Stark effect of the hyperfine structure of ICl in its rovibronic ground
... can be investigated precisely at present. Therefore, the experimental data can verify and improve the theory, which makes it possible to precisely study the weak interactions of the nuclear spin and the nuclear electric quadruple moment with electrons surrounding. In addition, the external field eff ...
... can be investigated precisely at present. Therefore, the experimental data can verify and improve the theory, which makes it possible to precisely study the weak interactions of the nuclear spin and the nuclear electric quadruple moment with electrons surrounding. In addition, the external field eff ...
Measurability of Wilson loop operators
... Any permissible way in which a quantum state can change is described by a quantum operation, a completely positive trace-nonincreasing linear map of density operators to density operators 关3,4兴. The orthogonal measurement E in Eq. 共1兲, summed over its possible outcomes, is a special type of quantum ...
... Any permissible way in which a quantum state can change is described by a quantum operation, a completely positive trace-nonincreasing linear map of density operators to density operators 关3,4兴. The orthogonal measurement E in Eq. 共1兲, summed over its possible outcomes, is a special type of quantum ...
Chemical reaction rates using the semiclassical
... applied to a variety of condensed phase problems. However, this model has been shown to be an approximate version of the linearized IVR and thus cannot describe quantum interference effects beyond the short time limit. Another idea for evaluating the full semiclassical IVR 共SC-IVR兲 expression withou ...
... applied to a variety of condensed phase problems. However, this model has been shown to be an approximate version of the linearized IVR and thus cannot describe quantum interference effects beyond the short time limit. Another idea for evaluating the full semiclassical IVR 共SC-IVR兲 expression withou ...
Field-dependence of relaxation time distributions in rock samples V
... Cycling NMR Relaxometer produced by Stelar Srl. Pre-polarized (PP/S) and non-polarized (NP/S) acquisition sequences have been used with the following parameters: * 128 logarithmically distributed values (times in the relaxation field) ranging from 0.1 ms up to 4 s, * polarization field of 25 MHz, ...
... Cycling NMR Relaxometer produced by Stelar Srl. Pre-polarized (PP/S) and non-polarized (NP/S) acquisition sequences have been used with the following parameters: * 128 logarithmically distributed values (times in the relaxation field) ranging from 0.1 ms up to 4 s, * polarization field of 25 MHz, ...
Partial phase transition and quantum effects in helimagnetic
... spin in the i − th layer is determined by two parameters which are the angle with its NN in the adjacent plane, say αi,i+1 , and the azimuthal angle βi formed with the c axis. Since there is no competing interaction in the xy planes, spins in each plane are parallel. In this paper we use the steepes ...
... spin in the i − th layer is determined by two parameters which are the angle with its NN in the adjacent plane, say αi,i+1 , and the azimuthal angle βi formed with the c axis. Since there is no competing interaction in the xy planes, spins in each plane are parallel. In this paper we use the steepes ...
Quantum effects in energy and charge transfer in an
... where ωμν = E μ − E ν , and the heat-bath operator Aμν is defined in Eq. (7). Here, we use the fact that the Hamiltonian H in Eq. (6) is also expressed in terms of the operators ρμν taken at the same moment of time t. For two of these operators, ρμν (t) and ραβ (t), we have simple multiplication rul ...
... where ωμν = E μ − E ν , and the heat-bath operator Aμν is defined in Eq. (7). Here, we use the fact that the Hamiltonian H in Eq. (6) is also expressed in terms of the operators ρμν taken at the same moment of time t. For two of these operators, ρμν (t) and ραβ (t), we have simple multiplication rul ...
