Go to the Indico Home Page Oldest event Older event Up to category Newer event Newest event
 
Focus on:  Hide Contributions
  • Compact style
  • Indico style
  • Indico style - inline minutes
  • Indico style - numbered
  • Indico style - numbered + minutes
  • Indico Weeks View
    • Switch to the management area of this event
    Login

    Flavour in the era of the LHC, 4th meeting

    9โ€“11 Oct 2006
    CERN
    Europe/Zurich timezone

    Contribution List

    83 out of 83 displayed
    Export to PDF
    1. 42. News on SuperKEKB physics reach
      Masashi Hazumi (KEK)
      09/10/2006, 09:00
    2. 1. Welcome/review of the Report plans for EDM/g-2
      Dr Yannis Semertzidis (BNL)
      09/10/2006, 09:00
    3. 0. The history of the neutron EDM
      Norman Ramsey (Harvard)
      09/10/2006, 09:15
      Before 1950 all theorists believed P (parity symmetry) and that there consequently could be no EDM for any elementary particle. Ramsey and Purcell [PR 78, 807 (1950)] pointed out that there was no experimental evidence for P in the case of nuclear forces so it should be tested. They proposed a search for a neutron EDM or dn, as a test of P. The 1953 neutron beam experiment at...
      Go to contribution page
    4. 43. linear super B update
      Francesco Forti (Pisa)
      09/10/2006, 09:30
    5. 44. LHCb Upgrade
      Franz Muheim (Edinburgh)
      09/10/2006, 10:00
    6. 2. Electric Dipole Moments as probes of new physics
      Adam Ritz (Victoria/Canada)
      09/10/2006, 10:05
      A review of the effective theory treatment of CP-odd operators contributing to EDMs, and the ensuing sensitivity to new CP-violating physics. As examples, new dimension-five operators in the MSSM, and a new Higgs-sector threshold allowing for electroweak baryogenesis, will be discussed.
      Go to contribution page
    7. 45. New physics signals using exclusive radiative B-decays
      Amarjit Soni (BNL)
      09/10/2006, 10:30
    8. 3. Review of the neutron EDMs (ILL and SNS)
      P. Harris (Sussex)
      09/10/2006, 11:15
      This talk will review three neutron EDM experiments: First, the room-temperature experiment at ILL, the results of which have just been published; second, the CryoEDM experiment at ILL that is now nearing the completion of its construction, and which promises an improvement in sensitivity of two orders of magnitude; and third, for the longer term, the cryogenic experiment that is...
      Go to contribution page
    9. 48. B-> K* gamma TDCP asymmetry: (quasi) null test for SM
      Roman Zwicky (Durham IPPP)
      09/10/2006, 11:30
    10. 46. Discovery potential for Bs->mu+mu- in CMS
      Christina Eggel (ETH Zurich)
      09/10/2006, 12:00
    11. 4. The neutron experiment at PSI plus the muon EDM prospects
      K. Kirch (PSI)
      09/10/2006, 12:10
      Status and plans for the neutron EDM experiment at PSI are updated. The idea for a compact muon EDM experiment with a sensitivity of 5x10^(-23) e-cm will be briefly discussed.
      Go to contribution page
    12. 47. Search for the decay Bs-> mu+ mu- at LHCb
      Frederic Teubert (CERN)
      09/10/2006, 12:30
    13. 49. B_s,d -> KK using QCD Factorization and flavour symmetries
      Sebastien Descotes-Genon (LPT Orsay)
      09/10/2006, 14:00
    14. 5. How to measure g-2 with 15 GeV muons
      F. Farley (Yale)
      09/10/2006, 14:00
      Dilating the muon lifetime to 300 microsec can lead to ten times better accuracy. This can be achieved with a new design of storage ring using discrete magnets and calibrating the field by means of polarised protons in flight.
      Go to contribution page
    15. 82. short introduction
      conveners
      09/10/2006, 14:00
    16. 28. CMS discovery potential for SUSY topologies
      Maria Spiropulu
      09/10/2006, 14:05
    17. 50. Higher order QCD in exclusive B decays
      Guido Bell (LMU Munich)
      09/10/2006, 14:30
    18. 29. Using the e^+- mu^-+ + E_Tmiss signature in the search for supersymmetry and lepton flavour violation in neutralino decays
      Nikolai Krasnikov
      09/10/2006, 14:30
    19. 6. The deuteron EDM experiment
      G. Onderwater (KVI)
      09/10/2006, 14:35
      A theoretical motivation for an EDM search on the deuteron will be presented, together with the so-called resonance method. The basic features of this method will be discussed in some detail.
      Go to contribution page
    20. 75. Neutralino spin measurement with ATLAS
      Dr Andrea Ventura (INFN Lecce)
      09/10/2006, 14:55
    21. 51. Update on charm results
      David Asner (Carleton)
      09/10/2006, 15:00
    22. 7. Polarimetry for the dEDM method
      G. Venanzoni (Frascati)
      09/10/2006, 15:25
    23. 52. Charm physics at LHCb
      Patrick Spradlin (Oxford)
      09/10/2006, 15:30
    24. 80. New Physics in b->sl+l-
      Christoph Bobeth (Dortmund)
      09/10/2006, 16:00
    25. 8. EDM of Proton and 3He
      W. Morse (BNL)
      09/10/2006, 16:10
    26. 53. Convenors and study group contacts: Write-up matters
      09/10/2006, 16:30
    27. 72. WG1, convener meeting
      09/10/2006, 16:30
    28. 9. A plan of comprehensive investigation of systematic errors and spin coherence time for the deuteron resonance EDM experiment
      Y. Orlov (Cornell)
      09/10/2006, 16:35
    29. 21. Spin and beam dynamics simulations
      A. Luccio (BNL)
      09/10/2006, 17:30
    30. 10. EDM searches on atoms with deformed nuclei: Ra-225
      J.R. Guest (Argonne)
      09/10/2006, 17:45
      Nuclei which are characterized by octupole deformation should have relatively large Schiff moments and therefore be particularly sensitive to T-violating interactions in the nucleus. Currently, the most stringent limits in this sector are set by measurements made at the University of Washington, which restrict the atomic EDM of Hg-199 to <2.1x10^{-28} e cm. We are developing an...
      Go to contribution page
    31. 11. (Cancelled, M. Kozlov covered some of the material) Overview of the electron EDM experiments
      N. Shafer-Ray (Oklahoma Univ.)
      10/10/2006, 09:00
      The experiment responsible for the current limit on the electron's electric dipole moment is described. A very brief overview of the many current efforts to push this limit is presented. Efforts underway at the University of Oklahoma to exploit the unique magnetic properties of PbF are described with a particular emphasis on the development of new resonant enhanced multiphoton...
      Go to contribution page
    32. 54. B-> K*ll and extra dimensions
      Fulvia De Fazio (INFN Bari)
      10/10/2006, 09:00
    33. 55. Charm resonances in b-> sll
      Alexander Khodjamirian (Siegen)
      10/10/2006, 09:30
    34. 30. Lepton flavour violation in neutralino decays
      Ian Hinchliffe
      10/10/2006, 09:30
    35. 12. Theory of molecular EDM experiments
      M. Kozlov (St. Petersburg)
      10/10/2006, 09:50
    36. 56. B-> K*ll at LHCb
      Dr Ulrik Egede (Imperial College London)
      10/10/2006, 10:00
    37. 77. Large Electroweak Logarithms in Heavy Quark Decay at LHC
      Alessia Gruzza
      10/10/2006, 10:00
    38. 13. EDM experiments as probes of SUSY
      Isabella Masina (Rome)
      10/10/2006, 10:20
    39. 57. B -> K*ll and B+-> tau nu from Belle
      Stefano Villa (Lausanne)
      10/10/2006, 10:30
    40. 32. The relevance of electroweak effects in the overall t-channel single top production at LHC
      Claudio Verzegnassi
      10/10/2006, 10:30
    41. 14. Measuring the Muon Anomaly to 0.25 ppm
      J. Miller (Boston)
      10/10/2006, 11:00
      A proposal has been approved at the BNL AGS to improve upon the muon magnetic anomaly measurement uncertainty by a factor of two, to 0.25 ppm. The current experimental value differs from the theoretical value by about 3 standard deviations. This suggests the possibility of new physics, and an increased data set could make the comparison between theory and experiment more definitive.
      Go to contribution page
    42. 58. CKM angles from Babar
      Luca Cavoto (Rome)
      10/10/2006, 11:30
    43. 33. Contributions from dimension five and six effective operators to flavour changing top physics
      Pedro Miguel Martins Ferreira
      10/10/2006, 11:30
    44. 15. Evaluation of the hadronic vacuum polarization contribution to the muon g-2
      Andreas Hoecker (CERN)
      10/10/2006, 11:40
      The contribution from hadronic vacuum polarization to the muon anomalous magnetic moment is calculated with a dispersion relation using experimental data and perturbative QCD as input. Its uncertainty is presently limiting the Standard Model prediction, and is of the same order as the experimental error on g-2. The state of the art of the calculation is discussed and perpectives...
      Go to contribution page
    45. 59. ICPV results from Belle
      Masashi Hazumi (KEK)
      10/10/2006, 12:00
    46. 71. Wtb Anomalous Top Quark Couplings
      Antonio Onofre
      10/10/2006, 12:00
    47. 16. Hadrons at VEPP-2M
      S. Redin (Novosibirsk)
      10/10/2006, 12:15
      The Budker Institute (Novosibirsk, Russia) is mostly dedicated to physics in $e^+ e^-$ colliders at relatively low energy. The VEPP-2M collider operated in 1992- 2000 at s = 0.36 to 1.4 GeV region and provided high luminosity for detectors CMD-2 and SND. High level of collected statistics as well as careful design, construction and operation of the detectors, and data...
      Go to contribution page
    48. 76. FCNC top decays
      Leonardo Benucci
      10/10/2006, 12:25
    49. 60. B-> h+h- at LHCb
      Alessio Sarti (LNF -INFN)
      10/10/2006, 12:30
    50. 17. e+e- Hadronic Cross Section measurement at DAFNE with the KLOE detector
      Debora Leone (Karlsruhe)
      10/10/2006, 12:40
      At the Frascati phi-factory DAFNE the pion form factor is measured by means of the "radiative return", i.e. by using events in which one of the collider electrons (positrons) has radiated an initial state radiation photon (ISR), lowering in such a way the invariant mass M(pi pi) of the two-pion-system. In a recent publication of the KLOE collaboration the initial state radiation...
      Go to contribution page
    51. 24. Leptogenesis and LFV in type I+II seesaw mechanism
      Stephane Lavignac (SPhT Saclay)
      10/10/2006, 14:00
    52. 34. Lepton mumber violation with muons at LHC
      Francisco del Aguila
      10/10/2006, 14:00
    53. 61. Rare Hadronic b->s and b->d transitions (BaBar)
      Adrian Bevan (QMUL)
      10/10/2006, 14:00
    54. 62. A_SL, DeltaGamma_s, phi_s
      Sergey Burdin (Fermilab)
      10/10/2006, 14:30
    55. 25. Lepton Flavor Violation, Leptogenesis and Neutrino Mixing in QLC scenarios
      Werner Rodejohann (TU Muenchen)
      10/10/2006, 14:30
    56. 35. Signals of new fermions at high transverse momenta
      Juan Antonio Aguilar-Saavedra
      10/10/2006, 14:30
    57. 36. Detection of heavy Majorana neutrinos and right-handed bosons
      Mikhail Kirsanov
      10/10/2006, 15:00
    58. 26. Flavour violation in ``minimal'' SUSY SU(5) models
      Toshifumi Yamashita (S.I.S.S.A.)
      10/10/2006, 15:00
      We compare the patterns of the flavor violating effects which are radiatively induced via the neutrino Yukawa couplings in "minimal" SU(5) models with the Type I or Type II seesaw mechanism for the neutrino masses. We pay special attention to the ratio between the lepton flavor violations and the quark flavor violations, and especially to its dependence on the UV physics, such as the GUT...
      Go to contribution page
    59. 63. Study of the decay B_s->J/psi phi with the CMS detector
      Lotte Wilke (Uni Zuerich)
      10/10/2006, 15:00
    60. 64. Missing particle reconstruction using vertexing
      Andrey Starodumov (ETH Zuerich)
      10/10/2006, 15:30
    61. 27. Unitarity in the leptonic sector
      Carla Biggio (Madrid)
      10/10/2006, 15:30
      We determine the leptonic mixing matrix elements without assuming unitarity. To do this, we firstly develop the formalism to study neutrino oscillations and then we perform the fits. We realize that oscillation experiments alone are not enough to constrain all the matrix elements. However, by combining them with other electroweak data, we can determine all of them.
      Go to contribution page
    62. 83. Rare B-decay backgrounds studies - update
      Nicolai Nikitine (Moscow)
      10/10/2006, 15:50
    63. 19. New Measurement of the Electron Magnetic Moment and the Fine Structure Constant
      Gerald Gabrielse (Harvard)
      10/10/2006, 16:30
    64. 65. Tools (where we are)
      Sven Heinemeyer (IFCA (CSIC-UC))
      10/10/2006, 16:30
    65. 66. Flavor benchmarks
      Sven Heinemeyer (IFCA (CSIC-UC))
      10/10/2006, 16:50
    66. 78. CMS benchmark analysis
      Michael Schmitt (University of Florida)
      10/10/2006, 17:10
    67. 20. More on EDM correlations in SUSY
      Oleg Lebedev (Bonn)
      10/10/2006, 17:20
      Certain relations among EDMs can be viewed as indirect evidence for supersymmetry. I will report on recent work on EDM correlations which includes analyses of non-universal SUSY models.
      Go to contribution page
    68. 67. Discussion
      10/10/2006, 17:30
    69. 68. Convenors and study group contacts: Write-up matters
      11/10/2006, 09:00
    70. 37. E6 and the HIggs boson
      Gokhan Unel
      11/10/2006, 09:00
    71. 22. Prospects for a Muon to Electron Conversion Experiment at Fermilab
      Jim Miller (Boston)
      11/10/2006, 09:00
      It is proposed to measure the rate of coherent muon to electron conversion in the field of a nucleus, without neutrino production, to a precision of 10^{-16} times the rate of ordinary muon capture on the nucleus. This is an example of charged lepton flavor violation. The measurement would be several thousand times more sensitive than previous experiments. A working group has been formed...
      Go to contribution page
    72. 38. Multi-W events at the LHC
      Geraldine Servant
      11/10/2006, 09:30
    73. 23. Search for B -> mu + e with LHCb
      Walter Bonivento (I.N.F.N. Cagliari, Italy)
      11/10/2006, 09:30
      We discuss the LHCb potential for the LFV B->e mu decay and the possibility of constraining the leptoquark mass within the context of the Pati-Salam SU(4) model.
      Go to contribution page
    74. 39. 4th family physics
      Erkcan Ozcan
      11/10/2006, 10:00
    75. 69. How can CP phases contribute to LFV processes ?
      Dr Tetsuo Shindou (SISSA)
      11/10/2006, 10:00
      We discuss the dependence of the rates of LFV processes mu -> e + gamma, tau -> e + gamma, tau -> mu + gamma (l_i -> l_j + gamma) and their ratios in MSSM with right-handed neutrinos on CP phases. We focus on the case of quasi-degenerate in mass heavy Majorana neutrinos. The three types of light neutrino mass spectrum - normal hierarchical, inverted hierarchical and quasi-degenerate -...
      Go to contribution page
    76. 40. Determination of the D-d mixing angle
      Gokhan Unel
      11/10/2006, 10:30
    77. 74. Neutrino Masses and Mixing in Split Supersymmetry
      Dr Marco Aurelio Diaz (Universidad Catolica de Chile)
      11/10/2006, 10:30
      We analyze the possibility of generating masses and mixing angles to neutrinos via bilinear R-Parity and lepton number violation alone (not trilinear).
      Go to contribution page
    78. 41. CMS discovery potential for Z'/ED and spin discrimination
      Barbara Clerbaux
      11/10/2006, 11:30
    79. 70. Discussion of the Yellow Book contribution
      11/10/2006, 11:30
    80. 81. WG progress reports
      11/10/2006, 14:00
    81. 73. Summary of the EDM and g-2 miniworkshop
      Dr Yannis Semertzidis (BNL)
      11/10/2006, 15:00
    82. 79. Bs -> Xs gamma at NNLO
      Mikolaj Misiak (Warsaw)
      11/10/2006, 15:30
      The B -> Xs gamma branching ratio estimate at the next-to-next-to-leading order in QCD is discussed. Constrains on certain beyond-SM effects are updated.
      Go to contribution page
    83. 18. Contributions of Magnetic Resonance to Other Sciences
      Norman Ramsey (Harvard University)
      11/10/2006, 16:30
      One of the attractive features of fundamental research is the frequency with which new methods or discoveries in one narrow field of research eventually often make very important contributions to other fields. This has been conspicuously true of magnetic resonance, with which I have been associated ever since I.I. Rabi invented and demonstrated the method for the important but...
      Go to contribution page

    Back to the event