COMPARISON OF SIGMA+P AND SIGMA-N SYSTEMS

[1] BALDOCEOLIN, 1957, NUOVO CIMENTO, V6, P144

[2] THE BINDING ENERGY OF SIGMA HYPERONS WITH NUCLEONS [J]. NUOVO CIMENTO, 1957, 6 (05): : 1027 - 1033

[3] FRY WF, 1957, P PADUA VENICE C ELE

[4] ISOTOPIC SPIN AND NEW UNSTABLE PARTICLES [J]. PHYSICAL REVIEW, 1953, 92 (03): : 833 - 834

[5] GELLMANN M, 1955, P INT C HIGH ENERGY

[6] GROBNER W, 1950, INTEGRALTAFEL 2, P166

[7] HOLLADAY WG, CITED INDIRECTLY

[8] JAHNKEEMDE, 1945, TABLES FUNCTIONS, P1

[9] PION CONTRIBUTION TO HYPERON-NUCLEON FORCES [J]. PHYSICAL REVIEW, 1957, 107 (06): : 1714 - 1721

[10] Morse P.M., 1953, METHODS THEORETICA 1, P551

[1] BALDOCEOLIN, 1957, NUOVO CIMENTO, V6, P144

[2] THE BINDING ENERGY OF SIGMA HYPERONS WITH NUCLEONS [J]. NUOVO CIMENTO, 1957, 6 (05): : 1027 - 1033

[3] FRY WF, 1957, P PADUA VENICE C ELE

[4] ISOTOPIC SPIN AND NEW UNSTABLE PARTICLES [J]. PHYSICAL REVIEW, 1953, 92 (03): : 833 - 834

[5] GELLMANN M, 1955, P INT C HIGH ENERGY

[6] GROBNER W, 1950, INTEGRALTAFEL 2, P166

[7] HOLLADAY WG, CITED INDIRECTLY

[8] JAHNKEEMDE, 1945, TABLES FUNCTIONS, P1

[9] PION CONTRIBUTION TO HYPERON-NUCLEON FORCES [J]. PHYSICAL REVIEW, 1957, 107 (06): : 1714 - 1721

[10] Morse P.M., 1953, METHODS THEORETICA 1, P551