1. Overview

2. Sensitivity to light quark flavor asymmetry in the proton

3. Z boson production

4. See also

5. References

The Drell–Yan process occurs in high energy hadron–hadron scattering. It takes place when a quark of one hadron and an antiquark of another hadron annihilate, creating a virtual photon or Z boson which then decays into a pair of oppositely-charged leptons. Importantly, the energy of the colliding quark-antiquark pair can be almost entirely transformed into the mass of new particles. This process was first suggested by Sidney Drell and Tung-Mow Yan in 1970^[1] to describe the production of lepton–antilepton pairs in high-energy hadron collisions. Experimentally, this process was first observed by J.H. Christenson et al.^[2] in proton–uranium collisions at the Alternating Gradient Synchrotron.

Overview

The Drell–Yan process is studied both in fixed-target and collider experiments. It provides valuable information about the parton distribution functions (PDFs) which describe the way the momentum of an incoming high-energy nucleon is partitioned among its constituent partons. These PDFs are basic ingredients for calculating essentially all processes at hadron colliders. Although PDFs should be derivable in principle, current ignorance of some aspects of the strong force prevents this. Instead, the forms of the PDFs are deduced from experimental data.

Sensitivity to light quark flavor asymmetry in the proton

One recent measurement using Drell-Yan scattering probed the flavor asymmetry of the proton.^[3][4][5] It had been naively believed that the quark sea in the proton was formed by quantum chromodynamics (QCD) processes that did not discriminate between up and down quarks. To leading order in the strong interaction coupling constant, α_s, the ratio of the Drell-Yan cross section from a proton beam on a deuterium target to a proton beam on a proton target is given by

where and are the anti-down and anti-up quark distributions in the proton sea and is the Bjorken- scaling variable (the momentum fraction of the target quark in the parton model).^[3]

Z boson production

The production of Z bosons through the Drell–Yan process affords the opportunity to study the couplings of the Z boson to quarks. The main observable is the forward–backward asymmetry in the angular distribution of the two leptons in their center-of-mass frame.

If heavier neutral gauge bosons exist (see Z' boson), they might be discovered as a peak in the dilepton invariant mass spectrum in much the same way that the standard Z boson appears by virtue of the Drell–Yan process.

See also

• Fermilab E-906/SeaQuest

References

• Epiphenomenal
• Epiphenomenalism
• Epiphenomenalist
• Epiphenomenon
• Epiphone
• Epiphora
• Epiphyllum
• Epiphyllum x buckleyi
• Epiphyseal ischemic necrosis
• Epiphysis
• Epiphyte
• Epiphytes
• Epiphytic
• Epipremnum aureum
• Epiprineae
• Epiprinus
• EPIRB
• Epirot Islands
• Epirrhoe alternata
• Epirrita autumnata
• Epirrita christyi
• Epirrita dilutata
• Epirubicin
• Epirubicin hydrochloride
• Epirus