'0 nn' diaporamas de présentation

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The physics of higher Intensity PS or SPS Kaons, Muons, Neutrinos

The physics of higher Intensity PS or SPS Kaons, Muons, Neutrinos. Augusto Ceccucci/CERN May 26, 2004 Workshop on Physics with a Multi-MW proton source. Framework. Short to medium term scenario: Current PS and SPS Intensity increase always welcome (x 1.5 ?)

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Future rare kaon decays experiments

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Rare Kaon Decays at the CERN SPS

Rare Kaon Decays at the CERN SPS. NA48-Future Working Group CERN-SPSC-2004-010 SPSC-EOI-002. NA48/1 Phase III Neutral hyperons (2006) NA48/3 K + ? p + n n EOI for Villars NA48/4 K L ? p 0 ee ( mm ) NA48/5 K L ? p 0 n n. CERN-SPSC-2004-010.

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Physics Requirements for the ILC Vertex Tracker

Physics Requirements for the ILC Vertex Tracker. Marco Battaglia UC Berkeley and LBNL. WWS ILC Vertex Tracker Review October 22, 2007. Physics Scenarios for the ILC Vertex Tracker. Test the SM through precision study of the Higgs boson profile;.

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Rare Kaon Decays Review and Prospects

Rare Kaon Decays Review and Prospects. Augusto Ceccucci/CERN Physics State of the Art Prospects. s. d. XL th Rencontres de Moriond, EW Interactions and Unified Theories. n. n. Motivations. Search for explicit violation of Standard Model Lepton Flavour Violation (LFV)

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Kyoto University H. Nanjo for E391a and K O TO collaboration

Kyoto University H. Nanjo for E391a and K O TO collaboration. Collaboration. KEK-PS E391a The first dedicated experiment for K L ? p 0 nn . J-PARC E14 to measure Br(K L ? p 0 nn ) at J-PARC K O TO (K0 at Tokai) Japan-USA-Russia-Taiwan-Korea 5 countries and 15 institutes.

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Current and Future Kaon Experiments CKM-2012, Cincinnati , OH. R. Tschirhart Fermilab

Current and Future Kaon Experiments CKM-2012, Cincinnati , OH. R. Tschirhart Fermilab. Photo: H. Hayano, KEK. Sensitivity Frontier of Kaon Physics Today: Parts per Trillion. CERN NA62: 100 x 10 -12 measurement sensitivity of K + g e + n

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Probing New Physics with ORKA

Probing New Physics with ORKA. Elizabeth Worcester (BNL) for the ORKA collaboration Snowmass on the Mississippi August 2 , 2013. Photo: Life of Sea blogspot. ORKA: The Golden Kaon Experiment. Precision measurement of K + ? p + nn BR with ~1000 expected events at FNAL MI

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The Data Acquisition System for the K0TO Detector

The Data Acquisition System for the K0TO Detector. Monica Tecchio University of Michigan on behalf of Myron Campbell, Shumin Li, Craig Harabedian , Jon Ameel University of Michigan Jiasen Ma, Yau Wah , Mircea Bogdan University of Chicago Joe Comfort, Duncan McFarland

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Future of Kaon Physics Augusto Ceccucci/CERN

Future of Kaon Physics Augusto Ceccucci/CERN. CERN-SPS Rare K decays LFV Chiral dynamics. Frequent K decays. U-70. J-PARC L X hypernuclei K Rare Decay. F factory Hadron xsec K S decays N ff. CKM Unitarity and Rare Kaon Decays.

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CP Violation Brazilian Physical Society Particles and Fields Meeting Caxambu, 10-14 August 1998

CP Violation Brazilian Physical Society Particles and Fields Meeting Caxambu, 10-14 August 1998 Tatsuya Nakada CERN * Geneva, Switzerland * On leave from Paul Scherrer Institute. I) Why CP violation is highly interesting?

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Working Group 3 Summary: V td , V ts , and Friends

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FUTURE OF KAON PHYSICS AT CERN

FUTURE OF KAON PHYSICS AT CERN. Future Kaon Initiatives. CERN-SPS Rare K decays LFV Chiral dynamics. Frequent K decays. U-70. J-PARC L X hypernuclei K Rare Decay. F factory Hadron xsec K S decays, interferometry. K → p nn : SM Theoretical Prediction. NLO Calculation:

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K L ? p 0 nn experiment at J-PARC

K L ? p 0 nn experiment at J-PARC. Mitsuhiro YAMAGA Osaka Univ. Oct. 7, 2004 Workshop on Physics at an Upgraded Fermilab Proton Driver. Contents: Introduction J-PARC K L ? p 0 nn experiment KEK PS-E391a At Proton Driver.

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?????? ?????????? ?????? ?????-??????, 12-13 ??? 2004 ?. ?????? ??????? ??????. ?.?. ???????. ???????? ??????? ???????????? ???. CKM ??????? : K ? pnn ? B ??????? K L ? p 0 nn K + ? p + nn. ????? , 12 ??? 2004. 1. CKM matrix.

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Measurement of K L ? p 0 nn decay

Measurement of K L ? p 0 nn decay. G.Y.Lim IPNS,KEK. Why K L ? p 0 nn ?. Flavor Changing Neutral Current Br(K L g p o n n ) = 6 k 1 ?Im(V td V ts ) 2 X 2 (x t ) ? = 1.94?10 -10 h 2 A 4 X 2. Strong Interaction : Factorized by K e3 Decay. *.

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The future of the E391a experiment

The future of the E391a experiment. G.Y.Lim IPNS,KEK. ?????????????? ???? 2003 ? 3 ? 4 ?. Goal Sensitivity < 10 -13 Standard Model events > 100 Dh / h < 5 %. Precise measurement of Br(K L g p 0 nn ). Direct CP violation ( D s =1) Clean measurement of Im(V td ) ? h

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