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Documentation
Documentation

... the opposite value, no matter how far both are apart; but until the measurement, the value of the property might be completely undetermined, but then they are “anti-” synchronized. This phenomenon had been rather controversial since it discovery by Einstein and his coworkers Podolsky and Rosen [3], ...
Talk Slides (pptx file) - University of Missouri
Talk Slides (pptx file) - University of Missouri

Quantum Game Theory
Quantum Game Theory

C. Heitzinger, C. Ringhofer. S. Ahmed, D. Vasileska
C. Heitzinger, C. Ringhofer. S. Ahmed, D. Vasileska

Quantum Game Theory
Quantum Game Theory

Density matrices
Density matrices

... Worked Exercise : Suppose a measurement described by projectors Pk is performed on an ensemble giving rise to the density matrix  . If the measurement gives result k show that the corresponding post-measurement density matrix is ...
Quantum Chaos and Quantum Information
Quantum Chaos and Quantum Information

2006
2006

... 2. The Role of Interactions in Quantum Reflection of Bose-Einstein Condensates Quantum reflection is the phenomena by which an atom is accelerated so abruptly by the Casimir-Polder potential that it reflects from the potential rather than being drawn into the surface. The usual model of quantum refl ...
Algorithms and Architectures for Quantum Computers
Algorithms and Architectures for Quantum Computers

... 1. Ion Lattices for Quantum Simulations During the past year, this project has demonstrated trapping of hot strontium ions in a mesh trap [5], had designed a method for optical coupling to ions for readout [6], has developed a detailed theoretical model of expected simulation performance [7], and ha ...
- Philsci-Archive
- Philsci-Archive

... old theory and therefore do not stand for natural classes. Of course, the persuasiveness of the objection depends on one’s understanding of information and explanatory power. In a certain way I believe that van Fraassen is right, although I don’t feel convinced by his argument. First, assume it is p ...
The Quantum Theory of the Electron
The Quantum Theory of the Electron

... The new quantum mechanics, when applied to the problem of the structure of the atom with point-charge electrons, does not give results in agreement with experiment. The discrepancies consist of " duplexity " phenomena, the observed number of stationary states for an electron in an atom being twice t ...
Introduction to Quantum Computation
Introduction to Quantum Computation

Modern Optics PHY485F/1485F www.physics.utoronto.ca/~phy485
Modern Optics PHY485F/1485F www.physics.utoronto.ca/~phy485

... PS#1 - due 2 October PS#2 - due 21 October Midterm Test: 28 October 2008, 5-7 pm OK? PS#3 - due 13 November PS#4 - due 4 December (zero extensions) Group seminar presentations 22 November 10-5pm ...
Are quantum particles objects? - General Guide To Personal and
Are quantum particles objects? - General Guide To Personal and

... description). Symmetrizing, in LS we say instead: (iv) There is x1 and x2 , where x1 is Bob-shaped and in the kitchen and x2 is Alice-shaped and not, or x2 is Bob-shaped and in the kitchen and x1 is Alice-shaped and not. Unlike the passage from (i) to (ii), there is no di¤erence between (iii) and (i ...
Quantum cryptography protocols robust against photon
Quantum cryptography protocols robust against photon

... uses single-photon sources. But the experimental realizations, especially the prototypes, use attenuated laser pulses as sources: in this case, a non-negligible fraction of the pulses contain more than one photon. In the year 2000, Lütkenhaus and co-workers realized that the presence of multi-photo ...
An introduction to quantum probability, quantum mechanics, and
An introduction to quantum probability, quantum mechanics, and

annalen der - Department of Physics and astronomy, Faculty of
annalen der - Department of Physics and astronomy, Faculty of

this document - ITP Lecture Archive
this document - ITP Lecture Archive

Chapter 12 Quantum gases
Chapter 12 Quantum gases

... Chapter 12 Quantum gases In classical statistical mechanics, we dealt with an ideal gas which was a good approximation for a real gas in the highly diluted limit. An important difference between classical and quantum mechanical many-body systems lies in the distinguishable character of their constit ...
Coupled Quantum– Atomistic and Quantum–Continuum Mechanics
Coupled Quantum– Atomistic and Quantum–Continuum Mechanics

Data-Intensive Analysis for High Energy Physics (DIANA/HEP)
Data-Intensive Analysis for High Energy Physics (DIANA/HEP)

Speculations on the Union of Science and Religion
Speculations on the Union of Science and Religion

Violation of Bell`s inequalities in a quantum realistic framework
Violation of Bell`s inequalities in a quantum realistic framework

Powerpoint 6/22
Powerpoint 6/22

... The system. This is like calling the probability distribution the State of the system and confuses our description of the system with the physical state of the system. For our classical machine, the system is always in one of the states. For the quantum system, this type of statement is much trickie ...
MORE ON ERROR CORRECTION. Slides in PPT.
MORE ON ERROR CORRECTION. Slides in PPT.

... Encode qubits (together with extra ancillary qubits) in a state where subsequent errors can be corrected. Allows long algorithms requiring many operations to run, as errors can be corrected after they occur. ...
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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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