UNITARY SYMMETRY AND LEPTONIC DECAYS

[1] BARKAS WH, 1960, 1960 P ANN INT C HIG, P878

[2] BECKER W, TO BE PUBLISHED

[3] CONSEQUENCES OF UNITARY SYMMETRY FOR WEAK AND ELECTROMAGNETIC TRANSITIONS [J]. NUOVO CIMENTO, 1961, 21 (05): : 872 - +

[4] ELY RP, 1962, 1962 P INT C HIGH EN, P445

[5] THEORY OF THE FERMI INTERACTION [J]. PHYSICAL REVIEW, 1958, 109 (01): : 193 - 198

[6] FEYNMAN RP, 1960, 1960 P ANN INT C HIG, P501

[7] THE AXIAL VECTOR CURRENT IN BETA-DECAY [J]. NUOVO CIMENTO, 1960, 16 (04): : 705 - 726

[8] GELLMANN M, 1961, CTSL20 REP

[9] Marshak R.E., 1958, PHYS REV, V109, P1860

[10] MARSHAK RE, 1958, 1957 P PAP VEN C MES

[1] BARKAS WH, 1960, 1960 P ANN INT C HIG, P878

[2] BECKER W, TO BE PUBLISHED

[3] CONSEQUENCES OF UNITARY SYMMETRY FOR WEAK AND ELECTROMAGNETIC TRANSITIONS [J]. NUOVO CIMENTO, 1961, 21 (05): : 872 - +

[4] ELY RP, 1962, 1962 P INT C HIGH EN, P445

[5] THEORY OF THE FERMI INTERACTION [J]. PHYSICAL REVIEW, 1958, 109 (01): : 193 - 198

[6] FEYNMAN RP, 1960, 1960 P ANN INT C HIG, P501

[7] THE AXIAL VECTOR CURRENT IN BETA-DECAY [J]. NUOVO CIMENTO, 1960, 16 (04): : 705 - 726

[8] GELLMANN M, 1961, CTSL20 REP

[9] Marshak R.E., 1958, PHYS REV, V109, P1860

[10] MARSHAK RE, 1958, 1957 P PAP VEN C MES