.
Timeline of quantum mechanics
This timeline of quantum mechanics shows the key steps, precursors and contributors to the development of quantum mechanics, quantum field theories and quantum chemistry.[1][2]
19th century
Image of Becquerel's photographic plate which has been fogged by exposure to radiation from a uranium salt. The shadow of a metal Maltese Cross placed between the plate and the uranium salt is clearly visible.
1859 – Kirchhoff introduces the concept of a blackbody and proves that its emission spectrum depends only on its temperature.[1]
1860–1900 – Ludwig Eduard Boltzmann, James Clerk Maxwell and others develop the theory of statistical mechanics. Boltzmann argues that entropy is a measure of disorder.[1]
1877 – Boltzmann suggests that the energy levels of a physical system could be discrete based on statistical mechanics and mathematical arguments; also produces the first circle diagram representation, or atomic model of a molecule (such as an iodine gas molecule) in terms of the overlapping terms α and β, later (in 1928) called molecular orbitals, of the constituting atoms.
1887 – Heinrich Hertz discovers the photoelectric effect, shown by Einstein in 1905 to involve quanta of light.
1888 – Hertz demonstrates experimentally that electromagnetic waves exist, as predicted by Maxwell.[1]
1888 – Johannes Rydberg modifies the Balmer formula to include all spectral series of lines for the hydrogen atom, producing the Rydberg formula which is employed later by Niels Bohr and others to verify Bohr's first quantum model of the atom.
1895 – Wilhelm Conrad Röntgen discovers X-rays in experiments with electron beams in plasma.[1]
1896 – Antoine Henri Becquerel accidentally discovers radioactivity while investigating the work of Wilhelm Conrad Röntgen; he finds that uranium salts emit radiation that resembled Röntgen's X-rays in their penetrating power. In one experiment, Becquerel wraps a sample of a phosphorescent substance, potassium uranyl sulfate, in photographic plates surrounded by very thick black paper in preparation for an experiment with bright sunlight; then, to his surprise, the photographic plates are already exposed before the experiment starts, showing a projected image of his sample.[1][3]
1896 – Pieter Zeeman first observes the Zeeman splitting effect by passing the light emitted by hydrogen through a magnetic field.
1896–1897 Marie Curie (née Skłodowska, Becquerel's doctoral student) investigates uranium salt samples using a very sensitive electrometer device that was invented 15 years before by her husband and his brother Jacques Curie to measure electrical charge. She discovers that rays emitted by the uranium salt samples make the surrounding air electrically conductive, and measures the emitted rays' intensity. In April 1898, through a systematic search of substances, she finds that thorium compounds, like those of uranium, emitted "Becquerel rays", thus preceding the work of Frederick Soddy and Ernest Rutherford on the nuclear decay of thorium to radium by three years.[4]
1897 – Ivan Borgman demonstrates that X-rays and radioactive materials induce thermoluminescence.
1899 to 1903 – Ernest Rutherford, 1st Baron, Lord Rutherford of Nelson, of Cambridge, OM, FRS: During the investigation of radioactivity he coins the terms alpha and beta rays in 1899 to describe the two distinct types of radiation emitted by thorium and uranium salts. Ernest Rutherford is joined at McGill University in 1900 by Frederick Soddy and together they discover nuclear transmutation when they find in 1902 that radioactive thorium is converting itself into radium through a process of nuclear decay and a gas (later found to be 4
2He); they report their interpretation of radioactivity in 1903.[5] Sir Ernest Rutherford becomes known as the "father of nuclear physics": with his nuclear atom model of 1911 he leads the exploration of nuclear physics.[6]
20th century
1900–1909
Einstein, in 1905, when he wrote the Annus Mirabilis papers
1900 – To explain black-body radiation (1862), Max Planck suggests that electromagnetic energy could only be emitted in quantized form, i.e. the energy could only be a multiple of an elementary unit E = hν, where h is Planck's constant and ν is the frequency of the radiation.
1902 – To explain the octet rule (1893), Gilbert N. Lewis develops the "cubical atom" theory in which electrons in the form of dots are positioned at the corner of a cube. Predicts that single, double, or triple "bonds" result when two atoms are held together by multiple pairs of electrons (one pair for each bond) located between the two atoms.
1903 – Antoine Becquerel, Pierre Curie and Marie Curie share the 1903 Nobel Prize in Physics for their work on spontaneous radioactivity.
1904 – Richard Abegg notes the pattern that the numerical difference between the maximum positive valence, such as +6 for H2SO4, and the maximum negative valence, such as −2 for H2S, of an element tends to be eight (Abegg's rule).
1905 – Albert Einstein explains the photoelectric effect (reported in 1887 by Heinrich Hertz), i.e. that shining light on certain materials can function to eject electrons from the material. He postulates, as based on Planck's quantum hypothesis (1900), that light itself consists of individual quantum particles (photons).
1905 – Einstein explains the effects of Brownian motion as caused by the kinetic energy (i.e., movement) of atoms, which was subsequently, experimentally verified by Jean Baptiste Perrin, thereby settling the century-long dispute about the validity of John Dalton's atomic theory.
1905 – Einstein publishes his Special Theory of Relativity.
1905 – Einstein theoretically derives the equivalence of matter and energy.
1907 to 1917 – Ernest Rutherford: To test his planetary model of 1904, later known as the Rutherford model, he sent a beam of positively charged alpha particles onto a gold foil and noticed that some bounced back, thus showing that an atom has a small-sized positively charged atomic nucleus at its center. However, he received in 1908 the Nobel Prize in Chemistry "for his investigations into the disintegration of the elements, and the chemistry of radioactive substances",[7] which followed on the work of Marie Curie, not for his planetary model of the atom; he is also widely credited with first "splitting the atom" in 1917. In 1911 Ernest Rutherford explained the Geiger–Marsden experiment by invoking a nuclear atom model and derived the Rutherford cross section.
1909 – Geoffrey Ingram Taylor demonstrates that interference patterns of light were generated even when the light energy introduced consisted of only one photon. This discovery of the wave–particle duality of matter and energy is fundamental to the later development of quantum field theory.
1909 and 1916 – Einstein shows that, if Planck's law of black-body radiation is accepted, the energy quanta must also carry momentum p = h / λ, making them full-fledged particles.
1910–1919
A schematic diagram of the apparatus for Millikan's refined oil drop experiment.
1911 – Lise Meitner and Otto Hahn perform an experiment that shows that the energies of electrons emitted by beta decay had a continuous rather than discrete spectrum. This is in apparent contradiction to the law of conservation of energy, as it appeared that energy was lost in the beta decay process. A second problem is that the spin of the Nitrogen-14 atom was 1, in contradiction to the Rutherford prediction of ½. These anomalies are later explained by the discoveries of the neutrino and the neutron.
1911 – Ștefan Procopiu performs experiments in which he determines the correct value of electron's magnetic dipole moment, μB = 9.27×10−21 erg·Oe−1 (in 1913 he is also able to calculate a theoretical value of the Bohr magneton based on Planck's quantum theory).
1912 – Victor Hess discovers the existence of cosmic radiation.
1912 – Henri Poincaré publishes an influential mathematical argument in support of the essential nature of energy quanta.[8][9]
1913 – Robert Andrews Millikan publishes the results of his "oil drop" experiment, in which he precisely determines the electric charge of the electron. Determination of the fundamental unit of electric charge makes it possible to calculate the Avogadro constant (which is the number of atoms or molecules in one mole of any substance) and thereby to determine the atomic weight of the atoms of each element.
1913 – Ștefan Procopiu publishes a theoretical paper with the correct value of the electron's magnetic dipole moment μB.[10]
1913 – Niels Bohr obtains theoretically the value of the electron's magnetic dipole moment μB as a consequence of his atom model
1913 – Johannes Stark and Antonino Lo Surdo independently discover the shifting and splitting of the spectral lines of atoms and molecules due to the presence of the light source in an external static electric field.
1913 – To explain the Rydberg formula (1888), which correctly modeled the light emission spectra of atomic hydrogen, Bohr hypothesizes that negatively charged electrons revolve around a positively charged nucleus at certain fixed "quantum" distances and that each of these "spherical orbits" has a specific energy associated with it such that electron movements between orbits requires "quantum" emissions or absorptions of energy.
1914 – James Franck and Gustav Hertz report their experiment on electron collisions with mercury atoms, which provides a new test of Bohr's quantized model of atomic energy levels.[11]
1915 – Einstein first presents to the Prussian Academy of Science what are now known as the Einstein field equations. These equations specify how the geometry of space and time is influenced by whatever matter is present, and form the core of Einstein's General Theory of Relativity. Although this theory is not directly applicable to quantum mechanics, theorists of quantum gravity seek to reconcile them.
1916 – Paul Epstein[12] and Karl Schwarzschild,[13] working independently, derive equations for the linear and quadratic Stark effect in hydrogen.
1916 – To account for the Zeeman effect (1896), i.e. that atomic absorption or emission spectral lines change when the light source is subjected to a magnetic field, Arnold Sommerfeld suggests there might be "elliptical orbits" in atoms in addition to spherical orbits.
1918 – Sir Ernest Rutherford notices that, when alpha particles are shot into nitrogen gas, his scintillation detectors shows the signatures of hydrogen nuclei. Rutherford determines that the only place this hydrogen could have come from was the nitrogen, and therefore nitrogen must contain hydrogen nuclei. He thus suggests that the hydrogen nucleus, which is known to have an atomic number of 1, is an elementary particle, which he decides must be the protons hypothesized by Eugen Goldstein.
1919 – Building on the work of Lewis (1916), Irving Langmuir coins the term "covalence" and postulates that coordinate covalent bonds occur when two electrons of a pair of atoms come from both atoms and are equally shared by them, thus explaining the fundamental nature of chemical bonding and molecular chemistry.
1920–1929
A plaque at the University of Frankfurt commemorating the Stern–Gerlach experiment.
1921–1922 – Frederick Soddy receives the Nobel Prize for 1921 in Chemistry one year later, in 1922, "for his contributions to our knowledge of the chemistry of radioactive substances, and his investigations into the origin and nature of isotopes"; he writes in his Nobel Lecture of 1922: "The interpretation of radioactivity which was published in 1903 by Sir Ernest Rutherford and myself ascribed the phenomena to the spontaneous disintegration of the atoms of the radio-element, whereby a part of the original atom was violently ejected as a radiant particle, and the remainder formed a totally new kind of atom with a distinct chemical and physical character."
1922 – Arthur Compton finds that X-ray wavelengths increase due to scattering of the radiant energy by free electrons. The scattered quanta have less energy than the quanta of the original ray. This discovery, known as the Compton effect or Compton scattering, demonstrates the particle concept of electromagnetic radiation.
1922 – Otto Stern and Walther Gerlach perform the Stern–Gerlach experiment, which detects discrete values of angular momentum for atoms in the ground state passing through an inhomogeneous magnetic field leading to the discovery of the spin of the electron.
1922 – Bohr updates his model of the atom to better explain the properties of the periodic table by assuming that certain numbers of electrons (for example 2, 8 and 18) corresponded to stable "closed shells", presaging orbital theory.
1923 – Pierre Auger discovers the Auger effect, where filling the inner-shell vacancy of an atom is accompanied by the emission of an electron from the same atom.
1923 – Louis de Broglie extends wave–particle duality to particles, postulating that electrons in motion are associated with waves. He predicts that the wavelengths are given by Planck's constant h divided by the momentum of the mv = p of the electron: λ = h / mv = h / p.[1]
1923 – Gilbert N. Lewis creates the theory of Lewis acids and bases based on the properties of electrons in molecules, defining an acid as accepting an electron lone pair from a base.
1924 – Satyendra Nath Bose explains Planck's law using a new statistical law that governs bosons, and Einstein generalizes it to predict Bose–Einstein condensate. The theory becomes known as Bose–Einstein statistics.[1]
1924 – Wolfgang Pauli outlines the "Pauli exclusion principle" which states that no two identical fermions may occupy the same quantum state simultaneously, a fact that explains many features of the periodic table.[1]
1925 – George Uhlenbeck and Samuel Goudsmit postulate the existence of electron spin.[1]
1925 – Friedrich Hund outlines Hund's rule of Maximum Multiplicity which states that when electrons are added successively to an atom as many levels or orbits are singly occupied as possible before any pairing of electrons with opposite spin occurs and made the distinction that the inner electrons in molecules remained in atomic orbitals and only the valence electrons needed to be in molecular orbitals involving both nuclei.
1925 – Werner Heisenberg, Max Born, and Pascual Jordan develops the matrix mechanics formulation of Quantum Mechanics.[1]
1926 – Lewis coins the term photon in a letter to the scientific journal Nature, which he derives from the Greek word for light, φως (transliterated phôs).[14]
1926 – Oskar Klein and Walter Gordon state their relativistic quantum wave equation, later called the Klein–Gordon equation.
1926 – Enrico Fermi discovers the spin-statistics theorem connection.
1926 – Paul Dirac introduces Fermi–Dirac statistics.
1926 – Erwin Schrödinger uses De Broglie's electron wave postulate (1924) to develop a "wave equation" that represents mathematically the distribution of a charge of an electron distributed through space, being spherically symmetric or prominent in certain directions, i.e. directed valence bonds, which gives the correct values for spectral lines of the hydrogen atom; also introduces the Hamiltonian operator in quantum mechanics.
1926 – Paul Epstein reconsiders the linear and quadratic Stark effect from the point of view of the new quantum theory, using the equations of Schrödinger and others. The derived equations for the line intensities are a decided improvement over previous results obtained by Hans Kramers.[15]
1926 to 1932 – John von Neumann lays the mathematical foundations of Quantum Mechanics in terms of Hermitian operators on Hilbert spaces, subsequently published in 1932 as a basic textbook of quantum mechanics.[1][16]
1927 – Werner Heisenberg formulates the quantum uncertainty principle.[1]
1927 – Max Born develops the Copenhagen interpretation of the probabilistic nature of wavefunctions.
1927 – Born and J. Robert Oppenheimer introduce the Born–Oppenheimer approximation, which allows the quick approximation of the energy and wavefunctions of smaller molecules.
1927 – Walter Heitler and Fritz London introduce the concepts of valence bond theory and apply it to the hydrogen molecule.
1927 – Thomas and Fermi develop the Thomas–Fermi model for a Gas in a box.
1927 – Chandrasekhara Venkata Raman studies optical photon scattering by electrons.
1927 – Dirac states his relativistic electron quantum wave equation, the Dirac equation.
1927 – Charles G. Darwin and Walter Gordon solve the Dirac equation for a Coulomb potential.
1927 – Charles Drummond Ellis (along with James Chadwick and colleagues) finally establish clearly that the beta decay spectrum is in fact continuous and not discrete, posing a problem that will later be solved by theorizing (and later discovering) the existence of the neutrino.
1927 – Walter Heitler uses Schrödinger's wave equation to show how two hydrogen atom wavefunctions join together, with plus, minus, and exchange terms, to form a covalent bond.
1927 – Robert Mulliken works, in coordination with Hund, to develop a molecular orbital theory where electrons are assigned to states that extend over an entire molecule and, in 1932, introduces many new molecular orbital terminologies, such as σ bond, π bond, and δ bond.
1927 – Eugene Wigner relates degeneracies of quantum states to irreducible representations of symmetry groups.
1927 – Hermann Klaus Hugo Weyl proves in collaboration with his student Fritz Peter a fundamental theorem in harmonic analysis—the Peter–Weyl theorem—relevant to group representations in quantum theory (including the complete reducibility of unitary representations of a compact topological group);[17] introduces the Weyl quantization, and earlier, in 1918, introduces the concept of gauge and a gauge theory; later in 1935 he introduces and characterizes with Richard Bauer the concept of spinor in n-dimensions.[18]
1928 – Linus Pauling outlines the nature of the chemical bond: uses Heitler's quantum mechanical covalent bond model to outline the quantum mechanical basis for all types of molecular structure and bonding and suggests that different types of bonds in molecules can become equalized by rapid shifting of electrons, a process called "resonance" (1931), such that resonance hybrids contain contributions from the different possible electronic configurations.
1928 – Friedrich Hund and Robert S. Mulliken introduce the concept of molecular orbitals.
1928 – Born and Vladimir Fock formulate and prove the adiabatic theorem, which states that a physical system shall remain in its instantaneous eigenstate if a given perturbation is acting on it slowly enough and if there is a gap between the eigenvalue and the rest of the Hamiltonian's spectrum.
1929 – Oskar Klein discovers the Klein paradox
1929 – Oskar Klein and Yoshio Nishina derive the Klein–Nishina cross section for high energy photon scattering by electrons
1929 – Sir Nevill Mott derives the Mott cross section for the Coulomb scattering of relativistic electrons
1929 – John Lennard-Jones introduces the linear combination of atomic orbitals approximation for the calculation of molecular orbitals.
1929 – Fritz Houtermans and Robert d'Escourt Atkinson propose that stars release energy by nuclear fusion.[1]
1930–1939
Electron microscope constructed by Ernst Ruska in 1933.
1930 – Dirac hypothesizes the existence of the positron.[1]
1930 – Dirac's textbook Principles of Quantum Mechanics is published, becoming a standard reference book that is still used today.
1930 – Erich Hückel introduces the Hückel molecular orbital method, which expands on orbital theory to determine the energies of orbitals of pi electrons in conjugated hydrocarbon systems.
1930 – Fritz London explains van der Waals forces as due to the interacting fluctuating dipole moments between molecules
1930 – Pauli suggests in a famous letter that, in addition to electrons and protons, atoms also contain an extremely light neutral particle which he calls the "neutron." He suggests that this "neutron" is also emitted during beta decay and has simply not yet been observed. Later it is determined that this particle is actually the almost massless neutrino.[1]
1931 – John Lennard-Jones proposes the Lennard-Jones interatomic potential
1931 – Walther Bothe and Herbert Becker find that if the very energetic alpha particles emitted from polonium fall on certain light elements, specifically beryllium, boron, or lithium, an unusually penetrating radiation is produced. At first this radiation is thought to be gamma radiation, although it is more penetrating than any gamma rays known, and the details of experimental results are very difficult to interpret on this basis. Some scientists begin to hypothesize the possible existence of another fundamental particle.
1931 – Erich Hückel redefines the property of aromaticity in a quantum mechanical context by introducing the 4n+2 rule, or Hückel's rule, which predicts whether an organic planar ring molecule will have aromatic properties.
1931 – Ernst Ruska creates the first electron microscope.[1]
1931 – Ernest Lawrence creates the first cyclotron and founds the Radiation Laboratory, later the Lawrence Berkeley National Laboratory; in 1939 he awarded the Nobel Prize in Physics for his work on the cyclotron.
1932 – Irène Joliot-Curie and Frédéric Joliot show that if the unknown radiation generated by alpha particles falls on paraffin or any other hydrogen-containing compound, it ejects protons of very high energy. This is not in itself inconsistent with the proposed gamma ray nature of the new radiation, but detailed quantitative analysis of the data become increasingly difficult to reconcile with such a hypothesis.
1932 – James Chadwick performs a series of experiments showing that the gamma ray hypothesis for the unknown radiation produced by alpha particles is untenable, and that the new particles must be the neutrons hypothesized by Fermi.[1]
1932 – Werner Heisenberg applies perturbation theory to the two-electron problem to show how resonance arising from electron exchange can explain exchange forces.
1932 – Mark Oliphant: Building upon the nuclear transmutation experiments of Ernest Rutherford done a few years earlier, observes fusion of light nuclei (hydrogen isotopes). The steps of the main cycle of nuclear fusion in stars are subsequently worked out by Hans Bethe over the next decade.
1932 – Carl D. Anderson experimentally proves the existence of the positron.[1]
1933 – Following Chadwick's experiments, Fermi renames Pauli's "neutron" to neutrino to distinguish it from Chadwick's theory of the much more massive neutron.
1933 – Leó Szilárd first theorizes the concept of a nuclear chain reaction. He files a patent for his idea of a simple nuclear reactor the following year.
1934 – Fermi publishes a very successful model of beta decay in which neutrinos are produced.
1934 – Fermi studies the effects of bombarding uranium isotopes with neutrons.
1934 – N. N. Semyonov develops the total quantitative chain chemical reaction theory, later the basis of various high technologies using the incineration of gas mixtures. The idea is also used for the description of the nuclear reaction.
1934 – Irène Joliot-Curie and Frédéric Joliot-Curie discover artificial radioactivity and are jointly awarded the 1935 Nobel Prize in Chemistry[19]
1935 – Einstein, Boris Podolsky, and Nathan Rosen describe the EPR paradox which challenges the completeness of quantum mechanics as it was theorized up to that time. Assuming that local realism is valid, they demonstrated that there would need to be hidden parameters to explain how measuring the quantum state of one particle could influence the quantum state of another particle without apparent contact between them.[20]
1935 - Schrödinger develops the Schrödinger's cat thought experiment. It illustrates what he saw as the problems of the Copenhagen interpretation of quantum mechanics if subatomic particles can be in two contradictory quantum states at once.
1935 – Hideki Yukawa formulates his hypothesis of the Yukawa potential and predicts the existence of the pion, stating that such a potential arises from the exchange of a massive scalar field, as it would be found in the field of the pion. Prior to Yukawa's paper, it was believed that the scalar fields of the fundamental forces necessitated massless particles.
1936 – Alexandru Proca publishes prior to Hideki Yukawa his relativistic quantum field equations for a massive vector meson of spin-1 as a basis for nuclear forces.
1936 – Garrett Birkhoff and John von Neumann introduce Quantum Logic[21] in an attempt to reconcile the apparent inconsistency of classical, Boolean logic with the Heisenberg Uncertainty Principle of quantum mechanics as applied, for example, to the measurement of complementary (noncommuting) observables in quantum mechanics, such as position and momentum;[22] current approaches to quantum logic involve noncommutative and non-associative many-valued logic.[23][24]
1936 – Carl D. Anderson discovers muons while he is studying cosmic radiation.
1937 – Carl Anderson experimentally proves the existence of the pion.
1937 – Hermann Arthur Jahn and Edward Teller prove, using group theory, that non-linear degenerate molecules are unstable.[25] The Jahn-Teller theorem essentially states that any non-linear molecule with a degenerate electronic ground state will undergo a geometrical distortion that removes that degeneracy, because the distortion lowers the overall energy of the complex. The latter process is called the Jahn-Teller effect; this effect was recently considered also in relation to the superconductivity mechanism in YBCO and other high temperature superconductors. The details of the Jahn-Teller effect are presented with several examples and EPR data in the basic textbook by Abragam and Bleaney (1970).
1938 – Charles Coulson makes the first accurate calculation of a molecular orbital wavefunction with the hydrogen molecule.
1938 – Otto Hahn and his assistant Fritz Strassmann send a manuscript to Naturwissenschaften reporting they have detected the element barium after bombarding uranium with neutrons. Hahn calls this new phenomenon a 'bursting' of the uranium nucleus. Simultaneously, Hahn communicate these results to Lise Meitner. Meitner, and her nephew Otto Robert Frisch, correctly interpret these results as being a nuclear fission. Frisch confirms this experimentally on 13 January 1939.
1939 – Leó Szilárd and Fermi discover neutron multiplication in uranium, proving that a chain reaction is indeed possible.
1940–1949
A Feynman diagram showing the radiation of a gluon when an electron and positron are annihilated.
1942 – Kan-Chang Wang first proposes the use of K-electron capture to experimentally detect neutrinos.
1942 – A team led by Enrico Fermi creates the first artificial self-sustaining nuclear chain reaction, called Chicago Pile-1, in a racquets court below the bleachers of Stagg Field at the University of Chicago on December 2, 1942.
1942 to 1946 – J. Robert Oppenheimer successfully leads the Manhattan Project, predicts quantum tunneling and proposes the Oppenheimer–Phillips process in nuclear fusion
1945 – the Manhattan Project produces the first nuclear fission explosion on July 16, 1945 in the Trinity test in New Mexico.
1945 – John Archibald Wheeler and Richard Feynman originate Wheeler–Feynman absorber theory, an interpretation of electrodynamics that supposes that elementary particles are not self-interacting.
1946 – Theodor V. Ionescu and Vasile Mihu report the construction of the first hydrogen maser by stimulated emission of radiation in molecular hydrogen.
1947 – Willis Lamb and Robert Retherford measure a small difference in energy between the energy levels 2S1/2 and 2P1/2 of the hydrogen atom, known as the Lamb shift.
1947 – George Rochester and Clifford Charles Butler publishes two cloud chamber photographs of cosmic ray-induced events, one showing what appears to be a neutral particle decaying into two charged pions, and one that appears to be a charged particle decaying into a charged pion and something neutral. The estimated mass of the new particles is very rough, about half a proton's mass. More examples of these "V-particles" were slow in coming, and they are soon given the name kaons.
1948 – Sin-Itiro Tomonaga and Julian Schwinger Independently introduce perturbative renormalization as a method of correcting the original Lagrangian of a quantum field theory so as to eliminate a series of infinite terms that would otherwise result.
1948 – Richard Feynman states the path integral formulation of quantum mechanics.
1949 – Freeman Dyson determines the equivalence of two formulations of quantum electrodynamics: Feynman's diagrammatic path integral formulation and the operator method developed by Julian Schwinger and Tomonaga. A by-product of that demonstration is the invention of the Dyson series.[26]
1950–1959
1951 – Clemens C. J. Roothaan and George G. Hall derive the Roothaan-Hall equations, putting rigorous molecular orbital methods on a firm basis.
1951 – Edward Teller, physicist and "father of the hydrogen bomb", and Stanislaw Ulam, mathematician, are reported to have written jointly in March 1951 a classified report on "Hydrodynamic Lenses and Radiation Mirrors" that results in the next step in the Manhattan Project.[27]
1951 and 1952 – at the Manhattan Project, the first planned fusion thermonuclear reaction experiment is carried out successfully in the Spring of 1951 at Eniwetok, based on the work of Edward Teller and Dr. Hans A. Bethe.[28] The Los Alamos Laboratory proposes a date in November 1952 for a hydrogen bomb, full-scale test that is apparently carried out.
1951 – Felix Bloch and Edward Mills Purcell receive a shared Nobel Prize in Physics for their first observations of the quantum phenomenon of nuclear magnetic resonance previously reported in 1949.[29][30][31] Purcell reports his contribution as Research in Nuclear Magnetism, and gives credit to his coworkers such as Herbert S. Gutowsky for their NMR contributions,[32][33] as well as theoretical researchers of nuclear magnetism such as John Hasbrouck Van Vleck.
1952 – Albert W. Overhauser formulates a theory of dynamic nuclear polarization, also known as the Overhauser Effect; other contenders are the subsequent theory of Ionel Solomon reported in 1955 that includes the Solomon equations for the dynamics of coupled spins, and that of R. Kaiser in 1963. The general Overhauser effect is first demonstrated experimentally by T. R. Carver and Charles P. Slichter in 1953.[34]
1952 – Donald A. Glaser creates the bubble chamber, which allows detection of electrically charged particles by surrounding them by a bubble. Properties of the particles such as momentum can be determined by studying of their helical paths. Glaser receives a Nobel prize in 1960 for his invention.
1953 – Charles H. Townes, collaborating with James P. Gordon, and H. J. Zeiger, builds the first ammonia maser; receives a Nobel prize in 1964 for his experimental success in producing coherent radiation by atoms and molecules.
1954 – Chen Ning Yang and Robert Mills derive a gauge theory for nonabelian groups, leading to the successful formulation of both electroweak unification and quantum chromodynamics.
1955 – Ionel Solomon develops the first nuclear magnetic resonance theory of magnetic dipole coupled nuclear spins and of the Nuclear Overhauser Effect.
1955 and 1956 – Murray Gell-Mann and Kazuhiko Nishijima independently derive the Gell-Mann–Nishijima formula, which relates the baryon number, the strangeness, and the isospin of hadrons to the charge, eventually leading to the systematic categorization of hadrons and, ultimately, the Quark Model of hadron composition.
1956 – P. Kuroda predicts that self-sustaining nuclear chain reactions should occur in natural uranium deposits.
1956 – Chien-Shiung Wu carries out the Wu Experiment, which observes parity violation in cobalt-60 decay, showing that parity violation is present in the weak interaction.
1956 – Clyde L. Cowan and Frederick Reines experimentally prove the existence of the neutrino.
1957 – John Bardeen, Leon Cooper and John Robert Schrieffer propose their quantum BCS theory of low temperature superconductivity, for which their receive a Nobel prize in 1972. The theory represents superconductivity as a macroscopic quantum coherence phenomenon involving phonon coupled electron pairs with opposite spin
1957 – William Alfred Fowler, Margaret Burbidge, Geoffrey Burbidge, and Fred Hoyle, in their 1957 paper Synthesis of the Elements in Stars, show that the abundances of essentially all but the lightest chemical elements can be explained by the process of nucleosynthesis in stars.
1957 – Hugh Everett formulates the many-worlds interpretation of quantum mechanics, which states that every possible quantum outcome is realized in divergent, non-communicating parallel universes in quantum superposition.[35][36]
1958–1959 – magic angle spinning described by Edward Raymond Andrew, A. Bradbury, and R. G. Eades, and independently in 1959 by I. J. Lowe.[37]
1960–1969
The baryon decuplet of the Eightfold Way proposed by Murray Gell-Mann in 1962. The Ω− particle at the bottom had not yet been observed at the time, but a particle closely matching these predictions was discovered[38] by a particle accelerator group at Brookhaven, proving Gell-Mann's theory.
1961 – Clauss Jönsson performs Young's double-slit experiment (1909) for the first time with particles other than photons by using electrons and with similar results, confirming that massive particles also behaved according to the wave–particle duality that is a fundamental principle of quantum field theory.
1961 – Anatole Abragam publishes the fundamental textbook on the quantum theory of Nuclear Magnetic Resonance entitled The Principles of Nuclear Magnetism;[39]
1961 – Sheldon Lee Glashow extends the electroweak interaction modelss developed by Julian Schwinger by including a short range neutral current, the Z_o. The resulting symmetry structure that Glashow proposes, SU(2) X U(1), forms the basis of the accepted theory of the electroweak interactions.
1962 – Leon M. Lederman, Melvin Schwartz and Jack Steinberger show that more than one type of neutrino exists by detecting interactions of the muon neutrino (already hypothesised with the name "neutretto")
1962 – Murray Gell-Mann and Yuval Ne'eman independently classify the hadrons according to a system that Gell-Mann called the Eightfold Way, and which ultimately led to the quark model (1964) of hadron composition.
1962 – Jeffrey Goldstone, Yoichiro Nambu, Abdus Salam, and Steven Weinberg develop what is now known as Goldstone's Theorem: if there is a continuous symmetry transformation under which the Lagrangian is invariant, then either the vacuum state is also invariant under the transformation, or there must be spinless particles of zero mass, thereafter called Nambu-Goldstone bosons.
1962 to 1973 – Brian David Josephson, predicts correctly the quantum tunneling effect involving superconducting currents while he is a PhD student under the supervision of Professor Brian Pippard at the Royal Society Mond Laboratory in Cambridge, UK; subsequently, in 1964, he applies his theory to coupled superconductors. The effect is later demonstrated experimentally at Bell Labs in the USA. For his important quantum discovery he is awarded the Nobel Prize in Physics in 1973.[40]
1963 – Eugene P. Wigner lays the foundation for the theory of symmetries in quantum mechanics as well as for basic research into the structure of the atomic nucleus; makes important "contributions to the theory of the atomic nucleus and the elementary particles, particularly through the discovery and application of fundamental symmetry principles"; he shares half of his Nobel prize in Physics with Maria Goeppert-Mayer and J. Hans D. Jensen.
1963 – Maria Goeppert Mayer and J. Hans D. Jensen share with Eugene P. Wigner half of the Nobel Prize in Physics in 1963 "for their discoveries concerning nuclear shell structure theory".[41]
1963 – Nicola Cabibbo develops the mathematical matrix by which the first two (and ultimately three) generations of quarks can be predicted.
1964 – Murray Gell-Mann and George Zweig independently propose the quark model of hadrons, predicting the arbitrarily named up, down, and strange quarks. Gell-Mann is credited with coining the term quark, which he found in James Joyce's book Finnegans Wake.
1964 – François Englert, Robert Brout, Peter Higgs, Gerald Guralnik, C. R. Hagen, and Tom Kibble postulate that a fundamental quantum field, now called the Higgs field, permeates space and, by way of the Higgs mechanism, provides mass to all the elementary subatomic particles that interact with it. While the Higgs field is postulated to confer mass on quarks and leptons, it represents only a tiny portion of the masses of other subatomic particles, such as protons and neutrons. In these, gluons that bind quarks together confer most of the particle mass. The result is obtained independently by three groups: François Englert and Robert Brout; Peter Higgs, working from the ideas of Philip Anderson; and Gerald Guralnik, C. R. Hagen, and Tom Kibble.[42][43][44][45][46][47][48]
1964 – Sheldon Lee Glashow and James Bjorken predict the existence of the charm quark. The addition is proposed because it allows for a better description of the weak interaction (the mechanism that allows quarks and other particles to decay), equalizes the number of known quarks with the number of known leptons, and implies a mass formula that correctly reproduced the masses of the known mesons.
1964 – John Stewart Bell puts forth Bell's theorem, which used testable inequality relations to show the flaws in the earlier Einstein–Podolsky–Rosen paradox and prove that no physical theory of local hidden variables can ever reproduce all of the predictions of quantum mechanics. This inaugurated the study of quantum entanglement, the phenomenon in which separate particles share the same quantum state despite being at a distance from each other.
1964 – Nikolai G. Basov and Aleksandr M. Prokhorov share the Nobel Prize in Physics in 1964 for, respectively, semiconductor lasers and Quantum Electronics; they also share the prize with Charles Hard Townes, the inventor of the ammonium maser.
1967 – Steven Weinberg and Abdus Salam publish a paper in which he describes Yang–Mills theory using the SU(2) X U(1) supersymmetry group, thereby yielding a mass for the W particle of the weak interaction via spontaneous symmetry breaking.
1968 – Stanford University: Deep inelastic scattering experiments at the Stanford Linear Accelerator Center (SLAC) show that the proton contains much smaller, point-like objects and is therefore not an elementary particle. Physicists at the time are reluctant to identify these objects with quarks, instead calling them partons — a term coined by Richard Feynman. The objects that are observed at SLAC will later be identified as up and down quarks. Nevertheless, "parton" remains in use as a collective term for the constituents of hadrons (quarks, antiquarks, and gluons). The existence of the strange quark is indirectly validated by the SLAC's scattering experiments: not only is it a necessary component of Gell-Mann and Zweig's three-quark model, but it provides an explanation for the kaon (K) and pion (π) hadrons discovered in cosmic rays in 1947.
1969 to 1977 – Sir Nevill Mott and Philip Warren Anderson publish quantum theories for electrons in non-crystalline solids, such as glasses and amorphous semiconductors; receive in 1977 a Nobel prize in Physics for their investigations into the electronic structure of magnetic and disordered systems, which allow for the development of electronic switching and memory devices in computers. The prize is shared with John Hasbrouck Van Vleck for his contributions to the understanding of the behavior of electrons in magnetic solids; he established the fundamentals of the quantum mechanical theory of magnetism and the crystal field theory (chemical bonding in metal complexes) and is regarded as the Father of modern Magnetism.
1969 and 1970 – Theodor V. Ionescu, Radu Pârvan and I.C. Baianu observe and report quantum amplified stimulation of electromagnetic radiation in hot deuterium plasmas in a longitudinal magnetic field; publish a quantum theory of the amplified coherent emission of radiowaves and microwaves by focused electron beams coupled to ions in hot plasmas.
1970 – Glashow, John Iliopoulos and Luciano Maiani predict the charmed quark that is subsequently found experimentally and share a Nobel prize for their theoretical prediction.
1971–1979
A 1974 photograph of an event in a bubble chamber at Brookhaven National Laboratory. Each track is left by a charged particle, one of which is a baryon containing the charm quark.[49]
1971 – Martinus J. G. Veltman and Gerardus 't Hooft show that, if the symmetries of Yang–Mills theory are broken according to the method suggested by Peter Higgs, then Yang–Mills theory can be renormalized. The renormalization of Yang–Mills Theory predicts the existence of a massless particle, called the gluon, which could explain the nuclear strong force. It also explains how the particles of the weak interaction, the W and Z bosons, obtain their mass via spontaneous symmetry breaking and the Yukawa interaction.
1972 – Francis Perrin discovers "natural nuclear fission reactors" in uranium deposits in Oklo, Gabon, where analysis of isotope ratios demonstrate that self-sustaining, nuclear chain reactions have occurred. The conditions under which a natural nuclear reactor could exist were predicted in 1956 by P. Kuroda.
1973 – Frank Anthony Wilczek discover the quark asymptotic freedom in the theory of strong interactions; receives the Lorentz Medal in 2002, and the Nobel Prize in Physics in 2004 for his discovery and his subsequent contributions to quantum chromodynamics.[50]
1973 – Makoto Kobayashi and Toshihide Maskawa note that the experimental observation of CP violation can be explained if an additional pair of quarks exist. The two new quarks are eventually named top and bottom.
1973 – Peter Mansfield formulates the physical theory of Nuclear magnetic resonance imaging (NMRI)[51][52][53][54]
1974 – Pier Giorgio Merli performs Young's double-slit experiment (1909) using a single electron with similar results, confirming the existence of quantum fields for massive particles.
1974 – Burton Richter and Samuel Ting: Charm quarks are produced almost simultaneously by two teams in November 1974 (see November Revolution) — one at SLAC under Burton Richter, and one at Brookhaven National Laboratory under Samuel Ting. The charm quarks are observed bound with charm antiquarks in mesons. The two discovering parties independently assign the discovered meson two different symbols, J and ψ; thus, it becomes formally known as the J/ψ meson. The discovery finally convinces the physics community of the quark model's validity.
1975 – Martin Lewis Perl, with his colleagues at the SLAC–LBL group, detects the tau in a series of experiments between 1974 and 1977.
1977 – Leon Lederman observes the bottom quark with his team at Fermilab. This discovery is a strong indicator of the top quark's existence: without the top quark, the bottom quark would be without a partner that is required by the mathematics of the theory.
1977 – Ilya Prigogine develops non-equilibrium, irreversible thermodynamics and quantum operator theory, especially the time superoperator theory; he is awarded the Nobel Prize in Chemistry in 1977 "for his contributions to non-equilibrium thermodynamics, particularly the theory of dissipative structures".[55]
1978 – Pyotr Kapitsa observes new phenomena in hot deuterium plasmas excited by very high power microwaves in attempts to obtain controlled thermonuclear fusion reactions in such plasmas placed in longitudinal magnetic fields, using a novel and low-cost design of thermonuclear reactor, similar in concept to that reported by Theodor V. Ionescu et al. in 1969. Receives a Nobel prize for early low temperature physics experiments on helium superfluidity carried out in 1937 at the Cavendish Laboratory in Cambridge, UK, and discusses his 1977 thermonuclear reactor results in his Nobel lecture on December 8, 1978.
1979 – Kenneth A. Rubinson and coworkers, at the Cavendish Laboratory, observe ferromagnetic spin wave resonant excite journals (FSWR) in locally anisotropic, FENiPB metallic glasses and interpret the observations in terms of two-magnon dispersion and a spin exchange Hamiltonian, similar in form to that of a Heisenberg ferromagnet.[56]
1980–1999
1980 to 1982 – Alain Aspect verify experimentally the quantum entanglement hypothesis; his Bell test experiments provide strong evidence that a quantum event at one location can affect an event at another location without any obvious mechanism for communication between the two locations.[57][58]
1982 to 1997 – Tokamak Fusion Test Reactor (TFTR) at PPPL, Princeton, USA: Operated since 1982, produces 10.7MW of controlled fusion power for only 0.21s in 1994 by using T-D nuclear fusion in a tokamak reactor with "a toroidal 6T magnetic field for plasma confinement, a 3MA plasma current and an electron density of 1.0×1020 m−3 of 13.5 keV" [59]
1983 – Carlo Rubbia and Simon van der Meer, at the Super Proton Synchrotron, see unambiguous signals of W particles in January. The actual experiments are called UA1 (led by Rubbia) and UA2 (led by Peter Jenni), and are the collaborative effort of many people. Simon van der Meer is the driving force on the use of the accelerator. UA1 and UA2 find the Z particle a few months later, in May 1983.
1983 to 2011 – The largest and most powerful experimental nuclear fusion tokamak reactor in the world, Joint European Torus (JET) begins operation at Culham Facility in UK; operates with T-D plasma pulses and has a reported gain factor Q of 0.7 in 2009, with an input of 40MW for plasma heating, and a 2800-ton iron magnet for confinement;[60] in 1997 in a tritium-deuterium experiment JET produces 16 MW of fusion power, a total of 22 MJ of fusion, energy and a steady fusion power of 4 MW which is maintained for 4 seconds.[61]
1985 to 2010 – The JT-60 (Japan Torus) begins operation in 1985 with an experimental D-D nuclear fusion tokamak similar to the JET; in 2010 JT-60 holds the record for the highest value of the fusion triple product achieved: 1.77×1028 K·s·m−3 = 1.53×1021 keV·s·m−3.;[62] JT-60 claims it would have an equivalent energy gain factor, Q of 1.25 if it were operated with a T-D plasma instead of the D-D plasma, and on May 9, 2006 attains a fusion hold time of 28.6 s in full operation; moreover, a high-power microwave gyrotron construction is completed that is capable of 1.5MW output for 1s,[63] thus meeting the conditions for the planned ITER, large-scale nuclear fusion reactor. JT-60 is disassembled in 2010 to be upgraded to a more powerful nuclear fusion reactor—the JT-60SA—by using niobium-titanium superconducting coils for the magnet confining the ultra-hot D-D plasma.
1986 – Johannes Georg Bednorz and Karl Alexander Müller produce unambiguous experimental proof of high temperature superconductivity involving Jahn-Teller polarons in orthorhombic La2CuO4, YBCO and other perovskite-type oxides; promptly receive a Nobel prize in 1987 and deliver their Nobel lecture on December 8, 1987.[64]
1986 – Vladimir Gershonovich Drinfeld introduces the concept of quantum groups as Hopf algebras in his seminal address on quantum theory at the International Congress of Mathematicians, and also connects them to the study of the Yang–Baxter equation, which is a necessary condition for the solvability of statistical mechanics models; he also generalizes Hopf algebras to quasi-Hopf algebras, and introduces the study of Drinfeld twists, which can be used to factorize the R-matrix corresponding to the solution of the Yang–Baxter equation associated with a quasitriangular Hopf algebra.
1988 to 1998 – Mihai Gavrilă discovers in 1988 the new quantum phenomenon of atomic dichotomy in hydrogen and subsequently publishes a book on the atomic structure and decay in high-frequency fields of hydrogen atoms placed in ultra-intense laser fields.[65][66][67][68][69][70][71]
1991 – Richard R. Ernst develops two-dimensional nuclear magnetic resonance spectroscopy (2D-FT NMRS) for small molecules in solution and is awarded the Nobel Prize in Chemistry in 1991 "for his contributions to the development of the methodology of high resolution nuclear magnetic resonance (NMR) spectroscopy."[72]
1977 to 1995 – The top quark is finally observed by a team at Fermilab after an 18-year search. It has a mass much greater than had been previously expected — almost as great as a gold atom.
1995 – Eric Cornell, Carl Wieman and Wolfgang Ketterle and co-workers at JILA create the first "pure" Bose–Einstein condensate. They do this by cooling a dilute vapor consisting of approximately two thousand rubidium-87 atoms to below 170 nK using a combination of laser cooling and magnetic evaporative cooling. About four months later, an independent effort led by Wolfgang Ketterle at MIT creates a condensate made of sodium-23. Ketterle's condensate has about a hundred times more atoms, allowing him to obtain several important results such as the observation of quantum mechanical interference between two different condensates.
1998 – The Super-Kamiokande (Japan) detector facility reports experimental evidence for neutrino oscillations, implying that at least one neutrino has mass.
1999 to 2013 – NSTX—The National Spherical Torus Experiment at PPPL, Princeton, USA launches a nuclear fusion project on February 12, 1999 for "an innovative magnetic fusion device that was constructed by the Princeton Plasma Physics Laboratory (PPPL) in collaboration with the Oak Ridge National Laboratory, Columbia University, and the University of Washington at Seattle"; NSTX is being used to study the physics principles of spherically shaped plasmas.[73]
21st century
Graphene is a planar atomic-scale honeycomb lattice made of carbon atoms which exhibits unusual and interesting quantum properties.
2000 – scientists at European Organization for Nuclear Research (CERN) publish experimental results in which they claim to have observed indirect evidence of the existence of a quark–gluon plasma, which they call a "new state of matter."
2001 – the Sudbury Neutrino Observatory (Canada) confirm the existence of neutrino oscillations. Lene Hau stops a beam of light completely in a Bose–Einstein condensate.[74]
2002 – Leonid Vainerman organizes a meeting at Strasbourg of theoretical physicists and mathematicians focused on quantum group and quantum groupoid applications in quantum theories; the proceedings of the meeting are published in 2003 in a book edited by the meeting organizer.[75]
2003 – Sir Anthony James Leggett receives the 2003 Nobel Prize in Physics for pioneering contributions to the quantum theory of superconductors, and superfluids such as Helium-3, shared with V. L. Ginzburg and A. A. Abrikosov.
2005 – the RHIC accelerator of Brookhaven National Laboratory generates a quark-gluon fluid, perhaps the quark–gluon plasma
2007 to 2010 – Charles Pence Slichter is awarded the National Medal of Science in 2007 for his studies of Nuclear Magnetic Resonance in Solids, and especially his NMR Studies of High-Temperature Superconductors.
2008 to 2010 – the Lithium Tokamak Experiment (LTX) starts in September 2008.[76]
2007 to 2010 – Alain Aspect, Anton Zeilinger and John Clauser present progress with the resolution of the non-locality aspect of quantum theory and in 2010 are awarded the Wolf Prize in Physics, together with Anton Zeilinger and John Clauser.[77]
2009 - Aaron D. O'Connell invents the first quantum machine, applying quantum mechanics to a macroscopic object just large enough to be seen by the naked eye, which is able to vibrate a small amount and large amount simultaneously.
2010 – Andre Geim and Konstantin Novoselov receive the Nobel Prize in Physics "for groundbreaking experiments regarding the two-dimensional material graphene".
2011 - Zachary Dutton demonstrates how photons can co-exist in superconductors. "Direct Observation of Coherent Population Trapping in a Superconducting Artificial Atom",[78]
2014 – Scientists transfer data by quantum teleportation over a distance of 10 feet with zero percent error rate, a vital step towards a quantum internet.[79][80]
See also
History of quantum mechanics
Timeline of atomic and subatomic physics
Timeline of particle physics
Timeline of physical chemistry
Learning materials related to the history of Quantum Mechanics at Wikiversity
References
Peacock 2008, pp. 175–183
Ben-Menahem 2009
Becquerel, Henri (1896). "Sur les radiations émises par phosphorescence". Comptes Rendus 122: 420–421.
Marie Curie and the Science of Radioactivity: Research Breakthroughs (1897–1904). Aip.org. Retrieved on 2012-05-17.
Frederick Soddy (December 12, 1922). "The origins of the conceptions of isotopes" (PDF). Nobel Lecture in Chemistry. Retrieved April 2012.
Ernest Rutherford, Baron Rutherford of Nelson, of Cambridge. Encyclopædia Britannica on-line. Retrieved on 2012-05-17.
The Nobel Prize in Chemistry 1908: Ernest Rutherford. nobelprize.org
McCormmach, Russell (Spring 1967). "Henri Poincaré and the Quantum Theory". Isis 58 (1): 37–55. doi:10.1086/350182.
Irons, F. E. (August 2001). "Poincaré's 1911–12 proof of quantum discontinuity interpreted as applying to atoms". American Journal of Physics 69 (8): 879–884. Bibcode:2001AmJPh..69..879I. doi:10.1119/1.1356056.
Ştefan Procopiu. 1913. "Determining the Molecular Magnetic Moment by M. Planck's Quantum Theory". Bulletin scientifique de l'Académie Roumaine de sciences., 1:151.
Pais, Abraham (1995). "Introducing Atoms and Their Nuclei". In Brown, Laurie M.; Pais, Abraham; Pippard, Brian. Twentieth Century Physics 1. American Institute of Physics Press. p. 89. ISBN 9780750303101. "Now the beauty of Franck and Hertz's work lies not only in the measurement of the energy loss E2-E1 of the impinging electron, but they also observed that, when the energy of that electron exceeds 4.9 eV, mercury begins to emit ultraviolet light of a definite frequency ν as defined in the above formula. Thereby they gave (unwittingly at first) the first direct experimental proof of the Bohr relation!"
P. S. Epstein, Zur Theorie des Starkeffektes, Annalen der Physik, vol. 50, pp. 489-520 (1916)
K. Schwarzschild, Sitzungsberichten der Kgl. Preuss. Akad. d. Wiss. April 1916, p. 548
Lewis, G.N. (1926). "The conservation of photons". Nature 118 (2981): 874–875. Bibcode:1926Natur.118..874L. doi:10.1038/118874a0.
P. S. Epstein, The Stark Effect from the Point of View of Schroedinger's Quantum Theory, Physical Review, vol 28, pp. 695-710 (1926)
John von Neumann. 1932. The Mathematical Foundations of Quantum Mechanics., Princeton University Press: Princeton, New Jersey, reprinted in 1955, 1971 and 1983 editions
Peter, F.; Weyl, H. (1927). "Die Vollständigkeit der primitiven Darstellungen einer geschlossenen kontinuierlichen Gruppe". Math. Ann. 97: 737–755. doi:10.1007/BF01447892.
Brauer, Richard; Weyl, Hermann (1935). "Spinors in n dimensions". American Journal of Mathematics (The Johns Hopkins University Press) 57 (2): 425–449. doi:10.2307/2371218. JSTOR 2371218.
Frédéric Joliot-Curie (December 12, 1935). "Chemical evidence of the transmutation of elements" (PDF). Nobel Lecture. Retrieved April 2012.
Einstein A, Podolsky B, Rosen N; Podolsky; Rosen (1935). "Can Quantum-Mechanical Description of Physical Reality Be Considered Complete?". Phys. Rev. 47 (10): 777–780. Bibcode:1935PhRv...47..777E. doi:10.1103/PhysRev.47.777.
Birkhoff, Garrett and von Neumann, J. (1936). "The Logic of Quantum Mechanics". Annals of Mathematics 37 (4): 823–843. doi:10.2307/1968621. JSTOR 1968621.
Roland Omnès (8 March 1999). Understanding Quantum Mechanics. Princeton University Press. ISBN 978-0-691-00435-8. Retrieved 17 May 2012.
Dalla Chiara, M. L.; Giuntini, R. (1994). "Unsharp quantum logics". Foundations of Physics 24 (8): 1161–1177. Bibcode:1994FoPh...24.1161D. doi:10.1007/BF02057862.
Georgescu, G. (2006). "N-valued Logics and Łukasiewicz-Moisil Algebras". Axiomathes 16 (1–2): 123. doi:10.1007/s10516-005-4145-6.
H. Jahn and E. Teller (1937). "Stability of Polyatomic Molecules in Degenerate Electronic States. I. Orbital Degeneracy". Proceedings of the Royal Society A 161 (905): 220–235. Bibcode:1937RSPSA.161..220J. doi:10.1098/rspa.1937.0142.
Dyson, F. (1949). "The S Matrix in Quantum Electrodynamics". Phys. Rev. 75 (11): 1736. Bibcode:1949PhRv...75.1736D. doi:10.1103/PhysRev.75.1736.
Stix, Gary (October 1999). "Infamy and honor at the Atomic Café: Edward Teller has no regrets about his contentious career". Scientific American: 42–43. Retrieved April 2012.
Hans A. Bethe (May 28, 1952). MEMORANDUM ON THE HISTORY OF THERMONUCLEAR PROGRAM (Report). Reconstructed version from only partially declassified documents, with certain words deliberately deleted.
Bloch, F.; Hansen, W.; Packard, Martin (1946). "Nuclear Induction". Physical Review 69 (3–4): 127. Bibcode:1946PhRv...69..127B. doi:10.1103/PhysRev.69.127.
Bloch, F.; Jeffries, C. (1950). "A Direct Determination of the Magnetic Moment of the Proton in Nuclear Magnetons". Physical Review 80 (2): 305. Bibcode:1950PhRv...80..305B. doi:10.1103/PhysRev.80.305.
Bloch, F. (1946). "Nuclear Induction". Physical Review 70 (7–8): 460. Bibcode:1946PhRv...70..460B. doi:10.1103/PhysRev.70.460.
Gutowsky, H. S.; Kistiakowsky, G. B.; Pake, G. E.; Purcell, E. M. (1949). "Structural Investigations by Means of Nuclear Magnetism. I. Rigid Crystal Lattices". The Journal of Chemical Physics 17 (10): 972. Bibcode:1949JChPh..17..972G. doi:10.1063/1.1747097.
Gardner, J.; Purcell, E. (1949). "A Precise Determination of the Proton Magnetic Moment in Bohr Magnetons". Physical Review 76 (8): 1262. Bibcode:1949PhRv...76.1262G. doi:10.1103/PhysRev.76.1262.2.
Carver, T. R.; Slichter, C. P. (1953). "Polarization of Nuclear Spins in Metals". Physical Review 92 (1): 212–213. Bibcode:1953PhRv...92..212C. doi:10.1103/PhysRev.92.212.2.
Hugh Everett Theory of the Universal Wavefunction, Thesis, Princeton University, (1956, 1973), pp 1–140
Everett, Hugh (1957). "Relative State Formulation of Quantum Mechanics". Reviews of Modern Physics 29 (3): 454–462. Bibcode:1957RvMP...29..454E. doi:10.1103/RevModPhys.29.454.
Jacek W. Hennel, Jacek Klinowski (2005). Jacek Klinowski, ed. "New techniques in solid-state NMR". Topics in Current Chemistry 246. Springer. pp. 1–14. doi:10.1007/b98646. ISBN 3-540-22168-9. |chapter= ignored (help) (New techniques in solid-state NMR, p. 1, at Google Books)
V.E. Barnes; Connolly, P.; Crennell, D.; Culwick, B.; Delaney, W.; Fowler, W.; Hagerty, P.; Hart, E.; Horwitz, N.; Hough, P.; Jensen, J.; Kopp, J.; Lai, K.; Leitner, J.; Lloyd, J.; London, G.; Morris, T.; Oren, Y.; Palmer, R.; Prodell, A.; Radojičić, D.; Rahm, D.; Richardson, C.; Samios, N.; Sanford, J.; Shutt, R.; Smith, J.; Stonehill, D.; Strand, R.; et al. (1964). "Observation of a Hyperon with Strangeness Number Three" (PDF). Physical Review Letters 12 (8): 204. Bibcode:1964PhRvL..12..204B. doi:10.1103/PhysRevLett.12.204.
Anatole Abragam (1961). The Principles of Nuclear Magnetism. Oxford: Clarendon Press. OCLC 242700.
Brian David Josephson (December 12, 1973). "The Discovery of Tunnelling Supercurrents" (PDF). Nobel Lecture. Retrieved April 2012.
Maria Goeppert Mayer (December 12, 1963). "The shell model" (PDF). Nobel Lecture. Retrieved April 2012.
F. Englert, R. Brout; Brout (1964). "Broken Symmetry and the Mass of Gauge Vector Mesons". Physical Review Letters 13 (9): 321–323. Bibcode:1964PhRvL..13..321E. doi:10.1103/PhysRevLett.13.321.
P.W. Higgs (1964). "Broken Symmetries and the Masses of Gauge Bosons". Physical Review Letters 13 (16): 508–509. Bibcode:1964PhRvL..13..508H. doi:10.1103/PhysRevLett.13.508.
G.S. Guralnik, C.R. Hagen, T.W.B. Kibble; Hagen; Kibble (1964). "Global Conservation Laws and Massless Particles". Physical Review Letters 13 (20): 585–587. Bibcode:1964PhRvL..13..585G. doi:10.1103/PhysRevLett.13.585.
G.S. Guralnik (2009). "The History of the Guralnik, Hagen and Kibble development of the Theory of Spontaneous Symmetry Breaking and Gauge Particles". International Journal of Modern Physics A 24 (14): 2601–2627. arXiv:0907.3466. Bibcode:2009IJMPA..24.2601G. doi:10.1142/S0217751X09045431.
T.W.B. Kibble (2009). "Englert–Brout–Higgs–Guralnik–Hagen–Kibble mechanism". Scholarpedia 4 (1): 6441. Bibcode:2009SchpJ...4.6441K. doi:10.4249/scholarpedia.6441.
M. Blume, S. Brown, Y. Millev (2008). "Letters from the past, a PRL retrospective (1964)". Physical Review Letters. Retrieved 2010-01-30.
"J. J. Sakurai Prize Winners". American Physical Society. 2010. Retrieved 2010-01-30.
"Discovery of the Charmed Baryon". Brookhaven History. Brookhaven National Laboratory.
Wilczek, Frank (1999). "Quantum field theory". Reviews of Modern Physics 71 (2): S85. arXiv:hep-th/9803075. Bibcode:1999RvMPS..71...85W. doi:10.1103/RevModPhys.71.S85.
Mansfield, P; Grannell, P K (1973). "NMR 'diffraction' in solids?". Journal of Physics C: Solid State Physics 6 (22): L422. Bibcode:1973JPhC....6L.422M. doi:10.1088/0022-3719/6/22/007.
Garroway, A N; Grannell, P K; Mansfield, P (1974). "Image formation in NMR by a selective irradiative process". Journal of Physics C: Solid State Physics 7 (24): L457. Bibcode:1974JPhC....7L.457G. doi:10.1088/0022-3719/7/24/006.
Mansfield, P.; Maudsley, A. A. (1977). "Medical imaging by NMR". British Journal of Radiology 50 (591): 188–94. doi:10.1259/0007-1285-50-591-188. PMID 849520.
Mansfield, P (1977). "Multi-planar image formation using NMR spin echoes". Journal of Physics C: Solid State Physics 10 (3): L55. Bibcode:1977JPhC...10L..55M. doi:10.1088/0022-3719/10/3/004.
Ilya Prigogine (8 December 1977). "Time, Structure and Fluctuations" (PDF). Nobel lecture. Retrieved April 2012.
Rubinson, K.A.; Rubinson, Kenneth A.; Patterson, John (1979). "Ferromagnetic resonance and spin wave excite journals in metallic glasses". J. Phys. Chem. Solids 40 (12): 941–950. Bibcode:1979JPCS...40..941B. doi:10.1016/0022-3697(79)90122-7.
Aspect, Alain; Grangier, Philippe; Roger, Gérard (1982). "Experimental Realization of Einstein-Podolsky-Rosen-Bohm Gedankenexperiment: A New Violation of Bell's Inequalities". Physical Review Letters 49 (2): 91. Bibcode:1982PhRvL..49...91A. doi:10.1103/PhysRevLett.49.91.
Aspect, Alain; Dalibard, Jean; Roger, Gérard (1982). "Experimental Test of Bell's Inequalities Using Time- Varying Analyzers". Physical Review Letters 49 (25): 1804. Bibcode:1982PhRvL..49.1804A. doi:10.1103/PhysRevLett.49.1804.
TFTR Machine Parameters. W3.pppl.gov (1996-05-10). Retrieved on 2012-05-17.
JET's Main Features-EFDA JET. Jet.efda.org. Retrieved on 2012-05-17.
European JET website. (PDF) . Retrieved on 2012-05-17.
Japan Atomic Energy Agency. Naka Fusion Institute
Fusion Plasma Research (FPR), JASEA, Naka Fusion Institute. Jt60.naka.jaea.go.jp. Retrieved on 2012-05-17.
Müller, KA; Bednorz, JG (1987). "The discovery of a class of high-temperature superconductors". Science 237 (4819): 1133–9. Bibcode:1987Sci...237.1133M. doi:10.1126/science.237.4819.1133. PMID 17801637.
Pont, M.; Walet, N.R.; Gavrila, M.; McCurdy, C.W. (1988). "Dichotomy of the Hydrogen Atom in Superintense, High-Frequency Laser Fields". Physical Review Letters 61 (8): 939–942. Bibcode:1988PhRvL..61..939P. doi:10.1103/PhysRevLett.61.939. PMID 10039473.
Pont, M.; Walet, N.; Gavrila, M. (1990). "Radiative distortion of the hydrogen atom in superintense, high-frequency fields of linear polarization". Physical Review A 41 (1): 477–494. Bibcode:1990PhRvA..41..477P. doi:10.1103/PhysRevA.41.477. PMID 9902891.
Mihai Gavrila: Atomic Structure and Decay in High-Frequency Fields, in Atoms in Intense Laser Fields, ed. M. Gavrila, Academic Press, San Diego, 1992, pp. 435–510. ISBN 0-12-003901-X
Muller, H.; Gavrila, M. (1993). "Light-Induced Excited States in H−". Physical Review Letters 71 (11): 1693–1696. Bibcode:1993PhRvL..71.1693M. doi:10.1103/PhysRevLett.71.1693. PMID 10054474.
Wells, J.C.; Simbotin, I.; Gavrila, M. (1998). "Physical Reality of Light-Induced Atomic States". Physical Review Letters 80 (16): 3479–3482. Bibcode:1998PhRvL..80.3479W. doi:10.1103/PhysRevLett.80.3479.
Ernst, E; van Duijn, M. Gavrila; Muller, H.G. (1996). "Multiply Charged Negative Ions of Hydrogen Induced by Superintense Laser Fields". Physical Review Letters 77 (18): 3759–3762. Bibcode:1996PhRvL..77.3759V. doi:10.1103/PhysRevLett.77.3759. PMID 10062301.
Shertzer, J.; Chandler, A.; Gavrila, M. (1994). "H2+ in Superintense Laser Fields: Alignment and Spectral Restructuring". Physical Review Letters 73 (15): 2039–2042. Bibcode:1994PhRvL..73.2039S. doi:10.1103/PhysRevLett.73.2039. PMID 10056956.
Richard R. Ernst (December 9, 1992). "Nuclear Magnetic Resonance Fourier Transform (2D-FT) Spectroscopy" (PDF). Nobel Lecture. Retrieved April 2012.
PPPL, Princeton, USA. Pppl.gov (1999-02-12). Retrieved on 2012-05-17.
"Lene Hau". Physicscentral.com. Retrieved 2013-01-30.
Leonid Vainerman (2003). Locally Compact Quantum Groups and Groupoids: Proceedings of the Meeting of Theoretical Physicists and Mathematicians, Strasbourg, February 21–23, 2002. Walter de Gruyter. pp. 247–. ISBN 978-3-11-020005-8. Retrieved 17 May 2012.
LTX EXperiment Achieves First Plasma (at PPPL). Pppl.gov. Retrieved on 2012-05-17.
Aspect, A. (2007). "To be or not to be local". Nature 446 (7138): 866–867. Bibcode:2007Natur.446..866A. doi:10.1038/446866a. PMID 17443174.
"Coherent Population". Defense Procurement News. 2010-06-22. Retrieved 2013-01-30.
Markoff, John (29 May 2014). "Scientists Report Finding Reliable Way to Teleport Data". New York Times. Retrieved 29 May 2014.
Pfaff, W.; et al. (29 May 2014). "Unconditional quantum teleportation between distant solid-state quantum bits". Science (journal). arXiv:1404.4369. Bibcode:2014Sci...345..532P. doi:10.1126/science.1253512. Retrieved 29 May 2014.
Bibliography
Peacock, Kent A. (2008). "The quantum revolution : a historical perspective". Westport, Conn.: Greenwood Press. ISBN 9780313334481.
Ben-Menahem, A. (2009). "Historical encyclopedia of natural and mathematical sciences" (1st ed.). Berlin: Springer. pp. 4342–4349. ISBN 9783540688310. |chapter= ignored (help)
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