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Gate-defined quantum confinement in suspended bilayer graphene
Gate-defined quantum confinement in suspended bilayer graphene

... control because of its rich system of degeneracies that couple to externally applied fields. At B = 0, breaking layer inversion symmetry opens an energy gap tunable up to 250 meV with an external perpendicular electric field E (refs 19–25) that can be used for confinement. In devices with low disord ...
LAPLACE TRANSFORM AND UNIVERSAL sl2 INVARIANTS
LAPLACE TRANSFORM AND UNIVERSAL sl2 INVARIANTS

Quantum connection and Poincare19 e-
Quantum connection and Poincare19 e-

... The present paper is aimed at analysing some aspects of the general relativistic classical and quantum mechanics on a curved spacetime with absolute time, in terms of recent formulations of a finite order Lagrangian bicomplex [Kru90, Kru95] and of a covariant approach to classical and quantum mechan ...
Quantum Information Processing - LANL Research Library
Quantum Information Processing - LANL Research Library

Pure Wave Mechanics and the Very Idea of Empirical Adequacy
Pure Wave Mechanics and the Very Idea of Empirical Adequacy

Multipartite entanglement, quantum- error
Multipartite entanglement, quantum- error

... 12, 13, 14, 15, 16, 17], but the task at hand is generally considered a difficult one and may never be completed. We are thus lead to consider simple computable measures of entanglement [18, 19] that although cannot fully characterize the multipartite nature of the correlations, may nevertheless sti ...
Distance between quantum states in the presence of initial qubit
Distance between quantum states in the presence of initial qubit

Exponential Decay of Quantum Wave Functions
Exponential Decay of Quantum Wave Functions

... geodesic distance as a minimum action and then applied the theory of large deviations in path space to get lower bounds. This paper influence my tunnelling paper [42]. (VI) This paper, joint with Elliot Lieb, studied asymptotic behavior of N –body ground states in the special two cluster region wher ...
Document
Document

... The Photoelectric Effect These light quanta are called photons. • Einstein’s theory that light behaves as a stream of particles explains the photoelectric effect and many other observations. • Light behaves as waves in other situations; we must consider that light possesses both wavelike and particl ...
The Effect of Communication Costs in Solid
The Effect of Communication Costs in Solid

Document
Document

Measurement and assignment of the size-dependent
Measurement and assignment of the size-dependent

... study the evolution of electronic behavior in a size regime intermediate between the molecular and bulk limits of matter. Interesting and strongly size-dependent optical properties arise in these materials when the quantum dot is small compared to the natural length scale of the electron-hole pair, ...
An exponential separation between quantum and classical one
An exponential separation between quantum and classical one

SOME CONVEXITY AND SUBADDITIVITY
SOME CONVEXITY AND SUBADDITIVITY

Quantum Objects - Philsci
Quantum Objects - Philsci

... state vector. This interpretation, according to Maudlin’s analysis, must overcome the “Three Measurement Problems”: The problem of outcomes. In QM, we encounter with some weird superposition states, which are linear combination of some pure states. The problem associated with these superposition st ...
Earman, John, "Aspects of Determinism in Modern Physics"
Earman, John, "Aspects of Determinism in Modern Physics"

One-way quantum computing with arbitrarily large time
One-way quantum computing with arbitrarily large time

Single-Photon Bus between Spin-Wave Quantum Memories.
Single-Photon Bus between Spin-Wave Quantum Memories.

Quantum vs. Classical Magnetization Plateaus of S=1/2 Frustrated
Quantum vs. Classical Magnetization Plateaus of S=1/2 Frustrated

DISTANCE EDUCATION M.Sc. (Physics) DEGREE EXAMINATION
DISTANCE EDUCATION M.Sc. (Physics) DEGREE EXAMINATION

Logical error rate in the Pauli twirling approximation Amara Katabarwa
Logical error rate in the Pauli twirling approximation Amara Katabarwa

... Simulation of a noisy quantum circuit is accomplished by performing each ideal operation followed by an error (a gate from Pauli or Clifford group) with some probability. It is then necessary to construct an error channel such that one approximates the true noise process as accurately as possible (w ...
Evaluating charge noise acting on semiconductor quantum dots in
Evaluating charge noise acting on semiconductor quantum dots in

The Free Particle (PowerPoint)
The Free Particle (PowerPoint)

... The dual nature of matter (Quick Time movie 9 MB from Wilson group, *** ) Linear polarized light ( a wave function in 1-D would propagate in a similar way) (1 MB Quick time movie from the Wilson Group, *****) Circular polarized light ( ( a wave function could propagate in a similar way) (6 MB Quick ...
Quantum electrical transport in samples of limited
Quantum electrical transport in samples of limited

Time reversal and the symplectic symmetry of the electron spin.
Time reversal and the symplectic symmetry of the electron spin.

... and an absolutely minimal requirement for success is that the large N limit respects key physical symmetries. Here we show that two vital discrete symmetries of electrons, the inversion of spin under time reversal, and the neutrality of spins under particle-hole transformations, are violated in a la ...
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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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