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{{Short description|Branch of physics concerning the nature of particles}}
{{Short description|Branch of physics concerning the nature of particles}}
{{other uses of|particle|Particle (disambiguation)}}
{{Use Oxford spelling|date=September 2016}}
{{Use Oxford spelling|date=September 2016}}
{{Use dmy dates|date=July 2020}}
{{Use dmy dates|date=July 2020}}
{{Distinguish|Nuclear physics}}
[[Image:Standard Model of Elementary Particles Anti.svg|right|350px|thumb|The [[Standard Model]] of particle physics, listing all [[elementary particle]]s]]'''Particle physics''' (also known as '''high energy physics''') is a branch of [[physics]] that studies the nature of the particles that constitute [[matter]] and [[radiation]]. Although the word ''[[particle]]'' can refer to various types of very small objects (e.g. [[protons]], gas particles, or even household dust), {{em|particle physics}} usually investigates the irreducibly smallest detectable particles and the [[fundamental interaction]]s necessary to explain their behaviour.


[[File:Cyclotron motion.jpg|right|thumb|upright=1.5|alt=see caption|A beam of [[electron]]s deflected by a magnetic field into a circle, ionizing the gas inside to fluoresce a purple ring]]
In current understanding, these [[elementary particle]]s are excitations of the [[Field (physics)#Quantum fields|quantum fields]] that also govern their interactions. The currently dominant theory explaining these fundamental particles and fields, along with their dynamics, is called the [[Standard Model]]. Thus, modern particle physics generally investigates the Standard Model and its various possible extensions, e.g. to the newest "known" particle, the [[Higgs boson]], or even to the oldest known force field, [[gravity]].<ref>{{cite web|url=http://home.web.cern.ch/topics/higgs-boson|title=The Higgs Boson|publisher=CERN|access-date=24 August 2014|archive-date=21 August 2014|archive-url=https://web.archive.org/web/20140821222159/http://home.web.cern.ch/topics/higgs-boson|url-status=live}}</ref><ref>{{cite web | url=https://www.nobelprize.org/nobel_prizes/physics/laureates/2013/advanced-physicsprize2013.pdf | title=The BEH-Mechanism, Interactions with Short Range Forces and Scalar Particles | date=8 October 2013 | access-date=14 June 2017 | archive-date=30 June 2018 | archive-url=https://web.archive.org/web/20180630190424/https://www.nobelprize.org/nobel_prizes/physics/laureates/2013/advanced-physicsprize2013.pdf | url-status=live }}</ref>


'''Particle physics''' or '''high energy physics''' is the study of [[Elementary particle|fundamental particles]] and [[fundamental interaction|interaction]]s that constitute [[matter]] and [[radiation]]. The fundamental particles in the [[universe]] are classified in the [[Standard Model]] as [[Fermion|fermions]] (matter particles) and [[Boson|bosons]] (force-carrying particles). There are three [[Generation (particle physics)|generations]] of fermions, which ordinary matter are made only from the first fermion generation. The first generation consists of [[Up quark|up]] and [[Down quark|down quarks]] composing [[Proton|protons]] and [[Neutron|neutrons]], [[Electron|electrons]], and [[Electron neutrino|electron neutrinos]]. The three fundamental interactions known to be mediated by bosons are [[electromagnetism]], the [[weak interaction]], and the [[strong interaction]]. The [[Quantum gravity|conciliation of gravity]] to the current particle physics theory is not solved; many theories have proposed to do so, such as [[string theory]] and [[Supersymmetry|supersymmetry theory]].
==Subatomic particles==
{| class="wikitable" style="float:left; margin-right:1em; background:#FFF;"
|+ Elementary Particles
|-
!
! scope="col" | [[Generation (particle physics)|Types]]
! scope="col" | [[Generation (particle physics)|Generations]]
! scope="col" | [[Antiparticle]]
! scope="col" | [[Color charge|Colours]]
! scope="col" | Total
|-
! scope="row" style="background:#DAF;" | [[Quark]]s
| rowspan="2" align="center"| 2
| rowspan="2" align="center"| 3
| align="center"|Pair
| align="center"|3
| align="center"|36
|-
! scope="row" style="background:#AF7;" | [[Lepton]]s
| align="center"|Pair
| align="center"|None
| align="center"|12
|-
! scope="row" style="background:#F97;" | [[Gluon]]s
|rowspan="5" align="center"|1
|rowspan="5" align="center"|None
| align="center"|Own
| align="center"|[[Gluon#Eight colors|8]]
| align="center"|8
|-
! scope="row" style="background:#F97;" | [[Photon]]
| align="center"|Own
| align="center" rowspan="4"|None
| align="center"|1
|-
! scope="row" style="background:#F97;" | [[W and Z bosons|Z Boson]]
| align="center"|Own
| align="center"|1
|-
! scope="row" style="background:#F97;" | [[W and Z bosons|W Boson]]
| align="center"|Pair
| align="center"|2
|-
! scope="row" style="background:#FE7;" | [[Higgs boson|Higgs]]
| align="center"|Own
| align="center"|1
|-
! colspan="5" align="right" ! scope="col" | Total number of (known) elementary particles:
| align="center"|'''61'''
|}
Modern particle physics research is focused on [[subatomic particle]]s, including atomic constituents, such as [[electron]]s, [[proton]]s, and [[neutron]]s (protons and neutrons are composite particles called [[baryon]]s, made of [[quark]]s), that are produced by [[Radioactive decay|radioactive]] and [[scattering]] processes; such particles are [[photon]]s, [[neutrino]]s, and [[muon]]s, as well as a wide range of [[exotic particle]]s.<ref>{{cite book |last1=Terranova |first1=Francesco |title=A Modern Primer in Particle and Nuclear Physics. |date=2021 |publisher=Oxford Univ. Press |isbn=978-0-19-284524-5}}</ref>


==History==
Dynamics of particles are also governed by [[quantum mechanics]]; they exhibit [[wave–particle duality]], displaying particle-like behaviour under certain experimental conditions and [[wave]]-like behaviour in others. In more technical terms, they are described by [[quantum state]] vectors in a [[Hilbert space]], which is also treated in [[quantum field theory]]. Following the convention of particle physicists, the term ''[[elementary particle]]s'' is applied to those particles that are, according to current understanding, presumed to be indivisible and not composed of other particles.<ref name="braibant"/>
{{main|History of subatomic physics}}


=== Early developments ===
All particles and their interactions observed to date can be described almost entirely by a quantum field theory called the [[Standard Model]].<ref name="ifj">{{cite web|title=Particle Physics and Astrophysics Research|url=http://www.ifj.edu.pl/pro/fiz_astro.php?lang=en|publisher=The Henryk Niewodniczanski Institute of Nuclear Physics|access-date=31 May 2012|archive-url=https://web.archive.org/web/20131002173825/http://www.ifj.edu.pl/pro/fiz_astro.php?lang=en|archive-date=2 October 2013|url-status=dead}}</ref> The Standard Model, as currently formulated, has 61 elementary particles.<ref name="braibant">{{cite book
{{See also|Atomic theory}}The idea that all [[matter]] is fundamentally composed of [[Elementary particle|elementary particles]] dates from at least the 6th century BC.<ref>{{cite web |title=Fundamentals of Physics and Nuclear Physics |url=http://novelresearchinstitute.org/library/PhysNuclphys196p.pdf |url-status=dead |archive-url=https://web.archive.org/web/20121002214053/http://novelresearchinstitute.org/library/PhysNuclphys196p.pdf |archive-date=2 October 2012 |access-date=21 July 2012}}</ref> In the 19th century, [[John Dalton]], through his work on [[stoichiometry]], concluded that each element of nature was composed of a single, unique type of particle.<ref>{{cite web |date=22 May 2012 |title=Scientific Explorer: Quasiparticles |url=http://sciexplorer.blogspot.com/2012/05/quasiparticles.html |url-status=dead |archive-url=https://web.archive.org/web/20130419032637/http://sciexplorer.blogspot.com/2012/05/quasiparticles.html |archive-date=19 April 2013 |access-date=21 July 2012 |publisher=Sciexplorer.blogspot.com}}</ref> The word ''[[atom]]'', after the Greek word ''[[wiktionary:ἄτομος|atomos]]'' meaning "indivisible", has since then denoted the smallest particle of a [[chemical element]].{{Cn|date=July 2022}}
|last1=Braibant
|first1=S.
|last2=Giacomelli
|first2=G.
|last3=Spurio
|first3=M.
|year=2009
|title=Particles and Fundamental Interactions: An Introduction to Particle Physics
|url=https://books.google.com/books?id=0Pp-f0G9_9sC&q=61+fundamental+particles&pg=PA314
|pages=313–314
|publisher=[[Springer Science+Business Media|Springer]]
|isbn=978-94-007-2463-1
|access-date=19 October 2020
|archive-date=15 April 2021
|archive-url=https://web.archive.org/web/20210415025723/https://books.google.com/books?id=0Pp-f0G9_9sC&q=61+fundamental+particles&pg=PA314
|url-status=live
}}</ref>
Those elementary particles can combine to form composite particles, accounting for the hundreds of other species of particles that have been discovered since the 1960s.


Physicists soon discovered that atoms are not, in fact, the fundamental particles of nature, but are conglomerates of even smaller particles, such as the [[electron]]. The early 20th century explorations of [[nuclear physics]] and [[quantum physics]] led to proofs of [[nuclear fission]] in 1939 by [[Lise Meitner]] (based on experiments by [[Otto Hahn]]), and [[nuclear fusion]] by [[Hans Bethe]] in that same year; both discoveries also led to the development of [[Nuclear weapon|nuclear weapons]].{{Cn|date=July 2022}}
The Standard Model has been found to agree with almost all the [[experiment]]al tests conducted to date. However, most particle physicists believe that it is an incomplete description of nature and that a more fundamental theory awaits discovery (See [[Theory of Everything]]). In recent years, measurements of [[neutrino]] [[rest mass|mass]] have provided the first experimental deviations from the Standard Model, since neutrinos are massless in the Standard Model.<ref>{{cite web|title=Neutrinos in the Standard Model|url=https://t2k-experiment.org/neutrinos/in-the-standard-model|publisher=The T2K Collaboration|access-date=15 October 2019|archive-date=16 October 2019|archive-url=https://web.archive.org/web/20191016010901/https://t2k-experiment.org/neutrinos/in-the-standard-model/|url-status=live}}</ref>


=== Quantum mechanics ===
==History==
Throughout the 1950s and 1960s, a bewildering variety of particles were found in collisions of particles from beams of increasingly high energy. It was referred to informally as the "[[particle zoo]]". Important discoveries such as the [[CP violation]] by [[James Cronin]] and [[Val Fitch]] brought new questions to [[Baryon asymmetry|matter-antimatter imbalance]].{{Cn|date=July 2022}} After the formulation of the Standard Model during the 1970s, physicists clarified the origin of the particle zoo. The large number of particles was explained as combinations of a (relatively) small number of more fundamental particles and framed in the context of [[Quantum field theory|quantum field theories]]. This reclassification marked the beginning of modern particle physics.<ref>{{cite book |last1=Weinberg |first1=Steven |title=The quantum theory of fields |date=1995–2000 |publisher=Cambridge University Press |isbn=978-0521670531 |location=Cambridge}}</ref><ref>{{Cite journal |last=Jaeger |first=Gregg |date=2021 |title=The Elementary Particles of Quantum Fields |journal=Entropy |volume=23 |issue=11 |pages=1416 |bibcode=2021Entrp..23.1416J |doi=10.3390/e23111416 |pmc=8623095 |pmid=34828114 |doi-access=free}}</ref>
{{Modern physics}}
{{main|History of subatomic physics}}
The idea that all [[matter]] is fundamentally composed of [[elementary particle]]s dates from at least the 6th century BC.<ref>{{cite web |url=http://novelresearchinstitute.org/library/PhysNuclphys196p.pdf |title=Fundamentals of Physics and Nuclear Physics |access-date=21 July 2012 |url-status=dead |archive-url=https://web.archive.org/web/20121002214053/http://novelresearchinstitute.org/library/PhysNuclphys196p.pdf |archive-date=2 October 2012}}</ref> In the 19th century, [[John Dalton]], through his work on [[stoichiometry]], concluded that each element of nature was composed of a single, unique type of particle.<ref>{{cite web |url=http://sciexplorer.blogspot.com/2012/05/quasiparticles.html |title=Scientific Explorer: Quasiparticles |publisher=Sciexplorer.blogspot.com |date=22 May 2012 |access-date=21 July 2012 |archive-url=https://web.archive.org/web/20130419032637/http://sciexplorer.blogspot.com/2012/05/quasiparticles.html |archive-date=19 April 2013 |url-status=dead }}</ref> The word ''[[atom]]'', after the Greek word ''[[wikt:ἄτομος|atomos]]'' meaning "indivisible", has since then denoted the smallest particle of a [[chemical element]], but physicists soon discovered that atoms are not, in fact, the fundamental particles of nature, but are conglomerates of even smaller particles, such as the [[electron]]. The early 20th century explorations of [[nuclear physics]] and [[quantum physics]] led to proofs of [[nuclear fission]] in 1939 by [[Lise Meitner]] (based on experiments by [[Otto Hahn]]), and [[nuclear fusion]] by [[Hans Bethe]] in that same year; both discoveries also led to the development of [[nuclear weapon]]s. Throughout the 1950s and 1960s, a bewildering variety of particles were found in collisions of particles from beams of increasingly high energy. It was referred to informally as the "[[particle zoo]]". Important discoveries such as the [[CP violation]] by [[James Cronin]] and [[Val Fitch]] brought new questions to [[Baryon asymmetry|matter-antimatter imbalance]].<ref>{{Cite web|title=Antimatter|url=https://home.cern/science/physics/antimatter|date=2021-03-01|access-date=12 March 2021|archive-date=11 September 2018|archive-url=https://web.archive.org/web/20180911042958/https://home.cern/topics/antimatter|url-status=live}}</ref> After the formulation of the Standard Model during the 1970s, physicists clarified the origin of the particle zoo. The large number of particles was explained as combinations of a (relatively) small number of more fundamental particles and framed in the context of [[Quantum field theory|quantum field theories]]. This reclassification marked the beginning of modern particle physics.<ref>{{cite book |last1=Weinberg |first1=Steven |title=The quantum theory of fields |date=1995–2000 |publisher=Cambridge University Press |location=Cambridge |isbn=978-0521670531}}</ref><ref>{{Cite journal|last=Jaeger|first=Gregg|date=2021|title=The Elementary Particles of Quantum Fields|journal=Entropy|volume=23|issue=11|pages=1416|doi=10.3390/e23111416|pmid=34828114|pmc=8623095|bibcode=2021Entrp..23.1416J|doi-access=free}}</ref>


==Standard Model==
=== Standard Model ===
{{Main|Standard Model}}
{{Main|Standard Model}}
[[File:Standard_Model_of_Elementary_Particles_Anti.svg|right|thumb|350x350px|The [[Standard Model]] of particle physics, listing all [[Elementary particle|elementary particles]]]]
The current state of the classification of all elementary particles is explained by the [[Standard Model]], which gained widespread acceptance in the mid-1970s after [[experimental confirmation]] of the existence of [[quark]]s. It describes the [[strong interaction|strong]], [[weak interaction|weak]], and [[electromagnetism|electromagnetic]] [[fundamental interaction]]s, using mediating [[gauge boson]]s. The species of gauge bosons are eight [[gluon]]s, [[W and Z bosons|{{SubatomicParticle|W boson-}}, {{SubatomicParticle|W boson+}} and {{SubatomicParticle|Z boson}} bosons]], and the [[photon]].<ref name=ifj /> The Standard Model also contains 24 [[fundamental particle|fundamental]] [[fermion]]s (12 particles and their associated anti-particles), which are the constituents of all [[matter]].<ref name=pdg>{{cite journal|last=Nakamura|first=K|title=Review of Particle Physics|journal=Journal of Physics G: Nuclear and Particle Physics|date=1 July 2010|volume=37|issue=7A|page=075021|doi=10.1088/0954-3899/37/7A/075021|pmid=10020536|bibcode = 2010JPhG...37g5021N |doi-access=free}}</ref> Finally, the Standard Model also predicted the existence of a type of [[boson]] known as the [[Higgs boson]]. On 4 July 2012, physicists with the Large Hadron Collider at CERN announced they had found a new particle that behaves similarly to what is expected from the Higgs boson.<ref>{{cite journal |last=Mann |first=Adam |url=https://www.wired.com/wiredscience/2012/07/higgs-boson-discovery/ |title=Newly Discovered Particle Appears to Be Long-Awaited Higgs Boson |journal=Wired Science |date=28 March 2013 |access-date=6 February 2014 |archive-date=11 February 2014 |archive-url=https://web.archive.org/web/20140211212906/http://www.wired.com/wiredscience/2012/07/higgs-boson-discovery/ |url-status=live }}</ref>
The current state of the classification of all elementary particles is explained by the [[Standard Model]], which gained widespread acceptance in the mid-1970s after [[experimental confirmation]] of the existence of [[Quark|quarks]]. It describes the [[Strong interaction|strong]], [[Weak interaction|weak]], and [[Electromagnetism|electromagnetic]] [[Fundamental interaction|fundamental interactions]], using mediating [[Gauge boson|gauge bosons]]. The species of gauge bosons are eight [[Gluon|gluons]], [[W and Z bosons|{{SubatomicParticle|W boson-}}, {{SubatomicParticle|W boson+}} and {{SubatomicParticle|Z boson}} bosons]], and the [[photon]].<ref name="ifj2">{{cite web |title=Particle Physics and Astrophysics Research |url=http://www.ifj.edu.pl/pro/fiz_astro.php?lang=en |url-status=dead |archive-url=https://web.archive.org/web/20131002173825/http://www.ifj.edu.pl/pro/fiz_astro.php?lang=en |archive-date=2 October 2013 |access-date=31 May 2012 |publisher=The Henryk Niewodniczanski Institute of Nuclear Physics}}</ref> The Standard Model also contains 24 [[Fundamental particle|fundamental]] [[Fermion|fermions]] (12 particles and their associated anti-particles), which are the constituents of all [[matter]].<ref name="pdg">{{cite journal |last=Nakamura |first=K |date=1 July 2010 |title=Review of Particle Physics |journal=Journal of Physics G: Nuclear and Particle Physics |volume=37 |issue=7A |page=075021 |bibcode=2010JPhG...37g5021N |doi=10.1088/0954-3899/37/7A/075021 |pmid=10020536 |doi-access=free}}</ref> Finally, the Standard Model also predicted the existence of a type of [[boson]] known as the [[Higgs boson]]. On 4 July 2012, physicists with the Large Hadron Collider at CERN announced they had found a new particle that behaves similarly to what is expected from the Higgs boson.<ref>{{cite journal |last=Mann |first=Adam |date=28 March 2013 |title=Newly Discovered Particle Appears to Be Long-Awaited Higgs Boson |url=https://www.wired.com/wiredscience/2012/07/higgs-boson-discovery/ |url-status=live |journal=Wired Science |archive-url=https://web.archive.org/web/20140211212906/http://www.wired.com/wiredscience/2012/07/higgs-boson-discovery/ |archive-date=11 February 2014 |access-date=6 February 2014}}</ref>


==Subatomic particles==
==Experimental laboratories==
{{Main|Subatomic particle|List of particles}}A subatomic particle is a particle that composes an [[atom]].{{Cn|date=July 2022}} Dynamics of these particles are governed by [[quantum mechanics]]; they exhibit [[wave–particle duality]], displaying particle-like behaviour under certain experimental conditions and [[wave]]-like behaviour in others. In more technical terms, they are described by [[quantum state]] vectors in a [[Hilbert space]], which is also treated in [[quantum field theory]]. The term [[Elementary particle|elementary particles]] is applied to those particles that are, according to current understanding, presumed to be indivisible and not composed of other particles.<ref name="braibant">{{cite book |last1=Braibant |first1=S. |url=https://books.google.com/books?id=0Pp-f0G9_9sC&q=61+fundamental+particles&pg=PA314 |title=Particles and Fundamental Interactions: An Introduction to Particle Physics |last2=Giacomelli |first2=G. |last3=Spurio |first3=M. |publisher=[[Springer Science+Business Media|Springer]] |year=2009 |isbn=978-94-007-2463-1 |pages=313–314 |access-date=19 October 2020 |archive-url=https://web.archive.org/web/20210415025723/https://books.google.com/books?id=0Pp-f0G9_9sC&q=61+fundamental+particles&pg=PA314 |archive-date=15 April 2021 |url-status=live}}</ref> Most particles and their interactions observed to date can be described by the [[Standard Model]].<ref name="ifj">{{cite web |title=Particle Physics and Astrophysics Research |url=http://www.ifj.edu.pl/pro/fiz_astro.php?lang=en |url-status=dead |archive-url=https://web.archive.org/web/20131002173825/http://www.ifj.edu.pl/pro/fiz_astro.php?lang=en |archive-date=2 October 2013 |access-date=31 May 2012 |publisher=The Henryk Niewodniczanski Institute of Nuclear Physics}}</ref>
[[File:02 Fermilab - Fermi National Accelerator Laboratory - American particle accelerator Fermilab near Chicago Illinois.jpg|thumb|Fermi National Accelerator Laboratory, USA]]
The world's major particle physics laboratories are:
* [[Brookhaven National Laboratory]] ([[Long Island]], [[United States]]). Its main facility is the [[Relativistic Heavy Ion Collider]] (RHIC), which collides [[Relativistic nuclear collisions|heavy ions]] such as gold ions and polarized protons. It is the world's first heavy ion collider, and the world's only polarized proton collider.<ref>{{Cite journal|last1=Harrison|first1=M.|last2=Ludlam|first2=T.|last3=Ozaki|first3=S.|date=March 2003|title=RHIC project overview|url=https://zenodo.org/record/1259915|journal=Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment|volume=499|issue=2–3|pages=235–244|doi=10.1016/S0168-9002(02)01937-X|bibcode=2003NIMPA.499..235H|access-date=16 September 2019|archive-date=15 April 2021|archive-url=https://web.archive.org/web/20210415022754/https://zenodo.org/record/1259915|url-status=live}}</ref><ref>{{Cite journal|last=Courant|first=Ernest D.|title=Accelerators, Colliders, and Snakes|date=December 2003|journal=[[Annual Review of Nuclear and Particle Science]]|volume=53|issue=1|pages=1–37|doi=10.1146/annurev.nucl.53.041002.110450|bibcode=2003ARNPS..53....1C|issn=0163-8998|doi-access=free}}</ref>
* [[Budker Institute of Nuclear Physics]] ([[Novosibirsk]], [[Russia]]). Its main projects are now the electron-positron [[collider]]s [[VEPP-2000]],<ref>{{cite web |url=http://vepp2k.inp.nsk.su/ |title=index |publisher=Vepp2k.inp.nsk.su |access-date=21 July 2012 |archive-url=https://web.archive.org/web/20121029223656/http://vepp2k.inp.nsk.su/ |archive-date=29 October 2012 |url-status=dead }}</ref> operated since 2006, and VEPP-4,<ref>{{cite web |url=http://v4.inp.nsk.su/index.en.html |title=The VEPP-4 accelerating-storage complex |publisher=V4.inp.nsk.su |access-date=21 July 2012 |archive-url=https://web.archive.org/web/20110716074832/http://v4.inp.nsk.su/index.en.html |archive-date=16 July 2011 |url-status=dead }}</ref> started experiments in 1994. Earlier facilities include the first electron–electron beam–beam [[collider]] VEP-1, which conducted experiments from 1964 to 1968; the electron-positron [[collider]]s VEPP-2, operated from 1965 to 1974; and, its successor VEPP-2M,<ref>{{cite web |url=http://www.inp.nsk.su/activity/old/vepp2m/index.ru.shtml |title=VEPP-2M collider complex |language=ru |publisher=Inp.nsk.su |access-date=21 July 2012 |archive-date=3 December 2013 |archive-url=https://web.archive.org/web/20131203005149/http://www.inp.nsk.su/activity/old/vepp2m/index.ru.shtml |url-status=live }}</ref> performed experiments from 1974 to 2000.<ref>{{cite web |url=http://englishrussia.com/2012/01/21/the-budker-institute-of-nuclear-physics/ |title=The Budker Institute of Nuclear Physics |publisher=English Russia |date=21 January 2012 |access-date=23 June 2012 |archive-date=28 June 2012 |archive-url=https://web.archive.org/web/20120628191134/http://englishrussia.com/2012/01/21/the-budker-institute-of-nuclear-physics |url-status=live }}</ref>
* [[CERN]] (European Organization for Nuclear Research) ([[France|Franco]]-[[Switzerland|Swiss]] border, near [[Geneva]]). Its main project is now the [[Large Hadron Collider]] (LHC), which had its first beam circulation on 10 September 2008, and is now the world's most energetic collider of protons. It also became the most energetic collider of heavy ions after it began colliding lead ions. Earlier facilities include the [[Large Electron–Positron Collider]] (LEP), which was stopped on 2 November 2000 and then dismantled to give way for LHC; and the [[Super Proton Synchrotron]], which is being reused as a pre-accelerator for the LHC and for fixed-target experiments.<ref>{{cite web |url=http://info.cern.ch/ |title=Welcome to |publisher=Info.cern.ch |access-date=23 June 2012 |archive-date=5 January 2010 |archive-url=https://web.archive.org/web/20100105103513/http://info.cern.ch/ |url-status=live }}</ref>
* [[DESY]] (Deutsches Elektronen-Synchrotron) ([[Hamburg]], [[Germany]]). Its main facility was the [[Hadron Elektron Ring Anlage]] (HERA), which collided electrons and positrons with protons.<ref>{{cite web |url=http://www.desy.de/index_eng.html |title=Germany's largest accelerator centre |publisher=Deutsches Elektronen-Synchrotron DESY |access-date=23 June 2012 |archive-date=26 June 2012 |archive-url=https://web.archive.org/web/20120626075024/http://www.desy.de/index_eng.html |url-status=live }}</ref> The accelerator complex is now focused on the production of synchrotron radiation with PETRA III, FLASH and the [[European XFEL]].
* [[Fermilab|Fermi National Accelerator Laboratory (Fermilab)]] ([[Batavia, Illinois|Batavia]], [[United States]]). Its main facility until 2011 was the [[Tevatron]], which collided protons and antiprotons and was the highest-energy particle collider on earth until the Large Hadron Collider surpassed it on 29 November 2009.<ref>{{cite web |url=http://www.fnal.gov/ |title=Fermilab &#124; Home |publisher=Fnal.gov |access-date=23 June 2012 |archive-date=5 November 2009 |archive-url=https://web.archive.org/web/20091105014508/http://www.fnal.gov/pub/publications/index.html |url-status=live }}</ref>
* [[Institute of High Energy Physics]] (IHEP) ([[Beijing]], [[China]]). IHEP manages a number of China's major particle physics facilities, including the [[Beijing Electron–Positron Collider II]](BEPC II), the Beijing Spectrometer (BES), the Beijing Synchrotron Radiation Facility (BSRF), the International Cosmic-Ray Observatory at Yangbajing in Tibet, the [[Daya Bay Reactor Neutrino Experiment]], the [[China Spallation Neutron Source]], the [[Hard X-ray Modulation Telescope]] (HXMT), and the Accelerator-driven Sub-critical System (ADS) as well as the [[Jiangmen Underground Neutrino Observatory]] (JUNO).<ref>{{cite web |url=http://english.ihep.cas.cn/au/ |title=IHEP &#124; Home |publisher=ihep.ac.cn |access-date=29 November 2015 |url-status=dead |archive-url=https://web.archive.org/web/20160201061558/http://english.ihep.cas.cn/au/ |archive-date=1 February 2016}}</ref>
* [[KEK]] ([[Tsukuba, Ibaraki|Tsukuba]], [[Japan]]). It is the home of a number of experiments such as the [[K2K experiment]], a [[neutrino oscillation]] experiment and [[Belle II experiment|Belle II]], an experiment measuring the [[CP violation]] of [[B meson]]s.<ref>{{cite web|url=http://legacy.kek.jp/intra-e/index.html |title=Kek &#124; High Energy Accelerator Research Organization |publisher=Legacy.kek.jp |access-date=23 June 2012 |url-status=dead |archive-url=https://web.archive.org/web/20120621201554/http://legacy.kek.jp/intra-e/index.html |archive-date=21 June 2012 }}</ref>
* [[SLAC National Accelerator Laboratory]] ([[Menlo Park, California|Menlo Park]], [[United States]]). Its 2-mile-long linear particle accelerator began operating in 1962 and was the basis for numerous [[electron]] and [[positron]] collision experiments until 2008. Since then the linear accelerator is being used for the [[Linac Coherent Light Source]] [[X-ray laser]] as well as advanced accelerator design research. SLAC staff continue to participate in developing and building many [[particle detector]]s around the world.<ref>{{cite web|title=SLAC National Accelerator Laboratory Home Page|url=http://www6.slac.stanford.edu/|access-date=19 February 2015|archive-date=5 February 2015|archive-url=https://web.archive.org/web/20150205100556/https://www6.slac.stanford.edu/|url-status=live}}</ref>
<!-- These are all accelerator-based... Should we mention a couple cosmic ray experiments as well? -->
Many other [[particle accelerator]]s also exist.
The techniques required for modern experimental particle physics are quite varied and complex, constituting a sub-specialty nearly completely distinct{{citation needed|date=December 2016}} from the theoretical side of the field.


=== Quarks and leptons ===
==Theory==
{{Main|Quark|Lepton}}
{{Quantum field theory|cTopic=Standard model}}
[[File:Beta Negative Decay.svg|thumb|A [[Feynman diagram]] of the [[Beta decay|{{SubatomicParticle|Beta-}}&nbsp;decay]], showing a neutron (n, udd) converted into a proton (p, udu). "u" and "d" are the [[Up quark|up]] and [[Down quark|down quarks]], "{{Subatomic particle|electron}}" is the [[electron]], and "{{Subatomic particle|Electron antineutrino}}" is the [[Electron Antineutrino|electron antineutrino]].]]
'''Theoretical particle physics''' attempts to develop the models, theoretical framework, and mathematical tools to understand current experiments and make predictions for future experiments (see also [[theoretical physics]]). There are several major interrelated efforts being made in theoretical particle physics today.


Ordinary [[matter]] is made from first-[[Generation (particle physics)|generation]] quarks ([[Up quark|up]], [[Down quark|down]]) and leptons ([[electron]], [[electron neutrino]]).<ref name="Povh02">{{cite book |author=B. Povh |title=Particles and Nuclei: An Introduction to the Physical Concepts |author2=K. Rith |author3=C. Scholz |author4=F. Zetsche |author5=M. Lavelle |date=2004 |publisher=Springer |isbn=978-3-540-20168-7 |edition=4th |chapter=Part I: Analysis: The building blocks of matter |quote=Ordinary matter is composed entirely of first-generation particles, namely the u and d quarks, plus the electron and its neutrino. |chapter-url=https://books.google.com/books?id=rJe4k8tkq7sC&q=povh+%22building+blocks+of+matter%22&pg=PA9 |access-date=28 July 2022 |archive-date=22 April 2022 |archive-url=https://web.archive.org/web/20220422024501/https://books.google.com/books?id=rJe4k8tkq7sC&q=povh+%22building+blocks+of+matter%22&pg=PA9 |url-status=live }}</ref> Collectively, quarks and leptons are called [[Fermion|fermions]], because they have a [[quantum spin]] of [[Half-integer|half-integers]] (-1/2, 1/2, 3/2, etc.). This cause the fermions to obey the [[Pauli exclusion principle]], where no two particles may occupy the same [[quantum state]].<ref>{{cite book |author=K. A. Peacock |url=https://archive.org/details/quantumrevolutio00peac |title=The Quantum Revolution |publisher=[[Greenwood Publishing Group]] |year=2008 |isbn=978-0-313-33448-1 |page=[https://archive.org/details/quantumrevolutio00peac/page/n143 125] |url-access=limited}}</ref> Quarks have fractional [[Elementary charge|elementary electric charge]] (-1/3 or 2/3)<ref>{{cite book |author=C. Quigg |title=The New Physics for the Twenty-First Century |publisher=[[Cambridge University Press]] |year=2006 |isbn=978-0-521-81600-7 |editor=G. Fraser |page=91 |chapter=Particles and the Standard Model}}</ref> and leptons have whole-numbered electric charge (0 or 1).{{Cn|date=July 2022}} Quarks also have [[color charge]], which is labeled arbitrarily with no correlation to actual light [[color]] as red, green and blue.<ref>{{cite web |author=R. Nave |title=The Color Force |url=http://hyperphysics.phy-astr.gsu.edu/hbase/forces/color.html#c2 |access-date=2009-04-26 |work=[[HyperPhysics]] |publisher=[[Georgia State University]], Department of Physics and Astronomy |archive-date=7 October 2018 |archive-url=https://web.archive.org/web/20181007142048/http://hyperphysics.phy-astr.gsu.edu/hbase/Forces/color.html#c2 |url-status=live }}</ref> Because the interactions between the quarks stores energy which can convert to other particles when the quarks are far apart enough, quarks cannot be observed independently. This is called [[color confinement]].<ref>{{cite web |author=R. Nave |title=The Color Force |url=http://hyperphysics.phy-astr.gsu.edu/hbase/forces/color.html#c2 |access-date=2009-04-26 |work=[[HyperPhysics]] |publisher=[[Georgia State University]], Department of Physics and Astronomy |archive-date=7 October 2018 |archive-url=https://web.archive.org/web/20181007142048/http://hyperphysics.phy-astr.gsu.edu/hbase/Forces/color.html#c2 |url-status=live }}</ref>
One important branch attempts to better understand the [[Standard Model]] and its tests. Theorists make quantitative predictions of observables at [[collider]] and [[Astroparticle physics|astronomical]] experiments, which along with experimental measurements is used to extract the parameters of the Standard Model with less uncertainty. This work probes the limits of the Standard Model and therefore expands scientific understanding of nature's building blocks. Those efforts are made challenging by the difficulty of calculating high precision quantities in [[quantum chromodynamics]]. Some theorists working in this area use the tools of perturbative [[quantum field theory]] and [[effective field theory]], referring to themselves as '''[[Particle physics phenomenology|phenomenologists]]'''.{{Citation needed|date=September 2020}} Others make use of [[lattice field theory]] and call themselves ''lattice theorists''.


There are three known generations of quarks (up and down, [[Strange quark|strange]] and [[Charm quark|charm]], [[Top quark|top]] and [[Bottom quark|bottom]]) and leptons (electron and its neutrino, [[muon]] and [[Muon neutrino|its neutrino]], [[Tau (particle)|tau]] and [[Tau neutrino|its neutrino]]), with strong indirect evidence that the fourth generation of fermions doesn't exist.<ref>{{cite journal |author=D. Decamp |year=1989 |title=Determination of the number of light neutrino species |journal=[[Physics Letters B]] |volume=231 |issue=4 |pages=519 |doi=10.1016/0370-2693(89)90704-1}}</ref>
Another major effort is in model building where model builders develop ideas for what physics may lie [[beyond the Standard Model]] (at higher energies or smaller distances). This work is often motivated by the [[hierarchy problem]] and is constrained by existing experimental data.{{Citation needed|date=September 2020}} It may involve work on [[supersymmetry]], alternatives to the [[Higgs mechanism]], extra spatial dimensions (such as the [[Randall–Sundrum model]]s), [[Preon]] theory, combinations of these, or other ideas.


=== Bosons ===
A third major effort in theoretical particle physics is [[string theory]]. ''String theorists'' attempt to construct a unified description of [[quantum mechanics]] and [[general relativity]] by building a theory based on small strings, and [[branes]] rather than particles. If the theory is successful, it may be considered a "[[Theory of Everything]]", or "TOE".<ref>{{Cite web |last=Wolchover |first=Natalie |date=2017-12-22 |title=The Best Explanation for Everything in the Universe |url=https://www.theatlantic.com/science/archive/2017/12/string-theory-everything/548774/ |access-date=2022-03-11 |website=The Atlantic |language=en |archive-date=15 November 2020 |archive-url=https://web.archive.org/web/20201115210213/https://www.theatlantic.com/science/archive/2017/12/string-theory-everything/548774/ |url-status=live }}</ref>
{{Main|Boson}}
Bosons are the [[Force carrier|mediators or carriers]] of fundamental interactions, such as [[electromagnetism]], the [[weak interaction]], and the [[strong interaction]].<ref name="DarkMatter">{{cite book |author=Carroll, Sean |title=Guidebook |publisher=The Teaching Company |year=2007 |isbn=978-1598033502 |series=Dark Matter, Dark Energy: The dark side of the universe |at=Part&nbsp;2, p.&nbsp;43 |quote=...&nbsp;boson: A force-carrying particle, as opposed to a matter particle (fermion). Bosons can be piled on top of each other without limit. Examples are photons, gluons, gravitons, weak bosons, and the Higgs boson. The spin of a boson is always an integer: 0, 1, 2, and so on&nbsp;...}}</ref> Electromagnetism is mediated by the [[photon]], the [[Quantum|quanta]] of [[light]].<ref>"Role as gauge boson and polarization" §5.1 in {{cite book |last1=Aitchison |first1=I.J.R. |url={{google books |plainurl=y |id=ZJ-ZY8NW9TIC}} |title=Gauge Theories in Particle Physics |last2=Hey |first2=A.J.G. |publisher=[[IOP Publishing]] |year=1993 |isbn=978-0-85274-328-7}}</ref>{{rp|29–30}} The weak interaction is mediated by the [[W and Z bosons]].<ref>{{cite book |author=Peter Watkins |url=http://books.google.co.uk/books?id=J808AAAAIAAJ&pg=PA70 |title=Story of the W and Z |publisher=[[Cambridge University Press]] |year=1986 |isbn=9780521318754 |location=Cambridge |page=70 |access-date=28 July 2022 |archive-date=14 November 2012 |archive-url=https://web.archive.org/web/20121114055111/http://books.google.co.uk/books?id=J808AAAAIAAJ&pg=PA70 |url-status=live }}</ref> The strong interaction is mediated by the [[gluon]], which can link quarks together to form composite particles.<ref name="HyperPhysics">{{cite web |author=C.R. Nave |title=The Color Force |url=http://hyperphysics.phy-astr.gsu.edu/hbase/forces/color.html |access-date=2012-04-02 |work=[[HyperPhysics]] |publisher=[[Georgia State University]], Department of Physics |archive-date=7 October 2018 |archive-url=https://web.archive.org/web/20181007142048/http://hyperphysics.phy-astr.gsu.edu/hbase/Forces/color.html |url-status=live }}</ref> Due to the aforementioned color confinement, gluons are never observed independently.<ref name=":0">{{cite journal |last=Debrescu |first=B. A. |year=2005 |title=Massless Gauge Bosons Other Than The Photon |journal=[[Physical Review Letters]] |volume=94 |issue=15 |page=151802 |arxiv=hep-ph/0411004 |bibcode=2005PhRvL..94o1802D |doi=10.1103/PhysRevLett.94.151802 |pmid=15904133 |s2cid=7123874}}</ref> The [[Higgs boson]] gives mass to the W and Z bosons via the [[Higgs mechanism]]<ref name="PDG">{{cite web |author1=Bernardi, G. |author2=Carena, M. |author3=Junk, T. |year=2007 |title=Higgs bosons: Theory and searches |url=http://pdg.lbl.gov/2008/reviews/higgs_s055.pdf |series=Review: Hypothetical particles and Concepts |publisher=Particle Data Group |access-date=28 July 2022 |archive-date=3 October 2018 |archive-url=https://web.archive.org/web/20181003190309/http://pdg.lbl.gov/2008/reviews/higgs_s055.pdf |url-status=live }}</ref> – the gluon and photon are expected to be [[Massless particle|massless]].<ref name=":0" /> All bosons have an integer quantum spin (0 and 1) and can have the same [[quantum state]].<ref name="DarkMatter" />


=== Antiparticles and color charge ===
There are also other areas of work in theoretical particle physics ranging from [[Particle physics in cosmology|particle cosmology]] to [[loop quantum gravity]].{{Citation needed|date=September 2020}}
{{Main|Antiparticle|Color charge}}Most aforementioned particles have corresponding [[Antiparticle|antiparticles]], which compose [[antimatter]]. Normal particles have positive [[Lepton number|lepton]] or [[baryon number]], and antiparticles have these numbers negative.<ref>{{cite journal |last=Tsan |first=Ung Chan |date=2013 |title=Mass, Matter, Materialization, Mattergenesis and Conservation of Charge |journal=International Journal of Modern Physics E |volume=22 |issue=5 |page=1350027 |bibcode=2013IJMPE..2250027T |doi=10.1142/S0218301313500274 |quote=Matter conservation means conservation of baryonic number ''A'' and leptonic number ''L'', ''A'' and ''L'' being algebraic numbers. Positive ''A'' and ''L'' are associated to matter particles, negative ''A'' and ''L'' are associated to antimatter particles. All known interactions do conserve matter.}}</ref> Most properties of corresponding antiparticles and particles are the same, with a few gets reversed; the electron's antiparticle, positron, has an opposite charge. To differentiate between antiparticles and particles, a plus or negative sign is added in [[superscript]]. For example, the electron and the positron are denoted {{Subatomic particle|Electron}} and {{Subatomic particle|positron}}.<ref name="raith">{{cite book |last1=Raith |first1=W. |title=Constituents of Matter: Atoms, Molecules, Nuclei and Particles |last2=Mulvey |first2=T. |publisher=[[CRC Press]] |year=2001 |isbn=978-0-8493-1202-1 |pages=777–781}}</ref> When a particle and an antiparticle interacts with each other, they are [[Annihilation|annihilated]] and convert to other particles.<ref>{{cite web |title=Antimatter |url=http://www.lbl.gov/abc/Antimatter.html |url-status=live |archive-url=https://web.archive.org/web/20080823180515/http://www.lbl.gov/abc/Antimatter.html |archive-date=23 August 2008 |access-date=3 September 2008 |publisher=[[Lawrence Berkeley National Laboratory]]}}</ref> Some particles have no antiparticles, such as the photon or gluon.{{Cn|date=July 2022}}


Quarks and gluons additionally have color charges, which influences the strong interaction. Quark's color charges are called red, green and blue (though the particle itself have no physical color), and in antiquarks are called antired, antigreen and antiblue.<ref>{{cite web |author=R. Nave |title=The Color Force |url=http://hyperphysics.phy-astr.gsu.edu/hbase/forces/color.html#c2 |access-date=2009-04-26 |work=[[HyperPhysics]] |publisher=[[Georgia State University]], Department of Physics and Astronomy |archive-date=7 October 2018 |archive-url=https://web.archive.org/web/20181007142048/http://hyperphysics.phy-astr.gsu.edu/hbase/Forces/color.html#c2 |url-status=live }}</ref> The gluon can have [[Gluon|eight color charges]], which are the result of quarks' interactions to form composite particles (gauge symmetry [[SU(3)]]).<ref name="PeskinSchroeder">Part III of {{cite book |author1=M. E. Peskin |url=https://archive.org/details/introductiontoqu0000pesk |title=An Introduction to Quantum Field Theory |author2=D. V. Schroeder |publisher=[[Addison–Wesley]] |year=1995 |isbn=978-0-201-50397-5 |url-access=registration}}</ref>
This division of efforts in particle physics is reflected in the names of categories on the [[arXiv]], a [[preprint]] archive:<ref>{{cite web|url=http://www.arxiv.org|title=arXiv.org e-Print archive|access-date=27 July 2022|archive-date=13 May 2008|archive-url=https://web.archive.org/web/20080513113255/http://www.arxiv.org/|url-status=live}}</ref> hep-th (theory), hep-ph (phenomenology), hep-ex (experiments), hep-lat ([[lattice gauge theory]]).


=== Composite ===
==Practical applications==
{{Main|Composite particle}}
In principle, all physics (and practical applications developed therefrom) can be derived from the study of fundamental particles. In practice, even if "particle physics" is taken to mean only "high-energy atom smashers", many technologies have been developed during these pioneering investigations that later find wide uses in society. Particle accelerators are used to produce [[Isotopes in medicine|medical isotopes]] for research and treatment (for example, isotopes used in [[PET imaging]]), or used directly in [[external beam radiotherapy]]. The development of [[superconductor]]s has been pushed forward by their use in particle physics. The [[World Wide Web]] and [[touchscreen]] technology were initially developed at [[CERN]]. Additional applications are found in medicine, national security, industry, computing, science, and workforce development, illustrating a long and growing list of beneficial practical applications with contributions from particle physics.<ref>{{cite web |url=http://www.fnal.gov/pub/science/benefits/ |title=Fermilab &#124; Science at Fermilab &#124; Benefits to Society |publisher=Fnal.gov |access-date=23 June 2012 |archive-date=9 June 2012 |archive-url=https://web.archive.org/web/20120609161544/http://www.fnal.gov/pub/science/benefits/ |url-status=live }}</ref>
[[File:Quark structure proton.svg|thumb|A [[proton]] consists of two up quarks and one down quark, linked together by [[Gluon|gluons]]. The quarks' color charge are also visible.]]


The [[Neutron|neutrons]] and [[Proton|protons]] in the [[Atomic nucleus|atomic nuclei]] are [[Baryon|baryons]] – the neutron is composed of two down quarks and one up quark, and the proton is composed of two up quarks and one down quark.<ref name="Knowing2">{{cite book |author=M. Munowitz |title=Knowing |publisher=[[Oxford University Press]] |year=2005 |isbn=0195167376 |page=35}}</ref> A baryon is composed of three quarks, and a [[meson]] is composed of two quarks (one normal, one anti). Baryons and mesons are collectively called [[Hadron|hadrons]]. Quarks inside hadrons are governed by the strong interaction, thus are subjected to [[quantum chromodynamics]] (color charges). The [[Bound state|bounded]] quarks must have their color charge to be neutral, or "white" for analogy with [[Additive color|mixing the primary colors]].<ref>{{cite book |author=B. A. Schumm |url=https://archive.org/details/deepdownthingsbr00schu/page/131 |title=Deep Down Things |publisher=[[Johns Hopkins University Press]] |year=2004 |isbn=978-0-8018-7971-5 |pages=[https://archive.org/details/deepdownthingsbr00schu/page/131 131–132]}}</ref> More [[Exotic hadron|exotic hadrons]] can have other types, arrangement or number of quarks ([[tetraquark]], [[pentaquark]]).<ref>{{cite journal |last=Close |first=F. E. |year=1988 |title=Gluonic Hadrons |journal=Reports on Progress in Physics |volume=51 |pages=833–882 |bibcode=1988RPPh...51..833C |doi=10.1088/0034-4885/51/6/002 |number=6}}</ref>
==Future==
The primary goal, which is pursued in several distinct ways, is to find and understand what physics may lie [[beyond the standard model]]. There are several powerful experimental reasons to expect new physics, including [[dark matter]] and [[neutrino mass]]. There are also theoretical hints that this new physics should be found at accessible energy scales.


A normal atom is made from protons, neutrons and electrons.{{Cn|date=July 2022}} By modifying the particles inside a normal atom, [[Exotic atom|exotic atoms]] can be formed.<ref>§1.8, ''Constituents of Matter: Atoms, Molecules, Nuclei and Particles'', Ludwig Bergmann, Clemens Schaefer, and Wilhelm Raith, Berlin: Walter de Gruyter, 1997, {{ISBN|3-11-013990-1}}.</ref> A simple example would be the [[hydrogen-4.1]], which has one of its electrons replaced with a muon.<ref>{{Cite journal |last1=Fleming |first1=D. G. |last2=Arseneau |first2=D. J. |last3=Sukhorukov |first3=O. |last4=Brewer |first4=J. H. |last5=Mielke |first5=S. L. |last6=Schatz |first6=G. C. |last7=Garrett |first7=B. C. |last8=Peterson |first8=K. A. |last9=Truhlar |first9=D. G. |date=28 Jan 2011 |title=Kinetic Isotope Effects for the Reactions of Muonic Helium and Muonium with H<sub>2</sub> |url=https://www.science.org/doi/abs/10.1126/science.1199421 |journal=Science |volume=331 |issue=6016 |pages=448–450 |doi=10.1126/science.1199421 |pmid=21273484 |s2cid=206530683}}</ref>
Much of the effort to find this new physics are focused on new collider experiments. The [[Large Hadron Collider]] (LHC) was completed in 2008 to help continue the search for the [[Higgs boson]], [[supersymmetric particle]]s, and other new physics. An intermediate goal is the construction of the [[International Linear Collider]] (ILC), which will complement the LHC by allowing more precise measurements of the properties of newly found particles. In August 2004, a decision for the technology of the ILC was taken but the site has still to be agreed upon.


=== Hypothetical ===
In addition, there are important non-collider experiments that also attempt to find and understand [[physics beyond the Standard Model]]. One important non-collider effort is the determination of the [[neutrino]] masses, since these masses may arise from neutrinos mixing with very heavy particles. In addition, [[physical cosmology|cosmological]] observations provide many useful constraints on the dark matter, although it may be impossible to determine the exact nature of the dark matter without the colliders. Finally, lower bounds on the very long [[proton decay|lifetime of the proton]] put constraints on [[Grand Unified Theory|Grand Unified Theories]] at energy scales much higher than collider experiments will be able to probe any time soon.
[[Graviton]] is a hypothetical particle that can mediate the gravitational interaction, but it has not being detected nor completely reconciled with current theories.<ref>{{cite news |last=Sokal |first=A. |author-link=Alan Sokal |date=July 22, 1996 |title=Don't Pull the String Yet on Superstring Theory |work=[[The New York Times]] |url=https://query.nytimes.com/gst/fullpage.html?res=9D0DE7DB1639F931A15754C0A960958260 |access-date=March 26, 2010 |archive-date=7 December 2008 |archive-url=https://web.archive.org/web/20081207212917/https://query.nytimes.com/gst/fullpage.html?res=9D0DE7DB1639F931A15754C0A960958260 |url-status=live }}</ref>


== Fundamental interactions ==
In May 2014, the [[Particle Physics Project Prioritization Panel]] released its report on particle physics funding priorities for the United States over the next decade. This report emphasized continued U.S. participation in the LHC and ILC, and expansion of the [[Deep Underground Neutrino Experiment]], among other recommendations.
{{Main|Fundamental interaction}}
=== Quantum fields ===
{{Main|Quantum field theory}}{{Empty section|date=July 2022}}

=== Conservation laws ===
{{Further|Conservation law}}{{Empty section|date=July 2022}}

=== Quantum gravity problem ===
{{Main|Quantum gravity}}
{{Further|String theory|Physics beyond the Standard Model|Theory of everything}}Another major effort is in model building where model builders develop ideas for what physics may lie [[beyond the Standard Model]] (at higher energies or smaller distances). There are several powerful experimental reasons to expect new physics, including [[dark matter]] and [[neutrino mass]]. This work is often motivated by the [[hierarchy problem]] and is constrained by existing experimental data. It may involve work on [[supersymmetry]], alternatives to the [[Higgs mechanism]], extra spatial dimensions (such as the [[Randall–Sundrum model|Randall–Sundrum models]]), [[Preon]] theory, combinations of these, or other ideas. A third major effort in theoretical particle physics is [[string theory]]. ''String theorists'' attempt to construct a unified description of [[quantum mechanics]] and [[general relativity]] by building a theory based on small strings, and [[branes]] rather than particles. If the theory is successful, it may be considered a "[[Theory of Everything]]".{{Citation needed|date=September 2020}}

== Experimental evidence ==
One important branch attempts to better understand the [[Standard Model]] and its tests. Theorists make quantitative predictions of observables at [[collider]] and [[Astroparticle physics|astronomical]] experiments, which along with experimental measurements is used to extract the parameters of the Standard Model with less uncertainty. This work probes the limits of the Standard Model and therefore expands scientific understanding of nature's building blocks. Those efforts are made challenging by the difficulty of calculating high precision quantities in [[quantum chromodynamics]]. Some theorists working in this area use the tools of perturbative [[quantum field theory]] and [[effective field theory]], referring to themselves as [[Particle physics phenomenology|phenomenologists]].{{Citation needed|date=September 2020}} Others make use of [[lattice field theory]] and call themselves ''lattice theorists''.

=== Facilities ===
[[File:02 Fermilab - Fermi National Accelerator Laboratory - American particle accelerator Fermilab near Chicago Illinois.jpg|thumb|Fermi National Accelerator Laboratory, USA]]The world's major particle physics laboratories are:

* [[Brookhaven National Laboratory]] ([[Long Island]], [[United States]]). Its main facility is the [[Relativistic Heavy Ion Collider]] (RHIC), which collides [[Relativistic nuclear collisions|heavy ions]] such as gold ions and polarized protons. It is the world's first heavy ion collider, and the world's only polarized proton collider.<ref>{{Cite journal |last1=Harrison |first1=M. |last2=Ludlam |first2=T. |last3=Ozaki |first3=S. |date=March 2003 |title=RHIC project overview |url=https://zenodo.org/record/1259915 |url-status=live |journal=Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment |volume=499 |issue=2–3 |pages=235–244 |bibcode=2003NIMPA.499..235H |doi=10.1016/S0168-9002(02)01937-X |archive-url=https://web.archive.org/web/20210415022754/https://zenodo.org/record/1259915 |archive-date=15 April 2021 |access-date=16 September 2019}}</ref><ref>{{Cite journal |last=Courant |first=Ernest D. |date=December 2003 |title=Accelerators, Colliders, and Snakes |journal=[[Annual Review of Nuclear and Particle Science]] |volume=53 |issue=1 |pages=1–37 |bibcode=2003ARNPS..53....1C |doi=10.1146/annurev.nucl.53.041002.110450 |issn=0163-8998 |doi-access=free}}</ref>
* [[Budker Institute of Nuclear Physics]] ([[Novosibirsk]], [[Russia]]). Its main projects are now the electron-positron [[Collider|colliders]] [[VEPP-2000]],<ref>{{cite web |title=index |url=http://vepp2k.inp.nsk.su/ |url-status=dead |archive-url=https://web.archive.org/web/20121029223656/http://vepp2k.inp.nsk.su/ |archive-date=29 October 2012 |access-date=21 July 2012 |publisher=Vepp2k.inp.nsk.su}}</ref> operated since 2006, and VEPP-4,<ref>{{cite web |title=The VEPP-4 accelerating-storage complex |url=http://v4.inp.nsk.su/index.en.html |url-status=dead |archive-url=https://web.archive.org/web/20110716074832/http://v4.inp.nsk.su/index.en.html |archive-date=16 July 2011 |access-date=21 July 2012 |publisher=V4.inp.nsk.su}}</ref> started experiments in 1994. Earlier facilities include the first electron–electron beam–beam [[collider]] VEP-1, which conducted experiments from 1964 to 1968; the electron-positron [[Collider|colliders]] VEPP-2, operated from 1965 to 1974; and, its successor VEPP-2M,<ref>{{cite web |title=VEPP-2M collider complex |url=http://www.inp.nsk.su/activity/old/vepp2m/index.ru.shtml |url-status=live |archive-url=https://web.archive.org/web/20131203005149/http://www.inp.nsk.su/activity/old/vepp2m/index.ru.shtml |archive-date=3 December 2013 |access-date=21 July 2012 |publisher=Inp.nsk.su |language=ru}}</ref> performed experiments from 1974 to 2000.<ref>{{cite web |date=21 January 2012 |title=The Budker Institute of Nuclear Physics |url=http://englishrussia.com/2012/01/21/the-budker-institute-of-nuclear-physics/ |url-status=live |archive-url=https://web.archive.org/web/20120628191134/http://englishrussia.com/2012/01/21/the-budker-institute-of-nuclear-physics |archive-date=28 June 2012 |access-date=23 June 2012 |publisher=English Russia}}</ref>
* [[CERN]] (European Organization for Nuclear Research) ([[France|Franco]]-[[Switzerland|Swiss]] border, near [[Geneva]]). Its main project is now the [[Large Hadron Collider]] (LHC), which had its first beam circulation on 10 September 2008, and is now the world's most energetic collider of protons. It also became the most energetic collider of heavy ions after it began colliding lead ions. Earlier facilities include the [[Large Electron–Positron Collider]] (LEP), which was stopped on 2 November 2000 and then dismantled to give way for LHC; and the [[Super Proton Synchrotron]], which is being reused as a pre-accelerator for the LHC and for fixed-target experiments.<ref>{{cite web |title=Welcome to |url=http://info.cern.ch/ |url-status=live |archive-url=https://web.archive.org/web/20100105103513/http://info.cern.ch/ |archive-date=5 January 2010 |access-date=23 June 2012 |publisher=Info.cern.ch}}</ref>
* [[DESY]] (Deutsches Elektronen-Synchrotron) ([[Hamburg]], [[Germany]]). Its main facility was the [[Hadron Elektron Ring Anlage]] (HERA), which collided electrons and positrons with protons.<ref>{{cite web |title=Germany's largest accelerator centre |url=http://www.desy.de/index_eng.html |url-status=live |archive-url=https://web.archive.org/web/20120626075024/http://www.desy.de/index_eng.html |archive-date=26 June 2012 |access-date=23 June 2012 |publisher=Deutsches Elektronen-Synchrotron DESY}}</ref> The accelerator complex is now focused on the production of synchrotron radiation with PETRA III, FLASH and the [[European XFEL]].
* [[Fermilab|Fermi National Accelerator Laboratory (Fermilab)]] ([[Batavia, Illinois|Batavia]], [[United States]]). Its main facility until 2011 was the [[Tevatron]], which collided protons and antiprotons and was the highest-energy particle collider on earth until the Large Hadron Collider surpassed it on 29 November 2009.<ref>{{cite web |title=Fermilab &#124; Home |url=http://www.fnal.gov/ |url-status=live |archive-url=https://web.archive.org/web/20091105014508/http://www.fnal.gov/pub/publications/index.html |archive-date=5 November 2009 |access-date=23 June 2012 |publisher=Fnal.gov}}</ref>
* [[Institute of High Energy Physics]] (IHEP) ([[Beijing]], [[China]]). IHEP manages a number of China's major particle physics facilities, including the [[Beijing Electron–Positron Collider II]](BEPC II), the Beijing Spectrometer (BES), the Beijing Synchrotron Radiation Facility (BSRF), the International Cosmic-Ray Observatory at Yangbajing in Tibet, the [[Daya Bay Reactor Neutrino Experiment]], the [[China Spallation Neutron Source]], the [[Hard X-ray Modulation Telescope]] (HXMT), and the Accelerator-driven Sub-critical System (ADS) as well as the [[Jiangmen Underground Neutrino Observatory]] (JUNO).<ref>{{cite web |title=IHEP &#124; Home |url=http://english.ihep.cas.cn/au/ |url-status=dead |archive-url=https://web.archive.org/web/20160201061558/http://english.ihep.cas.cn/au/ |archive-date=1 February 2016 |access-date=29 November 2015 |publisher=ihep.ac.cn}}</ref>
* [[KEK]] ([[Tsukuba, Ibaraki|Tsukuba]], [[Japan]]). It is the home of a number of experiments such as the [[K2K experiment]], a [[neutrino oscillation]] experiment and [[Belle II experiment|Belle II]], an experiment measuring the [[CP violation]] of [[B meson|B mesons]].<ref>{{cite web |title=Kek &#124; High Energy Accelerator Research Organization |url=http://legacy.kek.jp/intra-e/index.html |url-status=dead |archive-url=https://web.archive.org/web/20120621201554/http://legacy.kek.jp/intra-e/index.html |archive-date=21 June 2012 |access-date=23 June 2012 |publisher=Legacy.kek.jp}}</ref>
* [[SLAC National Accelerator Laboratory]] ([[Menlo Park, California|Menlo Park]], [[United States]]). Its 2-mile-long linear particle accelerator began operating in 1962 and was the basis for numerous [[electron]] and [[positron]] collision experiments until 2008. Since then the linear accelerator is being used for the [[Linac Coherent Light Source]] [[X-ray laser]] as well as advanced accelerator design research. SLAC staff continue to participate in developing and building many [[Particle detector|particle detectors]] around the world.<ref>{{cite web |title=SLAC National Accelerator Laboratory Home Page |url=http://www6.slac.stanford.edu/ |url-status=live |archive-url=https://web.archive.org/web/20150205100556/https://www6.slac.stanford.edu/ |archive-date=5 February 2015 |access-date=19 February 2015}}</ref><!--These are all accelerator-based... Should we mention a couple cosmic ray experiments as well?-->

Many other [[Particle accelerator|particle accelerators]] also exist. The techniques required for modern experimental particle physics are quite varied and complex, constituting a sub-specialty nearly completely distinct from the theoretical side of the field.{{citation needed|date=December 2016}}


==See also==
==See also==

{{Columns-list|colwidth=30em|
* [[Particle physics and representation theory]]
* [[Particle physics and representation theory]]
* [[Atomic physics]]
* [[Astronomy]]
* [[High pressure]]
* [[International Conference on High Energy Physics]]
* [[Introduction to quantum mechanics]]
* [[Introduction to quantum mechanics]]
* [[List of accelerators in particle physics]]
* [[List of particles]]
* [[Magnetic monopole]]
* [[Micro black hole]]
* [[Number theory]]
* [[Resonance (particle physics)]]
* [[Self-consistency principle in high energy physics]]
* [[Non-extensive self-consistent thermodynamical theory]]
* [[Standard Model (mathematical formulation)]]
* [[Stanford Physics Information Retrieval System]]
* [[Timeline of particle physics]]
* [[Unparticle physics]]
* [[Tetraquark]]
* [[Track significance]]
* [[International Conference on Photonic, Electronic and Atomic Collisions]]
}}


==References==
==References==
Line 236: Line 166:
* {{cite book | last=Boyarkin |first=Oleg | title=Advanced Particle Physics Two-Volume Set | publisher=CRC Press | year=2011 | isbn=978-1-4398-0412-4 }}
* {{cite book | last=Boyarkin |first=Oleg | title=Advanced Particle Physics Two-Volume Set | publisher=CRC Press | year=2011 | isbn=978-1-4398-0412-4 }}
* {{cite book |last1=Terranova |first1=Francesco |title=A Modern Primer in Particle and Nuclear Physics. |date=2021 |publisher=Oxford Univ. Press |isbn=978-0192845252}}
* {{cite book |last1=Terranova |first1=Francesco |title=A Modern Primer in Particle and Nuclear Physics. |date=2021 |publisher=Oxford Univ. Press |isbn=978-0192845252}}

==External links==
{{Commons category}}
{{Wikiquote}}
* [http://www.symmetrymagazine.org ''Symmetry'' magazine]
* [http://www.fnal.gov/ Fermilab]
* [http://www.iop.org/publications/iop/2009/page_38211.html Particle physics – it matters] – the [[Institute of Physics]]
* Nobes, Matthew (2002) "Introduction to the Standard Model of Particle Physics" on [[Kuro5hin]]: [http://www.kuro5hin.org/story/2002/5/1/3712/31700 Part 1], [http://www.kuro5hin.org/story/2002/5/14/19363/8142 Part 2], [http://www.kuro5hin.org/story/2002/7/15/173318/784 Part 3a], [http://www.kuro5hin.org/story/2002/8/21/195035/576 Part 3b.]
* [http://public.web.cern.ch/public/ CERN] – European Organization for Nuclear Research
* [https://web.archive.org/web/20190719141632/http://particleadventure.org/ The Particle Adventure] – educational project sponsored by the [[Particle Data Group]] of the [[Lawrence Berkeley National Laboratory]] (LBNL)


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[[Category:Particle physics]]

Revision as of 12:51, 28 July 2022

see caption
A beam of electrons deflected by a magnetic field into a circle, ionizing the gas inside to fluoresce a purple ring

Particle physics or high energy physics is the study of fundamental particles and interactions that constitute matter and radiation. The fundamental particles in the universe are classified in the Standard Model as fermions (matter particles) and bosons (force-carrying particles). There are three generations of fermions, which ordinary matter are made only from the first fermion generation. The first generation consists of up and down quarks composing protons and neutrons, electrons, and electron neutrinos. The three fundamental interactions known to be mediated by bosons are electromagnetism, the weak interaction, and the strong interaction. The conciliation of gravity to the current particle physics theory is not solved; many theories have proposed to do so, such as string theory and supersymmetry theory.

History

Early developments

The idea that all matter is fundamentally composed of elementary particles dates from at least the 6th century BC.[1] In the 19th century, John Dalton, through his work on stoichiometry, concluded that each element of nature was composed of a single, unique type of particle.[2] The word atom, after the Greek word atomos meaning "indivisible", has since then denoted the smallest particle of a chemical element.[citation needed]

Physicists soon discovered that atoms are not, in fact, the fundamental particles of nature, but are conglomerates of even smaller particles, such as the electron. The early 20th century explorations of nuclear physics and quantum physics led to proofs of nuclear fission in 1939 by Lise Meitner (based on experiments by Otto Hahn), and nuclear fusion by Hans Bethe in that same year; both discoveries also led to the development of nuclear weapons.[citation needed]

Quantum mechanics

Throughout the 1950s and 1960s, a bewildering variety of particles were found in collisions of particles from beams of increasingly high energy. It was referred to informally as the "particle zoo". Important discoveries such as the CP violation by James Cronin and Val Fitch brought new questions to matter-antimatter imbalance.[citation needed] After the formulation of the Standard Model during the 1970s, physicists clarified the origin of the particle zoo. The large number of particles was explained as combinations of a (relatively) small number of more fundamental particles and framed in the context of quantum field theories. This reclassification marked the beginning of modern particle physics.[3][4]

Standard Model

The Standard Model of particle physics, listing all elementary particles

The current state of the classification of all elementary particles is explained by the Standard Model, which gained widespread acceptance in the mid-1970s after experimental confirmation of the existence of quarks. It describes the strong, weak, and electromagnetic fundamental interactions, using mediating gauge bosons. The species of gauge bosons are eight gluons,
W
,
W+
and
Z
bosons
, and the photon.[5] The Standard Model also contains 24 fundamental fermions (12 particles and their associated anti-particles), which are the constituents of all matter.[6] Finally, the Standard Model also predicted the existence of a type of boson known as the Higgs boson. On 4 July 2012, physicists with the Large Hadron Collider at CERN announced they had found a new particle that behaves similarly to what is expected from the Higgs boson.[7]

Subatomic particles

A subatomic particle is a particle that composes an atom.[citation needed] Dynamics of these particles are governed by quantum mechanics; they exhibit wave–particle duality, displaying particle-like behaviour under certain experimental conditions and wave-like behaviour in others. In more technical terms, they are described by quantum state vectors in a Hilbert space, which is also treated in quantum field theory. The term elementary particles is applied to those particles that are, according to current understanding, presumed to be indivisible and not composed of other particles.[8] Most particles and their interactions observed to date can be described by the Standard Model.[9]

Quarks and leptons

A Feynman diagram of the
β
 decay
, showing a neutron (n, udd) converted into a proton (p, udu). "u" and "d" are the up and down quarks, "
e
" is the electron, and "
ν
e
" is the electron antineutrino.

Ordinary matter is made from first-generation quarks (up, down) and leptons (electron, electron neutrino).[10] Collectively, quarks and leptons are called fermions, because they have a quantum spin of half-integers (-1/2, 1/2, 3/2, etc.). This cause the fermions to obey the Pauli exclusion principle, where no two particles may occupy the same quantum state.[11] Quarks have fractional elementary electric charge (-1/3 or 2/3)[12] and leptons have whole-numbered electric charge (0 or 1).[citation needed] Quarks also have color charge, which is labeled arbitrarily with no correlation to actual light color as red, green and blue.[13] Because the interactions between the quarks stores energy which can convert to other particles when the quarks are far apart enough, quarks cannot be observed independently. This is called color confinement.[14]

There are three known generations of quarks (up and down, strange and charm, top and bottom) and leptons (electron and its neutrino, muon and its neutrino, tau and its neutrino), with strong indirect evidence that the fourth generation of fermions doesn't exist.[15]

Bosons

Bosons are the mediators or carriers of fundamental interactions, such as electromagnetism, the weak interaction, and the strong interaction.[16] Electromagnetism is mediated by the photon, the quanta of light.[17]: 29–30  The weak interaction is mediated by the W and Z bosons.[18] The strong interaction is mediated by the gluon, which can link quarks together to form composite particles.[19] Due to the aforementioned color confinement, gluons are never observed independently.[20] The Higgs boson gives mass to the W and Z bosons via the Higgs mechanism[21] – the gluon and photon are expected to be massless.[20] All bosons have an integer quantum spin (0 and 1) and can have the same quantum state.[16]

Antiparticles and color charge

Most aforementioned particles have corresponding antiparticles, which compose antimatter. Normal particles have positive lepton or baryon number, and antiparticles have these numbers negative.[22] Most properties of corresponding antiparticles and particles are the same, with a few gets reversed; the electron's antiparticle, positron, has an opposite charge. To differentiate between antiparticles and particles, a plus or negative sign is added in superscript. For example, the electron and the positron are denoted
e
and
e+
.[23] When a particle and an antiparticle interacts with each other, they are annihilated and convert to other particles.[24] Some particles have no antiparticles, such as the photon or gluon.[citation needed]

Quarks and gluons additionally have color charges, which influences the strong interaction. Quark's color charges are called red, green and blue (though the particle itself have no physical color), and in antiquarks are called antired, antigreen and antiblue.[25] The gluon can have eight color charges, which are the result of quarks' interactions to form composite particles (gauge symmetry SU(3)).[26]

Composite

A proton consists of two up quarks and one down quark, linked together by gluons. The quarks' color charge are also visible.

The neutrons and protons in the atomic nuclei are baryons – the neutron is composed of two down quarks and one up quark, and the proton is composed of two up quarks and one down quark.[27] A baryon is composed of three quarks, and a meson is composed of two quarks (one normal, one anti). Baryons and mesons are collectively called hadrons. Quarks inside hadrons are governed by the strong interaction, thus are subjected to quantum chromodynamics (color charges). The bounded quarks must have their color charge to be neutral, or "white" for analogy with mixing the primary colors.[28] More exotic hadrons can have other types, arrangement or number of quarks (tetraquark, pentaquark).[29]

A normal atom is made from protons, neutrons and electrons.[citation needed] By modifying the particles inside a normal atom, exotic atoms can be formed.[30] A simple example would be the hydrogen-4.1, which has one of its electrons replaced with a muon.[31]

Hypothetical

Graviton is a hypothetical particle that can mediate the gravitational interaction, but it has not being detected nor completely reconciled with current theories.[32]

Fundamental interactions

Quantum fields

Conservation laws

Quantum gravity problem

Another major effort is in model building where model builders develop ideas for what physics may lie beyond the Standard Model (at higher energies or smaller distances). There are several powerful experimental reasons to expect new physics, including dark matter and neutrino mass. This work is often motivated by the hierarchy problem and is constrained by existing experimental data. It may involve work on supersymmetry, alternatives to the Higgs mechanism, extra spatial dimensions (such as the Randall–Sundrum models), Preon theory, combinations of these, or other ideas. A third major effort in theoretical particle physics is string theory. String theorists attempt to construct a unified description of quantum mechanics and general relativity by building a theory based on small strings, and branes rather than particles. If the theory is successful, it may be considered a "Theory of Everything".[citation needed]

Experimental evidence

One important branch attempts to better understand the Standard Model and its tests. Theorists make quantitative predictions of observables at collider and astronomical experiments, which along with experimental measurements is used to extract the parameters of the Standard Model with less uncertainty. This work probes the limits of the Standard Model and therefore expands scientific understanding of nature's building blocks. Those efforts are made challenging by the difficulty of calculating high precision quantities in quantum chromodynamics. Some theorists working in this area use the tools of perturbative quantum field theory and effective field theory, referring to themselves as phenomenologists.[citation needed] Others make use of lattice field theory and call themselves lattice theorists.

Facilities

Fermi National Accelerator Laboratory, USA

The world's major particle physics laboratories are:

Many other particle accelerators also exist. The techniques required for modern experimental particle physics are quite varied and complex, constituting a sub-specialty nearly completely distinct from the theoretical side of the field.[citation needed]

See also

References

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Further reading

Introductory reading
Advanced reading