The LHC is the world's largest and highest-energy particle accelerator. The collider is contained in a circular tunnel, with a circumference of 27 kilometers (17 mi), at a depth ranging from 50 to 175 meters (164 to 574 ft) underground.

How long is the Hadron Collider tunnel?

The Large Hadron Collider (LHC) uses an array of 9,300 supercooled electromagnets to guide and accelerate particles – namely protons, around the 27km underground ring at CERN in Geneva, up to speeds extremely close to that of light. At their fastest, these particles travel at around 299.8 million metres per second completing 11,245 laps of this ring every second. This is equivalent to travelling around the circumference of the Earth seven and a half times in one second.

How fast is the Large Hadron Collider?

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The Large Hadron Collider (LHC ) is the world's largest and highest-energy <a href="/wiki/Collider">particle collider </a>.<a href="#cite_note-TheLHC-1">[1] </a> <a href="#cite_note-TGPngm-2">[2] </a> It was built by the <a href="/wiki/CERN">European Organization for Nuclear Research </a>(CERN) between 1998 and 2008 in collaboration with over 10,000 scientists and hundreds of universities and laboratories, as well as more than 100 countries.<a href="#cite_note-3">[3] </a> It lies in a tunnel 27 kilometres (17 mi) in circumference and as deep as 175 metres (574 ft) beneath the <a href="/wiki/France%E2%80%93Switzerland_border">France–Switzerland border </a>near <a href="/wiki/Geneva">Geneva </a>.

The first collisions were achieved in 2010 at an energy of 3.5 <a href="/wiki/Tera-">tera </a><a href="/wiki/Electronvolt">electronvolts </a>(TeV) per beam, about four times the previous world record.<a href="#cite_note-bbc20100330-4">[4] </a> <a href="#cite_note-CERN_Press_1-5">[5] </a> After upgrades it reached 6.5 TeV per beam (13 TeV total collision energy, the present world record).<a href="#cite_note-BBC-6">[6] </a> <a href="#cite_note-7">[7] </a> <a href="#cite_note-2015restart-8">[8] </a> <a href="#cite_note-9">[9] </a> At the end of 2018, it entered a two-year shutdown period for further upgrades.

The collider has four crossing points, around which are positioned <a href="#Detectors">seven detectors </a>, each designed for certain kinds of research. The LHC primarily collides proton beams, but it can also use beams of heavy <a href="/wiki/Ions">ions </a>: <a href="/wiki/Lead">lead </a>–lead collisions and <a href="/wiki/Proton">proton </a>–lead collisions are typically done for one month per year. The aim of the LHC's detectors is to allow physicists to test the predictions of different theories of <a href="/wiki/Particle_physics">particle physics </a>, including measuring the properties of the <a href="/wiki/Higgs_boson">Higgs boson </a><a href="#cite_note-10">[10] </a> and searching for the large family of new particles predicted by <a href="/wiki/Supersymmetry">supersymmetric theories </a>,<a href="#cite_note-11">[11] </a> as well as other <a href="/wiki/List_of_unsolved_problems_in_physics#High-energy_physics/particle_physics">unsolved questions of physics </a>.

<ul><li><a href="#Background">1 Background </a> </li><li><a href="#Purpose">2 Purpose </a> </li><li><a href="#Design">3 Design </a><ul><li><a href="#Detectors">3.1 Detectors </a> </li><li><a href="#Computing_and_analysis_facilities">3.2 Computing and analysis facilities </a> </li> </ul> </li><li><a href="#Operational_history">4 Operational history </a><ul><li><a href="#Construction">4.1 Construction </a><ul><li><a href="#Operational_challenges">4.1.1 Operational challenges </a> </li><li><a href="#Cost">4.1.2 Cost </a> </li><li><a href="#Construction_accidents_and_delays">4.1.3 Construction accidents and delays </a> </li><li><a href="#Initial_lower_magnet_currents">4.1.4 Initial lower magnet currents </a> </li> </ul> </li><li><a href="#Inaugural_tests_(2008)">4.2 Inaugural tests (2008) </a><ul><li><a href="#Quench_incident">4.2.1 Quench incident </a> </li> </ul> </li><li><a href="#Run_1:_first_operational_run_(2009–2013)">4.3 Run 1: first operational run (2009–2013) </a> </li><li><a href="#Long_Shutdown_1_(2013–2015)">4.4 Long Shutdown 1 (2013–2015) </a> </li><li><a href="#Run_2:_second_operational_run_(2015–2018)">4.5 Run 2: second operational run (2015–2018) </a> </li><li><a href="#Long_Shutdown_2_(2018–2021)_and_beyond">4.6 Long Shutdown 2 (2018–2021) and beyond </a> </li> </ul> </li><li><a href="#Timeline_of_operations">5 Timeline of operations </a> </li><li><a href="#Findings_and_discoveries">6 Findings and discoveries </a><ul><li><a href="#First_run_(data_taken_2009–2013)">6.1 First run (data taken 2009–2013) </a> </li><li><a href="#Second_run_(2015-2018)">6.2 Second run (2015-2018) </a> </li> </ul> </li><li><a href='#Planned_"high-luminosity"_upgrade'>7 Planned "high-luminosity" upgrade </a> </li><li><a href="#Safety_of_particle_collisions">8 Safety of particle collisions </a> </li><li><a href="#Popular_culture">9 Popular culture </a><ul><li><a href="#Fiction">9.1 Fiction </a> </li> </ul> </li><li><a href="#See_also">10 See also </a> </li><li><a href="#References">11 References </a> </li><li><a href="#External_links">12 External links </a> </li> </ul>

The term <a href="/wiki/Hadron">hadron </a> refers to <a href="/wiki/Subatomic_particle">subatomic </a><a href="/wiki/Composite_particle">composite particles </a>composed of <a href="/wiki/Quark">quarks </a><a href="/wiki/Bound_state">held together </a>by the <a href="/wiki/Strong_force">strong force </a>(as <a href="/wiki/Atom">atoms </a>and <a href="/wiki/Molecule">molecules </a>are held together by the <a href="/wiki/Electromagnetic_force">electromagnetic force </a>).<a href="#cite_note-12">[12] </a> The best-known hadrons are the <a href="/wiki/Baryon">baryons </a>such as <a href="/wiki/Proton">protons </a>and <a href="/wiki/Neutron">neutrons </a>; hadrons also include <a href="/wiki/Meson">mesons </a>such as the <a href="/wiki/Pion">pion </a>and <a href="/wiki/Kaon">kaon </a>, which were discovered during <a href="/wiki/Cosmic_ray">cosmic ray </a>experiments in the late 1940s and early 1950s.<a href="#cite_note-13">[13] </a>

A <a href="/wiki/Collider">collider </a> is a type of a <a href="/wiki/Particle_accelerator">particle accelerator </a>with two directed beams of <a href="/wiki/Particle">particles </a>. In <a href="/wiki/Particle_physics">particle physics </a>, colliders are used as a research tool: they accelerate particles to very high <a href="/wiki/Kinetic_energy">kinetic energies </a>and let them impact other particles.<a href="#cite_note-TheLHC-1">[1] </a> Analysis of the byproducts of these collisions gives scientists good evidence of the structure of the <a href="/wiki/Subatomic">subatomic </a>world and the laws of nature governing it. Many of these byproducts are produced only by high-energy collisions, and they decay after very short periods of time. Thus many of them are hard or nearly impossible to study in other ways.<a href="#cite_note-14">[14] </a>

Many <a href="/wiki/Physicist">physicists </a>hope that the Large Hadron Collider will help answer some of the <a href="/wiki/Unanswered_questions_in_physics">fundamental open questions </a>in physics, which concern the basic laws governing the interactions and forces among the <a href="/wiki/Elementary_particle">elementary objects </a>, the deep structure of space and time, and in particular the interrelation between <a href="/wiki/Quantum_mechanics">quantum mechanics </a>and <a href="/wiki/General_relativity">general relativity </a>.<a href="#cite_note-15">[15] </a>

Data are also needed from <a href="/wiki/High-energy_particle">high-energy particle </a>experiments to suggest which versions of current scientific models are more likely to be correct – in particular to choose between the <a href="/wiki/Standard_Model">Standard Model </a>and <a href="/wiki/Higgsless_model">Higgsless model </a>and to validate their predictions and allow further theoretical development.

Issues explored by LHC collisions include:<a href="#cite_note-16">[16] </a> <a href="#cite_note-17">[17] </a>

<ul><li>Is the <a href="/wiki/Mass">mass </a>of <a href="/wiki/Elementary_particle">elementary particles </a>being generated by the <a href="/wiki/Higgs_mechanism">Higgs mechanism </a>via <a href="/wiki/Electroweak">electroweak </a><a href="/wiki/Spontaneous_symmetry_breaking">symmetry breaking </a>?<a href="#cite_note-18">[18] </a> It was expected that the collider experiments will either demonstrate or rule out the existence of the elusive <a href="/wiki/Higgs_boson">Higgs boson </a>, thereby allowing physicists to consider whether the Standard Model or its Higgsless alternatives are more likely to be correct.<a href="#cite_note-19">[19] </a> <a href="#cite_note-quigg-20">[20] </a> </li><li>Is <a href="/wiki/Supersymmetry">supersymmetry </a>, an <a href="/wiki/Beyond_the_Standard_Model">extension of the Standard Model </a>and <a href="/wiki/Super-Poincar%C3%A9_algebra">Poincaré symmetry </a>, realized in nature, implying that all known particles have <a href="/wiki/Superpartner">supersymmetric partners </a>?<a href="#cite_note-21">[21] </a> <a href="#cite_note-22">[22] </a> <a href="#cite_note-23">[23] </a> </li><li>Are there <a href="/wiki/Superstring_theory">extra dimensions </a>,<a href="#cite_note-24">[24] </a> as predicted by various models based on <a href="/wiki/String_theory">string theory </a>, and can we detect them?<a href="#cite_note-25">[25] </a> </li><li>What is the nature of the <a href="/wiki/Dark_matter">dark matter </a>that appears to account for 27% of the mass-energy of the <a href="/wiki/Universe">universe </a>? </li> </ul>

Other open questions that may be explored using high-energy particle collisions:

<ul><li>It is already known that <a href="/wiki/Electromagnetism">electromagnetism </a>and the <a href="/wiki/Weak_nuclear_force">weak nuclear force </a>are different manifestations of a single force called the electroweak force. The LHC may clarify whether the electroweak force and the <a href="/wiki/Strong_nuclear_force">strong nuclear force </a>are similarly just different manifestations of one universal unified force, as predicted by various <a href="/wiki/Grand_unification_theory">Grand Unification Theories </a>. </li><li>Why is the fourth fundamental force (<a href="/wiki/Gravitation">gravity </a>) so many orders of magnitude weaker than the other three <a href="/wiki/Fundamental_interaction">fundamental forces </a>? See also <a href="/wiki/Hierarchy_problem#The_Higgs_mass">Hierarchy problem </a>. </li><li>Are there additional sources of <a href="/wiki/Quark">quark </a><a href="/wiki/Flavour_(particle_physics)">flavour </a>mixing, beyond those already present within the <a href="/wiki/Standard_Model">Standard Model </a>? </li><li>Why are there apparent violations of the <a href="/wiki/Symmetry_in_physics">symmetry </a>between matter and <a href="/wiki/Antimatter">antimatter </a>? See also <a href="/wiki/CP_violation">CP violation </a>. </li><li>What are the nature and properties of <a href="/wiki/Quark%E2%80%93gluon_plasma">quark–gluon plasma </a>, thought to have existed in the <a href="/wiki/Early_universe">early universe </a>and in certain <a href="/wiki/Compact_star">compact </a>and <a href="/wiki/Strange_matter">strange </a>astronomical objects today? This will be investigated by heavy ion collisions , mainly in <a href="/wiki/A_Large_Ion_Collider_Experiment">ALICE </a>, but also in <a href="/wiki/Compact_Muon_Solenoid">CMS </a>, <a href="/wiki/ATLAS_experiment">ATLAS </a>and <a href="/wiki/LHCb">LHCb </a>. First observed in 2010, findings published in 2012 confirmed the phenomenon of <a href="/wiki/Jet_quenching">jet quenching </a>in heavy-ion collisions.<a href="#cite_note-26">[26] </a> <a href="#cite_note-27">[27] </a> <a href="#cite_note-28">[28] </a> </li> </ul>

The collider is contained in a circular tunnel, with a circumference of 26.7 kilometres (16.6 mi), at a depth ranging from 50 to 175 metres (164 to 574 ft) underground. The variation in depth was deliberate, to reduce the amount of tunnel that lies under the <a href="/wiki/Jura_Mountains">Jura Mountains </a>to avoid having to excavate a vertical access shaft there. A tunnel was chosen to avoid having to purchase expensive land on the surface, which would also have an impact on the landscape and to take advantage of the shielding against background radiation that the earth's crust provides.<a href="#cite_note-29">[29] </a>

The 3.8-metre (12 ft) wide concrete-lined tunnel, constructed between 1983 and 1988, was formerly used to house the <a href="/wiki/Large_Electron%E2%80%93Positron_Collider">Large Electron–Positron Collider </a>.<a href="#cite_note-30">[30] </a> The tunnel crosses the border between Switzerland and France at four points, with most of it in France. Surface buildings hold ancillary equipment such as compressors, ventilation equipment, control electronics and refrigeration plants.

The collider tunnel contains two adjacent parallel <a href="/wiki/Beamline">beamlines </a>(or beam pipes ) each containing a beam, which travel in opposite directions around the ring. The beams intersect at four points around the ring, which is where the particle collisions take place. Some 1,232 <a href="/wiki/Dipole_magnet">dipole magnets </a>keep the beams on their circular path (see image<a href="#cite_note-31">[31] </a> ), while an additional 392 <a href="/wiki/Quadrupole_magnet">quadrupole magnets </a>are used to keep the beams focused, with stronger quadrupole magnets close to the intersection points in order to maximize the chances of interaction where the two beams cross. Magnets of <a href="/wiki/Multipole_expansion">higher multipole orders </a>are used to correct smaller imperfections in the field geometry. In total, about 10,000 <a href="/wiki/Superconducting_magnet">superconducting magnets </a>are installed, with the dipole magnets having a mass of over 27 tonnes.<a href="#cite_note-LHC_2008-20013-32">[32] </a> Approximately 96 tonnes of <a href="/wiki/Superfluid_helium-4">superfluid helium-4 </a>is needed to keep the magnets, made of copper-clad <a href="/wiki/Niobium-titanium">niobium-titanium </a>, at their <a href="/wiki/Operating_temperature">operating temperature </a>of 1.9 K (−271.25 °C), making the LHC the largest <a href="/wiki/Cryogenics">cryogenic </a>facility in the world at liquid helium temperature. LHC uses 470 tonnes of Nb–Ti superconductor.<a href="#cite_note-33">[33] </a>

During LHC operations, the CERN site draws roughly 200 <a href="/wiki/Megawatt">MW </a>of electrical power from the French <a href="/wiki/Electrical_grid">electrical grid </a>, which, for comparison, is about one-third the energy consumption of the city of Geneva; the LHC accelerator and detectors draw about 120 MW thereof.<a href="#cite_note-34">[34] </a> Each day of its operation generates 140 <a href="/wiki/Terabyte">terabytes </a>of data.<a href="#cite_note-35">[35] </a>

When running at the current energy record of 6.5 TeV per proton,<a href="#cite_note-36">[36] </a> once or twice a day, as the protons are accelerated from 450 <a href="/wiki/Electron_volt">GeV </a>to 6.5 <a href="/wiki/Electron_volt">TeV </a>, the field of the superconducting dipole magnets is increased from 0.54 to 7.7 <a href="/wiki/Tesla_(unit)">teslas (T) </a> . The protons each have an <a href="/wiki/Energy">energy </a>of 6.5 TeV, giving a total collision energy of 13 TeV. At this energy, the protons have a <a href="/wiki/Lorentz_factor">Lorentz factor </a>of about 6,930 and move at about 0.999999 990 c , or about 3.1 m/s (11 km/h) slower than the <a href="/wiki/Speed_of_light">speed of light </a>(c ). It takes less than 90 <a href="/wiki/Microsecond">microseconds </a>(μs) for a proton to travel 26.7 km around the main ring. This results in 11,245 revolutions per second for protons whether the particles are at low or high energy in the main ring, since the speed difference between these energies is beyond the fifth decimal.<a href="#cite_note-37">[37] </a>

Rather than having continuous beams, the protons are bunched together, into up to 2,808 bunches , with 115 billion protons in each bunch so that interactions between the two beams take place at discrete intervals, mainly 25 <a href="/wiki/Nanosecond">nanoseconds </a>(ns) apart, providing a bunch collision rate of 40 MHz. It was operated with fewer bunches in the first years. The design <a href="/wiki/Luminosity_(scattering_theory)">luminosity </a>of the LHC is 1034 cm−2 s−1 ,<a href="#cite_note-38">[38] </a> which was first reached in June 2016.<a href="#cite_note-designlumireached-39">[39] </a> By 2017, twice this value was achieved.<a href="#cite_note-endof2017-40">[40] </a>

Before being injected into the main accelerator, the particles are prepared by a series of systems that successively increase their energy. The first system is the <a href="/wiki/Linear_particle_accelerator">linear particle accelerator </a><a href="/wiki/LINAC_4">LINAC 4 </a>generating 160-MeV negative hydrogen ions (H− ions), which feeds the <a href="/wiki/Proton_Synchrotron_Booster">Proton Synchrotron Booster </a>(PSB). There, both electrons are stripped of the hydrogen ions leaving only the nucleus containing one proton. Protons are then accelerated to 2 GeV and injected into the <a href="/wiki/Proton_Synchrotron">Proton Synchrotron </a>(PS), where they are accelerated to 26 GeV. Finally, the <a href="/wiki/Super_Proton_Synchrotron">Super Proton Synchrotron </a>(SPS) is used to increase their energy further to 450 GeV before they are at last injected (over a period of several minutes) into the main ring. Here, the proton bunches are accumulated, accelerated (over a period of 20 minutes ) to their peak energy, and finally circulated for 5 to 24 hours while collisions occur at the four intersection points.<a href="#cite_note-irfu1-41">[41] </a>

The LHC physics programme is mainly based on proton–proton collisions. However, shorter running periods, typically one month per year, heavy-ion collisions are included in the programme. While lighter ions are considered as well, the baseline scheme deals with <a href="/wiki/Lead">lead </a>ions<a href="#cite_note-42">[42] </a> (see <a href="/wiki/A_Large_Ion_Collider_Experiment">A Large Ion Collider Experiment </a>). The lead ions are first accelerated by the linear accelerator <a href="/wiki/LINAC_3">LINAC 3 </a>, and the <a href="/wiki/Low_Energy_Ion_Ring">Low Energy Ion Ring </a>(LEIR) is used as an ion storage and cooler unit. The ions are then further accelerated by the PS and SPS before being injected into LHC ring, where they reach an energy of 2.3 TeV per <a href="/wiki/Nucleon">nucleon </a>(or 522 TeV per ion),<a href="#cite_note-43">[43] </a> higher than the energies reached by the <a href="/wiki/Relativistic_Heavy_Ion_Collider">Relativistic Heavy Ion Collider </a>. The aim of the heavy-ion programme is to investigate <a href="/wiki/Quark%E2%80%93gluon_plasma">quark–gluon plasma </a>, which existed in the <a href="/wiki/Early_universe">early universe </a>.<a href="#cite_note-44">[44] </a>

Seven detectors have been constructed at the LHC, located underground in large caverns excavated at the LHC's intersection points. Two of them, the <a href="/wiki/ATLAS_experiment">ATLAS experiment </a>and the <a href="/wiki/Compact_Muon_Solenoid">Compact Muon Solenoid </a>(CMS), are large general-purpose <a href="/wiki/Particle_detector">particle detectors </a>.<a href="#cite_note-TGPngm-2">[2] </a> <a href="/wiki/A_Large_Ion_Collider_Experiment">ALICE </a>and <a href="/wiki/LHCb">LHCb </a>have more specific roles and the last three, <a href="/wiki/TOTEM">TOTEM </a>, <a href="/wiki/MoEDAL">MoEDAL </a>and <a href="/wiki/LHCf">LHCf </a>, are very much smaller and are for very specialized research. The ATLAS and CMS experiments discovered the Higgs boson, which is strong evidence that the Standard Model has the correct mechanism of giving mass to elementary particles.<a href="#cite_note-45">[45] </a>

Computing and analysis facilities  [  edit  ]

Data produced by LHC, as well as LHC-related simulation, were estimated at approximately 15 <a href="/wiki/Petabyte">petabytes </a>per year (max throughput while running is not stated)<a href="#cite_note-46">[46] </a> —a major challenge in its own right at the time.

The <a href="/wiki/LHC_Computing_Grid">LHC Computing Grid </a><a href="#cite_note-citesciences-47">[47] </a> was constructed as part of the LHC design, to handle the massive amounts of data expected for its collisions. It is an international collaborative project that consists of a grid-based <a href="/wiki/Computer_network">computer network </a>infrastructure initially connecting 140 computing centres in 35 countries (over 170 in 36 countries as of 2012<a href="https://en.wikipedia.org/w/index.php?title=Large_Hadron_Collider&action=edit">[update] </a> ). It was designed by <a href="/wiki/CERN">CERN </a>to handle the significant volume of data produced by LHC experiments,<a href="#cite_note-wwlhccg-48">[48] </a> <a href="#cite_note-gridabout-49">[49] </a> incorporating both private fibre optic cable links and existing high-speed portions of the public <a href="/wiki/Internet">Internet </a>to enable data transfer from CERN to academic institutions around the world.<a href="#cite_note-50">[50] </a> The <a href="/wiki/Open_Science_Grid">Open Science Grid </a>is used as the primary infrastructure in the United States, and also as part of an interoperable federation with the LHC Computing Grid.

The <a href="/wiki/Distributed_computing">distributed computing </a>project <a href="/wiki/LHC@home">LHC@home </a>was started to support the construction and calibration of the LHC. The project uses the <a href="/wiki/Berkeley_Open_Infrastructure_for_Network_Computing">BOINC </a>platform, enabling anybody with an Internet connection and a computer running <a href="/wiki/OS_X">Mac OS X </a>, <a href="/wiki/Windows">Windows </a>or <a href="/wiki/Linux">Linux </a>to use their computer's idle time to simulate how particles will travel in the beam pipes. With this information, the scientists are able to determine how the magnets should be calibrated to gain the most stable "orbit" of the beams in the ring.<a href="#cite_note-LHC@home-51">[51] </a> In August 2011, a second application (Test4Theory) went live which performs simulations against which to compare actual test data, to determine confidence levels of the results.

By 2012, data from over 6 quadrillion (6 x 1015 ) LHC proton-proton collisions had been analysed,<a href="#cite_note-collisionnumber-52">[52] </a> LHC collision data was being produced at approximately 25 <a href="/wiki/Petabyte">petabytes </a>per year, and the LHC Computing Grid had become the world's largest <a href="/wiki/Computing_grid">computing grid </a>in 2012, comprising over 170 computing facilities in a <a href="/wiki/Distributed_computing">worldwide network </a>across 36 countries.<a href="#cite_note-msnbc-discovery-53">[53] </a> <a href="#cite_note-LHGG_main_page-54">[54] </a> <a href="#cite_note-lhc_comp_public_overview-55">[55] </a>

The LHC first went live on 10 September 2008,<a href="#cite_note-CERNPressFirstbeam-56">[56] </a> but initial testing was delayed for 14 months from 19 September 2008 to 20 November 2009, following a <a href="/wiki/Magnet_quench">magnet quench </a>incident that caused extensive damage to over 50 <a href="/wiki/Superconducting_magnet">superconducting magnets </a>, their mountings, and the <a href="/wiki/Beamline">vacuum pipe </a>.<a href="#cite_note-BBC_2008-57">[57] </a> <a href="#cite_note-perdue_2008-58">[58] </a> <a href="#cite_note-59">[59] </a> <a href="#cite_note-LHC-is-back-60">[60] </a> <a href="#cite_note-CERN20091123-61">[61] </a>

During its first run (2010–2013), the LHC collided two opposing <a href="/wiki/Charged_particle_beam">particle beams </a>of either <a href="/wiki/Proton">protons </a>at up to 4 <a href="/wiki/Electronvolt">teraelectronvolts </a>(4 TeV or 0.64 <a href="/wiki/Joule">microjoules </a>) , or <a href="/wiki/Lead">lead </a><a href="/wiki/Atomic_nucleus">nuclei </a>(574 TeV per nucleus, or 2.76 TeV per <a href="/wiki/Nucleon">nucleon </a>).<a href="#cite_note-LHCbooklet-62">[62] </a> <a href="#cite_note-63">[63] </a> Its first run discoveries included the <a href="/wiki/Search_for_the_Higgs_boson">long-sought </a><a href="/wiki/Higgs_boson">Higgs boson </a>, several composite particles (<a href="/wiki/Hadron">hadrons </a>) like the χb (3P) <a href="/wiki/Bottomonium">bottomonium </a>state, the first creation of a <a href="/wiki/Quark%E2%80%93gluon_plasma">quark–gluon plasma </a>, and the first observations of the very rare decay of the <a href="/wiki/Strange_B_meson">Bs meson </a>into two <a href="/wiki/Muon">muons </a>(Bs 0 → μ+ μ− ), which challenged the validity of existing models of <a href="/wiki/Supersymmetry">supersymmetry </a>.<a href="#cite_note-64">[64] </a>

The size of the LHC constitutes an exceptional engineering challenge with unique operational issues on account of the amount of energy stored in the magnets and the beams.<a href="#cite_note-irfu1-41">[41] </a> <a href="#cite_note-65">[65] </a> While operating, the total <a href="/wiki/Superconducting_magnetic_energy_storage">energy stored in the magnets </a>is 10 GJ (2,400 kilograms of TNT) and the total energy carried by the two beams reaches 724 MJ (173 kilograms of TNT).<a href="#cite_note-66">[66] </a>

Loss of only one ten-millionth part (10−7 ) of the beam is sufficient to <a href="/wiki/Magnet_quench">quench </a>a <a href="/wiki/Superconducting_magnet">superconducting magnet </a>, while each of the two <a href="/wiki/Beam_dump">beam dumps </a>must absorb 362 MJ (87 kilograms of TNT). These energies are carried by very little matter: under nominal operating conditions (2,808 bunches per beam, 1.15×1011 protons per bunch), the beam pipes contain 1.0×10−9 gram of hydrogen, which, in <a href="/wiki/Standard_conditions_for_temperature_and_pressure">standard conditions for temperature and pressure </a>, would fill the volume of one grain of fine sand.

With a budget of €7.5 billion (approx. $9bn or £6.19bn as of June 2010<a href="https://en.wikipedia.org/w/index.php?title=Large_Hadron_Collider&action=edit">[update] </a> ), the LHC is one of the most expensive scientific instruments<a href="#cite_note-TheLHC-1">[1] </a> ever built.<a href="#cite_note-67">[67] </a> The total cost of the project is expected to be of the order of 4.6bn <a href="/wiki/Swiss_franc">Swiss francs </a>(SFr) (approx. $4.4bn, €3.1bn, or £2.8bn as of January 2010<a href="https://en.wikipedia.org/w/index.php?title=Large_Hadron_Collider&action=edit">[update] </a> ) for the accelerator and 1.16bn (SFr) (approx. $1.1bn, €0.8bn, or £0.7bn as of January 2010<a href="https://en.wikipedia.org/w/index.php?title=Large_Hadron_Collider&action=edit">[update] </a> ) for the CERN contribution to the experiments.<a href="#cite_note-68">[68] </a>

The construction of LHC was approved in 1995 with a budget of SFr 2.6bn, with another SFr 210M toward the experiments. However, cost overruns, estimated in a major review in 2001 at around SFr 480M for the accelerator, and SFr 50M for the experiments, along with a reduction in CERN's budget, pushed the completion date from 2005 to April 2007.<a href="#cite_note-69">[69] </a> The superconducting magnets were responsible for SFr 180M of the cost increase. There were also further costs and delays owing to engineering difficulties encountered while building the cavern for the <a href="/wiki/Compact_Muon_Solenoid">Compact Muon Solenoid </a>,<a href="#cite_note-70">[70] </a> and also due to magnet supports which were insufficiently strongly designed and failed their initial testing (2007) and damage from a <a href="/wiki/Magnet_quench">magnet quench </a>and <a href="/wiki/Liquid_helium">liquid helium </a>escape (inaugural testing, 2008) (see: <a href="#Construction_accidents_and_delays">Construction accidents and delays </a>) .<a href="#cite_note-71">[71] </a> Because electricity costs are lower during the summer, the LHC normally does not operate over the winter months,<a href="#cite_note-72">[72] </a> although exceptions over the 2009/10 and 2012/2013 winters were made to make up for the 2008 start-up delays and to improve precision of measurements of the new particle discovered in 2012, respectively.

Construction accidents and delays  [  edit  ]

<ul><li>On 25 October 2005, José Pereira Lages, a technician, was killed in the LHC when a <a href="/wiki/Switchgear">switchgear </a>that was being transported fell on top of him.<a href="#cite_note-73">[73] </a> </li><li>On 27 March 2007, a cryogenic magnet support designed and provided by <a href="/wiki/Fermilab">Fermilab </a>and <a href="/wiki/KEK">KEK </a>broke during an initial pressure test involving one of the LHC's inner triplet (focusing quadrupole) magnet assemblies. No one was injured. Fermilab director Pier Oddone stated "In this case we are dumbfounded that we missed some very simple balance of forces". The fault had been present in the original design, and remained during four engineering reviews over the following years.<a href="#cite_note-74">[74] </a> Analysis revealed that its design, made as thin as possible for better insulation, was not strong enough to withstand the forces generated during pressure testing. Details are available in a statement from Fermilab, with which CERN is in agreement.<a href="#cite_note-75">[75] </a> <a href="#cite_note-76">[76] </a> Repairing the broken magnet and reinforcing the eight identical assemblies used by LHC delayed the start-up date, then planned for November 2007. </li><li>On 19 September 2008, during initial testing, a faulty electrical connection led to a <a href="/wiki/Magnet_quench">magnet quench </a>(the sudden loss of a <a href="/wiki/Superconducting_magnet">superconducting magnet </a>'s superconducting ability owing to warming or <a href="/wiki/Electric_field">electric field </a>effects). Six tonnes of supercooled <a href="/wiki/Liquid_helium">liquid helium </a>—used to cool the magnets—escaped, with sufficient force to break 10-ton magnets nearby from their mountings, and caused considerable damage and contamination of the vacuum tube (see <a href="#Quench_incident">2008 quench incident </a>) ; repairs and safety checks caused a delay of around 14 months.<a href="#cite_note-77">[77] </a> <a href="#cite_note-CERNsummer-78">[78] </a> <a href="#cite_note-79">[79] </a> </li><li>Two vacuum leaks were found in July 2009, and the start of operations was further postponed to mid-November 2009.<a href="#cite_note-July_2009_leaks-80">[80] </a> </li> </ul>

Initial lower magnet currents  [  edit  ]

In both of its runs (2010 to 2012 and 2015), the LHC was initially run at energies below its planned operating energy, and ramped up to just 2 x 4 TeV energy on its first run and 2 x 6.5 TeV on its second run, below the design energy of 2 x 7 TeV. This is because massive superconducting magnets require considerable <a href='/wiki/Superconducting_magnet#Magnet_"training"'>magnet training </a>to handle the high currents involved without <a href="/wiki/Magnet_quench">losing their superconducting ability </a>, and the high currents are necessary to allow a high proton energy. The "training" process involves repeatedly running the magnets with lower currents to provoke any quenches or minute movements that may result. It also takes time to cool down magnets to their operating temperature of around 1.9 <a href="/wiki/Kelvin">K </a>(close to <a href="/wiki/Absolute_zero">absolute zero </a>). Over time the magnet "beds in" and ceases to quench at these lesser currents and can handle the full design current without quenching; CERN media describe the magnets as "shaking out" the unavoidable tiny manufacturing imperfections in their crystals and positions that had initially impaired their ability to handle their planned currents. The magnets, over time and with training, gradually become able to handle their full planned currents without quenching.<a href="#cite_note-why13tev-81">[81] </a> <a href="#cite_note-training2-82">[82] </a>

The first beam was circulated through the <a href="/wiki/Collider">collider </a>on the morning of 10 September 2008.<a href="#cite_note-rincon-83">[83] </a> <a href="/wiki/CERN">CERN </a>successfully fired the protons around the tunnel in stages, three kilometres at a time. The particles were fired in a clockwise direction into the accelerator and successfully steered around it at 10:28 local time.<a href="#cite_note-CERNPressFirstbeam-56">[56] </a> The LHC successfully completed its major test: after a series of trial runs, two white dots flashed on a computer screen showing the protons travelled the full length of the collider. It took less than one hour to guide the stream of particles around its inaugural circuit.<a href="#cite_note-84">[84] </a> CERN next successfully sent a beam of protons in an anticlockwise direction, taking slightly longer at one and a half hours owing to a problem with the <a href="/wiki/Cryogenics">cryogenics </a>, with the full circuit being completed at 14:59.

<ul><li><a href="https://en.wikinews.org/wiki/CERN_says_repairs_to_LHC_particle_accelerator_to_cost_US$21_million">CERN says repairs to LHC particle accelerator to cost US$21 million </a> </li> </ul>

On 19 September 2008, a <a href="/wiki/Magnet_quench">magnet quench </a>occurred in about 100 bending <a href="/wiki/Magnet">magnets </a>in sectors 3 and 4, where an electrical fault led to a loss of approximately six tonnes of <a href="/wiki/Liquid_helium">liquid helium </a>(the magnets' <a href="/wiki/Cryogenic">cryogenic </a>coolant), which was vented into the tunnel. The escaping vapour expanded with explosive force, damaging a total of 53 <a href="/wiki/Superconducting_magnet">superconducting magnets </a>and their mountings, and contaminating the <a href="/wiki/Beamline">vacuum pipe </a>, which also lost vacuum conditions.<a href="#cite_note-BBC_2008-57">[57] </a> <a href="#cite_note-perdue_2008-58">[58] </a> <a href="#cite_note-interim_technical_report-85">[85] </a>

Shortly after the incident, CERN reported that the most likely cause of the problem was a <a href="/wiki/Electrical_fault">faulty electrical connection </a>between two magnets, and that – owing to the time needed to warm up the affected sectors and then cool them back down to operating temperature – it would take at least two months to fix.<a href="#cite_note-86">[86] </a> CERN released an interim technical report<a href="#cite_note-interim_technical_report-85">[85] </a> and preliminary analysis of the incident on 15 and 16 October 2008 respectively,<a href="#cite_note-87">[87] </a> and a more detailed report on 5 December 2008.<a href="#cite_note-CERNsummer-78">[78] </a> The analysis of the incident by CERN confirmed that an electrical fault had indeed been the cause. The faulty electrical connection had led (correctly) to a <a href="/wiki/Failsafe">failsafe </a>power abort of the electrical systems powering the superconducting magnets, but had also caused an <a href="/wiki/Electric_arc">electric arc </a>(or discharge) which damaged the integrity of the supercooled helium's enclosure and vacuum insulation, causing the coolant's temperature and pressure to rapidly rise beyond the ability of the safety systems to contain it,<a href="#cite_note-interim_technical_report-85">[85] </a> and leading to a temperature rise of about 100 degrees <a href="/wiki/Celsius">Celsius </a>in some of the affected magnets. Energy stored in the superconducting magnets and <a href="/wiki/Electrical_noise">electrical noise </a><a href="/wiki/Electromagnetic_induction">induced </a>in other quench detectors also played a role in the rapid heating. Around two <a href="/wiki/Tonne">tonnes </a>of liquid helium escaped explosively before detectors triggered an emergency stop, and a further four tonnes leaked at lower pressure in the aftermath.<a href="#cite_note-interim_technical_report-85">[85] </a> A total of 53 magnets were damaged in the incident and were repaired or replaced during the winter shutdown.<a href="#cite_note-88">[88] </a> This accident was thoroughly discussed in a 22 February 2010 Superconductor Science and Technology article by CERN physicist <a href="/wiki/Lucio_Rossi">Lucio Rossi </a>.<a href="#cite_note-89">[89] </a>

In the original schedule for LHC commissioning, the first "modest" high-energy collisions at a <a href="/wiki/Center_of_momentum_frame">centre-of-mass </a>energy of 900 GeV were expected to take place before the end of September 2008, and the LHC was expected to be operating at 10 TeV by the end of 2008.<a href="#cite_note-90">[90] </a> However, owing to the delay caused by the incident, the collider was not operational until November 2009.<a href="#cite_note-CERN_September-91">[91] </a> Despite the delay, LHC was officially inaugurated on 21 October 2008, in the presence of political leaders, science ministers from CERN's 20 Member States, CERN officials, and members of the worldwide scientific community.<a href="#cite_note-92">[92] </a>

Most of 2009 was spent on repairs and reviews from the damage caused by the quench incident, along with two further vacuum leaks identified in July 2009; this pushed the start of operations to November of that year.<a href="#cite_note-July_2009_leaks-80">[80] </a>

Run 1: first operational run (2009–2013)  [  edit  ]

On 20 November 2009, low-energy beams circulated in the tunnel for the first time since the incident, and shortly after, on 30 November, the LHC achieved 1.18 TeV per beam to become the world's highest-energy particle accelerator, beating the <a href="/wiki/Tevatron">Tevatron </a>'s previous record of 0.98 TeV per beam held for eight years.<a href="#cite_note-30_Nov_press-94">[94] </a>

The early part of 2010 saw the continued ramp-up of beam in energies and early physics experiments towards 3.5 TeV per beam and on 30 March 2010, LHC set a new record for high-energy collisions by colliding proton beams at a combined energy level of 7 TeV. The attempt was the third that day, after two unsuccessful attempts in which the protons had to be "dumped" from the collider and new beams had to be injected.<a href="#cite_note-95">[95] </a> This also marked the start of the main research programme.

The first proton run ended on 4 November 2010. A run with lead ions started on 8 November 2010, and ended on 6 December 2010,<a href="#cite_note-96">[96] </a> allowing the ALICE experiment to study matter under extreme conditions similar to those shortly after the Big Bang.<a href="#cite_note-97">[97] </a>

CERN originally planned that the LHC would run through to the end of 2012, with a short break at the end of 2011 to allow for an increase in beam energy from 3.5 to 4 TeV per beam.<a href="#cite_note-CERN_Press_1-5">[5] </a> At the end of 2012, the LHC was planned to get shut down until around 2015 to allow upgrade to a planned beam energy of 7 TeV per beam.<a href="#cite_note-98">[98] </a> In late 2012, in light of the July 2012 discovery of the <a href="/wiki/Higgs_boson">Higgs boson </a>, the shutdown was postponed for some weeks into early 2013, to allow additional data to be obtained before shutdown.

Long Shutdown 1 (2013–2015)  [  edit  ]

The LHC was shut down on 13 February 2013 for its 2-year upgrade called Long Shutdown 1 (LS1), which was to touch on many aspects of the LHC: enabling collisions at 14 TeV, enhancing its detectors and pre-accelerators (the Proton Synchrotron and Super Proton Synchrotron), as well as replacing its ventilation system and 100 km (62 mi) of cabling impaired by high-energy collisions from its first run.<a href="#cite_note-99">[99] </a> The upgraded collider began its long start-up and testing process in June 2014, with the Proton Synchrotron Booster starting on 2 June 2014, the final interconnection between magnets completing and the Proton Synchrotron circulating particles on 18 June 2014, and the first section of the main LHC supermagnet system reaching operating temperature of 1.9 K (−271.25 °C), a few days later.<a href="#cite_note-100">[100] </a> Due to the slow progress with <a href='/wiki/Superconducting_magnet#Magnet_"training"'>"training" </a>the superconducting magnets, it was decided to start the second run with a lower energy of 6.5 TeV per beam, corresponding to a current of 11,000 <a href="/wiki/Ampere">amperes </a>. The first of the main LHC magnets were reported to have been successfully trained by 9 December 2014, while training the other magnet sectors was finished in March 2015.<a href="#cite_note-101">[101] </a>

Run 2: second operational run (2015–2018)  [  edit  ]

On 5 April 2015, the LHC restarted after a two-year break, during which the electrical connectors between the bending magnets were upgraded to safely handle the current required for 7 TeV per beam (14 TeV).<a href="#cite_note-BBC-6">[6] </a> <a href="#cite_note-splices-102">[102] </a> However, the bending magnets were only <a href='/wiki/Superconducting_magnet#Magnet_"training"'>trained </a>to handle up to 6.5 TeV per beam (13 TeV total), which became the operating energy for 2015 to 2017.<a href="#cite_note-why13tev-81">[81] </a> The energy was first reached on 10 April 2015.<a href="#cite_note-103">[103] </a> The upgrades culminated in colliding protons together with a combined energy of 13 TeV.<a href="#cite_note-13TeVcollisions-104">[104] </a> On 3 June 2015, the LHC started delivering physics data after almost two years offline.<a href="#cite_note-:0-105">[105] </a> In the following months, it was used for proton-proton collisions, while in November, the machine switched to collisions of lead ions and in December, the usual winter shutdown started.

In 2016, the machine operators focused on increasing the luminosity for proton-proton collisions. The design value was first reached 29 June,<a href="#cite_note-designlumireached-39">[39] </a> and further improvements increased the collision rate to 40% above the design value.<a href="#cite_note-2016lumi-106">[106] </a> The total number of collisions in 2016 exceeded the number from Run 1 – at a higher energy per collision. The proton-proton run was followed by four weeks of proton-lead collisions.<a href="#cite_note-2016summary-107">[107] </a>

In 2017, the luminosity was increased further and reached twice the design value. The total number of collisions was higher than in 2016 as well.<a href="#cite_note-endof2017-40">[40] </a>

The 2018 physics run began on 17 April and stopped on 3 December, including four weeks of lead–lead collisions.<a href="#cite_note-108">[108] </a>

Long Shutdown 2 (2018–2021) and beyond  [  edit  ]

Long Shutdown 2 (LS2) started 10 December 2018. The LHC and the whole CERN accelerator complex is being maintained and upgraded. The goal of the upgrades is to implement the <a href="/wiki/High_Luminosity_Large_Hadron_Collider">High Luminosity Large Hadron Collider </a>(HL-LHC) project that will increase the luminosity by a factor of 10. LS2 is projected to end in 2021, followed by Run 3.<a href="#cite_note-109">[109] </a> The HL-LHC should be operational by 2026. The Long Shutdown (LS3) in 2020s will take place before HL-LHC project is done.

<ul><li><a href="/wiki/Hierarchy_problem">Hierarchy problem </a> </li><li><a href="/wiki/Dark_matter">Dark matter </a> </li><li><a href="/wiki/Dark_energy">Dark energy </a> </li><li><a href="/wiki/Quintessence_(physics)">Quintessence </a> </li><li><a href="/wiki/Phantom_energy">Phantom energy </a> </li><li><a href="/wiki/Dark_radiation">Dark radiation </a> </li><li><a href="/wiki/Dark_photon">Dark photon </a> </li><li><a href="/wiki/Cosmological_constant_problem">Cosmological constant problem </a> </li><li><a href="/wiki/CP_violation">Strong CP problem </a> </li><li><a href="/wiki/Neutrino_oscillation">Neutrino oscillation </a> </li> </ul>

<ul><li><a href="/wiki/Brans%E2%80%93Dicke_theory">Brans–Dicke theory </a> </li><li><a href="/wiki/Cosmic_censorship_hypothesis">Cosmic censorship hypothesis </a> </li><li><a href="/wiki/Fifth_force">Fifth force </a> </li><li><a href="/wiki/F-theory">F-theory </a> </li><li><a href="/wiki/Theory_of_everything">Theory of everything </a> </li><li><a href="/wiki/Unified_field_theory">Unified field theory </a> </li><li><a href="/wiki/Grand_Unified_Theory">Grand Unified Theory </a> </li><li><a href="/wiki/Technicolor_(physics)">Technicolor </a> </li><li><a href="/wiki/Kaluza%E2%80%93Klein_theory">Kaluza–Klein theory </a> </li><li><a href="/wiki/Topological_quantum_field_theory">Topological quantum field theory </a> </li><li><a href="/wiki/Local_quantum_field_theory">Local quantum field theory </a> </li><li><a href="/wiki/Liouville_field_theory">Liouville field theory </a> </li><li><a href="/wiki/6D_(2,0)_superconformal_field_theory">6D (2,0) superconformal field theory </a> </li><li><a href="/wiki/Noncommutative_quantum_field_theory">Noncommutative quantum field theory </a> </li><li><a href="/wiki/Quantum_cosmology">Quantum cosmology </a> </li><li><a href="/wiki/Brane_cosmology">Brane cosmology </a> </li><li><a href="/wiki/String_theory">String theory </a> </li><li><a href="/wiki/Superstring_theory">Superstring theory </a> </li><li><a href="/wiki/M-theory">M-theory </a> </li><li><a href="/wiki/Mathematical_universe_hypothesis">Mathematical universe hypothesis </a> </li><li><a href="/wiki/Mirror_matter">Mirror matter </a> </li><li><a href="/wiki/Randall%E2%80%93Sundrum_model">Randall–Sundrum model </a> </li><li><a href="/wiki/Yang%E2%80%93Mills_theory">Yang–Mills theory </a> </li><li><a href="/wiki/N_%3D_4_supersymmetric_Yang%E2%80%93Mills_theory">N = 4 supersymmetric Yang–Mills theory </a> </li><li><a href="/wiki/Twistor_string_theory">Twistor string theory </a> </li><li><a href="/wiki/Dark_fluid">Dark fluid </a> </li><li><a href="/wiki/Doubly_special_relativity">Doubly special relativity </a> </li><li><a href="/wiki/De_Sitter_invariant_special_relativity">de Sitter invariant special relativity </a> </li><li><a href="/wiki/Causal_fermion_system">Causal fermion systems </a> </li><li><a href="/wiki/Black_hole_thermodynamics">Black hole thermodynamics </a> </li><li><a href="/wiki/Unparticle_physics">Unparticle physics </a> </li><li><a href="/wiki/Graviphoton">Graviphoton </a> </li><li><a href="/wiki/Graviscalar">Graviscalar </a> </li><li><a href="/wiki/Graviton">Graviton </a> </li><li><a href="/wiki/Gravitino">Gravitino </a> </li><li><a href="/wiki/Massive_gravity">Massive gravity </a> </li><li><a href="/wiki/Gauge_gravitation_theory">Gauge gravitation theory </a> </li><li><a href="/wiki/Gauge_theory_gravity">Gauge theory gravity </a> </li><li><a href="/wiki/CPT_symmetry">CPT symmetry </a> </li> </ul>

<ul><li><a href="/wiki/Minimal_Supersymmetric_Standard_Model">MSSM </a> </li><li><a href="/wiki/Next-to-Minimal_Supersymmetric_Standard_Model">NMSSM </a> </li><li><a href="/wiki/Superstring_theory">Superstring theory </a> </li><li><a href="/wiki/M-theory">M-theory </a> </li><li><a href="/wiki/Supergravity">Supergravity </a> </li><li><a href="/wiki/Supersymmetry_breaking">Supersymmetry breaking </a> </li><li><a href="/wiki/Extra_dimensions">Extra dimensions </a> </li><li><a href="/wiki/Large_extra_dimensions">Large extra dimensions </a> </li> </ul>

<ul><li><a href="/wiki/False_vacuum">False vacuum </a> </li><li><a href="/wiki/String_theory">String theory </a> </li><li><a href="/wiki/Spin_foam">Spin foam </a> </li><li><a href="/wiki/Quantum_foam">Quantum foam </a> </li><li><a href="/wiki/Quantum_geometry">Quantum geometry </a> </li><li><a href="/wiki/Loop_quantum_gravity">Loop quantum gravity </a> </li><li><a href="/wiki/Quantum_cosmology">Quantum cosmology </a> </li><li><a href="/wiki/Loop_quantum_cosmology">Loop quantum cosmology </a> </li><li><a href="/wiki/Causal_dynamical_triangulation">Causal dynamical triangulation </a> </li><li><a href="/wiki/Causal_fermion_systems">Causal fermion systems </a> </li><li><a href="/wiki/Causal_sets">Causal sets </a> </li><li><a href="/wiki/Canonical_quantum_gravity">Canonical quantum gravity </a> </li><li><a href="/wiki/Semiclassical_gravity">Semiclassical gravity </a> </li><li><a href="/wiki/Superfluid_vacuum_theory">Superfluid vacuum theory </a> </li> </ul>

<ul><li><a href="/wiki/Accelerator_Neutrino_Neutron_Interaction_Experiment">ANNIE </a> </li><li><a href="/wiki/Laboratori_Nazionali_del_Gran_Sasso">Gran Sasso </a> </li><li><a href="/wiki/India-based_Neutrino_Observatory">INO </a> </li><li><a>LHC </a> </li><li><a href="/wiki/Sudbury_Neutrino_Observatory">SNO </a> </li><li><a href="/wiki/Super-Kamiokande">Super-K </a> </li><li><a href="/wiki/Tevatron">Tevatron </a> </li><li><a href="/wiki/NOvA">NOvA </a> </li> </ul>

An initial focus of research was to investigate the possible existence of the <a href="/wiki/Higgs_boson">Higgs boson </a>, a key part of the <a href="/wiki/Standard_Model">Standard Model </a>of physics which is predicted by theory, but had not yet been observed before due to its high mass and elusive nature. CERN scientists estimated that, if the Standard Model were correct, the LHC would produce several Higgs bosons every minute, allowing physicists to finally confirm or disprove the Higgs boson's existence. In addition, the LHC allowed the search for <a href="/wiki/Superpartner">supersymmetric particles </a>and other hypothetical particles as possible unknown areas of physics.<a href="#cite_note-LHCbooklet-62">[62] </a> Some extensions of the Standard Model predict additional particles, such as the heavy <a href="/wiki/W%27_and_Z%27_bosons">W' and Z' gauge bosons </a>, which are also estimated to be within reach of the LHC to discover.<a href="#cite_note-125">[125] </a>

First run (data taken 2009–2013)  [  edit  ]

The first physics results from the LHC, involving 284 collisions which took place in the <a href="/wiki/A_Large_Ion_Collider_Experiment">ALICE </a>detector, were reported on 15 December 2009.<a href="#cite_note-first_science_2009-111">[111] </a> The results of the first proton–proton collisions at energies higher than Fermilab's Tevatron proton–antiproton collisions were published by the <a href="/wiki/Compact_Muon_Solenoid">CMS </a>collaboration in early February 2010, yielding greater-than-predicted charged-<a href="/wiki/Hadron">hadron </a>production.<a href="#cite_note-first_proton-proton_2010-126">[126] </a>

After the first year of data collection, the LHC experimental collaborations started to release their preliminary results concerning searches for new physics beyond the Standard Model in proton-proton collisions.<a href="#cite_note-CMS-XD-127">[127] </a> <a href="#cite_note-CMS-SUSY-128">[128] </a> <a href="#cite_note-ATLAS-SUSY1-129">[129] </a> <a href="#cite_note-ATLAS-SUSY2-130">[130] </a> No evidence of new particles was detected in the 2010 data. As a result, bounds were set on the allowed parameter space of various extensions of the Standard Model, such as models with <a href="/wiki/Large_extra_dimensions">large extra dimensions </a>, constrained versions of the <a href="/wiki/Minimal_Supersymmetric_Standard_Model">Minimal Supersymmetric Standard Model </a>, and others.<a href="#cite_note-131">[131] </a> <a href="#cite_note-132">[132] </a> <a href="#cite_note-133">[133] </a>

On 24 May 2011, it was reported that <a href="/wiki/Quark%E2%80%93gluon_plasma">quark–gluon plasma </a>(the densest matter thought to exist besides <a href="/wiki/Black_hole">black holes </a>) had been created in the LHC.<a href="#cite_note-plasma-114">[114] </a>

Between July and August 2011, results of searches for the Higgs boson and for exotic particles, based on the data collected during the first half of the 2011 run, were presented in conferences in Grenoble<a href="#cite_note-134">[134] </a> and Mumbai.<a href="#cite_note-135">[135] </a> In the latter conference, it was reported that, despite hints of a Higgs signal in earlier data, ATLAS and CMS exclude with 95% confidence level (using the <a href="/wiki/CLs_upper_limits">CLs </a>method) the existence of a Higgs boson with the properties predicted by the Standard Model over most of the mass region between 145 and 466 GeV.<a href="#cite_note-136">[136] </a> The searches for new particles did not yield signals either, allowing to further constrain the parameter space of various extensions of the Standard Model, including its <a href="/wiki/Supersymmetry">supersymmetric extensions </a>.<a href="#cite_note-137">[137] </a> <a href="#cite_note-138">[138] </a>

On 13 December 2011, CERN reported that the Standard Model Higgs boson, if it exists, is most likely to have a mass constrained to the range 115–130 GeV. Both the CMS and ATLAS detectors have also shown intensity peaks in the 124–125 GeV range, consistent with either background noise or the observation of the Higgs boson.<a href="#cite_note-139">[139] </a>

On 22 December 2011, it was reported that a new composite particle had been observed, the χb (3P) <a href="/wiki/Bottomonium">bottomonium </a>state.<a href="#cite_note-dec_2011_particle-117">[117] </a>

On 4 July 2012, both the CMS and ATLAS teams announced the discovery of a boson in the mass region around 125–126 GeV, with a statistical significance at the level of 5 <a href="/wiki/Standard_deviation">sigma </a>each. This meets the formal level required to announce a new particle. The observed properties were consistent with the Higgs boson, but scientists were cautious as to whether it is formally identified as actually being the Higgs boson, pending further analysis.<a href="#cite_note-cern1207-140">[140] </a> On 14 March 2013, CERN announced confirmation that the observed particle was indeed the predicted Higgs Boson.<a href="#cite_note-141">[141] </a>

On 8 November 2012, the LHCb team reported on an experiment seen as a "golden" test of <a href="/wiki/Supersymmetry">supersymmetry </a>theories in physics,<a href="#cite_note-LCHb_Nov_2012-120">[120] </a> by measuring the very rare decay of the B s {\displaystyle B_{s}} <img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/892e2261c4e42600e7c96637afbfd3fad2dde027"> <a href="/wiki/Meson">meson </a>into two <a href="/wiki/Muon">muons </a>(B s 0 → μ + μ − {\displaystyle B_{s}^{0}\rightarrow \mu ^{+}\mu ^{-}} <img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/f505d906ab9a444d340d3d6e43ea11763bd78c76"> ). The results, which match those predicted by the non-supersymmetrical <a href="/wiki/Standard_Model">Standard Model </a>rather than the predictions of many branches of supersymmetry, show the decays are less common than some forms of supersymmetry predict, though could still match the predictions of other versions of supersymmetry theory. The results as initially drafted are stated to be short of proof but at a relatively high 3.5 <a href="/wiki/Standard_deviation">sigma </a>level of significance.<a href="#cite_note-142">[142] </a> The result was later confirmed by the CMS collaboration.<a href="#cite_note-cmsbsmumu-143">[143] </a>

In August 2013, the LHCb team revealed an anomaly in the angular distribution of <a href="/wiki/B_meson">B meson </a>decay products which could not be predicted by the Standard Model; this anomaly had a statistical certainty of 4.5 sigma, just short of the 5 sigma needed to be officially recognized as a discovery. It is unknown what the cause of this anomaly would be, although the <a href="/wiki/Z%27_boson">Z' boson </a>has been suggested as a possible candidate.<a href="#cite_note-newphysics-144">[144] </a>

On 19 November 2014, the LHCb experiment announced the discovery of two new heavy subatomic particles, Ξ′− b and Ξ∗− b . Both of them are baryons that are composed of one bottom, one down, and one strange quark. They are excited states of the bottom <a href="/wiki/Xi_baryon">Xi baryon </a>.<a href="#cite_note-145">[145] </a> <a href="#cite_note-146">[146] </a>

The <a href="/wiki/LHCb">LHCb collaboration </a>has observed multiple exotic hadrons, possibly <a href="/wiki/Pentaquarks">pentaquarks </a>or <a href="/wiki/Tetraquarks">tetraquarks </a>, in the Run 1 data. On 4 April 2014, the collaboration confirmed the existence of the tetraquark candidate <a href="/wiki/Z(4430)">Z(4430) </a>with a significance of over 13.9 sigma.<a href="#cite_note-147">[147] </a> <a href="#cite_note-LHCb-148">[148] </a> On 13 July 2015, results consistent with pentaquark states in the decay of <a href="/wiki/Bottom_Lambda_baryon">bottom Lambda baryons </a>(Λ0 b ) were reported.<a href="#cite_note-LHCb2015-149">[149] </a> <a href="#cite_note-150">[150] </a> <a href="#cite_note-151">[151] </a>

On 28 June 2016, the collaboration announced four tetraquark-like particles decaying into a J/ψ and a φ meson, only one of which was well established before (X(4274), X(4500) and X(4700) and <a href="/wiki/Y(4140)">X(4140) </a>).<a href="#cite_note-152">[152] </a> <a href="#cite_note-153">[153] </a>

In December 2016, ATLAS presented a measurement of the W boson mass, researching the precision of analyses done at the Tevatron.<a href="#cite_note-wmass-154">[154] </a>

At the conference EPS-HEP 2015 in July, the collaborations presented first cross-section measurements of several particles at the higher collision energy.

On 15 December 2015, the <a href="/wiki/ATLAS_experiment">ATLAS </a>and <a href="/wiki/Compact_Muon_Solenoid">CMS </a>experiments both reported a number of preliminary results for Higgs physics, <a href="/wiki/Supersymmetry">supersymmetry </a>(SUSY) searches and <a href="/wiki/Exotic_particle">exotics </a>searches using 13 TeV proton collision data. Both experiments saw a moderate excess around 750 GeV in the two-photon <a href="/wiki/Invariant_mass">invariant mass </a>spectrum,<a href="#cite_note-NYT-20151215-155">[155] </a> <a href="#cite_note-CMS-750GeV-156">[156] </a> <a href="#cite_note-ATLAS-750GeV-157">[157] </a> but the experiments did not confirm the existence of <a href="/wiki/750_GeV_diphoton_excess">the hypothetical particle </a>in an August 2016 report.<a href="#cite_note-158">[158] </a> <a href="#cite_note-NYT-20160805-159">[159] </a> <a href="#cite_note-160">[160] </a>

In July 2017, many analyses based on the large dataset collected in 2016 were shown. The properties of the Higgs boson were studied in more detail and the precision of many other results was improved.<a href="#cite_note-CERN_EPS2017-161">[161] </a>

As of March 2021, the LHC experiments have discovered 59 new hadrons in the data collected during the first two runs.<a href="#cite_note-162">[162] </a>

Planned "high-luminosity" upgrade  [  edit  ]

After some years of running, any <a href="/wiki/Particle_physics">particle physics </a>experiment typically begins to suffer from <a href="/wiki/Diminishing_returns">diminishing returns </a>: as the key results reachable by the device begin to be completed, later years of operation discover proportionately less than earlier years. A common response is to upgrade the devices involved, typically in collision energy, <a href="/wiki/Luminosity_(scattering_theory)">luminosity </a>, or improved detectors. In addition to a possible increase to 14 TeV collision energy, a luminosity upgrade of the LHC, called the High Luminosity Large Hadron Collider, started in June 2018 that will boost the accelerator's potential for new discoveries in physics, starting in 2027.<a href="#cite_note-163">[163] </a> The upgrade aims at increasing the luminosity of the machine by a factor of 10, up to 1035 cm−2 s−1 , providing a better chance to see rare processes and improving statistically marginal measurements.

Safety of particle collisions  [  edit  ]

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