The meson theory of nuclear forces I General theory

[1] Mesotron (intermediate particle) as a name for the new particles of intermediate mass [J]. NATURE, 1938, 142 : 878 - 878

[2] A new form of the baryteron equation and some related questions [J]. NATURE, 1939, 143 : 201 - 201

[3] BETHE HA, 1936, REV MOD PHYS, V8, P105

[4] BETHE HA, 1936, REV MOD PHYS, V8, P133

[5] BETHE HA, 1936, REV MOD PHYS, V8, P107

[6] BETHE HA, IN PRESS PHYS REV

[7] The fundamental lenght introduced by the theory of the mesotron (meson) [J]. NATURE, 1939, 143 : 276 - 277

[8] BHABHA JH, 1938, P ROY SOC, V166, P501

[9] BHABHA JH, 1938, NATURE, V141, P117

[10] BLACKETT PMS, 1939, REV MOD PHYS, V11, P278

[1] Mesotron (intermediate particle) as a name for the new particles of intermediate mass [J]. NATURE, 1938, 142 : 878 - 878

[2] A new form of the baryteron equation and some related questions [J]. NATURE, 1939, 143 : 201 - 201

[3] BETHE HA, 1936, REV MOD PHYS, V8, P105

[4] BETHE HA, 1936, REV MOD PHYS, V8, P133

[5] BETHE HA, 1936, REV MOD PHYS, V8, P107

[6] BETHE HA, IN PRESS PHYS REV

[7] The fundamental lenght introduced by the theory of the mesotron (meson) [J]. NATURE, 1939, 143 : 276 - 277

[8] BHABHA JH, 1938, P ROY SOC, V166, P501

[9] BHABHA JH, 1938, NATURE, V141, P117

[10] BLACKETT PMS, 1939, REV MOD PHYS, V11, P278