particularized wave equations and their parameters
... which we called their cross-over group properties. They reflect periodicities in the proton-meson (and proton-proton) structure of the elements′ nuclei. Other, finer periodicities of the elements are revealed in the detailed structure of the Periodic table of the elements itself. (See its scheme in ...
... which we called their cross-over group properties. They reflect periodicities in the proton-meson (and proton-proton) structure of the elements′ nuclei. Other, finer periodicities of the elements are revealed in the detailed structure of the Periodic table of the elements itself. (See its scheme in ...
Electron-electron interactions in graphene field- Linköping University Post Print
... in quantum computing (qubits) is being explored [3]. With the discovery of graphene in 2004 [4], there was a new and interesting material for quantum dot fabrication. Graphene has several important features that make it different from conventional semiconductors: (i) its low-energy electrons behave ...
... in quantum computing (qubits) is being explored [3]. With the discovery of graphene in 2004 [4], there was a new and interesting material for quantum dot fabrication. Graphene has several important features that make it different from conventional semiconductors: (i) its low-energy electrons behave ...
Band-structure calculations of Fe1/3TaS2 and Mn1/3TaS2
... in Mn,/3TaS2for about 85%. This is due to electron transfer from the Mn atom to the Ta 5d,2 band. The mixing of S 3p states with Ta 5d is stronger than the mixing of S 3p with Mn 3d, because the radial extension of Ta 5d states is larger than that of Mn 3d states. The S 3s and S 3p bands show very l ...
... in Mn,/3TaS2for about 85%. This is due to electron transfer from the Mn atom to the Ta 5d,2 band. The mixing of S 3p states with Ta 5d is stronger than the mixing of S 3p with Mn 3d, because the radial extension of Ta 5d states is larger than that of Mn 3d states. The S 3s and S 3p bands show very l ...
Interactions of Particles in Matter
... dx is the thickness of a very thin section of the material and N is the number of scattering centres per unit volume. The cross section has the dimensions of a surface. In nuclear and particle physics, the commonly used units for the cross section are the barn and cm2 , with 1 barn = 10−24 cm2 . It ...
... dx is the thickness of a very thin section of the material and N is the number of scattering centres per unit volume. The cross section has the dimensions of a surface. In nuclear and particle physics, the commonly used units for the cross section are the barn and cm2 , with 1 barn = 10−24 cm2 . It ...
Charge density waves in low-dimensional metals
... lowers the reduction in energy associated with the CDW formation and eventually quenches the CDW at a critical temperature TCDW . Above that temperature the metallic state is stable. The charge density of the conduction band exhibits a periodic variation with the same wavevector q as the periodic la ...
... lowers the reduction in energy associated with the CDW formation and eventually quenches the CDW at a critical temperature TCDW . Above that temperature the metallic state is stable. The charge density of the conduction band exhibits a periodic variation with the same wavevector q as the periodic la ...
Density of states
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In solid-state and condensed matter physics, the density of states (DOS) of a system describes the number of states per interval of energy at each energy level that are available to be occupied. Unlike isolated systems, like atoms or molecules in gas phase, the density distributions are not discrete like a spectral density but continuous. A high DOS at a specific energy level means that there are many states available for occupation. A DOS of zero means that no states can be occupied at that energy level. In general a DOS is an average over the space and time domains occupied by the system. Localvariations, most often due to distortions of the original system, are often called local density of states (LDOS). If the DOS of an undisturbedsystem is zero, the LDOS can locally be non-zero due to the presence of a local potential.