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Flavour in the era of the LHC, 4th meeting

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

Contribution List

83 / 83
42. News on SuperKEKB physics reach
Masashi Hazumi (KEK)
09/10/2006, 09:00
1. Welcome/review of the Report plans for EDM/g-2
Dr Yannis Semertzidis (BNL)
09/10/2006, 09:00
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...
43. linear super B update
Francesco Forti (Pisa)
09/10/2006, 09:30
44. LHCb Upgrade
Franz Muheim (Edinburgh)
09/10/2006, 10:00
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.
45. New physics signals using exclusive radiative B-decays
Amarjit Soni (BNL)
09/10/2006, 10:30
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...
48. B-> K* gamma TDCP asymmetry: (quasi) null test for SM
Roman Zwicky (Durham IPPP)
09/10/2006, 11:30
46. Discovery potential for Bs->mu+mu- in CMS
Christina Eggel (ETH Zurich)
09/10/2006, 12:00
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.
47. Search for the decay Bs-> mu+ mu- at LHCb
Frederic Teubert (CERN)
09/10/2006, 12:30
49. B_s,d -> KK using QCD Factorization and flavour symmetries
Sebastien Descotes-Genon (LPT Orsay)
09/10/2006, 14:00
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.
82. short introduction
conveners
09/10/2006, 14:00
28. CMS discovery potential for SUSY topologies
Maria Spiropulu
09/10/2006, 14:05
50. Higher order QCD in exclusive B decays
Guido Bell (LMU Munich)
09/10/2006, 14:30
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
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.
75. Neutralino spin measurement with ATLAS
Dr Andrea Ventura (INFN Lecce)
09/10/2006, 14:55
51. Update on charm results
David Asner (Carleton)
09/10/2006, 15:00
7. Polarimetry for the dEDM method
G. Venanzoni (Frascati)
09/10/2006, 15:25
52. Charm physics at LHCb
Patrick Spradlin (Oxford)
09/10/2006, 15:30
80. New Physics in b->sl+l-
Christoph Bobeth (Dortmund)
09/10/2006, 16:00
8. EDM of Proton and 3He
W. Morse (BNL)
09/10/2006, 16:10
53. Convenors and study group contacts: Write-up matters
09/10/2006, 16:30
72. WG1, convener meeting
09/10/2006, 16:30
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
21. Spin and beam dynamics simulations
A. Luccio (BNL)
09/10/2006, 17:30
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...
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...
54. B-> K*ll and extra dimensions
Fulvia De Fazio (INFN Bari)
10/10/2006, 09:00
55. Charm resonances in b-> sll
Alexander Khodjamirian (Siegen)
10/10/2006, 09:30
30. Lepton flavour violation in neutralino decays
Ian Hinchliffe
10/10/2006, 09:30
12. Theory of molecular EDM experiments
M. Kozlov (St. Petersburg)
10/10/2006, 09:50
56. B-> K*ll at LHCb
Dr Ulrik Egede (Imperial College London)
10/10/2006, 10:00
77. Large Electroweak Logarithms in Heavy Quark Decay at LHC
Alessia Gruzza
10/10/2006, 10:00
13. EDM experiments as probes of SUSY
Isabella Masina (Rome)
10/10/2006, 10:20
57. B -> K*ll and B+-> tau nu from Belle
Stefano Villa (Lausanne)
10/10/2006, 10:30
32. The relevance of electroweak effects in the overall t-channel single top production at LHC
Claudio Verzegnassi
10/10/2006, 10:30
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.
58. CKM angles from Babar
Luca Cavoto (Rome)
10/10/2006, 11:30
33. Contributions from dimension five and six effective operators to flavour changing top physics
Pedro Miguel Martins Ferreira
10/10/2006, 11:30
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...
59. ICPV results from Belle
Masashi Hazumi (KEK)
10/10/2006, 12:00
71. Wtb Anomalous Top Quark Couplings
Antonio Onofre
10/10/2006, 12:00
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...
76. FCNC top decays
Leonardo Benucci
10/10/2006, 12:25
60. B-> h+h- at LHCb
Alessio Sarti (LNF -INFN)
10/10/2006, 12:30
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...
24. Leptogenesis and LFV in type I+II seesaw mechanism
Stephane Lavignac (SPhT Saclay)
10/10/2006, 14:00
34. Lepton mumber violation with muons at LHC
Francisco del Aguila
10/10/2006, 14:00
61. Rare Hadronic b->s and b->d transitions (BaBar)
Adrian Bevan (QMUL)
10/10/2006, 14:00
62. A_SL, DeltaGamma_s, phi_s
Sergey Burdin (Fermilab)
10/10/2006, 14:30
25. Lepton Flavor Violation, Leptogenesis and Neutrino Mixing in QLC scenarios
Werner Rodejohann (TU Muenchen)
10/10/2006, 14:30
35. Signals of new fermions at high transverse momenta
Juan Antonio Aguilar-Saavedra
10/10/2006, 14:30
36. Detection of heavy Majorana neutrinos and right-handed bosons
Mikhail Kirsanov
10/10/2006, 15:00
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...
63. Study of the decay B_s->J/psi phi with the CMS detector
Lotte Wilke (Uni Zuerich)
10/10/2006, 15:00
64. Missing particle reconstruction using vertexing
Andrey Starodumov (ETH Zuerich)
10/10/2006, 15:30
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.
83. Rare B-decay backgrounds studies - update
Nicolai Nikitine (Moscow)
10/10/2006, 15:50
19. New Measurement of the Electron Magnetic Moment and the Fine Structure Constant
Gerald Gabrielse (Harvard)
10/10/2006, 16:30
65. Tools (where we are)
Sven Heinemeyer (IFCA (CSIC-UC))
10/10/2006, 16:30
66. Flavor benchmarks
Sven Heinemeyer (IFCA (CSIC-UC))
10/10/2006, 16:50
78. CMS benchmark analysis
Michael Schmitt (University of Florida)
10/10/2006, 17:10
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.
67. Discussion
10/10/2006, 17:30
68. Convenors and study group contacts: Write-up matters
11/10/2006, 09:00
37. E6 and the HIggs boson
Gokhan Unel
11/10/2006, 09:00
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...
38. Multi-W events at the LHC
Geraldine Servant
11/10/2006, 09:30
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.
39. 4th family physics
Erkcan Ozcan
11/10/2006, 10:00
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 -...
40. Determination of the D-d mixing angle
Gokhan Unel
11/10/2006, 10:30
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).
41. CMS discovery potential for Z'/ED and spin discrimination
Barbara Clerbaux
11/10/2006, 11:30
70. Discussion of the Yellow Book contribution
11/10/2006, 11:30
81. WG progress reports
11/10/2006, 14:00
73. Summary of the EDM and g-2 miniworkshop
Dr Yannis Semertzidis (BNL)
11/10/2006, 15:00
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.
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...

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