Would a transversal beam of electrons increase the energy collision in the LHC?

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Discussion Overview

The discussion revolves around the potential effects of introducing a transversal beam of electrons to the proton collisions in the Large Hadron Collider (LHC). Participants explore whether this could increase the energy of proton collisions by minimizing their repulsion, while considering the implications of such an approach on collision dynamics and energy requirements.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions if a transversal beam of electrons could reduce proton repulsion and increase collision energy, suggesting that significant energy would be needed to create such an electron beam.
  • Another participant argues that the potential energy from proton repulsion is negligible compared to their kinetic energy, implying that the introduction of electrons may not significantly affect collision outcomes.
  • It is noted that the space-charge effects of protons are small, and the use of magnets to focus beams is standard practice, which could mitigate concerns about beam size.
  • Calculations are presented regarding the potential energy associated with proton repulsion, estimating it to be around 1-2 MeV, which is considered minor in the context of high-energy collisions.
  • Some participants mention that while electron cooling is a technique used to enhance proton beam performance, implementing it in the LHC would be complex and costly due to the high energies involved.
  • Discussion includes the thermal energy exchange between protons and electrons, indicating that electrons could help cool the proton beam, thereby increasing collision rates.

Areas of Agreement / Disagreement

Participants express differing views on the significance of proton repulsion and the feasibility of using a transversal electron beam. While some acknowledge the potential benefits of electron cooling, there is no consensus on the effectiveness or practicality of the proposed approach.

Contextual Notes

Participants highlight that the space-charge effects and beam interactions near collision points are important considerations, but the discussion does not resolve the implications of these factors on the proposed electron beam approach.

viraltux
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Hi All,

Protons repel each other and in order to make them collide in the LHC huge amounts of energy have to be put in place, my question is; if we launch a beam of electrons transversal to the beam of protons and right in the collision point of the protons, would not this increase the energy at which the protons collide since the electrons would minimize the protons repulsion?

I imaging that to be able to squeeze a beam of electrons there we would also need lots of energy but I wonder if it would pay off.

Thank you.
 
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Hi,
Well, estimate the potential energy associated with the proton repulsion at the collision point and compare it to the their kinetic energy. Is it relevant? not really.

The reason allot of energy has to be put in the protons is that we wish to collide at them at very high energies, in order to produce particles with more mass. But they would collide at much lower energies.
 
viraltux said:
Hi All,

Protons repel each other and in order to make them collide in the LHC huge amounts of energy have to be put in place, my question is; if we launch a beam of electrons transversal to the beam of protons and right in the collision point of the protons, would not this increase the energy at which the protons collide since the electrons would minimize the protons repulsion?

I imaging that to be able to squeeze a beam of electrons there we would also need lots of energy but I wonder if it would pay off.

Thank you.

This is rather strange. The amount of space-charge for the proton beam is actually quite small since there's an extremely small number of protons to start with (significantly less than 1 nC per bunch). So the perceived problem that you are talking about here doesn't matter much.

Furthermore, there's a reason one uses magnets such as a solenoid or quadrupoles. One can FOCUS these beams to a very small point at various locations along the beamline. So getting them to get to a small cross-section isn't an issue either.

NOTE that at the LHC currently, the problem isn't too few collisions, but it is getting to be too many! Read the issue on a possible LHC data pile-up!

Zz.
 
Well, estimate the potential energy associated with the proton repulsion at the collision point
e2/r = (e2/ħc)(ħc/r) = (1/137)(197.5 MeV-f/1 f) = 1 or 2 MeV

Actually the goal is to make the protons collide any way at all, dumping their tremendous kinetic energy into an interaction, and if they want to do this via a photon that's fine. The probability of a collision at 8 TeV being elastic is negligible.
 
Oh, I see, so the repulsion among protons is negligible in the collision compared to their kinetic energy, that would explain it. Thank you all!
 
ZapperZ said:
This is rather strange. The amount of space-charge for the proton beam is actually quite small since there's an extremely small number of protons to start with (significantly less than 1 nC per bunch).
It is about 20nC (1.3*10^11 protons) per bunch.
Space charge effects are not negligible and the beam/beam interaction close to the collision points has to be taken into account.

In addition to Bill_K's calculation: This 1-2 MeV is related to the last femtometers of the proton/proton approach, while the collisions take place anywhere within ~10cm length.

An electron beam parallel to the beam can be used to cool a proton beam (and therefore reducing its width and increasing the collision rate), this is called electron cooling.
However, the LHC protons are so high-energetic that the required electron accelerator would be quite long and expensive. The acceleration itself is used to focus the protons, and this is enough to get a high collision rate for several hours.
 
mfb said:
It is about 20nC (1.3*10^11 protons) per bunch.
Space charge effects are not negligible and the beam/beam interaction close to the collision points has to be taken into account.

In addition to Bill_K's calculation: This 1-2 MeV is related to the last femtometers of the proton/proton approach, while the collisions take place anywhere within ~10cm length.

An electron beam parallel to the beam can be used to cool a proton beam (and therefore reducing its width and increasing the collision rate), this is called electron cooling.
However, the LHC protons are so high-energetic that the required electron accelerator would be quite long and expensive. The acceleration itself is used to focus the protons, and this is enough to get a high collision rate for several hours.

Oh, wow! so it even has a name; electron cooling. I guess the question wasn't that bad after all! :-p Though the beam is just parallel, never transversal, right? OK.

Thank you mfb!
 
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It is parallel to give the beams some time to exchange thermal energy. The protons have a design path and energy, but in addition they have some random motion around these design values, which is similar to a proton gas with some "temperature". If you add "cool" electrons to the beam, the protons can transfer a part of their thermal energy to the electrons.
 
mfb said:
It is parallel to give the beams some time to exchange thermal energy. The protons have a design path and energy, but in addition they have some random motion around these design values, which is similar to a proton gas with some "temperature". If you add "cool" electrons to the beam, the protons can transfer a part of their thermal energy to the electrons.

Oh I see! Well that makes sense. Thanks again mfb!
 

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