The NA58 experiment, or COMPASS (standing for "Common Muon and Proton Apparatus for Structure and Spectroscopy") is a 60-metre-long

fixed-target experiment A fixed-target experiment in particle physics is an experiment in which a beam of accelerated particles is collided with a stationary target. The moving beam (also known as a projectile) consists of charged particles such as electrons or protons a ...

at the M2 beam line of the SPS at CERN. The experimental hall is located at the CERN North Area, close to the French village of Prévessin-Moëns. The experiment is a two-staged

spectrometer A spectrometer () is a scientific instrument used to separate and measure spectral components of a physical phenomenon. Spectrometer is a broad term often used to describe instruments that measure a continuous variable of a phenomenon where the ...

with numerous tracking detectors, particle identification and calorimetry. The physics results are extracted by recording and analysing the final states of the scattering processes. The versatile set-up, the use of different targets and particle beams allow the investigation of various processes. The main physics goals are the investigation of the nucleon spin structure and hadron spectroscopy. The collaboration consists of 220 physicists from 13 different countries, involving 28 universities and research institutes.

History and physics goals

The COMPASS experiment was proposed in 1996 and approved by the CERN research committee. Between 1999 and 2001, the experiment was set up and finally in 2001, the first commissioning run was performed. Until the start of the LHC experiments, COMPASS was the largest data-taking experiment at CERN. It is also a pioneer in adopting new detector and readout technologies, such as MicroMegas, GEM detectors and most recently THGEM photon detection. The data taking is divided into the COMPASS I and II phases. COMPASS I (2002-2011) * Nucleon spin structure * Gluon polarisation in nucleons * u,d,s flavour decomposition of the nucleon spin * Transverse spin * Quark transverse momentum distribution * Pion polarisability * Search for exotic states: ** Light meson spectroscopy ** Baryon spectroscopy COMPASS II (2012-2021) * Nucleon tomography (Deep Virtual Compton Scattering) * Unpolarised quark transverse momentum distribution and strangeness * Pion and kaon polarisabilities * Polarised Drell-Yan: universality of transverse momentum distribution * d-Quark Transversity

Experimental Apparatus

The experiment consists of three major parts: the beam telescope, the target area and the two-staged spectrometer.

Particle beam

The M2 beam line is able to transport various secondary and tertiary

particle beams A particle beam is a stream of charged or neutral particles. In particle accelerators, these particles can move with a velocity close to the speed of light. There is a difference between the creation and control of charged particle beams and neu ...

, which all originate from the Super Proton Synchrotron. The primary proton beam (400 GeV/c and up to 1.5E13 protons per super cycle) is steered on a beryllium production target producing secondary hadrons, mainly consisting of (anti-) protons, pions and kaons. The production target and the experiment are separated by a 1.1 km long transfer line, allowing through weak decay and use of massive hadron absorbers the production of a naturally spin-polarised muon beam. The beam line is designed to transport beams up to a momentum of 280 GeV/c. Usually, five different beams are used by COMPASS: * positive and negative muon beams with a nominal momentum of 160 GeV/c or 200 GeV/c, * positive hadron beams with a nominal momentum of 190 GeV/c and a composition of 75% protons, 24% pions and 1% kaons, * negative hadron beams with a nominal momentum of 190 GeV/c and a composition of 1% anti-protons, 97% pions and 2% kaons, * low intensity electron beam for calibration purposes (60 and 40 GeV/c).

Beam telescope

The timing and the position of the incident particles are determined with cold silicon strip detectors and scintillating fibre detectors. These informations are crucial to determine the interaction point inside the target material. Depending on the beam type, modifications in the beam telescope are done: * For the muon beam, the momentum is measured using beam momentum stations, * To distinguish between the different particle types in the hadron beam, a Cherenkov detector is used.

Target

According to the physics goal, a suitable target is needed. For polarised physics, the spins of the target material need to be oriented in one direction. The target cell contains either ammonium or deuterium, which are polarised by the means of microwave radiation and strong magnetic fields. To keep up the polarisation grade, a ³He/⁴He

dilution refrigerator A 3He/4He dilution refrigerator is a cryogenic device that provides continuous cooling to temperatures as low as 2 mK, with no moving parts in the low-temperature region. The cooling power is provided by the heat of mixing of the Hel ...

is used to cool down the target material to 50 mK. The target material can be polarised longitudinal or transverse to the beam axis. For unpolarised physics, mostly liquid hydrogen is used, allowing to study the proton properties. For other physics, where high atomic numbers are needed, nickel, lead and other nuclear targets are used. The main advantage of a fixed target experiment is the large acceptance. Due to the

Lorentz boost In physics, the Lorentz transformations are a six-parameter family of linear transformations from a coordinate frame in spacetime to another frame that moves at a constant velocity relative to the former. The respective inverse transformation i ...

, most of the final states and the scattered particles are created along the beam axis. This leads to the distinctive set-up of a fixed-target experiment: most detectors are placed behind the target ("forward spectrometer"). For some processes it is necessary to detect the recoil nucleon from the target. Here, a recoil proton detector consisting of two barrels of scintillator material is used. The protons are identified by the time of flight and the energy loss.

Spectrometer

The COMPASS experiment consists of two spectrometer stages with various tracking detector types, each set-up around a spectrometer magnet to determine the momentum of the particles. The first stage is dedicated to tracks with large scattering (production) angles and the second one for small angles. In addition, the first stage holds a Ring-Imaging CHerenkov detector ("RICH"), able to distinguish pions and kaons between 10 and 50 GeV. The following detector types for measuring charged particles are used: * MicroMegas, micro mesh gas detector, * Pixelised MicroMegas, *GEMs, gaseous electron multiplier, *Pixelised GEMs, * Drift chambers, * Straws , *SciFis, scintillating fibre stations, * MWPC, multi wire proportional chambers, *Hodoscopes, scintillator counter used for triggering on scattered muons. Neutral particles, i.e. photons are detected with electro-magnetic calorimeters. The energy of produced hadrons are determined with hadronic calorimeters.

External links

Collaboration Official website

COMPASS experimental setup
*
COMPASS homes in on the nucleon spin
, ''The CERN Courier'', 25 July 2006 (accessed 26 June 2008).
CERN-NA-058 (COMPASS)
experiment record on INSPIRE-HEP {{SPS experiments CERN experiments Particle experiments Fixed-target experiments