Optical and Magnetic Properties of Copper(II) compounds.
... strength and the covalency of the metal-ligand chemical bonds, the electronic g tensor and hyperfine coupling constants are parameters that are all strongly dependent on the coordination environment of the transition metal ion.11, 16 In particular, the EPR technique is quite selective in studies of a ...
... strength and the covalency of the metal-ligand chemical bonds, the electronic g tensor and hyperfine coupling constants are parameters that are all strongly dependent on the coordination environment of the transition metal ion.11, 16 In particular, the EPR technique is quite selective in studies of a ...
S–I–S its S–I transition C.D. , Kwangmoo Kim
... are substantial differences. For example, even though the order parameter decays exponentially into the I region, as in an S–N–S junction, our junction will behave more like an S–I–S junction since the non-superconducting region in isolation would be insulating at zero temperature. Also, the composi ...
... are substantial differences. For example, even though the order parameter decays exponentially into the I region, as in an S–N–S junction, our junction will behave more like an S–I–S junction since the non-superconducting region in isolation would be insulating at zero temperature. Also, the composi ...
Interacting Cold Rydberg Atoms: a Toy Many-Body
... from the simple underlying physical laws that govern the interactions between constituents of matter, like atoms or molecules. Interactions between particles are for the most part well-understood, and the equations of quantum mechanics governing an ensemble of interacting particles are known. Howeve ...
... from the simple underlying physical laws that govern the interactions between constituents of matter, like atoms or molecules. Interactions between particles are for the most part well-understood, and the equations of quantum mechanics governing an ensemble of interacting particles are known. Howeve ...
The Large D Limit of Planar Diagrams arXiv:1701.01171v1 [hep
... This being said, large N matrix quantum mechanical models remain a huge technical challenge, because we do not know how to perform the sum over planar diagrams in the most interesting cases. In a very recent development that has attracted a lot of attention, Kitaev and followers have shown that much ...
... This being said, large N matrix quantum mechanical models remain a huge technical challenge, because we do not know how to perform the sum over planar diagrams in the most interesting cases. In a very recent development that has attracted a lot of attention, Kitaev and followers have shown that much ...
Chapter 7 Quantum Theory of the Atom
... The first three define the wave function for a particular electron. The fourth quantum number refers to the magnetic property of electrons. Copyright © Cengage Learning. All rights reserved. ...
... The first three define the wave function for a particular electron. The fourth quantum number refers to the magnetic property of electrons. Copyright © Cengage Learning. All rights reserved. ...
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... de ay of the wave fun tion at large distan es, and it is this requirement that must hold in a QC. Throughout the paper we use the term \parti les" and \sites" for ex itations and qubits, respe tively. For 1D hains there is one-to-one mapping of the ex itations onto fermions via the Jordan-Wigner tr ...
... de ay of the wave fun tion at large distan es, and it is this requirement that must hold in a QC. Throughout the paper we use the term \parti les" and \sites" for ex itations and qubits, respe tively. For 1D hains there is one-to-one mapping of the ex itations onto fermions via the Jordan-Wigner tr ...
Scattering theory - Theory of Condensed Matter
... In general, an expansion then leads to a formidible collection of contributing terms. However, for most of these contributions, there remains an exponential factor, e±ikr(1−cos θ) where θ denotes the angle between k and r. For r → ∞, the small angular integration implied by any physical measurement ...
... In general, an expansion then leads to a formidible collection of contributing terms. However, for most of these contributions, there remains an exponential factor, e±ikr(1−cos θ) where θ denotes the angle between k and r. For r → ∞, the small angular integration implied by any physical measurement ...
Exploring dynamical phase transitions and prethermalization with
... infinite-range Ising model to demonstrate that our claims are insensitive to the precise choice of the model. A characterization in terms of traditional critical exponents would suggest that the dynamical transition of the O(N ) model is of the same universality as the corresponding thermal phase tr ...
... infinite-range Ising model to demonstrate that our claims are insensitive to the precise choice of the model. A characterization in terms of traditional critical exponents would suggest that the dynamical transition of the O(N ) model is of the same universality as the corresponding thermal phase tr ...
A classical analogue for adiabatic Stark splitting in non-hydrogenic atoms Robicheaux
... during each radial period. If the angular momentum is in the y-direction, the equation of motion dβ/dt = Ly /(mr2 ) can be used to show that over a radial period the change in angle of the Runge–Lenz vector is ...
... during each radial period. If the angular momentum is in the y-direction, the equation of motion dβ/dt = Ly /(mr2 ) can be used to show that over a radial period the change in angle of the Runge–Lenz vector is ...
Adiabatic State Preparation of Interacting Two-Level Systems R. T. Brierley, C. Creatore,
... interaction, J ¼ 0, all crossings occur simultaneously and so may all occur within the window. In the presence of interactions, eventually the time of the first level crossing, J=, approaches the temporal pulse width, , and it will be pushed out of the pulse. Neglecting the change in avoided cross ...
... interaction, J ¼ 0, all crossings occur simultaneously and so may all occur within the window. In the presence of interactions, eventually the time of the first level crossing, J=, approaches the temporal pulse width, , and it will be pushed out of the pulse. Neglecting the change in avoided cross ...
Density Functional Theory for Systems with Electronic Edges
... Our modern picture of what a material is, on the smallest scale, has its foundation in the early 20th century with the discovery of the atom and the development of quantum mechanics. This picture describes a material as consisting of electrons and atomic nuclei behaving according to the probabilisti ...
... Our modern picture of what a material is, on the smallest scale, has its foundation in the early 20th century with the discovery of the atom and the development of quantum mechanics. This picture describes a material as consisting of electrons and atomic nuclei behaving according to the probabilisti ...
