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Page 1: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 2: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 3: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 4: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 5: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 6: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 7: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 8: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory

From left , Yoichiro Nambu, Makoto Kobayashi and Toshihide Masukawa, who shared the Nobel Prize in Physics on Tuesday

Page 9: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 10: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 11: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 12: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 13: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 14: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 15: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 16: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 17: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 18: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 19: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 20: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 21: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 22: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 23: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 24: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 25: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 26: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 27: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 28: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 29: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 30: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 31: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 32: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 33: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 34: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 35: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 36: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 37: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 38: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 39: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 40: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 41: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 42: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 43: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 44: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 45: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 46: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 47: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 48: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 49: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 50: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 51: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 52: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 53: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 54: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 55: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 56: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 57: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 58: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 59: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory
Page 60: lphe.epfl.ch · 2018. 5. 15. · of rare decays (AF = 1), of mixing phenomena (AF = 2) and of all CP violating observables at tree and loop level are consistent with the CKM theory

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