![Introductory Quantum Optics Section 2. A laser driven two](http://s1.studyres.com/store/data/007273697_1-ed2ea90097de979036d91ca6820516e2-300x300.png)
Kondo Screening Cloud Around a Quantum Dot
... exact diagonalization (ED) and density matrix renormalization group (DMRG) techniques. These techniques are essentially exact and superior to the variational and mean field approaches used in previous studies. The calculations have been performed using fully parallelized programs on distributed SHAR ...
... exact diagonalization (ED) and density matrix renormalization group (DMRG) techniques. These techniques are essentially exact and superior to the variational and mean field approaches used in previous studies. The calculations have been performed using fully parallelized programs on distributed SHAR ...
Driven Problems in Quantum and Classical Mechanics with Floquet
... where P(t+T)=P(t) is a periodic function with the the same period T. Second order problems, ẍ = A(t)x can be rewritten as ...
... where P(t+T)=P(t) is a periodic function with the the same period T. Second order problems, ẍ = A(t)x can be rewritten as ...
A Variational Approach to the Schrödinger–Poisson System
... The aim of this paper is to try to corroborate the qualitative results suggested by the Fig. 1 with special attention on the attractive case with finite energy whose asymptotic analysis in time have not been discussed in the previous literature. Let us summarize the techniques used through this pape ...
... The aim of this paper is to try to corroborate the qualitative results suggested by the Fig. 1 with special attention on the attractive case with finite energy whose asymptotic analysis in time have not been discussed in the previous literature. Let us summarize the techniques used through this pape ...
- City Research Online
... deformation parameter β used in [2] by τ employed in [1]. It is well known that when given only a non-Hermitian Hamiltonian, the metric operator can not be uniquely determined. However, as argued in [1] with the specification of the observable X, which coincides in [2] and [1], the outcome is unique ...
... deformation parameter β used in [2] by τ employed in [1]. It is well known that when given only a non-Hermitian Hamiltonian, the metric operator can not be uniquely determined. However, as argued in [1] with the specification of the observable X, which coincides in [2] and [1], the outcome is unique ...
fulltext - DiVA portal
... 3 Quantum chemistry 3.1 The Schrödinger equation . . . . . . . . . . . . . . 3.1.1 Hamiltonian . . . . . . . . . . . . . . . . . . ...
... 3 Quantum chemistry 3.1 The Schrödinger equation . . . . . . . . . . . . . . 3.1.1 Hamiltonian . . . . . . . . . . . . . . . . . . ...
Thermodynamics of the high temperature Quark-Gluon - IPhT
... These are at present the unique tools allowing a detailed study of the transition region where various interesting phenomena are taking place, such as colour deconfinement or chiral symmetry restoration. In these lectures, we shall not consider this transition region, but focus rather on the high te ...
... These are at present the unique tools allowing a detailed study of the transition region where various interesting phenomena are taking place, such as colour deconfinement or chiral symmetry restoration. In these lectures, we shall not consider this transition region, but focus rather on the high te ...
Quadratic response theory for spin-orbit coupling in semiconductor
... is the prototype of a class of 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 t ...
... is the prototype of a class of 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 t ...
Deviations from exponential law and Van Hove`s “2t” limit
... The purpose of this paper is to consider the eects that arise when the coupling constant is small but nonvanishing. This will enable us to give general estimates for deviations from exponential behavior. The paper is organized as follows. We shall rst look, in Section 2, at a simple system: we sum ...
... The purpose of this paper is to consider the eects that arise when the coupling constant is small but nonvanishing. This will enable us to give general estimates for deviations from exponential behavior. The paper is organized as follows. We shall rst look, in Section 2, at a simple system: we sum ...
--Fundamental Problems and Application to Material Science-
... seek for a universal theory behind the quantum chaos. In §4, we derive a universal dynamical system from generic quantum systems whose Hamiltonians possess only a singl~ nonintegrability parameter. In § 5, a high-dimensional field theory is constructed, corresponding to adiabatic-ansatz induced eige ...
... seek for a universal theory behind the quantum chaos. In §4, we derive a universal dynamical system from generic quantum systems whose Hamiltonians possess only a singl~ nonintegrability parameter. In § 5, a high-dimensional field theory is constructed, corresponding to adiabatic-ansatz induced eige ...
GlueX Photon Beam Preparation
... Discrete Symmetries The discrete transformations discussed here have eigenvalues Oˆ | | 1,1 ...
... Discrete Symmetries The discrete transformations discussed here have eigenvalues Oˆ | | 1,1 ...
Bogolyubov transformation
... corresponds to the momentum transfer by k Commutation rules do not involve a - function, because the BK momentum is discrete, albeit quasi-continuous: ...
... corresponds to the momentum transfer by k Commutation rules do not involve a - function, because the BK momentum is discrete, albeit quasi-continuous: ...
Quantization of the Free Electromagnetic Field: Photons and
... oscillators, at a collection of different wavevectors and wave-polarizations. The knowledge of how to quantize simple harmonic oscillators greatly simplifies the EM field problem. In the end, we get to see how the basic quanta of the EM fields, which are called photons, are created and annihilated i ...
... oscillators, at a collection of different wavevectors and wave-polarizations. The knowledge of how to quantize simple harmonic oscillators greatly simplifies the EM field problem. In the end, we get to see how the basic quanta of the EM fields, which are called photons, are created and annihilated i ...