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Impossibility of the Counterfactual Computation for All Possible
Impossibility of the Counterfactual Computation for All Possible

AntalyaQuantumComputingTutorial
AntalyaQuantumComputingTutorial

... Heisenberg uncertainty principle says we cannot determine both the position and the momentum of a quantum particle with arbitrary precision. In his Nobel prize lecture on December 11, 1954 Max Born says about this fundamental principle of Quantum Mechanics : ``... It shows that not only the determin ...
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... *Email: [email protected] In quantum many-body theory, all physical observables are described in terms of correlation functions between particle creation/annihilation operators. Measurement of such correlation functions can therefore be regarded as an operational solution to the quantum many-b ...
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... underlying physics of this era. Over the next decade, the inflationary era – perhaps 10−30 seconds after the Big Bang – will thus join nucleosynthesis (3 minutes) and recombination (380,000 years) as observational windows into the primordial universe. However, while the workings of recombination and ...
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... V1 V2 Since imaginary gravitational masses are equivalent to real gravitational masses then the equations of the Real Gravitational Interaction are also applied to the Imaginary Gravitational Interaction. However, due to imaginary gravitational mass, m g (imaginary ) , to be an imaginary quantity, i ...
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... between the Fermi Liquid theory, the BCS theory of superconductivity and the theory which is currently supposed to describe electron doped high-Tc superconductors at weak coupling. In chapter 2 we describe the aspects of the AdS/CFT correspondence that will be relevant throughout the reading of the ...
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... global time function, and the global sense of Laplacian determinism as defined above makes no sense.4 But if one global time function exists for a relativistic spacetime, then many exist. A poor choice of global time function can lead to the failure of Laplacian determinism on the above definition. Th ...
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... The magnets have to be good enough so that resonance phenomena do not occur. Non wanted magnetic field components (sextupolar, octupolar etc.) are comparable to 10-4 relative to the main component of a magnet (dipole in a bending magnet, quadrupole in a focussing magnet etc.). This is valid for LHC ...
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Propagator

In quantum mechanics and quantum field theory, the propagator gives the probability amplitude for a particle to travel from one place to another in a given time, or to travel with a certain energy and momentum. In Feynman diagrams, which calculate the rate of collisions in quantum field theory, virtual particles contribute their propagator to the rate of the scattering event described by the diagram. They also can be viewed as the inverse of the wave operator appropriate to the particle, and are therefore often called Green's functions.
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