"Hadron production in electron-positron storage rings", a review

Budnev, V.M.; Ginzburg, I.F.; Meledin, G.V.; Serbo, Valeriy G.

doi:10.1051/jphyscol:1974224

Cited by 2 publications

(3 citation statements)

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“…As far as experimental cuts on final state momenta imply restrictions also for the momentum transfers q 2 i , or the scale variable x, it would be straightforward to modify our expressions for the luminosities accordingly. (16), are evaluated most easily in their respective Breit systems B j using the expressions (48) and ( 50) for the four-momenta and the expressions ( 52) and ( 53) for the polarization vectors. The results are:…”

Section: Discussionmentioning

confidence: 99%

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Luminosities for vector-boson-vector-boson scattering at high energy colliders

Kuss

Spiesberger

1996

Phys. Rev. D

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We derive exact expressions for luminosities of massive vector-boson pairs which can be used to describe the cross sections for processes in hadron collisions or e + e − annihilation which proceed via two-vector-boson scattering. Our approach correctly takes into account the mutual influence of the emission of one vector boson on the emission of a second one. We show that only approximately the exact luminosities can be factorized into convolutions of single-vector-boson distributions. Numerical results are given and compared to simplified approaches.1

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Section: Discussionmentioning

confidence: 99%

“…In addition, interference contributions need not vanish, as has been noticed in the specific example of Higgs boson production in [15]. This is in analogy to two-photon processes [16] where it was shown already in [17] that the extension of the Weizsäcker-Williams method from one photon to the case of two photons is not straightforward.…”

Section: Introductionmentioning

confidence: 95%

Luminosities for vector-boson-vector-boson scattering at high energy colliders

Kuss

Spiesberger

1996

Phys. Rev. D

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“…In the direct case, H µν stands for the appropriate tensor describing the photon-photon scattering amplitudes (for a definition see e.g. [9,20]). Note, that the lepton tensor of the electron radiating the real photon integrated over the azimuthal and polar angle of the outgoing electron gives the Weizsäcker-Williams formula (4).…”

Section: General Structure Of the Cross Sectionsmentioning

confidence: 99%

Jet production in deep inelastic electron-photon scattering at e+e− colliders in next-to-leading order QCD

Pötter

1999

Nuclear Physics B

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A complete next-to-leading order QCD calculation of deep inelastic electron-photon scattering including direct and resolved real photon components is presented. Soft and collinear singularities are extracted using the phase space slicing method. Application of the results for the prediction of single-and dijet cross sections at the LEP e + e − collider are presented, using the Snowmass jet definition. The dependence of the cross sections on the transverse momentum and on the rapidities of the jets are discussed.

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"Hadron production in electron-positron storage rings", a review

Cited by 2 publications

References 0 publications

Luminosities for vector-boson-vector-boson scattering at high energy colliders

Luminosities for vector-boson-vector-boson scattering at high energy colliders

Jet production in deep inelastic electron-photon scattering at e+e− colliders in next-to-leading order QCD

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