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Profile Documents Logout
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lattice approximations
lattice approximations

... and extrinsic!), compatible with the structure of constraints. Positivity of gravitational energy implemented on every level of discrete approximations of geometry. Representation of the observable algebra on every level of ...
Physics 211 - University of Utah
Physics 211 - University of Utah

Quantum Numbers, Spectra Calculations
Quantum Numbers, Spectra Calculations

... - The human eye is most sensitive in this range ...
A Quantum Information Processing Explanation of Disjunction Effects
A Quantum Information Processing Explanation of Disjunction Effects

... possible states of thought that you can entertain about your opponent. There is some probability p of thinking ‘the other will compete’ and there is some complementary probability (1−p) of thinking ‘the other will cooperate.’ There are also two actions that you can take, compete or cooperate, condit ...
the problem book
the problem book

... 2 (Ek,l,n − E0,0,0 )
OPTICS14399
OPTICS14399

... Since the early days of quantum mechanics, it has been known that certain quantum states have a mysterious non-local behavior [1]. The phenomenon responsible for these non-local correlations among the subsystems of a composite quantum system is called entanglement [2]. Quantum entanglement, having n ...
Reversible universal quantum computation within translation
Reversible universal quantum computation within translation

Scanned copy Published in Physical Principles of Neuronal and
Scanned copy Published in Physical Principles of Neuronal and

... physicist, not because he hopes he can solve the problem of how the brain works, but because this behavior makes him reconsider some fundamental problems of physics. Perhaps this thinking also will result in a better understanding of how the brain works, but that is not the principle stimulus. What ...
Chirped-frequency excitation of gravitationally bound ultracold
Chirped-frequency excitation of gravitationally bound ultracold

No Slide Title
No Slide Title

... For centro-symmetric systems in which the force works in the same direction as r we must have dL dt = 0 : THE ANGULAR MOMENTUM IS CONSERVED ...
USER CASE - ID Quantique
USER CASE - ID Quantique

The Polynomial Method in Quantum and Classical
The Polynomial Method in Quantum and Classical

Complementarity in Quantum Mechanics and Classical Statistical
Complementarity in Quantum Mechanics and Classical Statistical

... experimental confirmation of these wave-particle duality for any kind of matter revealed the unity of material world. In fact, wave-particle duality is a property of matter as universal as the fact that any kind of matter is able to produce a gravitational interaction. While the state of a system in ...
View paper - UT Mathematics
View paper - UT Mathematics

... quantum radiation field may give rise to fluctuations of the position of the electron and these fluctuations may change the Coulomb potential so that the energy level shift such as the Lamb shift may occur. With this physical intuition, he derived the Lamb shift heuristically and perturbatively. After ...
PHYSICS VS. SEMANTICS: A PUZZLING CASE
PHYSICS VS. SEMANTICS: A PUZZLING CASE

... We shall therefore reformulate this issue in the form of ”missing quantum theories case”: why do we fail to recognize several distinct quantum theories in their own right? Why should we be content in this case (contrary to the entire history of science) not to inquire which-of the existing alternati ...
The evolution of arbitrary computational processes
The evolution of arbitrary computational processes

What is Solid State Physics? - Department of Physics and Astronomy
What is Solid State Physics? - Department of Physics and Astronomy

Measurement-based formulation of quantum heat engines and
Measurement-based formulation of quantum heat engines and

Commentary_Basti
Commentary_Basti

course objectives - Metropolitan Community College
course objectives - Metropolitan Community College

cosmic natural selection as an explanation for our fine
cosmic natural selection as an explanation for our fine

... populations of genes or phenotypes evolve on socalled fitness landscapes. The analogy was obvious. The possible vacua of string theory live on a “theory fitness landscape,” analogous to the fitness landscape of phenotypes. And the parameters of the standard model evolve, as do genes in biology. To c ...
A (very) brief tour of quantum mechanics, computation, and category
A (very) brief tour of quantum mechanics, computation, and category

class notes
class notes

... provide any systematic method for finding the conjugate momentums. He has chosen special examples from classical mechanics where he knows the conjugate momentums from his freshman physics work. I believe that his presentation fails to convey the real power of Hamilton's work. The Hamiltonian and the ...
Department of Physics MSc Handbook 2012/13 www.kcl.ac.uk/physics
Department of Physics MSc Handbook 2012/13 www.kcl.ac.uk/physics

2.2 Schrödinger`s wave equation
2.2 Schrödinger`s wave equation

... Electrons as waves de Broglie’s hypothesis is that the electron wavelength  is given by ...
< 1 ... 128 129 130 131 132 133 134 135 136 ... 252 >

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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