Formation | Data taking started on 18-04-2008 |
---|---|
Headquarters | Geneva, Switzerland |
Leader of Experiment | Marek Gazdzicki |
Website | https://shine.web.cern.ch/ |
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.
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.
The NA61/SHINE physics program has been designed to measure hadron production in three different types of collisions: [1]
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]
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.
Type of interaction | Beam momentum | Year | Citation |
---|---|---|---|
π + Be | 120 | 2016 | CERN-SPSC-2017-038 [4] |
π + C | 30, 60, 158, and 350 | 2009, 2012, 2016, and 2017 | CERN-SPSC-2016-038, [5] PR D100 112004, [6] and PR D100 112001 [7] |
π + Al | 60 | 2017 | CERN-SPSC-2016-038 [5] and PR D98 052001 [8] |
Kaon + C | 158 | 2012 | CERN-SPSC-2016-038 [5] and MPL A34 1950078 [9] |
p + p | 13, 20, 31, 40, 80, 158, and 400 | 2009, 2010, 2011, and 2016 | EPJ C80 460, [10] SQM 2019 315, [11] and EPJ C74 2794 [12] |
p + Be | 60, and 120 | 2016 and 2017 | CERN-SPSC-2017-038, [4] and PR D100 112001 [7] |
p + C p + (T2K replica target) p + (NOvA replica target) | 31, 60, 90, and 120 | 2007, 2009, 2010, 2012, 2016, 2017, and 2018 | CERN-SPSC-2017-038, [4] CERN-SPSC-2016-038, [5] CERN-SPSC-2019-041, [13] PR D100 112001 [7] and EPJ C76 617 [14] |
p + Al | 60 | 2016 | CERN-SPSC-2017-038 [4] and NP B732 1 [15] |
p + Pb | 30, 40, 80 and 158 | 2012, 2014, 2016, and 2017 | CERN-SPSC-2015-036 [16] |
Be + Be | 13A, 19A, 30A, 40A, 75A, and 150A | 2011, 2012, and 2013 | CERN-SPSC-2013-028, [17] PoS 364 305, [18] and EPJ C80 961 [19] |
C + C and C + CH | 13A | 2018 | CERN-SPSC-2019-041 [13] |
Ar + Sc | 13A, 19A, 30A, 40A, 75A and 150A | 2015 | CERN-SPSC-2015-036, [16] PoS 364 305, [18] Acta Phys. Pol. B Proc. Suppl. 10 645 [20] and EPJ C81 397 [21] |
Xe + La | 13A, 19A, 30A, 40A, 75A, and 150A | 2017 | CERN-SPSC-2018-029 [22] and PoS 364 305 [18] |
Pb + Pb | 13A, 30A, and 150A | 2016 and 2018 | CERN-SPSC-2016-038, [5] J. Phys. Conf. Ser. 1690 012127 [23] and PR C77 064908 [24] |
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]
A gluon is a type of massless elementary particle that mediates the strong interaction between quarks, acting as the exchange particle for the interaction. Gluons are massless vector bosons, thereby having a spin of 1. Through the strong interaction, gluons bind quarks into groups according to quantum chromodynamics (QCD), forming hadrons such as protons and neutrons.
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.
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 field. This coupling yt 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.
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.
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.
In high-energy physics, jet quenching is a phenomenon that can occur in the collision of ultra-high-energy particles. In general, the collision of high-energy particles can produce jets of elementary particles that emerge from these collisions. Collisions of ultra-relativistic heavy-ion particle beams create a hot and dense medium comparable to the conditions in the early universe, and then these jets interact strongly with the medium, leading to a marked reduction of their energy. This energy reduction is called "jet quenching".
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 other protons or with anti-protons at high energies, 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 corresponds to a crossing-odd term in the elastic scattering amplitude. In turn, the odderon's crossing-odd counterpart is the pomeron.
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.
Marek Gaździcki is a Polish high-energy nuclear physicist, and the initiator and spokesperson of the NA61/SHINE experiment at the CERN Super Proton Synchrotron (SPS).
The onset of deconfinement refers to the beginning of the creation of deconfined states of strongly interacting matter produced in nucleus-nucleus collisions with increasing collision energy.
In high-energy nuclear physics, strangeness production in relativistic heavy-ion collisions is a signature and diagnostic tool of quark–gluon plasma (QGP) formation and properties. Unlike up and down quarks, from which everyday matter is made, heavier quark flavors such as strange and charm typically approach chemical equilibrium in a dynamic evolution process. QGP is an interacting localized assembly of quarks and gluons at thermal (kinetic) and not necessarily chemical (abundance) equilibrium. The word plasma signals that color charged particles are able to move in the volume occupied by the plasma. The abundance of strange quarks is formed in pair-production processes in collisions between constituents of the plasma, creating the chemical abundance equilibrium. The dominant mechanism of production involves gluons only present when matter has become a quark–gluon plasma. When quark–gluon plasma disassembles into hadrons in a breakup process, the high availability of strange antiquarks helps to produce antimatter containing multiple strange quarks, which is otherwise rarely made. Similar considerations are at present made for the heavier charm flavor, which is made at the beginning of the collision process in the first interactions and is only abundant in the high-energy environments of CERN's Large Hadron Collider.
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 Giuseppe Ruggiero. The collaboration involves 308 participants from 33 institutions and 16 countries around the world.
The NA49 experiment was a particle physics experiment that investigated the properties of quark–gluon plasma. The experiment's synonym was Ions/TPC-Hadrons. It took place in the North Area of the Super Proton Synchrotron (SPS) at CERN from 1991-2002.
Terence Richard Wyatt is a Professor in the School of Physics and Astronomy at the University of Manchester, UK.
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.
The WA70 experiment was a collaboration between the Universities of Geneva, Glasgow, Liverpool, Milan and Neuchatel using the facilities of the OMEGA spectrometer at CERN.
FASER is one of the nine particle physics experiments in 2022 at the Large Hadron Collider at CERN. It is designed to both search for new light and weakly coupled elementary particles, and to detect and study the interactions of high-energy collider neutrinos. In 2023, FASER and SND@LHC reported the first observation of collider neutrinos.
The Search for Hidden Particle (SHiP) is a proposed 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. The experiment is planned to begin in 2027, and begin collecting data in 2030.
David M. Strom is an experimental high energy particle physicist on the faculty of the University of Oregon.