physics and narrative - Rutgers Philosophy Department
... All of this is as easy as can be. And all of it has been taken note of, on a number different occasions, in the literature of the foundations of quantum mechanics. It was pointed to in a 1984 paper by Yakir Aharonov and myself - for example - and in a paper by Wayne Myrvold from 2002, and it must a ...
... All of this is as easy as can be. And all of it has been taken note of, on a number different occasions, in the literature of the foundations of quantum mechanics. It was pointed to in a 1984 paper by Yakir Aharonov and myself - for example - and in a paper by Wayne Myrvold from 2002, and it must a ...
Quantum information processing by nuclear magnetic resonance
... process information, but it seemed one would have little control over what information! This problem was circumvented by taking advantage of the very ensemble nature of the system which gave rise to it in the first place. Namely, we define a ‘‘pseudopure’’ ensemble to be one in which the sum of the ...
... process information, but it seemed one would have little control over what information! This problem was circumvented by taking advantage of the very ensemble nature of the system which gave rise to it in the first place. Namely, we define a ‘‘pseudopure’’ ensemble to be one in which the sum of the ...
Chirality quantum phase transition in the Dirac oscillator - E
... right-handed interactions. In Sec. III, we describe two limiting cases: a weak magnetic field regime where the system displays a remarkable left-handed chirality, and a strong magnetic field regime with an opposite right-handed chirality. For intermediate couplings, we obtain the complete energy spe ...
... right-handed interactions. In Sec. III, we describe two limiting cases: a weak magnetic field regime where the system displays a remarkable left-handed chirality, and a strong magnetic field regime with an opposite right-handed chirality. For intermediate couplings, we obtain the complete energy spe ...
Barad_On Touching--The Inhuman That Therefore I Am (v1.1)
... field theory, frames the difficulty in explicitly moral terms: “Instead of going directly from one point to another, the electron goes along for a while and suddenly emits a photon; then (horrors!) it absorbs its own photon. Perhaps there’s something ‘immoral’ about that, but the electron does it!” ...
... field theory, frames the difficulty in explicitly moral terms: “Instead of going directly from one point to another, the electron goes along for a while and suddenly emits a photon; then (horrors!) it absorbs its own photon. Perhaps there’s something ‘immoral’ about that, but the electron does it!” ...
Quantum NP - A Survey Dorit Aharonov and Tomer Naveh
... V , then outputs the majority. The existence of a witness for the new verifier in case x ∈ L is trivial since it is simply duplicate copies of the original witness. To prove soundness, one might suspect that entanglement between the provers can be used to bypass the fact that the error goes exponent ...
... V , then outputs the majority. The existence of a witness for the new verifier in case x ∈ L is trivial since it is simply duplicate copies of the original witness. To prove soundness, one might suspect that entanglement between the provers can be used to bypass the fact that the error goes exponent ...
Quantum Energy–based P Systems - Computational Biology and
... since rules are defined by unitary operators, they are logically reversible. This means that f is a permutation on the set An . ...
... since rules are defined by unitary operators, they are logically reversible. This means that f is a permutation on the set An . ...
How to solve Fokker-Planck equation treating mixed eigenvalue
... been limited to the Schrödinger potential with a discrete eigenvalue spectrum. Here, we will show how this approach can be also applied to a mixed eigenvalue spectrum with bounded and free states. We solve the FPE with boundaries located at x = ±L/2 and take the limit L → ∞, considering the examples ...
... been limited to the Schrödinger potential with a discrete eigenvalue spectrum. Here, we will show how this approach can be also applied to a mixed eigenvalue spectrum with bounded and free states. We solve the FPE with boundaries located at x = ±L/2 and take the limit L → ∞, considering the examples ...
Higher-order energy level spacing distributions in the transition
... In section 2 we will derive the general form of higher-order spacing distributions by solving an integral equation for Pk (x), which depends on the level-repulsion function only. As a special case we will propose a spacing distribution which corresponds to a power-law level-repulsion function. In se ...
... In section 2 we will derive the general form of higher-order spacing distributions by solving an integral equation for Pk (x), which depends on the level-repulsion function only. As a special case we will propose a spacing distribution which corresponds to a power-law level-repulsion function. In se ...
