LHC beam: Standard or BCMS scheme

Taking a closer look at LHC

Taken from Accelerator Report: Exploring potential performance increases (by Rende Steerenberg).

Over the years, the teams responsible for the LHC proton injector chain (Linac 4, PS Booster, PS and SPS) have developed various production schemes for the LHC beam, pushed the performance of the beam and explored its potential to enhance the collisions in the LHC.

We consider here two modes: the Standard and the BCMS (Beam Compression, Merging and Splitting).

Standard mode of the LHC.

In the LHC injector chain, the standard beam is produced by injecting three bunches from the PS Booster into the PS. After an initial acceleration, the PS splits each bunch longitudinally (see explanation at bottom of page) into three, resulting in nine bunches. These nine bunches are then accelerated to the maximum energy of the PS, where each bunch is split into two, and then again into two, resulting in 36 bunches, each spaced by 25 ns (see Figure 1).

Figure 1: The standard production scheme. The three bands at the bottom of the diagram represent the three PS Booster bunches injected into the PS. The middle band shows the splitting into three, while the top band shows the double split into two, which results in 36 bunches. (Image: CERN)

The SPS receives three of these 36-bunch shots from the PS and accelerates them to an energy of 450 GeV before injecting them in the clockwise or counter-clockwise direction into the LHC. This means that one PS Booster bunch results in 12 bunches in the LHC. The number of protons per bunch (named intensity) required by the LHC is 16 x 1010. Taking the 12-fold splitting into account, this means that the number of protons per bunch which the PS Booster has to inject into the PS is 12 times higher than the LHC bunch intensity, i.e. 192 x 1010 protons per bunch.

BCMS mode of the LHC.

The BCMS beam is produced by injecting six bunches into the PS: three from a first cycle and three, 1.2 seconds later, from a second cycle. After an initial acceleration, these six bunches are compressed and merged, in pairs of two, into a single bunch, resulting in three bunches, which are then each split into three bunches. The remainder of this production scheme is identical to the standard production scheme, which also results in 36 bunches spaced by 25 ns. With this scheme, six bunches are manipulated to obtain 36 bunches, which gives a splitting factor of six. Therefore, to obtain a bunch intensity of 16 x 1010 protons for the LHC, the PS Booster needs to provide only 96 x 1010 protons per bunch (see Figure 2).

Figure 2: The BCMS production scheme. The six bunches injected from the PS Booster can be seen at the bottom of the diagram. These bunches are compressed in pairs of two and then merged into three bunches, after which each bunch is split into three. In the top part of the image, the same double split into two is applied, as in the standard production scheme, resulting in 36 bunches. (Image: CERN)

How is it that the BCMS beam results in more collisions in the LHC if it contains the same number of protons as a standard beam?

The BCMS beam has a greater brightness, which means that it contains the same number of protons but in a smaller beam size. This smaller beam size is the result of the lower intensity per bunch in the PS Booster.

The challenge is to preserve this increased brightness when the beam is accelerated in all the machines of the LHC injector chain and in the LHC itself. During acceleration in the LHC, the beam size seems to increase slightly more with the BCMS scheme than with the standard beam scheme.

A fact-based comparison will help to decide which production scheme is the most effective.

Bunch splitting, an explanation:

In the world of particle accelerators, we focus on two main spatial dimensions: transverse and longitudinal.

The transverse plane refers to the horizontal (left-right) and vertical (up-down) movements of the particles. When we talk about transverse beam size, we measure how wide and tall the beam is in these directions.

The longitudinal plane is the plane along the path of the accelerator, used to measure the length of the bunches and the spacing between them.

Bunch splitting refers to splitting a single bunch of particles into two or three shorter bunches along the longitudinal plane. The transverse size of the individual bunches remains unchanged.


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", "Ramon y Cajal" fellow (Spanish Postdoctoral Senior Grants), and Associate Professor. Since 2023 is Senior Lecturer 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 a Degree in Chemistry, and he is PhD for Santiago University (USC) (ORCID).



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 For the bibliography used when writing this Section please go to the References Section

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