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Theory and simulations of quantum glass forming liquids
Theory and simulations of quantum glass forming liquids

chapter 10. relation to quantum mechanics
chapter 10. relation to quantum mechanics

... Objectivity is a property of a class of experimenters on the system; it expresses the mutual consistency of descriptions of the system by the various experimenters in the class. At this level of analysis, the group J is associated to the class of experimenters; one does not need to have a “configura ...
Invited talks - Swinburne University
Invited talks - Swinburne University

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Computational advantage from quantum

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Seminar Report

... factoring a three digit number. The use of computational resources is enormous when we keep increasing the number of digits. The largest number that has been factorized as a mathematical challenge, i.e. a number whose factors were secretly chosen by mathematicians in order to present a challenge to ...
A Quantum Structure Description of the Liar Paradox
A Quantum Structure Description of the Liar Paradox

Kondo, Fano and Dicke effects in side quantum dots
Kondo, Fano and Dicke effects in side quantum dots

exploiting the superposition principle foundations and applications
exploiting the superposition principle foundations and applications

Scattering model for quantum random walks on a hypercube
Scattering model for quantum random walks on a hypercube

Quantum and Ecosystem Entropies
Quantum and Ecosystem Entropies

... specify their dimensions as M 1/4 L2 /T 3 , T M −1/4 , and M 3/4 /L2 , respectively. Equation (2) is consistent with the quarter-power scaling proposed by West et al. (1997). This specific scaling, along with the general issue of appropriateness of allometric equations in biology, are topics of live ...
Nonclassical States of Cold Atomic Ensembles and of Light Fields
Nonclassical States of Cold Atomic Ensembles and of Light Fields

... For an ensemble spin vector S oriented along the x axis, a state is spin squeezed [20] along the z-direction (or “number squeezed”) if the uncertainty ΔSz obeys (ΔSz)2 < |〈Sx〉|/2. For a maximally coherent system with |〈Sx〉| ≈ S0, where S0 = N0/2 is the maximum possible spin of the ensemble containin ...
Lecture Notes of my Course on Quantum Computing
Lecture Notes of my Course on Quantum Computing

Shamsul Kaonain
Shamsul Kaonain

... involving infinite energies, or electrons spiraling inexorably into the atomic nucleus. At first such problems were resolved by addition of ad hoc hypotheses to classical physics, but as we gained better understanding of atoms and radiation, these attempted explanations became more and more convolut ...
Pedestrian notes on quantum mechanics
Pedestrian notes on quantum mechanics

State Preparation Quantum Optics Quantum Information Theory
State Preparation Quantum Optics Quantum Information Theory

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A Landau-Ginzburg model, flat coordinates and a mirror theorem for

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Indistinguishable photons from a single-photon device

Quantum Computer Compilers
Quantum Computer Compilers

preskill-ARO-2013 - Caltech Particle Theory
preskill-ARO-2013 - Caltech Particle Theory

Δk/k
Δk/k

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Closed timelike curves make quantum and classical computing

A Scenario for a Natural Origin of Our Universe
A Scenario for a Natural Origin of Our Universe

An Introduction to Quantum Field Theory, Mrinal Dasgupta
An Introduction to Quantum Field Theory, Mrinal Dasgupta

- RZ User
- RZ User

Quantum Turing Test
Quantum Turing Test

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Max Born



Max Born (German: [bɔɐ̯n]; 11 December 1882 – 5 January 1970) was a German physicist and mathematician who was instrumental in the development of quantum mechanics. He also made contributions to solid-state physics and optics and supervised the work of a number of notable physicists in the 1920s and 30s. Born won the 1954 Nobel Prize in Physics for his ""fundamental research in Quantum Mechanics, especially in the statistical interpretation of the wave function"".Born was born in 1882 in Breslau, then in Germany, now in Poland and known as Wrocław. He entered the University of Göttingen in 1904, where he found the three renowned mathematicians, Felix Klein, David Hilbert and Hermann Minkowski. He wrote his Ph.D. thesis on the subject of ""Stability of Elastica in a Plane and Space"", winning the University's Philosophy Faculty Prize. In 1905, he began researching special relativity with Minkowski, and subsequently wrote his habilitation thesis on the Thomson model of the atom. A chance meeting with Fritz Haber in Berlin in 1918 led to discussion of the manner in which an ionic compound is formed when a metal reacts with a halogen, which is today known as the Born–Haber cycle.In the First World War after originally being placed as a radio operator, due to his specialist knowledge he was moved to research duties regarding sound ranging. In 1921, Born returned to Göttingen, arranging another chair for his long-time friend and colleague James Franck. Under Born, Göttingen became one of the world's foremost centres for physics. In 1925, Born and Werner Heisenberg formulated the matrix mechanics representation of quantum mechanics. The following year, he formulated the now-standard interpretation of the probability density function for ψ*ψ in the Schrödinger equation, for which he was awarded the Nobel Prize in 1954. His influence extended far beyond his own research. Max Delbrück, Siegfried Flügge, Friedrich Hund, Pascual Jordan, Maria Goeppert-Mayer, Lothar Wolfgang Nordheim, Robert Oppenheimer, and Victor Weisskopf all received their Ph.D. degrees under Born at Göttingen, and his assistants included Enrico Fermi, Werner Heisenberg, Gerhard Herzberg, Friedrich Hund, Pascual Jordan, Wolfgang Pauli, Léon Rosenfeld, Edward Teller, and Eugene Wigner.In January 1933, the Nazi Party came to power in Germany, and Born, who was Jewish, was suspended. He emigrated to Britain, where he took a job at St John's College, Cambridge, and wrote a popular science book, The Restless Universe, as well as Atomic Physics, which soon became a standard text book. In October 1936, he became the Tait Professor of Natural Philosophy at the University of Edinburgh, where, working with German-born assistants E. Walter Kellermann and Klaus Fuchs, he continued his research into physics. Max Born became a naturalised British subject on 31 August 1939, one day before World War II broke out in Europe. He remained at Edinburgh until 1952. He retired to Bad Pyrmont, in West Germany. He died in hospital in Göttingen on 5 January 1970.
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