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Commentary_Basti
Commentary_Basti

... our evolving universe. «Effects» are produced by «causes» not by «laws», which at last rule, and hence make pre-(retro-)dictable as to observers, the causal processes they rule. Hence, it is not «kinetics», as defining the geometrical laws of mechanics, but «dynamics», as defining the different type ...
Spontaneous four-wave mixing in microring resonators
Spontaneous four-wave mixing in microring resonators

Quantum Spacetime without Observers: Ontological
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Quantum Stabilizer Codes Embedding Qubits Into Qudits
Quantum Stabilizer Codes Embedding Qubits Into Qudits

Revealing novel quantum phases in quantum antiferromagnets on
Revealing novel quantum phases in quantum antiferromagnets on

Learning about order from noise Quantum noise studies of
Learning about order from noise Quantum noise studies of

A quantum logical and geometrical approach to the study of
A quantum logical and geometrical approach to the study of

... system兲 are in correspondence with closed subspaces of Hilbert space H. The set of subspaces C共H兲 with the partial order defined by set inclusion 債, intersection of subspaces 艚 as the lattice meet, closed linear spam of subspaces 丣 as the lattice join, and orthocomplementation ¬ as lattice complemen ...
God, Man, Chaos and Control: How God Might Control the
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Many-body systems

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Classical continuum theory of the dipole-forbidden collective excitations in quantum... W. L. Schaich M. R. Geller and G. Vignale

... grating as a flat 2D conductor whose ~local! resistivity varies periodically in the y direction. To enhance the signal strength and simplify the analysis, we assume that the single wire studied before has been periodically repeated in the y direction with the same period d.2W that the grating has. T ...
Strong no-go theorem for Gaussian quantum bit commitment
Strong no-go theorem for Gaussian quantum bit commitment

Adiabatic Geometric Phases and Response Functions
Adiabatic Geometric Phases and Response Functions

SUPERCONDUCTING QUBITS II: DECOHERENCE F.K. Wilhelm , M.J. Storcz and U. Hartmann
SUPERCONDUCTING QUBITS II: DECOHERENCE F.K. Wilhelm , M.J. Storcz and U. Hartmann

... which conserves entropy. Indeed, also the CPT theorem of relativistic quantum mechanics (Sakurai, 1967) states, that for each quantum system it is possible to find a counterpart (with inversed parity and charge) whose time arrow runs backwards. The apparent contradiction between microreversibility — ...
Partial Observation of Quantum Turing Machine and Weaker Well
Partial Observation of Quantum Turing Machine and Weaker Well

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Atomic Hong–Ou–Mandel experiment - HAL-IOGS

On Unitary Evolution in Quantum Field Theory in
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... hypersurfaces in a one-to-one correspondence, the associated quantum operator should be unitary. In a quantization context this comes from a one-to-one correspondence between classical solutions near the hypersurfaces. Such a correspondence occurs of course in the standard case of spacelike Cauchy h ...
Classical vs Quantum Information - UMD Math
Classical vs Quantum Information - UMD Math

... Bell’s locality argument Bell’s locality argument shows that if Alice and Bob are limited to classical resources, i.e., if they are required to reproduce the correlations on the basis of shared randomness or common causes established before they separate (after which no communication is allowed), th ...
Full Text - International Press of Boston
Full Text - International Press of Boston

... In particular, n1 = 1, n2 = 1, n3 = 12. This recursion formula for computing nd for CP2 was first derived by Kontsevich, using the composition law previously predicted by physicists and now proved in our paper [RT]. We can also compute the degree of the moduli space of genus g curves in CPn by using ...
From  Quantum  theory to Quantum  theology: Abstract J
From Quantum theory to Quantum theology: Abstract J

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Realism and Antirealism in Informational Foundations of

Gentzen-Like Methods in Quantum Logic*
Gentzen-Like Methods in Quantum Logic*

Measurement-based quantum computation with mechanical oscillators
Measurement-based quantum computation with mechanical oscillators

Linear optical controlled-NOT gate in the coincidence basis
Linear optical controlled-NOT gate in the coincidence basis

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Quantum teleportation



Quantum teleportation is a process by which quantum information (e.g. the exact state of an atom or photon) can be transmitted (exactly, in principle) from one location to another, with the help of classical communication and previously shared quantum entanglement between the sending and receiving location. Because it depends on classical communication, which can proceed no faster than the speed of light, it cannot be used for faster-than-light transport or communication of classical bits. It also cannot be used to make copies of a system, as this violates the no-cloning theorem. While it has proven possible to teleport one or more qubits of information between two (entangled) atoms, this has not yet been achieved between molecules or anything larger.Although the name is inspired by the teleportation commonly used in fiction, there is no relationship outside the name, because quantum teleportation concerns only the transfer of information. Quantum teleportation is not a form of transportation, but of communication; it provides a way of transporting a qubit from one location to another, without having to move a physical particle along with it.The seminal paper first expounding the idea was published by C. H. Bennett, G. Brassard, C. Crépeau, R. Jozsa, A. Peres and W. K. Wootters in 1993. Since then, quantum teleportation was first realized with single photons and later demonstrated with various material systems such as atoms, ions, electrons and superconducting circuits. The record distance for quantum teleportation is 143 km (89 mi).
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