23โ€“27 Apr 2012
Hotel Inter-Brugo EXCO
Asia/Seoul timezone

Contribution List

236 out of 236 displayed
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  1. 23/04/2012, 08:45
  2. Pier Oddone (FNAL)
    23/04/2012, 09:00
  3. Jonathan Bagger (Johns Hopkins University)
    23/04/2012, 09:20
  4. Gao Jie
    23/04/2012, 09:40
  5. Satoru Yamashita (U. Tokyo)
    23/04/2012, 10:00
  6. Sakue Yamada
    23/04/2012, 10:50
  7. Barry Barish
    23/04/2012, 11:25
  8. Tae Jeong Kim
    23/04/2012, 13:30
  9. Michael Peskin (SLAC, Stanford University)
    23/04/2012, 14:00
  10. Nicholas Walker (DESY)
    23/04/2012, 15:00
  11. Prof. Francois Le Diberder
    23/04/2012, 15:00
  12. Tomohiko Tanabe (University of Tokyo)
    23/04/2012, 15:30
  13. Dr Timothy Barklow (SLAC)
    23/04/2012, 16:00
  14. Dr Shinichiro Michizono (KEK)
    23/04/2012, 16:00
  15. 23/04/2012, 16:00
  16. 23/04/2012, 16:00
  17. Dr Shigeki Fukuda (KEK)
    23/04/2012, 16:20
  18. Lucie Linssen (CERN)
    23/04/2012, 16:30
  19. Dr Karsten Buesser
    23/04/2012, 17:00
  20. 23/04/2012, 17:00
  21. 23/04/2012, 17:00
    Joint with Costing Group
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  22. Dr Christopher Nantista (SLAC)
    23/04/2012, 17:10
  23. 24/04/2012, 08:30
  24. 24/04/2012, 08:30
  25. Dr Karsten Buesser (DESY)
    24/04/2012, 08:30
    MDI
  26. Rohini Godbole (Indian Institute of Science)
    24/04/2012, 08:30
  27. 24/04/2012, 08:30
    Joint Session with CFS Working Group
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  28. Dr Frank Simon (Max-Planck-Institut fuer Physik)
    24/04/2012, 08:30
  29. 24/04/2012, 08:30
  30. Hitoshi Hayano (KEK)
    24/04/2012, 08:30
  31. Alessandro Vivoli (FNAL), Dr Nikolay Solyak (FNAL)
    24/04/2012, 08:35
  32. Marco Oriunno (SLAC National Accelerator Laboratory)
    24/04/2012, 08:50
    MDI
  33. Dr Frank Simon (Max-Planck-Institut fuer Physik)
    24/04/2012, 08:50
  34. Dr Nikolay Solyak (FNAL), Valeri Kapin (FNAL)
    24/04/2012, 08:50
  35. 24/04/2012, 09:00
  36. Dr Kiyoshi Kubo (KEK)
    24/04/2012, 09:10
  37. Koji Tsumura (National Taiwan University)
    24/04/2012, 09:10
    We study the feasibility of Type-X two Higgs doublet model (THDM-X) at collider experiments. In THDM-X, new Higgs states are almost decaying into tau leptons. Such scalar bosons are less constrained by current experimental data, because production cross sections are not enhanced by quark Yukawa interaction, and decay products includes multiple missing neutrinos. In this talk, we discuss a...
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  38. John Hauptman
    24/04/2012, 09:10
  39. Dr Thomas Markiewicz (SLAC)
    24/04/2012, 09:10
    MDI
  40. Chris Adolphsen (SLAC)
    24/04/2012, 09:30
  41. Wolfgang Lohmann (DESY)
    24/04/2012, 09:30
    MDI
  42. Prof. Tohru Takeshita (Shinshu University)
    24/04/2012, 09:30
  43. Tetsuo Shindou (Kogakuin University)
    24/04/2012, 09:35
    We consider extended Higgs sectors in SUSY SM in which extra chiral superfields are introduced to the MSSM. In such extended models, deviations from the MSSM can remain in predictions of several Higgs measurements by the non-decoupling effect, even if the extra scalars are all heavy. It is interesting to see the property of such non-decoupling effects in various model. In this talk, we focus...
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  44. Olga Novgorodova (DESY)
    24/04/2012, 09:50
  45. Philip Bambade (Laboratoire de l''Accelerateur Lineaire (LAL) (IN2P3) (LAL))
    24/04/2012, 10:30
    MDI
  46. 24/04/2012, 10:30
  47. Marcel Vos (Instituto de Fisica Corpuscular (IFIC) - Universidad de Valencia)
    24/04/2012, 10:30
    This contribution aims to give an overview of the DEPFET project to develop ultra-thin vertex detectors for future collider applications. A brief status report for all detector components is presented. The focus of this report is on a recent achievement: the successful thinning of prototype sensors to a thickness of 50 micron. A characterization of the thermo-mechanical properties of a...
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  48. Frank Gaede (DESY)
    24/04/2012, 10:30
  49. 24/04/2012, 10:30
    Joint session with CFS Working Group
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  50. Hitoshi Hayano (KEK)
    24/04/2012, 10:30
  51. Dr Rongli Geng (Jefferson Lab)
    24/04/2012, 10:35
  52. H. Hyun, H. Park
    24/04/2012, 10:50
    MDI
  53. Camille Ginsburg (FNAL)
    24/04/2012, 11:00
  54. Norman Graf (SLAC)
    24/04/2012, 11:00
  55. Marc Winter (Institut de Recherches Subatomiques (IReS))
    24/04/2012, 11:00
    "Low power CMOS Pixel Sensors of the MIMOSA series are about to meet the specifications of the ILD vertex detector. This achievement relies on double-sided ladders where the sensors mounted on one face provide the necessary spatial resolution while faster sensors mounted on the other face offre the necessary time stamping. The establised MIMOSA architecture allows to reach resolutions of 3...
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  56. Dr Brett Parker (BNL)
    24/04/2012, 11:10
    MDI
  57. Dr yoshihisa iwashita (Kyoto Univ.)
    24/04/2012, 11:20
    MDI
  58. Eriko Kato (tohoku univ)
    24/04/2012, 11:30
    I would like to present the resent developments of the readout ASIC for FPCCD vertex detector at ILC. Using Fine Pixel CCD(FPCCD) for the vertex detector is one of the attractive options for realizing ILC's physics. FPCCD uses a pixel size of 5ร—5um2 , which enables high position resolution. However also causes the total number of read out pixels to become extremely large (20,000x128pix/ch)....
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  59. Paolo Pierini (INFN Milano LASA)
    24/04/2012, 11:30
  60. Frank Gaede (DESY)
    24/04/2012, 11:30
  61. Prof. Philip Burrows (Oxford University)
    24/04/2012, 11:40
    MDI
  62. Mikael Berggren (DESY Hamburg)
    24/04/2012, 11:50
  63. Lukic Strahinja
    24/04/2012, 12:00
    MDI
  64. Dr Yasuhiro Sugimoto (KEK)
    24/04/2012, 12:00
    FPCCD vertex detector will be operated at -40C in order to minimize the effect of radiation damage. The power consumption inside the cryostat may exceed 50W. Therefore, an effective cooling system is necessary for the FPCCD vertex detector. We plan to use 2-phase CO2 for the coolant of the vertex detector. We would like to present an idea of FPCCD vertex detector cooling system and the...
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  65. Hitoshi Hayano (KEK)
    24/04/2012, 12:00
  66. Prof. Sabine Riemanns (DESY)
    24/04/2012, 13:30
  67. 24/04/2012, 14:00
    Objective of this face-to-face meeting is to discuss a coordination of the ATF2 dedicated run in this fall, i.e. October through December and expected participation in this run from collaborators.
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  68. Prof. David Rubin (Cornell University)
    24/04/2012, 14:00
  69. Alberto Ruiz Jimeno (Universidad de Cantabria)
    24/04/2012, 14:00
    The design of the ILD FTD sub detector is one of the main tasks of the IFCA group. One of the main issues of tracking detectors is to know at each moment the exact position of every component. Having a deformation and displacement monitor system integrated in the sub detectors would be of great utility to deal with this task. Fiber Bragg Grating (FBG) is the primary technique used in several...
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  70. Michael E. Peskin (SLAC)
    24/04/2012, 14:00
    I will discuss a few theoretical models that motivate pushing the accuracy on Higgs branching ratios to the percent level.
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  71. 24/04/2012, 14:00
  72. 24/04/2012, 14:00
    Joint session with Main Linac Working Group
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  73. Hitoshi Hayano (KEK)
    24/04/2012, 14:00
  74. Prof. Akira Yamamoto (KEK)
    24/04/2012, 14:05
  75. Jim Kerby (Fermi National Accelerator Lab. (Fermilab))
    24/04/2012, 14:10
  76. Dr Rongli Geng (Jefferson Lab)
    24/04/2012, 14:20
  77. 24/04/2012, 14:30
  78. Joe Conway (Cornell University)
    24/04/2012, 14:30
  79. Hitoshi Hayano (KEK)
    24/04/2012, 14:30
  80. Dominik Dannheim
    24/04/2012, 14:30
    The CLIC vertex detector must have excellent spacial resolution, full geometrical coverage extending to low polar angles, extremely low mass, low occupancy facilitated by time-tagging, and sufficient heat removal from sensors and readout. These considerations, together with the physics needs and beam structure of CLIC, push the technological requirements to the limits and imply a very...
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  81. Hiroaki Ono (Nippon Dental University)
    24/04/2012, 14:40
    Recent LHC results indicate the light Higgs (115 < Mh < 131 GeV) and the possibility of the 250 GeV ILC machine is increasing. To catch up with these inputs, we update the Higgs BR results from LOI including H->WW* with concerning the several masses at the CM energy of 250 GeV. We also study the vvH BR at 1 TeV as a benchmarking process of DBD. In this talk, we present the latest results of...
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  82. Hitoshi Hayano (KEK)
    24/04/2012, 14:40
  83. Paolo Pierini (INFN Milano LASA), Mr Tom Peterson (FNAL)
    24/04/2012, 14:50
  84. Hubert Gerwig (CERN)
    24/04/2012, 15:00
    The talk describes the engineering approach of an air cooling system for the Pixel and Tracker detectors. It will address the individual problems of mechanical support, air flow and cabling and how they are linked together. Computational fluid dynamic analysis show the resulting necessary air velocities and the temperatures in the different detector parts.
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  85. 24/04/2012, 15:00
  86. 24/04/2012, 15:00
  87. Dr Christopher Nantista (SLAC), Dr Shigeki Fukuda (KEK)
    24/04/2012, 15:00
  88. Junping Tian (KEK)
    24/04/2012, 15:05
    WWH and ZZH couplings are two of the fundamental couplings. Precision measurement of these two couplings are crucial to test the SM and constraint the new physics models. In this talk, we will present the WWH coupling measurement using vvH at 500 GeV and also the ZZH coupling by combining all the possible channels.
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  89. Jim Kerby (Fermi National Accelerator Lab. (Fermilab))
    24/04/2012, 15:10
  90. Dr Marc Ross (FNAL)
    24/04/2012, 15:20
  91. 24/04/2012, 15:30
    ICB : International Collaboration Board Chaired by P. Burrows
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  92. 24/04/2012, 15:30
  93. Constantino Calancha (KEK)
    24/04/2012, 15:30
    The determination of the Higgs boson branching fractions is central to the ILC physics programme. In particular, the rare decay H -> gamma gamma is one of the benchmark process for the DBD. Assuming an integrated luminosity of 250 fb-1 with the ILD detector at sqrt(s)=250 Gev we present preliminary results on the estimation of the statistical uncertainty on this branching ratio.
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  94. 24/04/2012, 15:30
  95. Mr Philippe Gros (Saga University)
    24/04/2012, 15:30
    LCTPC (Linear Collider TPC) is the TPC concept considered for tracking within ILD. Its goal is to achieve a momentum resolution of 9x10-5/GeV/c in the 3.5T magnetic field. It also requires a very low material budget to enable precise measurement in the highly granular electromagnetic calorimeter. Different MicroPattern Gas Detector (MPGD) technologies are developped for electron...
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  96. Mr John Carwardine (Argonne)
    24/04/2012, 15:30
  97. mike church (Fermilab)
    24/04/2012, 15:40
  98. Hitoshi Hayano (KEK)
    24/04/2012, 15:50
  99. Frank Simon (MPI)
    24/04/2012, 15:55
    We present the status of a study of the physics performance of CLIC for a staged construction with three energy stages at 500 GeV, 1.4 TeV and 3 TeV. For each stage, detailed information on the luminosity spectrum and the background level, in particular of mini-jet production in two photon processes, is used in full detector simulations. At the first energy stage, the capability for a top...
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  100. Dr Jeff Gronberg (LLNL)
    24/04/2012, 16:00
  101. Hitoshi Yamamoto
    24/04/2012, 17:00
    Chaired by Hitoshi Yamamoto
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  102. 24/04/2012, 18:00
  103. 25/04/2012, 08:30
  104. Dr Mark Palmer (Cornell University LEPP)
    25/04/2012, 08:30
  105. Prof. Andrei Seryi (John Adams Institute)
    25/04/2012, 08:30
    MDI
  106. Prof. Xuejun Jia (IHEP, China)
    25/04/2012, 08:30
  107. Katsushige Kotera (Shinshu University, Faculty of Science,)
    25/04/2012, 08:30
  108. Marcel Vos (IFIC Valencia), Roman Poeschl (LAL)
    25/04/2012, 08:30
    A study of top quark production at the future International Linear Collider with a centre-of-mass energy of 500\,GeV has is presented. The emphasis is put on determining the sensitivity to physics beyond standard model. The analysis has been carried out with a full simulation of the ILD detector. The presentation introduces the top quark helicity as observable to increase the sensitivity to...
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  109. Hitoshi Hayano (KEK)
    25/04/2012, 08:30
  110. Chris Adolphsen (SLAC)
    25/04/2012, 08:35
  111. Prof. Akira Yamamoto (KEK)
    25/04/2012, 08:50
  112. Dr Rogelio Tomas (CERN)
    25/04/2012, 08:50
    MDI
  113. Joe Conway (Cornell University), Dr Yulin Li (Cornell University)
    25/04/2012, 09:00
  114. Hiraku Ueno (Kyushu Univ.)
    25/04/2012, 09:00
  115. Dr Karsten Buesser (DESY)
    25/04/2012, 09:00
    MDI
  116. Hitoshi Hayano (KEK)
    25/04/2012, 09:10
  117. Hajrah Tabassam (Quaid-i-Azam University Islamabad)
    25/04/2012, 09:10
    At a linear collider, $e^+e^- \to t\bar{t}H$ will give a direct measurement of top-Higgs Yukawa coupling. We present here the prospect of such measurement in the context of International Linear Collider at $\sqrt{s}=1$ TeV as an extension to our previous work at $\sqrt{s}=500$ GeV. The study will be constructed for a Standard Model Higgs boson with a mass of 120 GeV using the semi-leptonic and...
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  118. Joe Conway (Cornell University)
    25/04/2012, 09:30
  119. Paolo Pierini (INFN Milano LASA)
    25/04/2012, 09:30
  120. Ryo Katayama (University of Tokyo)
    25/04/2012, 09:35
    We report on the full simulation study of measuring the O(1 eV) mass of the stable very light gravitino. Such a light gravitino typically appears in GMSB scenarios and is attractive from the point of view of cosmological constraints. Assuming NLSP stau of ~120 GeV mass and ~100 um/c lifetime, we simulate stau pair creation events at Ecm=500 GeV ILC with the ILD detector model. Tau decays are...
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  121. 25/04/2012, 10:30
  122. Frank Gaede (DESY), Dr Steve Aplin (DESY)
    25/04/2012, 10:30
  123. Taikan Suehara (ICEPP, The University of Tokyo)
    25/04/2012, 10:30
    In SM, Higgs self-coupling is responsible for the EWSB and mass generation. It is almost impossible to measure it at LHC for a light Higgs. It's a crucial task to make the Higgs self-coupling measurement be possible at the ILC 500. In this talk, we will present the latest study based on the full detector simulation.
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  124. Dr Yusuke Suetsugu (KEK)
    25/04/2012, 10:30
  125. Hitoshi Hayano (KEK)
    25/04/2012, 10:30
  126. Mr Tom Peterson (FNAL)
    25/04/2012, 10:35
  127. Dr Shigeki Fukuda (KEK)
    25/04/2012, 10:50
  128. Mikael Berggren (DESY)
    25/04/2012, 10:55
    Full and fast simulations studies of determination of sparticle masses and production cross-sections in SUSY scenarios with low mass differences is presented. Models that realise such spectra while respecting LHC limits, the LHC Higgs-hint as well as low energy and cosmological constrains are discussed.
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  129. Wei Gai (ANL)
    25/04/2012, 11:00
  130. 25/04/2012, 11:00
  131. daisuke kamai (tohoku university)
    25/04/2012, 11:10
  132. Dr Christopher Nantista (SLAC)
    25/04/2012, 11:10
  133. Seong Youl Choi (Chonbuk National University)
    25/04/2012, 11:20
    In this talk, I describe how to distinguish MSSM neutralinos from Dirac neutralinos by exploiting simple kinematic variables at various relevant processes available the ILC.
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  134. All
    25/04/2012, 11:20
  135. Akiya Miyamoto (KEK)
    25/04/2012, 11:30
  136. Mr John Carwardine (Argonne)
    25/04/2012, 11:30
  137. Monalisa Patra (Indian Institute of Science)
    25/04/2012, 11:45
    We study the possibility of fingerprinting a strongly interacting $W$ boson sector, consistent with present day LHC searches at the ILC with longitudinal as well as transversely polarized electron and positron beams. We account for the final state interaction using a suitable Omn\`es formalism in terms of a plausible resonance description, and carry out thorough analyses of cross sections,...
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  138. Dr Taikan SUEHARA (The University of Tokyo)
    25/04/2012, 11:50
  139. Hitoshi Hayano (KEK)
    25/04/2012, 11:50
  140. Chris Adolphsen (SLAC)
    25/04/2012, 14:00
  141. 25/04/2012, 14:00
  142. Dr Mark Palmer (Cornell University LEPP)
    25/04/2012, 14:00
  143. Eibun Senaha (KIAS)
    25/04/2012, 14:00
    The nondecoupling phenomena of the Higgs sector is essential for successful electroweak baryogenesis and its collider test. It is known that in the 2HDM, the strong first order phase transition can be realized by the nondecoupling loop effects of the heavy Higgs bosons, and its effects inevitably lead to a significant deviation of the triple Higgs boson coupling from the standard model value...
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  144. 25/04/2012, 14:00
  145. 25/04/2012, 14:00
  146. Yohei Kikuta (KEK)
    25/04/2012, 14:25
    The composite Higgs is one of the candidates for the beyond the SM and the Linear Collider experiments can reveal the composite nature of the Higgs. In this talk, I derive the general structure of dimension-six derivative interactions in the N Higgs doublet models, where Higgs fields arise as pseudo Nambu-Goldstone modes of a strongly interacting sector. As phenomenological processes, I show...
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  147. Dr Shigeki Fukuda (KEK)
    25/04/2012, 14:30
  148. Joe Conway (Cornell University), Dr Yulin Li (Cornell University)
    25/04/2012, 14:30
  149. 25/04/2012, 14:30
  150. 25/04/2012, 14:30
  151. Kei Yagyu (National Central University)
    25/04/2012, 14:50
    Higgs triplet fields are introduced in several new physics models beyond the SM such as the type II seesaw model, the left-right symmetric model and so on. Therefore, studying properties of the Higgs sector with triplet fields are important to clarify new physics models. In this talk, we focus on the Higgs triplet model, where Y=1 triplet field is added to the SM. We first discuss the...
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  152. Prof. Ken-ichi Kanazawa (KEK), Dr Yusuke Suetsugu (KEK)
    25/04/2012, 15:00
  153. Dr Christopher Nantista (SLAC)
    25/04/2012, 15:00
  154. Dr Mauro Pivi (SLAC)
    25/04/2012, 16:00
  155. 25/04/2012, 16:00
  156. Paul Grannis (State University of New York)
    25/04/2012, 16:00
    Following the shutdown of the Tevatron in 2011, the CDF and DZero experiments are analyzing the full data set, focusing on those measurements that are unique or that complement the LHC experiments. I will summarize recent results that bear on our understanding of QCD, heavy flavor states, and electroweak symmetry breaking.
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  157. Andrea Gaddi (CERN)
    25/04/2012, 16:00
    MDI
  158. Dr Tamaki Yoshioka (ICEPP, Univ. of Tokyo)
    25/04/2012, 16:00
  159. Hubert Gerwig (CERN)
    25/04/2012, 16:20
    MDI
  160. Poeschl Roman
    25/04/2012, 16:20
  161. 25/04/2012, 16:30
  162. G. Orukawa, Dr Yasuhiro Sugimoto (KEK)
    25/04/2012, 16:40
    MDI
  163. Takehiro Nabeshima (University of Toyama)
    25/04/2012, 16:40
    I would like to talk about the TeV-scale seesaw model in which U(1)_{B-L} gauge symmetry can be the common origin of neutrino masses, the dark matter mass, and stability of the dark matter. In our model, Majorana masses of right handed neutrinos and Dirac mass of dark matter are induced by spontaneous U(1)_{B-L} breaking. After electroweak symmetry breaking, light neutrino masses are generated...
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  164. Kou Ohishi (Kyushu U.)
    25/04/2012, 16:40
  165. T. Okamura, Y. Makita
    25/04/2012, 17:00
    MDI
  166. Katsushige Kotera (Shinshu University, Faculty of Science,)
    25/04/2012, 17:00
  167. Oscar Stal (DESY)
    25/04/2012, 17:05
    In light of the recent hints from the LHC for a positive Higgs signal around 125 GeV, we discuss the possible interpretations of such a scenario in supersymmetry. We derive constraints on the parameters of the minimal supersymmetric extension of the SM, and discuss phenomenological implications for this model at the LHC and the ILC.
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  168. Mr Victor Kuchler (Fermilab)
    25/04/2012, 17:20
    MDI
  169. Katsushige Kotera (Shinshu University, Faculty of Science,)
    25/04/2012, 17:20
  170. 25/04/2012, 17:30
  171. Benedikt Vormwald (DESY)
    25/04/2012, 17:30
    Supersymmetric models with R-parity violation (RPV) offer a broad range of interesting phenomenologies that can differ from R-parity conserving SUSY, depending of the strength of the breaking. The most important consequence of RPV is that the lightest supersymmetric particle is no longer stable and can decay into Standard Model particles. This makes RPV SUSY much harder to test at the LHC. In...
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  172. Prof. Jae Yu
    25/04/2012, 17:40
  173. 25/04/2012, 17:40
    MDI
  174. Prof. Junji Urakawa (KEK)
    26/04/2012, 08:30
  175. Prof. Akira Yamamoto (KEK)
    26/04/2012, 08:30
  176. Dr Yasuhiro Sugimoto (KEK)
    26/04/2012, 08:30
    ILD
  177. 26/04/2012, 08:30
  178. Susanna Guiducci (INFN-LNF)
    26/04/2012, 08:30
  179. Tomohiko Tanabe (University of Tokyo)
    26/04/2012, 08:40
    ILD
  180. Akiya Miyamoto (KEK)
    26/04/2012, 08:50
    ILD
  181. Mr Hiroaki Ono (Nippon Dental University)
    26/04/2012, 09:00
    ILD
  182. 26/04/2012, 09:00
  183. Tomohiko Tanabe (University of Tokyo)
    26/04/2012, 09:10
    ILD
  184. Mikael Berggren (DESY Hamburg)
    26/04/2012, 09:20
    ILD
  185. Roman Poeschl (LAL Orsay)
    26/04/2012, 09:30
    ILD
  186. Dr Taikan SUEHARA (The University of Tokyo)
    26/04/2012, 09:40
    ILD
  187. 26/04/2012, 09:50
    ILD
  188. Prof. Akira Yamamoto (KEK)
    26/04/2012, 10:30
  189. 26/04/2012, 10:30
  190. Dr Karsten Buesser (DESY)
    26/04/2012, 10:30
    ILD
  191. 26/04/2012, 10:30
  192. Frank Gaede (DESY)
    26/04/2012, 11:00
    ILD
  193. 26/04/2012, 11:30
    ILD
  194. 26/04/2012, 11:30
  195. 26/04/2012, 11:30
  196. Gerald Dugan (Cornell University)
    26/04/2012, 14:00
  197. Dr Shinya Kanemura (University of Toyama)
    26/04/2012, 14:00
  198. Dr Toshiaki Tauchi (KEK)
    26/04/2012, 14:20
  199. Mr John Carwardine (Argonne)
    26/04/2012, 14:25
  200. Su Yong Choi (Sungkyunkwan Univ., Dept. of Phys.-Unknown-Unknown)
    26/04/2012, 14:37
  201. 26/04/2012, 14:50
  202. Dr Tamaki Yoshioka (ICEPP, Univ. of Tokyo)
    26/04/2012, 14:54
  203. Norman Graf (SLAC)
    26/04/2012, 15:11
  204. Donchul Son
    26/04/2012, 16:00
  205. Min Zhang, Rika Takahashi
    26/04/2012, 16:20
  206. Akiya Miyamoto
    26/04/2012, 16:40
  207. Akira Yamamoto
    26/04/2012, 17:10
  208. Namkung Won
    26/04/2012, 17:40
  209. Dr Christopher Nantista (SLAC)
  210. Dr Shigeki Fukuda (KEK)
  211. Dr Glen White (SLAC)
  212. Wei Gai (ANL)
  213. Joint session with WG3: Main Linac
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  214. Hitoshi Hayano (KEK)