ON SYMMETRIES OF WEAK INTERACTIONS

[1] DALITZ RH, CITED INDIRECTLY

[2] DESPAGNAT B, 1957, CR HEBD ACAD SCI, V245, P894

[3] INTERACTIONS FAIBLES DES HYPERONS ET DES MESONS LOURDS [J]. NUOVO CIMENTO, 1956, 3 (05): : 1045 - 1059

[4] FORMULATION MATHEMATIQUE DU MODELE DE GELL-MANN [J]. NUCLEAR PHYSICS, 1956, 1 (01): : 33 - 53

[5] SYMMETRIES IN ISOTOPIC SPIN SPACE AND THE CHARGE OPERATOR [J]. PHYSICAL REVIEW, 1956, 102 (06): : 1684 - 1685

[6] DESPAGNAT B, 1957, PADOVA VENICE C

[7] ISOTOPIC SPIN SELECTION RULES AND PARITY NON-CONSERVATION IN THE DECAY OF THE S-RANGE PARTICLES [J]. NUOVO CIMENTO, 1957, 6 (03): : 650 - 663

[8] GATTO R, 1956, NUOVO CIMENTO, V2, P318

[9] MODEL OF THE STRONG COUPLINGS [J]. PHYSICAL REVIEW, 1957, 106 (06): : 1296 - 1300

[10] MARSHAK RE, 1955, B AM PHYS SOC, V30, P25

[1] DALITZ RH, CITED INDIRECTLY

[2] DESPAGNAT B, 1957, CR HEBD ACAD SCI, V245, P894

[3] INTERACTIONS FAIBLES DES HYPERONS ET DES MESONS LOURDS [J]. NUOVO CIMENTO, 1956, 3 (05): : 1045 - 1059

[4] FORMULATION MATHEMATIQUE DU MODELE DE GELL-MANN [J]. NUCLEAR PHYSICS, 1956, 1 (01): : 33 - 53

[5] SYMMETRIES IN ISOTOPIC SPIN SPACE AND THE CHARGE OPERATOR [J]. PHYSICAL REVIEW, 1956, 102 (06): : 1684 - 1685

[6] DESPAGNAT B, 1957, PADOVA VENICE C

[7] ISOTOPIC SPIN SELECTION RULES AND PARITY NON-CONSERVATION IN THE DECAY OF THE S-RANGE PARTICLES [J]. NUOVO CIMENTO, 1957, 6 (03): : 650 - 663

[8] GATTO R, 1956, NUOVO CIMENTO, V2, P318

[9] MODEL OF THE STRONG COUPLINGS [J]. PHYSICAL REVIEW, 1957, 106 (06): : 1296 - 1300

[10] MARSHAK RE, 1955, B AM PHYS SOC, V30, P25