Particle Accelerators: Why Opposing Streams?

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Discussion Overview

The discussion revolves around the rationale behind using two counter-rotating streams of particles in particle accelerators, particularly in relation to their effective relative velocity upon collision and the advantages over a stationary target. The scope includes theoretical considerations, experimental setups, and historical context in high-energy physics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Historical

Main Points Raised

  • Some participants question the necessity of using opposing particle streams instead of a stationary target, noting that the effective relative velocity on impact cannot exceed the speed of light.
  • Others argue that using two beams allows for greater center-of-mass (CoM) energies compared to a fixed-target setup, as demonstrated by the example of proton beams in the LHC.
  • One participant emphasizes the importance of specific scattering processes, indicating that targeted collisions between specific particle species are crucial for desired outcomes.
  • Historical references are made to beam-on-target experiments, such as Rutherford scattering, highlighting the challenges of detection at high energies when using a stationary target.
  • Another participant clarifies that while the "closing velocity" in the lab frame may approach 2c, the relative velocity as perceived by an observer in one of the streams remains constrained by relativity.
  • It is noted that a fixed-target setup requires higher energy for the beam to achieve similar collision outcomes compared to a colliding-beam setup.

Areas of Agreement / Disagreement

Participants express differing views on the effectiveness and necessity of using opposing particle streams versus stationary targets, indicating that multiple competing perspectives remain unresolved.

Contextual Notes

Limitations include the dependence on relativistic kinematics and the specific definitions of relative velocity, which may affect the interpretations of the arguments presented.

Vacant
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If you have two counter-rotating streams of particles traveling at near luminal velocity then is there effective relative velocity on impact not greater than c? Of course it can't be so why bother having the particles strike a pain-stakingly engineered opposing particle stream than say a brick wall?
 
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No it's not greater than c, because the relative velocity in SR is not added in the same way as gallilean.
The reason you use 2 beams, instead of a stationary target, is mainly because you want to achieve greater cm energies... For example the beam of protons in LHC will be able to reach about 7TeV each... the cm energy then will be around 14TeV. You may not reach greater than c, but you'll reach higher relative velocities than by sending a 7TeV proton beam on a stationary target.

ps- i think this should go to High energy physics threads?
 
Vacant said:
Of course it can't be so why bother having the particles strike a pain-stakingly engineered opposing particle stream than say a brick wall?

Because we are interested in specific scattering processes ##1 + 2 \rightarrow 3 + 4 + 5 + ...## where the numbers represent particle species. This means we very specifically want particle of species ##1## to scatter off of particle of species ##2## to produce the desired outgoing particles with some probability. It isn't enough to have particle of species ##1## aimed at a wall.
 
Historically, there have been several beam-on-target experiments. The perhaps most famous of these being that of Rutherford scattering. However, in particle accelerators, energies are extreme and apart from the reasons already mentioned here, the CoM frame would be moving relative to the detector if you did a beam-on-target experiment at those energies. This would result in most of the resulting particles being collimated in the forward direction of the beam, which makes detection a problem. This is much less of an issue when the CoM system is the same as the lab one and the collision products spread in all directions.
 
Vacant said:
If you have two counter-rotating streams of particles traveling at near luminal velocity then is there effective relative velocity on impact not greater than c?

In the laboratory, the "closing velocity" of the two beams (the rate at which the two beams approach each other in the laboratory) is indeed nearly 2c.

However, when we talk of "relative velocity" we specifically mean "the velocity of one stream as 'viewed' by an observer who is traveling along with the other stream". This is the velocity that cannot exceed c in relativity.

why bother having the particles strike a pain-stakingly engineered opposing particle stream than say a brick wall?

Because of the way relativistic kinematics work out, in a fixed-target setup you have to accelerate the beam to a much higher energy than the two beams in a colliding-beam setup, in order to get the same "bang" per collision (center-of-mass energy).

http://pdg.web.cern.ch/pdg/cpep/more_collide.html

Note particularly the answer to the question at the end of that page.
 
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