Perturbation theory for anisotropic dielectric interfaces, and
... There have been several previous approaches to rigorous treatment of interface perturbations in electromagnetism, where classic approaches for small ∆ε perturbations fail because of the field discontinuities [1, 8, 9, 10, 11, 12]. One approach that was applied successfully to boundaries between isot ...
... There have been several previous approaches to rigorous treatment of interface perturbations in electromagnetism, where classic approaches for small ∆ε perturbations fail because of the field discontinuities [1, 8, 9, 10, 11, 12]. One approach that was applied successfully to boundaries between isot ...
... within the lowest Landau level approximation. The free energy maps onto that of a strictly c-axis field, but with a reduced interlayer coupling. We use this result to calculate the tilt modulus C 44 of a vortex lattice and vortex liquid. The vortex contribution to C 44 can be expressed in terms of t ...
Von Neumann algebra automorphisms and time
... above can be seen as a special case of such a general relation. This observation opens the possibility of widely extending the application of the idea described above, and to relate this idea to powerful mathematical results on the one side, and to the thermal properties of accelerated states in qua ...
... above can be seen as a special case of such a general relation. This observation opens the possibility of widely extending the application of the idea described above, and to relate this idea to powerful mathematical results on the one side, and to the thermal properties of accelerated states in qua ...
Strong shock waves in a dense gas: Burnett theory versus Monte
... role of bath particles is to sample the conditions in the upstream and downstream domains, so that their velocity distributions are kept to be Maxwellians. At integer times t 5Dt,2Dt,3Dt, . . . , the positions $ x i % and velocities $ vi % are updated due to free streaming and collisions. In the fre ...
... role of bath particles is to sample the conditions in the upstream and downstream domains, so that their velocity distributions are kept to be Maxwellians. At integer times t 5Dt,2Dt,3Dt, . . . , the positions $ x i % and velocities $ vi % are updated due to free streaming and collisions. In the fre ...
gauge-like variables for ordered media containing defects - HAL
... analogy with the Higgs phenomenon in superconductors, where the scalar phase of the matter field becomes part of a vector field, through coupling to the electromagnetic field. This replacement procedure has two attractive features, and one may say that it has both kinematic appeal and dynamic appeal ...
... analogy with the Higgs phenomenon in superconductors, where the scalar phase of the matter field becomes part of a vector field, through coupling to the electromagnetic field. This replacement procedure has two attractive features, and one may say that it has both kinematic appeal and dynamic appeal ...
A G2-QCD neutron star
... At large radius the free neutron gas allows larger masses, than the interacting case, which leads to a steeper rise. Conversely, at a smaller radius, about 11 km, the rise for the interacting case becomes much quicker. This can be traced back to the baryon density shown in figure 1. The correspondin ...
... At large radius the free neutron gas allows larger masses, than the interacting case, which leads to a steeper rise. Conversely, at a smaller radius, about 11 km, the rise for the interacting case becomes much quicker. This can be traced back to the baryon density shown in figure 1. The correspondin ...
The Influence of Retardation on the London
... particles, they found a discrepancy between their theory and the experimental results which could be removed only by assuming that at large distances the attractive force between two atoms decreases more rapidly than R '. Overbeek then pointed out that on the basis of the picture customarily used fo ...
... particles, they found a discrepancy between their theory and the experimental results which could be removed only by assuming that at large distances the attractive force between two atoms decreases more rapidly than R '. Overbeek then pointed out that on the basis of the picture customarily used fo ...
Ground-state properties of the attractive one
... The results we find from the study of incremental groundstate wave-function overlaps give overwhelmimg support to the mean-field results, viz. the general existence of two transitional couplings. Within the context of mean-field theory the system exhibits a broken symmetry phase. Our meanfield resul ...
... The results we find from the study of incremental groundstate wave-function overlaps give overwhelmimg support to the mean-field results, viz. the general existence of two transitional couplings. Within the context of mean-field theory the system exhibits a broken symmetry phase. Our meanfield resul ...
Simple Theory of the Magnetic Properties of Rare
... sense a strongly repulsive "hard-core" interaction. The long-rRnge coupling between spins is R one-electx"on effect, i.e., a small hybridization of the shell and the conduction states caused by the lattice potential. The conduction-electron dispersion relation, which defines the "polarizability" of ...
... sense a strongly repulsive "hard-core" interaction. The long-rRnge coupling between spins is R one-electx"on effect, i.e., a small hybridization of the shell and the conduction states caused by the lattice potential. The conduction-electron dispersion relation, which defines the "polarizability" of ...
3.4 Faraday`s Law
... Fleming's right hand rule (for generators) Fleming's right hand rule shows the direction of induced current flow when a conductor moves in a magnetic field. The right hand is held with the thumb, first finger and second finger mutually at right angles, as shown in the diagram The Thumb represents t ...
... Fleming's right hand rule (for generators) Fleming's right hand rule shows the direction of induced current flow when a conductor moves in a magnetic field. The right hand is held with the thumb, first finger and second finger mutually at right angles, as shown in the diagram The Thumb represents t ...
Chapter 4: Crystal Lattice Dynamics
... At first glance, a theory of lattice vibrations would appear impossibly daunting. We have N ≈ 1023 ions interacting strongly (with energies of about (e2 /A)) with N electrons. However, there is a natural expansion parameter for this problem, which is the ratio of the electronic to the ...
... At first glance, a theory of lattice vibrations would appear impossibly daunting. We have N ≈ 1023 ions interacting strongly (with energies of about (e2 /A)) with N electrons. However, there is a natural expansion parameter for this problem, which is the ratio of the electronic to the ...
Studies of effective theories beyond the Standard Model
... computers have allowed for a tremendous evolution of the discipline. It should be emphasized that the aim and scope of physics never is to explain Nature, only to describe it. Once more, in the words of Feynman “While I am describing to you how Nature works, you won’t understand why Nature works tha ...
... computers have allowed for a tremendous evolution of the discipline. It should be emphasized that the aim and scope of physics never is to explain Nature, only to describe it. Once more, in the words of Feynman “While I am describing to you how Nature works, you won’t understand why Nature works tha ...
Quantum Field Theory - damtp
... We will review Dirac’s argument for anti-particles later in this course, together with the better understanding that we get from viewing particles in the framework of quantum field theory. For now, we’ll quickly sketch the circumstances in which we expect the number of particles to change. Consider ...
... We will review Dirac’s argument for anti-particles later in this course, together with the better understanding that we get from viewing particles in the framework of quantum field theory. For now, we’ll quickly sketch the circumstances in which we expect the number of particles to change. Consider ...
Superconducting phase qubit coupled to a nanomechanical resonator:
... we may increase the junction-resonator coupling g and still have an accurate state transfer from the Josephson junction to the resonator. As before, we start at time t = 0 in the state 兩10典. In order to define the fidelity of the state transfer operation, we first determine the time tmin of the mini ...
... we may increase the junction-resonator coupling g and still have an accurate state transfer from the Josephson junction to the resonator. As before, we start at time t = 0 in the state 兩10典. In order to define the fidelity of the state transfer operation, we first determine the time tmin of the mini ...
Local density of states in quantum Hall systems with a smooth
... We are in a nonperturbative regime at high magnetic fields (kinetic energy frozen + degeneracy of Landau levels) Smooth disorder (finite correlation length) Complexity of diagrammatrics at high magnetic fields (unsolved problem) ...
... We are in a nonperturbative regime at high magnetic fields (kinetic energy frozen + degeneracy of Landau levels) Smooth disorder (finite correlation length) Complexity of diagrammatrics at high magnetic fields (unsolved problem) ...
A Very Short Introduction to Quantum Field Theory
... they have no size; they are point-like objects. How, for example, can something with no size – spin? • If we regard the mass of a particle as fixed, then its interactions violate the laws of conservation of momentum and energy. In order to make this consistent with relativity, we say that these thin ...
... they have no size; they are point-like objects. How, for example, can something with no size – spin? • If we regard the mass of a particle as fixed, then its interactions violate the laws of conservation of momentum and energy. In order to make this consistent with relativity, we say that these thin ...
- Sussex Research Online
... high energy scales has intrigued physicists for many years [1]. There are hints that the renormalization group evolution of the coupling constants of the standard model of particle physics, or possibly of its supersymmetric version, causes them to unify at a large energy scale of order 1016 GeV [2]. ...
... high energy scales has intrigued physicists for many years [1]. There are hints that the renormalization group evolution of the coupling constants of the standard model of particle physics, or possibly of its supersymmetric version, causes them to unify at a large energy scale of order 1016 GeV [2]. ...
CONCEPTUAL FOUNDATIONS OF THE UNI- FIED THEORY OF WEAK AND ELECTROMAG-
... breakdown of the SU(2) x SU(2) symmetry would then split the Q and Al by something like the Higgs mechanism, but since the theory would not be gauge invariant the pions would remain as physical Goldstone bosons. This theory gave an intriguing result, that the Al/e mass ratio should be r/2, and in tr ...
... breakdown of the SU(2) x SU(2) symmetry would then split the Q and Al by something like the Higgs mechanism, but since the theory would not be gauge invariant the pions would remain as physical Goldstone bosons. This theory gave an intriguing result, that the Al/e mass ratio should be r/2, and in tr ...
ON THE EQUATIONAL THEORY OF PROJECTION LATTICES OF
... Lemma 2.2. An ortholattice identity t = 0 with m occurences of variables holds in a given atomic MOL L if any only if it holds in all sections [0, u] of L with dim u ≤ m. Proof. As usual, we write x for sequences (x1 , . . . , xn ) with n varying according to the context. We show by induction on com ...
... Lemma 2.2. An ortholattice identity t = 0 with m occurences of variables holds in a given atomic MOL L if any only if it holds in all sections [0, u] of L with dim u ≤ m. Proof. As usual, we write x for sequences (x1 , . . . , xn ) with n varying according to the context. We show by induction on com ...
PDF document
... where ε is the depth of the potential well and σ is the size parameter. These two parameters can be determined from experiments (see, for example, Tables I and II of Reference6). The first term in the square brackets has the right functional form for the dispersion interaction for large r values. Th ...
... where ε is the depth of the potential well and σ is the size parameter. These two parameters can be determined from experiments (see, for example, Tables I and II of Reference6). The first term in the square brackets has the right functional form for the dispersion interaction for large r values. Th ...
