LHC & Bunch Crossing: Exploring the Why & How

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SUMMARY

The discussion centers on the concept of "bunch crossing" in the Large Hadron Collider (LHC), specifically highlighting that the bunch crossing time is 25 nanoseconds, resulting in approximately 22 proton-proton collisions per bunch crossing. Continuous proton beams are impractical due to the operational mechanics of linear accelerators (linacs), which utilize high-power RF sources from Klystrons to create oscillating electric fields. This oscillation requires precise timing for particle injection to ensure effective acceleration, which is not achievable with a continuous beam. The use of oscillating RF allows for higher gradients and reduced power consumption, making it a more efficient method for particle acceleration.

PREREQUISITES
  • Understanding of particle acceleration principles
  • Familiarity with linear accelerator (linac) technology
  • Knowledge of radio frequency (RF) systems in particle physics
  • Basic concepts of electric fields and phase synchronization
NEXT STEPS
  • Research the design and operation of linear accelerators (linacs)
  • Explore the role of Klystrons in RF generation for particle accelerators
  • Learn about phase synchronization techniques in particle physics
  • Investigate the efficiency of oscillating versus static electric fields in acceleration
USEFUL FOR

Particle physicists, accelerator engineers, and students studying high-energy physics will benefit from this discussion, particularly those interested in the mechanics of particle acceleration and the operational challenges of the LHC.

touqra
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I was reading about the LHC and came across the term "bunch crossing" in this sentence "The bunch crossing time will be 25ns and at full luminosity there will be approximately 22 proton-proton collisions per bunch crossing. "

It seems obvious that this means the protons are coming in bunches which will last for 25 ns. Why can't they make a continuous proton beam? Sorry if this question sounds stupid.
 
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There are several reasons, but I'll list just 1.

When charge particles are accelerated, the most common technology today is to use a "linac" structure. These consist of a series of cavities. However, these cavities are power by a high-power RF source from a Klystron. Essentially, what you have in each of the cavity is a standing wave oscillating E-field along the line of motion of the particles. So when you have a series of such cavities, and you only have one RF source for each linac structure, you then have E-field oscillating back and forth in each cavity.

So what happens here is that you need to inject the charge particle bunch at just the right phase when it enters the first cavity to get an acceleration. But you must also time it just right (by building just the right length between one cavity and the next), so that by the time it leaves the first cavity, enters a drift tube, and then enters the next cavity, the E-field phase will again start to build up in the right direction. This continues though the length of the linac. This is how most particle accelerator works.

So as you can see, if you have a continuous bunch, you will not get the same effect, because you will have bunches that will enter the linac at the wrong phase.

So why do you use oscillating RF as the source of the E-field for acceleration. Because we can get higher gradient at the right phase for smaller amount of power than using a static, continuous E-field. It is "cheaper" and less taxing on power consumption.

Zz.
 

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