1967
DOI: 10.1016/0550-3213(67)90055-7
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Experimental results on the and (Kp) systems as observed in the annihilations at rest

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Cited by 57 publications
(22 citation statements)
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“…where the value of BR(p#(3S1) ---, K*/{,/(*K) measured in [9] was increased by 30% to account for unobserved channels. In the absence of experimental data for the BR(p#(3S1) ~ p+p-(I = 1)) the value in (44) has been taken from the theoretical model [10] which overall well describes the measured two-meson branching ratios.…”
Section: + (2ae -52 --C 2) Log C + B ] C-b +2b(c-a) With a B And mentioning
confidence: 99%
“…where the value of BR(p#(3S1) ---, K*/{,/(*K) measured in [9] was increased by 30% to account for unobserved channels. In the absence of experimental data for the BR(p#(3S1) ~ p+p-(I = 1)) the value in (44) has been taken from the theoretical model [10] which overall well describes the measured two-meson branching ratios.…”
Section: + (2ae -52 --C 2) Log C + B ] C-b +2b(c-a) With a B And mentioning
confidence: 99%
“…In both cases the on-shell approximation has been evaluated, in addition the effect of vertex functions for the kaon exchanged in the crossed channel has been evaluated in [8]. Using experimental information [10] on the lower limit for the branching ratio of the subprocess Bpp_.K.~=23.4x10 -4 the branching ratio for q~ ~o in on-shell approximation is B(pp--*K*ff~--*4)7c~…”
Section: Two Meson Rescattering Mechanisms For Pp ~ No ~Bmentioning
confidence: 99%
“…All the amplitudes in Eq. (1) are then directly related to experimental information [2,3,4]. Similar equations hold for ρ + ρ − intermediate states.…”
Section: The Reaction Pp → πφmentioning
confidence: 99%