Timeline of quantum mechanics

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

Contents

19th century

Image of Becquerel's photographic plate that 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. Becquerel plate.jpg
Image of Becquerel's photographic plate that 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.

20th century

1900–1909

Einstein, in 1905, when he wrote the Annus Mirabilis papers Einstein patentoffice.jpg
Einstein, in 1905, when he wrote the Annus Mirabilis papers

1910–1919

A schematic diagram of the apparatus for Millikan's refined oil drop experiment Scheme of Millikan's apparatus.jpg
A schematic diagram of the apparatus for Millikan's refined oil drop experiment

1920–1929

A plaque at the University of Frankfurt commemorating the Stern-Gerlach experiment SternGerlach2.jpg
A plaque at the University of Frankfurt commemorating the Stern–Gerlach experiment

1930–1939

Electron microscope constructed by Ernst Ruska in 1933 Ernst Ruska Electron Microscope - Deutsches Museum - Munich-edit.jpg
Electron microscope constructed by Ernst Ruska in 1933

1940–1949

A Feynman diagram showing the radiation of a gluon when an electron and positron are annihilated Feynmann Diagram Gluon Radiation.svg
A Feynman diagram showing the radiation of a gluon when an electron and positron are annihilated

1950–1959

1960–1969

The baryon decuplet of the Eightfold Way proposed by Murray Gell-Mann in 1962. The
O
particle at the bottom had not yet been observed at the time, but a particle closely matching these predictions was discovered by a particle accelerator group at Brookhaven, proving Gell-Mann's theory. Baryon decuplet.png
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 by a particle accelerator group at Brookhaven, proving Gell-Mann's theory.

1971–1979

1980–1999

21st century

Graphene is a planar atomic-scale honeycomb lattice made of carbon atoms, which exhibits unusual and interesting quantum properties. Graphen.jpg
Graphene is a planar atomic-scale honeycomb lattice made of carbon atoms, which exhibits unusual and interesting quantum properties.

See also

Related Research Articles

<span class="mw-page-title-main">Atom</span> Smallest unit of a chemical element

Atoms are the basic particles of the chemical elements. An atom consists of a nucleus of protons and generally neutrons, surrounded by an electromagnetically bound swarm of electrons. 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. Atoms with the same number of protons but a different number of neutrons are called isotopes of the same element.

<span class="mw-page-title-main">History of atomic theory</span>

Atomic theory is the scientific theory that matter is composed of particles called atoms. The definition of the word "atom" has changed over the years in response to scientific discoveries. Initially, it referred to a hypothetical concept of there being some fundamental particle of matter, too small to be seen by the naked eye, that could not be divided. Then the definition was refined to being the basic particles of the chemical elements, when chemists observed that elements seemed to combine with each other in ratios of small whole numbers. Then physicists discovered that these particles had an internal structure of their own and therefore perhaps did not deserve to be called "atoms", but renaming atoms would have been impractical by that point.

<span class="mw-page-title-main">Bohr model</span> Atomic model introduced by Niels Bohr in 1913

In atomic physics, the Bohr model or Rutherford–Bohr model is an obsolete model of the atom, presented by Niels Bohr and Ernest Rutherford in 1913. It 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.

<span class="mw-page-title-main">Electron</span> Elementary particle with negative charge

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.

<span class="mw-page-title-main">Neutron</span> Subatomic particle with no charge

The neutron is a subatomic particle, symbol
n
or
n0
, 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, they are both referred to as nucleons. Nucleons have a mass of approximately one atomic mass unit, or dalton. Their properties and interactions are described by nuclear physics. Protons and neutrons are not elementary particles; each is composed of three quarks.

<span class="mw-page-title-main">Nuclear physics</span> Field of physics that studies atomic nuclei

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 photon is an elementary particle that is a quantum of the electromagnetic field, including electromagnetic radiation such as light and radio waves, and the force carrier for the electromagnetic force. Photons are massless particles that always move at the speed of light measured in vacuum. The photon belongs to the class of boson particles.

<span class="mw-page-title-main">Pauli exclusion principle</span> Quantum mechanics rule: identical fermions cannot occupy the same quantum state simultaneously

In quantum mechanics, the Pauli exclusion principle states that two or more identical particles with half-integer spins cannot simultaneously occupy the same quantum state within a system that obeys the laws of quantum mechanics. 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.

<span class="mw-page-title-main">Quantum mechanics</span> Description of physical properties at the atomic and subatomic scale

Quantum mechanics is a fundamental theory that describes the behavior of nature at and below the scale of atoms. It is the foundation of all quantum physics, which includes quantum chemistry, quantum field theory, quantum technology, and quantum information science.

Wave-particle duality is the concept in quantum mechanics that quantum entities exhibit particle or wave properties according to the experimental circumstances. It expresses the inability of the classical concepts such as particle or wave to fully describe the behavior of quantum objects. During the 19th and early 20th centuries, light was found to behave as a wave then later discovered to have a particulate behavior, whereas electrons behaved like particles in early experiments then later discovered to have wavelike behavior. The concept of duality arose to name these seeming contradictions.

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.

An exotic atom is an otherwise normal atom in which one or more sub-atomic particles have been replaced by other particles of the same charge. For example, electrons may be replaced by other negatively charged particles such as muons or pions. Because these substitute particles are usually unstable, exotic atoms typically have very short lifetimes and no exotic atom observed so far can persist under normal conditions.

A timeline of atomic and subatomic physics, including particle physics.

<span class="mw-page-title-main">Quantum number</span> Notation for conserved quantities in physics and chemistry

In quantum physics and chemistry, quantum numbers are quantities that characterize the possible states of the system. Quantum numbers are closely related to eigenvalues of observables. When the corresponding observable commutes with the Hamiltonian, the quantum number is said to be "good", and acts as a constant of motion in the quantum dynamics.

<span class="mw-page-title-main">Stern–Gerlach experiment</span> 1922 physical experiment demonstrating that atomic spin is quantized

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. Building on the technology developed in classical mechanics, the invention of wave mechanics by Erwin Schrödinger and expansion by many others triggers the "modern" era beginning around 1925. Paul 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.

In the history of quantum mechanics, the Bohr–Kramers–Slater (BKS) theory was perhaps the final attempt at understanding the interaction of matter and electromagnetic radiation on the basis of the so-called old quantum theory, in which quantum phenomena are treated by imposing quantum restrictions on classically describable behaviour. It was advanced in 1924, and sticks to a classical wave description of the electromagnetic field. It was perhaps more a research program than a full physical theory, the ideas that are developed not being worked out in a quantitative way. The purpose of BKS theory was to disprove Einstein's hypothesis of the light quantum.

<span class="mw-page-title-main">Discovery of the neutron</span> Scientific background leading to the discovery of subatomic particles

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.

The nucleon magnetic moments are the intrinsic magnetic dipole moments of the proton and neutron, symbols μp and μn. The nucleus of an atom comprises protons and neutrons, both nucleons that behave as small magnets. Their magnetic strengths are measured by their magnetic moments. The nucleons interact with normal matter through either the nuclear force or their magnetic moments, with the charged proton also interacting by the Coulomb force.

References

  1. 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 Peacock 2008 , pp. 175–183
  2. Becquerel, Henri (1896). "Sur les radiations émises par phosphorescence". Comptes Rendus. 122: 420–421.
  3. "Milestone 1 : Nature Milestones in Spin". www.nature.com. Retrieved 2018-09-09.
  4. Marie Curie and the Science of Radioactivity: Research Breakthroughs (1897–1904) Archived 2015-11-17 at the Wayback Machine . Aip.org. Retrieved on 2012-05-17.
  5. Histories of the Electron: The Birth of Microphysics edited by Jed Z. Buchwald, Andrew Warwick
  6. Larmor, Joseph (1897), "On a Dynamical Theory of the Electric and Luminiferous Medium, Part 3, Relations with material media"  , Philosophical Transactions of the Royal Society, 190: 205–300, Bibcode:1897RSPTA.190..205L, doi: 10.1098/rsta.1897.0020
  7. Larmor, Joseph (1897), "On a Dynamical Theory of the Electric and Luminiferous Medium, Part 3, Relations with material media"  , 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."
  8. Soddy, Frederick (December 12, 1922). "The origins of the conceptions of isotopes" (PDF). Nobel Lecture in Chemistry. Retrieved 25 April 2012.
  9. Ernest Rutherford, Baron Rutherford of Nelson, of Cambridge. Encyclopædia Britannica on-line. Retrieved on 2012-05-17.
  10. The Nobel Prize in Chemistry 1908: Ernest Rutherford. nobelprize.org
  11. J. W. Nicholson, Month. Not. Roy. Astr. Soc. lxxii. pp. 49,130, 677, 693, 729 (1912).
  12. 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.
  13. On the Constitution of Atoms and Molecules Niels Bohr, Philosophical Magazine, Series 6, Volume 26 July 1913, pp. 1–25
  14. McCormmach, Russell (Spring 1967). "Henri Poincaré and the Quantum Theory". Isis. 58 (1): 37–55. doi:10.1086/350182. S2CID   120934561.
  15. 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.
  16. On the Constitution of Atoms and Molecules, Niels Bohr, Philosophical Magazine, Series 6, Volume 26 July 1913, pp. 1–25
  17. Procopiu, Ştefan (1913). "Determining the Molecular Magnetic Moment by M. Planck's Quantum Theory". Bulletin Scientifique de l'Académie Roumaine de Sciences. 1: 151.
  18. 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 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!
  19. P. S. Epstein, Zur Theorie des Starkeffektes, Annalen der Physik, vol. 50, pp. 489–520 (1916)
  20. K. Schwarzschild, Sitzungsberichten der Kgl. Preuss. Akad. d. Wiss. April 1916, p. 548
  21. Lewis, G. N. (1916), "The Atom and the Molecule", J. Am. Chem. Soc., 38 (4): 762–85, doi:10.1021/ja02261a002, S2CID   95865413
  22. 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)
  23. Lewis, G.N. (1926). "The conservation of photons". Nature . 118 (2981): 874–875. Bibcode:1926Natur.118..874L. doi:10.1038/118874a0. S2CID   4110026.
  24. P. S. Epstein, "The Stark Effect from the Point of View of Schroedinger's Quantum Theory", Physical Review, vol 28, pp. 695–710 (1926)
  25. John von Neumann. 1932. The Mathematical Foundations of Quantum Mechanics, Princeton University Press: Princeton, New Jersey, reprinted in 1955, 1971 and 1983 editions
  26. 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 .
  27. 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.
  28. Brauer, Richard; Weyl, Hermann (1935). "Spinors in n dimensions". American Journal of Mathematics. 57 (2): 425–449. doi:10.2307/2371218. JSTOR   2371218.
  29. Frédéric Joliot-Curie (December 12, 1935). "Chemical evidence of the transmutation of elements" (PDF). Nobel Lecture. Retrieved 25 April 2012.
  30. 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)
  31. Birkhoff, Garrett & von Neumann, J. (1936). "The Logic of Quantum Mechanics". Annals of Mathematics. 37 (4): 823–843. doi:10.2307/1968621. JSTOR   1968621.
  32. Omnès, Roland (8 March 1999). Understanding Quantum Mechanics . Princeton University Press. ISBN   978-0-691-00435-8 . Retrieved 17 May 2012.
  33. 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.
  34. 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.
  35. 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 .
  36. 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.
  37. 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.
  38. 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.
  39. 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 .
  40. 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.
  41. Bloch, F. (1946). "Nuclear Induction". Physical Review. 70 (7–8): 460–474. Bibcode:1946PhRv...70..460B. doi: 10.1103/PhysRev.70.460 .
  42. 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.
  43. 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.
  44. 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.
  45. Hugh Everett Theory of the Universal Wavefunction, Thesis, Princeton University, (1956, 1973), pp 1–140
  46. 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.
  47. 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)
  48. Barnes, V.E.; 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.
  49. Abragam, Anatole (1961). The Principles of Nuclear Magnetism. Oxford: Clarendon Press. OCLC   242700.
  50. Brian David Josephson (December 12, 1973). "The Discovery of Tunnelling Supercurrents" (PDF). Nobel Lecture. Retrieved 25 April 2012.
  51. Maria Goeppert Mayer (December 12, 1963). "The shell model" (PDF). Nobel Lecture. Retrieved 25 April 2012.
  52. 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.
  53. 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.
  54. 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.
  55. 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.
  56. 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.
  57. 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.
  58. 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 .
  59. 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 .
  60. "Physical Review Letters – Volume 28 Issue 14".
  61. "The Nobel Prize in Physics 2022". NobelPrize.org. Retrieved 2024-04-20.
  62. TFTR Machine Parameters. W3.pppl.gov (1996-05-10). Retrieved on 2012-05-17.
  63. JET's Main Features-EFDA JET Archived 2011-11-20 at the Wayback Machine . Jet.efda.org. Retrieved on 2012-05-17.
  64. European JET website Archived 2012-03-20 at the Wayback Machine . (PDF) . Retrieved on 2012-05-17.
  65. Japan Atomic Energy Agency. Naka Fusion Institute Archived 2015-12-08 at the Wayback Machine
  66. 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.
  67. 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.
  68. 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.
  69. 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.
  70. 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
  71. 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.
  72. 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.
  73. 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.
  74. 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.
  75. Richard R. Ernst (December 9, 1992). "Nuclear Magnetic Resonance Fourier Transform (2D-FT) Spectroscopy" (PDF). Nobel Lecture. Retrieved 25 April 2012.
  76. Shor, P.W. (1994). "Algorithms for quantum computation: Discrete logarithms and factoring". Proceedings 35th Annual Symposium on Foundations of Computer Science. IEEE Comput. Soc. Press. pp. 124–134. doi:10.1109/SFCS.1994.365700. ISBN   978-0-8186-6580-6.
  77. Nielsen, Michael A.; Chuang, Isaac L. (2010-12-09). Quantum Computation and Quantum Information: 10th Anniversary Edition. doi:10.1017/CBO9780511976667. ISBN   978-1-107-00217-3 . Retrieved 2024-04-20.{{cite book}}: |website= ignored (help)
  78. PPPL, Princeton, USA Archived 2011-06-07 at the Wayback Machine . Pppl.gov (1999-02-12). Retrieved on 2012-05-17.
  79. Vandersypen, Lieven M. K.; Steffen, Matthias; Breyta, Gregory; Yannoni, Costantino S.; Sherwood, Mark H.; Chuang, Isaac L. (December 2001). "Experimental realization of Shor's quantum factoring algorithm using nuclear magnetic resonance". Nature. 414 (6866): 883–887. arXiv: quant-ph/0112176 . Bibcode:2001Natur.414..883V. doi:10.1038/414883a. ISSN   1476-4687. PMID   11780055.
  80. 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.
  81. 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.
  82. 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.
  83. "Coherent Population". Defense Procurement News. 2010-06-22. Retrieved 2013-01-30.
  84. "The Higgs boson | CERN". home.cern. Retrieved 2020-08-26.
  85. Markoff, John (29 May 2014). "Scientists Report Finding Reliable Way to Teleport Data". New York Times . Retrieved 29 May 2014.
  86. 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.

Bibliography