NA61 experiment

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NA61/SHINE experiment at CERN
FormationData taking started on 18-04-2008
Headquarters Geneva, Switzerland
Leader of Experiment
Marek Gazdzicki
Website https://shine.web.cern.ch/
Super Proton Synchrotron
(SPS)
LHC.svg
Key SPS Experiments
UA1 Underground Area 1
UA2 Underground Area 2
NA31 NA31 Experiment
NA32 Investigation of Charm Production in Hadronic Interactions Using High-Resolution Silicon Detectors
COMPASS Common Muon and Proton Apparatus for Structure and Spectroscopy
SHINE SPS Heavy Ion and Neutrino Experiment
NA62 NA62 Experiment
SPS preaccelerators
p and Pb Linear accelerators for protons (Linac 2) and Lead (Linac 3)
(not marked) Proton Synchrotron Booster
PS Proton Synchrotron

NA61/SHINE (standing for "SPS Heavy Ion and Neutrino Experiment") is a particle physics experiment at the Super Proton Synchrotron (SPS) at the European Organization for Nuclear Research (CERN). [1] The experiment studies the hadronic final states produced in interactions of various beam particles (pions, protons and beryllium, argon, and xenon nuclei) with a variety of fixed nuclear targets at the SPS energies.

Contents

About 135 physicists from 14 countries and 35 institutions work in NA61/SHINE, led by Marek Gazdzicki. NA61/SHINE is the second largest fixed target experiment at CERN.

Physics program

The NA61/SHINE physics program has been designed to measure hadron production in three different types of collisions: [1]

Detector

The NA61/SHINE experiment uses a large acceptance hadron spectrometer located on the H2 beam line in the North Area of CERN. [1] It consist of components used by the heavy ion NA49 experiment as well as those designed and constructed for NA61/SHINE. [2]

PSD detector for NA61 SHINE PSD.jpg
PSD detector for NA61

The main tracking devices are four large volume time projection chambers (TPCs), which are capable of detecting up to 70% of all charged particles created in the studied reactions. Two of them are located in the magnetic field of two super-conducting dipole magnets with maximum bending powers of 9  Tesla meters. Two others are positioned downstream of the magnets symmetrically with respect to the beam line. Additionally, four small volume TPCs placed directly along the beamline region are used in case of hadron and light ion beams. [2] [3]

The setup is supplemented by time of flight detector walls, which extend particle identification to low momenta (1 GeV/c < p ). Furthermore, the Projectile Spectator Detector (a calorimeter) is positioned downstream of the time of flight detectors to measure energy of projectile fragments.

Collected data

Type of interactionBeam momentum YearCitation
π + Be1202016CERN-SPSC-2017-038 [4]
π + C30, 60, 158, and 3502009, 2012, 2016, and 2017CERN-SPSC-2016-038, [5] PR D100 112004, [6] and PR D100 112001 [7]
π + Al602017CERN-SPSC-2016-038 [5] and PR D98 052001 [8]
Kaon + C1582012CERN-SPSC-2016-038 [5] and MPL A34 1950078 [9]
p + p13, 20, 31, 40, 80, 158, and 4002009, 2010, 2011, and 2016EPJ C80 460, [10] SQM 2019 315, [11] and EPJ C74 2794 [12]
p + Be60, and 1202016 and 2017CERN-SPSC-2017-038, [4] and PR D100 112001 [7]
p + C
p + (T2K replica target)
p + (NOvA replica target)
31, 60, 90, and 1202007, 2009, 2010, 2012, 2016, 2017, and 2018CERN-SPSC-2017-038, [4] CERN-SPSC-2016-038, [5] CERN-SPSC-2019-041, [13] PR D100 112001 [7] and EPJ C76 617 [14]
p + Al602016CERN-SPSC-2017-038 [4] and NP B732 1 [15]
p + Pb30, 40, 80 and 1582012, 2014, 2016, and 2017CERN-SPSC-2015-036 [16]
Be + Be13A, 19A, 30A, 40A, 75A, and 150A2011, 2012, and 2013CERN-SPSC-2013-028, [17] PoS 364 305, [18] and EPJ C80 961 [19]
C + C and C + CH13A2018CERN-SPSC-2019-041 [13]
Ar + Sc13A, 19A, 30A, 40A, 75A and 150A2015CERN-SPSC-2015-036, [16] PoS 364 305, [18] Acta Phys. Pol. B Proc. Suppl. 10 645 [20] and EPJ C81 397 [21]
Xe + La13A, 19A, 30A, 40A, 75A, and 150A2017CERN-SPSC-2018-029 [22] and PoS 364 305 [18]
Pb + Pb13A, 30A, and 150A2016 and 2018CERN-SPSC-2016-038, [5] J. Phys. Conf. Ser. 1690 012127 [23] and PR C77 064908 [24]

Extended program: after Long Shutdown 2

NA61 experiment at CERN after Long Shutdown 2 NA61 SHINE.jpg
NA61 experiment at CERN after Long Shutdown 2

In 2018 the NA61/SHINE collaboration published an addendum presenting an intent to upgrade the experimental facility and perform a new set of measurements after Long Shutdown 2. [25] As in the original program, the new one proposes studies of hadron-nucleus and nucleus-nucleus interactions for heavy ions, neutrino and cosmic-ray physics.

The heavy ions program will focus on study of charm hadron production (mostly D mesons) in lead-lead interactions.

In 2020 the SPS and PS Experiments Committee (SPSC) recommended approval of beam time in 2021. [26] The Research Board endorsed these recommendations. [27]

See also

Related Research Articles

<span class="mw-page-title-main">Pionium</span>

Pionium is a composite particle consisting of one
π+
and one
π
meson. It can be created, for instance, by interaction of a proton beam accelerated by a particle accelerator and a target nucleus. Pionium has a short lifetime, predicted by chiral perturbation theory to be 2.89×10−15 s. It decays mainly into two
π0
mesons, and to a smaller extent into two photons.

<span class="mw-page-title-main">Top quark</span> Type of quark

The top quark, sometimes also referred to as the truth quark, is the most massive of all observed elementary particles. It derives its mass from its coupling to the Higgs Boson. This coupling is very close to unity; in the Standard Model of particle physics, it is the largest (strongest) coupling at the scale of the weak interactions and above. The top quark was discovered in 1995 by the CDF and DØ experiments at Fermilab.

<span class="mw-page-title-main">Tetraquark</span> Exotic meson composed of four valence quarks

In particle physics, a tetraquark is an exotic meson composed of four valence quarks. A tetraquark state has long been suspected to be allowed by quantum chromodynamics, the modern theory of strong interactions. A tetraquark state is an example of an exotic hadron which lies outside the conventional quark model classification. A number of different types of tetraquark have been observed.

<span class="mw-page-title-main">Super Proton Synchrotron</span> Particle accelerator at CERN, Switzerland

The Super Proton Synchrotron (SPS) is a particle accelerator of the synchrotron type at CERN. It is housed in a circular tunnel, 6.9 kilometres (4.3 mi) in circumference, straddling the border of France and Switzerland near Geneva, Switzerland.

<span class="mw-page-title-main">Antiproton Decelerator</span> Particle storage ring at CERN, Switzerland

The Antiproton Decelerator (AD) is a storage ring at the CERN laboratory near Geneva. It was built from the Antiproton Collector (AC) to be a successor to the Low Energy Antiproton Ring (LEAR) and started operation in the year 2000. Antiprotons are created by impinging a proton beam from the Proton Synchrotron on a metal target. The AD decelerates the resultant antiprotons to an energy of 5.3 MeV, which are then ejected to one of several connected experiments.

In particle physics, the odderon corresponds to an elusive family of odd-gluon states, dominated by a three-gluon state. When protons collide elastically with protons or with anti-protons at high energies, even or odd numbers of gluons are exchanged. Exchanging an even number of gluons is a crossing-even part of elastic proton–proton and proton–antiproton scattering, while odderon exchange, i.e. exchange of odd number of gluons, corresponds to a crossing-odd term in the elastic scattering amplitude. It took about 48 years to find a definite signal of odderon exchange.

<span class="mw-page-title-main">Quark–gluon plasma</span> Phase of quantum chromodynamics (QCD)

Quark–gluon plasma is an interacting localized assembly of quarks and gluons at thermal and chemical (abundance) equilibrium. The word plasma signals that free color charges are allowed. In a 1987 summary, Léon van Hove pointed out the equivalence of the three terms: quark gluon plasma, quark matter and a new state of matter. Since the temperature is above the Hagedorn temperature—and thus above the scale of light u,d-quark mass—the pressure exhibits the relativistic Stefan-Boltzmann format governed by temperature to the fourth power and many practically massless quark and gluon constituents. It can be said that QGP emerges to be the new phase of strongly interacting matter which manifests its physical properties in terms of nearly free dynamics of practically massless gluons and quarks. Both quarks and gluons must be present in conditions near chemical (yield) equilibrium with their colour charge open for a new state of matter to be referred to as QGP.

<span class="mw-page-title-main">Marek Gazdzicki</span> Polish physicist

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<span class="mw-page-title-main">Onset of deconfinement</span>

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<span class="mw-page-title-main">NA62 experiment</span>

The NA62 experiment is a fixed-target particle physics experiment in the North Area of the SPS accelerator at CERN. The experiment was approved in February 2007. Data taking began in 2015, and the experiment is expected to become the first in the world to probe the decays of the charged kaon with probabilities down to 10−12. The experiment's spokesperson is Cristina Lazzeroni. The collaboration involves 333 individuals from 30 institutions and 13 countries around the world.

<span class="mw-page-title-main">NA49 experiment</span> Particle physics experiment

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<span class="mw-page-title-main">Terry Wyatt</span> British scientist

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<span class="mw-page-title-main">750 GeV diphoton excess</span> 2015 anomaly in the Large Hadron Collider

The 750 GeV diphoton excess in particle physics was an anomaly in data collected at the Large Hadron Collider (LHC) in 2015, which could have been an indication of a new particle or resonance. The anomaly was absent in data collected in 2016, suggesting that the diphoton excess was a statistical fluctuation. In the interval between the December 2015 and August 2016 results, the anomaly generated considerable interest in the scientific community, including about 500 theoretical studies. The hypothetical particle was denoted by the Greek letter Ϝ in the scientific literature, owing to the decay channel in which the anomaly occurred. The data, however, were always less than five standard deviations (sigma) different from that expected if there was no new particle, and, as such, the anomaly never reached the accepted level of statistical significance required to announce a discovery in particle physics. After the August 2016 results, interest in the anomaly sank as it was considered a statistical fluctuation. Indeed, a Bayesian analysis of the anomaly found that whilst data collected in 2015 constituted "substantial" evidence for the digamma on the Jeffreys scale, data collected in 2016 combined with that collected in 2015 was evidence against the digamma.

<span class="mw-page-title-main">WA70 experiment</span>

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<span class="mw-page-title-main">FASER experiment</span> 2022 particle physics experiment at the Large Hadron Collider at CERN

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<span class="mw-page-title-main">Fixed-target experiment</span>

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 consists of charged particles such as electrons or protons and is accelerated to relativistic speed. The fixed target can be a solid block or a liquid or a gaseous medium. These experiments are distinct from the collider-type experiments in which two moving particle beams are accelerated and collided. The famous Rutherford gold foil experiment, performed between 1908 and 1913, was one of the first fixed-target experiments, in which the alpha particles were targeted at a thin gold foil.

The Search for Hidden Particle (SHiP) is a fixed-target experiment at CERN's Super Proton Synchrotron (SPS) with the goal of searching for the interactions and measurements of the weakly interacting particles. In October 2013, the Expression of Interest letter for SHiP was submitted to the SPS Council (SPSC). Following which the Technical Proposal was submitted in April 2015, describing the experimental and detector facility. The Comprehensive Design Study was completed during 2016-19.

David M. Strom is an experimental high energy particle physicist on the faculty of the University of Oregon.

References

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