Electron Transport in Single Molecule Transistors
... As the conductor gets smaller, several effects that are negligible in a macroscopic conductor become increasingly important. In a very small object such as nanostructures and molecules, electron transport usually does not follow Ohm’s law. There are several reasons why Ohm’s law fails at such exceed ...
... As the conductor gets smaller, several effects that are negligible in a macroscopic conductor become increasingly important. In a very small object such as nanostructures and molecules, electron transport usually does not follow Ohm’s law. There are several reasons why Ohm’s law fails at such exceed ...
Experimental scaling of fluctuations and confinement with Lundquist
... experimental strategy and the coverage of parameter space are described. The method of determining the Lundquist number from measured quantities is also explained, and careful attention is paid to determining the scaling of the classical resistivity. Measurement of the classical resistivity and its ...
... experimental strategy and the coverage of parameter space are described. The method of determining the Lundquist number from measured quantities is also explained, and careful attention is paid to determining the scaling of the classical resistivity. Measurement of the classical resistivity and its ...
New polyanion-based cathode materials for alkali
... Li3 Fe2(HPO3)3Cl, LiFe(HPO3)2, Li0.8 Fe(H2O)2B[P2O8]•H2O and AFePO4NO3 (A = NH4/Li, K). Furthermore, for each material the electrochemical performance for insertion of Li+ ion has been studied by means of various electrochemical techniques to reveal the nature of alkali ion insertion. In addition Na ...
... Li3 Fe2(HPO3)3Cl, LiFe(HPO3)2, Li0.8 Fe(H2O)2B[P2O8]•H2O and AFePO4NO3 (A = NH4/Li, K). Furthermore, for each material the electrochemical performance for insertion of Li+ ion has been studied by means of various electrochemical techniques to reveal the nature of alkali ion insertion. In addition Na ...
The Casimir force: background, experiments, and
... is absent, implying that the electromagnetic field is not coupling to matter in the usual sense. Perhaps this is stating the obvious, but the plates impose boundary conditions on the field and so their microscopic properties, in the limit of perfect conductivity, are not important. The role of c in ...
... is absent, implying that the electromagnetic field is not coupling to matter in the usual sense. Perhaps this is stating the obvious, but the plates impose boundary conditions on the field and so their microscopic properties, in the limit of perfect conductivity, are not important. The role of c in ...
Neutron Scattering—A Non-destructive Microscope for Seeing
... Fourier transform of the time-dependent correlation function. This general result provides a unified description of all neutron scattering experiments. By inverting Equation (2.8)—easier said than done in many cases—we can obtain from neutron scattering information about both the equilibrium structu ...
... Fourier transform of the time-dependent correlation function. This general result provides a unified description of all neutron scattering experiments. By inverting Equation (2.8)—easier said than done in many cases—we can obtain from neutron scattering information about both the equilibrium structu ...
The LDA+U Approach: A Simple Hubbard Correction - cond
... wave function are allowed to decrease their weight (e.g., in a variational calculation) while the distance between the fragments increases. This is only possible if the N-electron wave function is constructed as a linear combination of multiple Slater determinants. In other words, when electrons are ...
... wave function are allowed to decrease their weight (e.g., in a variational calculation) while the distance between the fragments increases. This is only possible if the N-electron wave function is constructed as a linear combination of multiple Slater determinants. In other words, when electrons are ...
ABINIT : first-principles approach to material and nanosystem
... The standard representation of DFT and GW A quantities within ABINIT relies on planewaves, see Chapter 12 and 13 of RM ES. An alternative representation is provided by a set of wavelets obtained with the BigDFT library, see Sec. 4.2. While very promising, the use of wavelets is not yet possible with ...
... The standard representation of DFT and GW A quantities within ABINIT relies on planewaves, see Chapter 12 and 13 of RM ES. An alternative representation is provided by a set of wavelets obtained with the BigDFT library, see Sec. 4.2. While very promising, the use of wavelets is not yet possible with ...
Statistical study of the location and size of the electron edge of the
... of interest, such that 3-D data was telemetered at a higher than usual rate from the spacecraft). The electron moments were averaged over 16 s in order to remove high-frequency variability and emphasize the main trends. There is some disagreement between the ion and electron moments: the plasma dens ...
... of interest, such that 3-D data was telemetered at a higher than usual rate from the spacecraft). The electron moments were averaged over 16 s in order to remove high-frequency variability and emphasize the main trends. There is some disagreement between the ion and electron moments: the plasma dens ...
Quantum State Engineering and Information Processing with
... By coupling the ion’s motional and electronic degrees of freeedom, we can engineer entanglement between these systems. This allows us to study quantum mechanics, with all its pecularities, in a well-controlled environment. For example, we can study the interactions of superposition states with the i ...
... By coupling the ion’s motional and electronic degrees of freeedom, we can engineer entanglement between these systems. This allows us to study quantum mechanics, with all its pecularities, in a well-controlled environment. For example, we can study the interactions of superposition states with the i ...
I Ceramic Material Classes - Wiley-VCH
... components of ceramic materials, or ternary compounds such as titanates or spinels, have been excluded at this stage. ...
... components of ceramic materials, or ternary compounds such as titanates or spinels, have been excluded at this stage. ...
006_Material properties - SAFIR manual - UEE
... interpolation is made for intermediate temperatures. The properties can be defined by the user as reversible, meaning that their values only depend on the current temperature, be it during heating or cooling; or as irreversible, in which case during cooling from a maximum temperature Tmax, the prope ...
... interpolation is made for intermediate temperatures. The properties can be defined by the user as reversible, meaning that their values only depend on the current temperature, be it during heating or cooling; or as irreversible, in which case during cooling from a maximum temperature Tmax, the prope ...
Dark current mechanisms in amorphous Selenium X
... The observation of impact ionization, which leads to avalanche multiplication on the amorphous selenium, has great impact on the low dose medical application such as general radiographic and fluoroscopic applications. However, the dark current can be high and very critical due to extremely high fie ...
... The observation of impact ionization, which leads to avalanche multiplication on the amorphous selenium, has great impact on the low dose medical application such as general radiographic and fluoroscopic applications. However, the dark current can be high and very critical due to extremely high fie ...
Lecture 5extra - web page for staff
... up to the Fermi energy level EF0 (Fermi level at 0 K). The energy require to excite an e- from the Fermi level to the vacuum level is called the work function of the metal. The probability of finding an electron at 0 K at some energy E < EF0 is unity, and at E > EF0 is zero. The electrons in the e ...
... up to the Fermi energy level EF0 (Fermi level at 0 K). The energy require to excite an e- from the Fermi level to the vacuum level is called the work function of the metal. The probability of finding an electron at 0 K at some energy E < EF0 is unity, and at E > EF0 is zero. The electrons in the e ...
and P- Doped Tin Oxide Nanowires - PDXScholar
... in recent years [1-3] as they provide interesting possibilities for resistance-less transport due to quantum effects. Varieties of synthetic methods have been utilized to synthesize 1D nanomaterials. A most common method is based on vapor-liquid-solid (VLS) mechanism that can be carried out in a che ...
... in recent years [1-3] as they provide interesting possibilities for resistance-less transport due to quantum effects. Varieties of synthetic methods have been utilized to synthesize 1D nanomaterials. A most common method is based on vapor-liquid-solid (VLS) mechanism that can be carried out in a che ...
Here - 21st International Conference on General Relativity and
... On the conditions for the formation of exotic compact objects from gravitational collapse (Daniele Malafarina) . . . . . . . . . . . . . . . . . Universal Walker metrics (Tomas Malek ) . . . . . . . . . . . . . . . . . . . The Cartan Algorithm in Higher Dimensions with Applications (David McNutt) . ...
... On the conditions for the formation of exotic compact objects from gravitational collapse (Daniele Malafarina) . . . . . . . . . . . . . . . . . Universal Walker metrics (Tomas Malek ) . . . . . . . . . . . . . . . . . . . The Cartan Algorithm in Higher Dimensions with Applications (David McNutt) . ...
Quadratic response theory for spin-orbit coupling in semiconductor
... effective-mass Hamiltonians describing spin-orbit coupling in semiconductors.2 These models have been under intensive study in the past several years due to theoretical and experimental advances in spin-related phenomena such as the intrinsic spin Hall effect3–17 and the spin galvanic and circular p ...
... effective-mass Hamiltonians describing spin-orbit coupling in semiconductors.2 These models have been under intensive study in the past several years due to theoretical and experimental advances in spin-related phenomena such as the intrinsic spin Hall effect3–17 and the spin galvanic and circular p ...
Condensed matter physics
Condensed matter physics is a branch of physics that deals with the physical properties of condensed phases of matter. Condensed matter physicists seek to understand the behavior of these phases by using physical laws. In particular, these include the laws of quantum mechanics, electromagnetism and statistical mechanics.The most familiar condensed phases are solids and liquids, while more exotic condensed phases include the superconducting phase exhibited by certain materials at low temperature, the ferromagnetic and antiferromagnetic phases of spins on atomic lattices, and the Bose–Einstein condensate found in cold atomic systems. The study of condensed matter physics involves measuring various material properties via experimental probes along with using techniques of theoretical physics to develop mathematical models that help in understanding physical behavior.The diversity of systems and phenomena available for study makes condensed matter physics the most active field of contemporary physics: one third of all American physicists identify themselves as condensed matter physicists, and the Division of Condensed Matter Physics is the largest division at the American Physical Society. The field overlaps with chemistry, materials science, and nanotechnology, and relates closely to atomic physics and biophysics. Theoretical condensed matter physics shares important concepts and techniques with theoretical particle and nuclear physics.A variety of topics in physics such as crystallography, metallurgy, elasticity, magnetism, etc., were treated as distinct areas, until the 1940s when they were grouped together as solid state physics. Around the 1960s, the study of physical properties of liquids was added to this list, forming the basis for the new, related specialty of condensed matter physics. According to physicist Phil Anderson, the term was coined by him and Volker Heine when they changed the name of their group at the Cavendish Laboratories, Cambridge from ""Solid state theory"" to ""Theory of Condensed Matter"" in 1967, as they felt it did not exclude their interests in the study of liquids, nuclear matter and so on. Although Anderson and Heine helped popularize the name ""condensed matter"", it had been present in Europe for some years, most prominently in the form of a journal published in English, French, and German by Springer-Verlag titled Physics of Condensed Matter, which was launched in 1963. The funding environment and Cold War politics of the 1960s and 1970s were also factors that lead some physicists to prefer the name ""condensed matter physics"", which emphasized the commonality of scientific problems encountered by physicists working on solids, liquids, plasmas, and other complex matter, over ""solid state physics"", which was often associated with the industrial applications of metals and semiconductors. The Bell Telephone Laboratories was one of the first institutes to conduct a research program in condensed matter physics.References to ""condensed"" state can be traced to earlier sources. For example, in the introduction to his 1947 ""Kinetic theory of liquids"" book, Yakov Frenkel proposed that ""The kinetic theory of liquids must accordingly be developed as a generalization and extension of the kinetic theory of solid bodies"". As a matter of fact, it would be more correct to unify them under the title of ""condensed bodies"".