivan Esteban
    26/09/2018, 11:30
    Talk
  45. 134. Recent Results from MicroBooNE
    Wei Tang (University of Tennessee)
    26/09/2018, 11:55
    Talk

    MicroBooNE is a 85-ton active mass Liquid Argon Time Projection Chamber (LArTPC) which has been collecting data since 2015 from the Booster Neutrino Beam at Fermilab. LArTPCs are imaging detectors that record neutrino interactions with strong spatial resolution and are among the favored technology for the next generation of neutrino experiments. The main goal of MicroBooNE is to investigate...

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  46. 131. Recent results from reactor antineutrino experiments
    Hyunkwan Seo
    26/09/2018, 13:30
    Talk

    The smallest neutrino mixing angle θ_13 has been successfully measured by the disappearance of reactor antineutrinos at RENO, Daya Bay, and Double Chooz. The oscillation frequency is also measured based on energy and baseline dependent disappearance probability of reactor antineutrinos. Recent results find a variation in the observed reactor antineutrino flux as a function of the reactor fuel...

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  47. 130. Final results of the OPERA experiment on nu-tau appearance in the CNGS neutrino beam
    Giuliana Galati (Universita e sezione INFN di Napoli (IT))
    26/09/2018, 13:50
    Talk

    The OPERA experiment at the Gran Sasso Laboratory was designed to study nu_mu → nu_tau oscillations in appearance mode in the CERN-to-Gran Sasso neutrino beam. We report the final analysis of the full data sample based on looser selection criteria than in previous analyses, and multivariate approach. Oscillation parameters have been determined with a reduced statistical uncertainty, and the...

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  48. 132. Beams T2K, NOvA and resulting picture
    Pablo Fernandez Menendez (Univ. of Valencia and CSIC (ES))
    26/09/2018, 14:10
    Talk
  49. 135. Cosmic neutrinos: IC, KM3NeT, ANTARES, AUGER
    Daan van Eijk (WIPAC)
    26/09/2018, 14:35
    Talk
  50. 139. Introduction
    William Marciano (Brookhaven)
    27/09/2018, 08:30
    Talk
  51. 140. Hadronic vacuum polarization
    Christoph Lehner (BNL)
    27/09/2018, 09:15
    Talk
  52. 141. Hadronic light-by-light
    Harvey Meyer
    27/09/2018, 09:40
    Talk
  53. 143. Historical Overview
    Bradley Lee Roberts (Boston University)
    27/09/2018, 10:30
    Talk
  54. 144. E989 @ FNAL
    Anna Driutti
    27/09/2018, 11:00
    Talk
  55. 145. E34 @ KEK
    Tsutomu Mibe
    27/09/2018, 11:20
    Talk
  56. 146. Auxiliary measurements, esp. mumu/mup in Muonium; MuSEUM experiment
    Shimomura
    27/09/2018, 11:40
    Talk
  57. 147. Search for the Electric Dipole Moment and anomalous magnetic moment of the tau lepton at tau factories
    Xin Chen (Tsinghua University (CN))
    27/09/2018, 12:00
    Talk

    Precise measurement of the Electric Dipole Moment (EDM) and anomalous magnetic moment (g-2) of particles is an important test of Beyond Standard Model (BSM) physics. It is generally believed that the tau lepton couples more strongly to BSM due to its large mass, and can be searched for at collider experiments. A new method to approximately reconstruct the neutrinos from the hadronic decays of...

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  58. 148. Experimental input from e+e- machines to hadronic contribution to muon (g-2)
    Boris Shwartz (Budker Institute of Nuclear Physics, Novosibirsk)
    27/09/2018, 12:20
    Talk

    The VEPP-2000 e+e− collider has been operating at BINP (Novosibirsk) from 2010 in the center-of-mass energy range from 0.3 to 2 GeV. The project luminosity of this machine, exploiting the idea of the round beams, has to amount to 1032cm−2s−1. In 2017 experiments at VEPP-2000 were renewed after three year shutdown taken for new intensive positron injection source implementation as well as for...

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  59. 149. e+e- for g-2 light-by-light
    Yuping Guo
    27/09/2018, 12:40
    Talk
  60. 136. Alpha_s from lattice
    Stefan Sint (Trinity College Dublin (IE))
    27/09/2018, 14:30
    Talk
  61. 137. The strong coupling from e+e−→ hadrons
    Maarten Golterman (San Francisco State University)
    27/09/2018, 14:50
    Talk

    We use a new compilation of the hadronic R-ratio from available data for the process e+e−→ hadrons below the charm mass to determine the strong coupling αs, using finite-energy sum rules. Quoting our results at the τ mass to facilitate comparison to the results obtained from similar analyses of hadronic τ-decay data, we find αs(m2τ)=0.298±0.016±0.006 in fixed-order perturbation theory, and...

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  62. 138. Alpha_s from tau data
    Antonio Pich (IFIC, U. Valencia -.)
    27/09/2018, 15:10
    Talk
  63. 150. General features of LFV experiments with muons
    Yoshitaka Kuno (Osaka University)
    27/09/2018, 16:00
    Talk
  64. 151. The Mu3e Experiment at PSI
    Alessandro Bravar (Universite de Geneve (CH))
    27/09/2018, 16:30
    Talk

    Lepton Flavor Violation (LFV) is strongly suppressed in the Standard Model, whilst several models based on {\it new physics} predict observable effects accessible to the new generation of experiments. Mu3e will search for the LFV neutrinoless muon decay μ+→e+e−e+ with a sensitivity down to 10−16 (at 90\% C.L.) using the world most intense continuous muon beam at the Paul Scherrer...

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  65. 152. Searching for Muon to electron conversion : The Mu2e experiment at Fermilab
    Richard Bonventre (Lawrence Berkeley National Laboratory)
    27/09/2018, 16:50
    Talk

    The Mu2e experiment will measure the charged-lepton flavor violating (CLFV) neutrino-less conversion of a negative muon into an electron in the field of a nucleus. Mu2e will improve the previous measurement by four orders of magnitude, reaching a SES (single event sensitivity) of 3×10−17 on the conversion rate. The experiment will reach mass scales of nearly 104 TeV, far beyond the direct...

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  66. 153. mu-e conversion experiments in J-PARC
    Natsuki Teshima (Osaka City University)
    27/09/2018, 17:10
    Talk
  67. 154. MEG final results and progress towards MEG-II
    Toshiyuki Iwamoto
    27/09/2018, 17:30
    Talk
  68. 156. Tau physics at the High Luminosity LHC
    Emilie Passemar (Indiana University/JLab)
    28/09/2018, 08:30
  69. 155. Tau physics at CEPC/ILC
    Manqi Ruan (Chinese Academy of Sciences (CN))
    28/09/2018, 08:50
    Talk
  70. 157. Tau physics at FCC
    Mogens Dam (University of Copenhagen (DK))
    28/09/2018, 09:10
    Talk
  71. 159. GRAND: A Giant Radio Array for Neutrino Detection
    Charles Timmermans
    28/09/2018, 09:30
    Talk

    Precise detection of cosmogenic ultra-high-energy (UHE) neutrinos, with energy in excess of 108 GeV, will confirm the photo-dissociation of UHE cosmic rays and the identification of the sources of UHE neutrinos will directly point to sources of UHE cosmic rays.

    GRAND will look for ντs interacting in rock, thereby creating an UHE τ lepton, which can escape from the rock.The τ decay products...

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  72. 160. Status of the DUNE Experiment
    Alessandra Tonazzo
    28/09/2018, 10:20
    Talk

    The Deep Underground Neutrino Experiment (DUNE) provides a rich science program with the focus on the neutrino oscillation physics, proton decay studies and Supernova explosions. The high-intensity wide-band neutrino beam will be produced at Fermilab and will be directed to the 40 kt Liquid Argon far detector at the Sanford Underground Research Facility (SURF), 1300 km from Fermilab. One of...

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  73. 158. Super tau charm factory, HIEPA
    Guangshun Huang (University of Science and Technology of China (CN))
    28/09/2018, 10:40
    Talk
  74. 161. Novosibirsk: tau-charm factory and di-muonium experiment
    Pavel Piminov (Budker Institute of Nuclear Physics (RU))
    28/09/2018, 11:00
    Talk
  75. 162. SHIP
    Kyrylo Bondarenko
    28/09/2018, 11:20
    Talk
  76. 194. 4th place: Search for ultra-high energy neutrinos with the Pierre Auger Observatory
    Marta Trini
    28/09/2018, 12:00
  77. 195. 3rd place: Study of Michel parameters in tau decays at Belle
    Denis Epifanov (BINP)
    28/09/2018, 12:10
  78. 196. 2nd place: The Rare and Forbidden: Testing Physics Beyond the Standard Model with Mu3e
    Ann-Kathrin Perrevoort (Nikhef National institute for subatomic physics (NL))
    28/09/2018, 12:20
  79. 197. 1st place: On isospin breaking in tau input for (g-2) from Lattice QCD
    Mattia Bruno (BNL)
    28/09/2018, 12:35
  80. 164. Summary talk
    Simon Eydelman (Budker Institute of Nuclear Physics (RU))
    28/09/2018, 12:45
    Talk
  81. 142. Beyond the SM
    Dominik Stockinger (University Glasgow)
    Talk
  82. 114. CMS LFV searches
    Talk
  83. 163. Poster talks
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