A Theoretical Study of Charge Transport in Molecular Crystals Elham Mozafari
... we focus on the lattice deformation here. Such quasiparticles are termed electron(hole-) "Polaron"s, P − (P + ). Polarons can either be spatially extended, "large polaron" (Fröhlich polaron[Fröhlich 1954]), or localized in space, "small polaron" (Holstein polaron[Holstein 1959]). The general concept ...
... we focus on the lattice deformation here. Such quasiparticles are termed electron(hole-) "Polaron"s, P − (P + ). Polarons can either be spatially extended, "large polaron" (Fröhlich polaron[Fröhlich 1954]), or localized in space, "small polaron" (Holstein polaron[Holstein 1959]). The general concept ...
Inner-shell excitation of open-shell atoms - Shih
... energy is calculated directly from the single Slater determinant. For a multiplet state that cannot be represented by a single determinant, the energy can be calculated by means of Slater’s diagonal sum rule [10] from the single-Slater-determinant energies [9, 11]. Similar procedures have been emplo ...
... energy is calculated directly from the single Slater determinant. For a multiplet state that cannot be represented by a single determinant, the energy can be calculated by means of Slater’s diagonal sum rule [10] from the single-Slater-determinant energies [9, 11]. Similar procedures have been emplo ...
Magnetic Properties of the One-Band Hubbard Model
... Clearly, in order to obtain reliable results for lattice models from the DMFT, an accurate method is needed to solve the impurity problem. In particular, this method should be non-perturbative, so that all the different parameter regimes are accessible, and furthermore, it should work in the thermod ...
... Clearly, in order to obtain reliable results for lattice models from the DMFT, an accurate method is needed to solve the impurity problem. In particular, this method should be non-perturbative, so that all the different parameter regimes are accessible, and furthermore, it should work in the thermod ...
Communication: creation of molecular vibrational motions via the
... Hz). This frequency is off-resonant with respect to the ωHF = 4038 cm−1 vibrational frequency of HF and the duration of the IR pulse is similar to the vibrational period of HF (∼8.25 fs). Figure 3 shows the expectation value of the displacement R − R0 as a function of the intensity of the IR laser p ...
... Hz). This frequency is off-resonant with respect to the ωHF = 4038 cm−1 vibrational frequency of HF and the duration of the IR pulse is similar to the vibrational period of HF (∼8.25 fs). Figure 3 shows the expectation value of the displacement R − R0 as a function of the intensity of the IR laser p ...
RADIATION REACTION AND SELF-FORCE IN CURVED SPACETIME IN A FIELD THEORY APPROACH
... motion of relativistic particles and compact objects in an arbitrary curved spacetime from a field theory approach and depicts the quantum and stochastic (part I), semiclassical (parts I and II), and completely classical regimes (part III). In the semiclassical limit of an open quantum system descri ...
... motion of relativistic particles and compact objects in an arbitrary curved spacetime from a field theory approach and depicts the quantum and stochastic (part I), semiclassical (parts I and II), and completely classical regimes (part III). In the semiclassical limit of an open quantum system descri ...
Quantum electrodynamics of strong fields?
... of this process. If the vacuum is defined as a part of space free of real particles, this vacuum can be subject to certain conditions, like penetration by fields. If these fields become strong enough, the particle-free vacuum can no longer exist: it must contain real particles (in our special case s ...
... of this process. If the vacuum is defined as a part of space free of real particles, this vacuum can be subject to certain conditions, like penetration by fields. If these fields become strong enough, the particle-free vacuum can no longer exist: it must contain real particles (in our special case s ...
Square Van Atta Reflector with Conducting Mounting Plane
... have been calculat.ed, assuming that all elements not under consideration have been removed.This approximation has been tested by Davies [9] and may be expected to give good results when t.he spacing between the dipoles is as great as is the case for TTan h t t a reflectors, and t,he largest dimensi ...
... have been calculat.ed, assuming that all elements not under consideration have been removed.This approximation has been tested by Davies [9] and may be expected to give good results when t.he spacing between the dipoles is as great as is the case for TTan h t t a reflectors, and t,he largest dimensi ...
Mass hierarchy and physics beyond the Standard Theory
... exclusion : spin 2 and pseudoscalar at > ∼ 95% CL Agreement with Standard Model expectation at ∼ 2 σ I. Antoniadis (CERN) ...
... exclusion : spin 2 and pseudoscalar at > ∼ 95% CL Agreement with Standard Model expectation at ∼ 2 σ I. Antoniadis (CERN) ...
Quantum Mechanics from Self
... where the average is taken over a zbw period. This vector defines an instantaneous rest frame for the electron. In accordance with our assumptions above, we identify p as the total self-energy-momentum vector of the electron, and we have p2 = m2 c2 . In the absence of external fields, p is constant ...
... where the average is taken over a zbw period. This vector defines an instantaneous rest frame for the electron. In accordance with our assumptions above, we identify p as the total self-energy-momentum vector of the electron, and we have p2 = m2 c2 . In the absence of external fields, p is constant ...
Long Josephson junction in a resonant cavity * I. Tornes and D. Stroud
... other junctions. Thus, there is a long range interaction for which phase locking occurs when the coupling strength, multiplied by the junction number, exceeds a critical value. Several models have been developed to describe these steps.7–11 These models generally succeed in reproducing many of the s ...
... other junctions. Thus, there is a long range interaction for which phase locking occurs when the coupling strength, multiplied by the junction number, exceeds a critical value. Several models have been developed to describe these steps.7–11 These models generally succeed in reproducing many of the s ...
The Automorphic Universe
... set B ⊂ X we have µ(B) = 0 or µ(B) = 1. Equivalently, for any T −invariant (mod 0) set B ⊂ X we have µ(B) = 0 or µ(B) = 1. A T −invariant measure µ is ergodic iff any T − invariant function f : X → R is a.e. constant, i.e. µ(x : f (c) = c) = 1 for some c ∈ R. Equivalently, µ is ergodic iff any T −in ...
... set B ⊂ X we have µ(B) = 0 or µ(B) = 1. Equivalently, for any T −invariant (mod 0) set B ⊂ X we have µ(B) = 0 or µ(B) = 1. A T −invariant measure µ is ergodic iff any T − invariant function f : X → R is a.e. constant, i.e. µ(x : f (c) = c) = 1 for some c ∈ R. Equivalently, µ is ergodic iff any T −in ...
15. GRAND UNIFIED THEORIES 15. Grand Unified Theories 15.1. Grand Unification 1
... These are the problems which grand unified theories hope to address. 15.1.2. Charge Quantization : In the Standard Model, quarks and leptons are on an equal footing; both fundamental particles without substructure. It is now clear that they may be two faces of the same coin; unified, for example, by e ...
... These are the problems which grand unified theories hope to address. 15.1.2. Charge Quantization : In the Standard Model, quarks and leptons are on an equal footing; both fundamental particles without substructure. It is now clear that they may be two faces of the same coin; unified, for example, by e ...
A Dissertation entitled Quantum Theory of Ion
... on the analytic solutions for the long-range, −1/R4 , polarization potential. Ion-atom interactions, especially at cold temperatures of a few kelvin or lower, are complicated by the rapid energy variations induced by the long-range polarization potential, by the generally large number of contributin ...
... on the analytic solutions for the long-range, −1/R4 , polarization potential. Ion-atom interactions, especially at cold temperatures of a few kelvin or lower, are complicated by the rapid energy variations induced by the long-range polarization potential, by the generally large number of contributin ...
Quantum theory of ion-atom interactions
... on the analytic solutions for the long-range, −1/R4 , polarization potential. Ion-atom interactions, especially at cold temperatures of a few kelvin or lower, are complicated by the rapid energy variations induced by the long-range polarization potential, by the generally large number of contributin ...
... on the analytic solutions for the long-range, −1/R4 , polarization potential. Ion-atom interactions, especially at cold temperatures of a few kelvin or lower, are complicated by the rapid energy variations induced by the long-range polarization potential, by the generally large number of contributin ...
Exact M-Theory Solutions, Integrable Systems, eralgebras ?
... The radii of the anti-de-Sitter space AdS3 and of the spheres S 3 are functions of the twodimensional Riemann surface Σ, so that the product n with Σ is warped. The construction of [16] proceeds by reducing the BPS equations of 11-dimensional supergravity to the spacetime (1.1), and then mapping the ...
... The radii of the anti-de-Sitter space AdS3 and of the spheres S 3 are functions of the twodimensional Riemann surface Σ, so that the product n with Σ is warped. The construction of [16] proceeds by reducing the BPS equations of 11-dimensional supergravity to the spacetime (1.1), and then mapping the ...
NOT EVEN WRONG tells a fascinating and complex story about
... T h i s book is an attempt to come to terms with this question from a very particular point of view. T h i s point of view is a little bit unusual, so I'll begin with some personal history. My earliest memories of being concerned with the issues to be discussed in this book go back to the first year ...
... T h i s book is an attempt to come to terms with this question from a very particular point of view. T h i s point of view is a little bit unusual, so I'll begin with some personal history. My earliest memories of being concerned with the issues to be discussed in this book go back to the first year ...
Phenomenology of Higgs Bosons Beyond the Standard Model
... where i = 1, 2, 3 is the color index of the quark. The terms inside the large parenthesis in (2.11) make up the covariant derivative Dμi j , and Aaμ are the gauge fields which are called gluons and there are 8 of them. This theory, where the fields Ψi are transformed into a linear combination of thems ...
... where i = 1, 2, 3 is the color index of the quark. The terms inside the large parenthesis in (2.11) make up the covariant derivative Dμi j , and Aaμ are the gauge fields which are called gluons and there are 8 of them. This theory, where the fields Ψi are transformed into a linear combination of thems ...
ElectroGravitics_01
... Digital Equipment Corp's Alta Vista web search engine (note: If you can't find it with this, it ain't out ...
... Digital Equipment Corp's Alta Vista web search engine (note: If you can't find it with this, it ain't out ...
Linear and non-linear response phenomena of molecular systems
... the same type of perturbation, but this does not have to be the case, we might as well look at the magnetic field induced by an electric field or other kind of mixed responses. It is important to notice that, from the theoretical point of view we do not make a distinction between applied and observe ...
... the same type of perturbation, but this does not have to be the case, we might as well look at the magnetic field induced by an electric field or other kind of mixed responses. It is important to notice that, from the theoretical point of view we do not make a distinction between applied and observe ...