On the Theory of Oxidation-Reduction Reactions
... the reacting particles. Therefore, the average configuration of the solvent in the activated complex cannot be an equilibrium one. (In this respect it differs from the large-overlap complex, as discussed in a later section.) The average configuration of the solvent in the activated complex must also ...
... the reacting particles. Therefore, the average configuration of the solvent in the activated complex cannot be an equilibrium one. (In this respect it differs from the large-overlap complex, as discussed in a later section.) The average configuration of the solvent in the activated complex must also ...
Scandium Nitride Thin Films for Thermoelectrics Sit Kerdsongpanya Licentiate Thesis No. 1559
... I have discovered that ScN has high power factor 2.5 mW/(mK2) at 800 K, due to low metalliclike electrical resistivity (∼3.0 µΩm) with retained relatively large Seebeck coefficient of -86 µV/K. The ScN thin films were grown by reactive dc magnetron sputtering from Sc targets. For ScN, X-ray diffract ...
... I have discovered that ScN has high power factor 2.5 mW/(mK2) at 800 K, due to low metalliclike electrical resistivity (∼3.0 µΩm) with retained relatively large Seebeck coefficient of -86 µV/K. The ScN thin films were grown by reactive dc magnetron sputtering from Sc targets. For ScN, X-ray diffract ...
Counterion Penetration and Effective Electrostatic Interactions in
... is that it encompasses the volume energy, which can be important for describing phase behavior [18, 21, 23–26]. Moreover, response theory can be straightforwardly generalized to incorporate nonlinear response, which entails both many-body effective interactions and corrections to the pair potential ...
... is that it encompasses the volume energy, which can be important for describing phase behavior [18, 21, 23–26]. Moreover, response theory can be straightforwardly generalized to incorporate nonlinear response, which entails both many-body effective interactions and corrections to the pair potential ...
Electron Cloud Dynamics in the CesrTA Wiggler
... synchrotron radiation from the beam hits the vacuum wall, when lost beam particles strike the wall, or by ionization by the beam of background gas. These “primary electrons” or "photoelectrons" can then produce secondary electrons upon impact with the chamber wall. Secondaries can also strike the wa ...
... synchrotron radiation from the beam hits the vacuum wall, when lost beam particles strike the wall, or by ionization by the beam of background gas. These “primary electrons” or "photoelectrons" can then produce secondary electrons upon impact with the chamber wall. Secondaries can also strike the wa ...
Nonresonant beat-wave excitation of relativistic plasma
... gas and mobile ions 关13兴 to model the growth and saturation of the beat wave-driven RPW and in particular to follow the phase relationship between the plasmon and the driver. We first illustrate the dephasing induced by plasma density inhomogeneities introduced by the ponderomotive force of the lase ...
... gas and mobile ions 关13兴 to model the growth and saturation of the beat wave-driven RPW and in particular to follow the phase relationship between the plasmon and the driver. We first illustrate the dephasing induced by plasma density inhomogeneities introduced by the ponderomotive force of the lase ...
Distribution of density along magnetospheric field lines
... lines; nevertheless, Gallagher et al. [2000] found that the sum of the H+ and He+ densities was roughly constant along field lines within the plasmasphere in the range LTRE = 3– 5RE for R > 2RE. [6] The field line dependence of mass density has also been investigated using the frequencies of toroida ...
... lines; nevertheless, Gallagher et al. [2000] found that the sum of the H+ and He+ densities was roughly constant along field lines within the plasmasphere in the range LTRE = 3– 5RE for R > 2RE. [6] The field line dependence of mass density has also been investigated using the frequencies of toroida ...
Seven years after the unexpected discovery of superconductivity in
... explains its mechanism was formulated. This theory, which is called “BCS” after its discoverers John Bardeen, Leon Cooper and Robert Schrieffer, is now firmly established, having celebrated its half-centenary a few years ago (see April 2011 pp18–22). The discovery of high-temperature cuprate superco ...
... explains its mechanism was formulated. This theory, which is called “BCS” after its discoverers John Bardeen, Leon Cooper and Robert Schrieffer, is now firmly established, having celebrated its half-centenary a few years ago (see April 2011 pp18–22). The discovery of high-temperature cuprate superco ...
Spin density waves in bilayer cold polar molecules
... extremely short-range and is labeled as the so-called contact interaction. Indeed, ultracold molecules offer a diverse scientific direction and promised application such as study of novel dynamics in the low-energy collisions, long-range collective quantum effects and quantum phase transitions, prec ...
... extremely short-range and is labeled as the so-called contact interaction. Indeed, ultracold molecules offer a diverse scientific direction and promised application such as study of novel dynamics in the low-energy collisions, long-range collective quantum effects and quantum phase transitions, prec ...
Homework Section 1
... conservative. Determine and write the electric potential in rectangular (cartesian) and cylindrical coordinates. Find E using both cartesian and cylindrical coordinates and show that the results are the same as in spherical coordinates. P(x, y) 33) Derive P(x,y) dx dxdy using method ...
... conservative. Determine and write the electric potential in rectangular (cartesian) and cylindrical coordinates. Find E using both cartesian and cylindrical coordinates and show that the results are the same as in spherical coordinates. P(x, y) 33) Derive P(x,y) dx dxdy using method ...
New features of ion acoustic waves in inhomogeneous and
... n(x0 , z1 ), n(x0 , z2 ) at the points A(x0 , z1 ) and B(x0 , z2 ) will no longer be the same. ii) In addition, because of opposite motion of electrons and ions due to the transverse electric field in x-direction, there will be excess of charge of one or another sign at every point for any z, and th ...
... n(x0 , z1 ), n(x0 , z2 ) at the points A(x0 , z1 ) and B(x0 , z2 ) will no longer be the same. ii) In addition, because of opposite motion of electrons and ions due to the transverse electric field in x-direction, there will be excess of charge of one or another sign at every point for any z, and th ...
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.