Drell-Yan at LHC: Proton+Proton Feynman Diagram

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SUMMARY

The Drell-Yan process in proton-proton collisions at the LHC involves interactions where a quark from one proton interacts with a sea antiquark from the other proton, resulting in a virtual photon that decays into a lepton pair. The discussion clarifies that in proton-proton collisions, sea antiquarks play a crucial role, and additional processes such as quark-gluon interactions can also contribute to the Drell-Yan mechanism. These interactions are referred to as QCD corrections, which are essential for accurately modeling the Drell-Yan process in experimental settings.

PREREQUISITES
  • Understanding of Drell-Yan process in particle physics
  • Familiarity with Feynman diagrams and their interpretation
  • Knowledge of Quantum Chromodynamics (QCD)
  • Basic concepts of proton-proton collisions at the LHC
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  • Study the role of sea quarks in high-energy collisions
  • Learn about QCD corrections in particle physics
  • Explore Feynman diagrams specific to Drell-Yan processes
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Particle physicists, researchers in high-energy physics, and students studying the Drell-Yan process and QCD corrections will benefit from this discussion.

Dan2009
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Hey everyone,

Okay so usually drell-yan is shown as interaction of p + p^bar: quark + antiquark -> virtual photon -> lepton(+) + lepton(-). I have seen diagrams of this for the LHC, which is a PROTON+PROTON collider yet drell-yan is still shown as an antiquark coming from one of the protons which cannot be so. Is there an included process which is not being showing on the spectator diagram?

i.e. What is the Feynman diagram (or spectator model diagram) for Drell-Yan from a Proton+Proton Collision?

Regards,

Dan
 
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There are sea antiquarks. That's where the Drell-Yan comes from.
 
You also have the case where you have a quark-gluon initial state, where the gluon splits into a quark anti-quark pair. The anti-quark then interacts with a quark from the other proton to give the Drell-Yan part, along with an associated jet in the final state from the 'left-over' quark. Note that here, as well, quark and anti-quark can be swapped (so the initial state is a gluon and anti-quark).

Such processes are normally termed (to experimentalists, at least) QCD corrections to the DY process.
 

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