Quantum Energy Teleportation - UWSpace
... In some sense the entropy is a measure of uncertainty in a random variable. Here is a rough sketch of how this concept applies to certain situations: say we have an alphabet X and for any given message there is a probability p(x) that a given letter X is x. Then, if we consider how one could optimal ...
... In some sense the entropy is a measure of uncertainty in a random variable. Here is a rough sketch of how this concept applies to certain situations: say we have an alphabet X and for any given message there is a probability p(x) that a given letter X is x. Then, if we consider how one could optimal ...
Clustered states in the fractional quantum Hall effect
... academic example, it included a description of the 21 state. What makes the Moore-Read state so special is its prediction of the low-energy excitations. Similar to the case of the Laughlin states, these excitation are predicted to carry a fractional charge. But the statistics they obey is a radical ...
... academic example, it included a description of the 21 state. What makes the Moore-Read state so special is its prediction of the low-energy excitations. Similar to the case of the Laughlin states, these excitation are predicted to carry a fractional charge. But the statistics they obey is a radical ...
Quantum heating of a parametrically modulated oscillator: Spectral signatures M. Marthaler,
... (1 + µ)1/2 ,P0 ≈ 0 from Eq. (4). The states are symmetrical, since they correspond to time translation by the modulation period, in the laboratory frame. The contributions to (ω) from fluctuations about the stable states are equal, and it is sufficient to study one of them. For concreteness, we wil ...
... (1 + µ)1/2 ,P0 ≈ 0 from Eq. (4). The states are symmetrical, since they correspond to time translation by the modulation period, in the laboratory frame. The contributions to (ω) from fluctuations about the stable states are equal, and it is sufficient to study one of them. For concreteness, we wil ...
Prime Factorization by Quantum Adiabatic Computation
... The last term in Eq. (2.1.12) was dropped because of the adiabatic assumption that H varies slowly. However if En − Em is also very small and/or H changes with a finite velocity it is not clear that this term can be ignored and the adiabatic theorem Eq. (2.1.16) might not be valid. Thus it is necess ...
... The last term in Eq. (2.1.12) was dropped because of the adiabatic assumption that H varies slowly. However if En − Em is also very small and/or H changes with a finite velocity it is not clear that this term can be ignored and the adiabatic theorem Eq. (2.1.16) might not be valid. Thus it is necess ...
On molecular origin of mass-independent fractionation of oxygen
... Eqs. 12 and 13 demonstrate that some metastable states may be more important for the recombination process than others due to higher weights wi . Energies and widths of scattering resonances, entering the numerator of Eq. 13, are the most important factors to consider. According to Eq. 13, very narr ...
... Eqs. 12 and 13 demonstrate that some metastable states may be more important for the recombination process than others due to higher weights wi . Energies and widths of scattering resonances, entering the numerator of Eq. 13, are the most important factors to consider. According to Eq. 13, very narr ...
Physics Today
... Although impressed with Bohr’s success, many contemporary scientists were offended by his blithe introduction of amenable postulates.1,3 Yet three of his key postulates were destined to become pervasive in quantum mechanics. Foremost was his concept of stationary states, although bereft of electron ...
... Although impressed with Bohr’s success, many contemporary scientists were offended by his blithe introduction of amenable postulates.1,3 Yet three of his key postulates were destined to become pervasive in quantum mechanics. Foremost was his concept of stationary states, although bereft of electron ...
Electrostatics - PRADEEP KSHETRAPAL PHYSICS
... (4) Dimension : [ML2 T 0 ] (5) S.I. unit : kgm2. (6) Moment of inertia depends on mass, distribution of mass and on the position of axis of rotation. (7) Moment of inertia does not depend on angular velocity, angular acceleration, torque, angular momentum and rotational kinetic energy. (8) It is not ...
... (4) Dimension : [ML2 T 0 ] (5) S.I. unit : kgm2. (6) Moment of inertia depends on mass, distribution of mass and on the position of axis of rotation. (7) Moment of inertia does not depend on angular velocity, angular acceleration, torque, angular momentum and rotational kinetic energy. (8) It is not ...
Unconditionally Secure Quantum Signatures
... lie, e.g., in what resources are needed or in exactly which parties have to be connected by what type of communication channels and in how many of, e.g., pairwise quantum channels are needed. All known information-theoretically secure “classical” signature schemes also use shared secret keys, which ...
... lie, e.g., in what resources are needed or in exactly which parties have to be connected by what type of communication channels and in how many of, e.g., pairwise quantum channels are needed. All known information-theoretically secure “classical” signature schemes also use shared secret keys, which ...
The Path Integral Approach to Quantum Mechanics
... x̂H (t)|x, t >= e (i/h̄)tĤ x̂e −(i/h̄)tĤ e (i/h̄)tĤ |x >= x|x, t > . ...
... x̂H (t)|x, t >= e (i/h̄)tĤ x̂e −(i/h̄)tĤ e (i/h̄)tĤ |x >= x|x, t > . ...
COMPUTING RAY CLASS GROUPS, CONDUCTORS AND
... Step 1. Computation of (1 + pa )/(1 + pb ) for a ≤ b ≤ 2a. Using Proposition 1.5 (2), we only need to compute pa /pb and the simplest way is probably as follows. Let p = pZK + πZK be a two-element representation of p, where we may assume π chosen so that vp (π) = 1 (if this is not the case, then vp ...
... Step 1. Computation of (1 + pa )/(1 + pb ) for a ≤ b ≤ 2a. Using Proposition 1.5 (2), we only need to compute pa /pb and the simplest way is probably as follows. Let p = pZK + πZK be a two-element representation of p, where we may assume π chosen so that vp (π) = 1 (if this is not the case, then vp ...
Solvation of electronically excited I2-
... While the weak field Hamiltonian does capture the essence of the model, its extension to include arbitrary electrostatic interactions requires matrix elements of the electrostatic interaction with respect to the many-electron eigenfunctions of isolated Ii. These eigenfunctions have a relatively comp ...
... While the weak field Hamiltonian does capture the essence of the model, its extension to include arbitrary electrostatic interactions requires matrix elements of the electrostatic interaction with respect to the many-electron eigenfunctions of isolated Ii. These eigenfunctions have a relatively comp ...
Computer simulation by quantum mechanical time dependent wave
... computer simulation. The present work emphasises this computer simulation method (CSM). For an actual CSM an appropriate experimental method at the detector region (TEAS) is required. Moreover a theoretical model for the TEAS (e.g. a one particle quantum mechanical wave packet model governed by the ...
... computer simulation. The present work emphasises this computer simulation method (CSM). For an actual CSM an appropriate experimental method at the detector region (TEAS) is required. Moreover a theoretical model for the TEAS (e.g. a one particle quantum mechanical wave packet model governed by the ...
