-
Giulia Ricciardi15/09/2009, 11:00
-
Georges Vasseur15/09/2009, 11:30Weak Decays, CP violation and CKM
-
Chih-Hsiang Cheng15/09/2009, 12:00Weak Decays, CP violation and CKM
-
Tagir Aushev15/09/2009, 15:30
-
Matthew Moulson15/09/2009, 16:00Weak Decays, CP violation and CKM
-
Sandra Leone15/09/2009, 17:30Weak Decays, CP violation and CKM
-
Anze Zupanc15/09/2009, 18:00Weak Decays, CP violation and CKM
-
MyeongJae Lee15/09/2009, 18:30Weak Decays, CP violation and CKM
-
Damir Becirevic16/09/2009, 09:00Weak Decays, CP violation and CKM
-
Gerhard Ecker16/09/2009, 09:30Weak Decays, CP violation and CKM
-
Giancarlo D'Ambrosio16/09/2009, 10:00Weak Decays, CP violation and CKM
-
Bjoren Duling16/09/2009, 11:00Weak Decays, CP violation and CKM
-
Antonio Limosani16/09/2009, 15:30Weak Decays, CP violation and CKM
-
Silke Nelson16/09/2009, 16:00Weak Decays, CP violation and CKM
-
Rainer Wanke16/09/2009, 17:30Weak Decays, CP violation and CKM
-
Mauro Piccini16/09/2009, 18:00Weak Decays, CP violation and CKM
-
Alejandro Ibarra17/09/2009, 09:00Weak Decays, CP violation and CKM
-
Alessandro Baldini17/09/2009, 09:40Weak Decays, CP violation and CKM
-
Riccardo Cenci17/09/2009, 11:00Weak Decays, CP violation and CKM
-
Peter Fierlinger17/09/2009, 11:30Weak Decays, CP violation and CKM
-
Jaap Panman18/09/2009, 09:00Weak Decays, CP violation and CKM
-
Marcello GIORGI18/09/2009, 09:30Weak Decays, CP violation and CKM
-
Masanori Yamauchi18/09/2009, 10:00Weak Decays, CP violation and CKM
-
Steve kettell18/09/2009, 11:00Weak Decays, CP violation and CKMThe extremely rare decay K+ -> pi+ neutrino anti-neutrino has been studied for the last 20 years with the E787 and E949 experiments and the high-intensity proton beam of the AGS accelerator at Brookhaven National Laboratory. The E949 experiment previously reported results above the K+ -> pi+pi0 peak, in the pion momentum region [211,229] MeV/c {Phys.Rev.Lett.93:031801(2004);...Go to contribution page
-
Augusto Ceccucci18/09/2009, 11:30Weak Decays, CP violation and CKM
-
Taku Yamanaka18/09/2009, 12:00The purpose of the J-PARC E14 KOTO experiment is to search for new physics beyond the standard model that enhances the branching ratio of the \(K_L \to \pi^0 \nu \bar{\nu}\) decay. The experiment looks for two and only two photons from the decay that have a finite transverse momentum. The detector consists of a pure CsI calorimeter and hermetic photon veto counters placed in a vacuum...Go to contribution page
Choose timezone
Your profile timezone: