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Observations on Hyperplane: II. Dynamical Variables and
Observations on Hyperplane: II. Dynamical Variables and

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MODULE MAPS OVER LOCALLY COMPACT QUANTUM GROUPS

... Let G = (L∞ (G), Γ, ϕ, ψ) be a von Neumann algebraic locally compact quantum group and let L1 (G) be the convolution quantum group algebra of G. If we let C0 (G) be the reduced C ∗ -algebra associated with G, then its operator dual M (G) is a faithful completely contractive Banach algebra containing ...
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... Conventional combinational logic circuits are known to dissipate heat for every bit of information that is lost. This is also evident from the second law of thermodynamics which states that any irreversible process leads to loss of energy. Landauer [3] showed that any gate that is irreversible, nece ...
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What Makes a Classical Concept Classical? Toward a

... to Bohr’s words, and, at the same time, to make both physical and philosophical sense. At the heart of this reconstruction are proposals regarding both of the supposedly non-problematic issues: one regarding what it means to describe a system classically, and one regarding where a classical descript ...
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Elliptic Curve Cryptography and Quantum Computing

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Continuous Variable Quantum Information: Gaussian States and

... with a variety of quantum hardware, and entered a stage of commercial exploitation [6]. The time seems ripe for selected quantum computing devices to live up to their high expectations [7]. Traditionally, two main approaches to quantum information processing have been pursued. On one hand, a “digita ...
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Wick Rotation as a New Symmetry

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Toward the Unification of Physics and Number Theory

... freedom. This is in contrast to deterministic algorithms which also use a finite set of symbols and rules but have no degrees of freedom. We define symbol here as “an object that represents itself or something else”. And, finally, we define an object as “anything which can be thought of”. Fundamenta ...
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Sharp Tunneling Peaks in a Parametric Oscillator: Quantum Resonances Missing

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Introduction to Loop Quantum Gravity and Spin Foams

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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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