Direct photon cross sections obtained in ppBAR and pp collisions at square-root s = 24.3 GeV at the CERN SPS, are used in a next-to-leading order QCD analysis. From the cross-section difference sigma(ppBAR --> gammaX) - sigma(pp --> gammaX), and quark distributions measured in deep inelastic scattering, a determination of the strong coupling constant, alpha(s), is performed via a measurement of LAMBDA(4)/MS . This first measurement of LAMBDA(4)/MS using direct photon data yields a value LAMBDA(4)/MS = 235 +/- 79 (stat.) +/- 70 (syst.) MeV. The corresponding value of alpha(s) expressed at M(Z)2 is alpha(s) (M(Z)2) = 0.112 +/- 0.006 (stat.) +/- 0.005 (syst.) +0.009/-0.001 (theor.). The gluon distribution in the proton for x > 0.2 is determined both from the pp and from the pp data, and the results agree with each other and with previous determinations using the same method.
DETERMINATION OF ALPHA(S) AND THE GLUON DISTRIBUTION USING DIRECT PHOTON PRODUCTION IN (P)OVER-BAR-P AND PP COLLISIONS
VACCHI, Andrea
1993-01-01
Abstract
Direct photon cross sections obtained in ppBAR and pp collisions at square-root s = 24.3 GeV at the CERN SPS, are used in a next-to-leading order QCD analysis. From the cross-section difference sigma(ppBAR --> gammaX) - sigma(pp --> gammaX), and quark distributions measured in deep inelastic scattering, a determination of the strong coupling constant, alpha(s), is performed via a measurement of LAMBDA(4)/MS . This first measurement of LAMBDA(4)/MS using direct photon data yields a value LAMBDA(4)/MS = 235 +/- 79 (stat.) +/- 70 (syst.) MeV. The corresponding value of alpha(s) expressed at M(Z)2 is alpha(s) (M(Z)2) = 0.112 +/- 0.006 (stat.) +/- 0.005 (syst.) +0.009/-0.001 (theor.). The gluon distribution in the proton for x > 0.2 is determined both from the pp and from the pp data, and the results agree with each other and with previous determinations using the same method.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.