1 / 11

Exclusive Production of Heavy Quark Mesons in pp and pp collisions

Exclusive Production of Heavy Quark Mesons in pp and pp collisions. Spencer Klein, LBNL & Joakim Nystrand, Bergen. Photoproduction of heavy vector mesons in pp/pp collisions Rates and rapidity distributions Interference and p T spectra Backgrounds Conclusions. Photoproduction.

lenka
Télécharger la présentation

Exclusive Production of Heavy Quark Mesons in pp and pp collisions

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Exclusive Production of Heavy Quark Mesons in pp and pp collisions Spencer Klein, LBNL & Joakim Nystrand, Bergen Photoproduction of heavy vector mesons in pp/pp collisions Rates and rapidity distributions Interference and pT spectra Backgrounds Conclusions

  2. Photoproduction • A photon from the electromagnetic field of one nucleus interacts with the other nucleus, producing a vector meson • Either nucleus can be photon source • The photon flux extends up to 0.1 Ep or higher • These photons can probe low-x gluons S. Klein,LBNL

  3. Photon Flux • From Weizsacker-Williams • b > 2Rp; • no hadronic interactions • Clean event signatures • Take bmin ~ 0.7 fm • Change to bmin = 1.0 fm is error estimate • Sensitive to proton form factor • Qmin2=k/g Drees and Zeppenfield, 1989 S. Klein,LBNL

  4. Vector Meson production ITheory • gg collision at lowest order • Need another gluon to conserve color • Refinements • Relativistic wave functions • Off diagonal parton dists. • NLO contributions • Sensitive to gluon distributions • Q2=MV2/4 Ryskin, 1993 S. Klein,LBNL

  5. ZEUS U Vector Meson production II Experiment • HERA data • J/Y: s~ W0.8 • agreement with theory • U: s ~ W1.7 • limited statistics • U(1), U(2), U(3) not separated • Estimate 80% U(1) • Alternately, use s~ W0.8 • So-so match with theory • Tevatron reaches slightly higher Wgp • Lower gluon x Wgp (GeV) H1/ZEUS J/y Wgp (GeV) Wgp (GeV) S. Klein,LBNL

  6. Cross Sections, Rates and ds/dy RHIC @ 500 GeV (top) • Photon energy -> rapidity • Y = ½ ln (2k/MV) • The U @ RHIC (500 GeV, 1031cm-2 s-1) • 0.4/hr • difficult • The U @ the Tevatron (1.8 TeV, 2*1032cm-2s-1) • 76/hr • Easy • J/Y rates are high The Tevatron (bottom) S. Klein,LBNL

  7. Interference • Either proton can act as emitter or target • Can’t differentiate between • How to transform diagram 1 into 2? • For pp -> parity transform • For pp -> CP transform • U and J/y are JPC = 1-- • pp: subtract amplitudes • pp add amplitudes S. Klein,LBNL

  8. pp --> ppU (RHIC) pp --> ppU (the Tevatron) dN/dpT2 dN/dpT2 Solid – interference Dashed – no interference pT spectra • pp & pp are very different! • <b> ~ few rp • pTP >> pTg • Different from AA • Interference is relevant for most of production pT range S. Klein,LBNL

  9. Interference or no interference? • Interference occurs when we can’t tell which nucleus emitted the photon • What if scattered proton is detected in a Roman pot? • Most of the VM pT comes from the target proton, so a measurement of the proton pT can determine where the photon came from. • But, what about timing? • What if the J/Y or U is detected before the proton hits the Roman pot? • If detection in a Roman pot destroys the interference, then this can be used to remove the 2-fold ambiguity and study gluons at very low x values S. Klein,LBNL

  10. Backgrounds • s(p(g)p --> (J/Y or U)pp) ~ 10-3 s(pp --> (J/Y or U)X). • Is the signal visible? • Cutting on pT < 1 GeV/c eliminates 94% of the hadroproduction. • Rapidity gaps eliminate the rest. • At the Tevatron dnch/dy ~ 3.9. • 3 units of rapidity gap --> exp(-3*3.9) ~ 10-5. • There are gaps on both sides. • The 3 units can be split between both sides. • 3 units of coverage is easy. • Similar numerology at RHIC; even easier at the LHC. • Quantum numbers wrong for Pomeron-Pomeron. S. Klein,LBNL

  11. Conclusions • Photoproduction of heavy vector mesons is substantial in pp and pp colliders. • The rates are sensitive to the gluon distribution in the proton. • Production at the two sources can interfere. The sign of this interference is different for pp and pp collisions. • The pT spectrum of produced mesons is very different for pp and pp collisions. S. Klein,LBNL

More Related