Flavor Mixing of Quarks and Neutrinos

63
Flavor Mixing Flavor Mixing of of Quarks and Quarks and Neutrinos Neutrinos H. Fritzsch H. Fritzsch LMU Munich LMU Munich

description

Flavor Mixing of Quarks and Neutrinos. H. Fritzsch LMU Munich. W. Pauli: 1930  Neutrino mass ~ m(e). 1956: maximal parity violation neutrinos massless. 1998: Y. Totsuka … (Kamioka)  neutrino oscillations. neutrinos  massive. -. texture zero - PowerPoint PPT Presentation

Transcript of Flavor Mixing of Quarks and Neutrinos

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Flavor Mixing of Flavor Mixing of Quarks and Quarks and

NeutrinosNeutrinosH. Fritzsch H. Fritzsch LMU MunichLMU Munich

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W. Pauli: 1930 Neutrino mass ~ m(e)

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1956:1956:maximal parity maximal parity

violationviolation

neutrinos neutrinos masslessmassless

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1998:

Y. Totsuka …(Kamioka)

neutrino oscillations

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III

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New parametrization:New parametrization:

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Observation:Observation:

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mm

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25221 108 eVm

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:

42.0/ 21 mm

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m(1) = ( 0.004 +/- 0.0012 ) m(1) = ( 0.004 +/- 0.0012 ) eVeV

m(2) = ( 0.011 +/- 0.002 ) m(2) = ( 0.011 +/- 0.002 ) eVeV

m(3) = ( 0.051 +/- 0.007 )eV m(3) = ( 0.051 +/- 0.007 )eV

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006.0049.0sin 133 eV

0022.00096.02sin 132

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0022.00096.02sin 132

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Neutrinoless Double Beta Neutrinoless Double Beta DecayDecay

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332211. mVmVmVm eeeeff

.........................................

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neutrino masses:neutrino masses:

m(1)/m(2)=0.42, m(2)/m(3)=0.19m(1)/m(2)=0.42, m(2)/m(3)=0.19

m(1): 0.0041 eV m(1): 0.0041 eV m(2): 0.0097 eVm(2): 0.0097 eVm(3): 0.051 eVm(3): 0.051 eV

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neutrinoless double neutrinoless double beta decay: beta decay:

improvement by factor improvement by factor 20 necessary20 necessary

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05.03 eV