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... This section offers a brief background on basic concepts in quantum computation. Quantum States and Superposition: While classical bits exist in only one of the binary states at any given time, quantum bits, or qubits, can exist in a superposition state, which is a linear combination of the |0i and ...
Nonlinear scattering of atomic bright solitons in disorder
Nonlinear scattering of atomic bright solitons in disorder

Quantum computation of scattering in scalar quantum field theories
Quantum computation of scattering in scalar quantum field theories

1996 Orchestrated Objective Reduction of Quantum Coherence in
1996 Orchestrated Objective Reduction of Quantum Coherence in

... Quantum theory describes the surprising behavior at a fundamental level of matter and energy which comprise our universe. At the base of quantum theory is the wave/particle duality of atoms and their components. As long as a quantum system such as an atom or sub-atomic particle remains isolated from ...
Experimental Implementation of Adiabatic Passage between
Experimental Implementation of Adiabatic Passage between

... Over the past thirty years, it has become increasingly clear that the Landau symmetry-breaking theory cannot describe all phases of matter and their quantum phase transitions (QPTs) [1–3]. The discovery of the fractional quantum Hall (FQH) effect [4] indicates the existence of an exotic state of mat ...
Born−Oppenheimer Time-Dependent Systems
Born−Oppenheimer Time-Dependent Systems

Adding quantum effects to the semi-classical molecular
Adding quantum effects to the semi-classical molecular

Pauline Oliveros and Quantum Sound
Pauline Oliveros and Quantum Sound

... change, all structures come to be understood in completely new ways. David Bohm discusses, for instance, radical changes in language structure, necessitated by the fact that language as constructed within the framework of a classical physics worldview is by necessity itself atomistic and fragmentary ...
Superconducting Circuits and Quantum Computation T. P. Orlando
Superconducting Circuits and Quantum Computation T. P. Orlando

... particularly promising feature of using superconducting technology is the potential of developing highspeed, on-chip control circuitry with classical, high-speed superconducting electronics. The picosecond time scales of this electronics means that the superconducting qubits scan be controlled rapid ...
The next stage: quantum game theory
The next stage: quantum game theory

Fractionalization, Topological Order, and
Fractionalization, Topological Order, and

... natural and is independent of the concrete model or mechanism of the fractionalization, while it naturally applies to all the known cases. Let us assume that the fractional charge of the quasiparticle is p=q, where p and q are mutually prime integers. For simplicity, let us, for a moment, consider a ...
Spin-Mediated Consciousness Theory: Possible Roles
Spin-Mediated Consciousness Theory: Possible Roles

The Quantum Mechanical Frame of  Reference Andrew Soltau
The Quantum Mechanical Frame of  Reference Andrew Soltau

litera_1
litera_1

From Quantum Gates to Quantum Learning: recent research and
From Quantum Gates to Quantum Learning: recent research and

... Quantum Parallelism • Put all 7-bits into a superposition state • superposition allows quantum computer to make calculations on all 128 possible numbers (27) in ONE iteration i.e. finishes in 1 second. • Tremendous possibilities… imagine doing computations on even larger sample spaces all at the sa ...
Quantum Symmetric States - UCLA Department of Mathematics
Quantum Symmetric States - UCLA Department of Mathematics

... Thus, the expectation E can be seen as an integral (w.r.t. a probability measure on the tail algebra) — that is, as a sort of convex combination — of expectations with respect to which the random variables x1 , x2 , . . . are independent and identically distributed (i.i.d.). Dykema (TAMU) ...
Many Body Quantum Mechanics
Many Body Quantum Mechanics

... 1.6 PROBLEM. Prove that (1) holds if and only if (ψ, Aψ) ∈ R for all ψ ∈ D(A). 1.7 REMARK. It is in general not easy to define the sum of two operators A and B. The problem is that the natural domain of A + B would be D(A) ∩ D(B), which is not necessarily densely defined. 1.8 EXAMPLE. The Hilbert sp ...
Machine invention of quantum computing circuits by means
Machine invention of quantum computing circuits by means

Quantum critical temperature of a modulated oscillator Lingzhen Guo, Vittorio Peano, M. Marthaler,
Quantum critical temperature of a modulated oscillator Lingzhen Guo, Vittorio Peano, M. Marthaler,

... in this respect are large rare quantum fluctuations that lead to switching between coexisting stable vibrational states (SVSs) and the occurrence of switching mechanisms that have no analog in equilibrium systems. The switching is important also for applications in quantum information [2–9]. For a r ...
Quantum Theory: a Pragmatist Approach
Quantum Theory: a Pragmatist Approach

Document
Document

... coding + Steane ancilla) • The quantum configuration is used in order to dictate a superposition of distinct correcting circuits. The configuration register is measured => just one of the circuits (corresponding to the measured configuration) is used for the actual correction. • k superposed correct ...
What is matter? The fundamental ontology of atomism and structural
What is matter? The fundamental ontology of atomism and structural

... admits only the quantum state of the universe in its ontology (as represented by the universal wave function); this state always undergoes a linear evolution (as represented e.g. by the Schrödinger equation) (see Wallace (2012) for the most detailed contemporary account). However, although it is a ...
view Pdf - Informatik - FB3
view Pdf - Informatik - FB3

to get the file
to get the file

... The recent expriments on photonic topological insuolators signified a new direction in photonics. The progress in this area will be reviewed, with an emphasis on universal ideas common to optics, cold atoms and quantum systems. ...
Introduction to Quantum Computation
Introduction to Quantum Computation

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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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