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The 1925 Born and Jordan paper “On quantum mechanics”
The 1925 Born and Jordan paper “On quantum mechanics”

What is reality? - Brian Whitworth
What is reality? - Brian Whitworth

Quantum mechanics and path integrals
Quantum mechanics and path integrals

MATHEMATICS OF TOPOLOGICAL QUANTUM COMPUTING 1
MATHEMATICS OF TOPOLOGICAL QUANTUM COMPUTING 1

Machine invention of quantum computing circuits by means
Machine invention of quantum computing circuits by means

... here uses a simulator that runs on ordinary classical digital hardware. Such simulators are necessarily inefficient, in many cases they are exponentially costly in terms of time and space resources, but they allow us to determine how a quantum circuit would perform if it were implemented in real qua ...
Quantum Phenomena in Condensed Phase
Quantum Phenomena in Condensed Phase

... the quantum system density matrix that incorporates ideas from both methods yet maintains the ease of implementation of linearized methods. The method is based on a time stepping procedure arising from a Trotter factorization, combining the forward and backward incremental propagators, and treating ...
CS286.2 Lectures 5-6: Introduction to Hamiltonian Complexity, QMA
CS286.2 Lectures 5-6: Introduction to Hamiltonian Complexity, QMA

`universal` phase for electron transmission in quantum dots
`universal` phase for electron transmission in quantum dots

pdf - at www.arxiv.org.
pdf - at www.arxiv.org.

Single-electron computing: Quantum dot logic gates
Single-electron computing: Quantum dot logic gates

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PDF

bohr`s semiclassical model of the black hole
bohr`s semiclassical model of the black hole

Entropy is in Flux - James Franck Institute
Entropy is in Flux - James Franck Institute

Probability and Empirical Frequency
Probability and Empirical Frequency

On the equivalence between non-factorizable mixed
On the equivalence between non-factorizable mixed

Affine computation and affine automaton
Affine computation and affine automaton

Assessing the applicability of quantum corrections to classical
Assessing the applicability of quantum corrections to classical

Geometry of entangled states, Bloch spheres and Hopf fibrations R´emy Mosseri
Geometry of entangled states, Bloch spheres and Hopf fibrations R´emy Mosseri

... x3 = sin 2 Vj (Q ) = 2 Re(αδ − βγ ) x4 = sin 2 Vk (Q ) = 2 Im(αδ − βγ ) with sin 2 = 2|q1 q2 |. Q is the normalized image of the h1 map (Q = Q/ |Q|), S(Q ) and Vi,j,k (Q ) are, respectively, the scalar and vectorial parts of Q (see appendix). We recalled above that the X, Y and Z Bloch sp ...
QUANTUM COMPUTING WITH SUPERCONDUCTORS I: ARCHITECTURES Michael R. Geller Andrew T. Sornborger
QUANTUM COMPUTING WITH SUPERCONDUCTORS I: ARCHITECTURES Michael R. Geller Andrew T. Sornborger

... The modern era of superconducting quantum computation began in 2002. That year, the group of Siyuan Han at the University of Kansas and the group of John Martinis, then at NIST Boulder and currently at UC Santa Barbara, independently showed that long-lived quantum states in a current-biassed JJ can ...
Spin Hamiltonians and Exchange interactions
Spin Hamiltonians and Exchange interactions

Deriving new operator identities by alternately using normally
Deriving new operator identities by alternately using normally

A Factor-Graph Representation of Probabilities in Quantum Mechanics
A Factor-Graph Representation of Probabilities in Quantum Mechanics

Quantum Rotations: A Case Study in Static and Dynamic Machine
Quantum Rotations: A Case Study in Static and Dynamic Machine

Stability of Complex Biomolecular Structures: van der Waals
Stability of Complex Biomolecular Structures: van der Waals

353, 216 (2006) .
353, 216 (2006) .

... the exponential decay as the first one. Detail refer to the text. ...
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Quantum entanglement

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