Top Quark Production in p-p Collisions

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Discussion Overview

The discussion centers on the production of top quarks in proton-proton (p-p) collisions, specifically examining the channels available for fermions in processes involving photon and Z0 boson exchanges. Participants explore the conditions under which top quarks can be produced and the implications of collision energy on these processes.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant inquires about the channels available for fermions in the process u ubar → γ → f fbar, questioning whether f can be the top quark.
  • Another participant states that the possibility of producing all quarks, including the top quark, depends on the collision energy, particularly at high-energy colliders like the LHC.
  • A third participant clarifies that any channel where f carries electric charge is allowed if sufficient energy is available, noting that neutrinos are excluded due to their lack of charge.
  • This participant also mentions that the book by Kane excludes the top quark in certain contexts due to kinematic constraints at lower energy machines.
  • It is noted that the dominant mode of top quark production at the LHC is through strong interactions, rather than the processes discussed.
  • There is a question regarding which edition of Kane's book is being referenced, highlighting the advancements in research over the years.

Areas of Agreement / Disagreement

Participants generally agree that the production of top quarks is contingent on collision energy, but there are differing views on the implications of Kane's book and the specific processes involved in top quark production.

Contextual Notes

Participants mention the dependence on collision energy and the specific context of the machines being referenced, which may affect the availability of certain channels for top quark production.

Avogadro Number
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Hi,

In a p-p collision, where a we look at u ubar → γ → f fbar, where f is a fermion,
what channels are available for f? Is f also allowed to be the top quark?
In an analogous process where the γ is replaced for example by the Z0 boson,
the book by Kane takes f to be all except the top quark.
Could someone please clarify this for me? Thanks!
 
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It depends on the collision energy. With sufficient energy (e.g. at the LHC) all quarks are possible. The book might look at a particular machine with a lower energy.
 
Avogadro Number said:
In a p-p collision, where a we look at u ubar → γ → f fbar, where f is a fermion,
what channels are available for f? Is f also allowed to be the top quark?
Any channel that is energetically allowed where ##f## carries electric charge is allowed. In other words, if you have sufficient energy, everything except neutrinos (which do not carry electric charge).

Avogadro Number said:
In an analogous process where the γ is replaced for example by the Z0 boson,
the book by Kane takes f to be all except the top quark.
As stated in #2, the only reason to do this is to look at a particular machine where ##t\bar t## is not kinematically accessible.

Neither of those processes would be the dominant mode of ##t\bar t## production at (e.g.) the LHC as ##t\bar t## production can occur through strong interactions.

Are you looking at the first or second edition of Kane's book? There are some 25 years of intensive research separating the two editions.
 
I see. This helps me follow! I was looking at the latest edition, but I suppose even that is probably a few years old now. Thanks again!
 

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