Atomic orbitals and their representation: Can 3-D
... Influenced by the interpretation of the Compton effect, the French Louis de Broglie suggested, in 1924, that the accepted wave-particle duality for photons could be extended to any moving particle which would then have a wavelength associated with it. The somewhat mysterious wave of de Broglie was t ...
... Influenced by the interpretation of the Compton effect, the French Louis de Broglie suggested, in 1924, that the accepted wave-particle duality for photons could be extended to any moving particle which would then have a wavelength associated with it. The somewhat mysterious wave of de Broglie was t ...
What is quantum unique ergodicity?
... sequence of probability measures |φj |2 converges in the weak-∗ sense to the uniform measure on B. The fully-fledged definition of QUE actually is more elaborate, and involves equidistribution not just in space but also in the momentum variables. This requires use of either the Bargmann transform or ...
... sequence of probability measures |φj |2 converges in the weak-∗ sense to the uniform measure on B. The fully-fledged definition of QUE actually is more elaborate, and involves equidistribution not just in space but also in the momentum variables. This requires use of either the Bargmann transform or ...
Quantum stochastic processes as models for state vector reduction
... stochastic rules in addition to the ordinary causal quantum dynamics. Such a quantumstochastic process (QSP) was first introduced long ago [18]. A general theory of QSP has recently been constructed [ 191 in terms of quantum-stochastic differential equations (QSDE). The underlying idea is that the s ...
... stochastic rules in addition to the ordinary causal quantum dynamics. Such a quantumstochastic process (QSP) was first introduced long ago [18]. A general theory of QSP has recently been constructed [ 191 in terms of quantum-stochastic differential equations (QSDE). The underlying idea is that the s ...
Quantum Random Walk via Classical Random Walk With Internal
... some probabilities. However, this model is not possible as it is easy to show that the sum of probabilities over all its possible positions will not be unitary. Fortunately, it is still possible to construct such a random quantum walk if an extra degree of freedom, e.g., the particle’s spin, is inco ...
... some probabilities. However, this model is not possible as it is easy to show that the sum of probabilities over all its possible positions will not be unitary. Fortunately, it is still possible to construct such a random quantum walk if an extra degree of freedom, e.g., the particle’s spin, is inco ...
Fault-Tolerant Quantum Computation and the Threshold Theorem
... for our purposes of getting the basic outline of fault-tolerance, the simpler model will be fine.) If the procedure is fault-tolerant, then for any of these procedures, the probability of the encoded operations failing is at most cp2 for some constant c. If pleq 1c , then we see that we will have de ...
... for our purposes of getting the basic outline of fault-tolerance, the simpler model will be fine.) If the procedure is fault-tolerant, then for any of these procedures, the probability of the encoded operations failing is at most cp2 for some constant c. If pleq 1c , then we see that we will have de ...
Individuality and Indiscernibility
... “x is two miles from y.” Consider a valuation that assigns one sphere to x and the other to y.1 On this valuation, the sentence (2) comes out false. Each sphere is not two miles from exactly those things that the other sphere is two miles from, for each sphere is two miles from the other and not two ...
... “x is two miles from y.” Consider a valuation that assigns one sphere to x and the other to y.1 On this valuation, the sentence (2) comes out false. Each sphere is not two miles from exactly those things that the other sphere is two miles from, for each sphere is two miles from the other and not two ...
On the minimum quantum dimension for a given quantum correlation
... The difficulties in physical realizations: ◦ Measurement disturbs states, cannot clone unknown information: error-correcting is hard, though possible ◦ Quantum states are fragile; memory is short ◦ The accuracy of quantum operations is limited ...
... The difficulties in physical realizations: ◦ Measurement disturbs states, cannot clone unknown information: error-correcting is hard, though possible ◦ Quantum states are fragile; memory is short ◦ The accuracy of quantum operations is limited ...
The classical electromagnetism as used nowadays is not the theory
... important sense incomplete. Without substantive additional assumptions concerning how charged particles are to be modelled, the theory cannot be understood as describing the behaviour of the particle-field system” (Frisch, 2005, p. 47). Basically we only have general rules from relativistic mechanic ...
... important sense incomplete. Without substantive additional assumptions concerning how charged particles are to be modelled, the theory cannot be understood as describing the behaviour of the particle-field system” (Frisch, 2005, p. 47). Basically we only have general rules from relativistic mechanic ...
L. Bell*, et. al., "THz emission by Quantum Beating in a Modulation
... = ! -4 "1/4u0e−u0, where u0 = 2eE / )hm$20, $0 is the classical frequency of the oscillator and we have taken mh = me for simplicity. For weak fields the oscillating dipole moment is thus proportional to electric field. A numerical simulation of our quantum well yields z31 / z21 * 0.5E / !1 kV/ cm". ...
... = ! -4 "1/4u0e−u0, where u0 = 2eE / )hm$20, $0 is the classical frequency of the oscillator and we have taken mh = me for simplicity. For weak fields the oscillating dipole moment is thus proportional to electric field. A numerical simulation of our quantum well yields z31 / z21 * 0.5E / !1 kV/ cm". ...
