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Three-Level L-Type Atomic System Localized by the Parameters of
Three-Level L-Type Atomic System Localized by the Parameters of

... of parameters, we consider the atomic position probability distribution dependent different intensities of SGC (depicted by p). The position-dependent the intensities of SGC is shown in Figure 2, in which χ ′′ is plotted versus position x and y within the optical wavelength. The intensities of SGC a ...
Time Evolution of States for Open Quantum
Time Evolution of States for Open Quantum

Feshbach Resonances in Ultracold Gases
Feshbach Resonances in Ultracold Gases

... scattering between two particles when their incoming energies are very close to those of a two-particle bound state. Feshbach resonances were first applied to tune the interactions between ultracold Fermi gases in the late 1990’s. Here, we review two simple models of a Feshbach resonance: a spherica ...
Inserting Two Atoms into a Single Optical Micropotential
Inserting Two Atoms into a Single Optical Micropotential

... So far, these experiments were carried out with large samples of ultracold or quantum degenerate atoms, transferred into the motional ground state of optical lattices [9]. In combination with the high atomic densities, this results in excellent starting conditions for the above schemes, albeit at th ...
Deviations from exponential law and Van Hove`s “2t” limit
Deviations from exponential law and Van Hove`s “2t” limit

electric field effect on the binding energy of a non
electric field effect on the binding energy of a non

Problem Set 3: Bohr`s Atom Solution
Problem Set 3: Bohr`s Atom Solution

1. Conduction electrons in a metal: the free
1. Conduction electrons in a metal: the free

Semiclassical methods in solid state physics : two examples
Semiclassical methods in solid state physics : two examples

Lecture Notes in Statistical Mechanics and Mesoscopics
Lecture Notes in Statistical Mechanics and Mesoscopics

... Where the sum is for even or for odd values of l, therefore, if the particles are fermions or bozons. We’ll define ...
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Wave properties of particles
Wave properties of particles

Spatial entanglement in two-electron atomic systems
Spatial entanglement in two-electron atomic systems

First Principles Calculations of Off-Normal LEEM
First Principles Calculations of Off-Normal LEEM

... Our method: Find self-consistent potential and scattering states with DFT packages for solids  Introduce a supercell  Match incoming and outgoing plane waves to Bloch solutions at interfaces Quantum ESPRESSO (plane wave basis) Specular reflection only; lowest energy range Focus on Free-Standing Gr ...
Entanglement Measures for Single-and Multi
Entanglement Measures for Single-and Multi

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... resonances can be used to increase the collisional interactions and thereby speed up gate operations. However, the ‘unitarity limit’ in scattering theory does not allow the collisional interaction energy to be increased beyond the on-site vibrational oscillation frequency, so the lower timescale for ...
Chapter 3 MAGNETISM OF THE ELECTRON
Chapter 3 MAGNETISM OF THE ELECTRON

... The angular frequency ! c = 2 fc :Any component of the electron velocity parallel to the magnetic …eld is unin‡uenced by the Lorentz force, so the trajectory or the electron is a helix along the …eld direction. Electrons which follow cyclotron orbits radiate energy of frequency fc . The cyclotron fr ...
Scanning-probe spectroscopy of semiconductor donor molecules LETTERS
Scanning-probe spectroscopy of semiconductor donor molecules LETTERS

... V exc = 15 mV r.m.s. The local measurements consistently showed three broad peaks labelled A, B and C. b, Capacitance curves acquired at the same position as in a, but over the indicated expanded voltage range. To investigate the structure in detail, here we used a smaller excitation amplitude of 3. ...
Chapter 35 Bohr Theory of Hydrogen
Chapter 35 Bohr Theory of Hydrogen

Multiscale theory of finite-size Bose systems: Implications for collective
Multiscale theory of finite-size Bose systems: Implications for collective

... of others responding to the first兲. For identical quantum particles the latter quasiparticle excitations are not identifiable with a specific particle. In contrast to these global processes, short-scale ones reflect close encounters of particles related to the interparticle potential. For fermions, ...
MU08-CHAPTER6.doc
MU08-CHAPTER6.doc

... Fq= force on a single orbital particle me = the electron rest mass re = the classical electron radius c = light velocity in relative rest D = distance between charged particles Z = the number of charged particles in the core XXX The orbital electron moves with velocity vo. We suppose the velocity is ...
The role of chemical reactions in the laser destruction of transparent
The role of chemical reactions in the laser destruction of transparent

... not have a threshold for the onset of instability, for values of So that a r e too small the induction time becomes so long that for practicable durations of the action of the laser radiation the instability does not arise. In view of the exponential dependence of to on E and the absence of data on ...
Excited state entanglement - FaMAF
Excited state entanglement - FaMAF

Advancing Large Scale Many-Body QMC Simulations on GPU
Advancing Large Scale Many-Body QMC Simulations on GPU

Three-sublattice order in the SU (3) Heisenberg model on the
Three-sublattice order in the SU (3) Heisenberg model on the

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Tight binding

In solid-state physics, the tight-binding model (or TB model) is an approach to the calculation of electronic band structure using an approximate set of wave functions based upon superposition of wave functions for isolated atoms located at each atomic site. The method is closely related to the LCAO method used in chemistry. Tight-binding models are applied to a wide variety of solids. The model gives good qualitative results in many cases and can be combined with other models that give better results where the tight-binding model fails. Though the tight-binding model is a one-electron model, the model also provides a basis for more advanced calculations like the calculation of surface states and application to various kinds of many-body problem and quasiparticle calculations.
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