Taking a closer look at LHC
The RF Cavities generate a longitudinal oscillanting voltage, which is applied across an isolated gap in the vacuum chamber, so that the particle sees an accelerating voltage at the gap, and the voltage then cancels out as the particle goes around the rest of the machine. However we must make sure that the particle always sees an accelerating voltage at the gap, so the RF frequency must always be an integer multiple (h) of the revolution frequency.
fRF = h·frev
where h is known as the harmonic number.
A particle with a speed v = βc circulates around the machine with a period or frecuency:
Trev= 2πR/ βc or frev= βc/2πR
In LHC h is very large.
RF cavities frecuency is 400 MHz, the speed of protons is βc ~c , 2πR = 26659 m.
So, we have;
Harmonic Number: h = fRF/frev
h = (400·106)/(c/26659)
Harmonic Number ≈ 35640
The segments of the circumference centred on these points are called BUCKETS.
A particle exactly synchronised with the RF frequency is called synchronous particle. As we will see below, all the other particles in the accelerator will oscillate longitudinally around the synchronous particles under the influence of the RF system. This means that instead of being spread uniformly around the circumference of the accelerator the particles get “clumped” around the synchronous particle in a BUNCH. This bunch is contained in an RF bucket.
So, LHC might accelerate a beam made up of 35640 bunches.
It is important to note that two synchrotrons are included in LHC injection chain: PS and SPS. In fact PS is responsible for providing the bunch packets with 25 ns spacing that finally will be injected from SPS in the LHC.
But let's go back to LHC. Not all LHC Buckets need to be filled with bunches. The buckets are just virtual positions on LHC circumference. Each bucket can hold a bunch of protons or can be empty.
The abort gap is a number of buckets in a row which are supposed to be never loaded with protons and form a gap in the circumference. The purpose of this gap is that in the dump process it takes a short, but signifficant time to switch on the magnets which divert the beam from the LHC into the dump.
Besides, the bucket configuration will determine where the protons in the two beams will cross over and collide (in which detectors specific bunches will be colliding).
The number of occupied buckets in LHC is 2808.
It is important to recall that: higher energy particles will have a longer orbit and a lower revolution frequency, which will delay their arrival at the accelerating cavity. Conversely lower energy particles will have a shorter orbit, a higher revolution frequency, and will arrive earlier at the accelerating cavity.
Imagine two particles in a bunch: particle A which has an energy (or momentum), which corresponds properly to the RF frequency, and particle B which initially arrives at the cavity at the same time as A, but its energy is slightly higher than A’s (therefore its revolution frequency is slightly lower). See next figure.
Suppose that when a particle A passes through the RF cavity, the voltage is zero. In this case every time A passes through the cavity it will see zero voltage. Particle A is synchronous with the RF voltage. Let’s suposse tha particle B on the first turn arrives at the same time as A but with a higher energy, therefore on the second turn it arrives later than A and sees a decelerating RF voltage and lossing energy. Several turns after its energy will be equal to that of A but arriving still later, and therefore being decelerated until its energy is enough lower to surpass the revolution frecuency of A. Then B will see an accelerating RF voltage which increase its energy until reaching the same situation than discussed for the first turn and the cycle will be restarted.
As we said above, particle A is called the synchronous particle. All the other particles, like particle B, will oscillate longitudinally around A under the influence of the RF system. These oscillations are called synchrotron oscillations.
For larger energy deviations these circles get flattened into ellipses, as the restoring force drops off from the linear central valves.
The Bucket area is called longitudinal acceptance and has unites of energy x time (eV·s)
The Bunch area is called longitudinal emittance and it has also unites of energy x time (eV·s)
Bunch area (ellipse) = π·a·b → Area = π·(ΔE/2)·(Δt/2)
So, the Longitudinal Emittance = π·ΔE·Δt/4
The LHC longitudinal acceptance (Bucket area) at 7 TeV is 7.91 eVs
Longitudinal Emittance for LHC is 2.5 eVs for top energy
For more details see Baird S. (2007). “ACCELERATORS FOR PEDESTRIANS”, AB-Note-2007-014 OP, CERN February 2007
Xabier Cid Vidal, PhD in experimental Particle Physics for Santiago University (USC). Research Fellow in experimental Particle Physics at CERN from January 2013 to Decembre 2015. He was until 2022 linked to the Department of Particle Physics of the USC as a "Juan de La Cierva" and "Ramon y Cajal" fellow (Spanish Postdoctoral Senior Grants), and he is currently Associate Professor in that Department.(ORCID).
Ramon Cid Manzano, until his retirement in 2020 was secondary school Physics Teacher at IES de SAR (Santiago - Spain), and part-time Lecturer (Profesor Asociado) in Faculty of Education at the University of Santiago (Spain). He has a Degree in Physics and in Chemistry, and he is PhD for Santiago University (USC) (ORCID).
CERN Experimental Physics DepartmentCERN and the Environment
For the bibliography used when writing this Section please go to the References Section
© Xabier Cid Vidal & Ramon Cid - firstname.lastname@example.org | SANTIAGO (SPAIN) |