Physics topic timeline
Particle Physics Timeline
Records in the Physics collection relating to particles, particle theory, accelerators, colliders and experimental particle physics.
About this Particle Physics timeline
Explore the discovery and theory of subatomic particles, accelerators, colliders and the experimental development of particle physics.
This page contains 170 records spanning 1602–2026. Frequently represented countries include Great Britain, Italy, United States of America, Germany, Belgium. Example event labels include Law of Chords, Discovery of Electrons, Electron Theory of Matter, Zeeman Effect and Charged Oscillators, Cathode-Ray Charge-to-Mass Ratio.
Physicists frequently represented in these records
Timeline records
| Date | Person | Event | Place | Description |
|---|---|---|---|---|
| 19 November 1602 | Galileo Galilei | Law of Chords | Italy | In the same letter, Galileo formulates the law of chords concerning descent times along chords of a vertical circle. |
| 1838 | Richard Laming | Discovery of Electrons | Great Britain | Between 1838 and 1851, British natural philosopher Richard Laming developed the idea that an atom is composed of a core of matter surrounded by subatomic particles that had unit electric charge |
| 1892 | Hendrik Antoon Lorentz Physicist | Electron Theory of Matter | Leiden, Netherlands | Develops an electrodynamic theory in which charged microscopic particles account for electrical and optical behaviour in matter. |
| 1896 | Pieter Zeeman Physicist | Zeeman Effect and Charged Oscillators | Leiden, Netherlands | Finds that magnetic fields split spectral lines, providing evidence for charged particles participating in atomic radiation. |
| 1897 | Joseph John Thomson Physicist | Cathode-Ray Charge-to-Mass Ratio | Cambridge, Great Britain | Measures the charge-to-mass ratio of cathode-ray particles and shows they are far lighter than atoms. |
| 1897 | Emil Wiechert Physicist | Cathode Ray Charge-to-Mass Ratio | Konigsberg, Germany | Measures a very small mass-to-charge ratio for cathode-ray particles, evidence that they are much lighter than atoms. |
| 1897 | Emil Wiechert Physicist | Cathode-Ray Charge-to-Mass Measurement | Konigsberg, Germany | Obtains an early charge-to-mass estimate for cathode-ray particles, supporting their subatomic character. |
| 1899 | Philipp Lenard Physicist | Cathode-Ray Absorption Studies | Kiel, Germany | Studies how cathode rays penetrate matter and helps establish their particle-like behaviour. |
| 1900 | Paul Drude Physicist | Electron Theory of Metals | Leipzig, Germany | Models conduction in metals as the motion of mobile charged particles and lays foundations for the classical electron theory of conductivity. |
| 1909 | Albert Einstein Physicist | Salzburg Quantum Lecture | Salzburg, Switzerland | Presents a major lecture arguing that radiation displays both wave-like and particle-like properties. |
| 30 October 1911 | Arnold Sommerfeld Theoretical Physicist | Quantum Physics Discussions | Brussels, Germany | Contributes to discussions concerning emerging quantum concepts. |
| 10 December 1911 | Wilhelm Wien Professor of Physics | Heat Radiation Recognition | Stockholm, Germany | Is honored for foundational discoveries concerning black-body heat radiation. |
| 1911 | Wilhelm Wien Physicist | Nobel Prize | Stockholm, Germany | Receives the Nobel Prize in Physics for discoveries concerning the laws governing thermal radiation, including the displacement law bearing his name. |
| 1912 | Charles Thomson Rees Wilson Physicist | Cloud Chamber Particle Tracks | Cambridge, Great Britain | Photographs tracks made by charged particles in a cloud chamber. |
| 1919 | Ernest Rutherford Physicist | Proton as Nuclear Charge Carrier | Cambridge, Great Britain | Identifies the hydrogen nucleus as a fundamental positive particle, helping connect atomic number with the positive charge of the atomic nucleus. |
| 3 June 1920 | Ernest Rutherford Physicist | Neutral Nuclear Particle Proposal | Cambridge, New Zealand | Suggests that a neutral proton-electron combination could exist inside atomic nuclei, anticipating the neutron. |
| 1924 | Louis Victor de Broglie Theoretical Physicist | Matter Waves | Paris, France | Proposes that material particles possess wave properties. |
| 1924 | Albert Einstein Physicist | Bose-Einstein Condensation Prediction | Berlin, Germany | Predicts that ideal bosonic particles can accumulate in the lowest quantum state at low temperature. |
| 1924 | Albert Einstein Physicist | Bose-Einstein Statistics | Berlin, Germany | Extends Bose's statistical method from photons to particles of an ideal gas. |
| 1924 | Erwin Rudolf Josef Alexander Schrodinger Professor | Quantum Statistics Research | Zurich, Austria | Begins intensive work on quantum statistics and the statistical behaviour of particles, helping redirect his research toward quantum foundations. |
| 1926 | Enrico Fermi Physicist | Fermi Gas Theory | Florence, Italy | Applies his new statistics to an ideal gas of particles subject to the Pauli exclusion principle and establishes the theoretical basis of a degenerate Fermi gas. |
| 1926 | Enrico Fermi Physicist | Fermi-Dirac Electron Statistics | Rome, Italy | Develops quantum statistics for indistinguishable particles obeying the Pauli exclusion principle, providing the statistical framework now known as Fermi-Dirac statistics. |
| 1926 | Oskar Benjamin Klein Theoretical Physicist | Klein-Gordon Equation | Copenhagen, Sweden | Co-develops a relativistic wave equation for spin-zero particles. |
| 1926 | Oskar Benjamin Klein Theoretical Physicist | Relativistic Wave Equation | Copenhagen, Sweden | Extends quantum wave mechanics to particles moving near light speed. |
| 1927 | Arthur Holly Compton Physicist | Nobel Prize | Stockholm, United States of America | Shares the Nobel Prize in Physics for discovering the change in wavelength that occurs when X-rays scatter from electrons, demonstrating the particle-like properties of radiation. |
| 1927 | Albert Einstein Physicist | Motion from Field Equations | Berlin, Germany | Investigates with Jakob Grommer whether particle motion can follow directly from gravitational field equations. |
| 1927 | Enrico Fermi Professor | Rome Physics Group Formation | Rome, Italy | Builds a collaborative group of young physicists in Rome that later becomes famous for major advances in nuclear and particle physics. |
| 1927 | Charles Thomson Rees Wilson Physicist | Nobel Prize | Stockholm, Great Britain | Shares the Nobel Prize in Physics for developing the cloud-chamber method that makes the tracks of electrically charged particles visible. |
| 1930 | Herbert Becker Physicist | Beryllium Penetrating Radiation | Giessen, Germany | With Walther Bothe, detects penetrating radiation from beryllium bombarded by alpha particles. |
| 1930 | Walther Bothe Physicist | Beryllium Penetrating Radiation | Giessen, Germany | With Herbert Becker, observes unusually penetrating radiation when alpha particles strike beryllium. |
| 27 February 1932 | James Chadwick Physicist | Possible Existence of a Neutron | Cambridge, Great Britain | Publishes evidence that the penetrating beryllium radiation consists of neutral particles with roughly proton mass. |
| June 1932 | James Chadwick Physicist | The Existence of a Neutron | Cambridge, Great Britain | Publishes a fuller experimental account establishing the neutron as a distinct nuclear particle. |
| 1933 | Enrico Fermi Physicist | Beta Decay Theory Development | Rome, Italy | Formulates the fundamental ideas of his beta-decay theory by combining quantum field concepts with Wolfgang Pauli's neutrino hypothesis. |
| 1934 | Pavel Alekseyevich Cherenkov Physicist | Cherenkov Radiation | Moscow, Russia | Observes blue light emitted when charged particles move rapidly through a medium. |
| 1934 | Enrico Fermi Physicist | Beta Decay Electron Theory | Rome, Italy | Develops a quantitative theory of beta decay in which an electron and a neutrino are created during a weak nuclear transformation. |
| 1935 | James Chadwick Physicist | Nobel Prize | Stockholm, Great Britain | Receives the Nobel Prize in Physics for discovering the neutron, a neutral nuclear particle fundamental to understanding atomic nuclei. |
| 1936 | Niels Henrik David Bohr Theoretical Physicist | Compound Nucleus Model | Copenhagen, Denmark | Proposes that an incoming particle forms a temporary compound nucleus. |
| 1937 | Carl David Anderson | Discovery of Meson Particles | United States of America | Discovers the meson muon particle |
| 1937 | Marietta Blau Nuclear Physicist | Photographic Nuclear Emulsions | Hafelekar, Austria | Demonstrates a powerful photographic method for detecting high-energy particle interactions. |
| 1938 | Enrico Fermi | Nobel Prize | Stockholm, Italy | Receives the Nobel Prize in Physics for demonstrating neutron-induced radioactivity and for discoveries concerning nuclear reactions produced by slow neutrons. |
| 1940 | Bibha Chowdhuri Physicist | Cosmic Ray Tracks | Darjeeling, India | Bibha Chowdhuri works with D. M. Bose using photographic plates at high altitude to study charged particles in cosmic rays. |
| 1941 | Bibha Chowdhuri Physicist | Meson Measurements | Darjeeling, India | Bibha Chowdhuri and D. M. Bose publish measurements of cosmic-ray particle tracks that provide early evidence for particles of meson-like mass. |
| 1944 | Enrico Fermi Physicist | Los Alamos F Division Leadership | Los Alamos, United States of America | Leads a Los Alamos division concerned with advanced theoretical and experimental problems related to neutron physics and weapon development. |
| 1945 | Enrico Fermi Physicist | Interim Committee Scientific Panel | Washington, United States of America | Serves on the scientific panel advising the Interim Committee on issues concerning the wartime use and postwar implications of atomic energy. |
| 1945 | Cecil Frank Powell Physicist | Nuclear Emulsion Research | Bristol, Great Britain | Powell develops particle physics research at the University of Bristol. |
| 1946 | Enrico Fermi Professor | Postwar Nuclear Physics Programme | Chicago, United States of America | Establishes an energetic postwar research programme at Chicago spanning nuclear physics, particle physics and theoretical problems. |
| 1947 | Enrico Fermi Physicist | Cosmic Ray Research | Chicago, United States of America | Studies high-energy cosmic-ray interactions and develops theoretical models for how energetic particles produce secondary particles in the atmosphere. |
| 1948 | Enrico Fermi Physicist | Particle Acceleration Theory | Chicago, United States of America | Develops ideas explaining how charged particles can gain energy through repeated interactions with moving magnetic fields in astrophysical environments. |
| 1949 | Enrico Fermi Physicist | Fermi Acceleration Mechanism | Chicago, United States of America | Publishes a theory of stochastic particle acceleration that later becomes known as second-order Fermi acceleration. |
| 1950 | Enrico Fermi Physicist | Pion Nucleon Scattering Research | Chicago, United States of America | Uses the Chicago cyclotron to investigate pion-nucleon interactions and helps establish important experimental results in emerging particle physics. |
| 1951 | Enrico Fermi Physicist | High Energy Particle Experiments | Chicago, United States of America | Continues high-energy experiments with mesons and nucleons, combining rapid estimates with detailed measurements to test models of particle interactions. |
| 1953 | Aage Niels Bohr Nuclear Physicist | Collective Nuclear Model | Copenhagen, Denmark | Co-develops a model combining individual particles with collective nuclear motion. |
| 1953 | Enrico Fermi Professor | Final Chicago Research Programme | Chicago, United States of America | Continues teaching and conducting research at the University of Chicago while advising younger physicists on nuclear and particle physics problems. |
| 1954 | Enrico Fermi Physicist | Legacy in Nuclear and Particle Physics | Chicago, United States of America | Leaves a scientific legacy spanning quantum statistics, beta decay, neutron physics, controlled chain reactions, particle acceleration and high-energy physics. |
| 1956 | Lev Davidovich Landau Physicist | Fermi Liquid Theory of Electrons | Moscow, Russia | Develops the Fermi-liquid description of interacting electrons in metals as long-lived quasiparticles near the Fermi surface. |
| 1962 | Ennackal Chandy George Sudarshan Physicist | Faster-than-light Particles | United States, India | E. C. G. Sudarshan and collaborators publish a theoretical analysis showing how hypothetical faster-than-light particles can fit within special relativity. |
| 1963 | Eugene Paul Wigner | Nobel Prize | Stockholm, United States of America | Shares the Nobel Prize in Physics for contributions to nuclear and particle theory, especially symmetry principles. |
| 31 August 1964 | Robert Brout Theoretical Physicist | Higgs Boson | Brussels, Belgium | Coauthors with Francois Englert the Physical Review Letters paper Broken Symmetry and the Mass of Gauge Vector Mesons. |
| 31 August 1964 | Francois Englert Theoretical Physicist | Higgs Boson | Brussels, Belgium | Publishes with Robert Brout the first 1964 gauge-symmetry paper establishing a mechanism by which gauge vector bosons can acquire mass. |
| 19 October 1964 | Peter Ware Higgs Theoretical Physicist | Higgs Boson | Edinburgh, Great Britain | Publishes Broken Symmetries and the Masses of Gauge Bosons, explicitly identifying the massive scalar excitation later called the Higgs boson. |
| 19 October 1964 | Peter Ware Higgs Theoretical Physicist | Higgs Boson | Edinburgh, Great Britain | Shows that spontaneous symmetry breaking in a gauge theory can avoid an unwanted massless particle while leaving a massive scalar particle in the theory. |
| 16 November 1964 | Gerald Guralnik Theoretical Physicist | Higgs Boson | London, Great Britain | Coauthors a third independent 1964 paper explaining spontaneous symmetry breaking in relativistic gauge theory and the generation of gauge-boson masses. |
| 16 November 1964 | Carl Richard Hagen Theoretical Physicist | Higgs Boson | London, Great Britain | Publishes with Gerald Guralnik and Tom Kibble an independent formulation of the gauge-symmetry-breaking mechanism. |
| 16 November 1964 | Tom Kibble Theoretical Physicist | Higgs Boson | London, Great Britain | Coauthors Global Conservation Laws and Massless Particles, completing one of the independent 1964 formulations associated with the Higgs mechanism. |
| 1964 | Robert Brout Theoretical Physicist | Gauge Symmetry | Brussels, Belgium | Develops with Francois Englert a mechanism in which spontaneous symmetry breaking gives mass to gauge vector particles without abandoning local gauge symmetry. |
| 1964 | Peter Ware Higgs Theoretical Physicist | Scalar Boson Prediction | Edinburgh, Great Britain | Develops the consequence that the symmetry-breaking mechanism should leave a massive scalar particle that could in principle be detected experimentally. |
| 1964 | Peter Ware Higgs Theoretical Physicist | Symmetry Breaking Paper | Edinburgh, Great Britain | Publishes a short paper on broken symmetries that identifies a loophole allowing gauge theories to evade the usual massless-particle conclusion. |
| 1964 | Jayant Vishnu Narlikar Astrophysicist | Hoyle-Narlikar Gravity | Cambridge, India | Jayant Narlikar and Fred Hoyle publish a new Machian theory of gravitation based on direct particle interactions. |
| 20 November 1967 | Steven Weinberg Theoretical Physicist | Higgs Boson | Cambridge, Massachusetts, United States of America | Uses spontaneous symmetry breaking in A Model of Leptons to construct a unified electroweak theory incorporating a Higgs-type scalar field. |
| 1968 | Brandon Carter Physicist | Carter Constant | Australia | Shows that particle motion in Kerr spacetime is separable and identifies the additional conserved quantity now called the Carter constant. |
| 1968 | Abdus Salam Theoretical Physicist | Electroweak Theory | London, Pakistan | Formulates the electroweak gauge theory independently along lines closely related to Steven Weinberg's model, using spontaneous symmetry breaking to generate weak-boson masses. |
| 1968 | Abdus Salam Theoretical Physicist | Higgs Boson | London, Pakistan | Presents an electroweak gauge theory in which spontaneous symmetry breaking supplies masses to weak force carriers while preserving the underlying gauge structure. |
| 1969 | Steven Weinberg Theoretical Physicist | MIT Appointment | Cambridge, Massachusetts, United States of America | Joins the Massachusetts Institute of Technology faculty and continues research in particle theory. |
| 10 December 1970 | Hannes Olof Gosta Alfven Plasma Physicist | Magnetohydrodynamics Recognition | Stockholm, Sweden | Is recognized for discoveries concerning plasma and magnetic-field interactions. |
| 1971 | Gerardus 't Hooft Theoretical Physicist | Higgs Boson | Utrecht, Netherlands | Demonstrates the renormalizability of spontaneously broken gauge theories, helping establish the mathematical consistency needed for the electroweak Higgs mechanism. |
| December 1973 | Leo Esaki Physicist | Nobel Prize for Electron Tunnelling | Stockholm, Japan | Shares the Nobel Prize in Physics for experimental discoveries concerning tunnelling in semiconductors. |
| December 1973 | Ivar Giaever Physicist | Nobel Prize for Superconducting Tunnelling | Stockholm, Norway | Shares the Nobel Prize in Physics for experimental discoveries concerning tunnelling in superconductors. |
| 1973 | Abdus Salam Theoretical Physicist | Higgs Boson | Trieste, Pakistan | Sees the discovery of weak neutral currents provide major experimental support for the electroweak framework in which the Higgs mechanism operates. |
| 1973 | Steven Weinberg Theoretical Physicist | Higgs Boson | Cambridge, Massachusetts, United States of America | Sees neutral-current observations strengthen the electroweak theory that he had formulated using spontaneous symmetry breaking. |
| November 1974 | Samuel Ting Physicist | J-Psi Discovery | Brookhaven, United States of America | Leads the team that discovers the J/psi particle using high-energy particle interactions. |
| 1974 | Burton Richter Physicist | Electron-Positron J-Psi Discovery | Stanford, United States of America | Leads the SPEAR electron-positron collider team that discovers the J-psi particle, demonstrating the power of lepton colliders for particle physics. |
| 15 January 1976 | Don Page Physicist | Black Hole Particle Emission | Canada | Calculates emission rates for massless particles from an uncharged, nonrotating black hole using Hawking radiation and black hole perturbation theory. |
| 15 August 1976 | William Unruh Physicist | Notes on Black-Hole Evaporation | Canada | Analyzes black hole evaporation and shows the close relation between particle detection by accelerated observers and quantum effects near event horizons. |
| December 1976 | Samuel Ting Physicist | Nobel Prize for J-Psi Discovery | Stockholm, United States of America | Shares the Nobel Prize in Physics for discovery of a new kind of heavy elementary particle. |
| 15 October 1977 | Don Page Physicist | Charged Lepton Emission | Canada | Calculates Hawking emission of electrons and muons from a nonrotating black hole and analyzes fluctuations in the hole's electric charge. |
| 10 December 1979 | Abdus Salam Theoretical Physicist · Nobel Laureate | Higgs Boson | Stockholm, Pakistan | Shares the Nobel Prize in Physics for electroweak unification, the theory whose massive weak bosons depend on spontaneous gauge-symmetry breaking. |
| 10 December 1979 | Steven Weinberg Theoretical Physicist · Nobel Laureate | Higgs Boson | Stockholm, United States of America | Shares the Nobel Prize in Physics for the electroweak theory, which incorporates the symmetry-breaking mechanism later tested through Higgs-boson measurements. |
| 1983 | Carlo Rubbia Experimental Physicist | Higgs Boson | Geneva, Italy | Leads the UA1 collaboration as CERN experiments discover the W and Z bosons whose masses are explained within electroweak theory by the Higgs mechanism. |
| 10 December 1984 | Simon van der Meer | Nobel Prize | Stockholm, Netherlands | Shares the Nobel Prize in Physics for decisive contributions enabling discovery of the W and Z particles. |
| 10 December 1984 | Carlo Rubbia | Nobel Prize | Stockholm, Italy | Shares the Nobel Prize in Physics for discoveries leading to the W and Z particles, carriers of the weak interaction. |
| 1989 | Peter Ware Higgs Theoretical Physicist | Higgs Boson | Geneva, Great Britain | Sees CERN's LEP collider begin precision tests of electroweak theory and searches that increasingly constrain the possible mass of the Higgs boson. |
| 16 December 1994 | Hubert Curien Physicist | Large Hadron Collider Approval | Geneva, France | Chairs the CERN Council meeting that approves construction of the Large Hadron Collider by consensus. |
| 16 December 1994 | Christopher Llewellyn Smith Physicist | Large Hadron Collider Approval | Geneva, Great Britain | Welcomes CERN Council approval for construction of the Large Hadron Collider as the laboratory's next major high-energy physics project. |
| 21 November 1996 | Abdus Salam Theoretical Physicist | Death | Oxford, Pakistan | Dies in Oxford after a career combining fundamental particle physics with advocacy for scientific development in poorer countries. |
| 20 December 1996 | Hubert Curien Physicist | Large Hadron Collider Construction Plan | Geneva, France | Presides as CERN Council approves completing the Large Hadron Collider in a single construction stage rather than the original two-stage plan. |
| 8 December 1997 | Federico Pena Government Official | Large Hadron Collider International Participation | Geneva, United States of America | Signs an agreement establishing major United States participation in construction of the Large Hadron Collider and its experiments. |
| 1997 | Robert Brout Theoretical Physicist | European Physics Prize | Europe, Belgium | Shares the European Physical Society High Energy and Particle Physics Prize with Francois Englert and Peter Higgs. |
| 1997 | Francois Englert Theoretical Physicist | European Physics Prize | Europe, Belgium | Shares the European Physical Society High Energy and Particle Physics Prize with Robert Brout and Peter Higgs. |
| 1997 | Peter Ware Higgs Theoretical Physicist | Dirac Medal | Great Britain, Great Britain | Receives the Institute of Physics Paul Dirac Medal and Prize for his contributions to theoretical particle physics. |
| 1997 | Anton Zeilinger Quantum Physicist | Teleportation of a Photon State | Innsbruck, Austria | Transfers an unknown photon state without transporting the original particle. |
| 10 August 1998 | Lionel Jospin Prime Minister | Large Hadron Collider Civil Engineering | France, France | Authorizes French civil-engineering work needed for Large Hadron Collider construction on the French side of the CERN site. |
| 2000 | Peter Ware Higgs Theoretical Physicist | Higgs Boson | Geneva, Great Britain | Sees the LEP collider finish operations without a confirmed Higgs discovery, leaving the particle as a central target for future collider experiments. |
| 2004 | Robert Brout Theoretical Physicist | Higgs Boson | Jerusalem, Belgium | Shares the Wolf Prize in Physics with Francois Englert and Peter Higgs for the theoretical mechanism underlying gauge-particle mass generation. |
| 2004 | Francois Englert Theoretical Physicist | Higgs Boson | Jerusalem, Belgium | Shares the Wolf Prize in Physics with Robert Brout and Peter Higgs for pioneering work on mass generation through broken gauge symmetry. |
| 2004 | Peter Ware Higgs Theoretical Physicist | Higgs Boson | Jerusalem, Great Britain | Shares the Wolf Prize in Physics with Robert Brout and Francois Englert for pioneering work that established the mechanism of mass generation. |
| 7 March 2005 | Lyn Evans Physicist | Large Hadron Collider Magnet Installation | Geneva, Great Britain | Oversees the project as the first superconducting dipole magnet is lowered into the Large Hadron Collider tunnel. |
| 25 August 2005 | Lyn Evans Physicist | Large Hadron Collider Installation | Geneva, Great Britain | Sees major detector magnet milestones reached for ATLAS and CMS while installation of the Large Hadron Collider continues. |
| 23 June 2006 | Lyn Evans Physicist | Large Hadron Collider Start-Up Planning | Geneva, Great Britain | Reports plans for initial Large Hadron Collider collisions as accelerator and detector installation approaches its final commissioning phase. |
| 22 June 2007 | Robert Aymar Physicist | Large Hadron Collider Start-Up Schedule | Geneva, France | Announces a revised Large Hadron Collider start-up schedule after delays in installation and commissioning. |
| 10 September 2008 | Lyn Evans Physicist | Large Hadron Collider First Beam | Geneva, Great Britain | Leads the project as the first proton beam successfully circulates around the full 27-kilometre Large Hadron Collider ring. |
| 19 September 2008 | Lyn Evans Physicist | Large Hadron Collider Incident | Geneva, Great Britain | Sees an electrical connection failure cause serious damage in one Large Hadron Collider sector, forcing an extended repair programme. |
| 21 October 2008 | Robert Aymar Physicist | Large Hadron Collider Inauguration | Geneva, France | Participates in the official inauguration of the Large Hadron Collider following the successful circulation of its first beam. |
| 20 November 2009 | Rolf-Dieter Heuer Physicist | Large Hadron Collider Restart | Geneva, Germany | Sees proton beams circulate again in the Large Hadron Collider after repairs and consolidation following the 2008 incident. |
| 30 November 2009 | Rolf-Dieter Heuer Physicist | Large Hadron Collider Beam Energy Record | Geneva, Germany | Announces that the Large Hadron Collider has set a world record for particle-beam energy at 1.18 TeV per beam. |
| 16 December 2009 | Rolf-Dieter Heuer Physicist | Large Hadron Collider Collision Record | Geneva, Germany | Sees the Large Hadron Collider produce 2.36 TeV proton collisions, setting a new world record for collider energy. |
| 30 March 2010 | Rolf-Dieter Heuer Physicist | Large Hadron Collider High-Energy Collisions | Geneva, Germany | Welcomes the first Large Hadron Collider proton collisions at a total energy of 7 TeV, beginning sustained high-energy physics running. |
| 13 October 2010 | Steve Myers Physicist | Large Hadron Collider Luminosity | Geneva, Great Britain | Sees the Large Hadron Collider reach its 2010 luminosity target ahead of schedule during the first year of 7 TeV proton physics. |
| 8 November 2010 | Rolf-Dieter Heuer Physicist | Large Hadron Collider Lead Ions | Geneva, Germany | Sees lead-ion beams introduced into the Large Hadron Collider, opening a programme studying extremely hot and dense strongly interacting matter. |
| 2010 | Francois Englert Theoretical Physicist | Higgs Boson | Washington, Belgium | Shares the J. J. Sakurai Prize with five other theorists for elucidating spontaneous symmetry breaking and consistent vector-boson mass generation. |
| 2010 | Peter Ware Higgs Theoretical Physicist | Higgs Boson | Washington, Great Britain | Shares the J. J. Sakurai Prize for work explaining spontaneous symmetry breaking in relativistic gauge theory. |
| 22 April 2011 | Rolf-Dieter Heuer Physicist | Large Hadron Collider Beam Intensity Record | Geneva, Germany | Announces that the Large Hadron Collider has surpassed the Tevatron's hadron-collider luminosity record, increasing its discovery potential. |
| 2011 | Steve Myers Physicist | Large Hadron Collider Operations | Geneva, Great Britain | Guides accelerator operations as the Large Hadron Collider substantially increases delivered collision data during its second year of proton running. |
| 5 April 2012 | Steve Myers Physicist | Large Hadron Collider 8 TeV Collisions | Geneva, Great Britain | Sees the Large Hadron Collider begin proton collisions at a total centre-of-mass energy of 8 TeV. |
| 4 July 2012 | Robert Brout Theoretical Physicist | Experimental Confirmation | Geneva, Belgium | Receives posthumous scientific vindication when ATLAS and CMS announce a new particle consistent with the boson implied by the Brout-Englert-Higgs mechanism. |
| 4 July 2012 | Fabiola Gianotti Experimental Physicist | Higgs Boson | Geneva, Italy | Presents the ATLAS collaboration's evidence for a new particle near 125 GeV at CERN during the Higgs discovery seminar. |
| 4 July 2012 | Fabiola Gianotti Physicist | Higgs Boson Discovery | Geneva, Italy | Presents the ATLAS collaboration's evidence for a new particle near 125 GeV during CERN's Higgs boson discovery announcement. |
| 4 July 2012 | Rolf-Dieter Heuer Physicist · CERN Director-General | Higgs Boson | Geneva, Germany | As CERN Director-General, welcomes the ATLAS and CMS results announcing observation of a new particle consistent with the long-sought Higgs boson. |
| 4 July 2012 | Rolf-Dieter Heuer Physicist | Higgs Boson Discovery | Geneva, Germany | Announces that ATLAS and CMS have observed a new particle consistent with the long-sought Higgs boson. |
| 4 July 2012 | Peter Ware Higgs Physicist | Large Hadron Collider Higgs Result | Geneva, Great Britain | Witnesses CERN announce a new particle consistent with the boson predicted by the symmetry-breaking mechanism associated with his work. |
| 4 July 2012 | Joe Incandela Experimental Physicist | Higgs Boson | Geneva, United States of America | Presents the CMS collaboration's independent evidence for a new particle near 125 GeV during CERN's announcement of the discovery. |
| 4 July 2012 | Joe Incandela Physicist | Higgs Boson Discovery | Geneva, United States of America | Presents the CMS collaboration's independent evidence for a new particle near 125 GeV during CERN's Higgs boson discovery announcement. |
| 28 September 2012 | Steve Myers Physicist | Large Hadron Collider Data Target | Geneva, Great Britain | Sees the Large Hadron Collider reach its 2012 target of delivering 15 inverse femtobarns of data to ATLAS and CMS. |
| 14 February 2013 | Rolf-Dieter Heuer Physicist | Large Hadron Collider Run 1 Completion | Geneva, Germany | Marks the end of the Large Hadron Collider's first three-year running period before the machine enters its first long shutdown. |
| 14 March 2013 | Fabiola Gianotti Physicist | Higgs Boson Properties | Geneva, Italy | Sees additional ATLAS and CMS measurements strengthen the identification of the 2012 particle as a Higgs boson. |
| 14 March 2013 | Peter Ware Higgs Theoretical Physicist | Higgs Boson | Geneva, Great Britain | Sees CERN report that additional data support the new particle having spin zero and positive parity, strengthening its identification as a Higgs boson. |
| 14 March 2013 | Peter Ware Higgs Physicist | Higgs Boson Confirmation | Geneva, Great Britain | Sees CERN report that accumulating measurements increasingly support the new particle having the properties expected of a Higgs boson. |
| 10 December 2013 | Francois Englert Theoretical Physicist · Nobel Laureate | Higgs Boson | Stockholm, Belgium | Shares the Nobel Prize in Physics after CERN measurements confirm a particle associated with the symmetry-breaking mechanism proposed in 1964. |
| 2013 | Francois Englert Theoretical Physicist | Prince of Asturias Award | Oviedo, Belgium | Shares the Prince of Asturias Award for Technical and Scientific Research with Peter Higgs and CERN. |
| 2013 | François Englert | Nobel Prize | Stockholm, Belgium | Shares the Nobel Prize in Physics for the theoretical discovery of the mechanism explaining the origin of mass of subatomic particles. |
| 2013 | Peter Higgs | Nobel Prize | Stockholm, Great Britain | Shares the Nobel Prize in Physics for the theoretical discovery of the mechanism explaining the origin of mass of subatomic particles. |
| 23 June 2014 | Peter Ware Higgs Theoretical Physicist | Higgs Boson | Geneva, Great Britain | Sees CERN report stronger evidence that the Higgs boson decays directly to fermions, extending tests of how the Higgs field couples to matter particles. |
| 2014 | Fabiola Gianotti Physicist | Large Hadron Collider Preparations | Geneva, Italy | Prepares for renewed high-energy physics as the Large Hadron Collider and its experiments approach the end of the first long shutdown. |
| 14 July 2015 | Guy Wilkinson Physicist | Pentaquark Discovery | Geneva, Great Britain | Sees the LHCb collaboration report structures interpreted as pentaquark states in decays recorded with Large Hadron Collider data. |
| 25 November 2015 | Fabiola Gianotti Physicist | Large Hadron Collider Lead-Ion Collisions | Geneva, Italy | Sees the Large Hadron Collider begin lead-ion collisions at roughly twice the energy achieved in its previous heavy-ion programme. |
| 2015 | Fabiola Gianotti Physicist | Large Hadron Collider Run 2 | Geneva, Italy | Sees the Large Hadron Collider begin Run 2 with proton collisions at the new energy frontier of 13 TeV. |
| 2015 | Peter Ware Higgs Theoretical Physicist | Copley Medal | London, Great Britain | Receives the Royal Society's Copley Medal for his fundamental contribution to particle physics. |
| 2015 | Takaaki Kajita | Nobel Prize | Stockholm, Japan | Shares the Nobel Prize in Physics for discovering neutrino oscillations, showing that neutrinos have mass. |
| 2015 | Arthur B. McDonald | Nobel Prize | Stockholm, Canada | Shares the Nobel Prize in Physics for discovering neutrino oscillations, showing that neutrinos have mass. |
| 11 July 2016 | Fabiola Gianotti Physicist | Large Hadron Collider Luminosity | Geneva, Italy | Sees Large Hadron Collider performance exceed expectations as ATLAS and CMS rapidly accumulate substantially more Run 2 collision data. |
| 2016 | Mike Lamont Physicist | Large Hadron Collider Operations | Geneva, Great Britain | Helps oversee accelerator performance as the Large Hadron Collider operates with more than two thousand proton bunches per beam. |
| 2017 | Fabiola Gianotti Physicist | Large Hadron Collider Physics | Geneva, Italy | Sees Run 2 continue producing large proton-collision datasets for precision Standard Model measurements and searches for physics beyond it. |
| 3 December 2018 | Fabiola Gianotti Physicist | Large Hadron Collider Run 2 Completion | Geneva, Italy | Marks the end of Large Hadron Collider Run 2 after four years of 13 TeV proton collisions and extensive heavy-ion running. |
| 3 December 2018 | Mike Lamont Physicist | Large Hadron Collider Long Shutdown 2 | Geneva, Great Britain | Sees the Large Hadron Collider enter Long Shutdown 2 for major maintenance, consolidation and upgrades. |
| 2018 | Fabiola Gianotti Physicist | Higgs Bottom-Quark Decay | Geneva, Italy | Sees ATLAS and CMS report observation of Higgs boson decay into bottom quarks using Large Hadron Collider data. |
| 2018 | Peter Ware Higgs Theoretical Physicist | Higgs Boson | Geneva, Great Britain | Sees ATLAS and CMS report observation of Higgs-boson decay to bottom quarks, confirming an important predicted coupling to fermionic matter. |
| 2019 | Fabiola Gianotti Physicist | Large Hadron Collider Upgrade | Geneva, Italy | Oversees CERN while accelerator teams begin extensive Long Shutdown 2 upgrades to the Large Hadron Collider and its injector chain. |
| 2020 | Fabiola Gianotti Physicist | Large Hadron Collider Detector Upgrades | Geneva, Italy | Sees ATLAS, CMS, ALICE and LHCb continue major detector and data-acquisition upgrades in preparation for higher-rate Run 3 collisions. |
| 23 July 2021 | Steven Weinberg Theoretical Physicist | Death | Austin, United States of America | Dies in Austin after a career that reshaped particle physics, quantum field theory and modern cosmology. |
| 2021 | Fabiola Gianotti Physicist | Large Hadron Collider Run 3 Preparations | Geneva, Italy | Oversees final preparations for restarting the Large Hadron Collider after the extended maintenance and upgrade programme. |
| 22 April 2022 | Fabiola Gianotti Physicist | Large Hadron Collider Restart | Geneva, Italy | Sees proton beams circulate in the Large Hadron Collider again after more than three years of maintenance, consolidation and upgrades. |
| 4 July 2022 | Fabiola Gianotti Physicist | Higgs Boson Tenth Anniversary | Geneva, Italy | Marks ten years since the ATLAS and CMS collaborations announced the discovery of a Higgs boson using Large Hadron Collider data. |
| 4 July 2022 | Peter Ware Higgs Theoretical Physicist | Higgs Boson | Geneva, Great Britain | Sees CERN mark ten years since the discovery with increasingly precise measurements supporting the Higgs boson's predicted spin-zero Standard Model properties. |
| 4 July 2022 | Peter Ware Higgs Physicist | Higgs Boson Tenth Anniversary | Geneva, Great Britain | Sees CERN commemorate ten years of increasingly precise measurements of the Higgs boson discovered with Large Hadron Collider data. |
| 5 July 2022 | Fabiola Gianotti Physicist | Large Hadron Collider Record Energy | Geneva, Italy | Sees the Large Hadron Collider establish routine physics collisions at 13.6 TeV, the highest centre-of-mass energy then achieved by a collider. |
| 5 July 2022 | Fabiola Gianotti Physicist | Large Hadron Collider Run 3 | Geneva, Italy | Marks the start of Run 3 physics as the Large Hadron Collider delivers proton collisions at the record energy of 13.6 TeV. |
| 2022 | Fabiola Gianotti Physicist | Large Hadron Collider Experiment Upgrades | Geneva, Italy | Sees upgraded ATLAS, CMS, ALICE and LHCb systems begin collecting larger and higher-quality Run 3 datasets. |
| 2022 | Joe Incandela Physicist | Large Hadron Collider Run 3 | Geneva, United States of America | Sees CMS exploit rapidly accumulated 13.6 TeV collision data to produce early Run 3 measurements of top-quark pair production. |
| 2023 | Fabiola Gianotti Physicist | Large Hadron Collider Run 3 Physics | Geneva, Italy | Sees the Large Hadron Collider continue Run 3 measurements of Higgs physics, heavy flavours, heavy ions and precision Standard Model processes. |
| 8 April 2024 | Peter Ware Higgs Theoretical Physicist | Death | Edinburgh, Great Britain | Dies at home in Edinburgh at the age of ninety-four, leaving a central legacy in the Standard Model of particle physics. |
| 18 June 2026 | Francois Englert Theoretical Physicist | Death | Uccle, Belgium | Dies in Uccle at the age of ninety-three after a career spanning particle physics, cosmology and quantum field theory. |