Weak-boson production at Fermilab Tevatron energies

Weak bosons are produced in hadron collisions by quarks and antiquarks withaverage fractional momenta /ital x/=/ital M//sub /ital W/,/ital Z/// /radical/s . When /radical//ital s/is increased by a factor of 3, the average value of /ital x/ shifts fromabout 0.15 at CERN /ital pp/bar // collider energ...

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Veröffentlicht in:	Phys. Rev. D; (United States) 1989-07, Vol.40 (1), p.83-91
Hauptverfasser:	Berger, EL, Halzen, F, Kim, CS, Willenbrock, S
Format:	Artikel
Sprache:	eng
Schlagworte:	645102 - High Energy Physics- Particle Interactions & Properties-Experimental- Weak Interactions & Properties 645203 - High Energy Physics- Particle Interactions & Properties-Theoretical- Weak Interactions & Properties BARYON-BARYON INTERACTIONS BOSONS CROSS SECTIONS DEEP INELASTIC SCATTERING ELEMENTARY PARTICLES ENERGY RANGE FERMIONS FUNCTIONS HADRON-HADRON INTERACTIONS INELASTIC SCATTERING INTERACTIONS INTERMEDIATE BOSONS INTERMEDIATE VECTOR BOSONS LEPTON-BARYON INTERACTIONS LEPTON-HADRON INTERACTIONS LEPTON-NUCLEON INTERACTIONS MATHEMATICAL MODELS NUCLEON-ANTINUCLEON INTERACTIONS PARTICLE INTERACTIONS PARTICLE MODELS PARTICLE PRODUCTION PARTICLE PROPERTIES PARTICLE RAPIDITY PARTONS PHYSICS OF ELEMENTARY PARTICLES AND FIELDS POSTULATED PARTICLES PROTON-ANTIPROTON INTERACTIONS QUARKS SCATTERING STANDARD MODEL STRUCTURE FUNCTIONS TEV RANGE TOP PARTICLES UNIFIED GAUGE MODELS W MINUS BOSONS W PLUS BOSONS
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