Michael Kosterlitz | |
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Born | John Michael Kosterlitz June 22, 1943 [1] Aberdeen, Scotland, United Kingdom |
Nationality | British |
Citizenship | United States |
Alma mater |
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Known for | Berezinskii–Kosterlitz–Thouless transition KTHNY theory |
Awards |
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Scientific career | |
Fields | Condensed matter physics |
Institutions | Brown University University of Birmingham Cornell University |
Thesis | Problems in strong interaction physics (1969) |
Academic advisors | David Thouless (postdoc) |
Website | vivo |
John Michael Kosterlitz (born June 22, 1943) is a Scottish-American physicist. He is a professor of physics at Brown University [4] and the son of biochemist Hans Kosterlitz. He was awarded the 2016 Nobel Prize in physics along with David Thouless and Duncan Haldane for work on condensed matter physics. [2]
He was born in Aberdeen, Scotland, [5] to German-Jewish émigrés, the son of the pioneering biochemist [6] Hans Walter Kosterlitz and Hannah Gresshöner. He was educated independently at Robert Gordon's College before transferring to the Edinburgh Academy to prepare for his university entrance examinations. [7] He received his BA degree, subsequently converted to an MA degree, at Gonville and Caius College, Cambridge. [5] In 1969, he earned a DPhil degree [8] from the University of Oxford as a postgraduate student of Brasenose College, Oxford. [5]
After a few postdoctoral positions, including positions at the University of Birmingham, collaborating with David Thouless, [5] and at Cornell University, [5] he was appointed to the faculty of the University of Birmingham in 1974, [5] first as a lecturer and, later, as a reader. Since 1982, he has been professor of physics at Brown University. Kosterlitz is currently[ when? ] a visiting research fellow at Aalto University in Finland[ citation needed ] and since 2016 a distinguished professor at Korea Institute for Advanced Study.
Kosterlitz does research in condensed matter theory, one- and two-dimensional physics; in phase transitions: random systems, electron localization, and spin glasses; and in critical dynamics: melting and freezing.[ citation needed ]
Michael Kosterlitz was awarded the Nobel Prize in Physics in 2016, “for theoretical discoveries of topological phase transitions and topological phases of matter”; [9] the Maxwell Medal and Prize from the British Institute of Physics in 1981, and the Lars Onsager Prize from the American Physical Society in 2000, especially, for his work on the Berezinskii–Kosterlitz–Thouless transition. Since 1992, he has been a Fellow of the American Physical Society. [10]
The Kosterlitz Centre at the University of Aberdeen is named in honour of his father, Hans Kosterlitz, a pioneering biochemist specializing in endorphins, who joined the faculty after fleeing Nazi persecution of Jews in 1934. [11]
Kosterlitz was a pioneer in Alpine climbing in the 1960s, known for working routes in the UK, Italian Alps, and Yosemite. [12] There is 6a+ graded route bearing his name in the Orco Valley of the Italian Alps named Fessura Kosterlitz. [13] Kosterlitz is an American citizen and is an atheist. [14] He was diagnosed with multiple sclerosis in 1978. [15]
Lars Onsager was a Norwegian American physical chemist and theoretical physicist. He held the Gibbs Professorship of Theoretical Chemistry at Yale University. He was awarded the Nobel Prize in Chemistry in 1968.
Yang Chen-Ning or Chen-Ning Yang, also known as C. N. Yang or by the English name Frank Yang, is a Chinese theoretical physicist who made significant contributions to statistical mechanics, integrable systems, gauge theory, and both particle physics and condensed matter physics. He and Tsung-Dao Lee received the 1957 Nobel Prize in Physics for their work on parity non-conservation of weak interaction. The two proposed that the conservation of parity, a physical law observed to hold in all other physical processes, is violated in the so-called weak nuclear reactions, those nuclear processes that result in the emission of beta or alpha particles. Yang is also well known for his collaboration with Robert Mills in developing non-abelian gauge theory, widely known as the Yang–Mills theory.
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Leo Philip Kadanoff was an American physicist. He was a professor of physics at the University of Chicago and a former president of the American Physical Society (APS). He contributed to the fields of statistical physics, chaos theory, and theoretical condensed matter physics.
The Berezinskii–Kosterlitz–Thouless (BKT) transition is a phase transition of the two-dimensional (2-D) XY model in statistical physics. It is a transition from bound vortex-antivortex pairs at low temperatures to unpaired vortices and anti-vortices at some critical temperature. The transition is named for condensed matter physicists Vadim Berezinskii, John M. Kosterlitz and David J. Thouless. BKT transitions can be found in several 2-D systems in condensed matter physics that are approximated by the XY model, including Josephson junction arrays and thin disordered superconducting granular films. More recently, the term has been applied by the 2-D superconductor insulator transition community to the pinning of Cooper pairs in the insulating regime, due to similarities with the original vortex BKT transition.
In physics, a topological quantum number is any quantity, in a physical theory, that takes on only one of a discrete set of values, due to topological considerations. Most commonly, topological quantum numbers are topological invariants associated with topological defects or soliton-type solutions of some set of differential equations modeling a physical system, as the solitons themselves owe their stability to topological considerations. The specific "topological considerations" are usually due to the appearance of the fundamental group or a higher-dimensional homotopy group in the description of the problem, quite often because the boundary, on which the boundary conditions are specified, has a non-trivial homotopy group that is preserved by the differential equations. The topological quantum number of a solution is sometimes called the winding number of the solution, or, more precisely, it is the degree of a continuous mapping.
Thouless may refer to:
Michael Ellis Fisher was an English physicist, as well as chemist and mathematician, known for his many seminal contributions to statistical physics, including but not restricted to the theory of phase transitions and critical phenomena. He was the Horace White Professor of Chemistry, Physics, and Mathematics at Cornell University. Later he moved to the University of Maryland College of Computer, Mathematical, and Natural Sciences, where he was University System of Maryland Regents Professor, a Distinguished University Professor and Distinguished Scholar-Teacher.
The superconductor–insulator transition is an example of a quantum phase transition, whereupon tuning some parameter in the Hamiltonian, a dramatic change in the behavior of the electrons occurs. The nature of how this transition occurs is disputed, and many studies seek to understand how the order parameter, , changes. Here is the amplitude of the order parameter, and is the phase. Most theories involve either the destruction of the amplitude of the order parameter - by a reduction in the density of states at the Fermi surface, or by destruction of the phase coherence; which results from the proliferation of vortices.
David James Thouless was a British condensed-matter physicist. He was the winner of the 1990 Wolf Prize and a laureate of the 2016 Nobel Prize for physics along with F. Duncan M. Haldane and J. Michael Kosterlitz for theoretical discoveries of topological phase transitions and topological phases of matter.
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Frederick Duncan Michael Haldane, known as F. Duncan Haldane, is a British-born physicist who is currently the Sherman Fairchild University Professor of Physics at Princeton University. He is a co-recipient of the 2016 Nobel Prize in Physics, along with David J. Thouless and J. Michael Kosterlitz.
Vadim L'vovich Berezinskii was a Soviet physicist. He was born in Kyiv, graduated from Moscow State University in 1959, and worked in Moscow and the Landau Institute for Theoretical Physics. He is famous for having identified the role played by topological defects in the low-temperature phase of two-dimensional systems with a continuous symmetry. His work led to the discovery of the Berezinskii–Kosterlitz–Thouless transition, for which John M. Kosterlitz and David J. Thouless were awarded the Nobel Prize in 2016. He also developed a technique for treating electrons in one-dimensional disordered systems and provided first consistent proof of one-dimensional localization, and predicted negative-gap superconductivity.
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