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Diego Martinez Santos (Universidade de Santiago de Compostela (ES))08/06/2020, 09:35
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Yifan Jin (INFN-Trieste)08/06/2020, 09:45
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Toshiyuki Iwamoto08/06/2020, 10:15
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Admir Greljo (CERN)08/06/2020, 10:40
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Quanyin Li (University of Science and Technology of China (CN))08/06/2020, 11:35
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Gino Isidori (Universitaet Zuerich (CH))08/06/2020, 12:00
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Dayong Wang (Peking University (CN))08/06/2020, 12:30
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Mick Mulder (CERN)08/06/2020, 12:55
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Sebastien Descotes-Genon (Laboratoire de Physique Théorique d'Orsay)08/06/2020, 13:20
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Danny van Dyk (TU München)08/06/2020, 15:00
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Matthias Steinhauser (KIT)08/06/2020, 15:25
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Shun Watanuki08/06/2020, 15:50
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Srishti Bhasin (University of Bristol (GB))08/06/2020, 16:45
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Roy Briere (Carnegie Mellon University)08/06/2020, 16:45
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Dr Fernando Abudinén (INFN Sezione di Trieste)08/06/2020, 17:00
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Guenakh Mitselmakher (University of Florida (US))08/06/2020, 17:00
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Oleg Meshkov08/06/2020, 17:15
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Alexei Sibidanov (University of Victoria)08/06/2020, 17:15
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Mario Merola (University of Napoli Federico II and INFN - National Institute for Nuclear Physics)08/06/2020, 17:30
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Michel Hernandez Villanueva (University of Mississippi)08/06/2020, 17:30
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Marcello Rotondo (INFN e Laboratori Nazionali di Frascati (IT))09/06/2020, 09:00
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Saurabh Sandilya (University of Cincinnati)09/06/2020, 09:30
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Elvira Gamiz (University of Granada)09/06/2020, 10:00
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paolo gambino (università di torino)09/06/2020, 10:30
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Antonio Pich (IFIC, U. Valencia -.)09/06/2020, 11:30
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Chris Sachrajda (University of Southampton)09/06/2020, 12:00
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koji shiomi (High Energy Accelerator Research Organization)09/06/2020, 12:30
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Riccardo Fantechi (INFN Sezione di Pisa, Universita' e Scuola Normale Superiore, P)09/06/2020, 12:55
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Francesco Dettori (Universita e INFN, Cagliari (IT))09/06/2020, 13:20
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Yuval Grossman (Cornell University (US))09/06/2020, 15:00
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Gudrun Hiller (Technische Universitaet Dortmund (DE))09/06/2020, 15:30
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Alex Gilman09/06/2020, 16:00
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Dominik Stefan Mitzel (CERN)09/06/2020, 16:30
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Luke Pickering (Michigan State University)09/06/2020, 17:30
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Prof. Dawn Williams09/06/2020, 18:00
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Josh Renner (Univ. of Valencia and CSIC (ES))09/06/2020, 18:30
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Dr Zhang Yan10/06/2020, 09:00
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Bertrand Echenard (California Institute of Technology)10/06/2020, 09:00
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Alina Kleimenova (Universite Catholique de Louvain (UCL) (BE))10/06/2020, 09:15
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Elena Perez Del Rio (INFN - National Institute for Nuclear Physics)10/06/2020, 09:15
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Miguel Escudero (King's College London)10/06/2020, 09:30
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Gerald Eigen (University of Bergen (NO))10/06/2020, 09:30
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Patrick Foldenauer10/06/2020, 09:45
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Meng Wang10/06/2020, 09:45
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Maria Ramos (LIP)10/06/2020, 10:00
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Mr Evgeny Kozyrev (Budker Institute of Nuclear Physics)10/06/2020, 10:00
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Yanxi Zhang (CERN)10/06/2020, 10:15
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Silvia Delsanto (Universita e INFN Torino (IT))10/06/2020, 10:45
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Feng-Kun Guo10/06/2020, 12:10
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Dr Cong Geng10/06/2020, 12:35
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Roberta Cardinale (INFN e Universita Genova (IT))10/06/2020, 13:00
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Chengping Shen (Beihang University)10/06/2020, 13:25
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Luciano Maiani (Sapienza Universita e INFN, Roma I (IT))10/06/2020, 15:00
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Siavash Neshatpour (Université Lyon 1 - IP2I)10/06/2020, 15:30
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Nestor Armesto Perez (Universidade de Santiago de Compostela (ES))10/06/2020, 15:30
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Soumen Halder (Tata Institute of Fundamental Research)10/06/2020, 15:45
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Daniele Marangotto (Università degli Studi e INFN Milano (IT))10/06/2020, 15:54
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Paolo Iengo (CERN)10/06/2020, 16:00
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Luiz Vale Silva10/06/2020, 16:15
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Cynthia Hadjidakis (Université Paris-Saclay (FR))10/06/2020, 16:16
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Holger Arnold Herr (Johannes Gutenberg Universitaet Mainz (DE))10/06/2020, 16:30
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Enrico Fragiacomo (Universita e INFN Trieste (IT))10/06/2020, 16:38
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Dawid Piotr Gerstel (Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France)10/06/2020, 16:45
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Dominik Stoeckinger (TU Dresden)10/06/2020, 17:20
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Dr Esra Barlas Yucel10/06/2020, 17:45
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Dr Stefano Gariazzo (IFIC-CSIC/University of Valencia)10/06/2020, 18:15
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Ivan Esteban (Universitat de Barcelona)10/06/2020, 18:45
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Mingrui Zhao (China Institute of Atomic Energy (CN))11/06/2020, 09:30
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Mikhail Barabanov (JINR)11/06/2020, 09:30
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Alexander Nass (Forschungszentrum Jülich GmbH)11/06/2020, 09:45
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Dr Yi Zheng (Peking University)11/06/2020, 09:45
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Lennart Rustige (Université Clermont Auvergne (FR))11/06/2020, 10:00
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Slavomira Stefkova (DESY)11/06/2020, 10:00
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Claire Prouve (Universidade de Santiago de Compostela (ES))11/06/2020, 10:15
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di Gregorio Giulia11/06/2020, 10:15
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Valentina Mariani (Universita e INFN, Perugia (IT))11/06/2020, 10:30
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Guy Wilkinson (University of Oxford (GB))11/06/2020, 10:30
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Serhat Ordek (Georg August Universitaet Goettingen (DE))11/06/2020, 10:45
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Kenkichi Miyabayashi (Nara Women's University)11/06/2020, 11:30
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Vitaly Vorobyev (Novosibirsk State University)11/06/2020, 11:55
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Dr Yingrui Hou (UCAS)11/06/2020, 12:20
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Matthew William Kenzie (University of Warwick (GB))11/06/2020, 12:45
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Eduardo Rodrigues (University of Liverpool (GB))11/06/2020, 13:10
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Christine Davies (University of Glasgow)11/06/2020, 15:00
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Maria Vieites Diaz (EPFL - Ecole Polytechnique Federale Lausanne (CH))11/06/2020, 15:25
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Jhovanny Andres Mejia Guisao (Universidad de Antioquia (CO))11/06/2020, 15:50
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David London (Universite de Montreal)11/06/2020, 16:15
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Javier Cuevas (Universidad de Oviedo (ES))11/06/2020, 17:15
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Yotam Soreq (CERN)11/06/2020, 17:40
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Kenneth Johns (University of Arizona (US))11/06/2020, 18:05
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12/06/2020, 07:30
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Bedrich Roskovec (Charles University in Prague)12/06/2020, 09:00
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Mr Hirohisa A. Tanaka (SLAC/Stanford University)12/06/2020, 09:30
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Maria Cepeda (CIEMAT)12/06/2020, 10:00
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Cristina Lazzeroni (University of Birmingham (GB)), Matthew Moulson (INFN e Laboratori Nazionali di Frascati (IT))12/06/2020, 10:30
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Frederic Teubert (CERN)12/06/2020, 11:30
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Phillip Urquijo (University of Melbourne (AU))12/06/2020, 12:00
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Nicholas Ayres (ETH Zurich)12/06/2020, 12:30
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Alexander Lenz (IPPP, Durham)12/06/2020, 13:00
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Prof. Chenging Shen12/06/2020, 13:30
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Toru Iijima (Nagoya University)12/06/2020, 13:40
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Fabio Anulli (Sapienza Universita e INFN, Roma I (IT))Talk for parallel
We report on a precision measurement of the ratio $R_{\tau\mu} = BF(\Upsilon(3S)\to\tau^+\tau^-)/BF(\Upsilon(3S)\to\mu^+\mu^-)$ using data collected with the BABAR detector at the SLAC PEP-II $e^+e^-$ collider. The measurement is based on a 28 ${\mathrm{fb^-1}}$ data sample collected at a center-of-mass energy of 10.355 ${\mathrm{GeV}}/c^2$ which corresponds to a sample 122 million...
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Jingzhi Zhang (IHEP)Talk for parallel
BESIII has collected data samples corresponding to luminosities of 2.93 fb-1 and 3.19 fb-1 at center-of-mass energies of 3.773 and 4.178 GeV, respectively. The data set collected at 3.773 GeV contains quantum-correlated D0D0bar pairs that allow access to the phase differences between amplitudes. We report the measurements of strong phase differences in D0 decays, including KS/L pi+ pi-, which...
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Jingzhi Zhang (IHEP)Talk for parallel
Due to the high production rate of light mesons in J/psi decays, the hight statistics sample of 1.3 billion Jpsi events provide an ideal lab to investigate the decay dynamics of light mesons, in particular for eta and etaprime. Recently the BESIII experiment made significant progresses in eta and prime decays, including their hadronic and rare decays, which will be reported in this talk
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Luiz Vale SilvaTalk for parallel
Four-fermion effective interactions have played a major role in the formulation of the Standard Model (SM) of particle physics. Nowadays, they are of fundamental importance in establishing the viability of extensions of the SM, since this category of operators is sensitive to the flavor structure of New Physics (NP), including new sources of CP violation. Following the renormalization of...
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Prof. Mikhail Barabanov (JINR)Talk for parallel
The spectroscopy of charmonium-like mesons with masses above the 2_mD open charm threshold has been full of surprises and remains poorly understood [1]. The currently most compelling theoretical descriptions of the mysterious XYZ mesons attribute them to hybrid structure with a tightly bound cc\bar diquark [2] or cq(cq)\bar tetraquark core [3 - 5] that strongly couples to S-wave DD\bar...
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Fabio Anulli (Sapienza Universita e INFN, Roma I (IT))Talk for parallel
We report the observation of the rare charm decay $D^0 \to K^-\pi^+e^+e^-$, a search for nine lepton-number-violating and three lepton-flavor-violating neutral charm decays of the type $D^0 \rightarrow h^- h^{'-} \ell^+ \ell^{'+}$, and $D^0 \rightarrow h^- h^{'+} \ell^+ \ell^{'-}$, and a search for seven lepton-number-violating decays of the type $D^{0}\rightarrow X^{0} e^{\pm} \mu^{\mp}$,...
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Dawid Piotr Gerstel (Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France)Talk for parallel
Recent results from semileptonic b->clnu and b->ulnu decays studied at 7 TeV, 8 TeV and 13 TeV centre-of-mass energy with the LHCb detector will be reported. These include the measurement of hadronic form-factors in the Bs->Ds*munu decay and the first observation of the B->ppbarmunu decay.
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Fabio Anulli (Sapienza Universita e INFN, Roma I (IT))Talk for parallel
Many models of dark matter and hidden sectors predict new particles with masses below the electroweak scale. Low-energy electron-positron colliders such as BABAR are ideally suited to discover these hidden-sector particles. We present several recent BABAR searches for low-mass hidden- sector particles, including new searches for prompt and long-lived leptonically decaying hidden scalars...
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OTHER AUTHORSTalk for parallel
The NA62 experiment at the CERN SPS is designed to measure the branching ratio of the K+→π+vv decay, one of the best candidates to reveal indirect effects of new physics at the highest mass scales. NA62 took data in 2016-2018. The high-intensity fixed-target setup and detector performance make the NA62 experiment particularly suited for searches of new physics from faintly interacting...
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89. Study of resonant-states production in $e^+e^-$ annihilation in the energy region around 2.2 GeVFabio Anulli (Sapienza Universita e INFN, Roma I (IT))Talk for parallel
Two vector resonances with a mass near 2.2 GeV/$c^2$ are presently known: the $\phi(2170)$ observed in several production processes, but seen to decay only to $\phi(2170)\to\phi(1020)f_0(980)$, and the not well established $\rho(2150)$. Recently the BES-III experiment observed a clear interference pattern in the same energy region in $e^+e^-\to K^+K^-$, interpreted as a resonance with a mass...
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Simona Giovannella (INFN)Talk for parallel
The KLOE-2 experiment at DA$\Phi$NE, the LNF Frascati $\phi$-factory, has completed its data taking in 2018, collecting 5.5 fb-1 of integrated luminosity. The goal of KLOE-2 is to extend and expand the physics program of KLOE. The original 'general purpose' central detector, made by a large drift chamber - 4 m in diameter - surrounded by a lead/scintillating fibre electromagnetic calorimeter,...
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Alexander Nass (Forschungszentrum Jülich GmbH)Talk for parallel
The Standard Model (SM) of Particle Physics is not capable to account for the apparent matter-antimatter asymmetry of our Universe. Physics beyond the SM is required and is either probed by employing highest energies (e.g., at LHC), or by striving for ultimate precision and sensitivity (e.g., in the search for electric dipole moments). Permanent electric dipole moments (EDMs) of particles...
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Jingzhi Zhang (IHEP)Talk for parallel
From 2011, BESIII has taken about 20 fb^-1 data samples at center of mass energies from 3.8 to 4.6 GeV, containing 21 energy points with luminosity larger than 400 pb^-1. This makes the study of vector states Y, charged states Z, X states, as well as the connections between them through transition processes possible. Using these data samples, new information about X(3872) decays, Y states from...
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