This article possibly contains original research .(April 2012) |

The **timeline of quantum mechanics** is a list of key events in the history of quantum mechanics, quantum field theories and quantum chemistry.

- 1801 – Thomas Young establishes that light made up of waves with his Double-slit experiment.
- 1859 – Gustav 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.
- 1885 – Johann Jakob Balmer discovers a numerical relationship between visible spectral lines of hydrogen, the Balmer series.
- 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] }^{ [2] } - 1896-1897 – Pieter Zeeman first observes the Zeeman splitting effect by applying a magnetic field to light sources.
^{ [3] } - 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.
- 1897 – J. J. Thomson's experimentation with cathode rays led him to suggest a fundamental unit more than a 1,000 times smaller than an atom, based on the high charge-to-mass ratio. He called the particle a "corpuscle", but later scientists preferred the term electron.
- 1897- Joseph Larmor explained the splitting of the spectral lines in a magnetic field by the oscillation of electrons.
^{ [5] }^{ [6] } - 1897 - Physicist, Joseph Larmor, created the first solar system model of the atom in 1897. He also postulated the proton, calling it a “positive electron.” He said the destruction of this type of atom making up matter “is an occurrence of infinitely small probability.”
^{ [7] } - 1899 to 1903 – Ernest Rutherford investigates 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. 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}_{2}He^{}); they report their interpretation of radioactivity in 1903.^{ [8] }Rutherford becomes known as the "father of nuclear physics" with his nuclear atom model of 1911.^{ [9] }

- 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
*H*, and the maximum negative valence, such as −2 for_{2}SO_{4}*H*, of an element tends to be eight (Abegg's rule)._{2}S - 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",^{ [10] }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.

- 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,
*μ*_{B}= 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). - 1911 - John William Nicholson is noted as the first to create an atomic model that quantized angular momentum as h/2pi.
^{ [11] }^{ [12] }Niels Bohr quoted him in his 1913 paper of the Bohr model of the atom.^{ [13] } - 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.
^{ [14] }^{ [15] } - 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 - Niels Bohr publishes his 1913 paper of the Bohr model of the atom.
^{ [16] } - 1913 – Ștefan Procopiu publishes a theoretical paper with the correct value of the electron's magnetic dipole moment
*μ*_{B}.^{ [17] } - 1913 – Niels Bohr obtains theoretically the value of the electron's magnetic dipole moment
*μ*_{B}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.
^{ [18] } - 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
^{ [19] }and Karl Schwarzschild,^{ [20] }working independently, derive equations for the linear and quadratic Stark effect in hydrogen. - 1916 – Gilbert N. Lewis conceives the theoretical basis of Lewis dot formulas, diagrams that show the bonding between atoms of a molecule and the lone pairs of electrons that may exist in the molecule.
^{ [21] } - 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 - Hendrik Kramers uses Bohr–Sommerfeld quantization to derive formulas for intensities of spectral transitions of the Stark effect. Kramers also includes the effect of fine structure, including corrections for relativistic kinetic energy and coupling between electron spin and orbit.
^{ [22] } - 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 develop 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).^{ [23] } - 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.
^{ [24] } - 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] }^{ [25] }^{ [26] } - 1927 – Werner Heisenberg formulates the quantum uncertainty principle.
^{ [1] } - 1927 – Niels Bohr and Werner Heisenberg 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 Galton 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);
^{ [27] }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.^{ [28] } - 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 – Dirac hypothesizes the existence of the positron.
^{ [1] } - 1930 – Dirac's textbook
*The 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 was 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
^{ [29] } - 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.
^{ [30] } - 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 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
^{ [31] }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;^{ [32] }current approaches to quantum logic involve noncommutative and non-associative many-valued logic.^{ [33] }^{ [34] } - 1936 – Carl D. Anderson discovers muons while he is studying cosmic radiation.
- 1937 – Hermann Arthur Jahn and Edward Teller prove, using group theory, that non-linear degenerate molecules are unstable.
^{ [35] }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 communicates 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.

- 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
^{2}*S*_{1/2}and^{2}*P*_{1/2}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.
^{ [36] }

- 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.
^{ [37] } - 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.
^{ [38] }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.
^{ [39] }^{ [40] }^{ [41] }Purcell reports his contribution as*Research in Nuclear Magnetism*, and gives credit to his coworkers such as Herbert S. Gutowsky for their NMR contributions,^{ [42] }^{ [43] }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.^{ [44] } - 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 Herbert 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.
- 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 they 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.
^{ [45] }^{ [46] } - 1958–1959 – magic angle spinning described by Edward Raymond Andrew, A. Bradbury, and R. G. Eades, and independently in 1959 by I. J. Lowe.
^{ [47] }

- 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*;^{ [49] } - 1961 – Sheldon Glashow extends the electroweak interaction models 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 – 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.
^{ [50] } - 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".
^{ [51] } - 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.
- 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.

- 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 – Peter Mansfield formulates the physical theory of Nuclear magnetic resonance imaging (NMRI)
^{ [52] }^{ [53] }^{ [54] }^{ [55] } - 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.
- 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".
^{ [56] } - 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.
^{ [57] }

- 1980 to 1982 – Alain Aspect verifies 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.
^{ [58] }^{ [59] }This remarkable result confirmed the experimental verification of quantum entanglement by J.F.Clauser. and. S.J.Freedman in 1972.^{ [60] } - 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 1.0×10
^{20}m^{−3}of 13.5 keV"^{ [61] } - 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;^{ [62] }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.^{ [63] } - 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: 1.77×10
^{28}K·s·m^{−3}= 1.53×10^{21}keV·s·m^{−3}.;^{ [64] }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*,^{ [65] }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 La
_{2}CuO_{4}, YBCO and other perovskite-type oxides; promptly receive a Nobel prize in 1987 and deliver their Nobel lecture on December 8, 1987.^{ [66] } - 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.^{ [67] }^{ [68] }^{ [69] }^{ [70] }^{ [71] }^{ [72] }^{ [73] } - 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."
^{ [74] } - 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.
- 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.
^{ [75] }

- 2002 – Leonid I. 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.
^{ [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.
^{ [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.
^{ [78] } - 2011 - Zachary Dutton demonstrates how photons can co-exist in superconductors. "Direct Observation of Coherent Population Trapping in a Superconducting Artificial Atom",
^{ [79] } - 2012 - The existence of Higgs boson was confirmed by the ATLAS and CMS collaborations based on proton-proton collisions in the large hadron collider at CERN. Peter Higgs and François Englert were awarded the 2013 Nobel Prize in Physics for their theoretical predictions.
^{ [80] } - 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.
^{ [81] }^{ [82] }

An **atom** is a particle that consists of a nucleus of protons and neutrons surrounded by an electromagnetically-bound cloud of electrons. The atom is the basic particle of the chemical elements, and the chemical elements are distinguished from each other by the number of protons that are in their atoms. For example, any atom that contains 11 protons is sodium, and any atom that contains 29 protons is copper. The number of neutrons defines the isotope of the element.

The **plum pudding model** is one of several historical scientific models of the atom. First proposed by J. J. Thomson in 1904 soon after the discovery of the electron, but before the discovery of the atomic nucleus, the model tried to explain two properties of atoms then known: that electrons are negatively charged particles and that atoms have no net electric charge. The plum pudding model has electrons surrounded by a volume of positive charge, like negatively charged "plums" embedded in a positively charged "pudding".

**Atomic theory** is the scientific theory that matter is composed of particles called atoms. The concept that matter is composed of discrete particles is an ancient idea, but gained scientific credence in the 18th and 19th centuries when scientists found it could explain the behaviors of gases and how chemical elements reacted with each other. By the end of the 19th century, atomic theory had gained widespread acceptance in the scientific community.

In atomic physics, the **Bohr model** or **Rutherford–Bohr model** of the atom, presented by Niels Bohr and Ernest Rutherford in 1913, consists of a small, dense nucleus surrounded by orbiting electrons. It is analogous to the structure of the Solar System, but with attraction provided by electrostatic force rather than gravity, and with the electron energies quantized.

The **electron** is a subatomic particle with a negative one elementary electric charge. Electrons belong to the first generation of the lepton particle family, and are generally thought to be elementary particles because they have no known components or substructure. The electron's mass is approximately 1/1836 that of the proton. Quantum mechanical properties of the electron include an intrinsic angular momentum (spin) of a half-integer value, expressed in units of the reduced Planck constant, ħ. Being fermions, no two electrons can occupy the same quantum state, per the Pauli exclusion principle. Like all elementary particles, electrons exhibit properties of both particles and waves: They can collide with other particles and can be diffracted like light. The wave properties of electrons are easier to observe with experiments than those of other particles like neutrons and protons because electrons have a lower mass and hence a longer de Broglie wavelength for a given energy.

The **neutron** is a subatomic particle, symbol ^{}n^{} or ^{}n^{0}_{}, which has a neutral charge, and a mass slightly greater than that of a proton. Protons and neutrons constitute the nuclei of atoms. Since protons and neutrons behave similarly within the nucleus, and each has a mass of approximately one dalton, they are both referred to as nucleons. Their properties and interactions are described by nuclear physics. Protons and neutrons are not elementary particles; each is composed of three quarks.

**Nuclear physics** is the field of physics that studies atomic nuclei and their constituents and interactions, in addition to the study of other forms of nuclear matter.

A **proton** is a stable subatomic particle, symbol ^{}p^{}, H^{+}, or ^{1}H^{+} with a positive electric charge of +1 *e* (elementary charge). Its mass is slightly less than that of a neutron and 1,836 times the mass of an electron (the proton-to-electron mass ratio). Protons and neutrons, each with masses of approximately one atomic mass unit, are jointly referred to as "nucleons" (particles present in atomic nuclei).

In quantum mechanics, the **Pauli exclusion principle** states that two or more identical particles with half-integer spins cannot occupy the same quantum state within a quantum system simultaneously. This principle was formulated by Austrian physicist Wolfgang Pauli in 1925 for electrons, and later extended to all fermions with his spin–statistics theorem of 1940.

**Quantum mechanics** is a fundamental theory in physics that provides a description of the physical properties of nature at the scale of atoms and subatomic particles. It is the foundation of all quantum physics including quantum chemistry, quantum field theory, quantum technology, and quantum information science.

**Atomic, molecular, and optical physics** (**AMO**) is the study of matter–matter and light–matter interactions, at the scale of one or a few atoms and energy scales around several electron volts. The three areas are closely interrelated. AMO theory includes classical, semi-classical and quantum treatments. Typically, the theory and applications of emission, absorption, scattering of electromagnetic radiation (light) from excited atoms and molecules, analysis of spectroscopy, generation of lasers and masers, and the optical properties of matter in general, fall into these categories.

A timeline of atomic and subatomic physics.

In physics, a **subatomic particle** is a particle smaller than an atom. According to the Standard Model of particle physics, a subatomic particle can be either a composite particle, which is composed of other particles, or an elementary particle, which is not composed of other particles. Particle physics and nuclear physics study these particles and how they interact.

In quantum physics, the **Stern–Gerlach experiment** demonstrated that the spatial orientation of angular momentum is quantized. Thus an atomic-scale system was shown to have intrinsically quantum properties. In the original experiment, silver atoms were sent through a spatially-varying magnetic field, which deflected them before they struck a detector screen, such as a glass slide. Particles with non-zero magnetic moment were deflected, owing to the magnetic field gradient, from a straight path. The screen revealed discrete points of accumulation, rather than a continuous distribution, owing to their quantized spin. Historically, this experiment was decisive in convincing physicists of the reality of angular-momentum quantization in all atomic-scale systems.

**Quantum mechanics** is the study of matter and its interactions with energy on the scale of atomic and subatomic particles. By contrast, classical physics explains matter and energy only on a scale familiar to human experience, including the behavior of astronomical bodies such as the moon. Classical physics is still used in much of modern science and technology. However, towards the end of the 19th century, scientists discovered phenomena in both the large (macro) and the small (micro) worlds that classical physics could not explain. The desire to resolve inconsistencies between observed phenomena and classical theory led to a revolution in physics, a shift in the original scientific paradigm: the development of quantum mechanics.

The history of quantum mechanics is a fundamental part of the history of modern physics. The major chapters of this history begin with the emergence of quantum ideas to explain individual phenomena -- blackbody radiation, the photoelectric effect, solar emission spectra -- an era called the Old or Older quantum theories. The invention of wave mechanics by Schrodinger and expanded by many others triggers the "modern" era beginning around 1925. Dirac's relativistic quantum theory work lead him to explore quantum theories of radiation, culminating in quantum electrodynamics, the first quantum field theory. The history of quantum mechanics continues in the history of quantum field theory. The history of quantum chemistry, theoretical basis of chemical structure, reactivity, and bonding, interlaces with the events discussed in this article.

The **dihydrogen cation** or **hydrogen molecular ion** is a cation with formula **H ^{+}_{2}**. It consists of two hydrogen nuclei (protons) sharing a single electron. It is the simplest molecular ion.

**Michał Gryziński** was a Polish nuclear physicist, plasma physics specialist and the founder of the free-fall atomic model, an alternative theoretical formulation, a classical approximation asking for trajectories of electron averaging to probability densities described by quantum mechanics.

In physics, the **hydrodynamic quantum analogs** refer to experimentally-observed phenomena involving bouncing fluid droplets over a vibrating fluid bath that behave analogously to several quantum-mechanical systems.

The **discovery of the neutron** and its properties was central to the extraordinary developments in atomic physics in the first half of the 20th century. Early in the century, Ernest Rutherford developed a crude model of the atom, based on the gold foil experiment of Hans Geiger and Ernest Marsden. In this model, atoms had their mass and positive electric charge concentrated in a very small nucleus. By 1920, isotopes of chemical elements had been discovered, the atomic masses had been determined to be (approximately) integer multiples of the mass of the hydrogen atom, and the atomic number had been identified as the charge on the nucleus. Throughout the 1920s, the nucleus was viewed as composed of combinations of protons and electrons, the two elementary particles known at the time, but that model presented several experimental and theoretical contradictions.

- 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 Peacock 2008 , pp. 175–183
- ↑ Becquerel, Henri (1896). "Sur les radiations émises par phosphorescence".
*Comptes Rendus*.**122**: 420–421. - ↑ "Milestone 1 : Nature Milestones in Spin".
*www.nature.com*. Retrieved 2018-09-09. - ↑ Marie Curie and the Science of Radioactivity: Research Breakthroughs (1897–1904). Aip.org. Retrieved on 2012-05-17.
- ↑ Histories of the Electron: The Birth of Microphysics edited by Jed Z. Buchwald, Andrew Warwick
- ↑ Larmor, Joseph (1897),
*Philosophical Transactions of the Royal Society*,**190**: 205–300, Bibcode:1897RSPTA.190..205L, doi: 10.1098/rsta.1897.0020 , - ↑ Larmor, Joseph (1897),
*Philosophical Transactions of the Royal Society*,**190**: 205–300, Bibcode:1897RSPTA.190..205L, doi: 10.1098/rsta.1897.0020 Quotes from one of Larmor’s voluminous work include: “while atoms of matter are in whole or in part aggregations of electrons in stable orbital motion. In particular, this scheme provides a consistent foundation for the electrodynamic laws, and agrees with the actual relations between radiation and moving matter.”- “A formula for optical dispersion was obtained in § 11 of the second part of this memoir, on the simple hypothesis that the electric polarization of the molecules vibrated as a whole in unison with the electric field of the radiation.”
- “…that of the transmission of radiation across a medium permeated by molecules, each consisting of a system of electrons in steady orbital motion, and each capable of free oscillations about the steady state of motion with definite free periods analogous to those of the planetary inequalities of the Solar System;”
- “‘A’ will be a positive electron in the medium, and ‘B’ will be the complementary negative one…We shall thus have created two permanent conjugate electrons A and B ; each of them can be moved about through the medium, but they will both persist until they are destroyed by an extraneous process the reverse of that by which they are formed.”

- ↑ Soddy, Frederick (December 12, 1922). "The origins of the conceptions of isotopes" (PDF).
*Nobel Lecture in Chemistry*. Retrieved 25 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
- ↑ J. W. Nicholson, Month. Not. Roy. Astr. Soc. lxxii. pp. 49,130, 677, 693, 729 (1912).
- ↑ The Atomic Theory of John William Nicholson, Russell McCormmach, Archive for History of Exact Sciences, Vol. 3, No. 2 (25.8.1966), pp. 160-184 (25 pages), Springer.
- ↑ On the Constitution of Atoms and Molecules Niels Bohr, Philosophical Magazine, Series 6, Volume 26 July 1913, p. 1-25
- ↑ McCormmach, Russell (Spring 1967). "Henri Poincaré and the Quantum Theory".
*Isis*.**58**(1): 37–55. doi:10.1086/350182. S2CID 120934561. - ↑ 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. - ↑ On the Constitution of Atoms and Molecules, Niels Bohr, Philosophical Magazine, Series 6, Volume 26 July 1913, p. 1-25
- ↑ Procopiu, Ştefan (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 (eds.).
*Twentieth Century Physics*. Vol. 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

*E*_{2}-*E*_{1}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. (1916), "The Atom and the Molecule",
*J. Am. Chem. Soc.*,**38**(4): 762–85, doi:10.1021/ja02261a002, S2CID 95865413 - ↑ H. A. Kramers, Roy. Danish Academy,
*Intensities of Spectral Lines. On the Application of the Quantum Theory to the Problem of Relative Intensities of the Components of the Fine Structure and of the Stark Effect of the Lines of the Hydrogen Spectrum*, p. 287 (1919);*Über den Einfluß eines elektrischen Feldes auf die Feinstruktur der Wasserstofflinien*(On the influence of an electric field on the fine structure of hydrogen lines), Zeitschrift für Physik, vol.**3**, pp. 199–223 (1920) - ↑ Lewis, G.N. (1926). "The conservation of photons".
*Nature*.**118**(2981): 874–875. Bibcode:1926Natur.118..874L. doi:10.1038/118874a0. S2CID 4110026. - ↑ 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 - ↑ Van Hove, Léon (1958). "Von Neumann's Contributions to Quantum Theory".
*Bulletin of the American Mathematical Society*.**64**(3): 95–100. doi: 10.1090/s0002-9904-1958-10206-2 . - ↑ Peter, F.; Weyl, H. (1927). "Die Vollständigkeit der primitiven Darstellungen einer geschlossenen kontinuierlichen Gruppe".
*Math. Ann*.**97**: 737–755. doi:10.1007/BF01447892. S2CID 120013521. - ↑ Brauer, Richard; Weyl, Hermann (1935). "Spinors in n dimensions".
*American Journal of Mathematics*.**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 25 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 .`{{cite journal}}`

: CS1 maint: multiple names: authors list (link) - ↑ Birkhoff, Garrett & von Neumann, J. (1936). "The Logic of Quantum Mechanics".
*Annals of Mathematics*.**37**(4): 823–843. doi:10.2307/1968621. JSTOR 1968621. - ↑ Omnès, Roland (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. S2CID 122872424. - ↑ Georgescu, G. (2006). "N-valued Logics and Łukasiewicz-Moisil Algebras".
*Axiomathes*.**16**(1–2): 123–136. doi:10.1007/s10516-005-4145-6. S2CID 121264473. - ↑ 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): 1736–1755. 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. Archived from the original on 2012-10-18. Retrieved 25 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): 305–306. Bibcode:1950PhRv...80..305B. doi:10.1103/PhysRev.80.305. - ↑ Bloch, F. (1946). "Nuclear Induction".
*Physical Review*.**70**(7–8): 460–474. 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): 1262–1263. 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. Archived from the original on 2011-10-27. - ↑ Jacek W. Hennel; Jacek Klinowski (2005). "Magic Angle Spinning: A Historical Perspective". In Jacek Klinowski (ed.).
*New techniques in solid-state NMR*. Topics in Current Chemistry. Vol. 246. Springer. pp. 1–14. doi:10.1007/b98646. ISBN 978-3-540-22168-5. PMID 22160286. (*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): 204–206. Bibcode:1964PhRvL..12..204B. doi:10.1103/PhysRevLett.12.204. OSTI 12491965. - ↑ Abragam, Anatole (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 25 April 2012. - ↑ Maria Goeppert Mayer (December 12, 1963). "The shell model" (PDF).
*Nobel Lecture*. Retrieved 25 April 2012. - ↑ 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. S2CID 4992859. - ↑ 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. S2CID 4981940. - ↑ 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. S2CID 26374556. - ↑ Mansfield, P (1977). "Multi-planar image formation
*using NMR*spin echoes".*Journal of Physics C: Solid State Physics*.**10**(3): L55–L58. Bibcode:1977JPhC...10L..55M. doi:10.1088/0022-3719/10/3/004. S2CID 121696469. - ↑ Prigogine, Ilya (8 December 1977). "Time, Structure and Fluctuations" (PDF).
*Science*.**201**(4358): 777–85. doi:10.1126/science.201.4358.777. PMID 17738519. S2CID 9129799 . Retrieved 25 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): 91–94. 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" (PDF).
*Physical Review Letters*.**49**(25): 1804–1807. Bibcode:1982PhRvL..49.1804A. doi: 10.1103/PhysRevLett.49.1804 . - ↑ "Physical Review Letters - Volume 28 Issue 14".
- ↑ 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 Archived 2012-03-20 at the Wayback Machine . (PDF) . Retrieved on 2012-05-17.
- ↑ Japan Atomic Energy Agency. Naka Fusion Institute Archived 2015-12-08 at the Wayback Machine
- ↑ Fusion Plasma Research (FPR), JASEA, Naka Fusion Institute Archived 2015-12-08 at the Wayback Machine . 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. S2CID 34578587. - ↑ 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). "H
_{2}^{+}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 25 April 2012. - ↑ PPPL, Princeton, USA Archived 2011-06-07 at the Wayback Machine . Pppl.gov (1999-02-12). Retrieved on 2012-05-17.
- ↑ Vainerman, Leonid (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. - ↑ 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. - ↑ Cho, Adrian (2010-12-17). "Breakthrough of the Year: The First Quantum Machine".
*Science*.**330**(6011): 1604. Bibcode:2010Sci...330.1604C. doi:10.1126/science.330.6011.1604. PMID 21163978. - ↑ "Coherent Population". Defense Procurement News. 2010-06-22. Retrieved 2013-01-30.
- ↑ "The Higgs boson | CERN".
*home.cern*. Retrieved 2020-08-26. - ↑ 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*.**345**(6196): 532–535. arXiv: 1404.4369 . Bibcode:2014Sci...345..532P. doi:10.1126/science.1253512. PMID 25082696. S2CID 2190249.

- Peacock, Kent A. (2008).
*The Quantum Revolution : A Historical Perspective**. Westport, Conn.: Greenwood Press. ISBN 9780313334481.* - Ben-Menahem, A. (2009). "Historical timeline of quantum mechanics 1925–1989".
*Historical Encyclopedia of Natural and Mathematical Sciences**(1st ed.). Berlin: Springer. pp. 4342–4349. ISBN 9783540688310.*

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