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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
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Flavor Mixing of Quarks and Neutrinos H. Fritzsch LMU Munich
W. Pauli: 1930 Neutrino mass ~ m(e)
1998: Y. Totsuka … (Kamioka) neutrino oscillations neutrinos massive
- texturezero massmatrices neutrinomasses V(e3) …
- - III 2 families flavor mixing II I
mass matrices texture 0 H. Fritzsch S. Weinberg 1978 u,c - d,s ( beyond Standard Model )
texture zero: SU(2) x SU(2) x U(1) Reflection symmetries (~parity)
Grand Unification SO (10)
- ==> mass matrix
- mixing angles <=> masses
Cabibbo angle Exp.: phase 90 degrees ( symmetry ! )
III II I
- flavor mixing => CKM - matrix: three angles - one phase
CKM matrix standard parametrization
New parametrization: Fritzsch / Xing
- texture zeros:
- and can be measured separately.
SLAC DESY KEK FNAL CERN
- theory:
- theory:
theory - x x theory -
- unitarity triangle
- - - 0 0 alpha: 86 ... 95
Cabibbo angle unitarity triangle (rectangular)
- maximal CP-violation
- V = U x P V = U x P
- V = U x P H. F., Z. Xing
Theory: 3 texture zeros ( charged leptons and neutrinos )
Observation: weak mass hierarchy for neutrinos
result: 0.05 eV - 0.01 eV 0.01 eV 0.005 eV - -
m(1) = ( 0.004 +/- 0.0012 ) eVm(2) = ( 0.011 +/- 0.002 ) eVm(3) = ( 0.051 +/- 0.007 )eV normal mass hierarchy ( no inversion )
Masses (relative)
weak mass hierarchy for neutrinos large mixing angles
Neutrino Mixing Matrix: <=====
- prediction: -
Chooz Maas detector
present limit from CHOOZ: V(e3) < 0.2 expected: 0.05