Gravitational Quantum States of Neutrons and the New GRANIT
... gravitational quantum states of matter were first observed in a series of experiments15–18 at the Institut Laue-Langevin3 (ILL). Overviews of these experiments and of physics relevant to this observation could be found, for instance, in Refs. 19 and 20. Serious efforts are devoted to confirm this ob ...
... gravitational quantum states of matter were first observed in a series of experiments15–18 at the Institut Laue-Langevin3 (ILL). Overviews of these experiments and of physics relevant to this observation could be found, for instance, in Refs. 19 and 20. Serious efforts are devoted to confirm this ob ...
Is a random state entangled ?
... While the “curse of dimensionality” makes numerical method impractical, high dimensions usually boost random techniques (“blessom of dimensionality”). In QIT, the probabilistic method has been applied successfully by Hastings (counterexample to the additivity conjecture). An important pioneering wor ...
... While the “curse of dimensionality” makes numerical method impractical, high dimensions usually boost random techniques (“blessom of dimensionality”). In QIT, the probabilistic method has been applied successfully by Hastings (counterexample to the additivity conjecture). An important pioneering wor ...
PPT
... theory is at variance with standard quantum mechanics, but the two are indistinguishable in observational respect. “Testability” militates against Bohm’s theory. The historical fact is that the scientific community does not rest undecided, wavering helplessly between different Duhem-Quine options. T ...
... theory is at variance with standard quantum mechanics, but the two are indistinguishable in observational respect. “Testability” militates against Bohm’s theory. The historical fact is that the scientific community does not rest undecided, wavering helplessly between different Duhem-Quine options. T ...
Quantum boolean functions - Chicago Journal of Theoretical
... This paper draws heavily on the classical field of the analysis of boolean functions, which for our purposes essentially began with the seminal paper of Kahn, Kalai and Linial [KKL88], which proved that every balanced boolean function must have an influential variable (see Section 10). Since then, a ...
... This paper draws heavily on the classical field of the analysis of boolean functions, which for our purposes essentially began with the seminal paper of Kahn, Kalai and Linial [KKL88], which proved that every balanced boolean function must have an influential variable (see Section 10). Since then, a ...
Chapter 3 Foundations II: Measurement and Evolution 3.1
... by turning on a coupling between that observable and a “pointer” variable that will serve as the apparatus. The coupling establishes entanglement between the eigenstates of the observable and the distinguishable states of the pointer, so that we can prepare an eigenstate of the observable by “observ ...
... by turning on a coupling between that observable and a “pointer” variable that will serve as the apparatus. The coupling establishes entanglement between the eigenstates of the observable and the distinguishable states of the pointer, so that we can prepare an eigenstate of the observable by “observ ...
Robust dynamical decoupling for quantum computing and quantum
... duty cycle (total irradiation time divided by total time). The relaxation times are defined as the 1/e decay time of the magnetization. In the first set of experiments, Fig. 4, we compare different members of the XY family. The sequences were constructed, as explained in [20], using the standard def ...
... duty cycle (total irradiation time divided by total time). The relaxation times are defined as the 1/e decay time of the magnetization. In the first set of experiments, Fig. 4, we compare different members of the XY family. The sequences were constructed, as explained in [20], using the standard def ...
IEEE Transactions on Magnetics
... entangled? Of course we can, since we still don’t know where the black or white pieces are located. Therefore, the states are still completely entangled, and as a consequence, non-locality emerges. Einstein found it very disturbing to consider that a measurement of one of the entangled states in one ...
... entangled? Of course we can, since we still don’t know where the black or white pieces are located. Therefore, the states are still completely entangled, and as a consequence, non-locality emerges. Einstein found it very disturbing to consider that a measurement of one of the entangled states in one ...
Unified treatment of quantum coherent and incoherent hopping
... the environmental degrees of freedom. The most commonly used theory from this approach is the Redfield equation,15–18 which is based on second-order perturbative truncation with respect to electron-environment interaction and the Markov approximation. In photosynthetic EET, each site of a multichrom ...
... the environmental degrees of freedom. The most commonly used theory from this approach is the Redfield equation,15–18 which is based on second-order perturbative truncation with respect to electron-environment interaction and the Markov approximation. In photosynthetic EET, each site of a multichrom ...
Classical analogy of Fano resonances
... already decayed) and the displacement x1 is eventually π out of phase with respect to the external force. Next, as the frequency passes through the anti-resonance at ω = ωzero , the phase of the oscillator drops by π abruptly. Finally, when the frequency sweeps through the second resonance, the osci ...
... already decayed) and the displacement x1 is eventually π out of phase with respect to the external force. Next, as the frequency passes through the anti-resonance at ω = ωzero , the phase of the oscillator drops by π abruptly. Finally, when the frequency sweeps through the second resonance, the osci ...
Nature physics
... exist. Intriguingly, we found the timescale for the many-body system to switch from a Mott insulating state to a superfluid state to be of the order of a few tunnelling time constants3, which is remarkable considering the huge rearrangement of the system. Indeed, the dynamical evolution of the quant ...
... exist. Intriguingly, we found the timescale for the many-body system to switch from a Mott insulating state to a superfluid state to be of the order of a few tunnelling time constants3, which is remarkable considering the huge rearrangement of the system. Indeed, the dynamical evolution of the quant ...
On inelastic hydrogen atom collisions in stellar atmospheres
... and extensions of the classical formula for ionization of atoms by electron impact due to Thomson (1912). In Thomson’s theory, the bound electron in the target atom is considered as a stationary free classical electron. The Coulomb interaction of an incident classical electron with the atomic electr ...
... and extensions of the classical formula for ionization of atoms by electron impact due to Thomson (1912). In Thomson’s theory, the bound electron in the target atom is considered as a stationary free classical electron. The Coulomb interaction of an incident classical electron with the atomic electr ...
metal
... 2. What is the distribution of the non-equilibrium steady state? Quantum random walk, suppression of tunneling ...
... 2. What is the distribution of the non-equilibrium steady state? Quantum random walk, suppression of tunneling ...