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Schumacher Compression
Schumacher Compression

indistinguishability - University of Oxford
indistinguishability - University of Oxford

... number Ns of ‘energy elements’ over a system of Cs states (or ‘resonators’)? The distribution of energy over each type of resonator must now be considered, first, the distribution of the energy Es over the Cs resonators with frequency s . If Es is regarded as infinitely divisible, an infinite number ...
Subjective Bayesian probabilities
Subjective Bayesian probabilities

... inside information relative to a party Z is when Z assigns a pure state. Z is said to have a maximal belief structure. Subjective Bayesian answer We trust quantum over classical coin tossing because an insider attack on classical coin tossing can never be ruled out, whereas the beliefs that lead to ...
Non-local quantum effects in cosmology 1
Non-local quantum effects in cosmology 1

Block Weighing Matrices
Block Weighing Matrices

A Review and Prospects of Quantum Teleportation
A Review and Prospects of Quantum Teleportation

An Effective Quantum Potential for Particle
An Effective Quantum Potential for Particle

pdf - ISI Foundation
pdf - ISI Foundation

... In recent years topological phases have been intensively studied in condensed-matter systems. These exotic states appear in different contexts, such as fractional quantum Hall physics, spin liquids, and topological insulators 关1–7兴. Their understanding is relevant to topological quantum computation, ...
Triple to quintuple quantum dots for making multiple qubits
Triple to quintuple quantum dots for making multiple qubits

... understanding the foundation of quantum physics but also a critical issue in quantum information technologies. Studying central spin decoherence caused by environmental fluctuations may yield key insights into the nature of many-body interactions in the environment. Furthermore, dynamical control ov ...
Are there basic laws of quantum information processing?
Are there basic laws of quantum information processing?

... information and another system in an established state (hence representing no quantum information). Now, if the unitary transformation over the whole system is performed, one can observe how the information is spread over the system. As there was one qubit of initial amount of information and the in ...
Zeno dynamics in quantum open systems
Zeno dynamics in quantum open systems

... states[14, 15]. QZE has become a focus of attention not only because it can be applied in robust quantum information processing, but also because of its foundational implications about the nature of quantum measurement[2] as well as indistinguishability of state[16] and entanglement[17]. Recently, i ...
Private Quantum Channels
Private Quantum Channels

Level Repulsion of Localized Excitons in Disordered Quantum Wells
Level Repulsion of Localized Excitons in Disordered Quantum Wells

SELECTED TOPICS IN QUANTUM MECHANICS Pietro Menotti
SELECTED TOPICS IN QUANTUM MECHANICS Pietro Menotti

Prime Factorization Using Quantum Annealing and Algebraic
Prime Factorization Using Quantum Annealing and Algebraic

The pressure increase at 4He l–point explained by means of the
The pressure increase at 4He l–point explained by means of the

slides on Quantum Isometry Groups
slides on Quantum Isometry Groups

Indexing terms/Keywords
Indexing terms/Keywords

Unbounded operators and the incompleteness of quantum mechanics
Unbounded operators and the incompleteness of quantum mechanics

Some Problems in Quantum Information Theory
Some Problems in Quantum Information Theory

Time in Thermodynamics
Time in Thermodynamics

... reverse-running film as much as to the forward-playing one. Intuitively, the law does not contain any direction of time in it. We can see this by noting that each quantity in the law has the same value in both films: in the backward film, the forces between the particles are the same as in the forwa ...
Chapter 8 Path Integrals in Statistical Mechanics
Chapter 8 Path Integrals in Statistical Mechanics

Teleportation of an atomic state between two cavities using nonlocal
Teleportation of an atomic state between two cavities using nonlocal

... easily achieved by properly setting, through Stark field adjustments, the times during which the atom is resonant with each cavity. The atomic transitions are accompanied by corresponding photon number changes. When c has undergone the first m. /2 pulse, the second cavity is still empty and the "ato ...
ppt - QEC14
ppt - QEC14

... examples from current work in quantum-dot qubits. Mighty efforts are underway to improve laboratory fidelities, which are however neither quantitatively nor methodologically complete. Leakage reduction units are starting to come over the horizon, but QEC could probably help more with this. There are ...
ESSAY REVIEW: The many Metaphysics within Physics 1 9
ESSAY REVIEW: The many Metaphysics within Physics 1 9

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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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