'Lfv' diaporamas de présentation

Observations on Lepton Flavor Violation Experiments

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?- LFV and related topics

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Shinya Kanemura (Osaka Univ.) on behalf of

Search for LFV (tau-mu and tau-e) via DIS processes with high energy intense muons and electrons. Shinya Kanemura (Osaka Univ.) on behalf of. S.K., Y. Kuno, T. Ota, M. Kuze. PLB607(2005)165. S.K., Y. Kuno, T. Ota, M. Kuze, T. Takai. Work in progress.

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Anna Rossi ( Padova University )

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Search for tau-e (tau-mu) flavor mixing at a future collider

Search for tau-e (tau-mu) flavor mixing at a future collider. Shinya KANEMURA (Osaka Univ.) with. Yoshitaka KUNO, Toshihiko OTA (Osaka Univ.) Masahiro Kuze (Tokyo Inst. Tech.). CP ????????????????? Jan 12-14. 2005. Contents. Introduction

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Search for in muonic atom at COMET experiment

Search for in muonic atom at COMET experiment. m. e. e. e. Masato Yamanaka (ICRR, Univ. of Tokyo). Masafumi Koike (Saitama Univ.) Yoshitaka Kuno (Osaka Univ.) Joe Sato (Saitama Univ. ). Collaborators. Introduction. Introduction. In Standard Model (SM).

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Search for Lepton Flavor Violation at the ILC

Search for Lepton Flavor Violation at the ILC. Shinya Kanemura (Osaka Univ.). 8th ACFA LC Workshop ? Taegue, Korea, July 11-14. 2005. Contents. Introduction Lepton Flavor Violation (LFV) LFV in SUSY Gauge boson mediation & Higgs boson mediation LFV search at a LC LFV in LFV in

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Search for tau-e (tau-mu) flavor mixing at a linear collider

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Search for lepton flavor violating ? ?? ? ?? reaction with high energy muons

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Search for L epton F lavor V iolation in the m + N -> t + N conversion (preliminary)

Search for L epton F lavor V iolation in the m + N -> t + N conversion (preliminary). S.N. Gninenko INR, Moscow. SPSC meeting, Villars, September 22-28, 2004. Outline. Introduction m +N-> t +N conversion Choice of signature Experimental setup

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CONTENT Standard model does not permit LFV Most common introduction of neutrino masses

Lepton flavour violation (tau decays) A.Ilakovac, Dept. of Physics, Faculty of Science, U. of Zagreb, Croatia. CONTENT Standard model does not permit LFV Most common introduction of neutrino masses Sources of LFV/LNV Model-independent (operator) analysis of LFV with SM fields LFV mechanisms

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Lepton Flavor Violation

Lepton Flavor Violation. Yasuhiro Okada (KEK) October 7, 2005 3 rd International Conference on Flavor Physics National Central University, Taiwan. Lepton Flavor Violation in charged lepton processes. Charged lepton LFV is a clear evidence of physics beyond the Standard Model.

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Search for lepton flavor violation via the intense high-energy muon beam

Search for lepton flavor violation via the intense high-energy muon beam. Shinya KANEMURA (Osaka Univ.) with. Yoshitaka KUNO, Masahiro KUZE, Toshihiko OTA. Nufact 2004, July 28, Osaka Univ., Osaka, JAPAN. Contents. Introduction LFV Experimental bounds Gauge mediation and Higgs mediation

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Maurice Blackmon Symposium October 29, 2007

Maurice Blackmon Symposium October 29, 2007. Intraseasonal Low-Frequency Variability: At the Interface Between Weather and Climate Randall M. Dole NOAA Earth System Research Laboratory Physical Sciences Division. Maurice (shortly after leaving NOAA). Meeting Maurice.

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Low Frequency Atmospheric Variability in GFS Models

Low Frequency Atmospheric Variability in GFS Models. Peitao Peng Acknowledgment: Bhaskar, Arun and Huug. Purposes. The performance of GFS models in simulating the low frequency variability (LFV) of the atmosphere; Differences between the two versions of GFS models in LFV;

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Low Frequency Atmospheric Variability in GFS Models

Low Frequency Atmospheric Variability in GFS Models. Peitao Peng Acknowledgment: Bhaskar, Arun and Huug. Purposes. The performance of GFS models in simulating the low frequency variability (LFV) of the atmosphere; Differences between the two versions of GFS models in LFV;

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6/26/09

6/26/09. First Attempt. 8/13/09. mSUGRA base point (modified from the 0802.2968 paper) m 0 =250 GeV ; m 1/2 =350 GeV ; tan b =40 ; A 0 =0 ; m >0 Ngen = 200,000 events 1) M( c 2 0 ) - M( c 1 0 ) ? M( tt ) endpoint ~ 124 GeV for the 2) M( t 1 +/- ) - M( c 1 0 ) ~ 49 GeV .

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