Physics topic timeline
Quantum Physics Timeline
Records in the Physics collection relating to quantum theory, quantum mechanics, quantum states and quantum experiments.
About this Quantum Physics timeline
Trace quantum theory from early radiation problems through quantum mechanics, quantum statistics, atomic states and later applications.
This page contains 150 records spanning 1858–2026. Frequently represented countries include Germany, United States of America, Austria, Great Britain, Switzerland. Example event labels include Birth of Max Karl Ernst Planck, Max Born Born, Radiation Energy Fluctuations, Photoelectric Effect Paper Submitted, Photoelectric Quantum Explanation.
Physicists frequently represented in these records
Timeline records
| Date | Person | Event | Place | Description |
|---|---|---|---|---|
| 1858 | Max Karl Ernst Planck | Birth of Max Karl Ernst Planck | Germany | Birth of Max Karl Ernst Planck, developed quantum theory |
| 11 December 1882 | Max Born Physicist | Max Born Born | Breslau, Germany | The future quantum physicist and Nobel laureate is born. |
| 1904 | Albert Einstein Physicist | Radiation Energy Fluctuations | Bern, Switzerland | Studies fluctuations in radiation energy, an important precursor to his later quantum work. |
| 17 March 1905 | Albert Einstein Physicist | Photoelectric Effect Paper Submitted | Bern, Switzerland | Sends his light-quantum paper to Annalen der Physik, using quanta to explain the photoelectric effect. |
| 1905 | Albert Einstein Physicist | Photoelectric Quantum Explanation | Bern, Switzerland | Explains photoelectric emission by proposing that light transfers energy in discrete quanta to electrons. |
| 1906 | Albert Einstein Physicist | Light Production and Absorption Paper | Bern, Switzerland | Publishes work extending the light-quantum hypothesis to the production and absorption of radiation. |
| 1907 | Albert Einstein Physicist | Quantum Theory of Specific Heat | Bern, Switzerland | Applies quantum ideas to the specific heat of solids, an early success of quantum theory. |
| 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 | Walther Nernst Physical Chemist | Radiation and Quanta Conference | Brussels, Germany | Engages in international debate on quantum and thermodynamic problems. |
| 30 October 1911 | Max Planck Theoretical Physicist | Quantum Theory Conference | Brussels, Germany | Discusses quantum theory with leading European physicists in Brussels. |
| 30 October 1911 | Arnold Sommerfeld Theoretical Physicist | Quantum Physics Discussions | Brussels, Germany | Contributes to discussions concerning emerging quantum concepts. |
| 11 December 1911 | Wilhelm Wien Professor of Physics | Laws of Thermal Radiation | Stockholm, Germany | Reviews experimental and theoretical work leading toward quantum physics. |
| 1911 | Albert Einstein Physicist | First Solvay Conference | Brussels, Switzerland | Participates in the first Solvay Conference, discussing radiation and quantum theory with leading physicists. |
| 1913 | Niels Henrik David Bohr Theoretical Physicist | Quantized Electron Orbits | Copenhagen, Denmark | Explains the hydrogen spectrum through quantum transitions between stationary orbits. |
| 1916 | Albert Einstein Physicist | Quantum Theory of Radiation | Berlin, Germany | Develops a quantum theory of radiation introducing transition probabilities later represented by Einstein coefficients. |
| 1917 | Albert Einstein Physicist | Stimulated Emission | Berlin, Germany | Formulates stimulated emission in his quantum theory of radiation, a principle later fundamental to lasers. |
| 1918 | Albert Einstein Physicist | Zurich Guest Lectures | Zurich, Germany | Returns to Zurich for guest lectures while continuing work on relativity and quantum theory. |
| 1918 | Max Planck Physicist | Nobel Prize | Stockholm, Germany | Receives the Nobel Prize in Physics for originating quantum theory through his discovery of energy quanta in the study of black-body radiation. |
| 3 March 1921 | Niels Henrik David Bohr Theoretical Physicist | Copenhagen Physics Institute Opened | Copenhagen, Denmark | Creates an international centre for atomic and quantum research. |
| 10 December 1922 | Niels Henrik David Bohr Theoretical Physicist | Atomic Structure Recognition | Stockholm, Denmark | Gains recognition for applying quantum ideas to the structure of atoms. |
| 1923 | Enrico Fermi Physicist | Quantum Theory Studies | Göttingen, Italy | Studies emerging quantum theory in Göttingen and deepens his familiarity with the mathematical methods being applied to atomic physics. |
| 1923 | Erwin Rudolf Josef Alexander Schrodinger Professor | Atomic Spectra Research | Zurich, Austria | Investigates problems in atomic spectra as his attention increasingly shifts toward unresolved questions in quantum theory. |
| 1924 | Satyendra Nath Bose Physicist | Quantum Statistics Paper | Berlin, India | Bose's paper on Planck's law is translated and submitted for publication by Albert Einstein, bringing Bose statistics to international attention. |
| 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 | 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. |
| 30 November 1925 | Albert Einstein Physicist | Copley Medal | London, Germany | Awarded the Royal Society's Copley Medal for relativity and contributions to quantum theory. |
| 1925 | Albert Einstein Physicist | Quantum Mechanics Critique Begins | Berlin, Germany | Engages critically with the emerging matrix and wave formulations of quantum mechanics. |
| 1925 | Albert Einstein Physicist | Second Quantum Gas Paper | Berlin, Germany | Publishes further work on the quantum theory of the ideal monatomic gas. |
| 1925 | Enrico Fermi Lecturer | Quantum Gas Research | Florence, Italy | Investigates quantum gases and statistical problems that directly precede his formulation of Fermi statistics. |
| 1925 | Wolfgang Ernst Pauli Theoretical Physicist | Electron State Restriction | Hamburg, Austria | Explains atomic shell structure through a fundamental quantum restriction. |
| 1925 | Wolfgang Ernst Pauli Theoretical Physicist | Pauli Exclusion Principle | Hamburg, Austria | Formulates the rule preventing identical electrons from sharing one quantum state. |
| 4 May 1926 | Erwin Rudolf Josef Alexander Schrodinger Professor | Wave and Matrix Mechanics Equivalence | Zurich, Austria | Publishes a demonstration that his wave mechanics and Heisenberg's matrix mechanics are mathematically equivalent formulations of quantum theory. |
| 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 | Relativistic Wave Equation | Copenhagen, Sweden | Extends quantum wave mechanics to particles moving near light speed. |
| 1926 | Erwin Rudolf Josef Alexander Schrodinger Professor | Wave Function Interpretation | Zurich, Austria | Proposes a continuous wave-based physical interpretation of the quantum state while developing his new formulation of quantum mechanics. |
| September 1927 | Niels Henrik David Bohr Theoretical Physicist | Complementarity Principle | Como, Denmark | Presents complementarity as a principle for interpreting quantum phenomena. |
| September 1927 | Niels Henrik David Bohr Theoretical Physicist | Quantum Measurement Interpretation | Como, Denmark | Argues that mutually exclusive experimental descriptions can both be necessary. |
| October 1927 | Erwin Rudolf Josef Alexander Schrodinger Professor | Solvay Quantum Theory Discussions | Brussels, Austria | Takes part in the fifth Solvay Conference, where leading physicists debate the interpretation and foundations of the newly developed quantum mechanics. |
| 1927 | Albert Einstein Physicist | Bohr-Einstein Quantum Debate | Brussels, Germany | Challenges Niels Bohr with thought experiments testing the completeness of quantum mechanics. |
| 1927 | Albert Einstein Physicist | Fifth Solvay Conference | Brussels, Germany | Participates in the fifth Solvay Conference and debates the interpretation of quantum mechanics. |
| 1928 | Paul Adrien Maurice Dirac Physicist | Relativistic Electron Equation | Cambridge, Great Britain | Formulates a relativistic quantum equation for the electron that naturally incorporates spin and implies antimatter states. |
| 1928 | Enrico Fermi Professor | Introduction to Atomic Physics Teaching | Rome, Italy | Expands advanced teaching in atomic and theoretical physics at Rome and trains a generation of Italian physicists in modern quantum methods. |
| 1928 | Ralph Howard Fowler Physicist | Field Electron Emission Theory | Cambridge, Great Britain | With Lothar Nordheim, explains electron emission from metals in strong electric fields as quantum tunnelling. |
| 1928 | Werner Heisenberg Physicist | Quantum Theory Research | Leipzig, Germany | Develops applications of quantum mechanics to atomic, molecular and solid-state physics in Leipzig. |
| 1928 | Lothar Nordheim Physicist | Field Electron Emission Theory | Cambridge, Germany | With Ralph Fowler, explains strong-field electron emission from metals using quantum tunnelling. |
| 1928 | Arnold Sommerfeld Physicist | Quantum Free-Electron Model | Munich, Germany | Applies Fermi-Dirac statistics to conduction electrons in metals, improving the classical Drude model. |
| 1929 | Erwin Rudolf Josef Alexander Schrodinger Professor | Wave Mechanics Recognition | Berlin, Austria | Continues receiving international recognition for wave mechanics as his formulation becomes a standard foundation of quantum theory. |
| 1930 | Albert Einstein Physicist | Sixth Solvay Conference | Brussels, Germany | Attends the sixth Solvay Conference and continues discussions on quantum theory and field physics. |
| 1930 | Enrico Fermi Professor | Quantum Electrodynamics Work | Rome, Italy | Pursues research in quantum electrodynamics and spectroscopic theory while leading the theoretical physics programme in Rome. |
| 1930 | Friedrich Hund Physicist | Molecular Quantum Theory | Leipzig, Germany | Develops quantum-mechanical approaches to molecular structure while working in Leipzig. |
| 1930 | Nevill Francis Mott Physicist | Relativistic Electron Scattering | Cambridge, Great Britain | Develops a quantum treatment of electron scattering by atoms that includes electron spin and relativistic effects. |
| 1930 | Erwin Rudolf Josef Alexander Schrodinger Professor | Quantum Foundations Research | Berlin, Austria | Continues research on the conceptual foundations of quantum theory while questioning purely statistical interpretations of the wave function. |
| 1931 | Erwin Rudolf Josef Alexander Schrodinger Professor | Berlin Theoretical Physics Research | Berlin, Austria | Maintains an active programme of theoretical research in Berlin while engaging with leading physicists working on quantum mechanics and field theory. |
| 1932 | Werner Heisenberg Physicist | Nobel Prize | Stockholm, Germany | Receives the Nobel Prize in Physics for creating quantum mechanics and applying the theory to the allotropic forms of hydrogen. |
| 1932 | Werner Heisenberg Physicist | Quantum Mechanics Recognition | Leipzig, Germany | His Leipzig institute gains international prominence after his Nobel recognition for quantum mechanics. |
| 1932 | Erwin Rudolf Josef Alexander Schrodinger Professor | Quantum Interpretation Debate | Berlin, Austria | Continues challenging aspects of the emerging Copenhagen interpretation and argues for a more complete wave-based account of quantum phenomena. |
| December 1933 | Paul Adrien Maurice Dirac Physicist | Nobel Prize for Quantum Electron Theory | Stockholm, Great Britain | Shares the Nobel Prize in Physics for new forms of atomic theory that include relativistic electron states. |
| 1933 | Paul Adrien Maurice Dirac Physicist | Nobel Prize | Stockholm, Great Britain | Shares the Nobel Prize in Physics for developing new productive forms of atomic theory, including a relativistic quantum theory of the electron. |
| 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. |
| 1933 | Erwin Rudolf Josef Alexander Schrodinger Nobel Laureate | Nobel Lecture on Wave Mechanics | Stockholm, Austria | Presents his Nobel lecture on wave mechanics and explains the development and physical meaning of the new quantum formalism. |
| 1933 | Erwin Rudolf Josef Alexander Schrodinger | Nobel Prize | Stockholm, Austria | Shares the Nobel Prize in Physics for discoveries in atomic theory and quantum mechanics. |
| 1934 | Erwin Rudolf Josef Alexander Schrodinger Visiting Lecturer | Princeton Lectures | Princeton, Austria | Delivers lectures at Princeton University on quantum mechanics and related theoretical problems after leaving Germany. |
| 15 May 1935 | Albert Einstein Physicist | EPR Paper | Princeton, Switzerland | Einstein, Podolsky and Rosen publish their argument that quantum mechanics may not provide a complete description of physical reality. |
| 1935 | Werner Heisenberg Physicist | Nuclear Physics Research | Leipzig, Germany | Continues nuclear and quantum research at Leipzig with students from several countries. |
| 1935 | Erwin Rudolf Josef Alexander Schrodinger Theoretical Physicist | Entanglement Concept | Oxford, Austria | Introduces and develops the concept later known as quantum entanglement to describe the inseparability of correlated quantum systems. |
| 1935 | Erwin Rudolf Josef Alexander Schrodinger Theoretical Physicist | EPR Response Papers | Oxford, Austria | Responds to the Einstein-Podolsky-Rosen argument with papers exploring the consequences of quantum correlations and the completeness of quantum mechanics. |
| 1935 | Erwin Rudolf Josef Alexander Schrodinger Theoretical Physicist | Quantum Superposition Thought Experiment | Oxford, Austria | Highlights the tension between microscopic superposition and everyday observation. |
| 1935 | Erwin Rudolf Josef Alexander Schrodinger Theoretical Physicist | Schrodingers Cat | Oxford, Austria | Introduces the cat thought experiment to illustrate quantum measurement problems. |
| 1935 | Erwin Rudolf Josef Alexander Schrodinger Theoretical Physicist | Steering Discussion | Oxford, Austria | Analyzes how measurement choices on one part of an entangled system can constrain descriptions of the other, anticipating the modern concept of quantum steering. |
| 1945 | Erwin Rudolf Josef Alexander Schrodinger Director | Postwar Dublin Research | Dublin, Austria | Continues leading theoretical research in Dublin after the Second World War while working on quantum foundations and unified-field ideas. |
| 1947 | Polykarp Kusch Physicist | Electron Magnetic Moment Anomaly | New York, United States of America | Measures a deviation of the electron magnetic moment from the simplest Dirac prediction, providing another key test for quantum electrodynamics. |
| 1947 | Willis Eugene Lamb Physicist | Lamb Shift | New York, United States of America | With Robert Retherford, measures a small shift between hydrogen electron energy levels that becomes a decisive test of quantum electrodynamics. |
| 1948 | Julian Seymour Schwinger Physicist | Electron Anomalous Magnetic Moment | Cambridge Massachusetts, United States of America | Calculates the leading quantum-electrodynamic correction to the electron magnetic moment with striking agreement to experiment. |
| 1948 | Sin-Itiro Tomonaga Physicist | Renormalized Quantum Electrodynamics | Tokyo, Japan | Develops a renormalized formulation of quantum electrodynamics for calculating electron-photon interactions. |
| 1949 | Freeman John Dyson Physicist | Unified Quantum Electrodynamics | Princeton, Great Britain | Shows the equivalence of major formulations of quantum electrodynamics and systematizes renormalized calculations involving electrons. |
| 1949 | Richard Phillips Feynman Physicist | Space-Time Quantum Electrodynamics | Ithaca, United States of America | Publishes a space-time formulation of quantum electrodynamics and diagrammatic methods for calculating electron-photon interactions. |
| 1949 | Erwin Rudolf Josef Alexander Schrodinger Director | Quantum Foundations Lectures | Dublin, Austria | Continues lecturing and writing on the conceptual foundations of quantum mechanics, emphasizing unresolved questions about measurement and physical reality. |
| 1950 | Alfred Kastler Physicist | Optical Pumping | Paris, France | Proposes using light to redistribute atoms among quantum energy states. |
| 1951 | Abdus Salam Theoretical Physicist | Doctorate | Cambridge, Pakistan | Completes a doctorate in theoretical physics at Cambridge with research that advances quantum electrodynamics. |
| 28 November 1954 | Enrico Fermi Physicist | Death of Enrico Fermi | Chicago, United States of America | Enrico Fermi dies in Chicago on 28 November 1954 after a career that transformed quantum statistics, nuclear physics and reactor science. |
| 1954 | Max Born | Nobel Prize | Stockholm, Great Britain | Shares the Nobel Prize in Physics for fundamental research in quantum mechanics, especially the statistical interpretation of the wavefunction. |
| 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 | Erwin Rudolf Josef Alexander Schrodinger Lecturer | Vienna Quantum Mechanics Lectures | Vienna, Austria | Resumes university teaching in Vienna and presents lectures on quantum mechanics, statistical physics and the conceptual foundations of modern physics. |
| January 1957 | John Archibald Wheeler Physicist | Quantum Gravity | Chapel Hill, United States of America | Discusses singularities and the need for quantum gravity beyond classical general relativity. |
| 1957 | Leo Esaki Physicist | Semiconductor Electron Tunnelling | Tokyo, Japan | Demonstrates quantum tunnelling of electrons through a semiconductor junction, leading to the tunnel diode. |
| 1959 | Erwin Rudolf Josef Alexander Schrodinger Professor | Late Quantum Foundations Work | Vienna, Austria | Continues writing and lecturing on quantum theory and philosophy during the final years of his academic life. |
| 1963 | Ennackal Chandy George Sudarshan Physicist | Optical Equivalence Theorem | Rochester, India | E. C. G. Sudarshan develops the diagonal coherent-state representation and optical equivalence theorem foundational to quantum optics. |
| 10 December 1964 | Nikolay Gennadiyevich Basov Physicist | Nobel Prize in Physics | Stockholm, Russia | Shares the Nobel Prize for fundamental work in quantum electronics. |
| 10 December 1964 | Nikolay Gennadiyevich Basov Physicist | Quantum Electronics | Stockholm, Russia | The achievement marks quantum electronics as an important Russian scientific milestone. |
| December 1965 | Richard Phillips Feynman Physicist | Nobel Prize for Quantum Electrodynamics | Stockholm, United States of America | Shares the Nobel Prize in Physics for fundamental work in quantum electrodynamics. |
| December 1965 | Julian Seymour Schwinger Physicist | Nobel Prize for Quantum Electrodynamics | Stockholm, United States of America | Shares the Nobel Prize in Physics for fundamental work in quantum electrodynamics. |
| December 1965 | Sin-Itiro Tomonaga Physicist | Nobel Prize for Quantum Electrodynamics | Stockholm, Japan | Shares the Nobel Prize in Physics for fundamental work in quantum electrodynamics. |
| 1965 | Richard Phillips Feynman | Nobel Prize | Stockholm, United States of America | Shares the Nobel Prize in Physics for fundamental work in quantum electrodynamics. |
| 1965 | Julian Schwinger | Nobel Prize | Stockholm, United States of America | Shares the Nobel Prize in Physics for fundamental work in quantum electrodynamics. |
| 1965 | Sin-Itiro Tomonaga | Nobel Prize | Stockholm, Japan | Shares the Nobel Prize in Physics for fundamental work in quantum electrodynamics. |
| 15 May 1976 | Paul Davies Physicist | Evaporating Black Hole Stress Tensor | Great Britain | With Stephen Fulling and William Unruh, calculates the quantum stress-energy tensor in a collapse model supporting the standard picture of black hole evaporation. |
| 15 May 1976 | Stephen Fulling Physicist | Evaporating Black Hole Stress Tensor | United States of America | With Paul Davies and William Unruh, calculates the quantum stress-energy tensor near an evaporating black hole. |
| 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. |
| 1976 | Stephen William Hawking Physicist | Breakdown of Predictability | Great Britain | Argues that black hole evaporation creates a fundamental challenge for predictability and quantum information conservation. |
| 1976 | William George Unruh Physicist | Relativity, Theory of | Vancouver, Great Britain | Unruh predicts that accelerated observers detect thermal radiation, connecting quantum theory and relativity |
| 1980 | Klaus von Klitzing Physicist | Integer Quantum Hall Effect | Grenoble, Germany | Discovers precisely quantized Hall resistance in a two-dimensional electron system at low temperature and high magnetic field. |
| 12 May 1982 | Francois Englert Theoretical Physicist | Francqui Prize | Brussels, Belgium | Receives the Francqui Prize for major contributions including spontaneous symmetry breaking, quantum field theory, statistical physics, relativity and cosmology. |
| 1982 | Alain Aspect Physicist | Quantum Entanglement Test | Orsay, France | Finds correlations incompatible with local hidden-variable theories. |
| 1982 | Horst Ludwig Stormer Physicist | Fractional Quantum Hall Effect | Murray Hill, Germany | With Daniel Tsui, discovers the fractional quantum Hall effect in a two-dimensional electron system. |
| 1982 | Daniel Tsui Physicist | Fractional Quantum Hall Effect | Murray Hill, United States of America | With Horst Stormer, discovers fractional quantization in a two-dimensional electron gas. |
| 1983 | Robert Betts Laughlin Physicist | Fractional Quantum Hall Theory | Livermore, United States of America | Explains fractional quantum Hall states as a strongly correlated many-electron quantum fluid with fractionally charged excitations. |
| December 1985 | Klaus von Klitzing Physicist | Nobel Prize for Quantum Hall Effect | Stockholm, Germany | Receives the Nobel Prize in Physics for discovery of the quantized Hall effect. |
| 1985 | Gerard 't Hooft Physicist | Brick Wall Model | Netherlands | Introduces the brick wall model for calculating black hole entropy from quantum fields near an event horizon. |
| 1993 | Donald Eigler Physicist | Quantum Corral Electron Standing Waves | San Jose, United States of America | Builds a ring of atoms with a scanning tunnelling microscope and images standing-wave patterns of surface electrons confined inside it. |
| 1995 | Steven Weinberg Theoretical Physicist | Quantum Theory of Fields | United States of America, United States of America | Publishes the first volume of The Quantum Theory of Fields, synthesizing modern quantum field theory for advanced researchers and students. |
| 1997 | Juan Maldacena Physicist | AdS-CFT Correspondence | Argentina | Proposes the AdS-CFT correspondence, providing a non-gravitational description of quantum gravity that became central to modern studies of black holes and information. |
| 1997 | Anton Zeilinger Quantum Physicist | Quantum Teleportation Experiment | Innsbruck, Austria | Co-demonstrates experimental quantum teleportation using entangled photons. |
| 1997 | Anton Zeilinger Quantum Physicist | Teleportation of a Photon State | Innsbruck, Austria | Transfers an unknown photon state without transporting the original particle. |
| December 1998 | Robert Betts Laughlin Physicist | Nobel Prize for Fractional Quantum Hall Effect | Stockholm, United States of America | Shares the Nobel Prize in Physics for explaining the fractional quantum Hall effect. |
| December 1998 | Horst Ludwig Stormer Physicist | Nobel Prize for Fractional Quantum Hall Effect | Stockholm, Germany | Shares the Nobel Prize in Physics for discovery of the fractional quantum Hall effect. |
| December 1998 | Daniel Tsui Physicist | Nobel Prize for Fractional Quantum Hall Effect | Stockholm, United States of America | Shares the Nobel Prize in Physics for discovery of the fractional quantum Hall effect. |
| 1998 | David DiVincenzo Physicist | Electron Spin Qubit Proposal | United States of America, United States of America | With Daniel Loss, proposes quantum-dot electron spins as controllable quantum bits. |
| 1998 | Daniel Loss Physicist | Electron Spin Qubit Proposal | Basel, Switzerland | With David DiVincenzo, proposes using the spin states of individual electrons in quantum dots as quantum bits. |
| 1999 | Geradus 't Hooft | Nobel Prize | Stockholm, Netherlands | Shares the Nobel Prize in Physics for elucidating the quantum structure of electroweak interactions. |
| 1999 | Martinus Veltman | Nobel Prize | Stockholm, Netherlands | Shares the Nobel Prize in Physics for elucidating the quantum structure of electroweak interactions. |
| 2001 | Hartmut Haffner Physicist | Bound Electron g-Factor Measurement | Mainz, Germany | Helps measure the magnetic moment of a bound electron in hydrogenlike carbon with a Penning trap, providing a precision test of strong-field quantum electrodynamics. |
| 2002 | Samir Mathur Physicist | Fuzzball Proposal | India | Develops the fuzzball proposal in string theory, replacing the conventional black hole interior with horizon-scale quantum microstate structure. |
| 2004 | Stephen William Hawking Physicist | Black Hole Information Revision | Dublin, Great Britain | Announces a revised position on the black hole information problem, arguing that quantum information need not be permanently lost. |
| 2005 | Charles Kane Physicist | Quantum Spin Hall Effect Theory | Philadelphia, United States of America | With Eugene Mele, predicts a two-dimensional topological state whose edge channels carry spin-filtered electrons protected by time-reversal symmetry. |
| 2005 | Philip Kim Physicist | Graphene Quantum Hall Effect | New York, South Korea | Demonstrates unusual quantum Hall behaviour of charge carriers in graphene. |
| 2005 | Eugene Mele Physicist | Quantum Spin Hall Theory | Philadelphia, United States of America | With Charles Kane, develops the theoretical model for a quantum spin Hall state with protected electron edge channels. |
| 2006 | Shoucheng Zhang Physicist | HgTe Quantum Spin Hall Prediction | Stanford, United States of America | With collaborators, predicts a quantum spin Hall state in mercury-telluride quantum wells. |
| 2007 | Laurens Molenkamp Physicist | Quantum Spin Hall Effect Observed | Wurzburg, Netherlands | Leads experiments in mercury-telluride quantum wells that observe edge conduction associated with the quantum spin Hall state. |
| 2007 | Laurens Molenkamp Physicist | Quantum Spin Hall Experiment | Wurzburg, Netherlands | Leads experiments observing edge conduction consistent with the quantum spin Hall effect in mercury-telluride wells. |
| 2010 | Charles Marcus Physicist | Coherent Single-Electron Transport | Cambridge Massachusetts, United States of America | Advances controlled quantum transport of individual electrons in semiconductor nanostructures. |
| 2011 | Francois Englert Theoretical Physicist | Chapman University | Orange, California, Belgium | Joins Chapman University's Institute for Quantum Studies as a distinguished visiting professor and founding member. |
| 2012 | Serge Haroche | Nobel Prize | Stockholm, France | Shares the Nobel Prize in Physics for experimental methods enabling measurement and manipulation of individual quantum systems. |
| 2012 | Donald Marolf Physicist | Black Hole Firewall | United States of America | With collaborators, formulates the firewall paradox as a challenge to conventional assumptions about black hole horizons and quantum information. |
| 2012 | David J. Wineland | Nobel Prize | Stockholm, United States of America | Shares the Nobel Prize in Physics for experimental methods enabling measurement and manipulation of individual quantum systems. |
| 2013 | Juan Maldacena Physicist | ER Equals EPR | Argentina | With Leonard Susskind, proposes that quantum entanglement and Einstein-Rosen bridges may be deeply connected, a conjecture known as ER equals EPR. |
| 2013 | Leonard Susskind Physicist | ER Equals EPR | United States of America | With Juan Maldacena, proposes the ER equals EPR conjecture connecting entanglement with wormhole geometry in quantum gravity. |
| 2016 | Stephen William Hawking Physicist | Soft Hair on Black Holes | Great Britain | With Malcolm Perry and Andrew Strominger, proposes that soft quantum degrees of freedom on horizons may carry information about black holes. |
| 2016 | Malcolm Perry Physicist | Soft Hair on Black Holes | Great Britain | With Stephen Hawking and Andrew Strominger, develops the proposal that black hole horizons can carry soft quantum hair. |
| 2019 | Geoffrey Penington Physicist | Entanglement Wedge Reconstruction | Great Britain | Shows how quantum extremal surfaces can reproduce a Page curve and recover information from an evaporating black hole in holographic models. |
| 2020 | Juan Maldacena Physicist | Semiclassical Page Curve | Argentina | With collaborators, derives the Page curve of Hawking radiation from semiclassical gravity using replica methods and quantum extremal surfaces. |
| 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. |
| 10 December 2022 | Alain Aspect Physicist | Nobel Prize in Physics | Stockholm, France | Shares the physics prize for experiments with entangled photons and advances in quantum information science. |
| 10 December 2022 | Anton Zeilinger Physicist | Nobel Prize in Physics | Stockholm, Austria | Shares the physics prize for experiments with entangled photons and advances in quantum information science. |
| 2022 | Alain Aspect | Nobel Prize | Stockholm, France | Shares the Nobel Prize in Physics for experiments with entangled photons, Bell inequality violations and pioneering quantum information science. |
| 2022 | John F. Clauser | Nobel Prize | Stockholm, United States of America | Shares the Nobel Prize in Physics for experiments with entangled photons, Bell inequality violations and pioneering quantum information science. |
| 2022 | Anton Zeilinger | Nobel Prize | Stockholm, Austria | Shares the Nobel Prize in Physics for experiments with entangled photons, Bell inequality violations and pioneering quantum information science. |
| 2025 | John Clarke | Nobel Prize | Stockholm, Great Britain | Shares the Nobel Prize in Physics for discovering macroscopic quantum tunnelling and energy quantisation in an electric circuit. |
| 2025 | Michel H. Devoret | Nobel Prize | Stockholm, France | Shares the Nobel Prize in Physics for discovering macroscopic quantum tunnelling and energy quantisation in an electric circuit. |
| 2025 | John M. Martinis | Nobel Prize | Stockholm, United States of America | Shares the Nobel Prize in Physics for discovering macroscopic quantum tunnelling and energy quantisation in an electric circuit. |
| 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. |