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Matthews, J. A. J.; Prentice, J. D.; Yoon, T. S.; Carroll, J. T.; Firebaugh, M. W.; Walker, W. D.

doi:10.1103/physrevlett.26.400

Cited by 39 publications

(3 citation statements)

References 14 publications

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“…The statistical error in the moment, <f(0,0)> is given by 6<f(0,0)> = 7 (4) . <(f (0,0)) 2> -<f (0,0)>2…”

Section: Binsmentioning

confidence: 99%

High statistics study of ω<sup>0</sup> production at 6 GeV/c

Shaevitz¹

1975

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“…The statistical error in the moment, <f(0,0)> is given by 6<f(0,0)> = 7 (4) . <(f (0,0)) 2> -<f (0,0)>2…”

Section: Binsmentioning

confidence: 99%

High statistics study of ω<sup>0</sup> production at 6 GeV/c

Shaevitz¹

1975

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“…Completely transverse w production i s expected in a simple exchange model since naturalparity-exchange ( p ) would be expected to dominate w production a t large energies. It is clear f r o m h e data of Matthews --et al 71 that some unnatural parity exchange* (e.g., B) must still be present a t 7 GeV/c, since pO0 # 0.…”

mentioning

confidence: 99%

Rho-meson production by pions at 15 GeV/c: A study of vector dominance and of rho-omega interference

Ratcliff¹

1971

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“…Here, of course, the main concern is the correlation of the transverse co production data with the photoproductlon data and not with the unexpected abundance of zero hehcity co mesons*. In order to do this the density matrix elements observed at 4.19 and 5.08 GeV/c [29,30] were rotated from the Gottfried-Jackson frame to the heliclty frame, and compared with the measured values at 6.95 GeV/c [31 ]. We found no evidence for any energy dependence of either the magnitude or the t-dependence of oH .…”

Section: Co-meson Productionmentioning

confidence: 99%

Comparison of the high energy models for neutral meson photoproduction and the related hadronic processes

1971

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To cntlcaUy compare the Michigan and Argonne models we perform stmultaneous fits to the high-energy data for rr o and r/photoproductlon together with that for the related hadronic vector meson production reactions, in particular that for 7r+n ~ top. Thus all constraints on these models are considered simultaneously. Particular attention IS given to the strength of absorptive cuts in both models, and to the role of the B-meson exchange in filling dips m the Argonne model. We fred that the o-Pomeron cuts 0.e. cuts associated with large hehcity flip at the NN vertex) are essential to introducing unnatural panty exchange m the Michigan model, and that the B-meson contribution Is incapable of filling unwanted dips which appear m any model with nonsense wrong signature zeros as required by exchange degeneracy. The flap and non-flap 0 and to coupling strengths at the NNvertex are determined. Predactlons are made for vaiaous polarization asymmetraes for 3'P ~ rr°P and ~,p ~ r/p. The dffferentaal cross sectaon for K~p ~ K~p as calculated and compared with the exastmg data.

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ωProduction inπ+d→ppπ+

Cited by 39 publications

References 14 publications

High statistics study of ω<sup>0</sup> production at 6 GeV/c

High statistics study of ω<sup>0</sup> production at 6 GeV/c

Rho-meson production by pions at 15 GeV/c: A study of vector dominance and of rho-omega interference

Comparison of the high energy models for neutral meson photoproduction and the related hadronic processes

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