Taking a closer look at LHC


The goal of the Linac4 (160 MeV) is to replace Linac2 (50 MeV) as injector to the PS Booster (PSB). The new linac will increase the beam brightness out of the PSB by a factor of 2, making possible an upgrade of the LHC injectors for higher intensity and eventually an increase of the LHC luminosity.

During the long shutdown planned for 2019-20, it will replace Linac 2. It is an important milestone in the project to increase the luminosity of the LHC during the next decade.

Linac4 is located in an underground tunnel connected to the Linac4-PSB transfer line. A surface building house RF equipment, power supplies, electronics and other infrastructure.


An ordinary hydrogen atom has one electron and one proton. Its electric charge is zero. We could strip off the electron and accelerate the protons. This is precisely what is happening at present in LINAC2, which is the first step in LHC current accelerator chain. Actually, to be more precise, the linac is not the first stage of the accelerator chain, because a source of charged particles and an injector system are needed to put particle into the linac.

Instead creating protons from H, an electron is added, making a negatively charged hydrogen-ion. The ion source is fed with hydrogen gas. A discharge plasma is formed and a strong  electric field strips away an electron from each hydogen atom.


The positively charged  (protons) from the plasma are attracted towards a cathode surface (metal surface with caesium). The deposition of caesium reduces the work function of the cathode, making it a more efficient donor of electrons to the positively charged hydrogen ions, thus enhancing H- ion production

Because of its negative charge, the H- ion will move away from the negative surface.

The H- ions are extracted from the ion source in 400 μs long pulses to form a beam which is then passed through a small magnet to remove any electrons.

The H- ions leave the ion source with an energy of 45 keV and across 86 m line  (Radio Frequency Quadrupole, Chopper line, an Alvarez Drift Tube Linac (DTL), a Cell-Coupled Drift Tube Linac (CCDTL) and a Pi-mode structure (PIMS), will be finally adquiring 160 MeV.



Basically Linac4 works in the same way that any linear accelerator. It uses radiofrequency cavities to charge cylindrical conductors. The ions pass through the conductors, which are alternately charged positive or negative. The conductors behind them push particles and the conductors ahead of them pull, causing the particles to accelerate. Small quadrupole magnets ensure the hydrogen ions remain in a tight beam. As particles approach the speed of light, the energy imparted by the conductors is converted into mass.

The Linac4 basic architecture is shown here:

After leaving Linac4 the two electrons belonging to H- ion are stripped off and the bare protons injected into the Booster (PSB) for acceleration in the rest of the chain.

Because electrons are very light, the ion has nearly the same mass as a proton but with opposite charge. Due to the H- ion has the opposite charge of a proton, a proton beam and H- beam would converge when passed through a single magnet. The “merged” beams would diverge again if passed through a second magnet

The electrons in the H- ion are weakly bound to the proton and can be easily stripped if passed though a thin Carbon foil.   Because the foil is thin and the protons have high energy, the foil will not bother the protons. This allows more particles to accumulate in the synchrotron, simplifies injection, reduces beam loss at injection and gives a more brilliant beam.

Linac 4 is scheduled to become the source of proton beams for the Large Hadron Collider after the long shutdown in 2017-18. It is the first step in the project to increase the luminosity of the LHC during the next decade.

Some Physics in LINAC4...

The main Linac4 beam parameters are as follows:

Ion species


Output energy

160 MeV

Bunch frequency

352.2 MHz

Max. rep. rate

2 Hz

Beam pulse Length

400 microsec

Chopping scheme

222/133 transmitted bunches/empty buckets

Mean pulse current

40 mA

Beam power

5.1 kW

N. particles per pulse


N. particles per bunch


Beam transverse emittance

0.4 pmm mrad (rms)


Let’s calculate the Beam power:

(Nº Particles per pulse) x (Output energy) x (Max. rep. rate)

(1014 particles/pulse) x (160·106 eV/particle) x (1,6·10-19 J/eV) x  (2 pulses/s)

Beam power = 5100 J/s = 5,1 kW

Now we calculate the Mean pulse current:

(Nº Particles per pulse) x (Electric charge/particle) / (Beam pulse Length)

(1014 particles/pulse) x (1,6·10-19 Culomb/particle) / (400·10-6 s/pulse)

Mean pulse current = 0,04 A = 40 mA

(Very special thanks to MAURIZIO VRETENAR - LINAC4 Project Leader )

More information:



LINAC4 ISWP review, Nov 2013



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. Currently, he is in USC Particle Physics Department ("Ramon y Cajal", Spanish Postdoctoral Senior Grants).

Ramon Cid Manzano, 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 is PhD for Santiago University (USC).



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

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