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Lorentz

The source is brought to a. positive poteptial (I/) of several kilovolts and the ions are extracted by a plate at ground potential. They acquire kinetic energy and thus velocity according to their mass and charge. They enter a magnetic field whose direction is perpendicular to their trajectory. Under the effect of the field, Bg, the trajectory is curved by Lorentz forces that produce a centripetal acceleration perpendicular to both the field and the velocity. [Pg.47]

The parameters in simple potential models for interactions between unlike molecules A and B are often deduced from tlie corresponding parameters for the A-A and B-B interactions using combination mles . For example, the a and e parameters are often estimated from the Lorentz-Berthelot mles ... [Pg.205]

In order to illustrate some of the basic aspects of the nonlinear optical response of materials, we first discuss the anliannonic oscillator model. This treatment may be viewed as the extension of the classical Lorentz model of the response of an atom or molecule to include nonlinear effects. In such models, the medium is treated as a collection of electrons bound about ion cores. Under the influence of the electric field associated with an optical wave, the ion cores move in the direction of the applied field, while the electrons are displaced in the opposite direction. These motions induce an oscillating dipole moment, which then couples back to the radiation fields. Since the ions are significantly more massive than the electrons, their motion is of secondary importance for optical frequencies and is neglected. [Pg.1266]

While the Lorentz model only allows for a restoring force that is linear in the displacement of an electron from its equilibrium position, the anliannonic oscillator model includes the more general case of a force that varies in a nonlinear fashion with displacement. This is relevant when tire displacement of the electron becomes significant under strong drivmg fields, the regime of nonlinear optics. Treating this problem in one dimension, we may write an appropriate classical equation of motion for the displacement, v, of the electron from equilibrium as... [Pg.1266]

The scattered intensity measured from the isotropic three-dimensional object can be transfonned to the onedimensional mtensity fiinction/j(<3 ) by means of the Lorentz correction [15]... [Pg.1406]

The molecular refractivity can be computed from the Lorenz and Lorentz equation ... [Pg.1034]

The specific refraction r is given by the Lorentz and Lorenz equation. [Pg.494]

Transmission Electron Microscopy Transmission Electron Microscope Conventional Transmission Electron Microscopy Scannir Transmission Electron Microscopy High Resolution Transmission Electron Microscopy Selected Area Diffraction Analytical Elearon Microscopy Convergent Beam Elearon DifFraaion Lorentz Transmission Electron Microscopy... [Pg.769]

Magnetic Sector Field. In a magnetic field B an ion with the velocity v and the charge q experiences a centripetal force, the Lorentz force P ... [Pg.109]

We now want to study the consequences of such a model with respect to the optical properties of a composite medium. For such a purpose, we will consider the phenomenological Lorentz-Drude model, based on the classical dispersion theory, in order to describe qualitatively the various components [20]. Therefore, a Drude term defined by the plasma frequency and scattering rate, will describe the optical response of the bulk metal or will define the intrinsic metallic properties (i.e., Zm((a) in Eq.(6)) of the small particles, while a harmonic Lorentz oscillator, defined by the resonance frequency, the damping and the mode strength parameters, will describe the insulating host (i.e., /((0) in Eq.(6)). [Pg.97]

Fig. 7. Model calculations for the reflectivity (a) and the optical conductivity (b) for a simple (bulk) Drude metal and an effective medium of small metallic spherical particles in a dielectric host within the MG approach. The (bulk) Drude and the metallic particles are defined by the same parameters set the plasma frequency = 2 eV, the scattering rate hr = 0.2 eV. A filling factor/ = 0.5 and a dielectric host-medium represented by a Lorentz harmonic oscillator with mode strength fttOy, 1 = 10 eV, damping ftF] = I eV and resonance frequency h(H = 15 eV were considered for the calculations. Fig. 7. Model calculations for the reflectivity (a) and the optical conductivity (b) for a simple (bulk) Drude metal and an effective medium of small metallic spherical particles in a dielectric host within the MG approach. The (bulk) Drude and the metallic particles are defined by the same parameters set the plasma frequency = 2 eV, the scattering rate hr = 0.2 eV. A filling factor/ = 0.5 and a dielectric host-medium represented by a Lorentz harmonic oscillator with mode strength fttOy, 1 = 10 eV, damping ftF] = I eV and resonance frequency h(H = 15 eV were considered for the calculations.
The molar refraction, / m, is a measure of the size of a molecule. It is calculated with Eq. (8.5), the Lorenz-Lorentz equation, where , d, and M are the refractive index, the density, and the molecular weight, respectively. [Pg.389]

It gets worse with magnetic properties, and the Lorentz force... [Pg.21]


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Broadening Lorentz

Classification of Lorentz Transformations

Clausius-Mosotti-Lorentz equation

Clausius-Mossotti/Lorentz-Lorenz

Clausius-Mossotti/Lorentz-Lorenz model

Complex Lorentz function

Definition of General Lorentz Transformations

Dielectric Lorentz model

Dirac Lorentz covariance

Dirac equation Lorentz invariance

Dirac-Lorentz

Dispersion model Lorentz

Distribution Lorentz

Drude-Lorentz theory

Einsteins Relativity Principle and Lorentz Transformations

Electric Lorentz

FitzGerald Lorentz contraction

Force electromagnetic (Lorentz

Four-vector Lorentz transformation

General Lorentz Boost

Generalized Lorentz-Lorenz law

H. A. Lorentz

Hard-disk Lorentz gas

Inverse Lorentz Transformation

Line profile Lorentz

Lorentz Antoon

Lorentz Berthelot rule

Lorentz Boost in One Direction

Lorentz Committee

Lorentz Lorenz

Lorentz Lorenz correction

Lorentz Lorenz relation

Lorentz Zeeman effect)

Lorentz and Lorenz equation

Lorentz and polarisation factors

Lorentz approximation

Lorentz band

Lorentz band shape

Lorentz boost

Lorentz cavity

Lorentz condition

Lorentz constant

Lorentz contraction

Lorentz correction

Lorentz correction factor

Lorentz covariance

Lorentz covariant 4-vector

Lorentz different

Lorentz electron model

Lorentz electron theory

Lorentz electronic theory

Lorentz equation

Lorentz equations corrections

Lorentz equations elements

Lorentz equations relativity theory

Lorentz factor

Lorentz field

Lorentz field Matrices

Lorentz field polarization

Lorentz force

Lorentz force electromagnetic field

Lorentz force equation

Lorentz force law

Lorentz function

Lorentz gas

Lorentz gas model

Lorentz gauge

Lorentz gauge condition

Lorentz geometric

Lorentz group

Lorentz homogeneous

Lorentz inhomogeneous

Lorentz interaction

Lorentz invariant

Lorentz lemma

Lorentz lemma and reciprocity relations

Lorentz lenses

Lorentz line

Lorentz line broadening

Lorentz line shape

Lorentz local field

Lorentz local field correction

Lorentz local field theory

Lorentz mean

Lorentz microscopy

Lorentz model

Lorentz model, application

Lorentz number

Lorentz oscillator

Lorentz oscillator model

Lorentz polarization

Lorentz profile

Lorentz proper

Lorentz radius

Lorentz representation

Lorentz rule

Lorentz shape

Lorentz shape signal

Lorentz shift

Lorentz structure tensor

Lorentz symmetric regauging

Lorentz tensor

Lorentz theory

Lorentz transformation

Lorentz transformation electrodynamics

Lorentz transformation general

Lorentz transformation operator

Lorentz transformation principles

Lorentz transformation special relativity

Lorentz transformation theory

Lorentz triplet

Lorentz uniqueness

Lorentz velocity)

Lorentz weight

Lorentz, Hendrik

Lorentz, Hendrik Antoon

Lorentz-Berthelot combination

Lorentz-Berthelot combination rules

Lorentz-Berthelot combining rules

Lorentz-Berthelot mixing rules

Lorentz-Boltzmann equation

Lorentz-Drude model

Lorentz-Gauss functions

Lorentz-Gauss transformation

Lorentz-Gaussian transformation

Lorentz-Lorenz Model

Lorentz-Lorenz internal field

Lorentz-Lorenz law

Lorentz-Lorenz refraction equation

Lorentz-Lorenz refraction equation index

Lorentz-Lorenz scattering

Lorentz-Mie

Lorentz-corrected SAXS profile

Lorentz-invariance

Lorentz-polarization factor

Lorentz-polarization factor table

Lorentz-type shape

Lorentz/Gauss window

Lorentz’s equation

Lorenz and Lorentz

Lorenz-Lorentz equation

Lorenz-Lorentz expression

Lorenz-Lorentz formula

Lorenz-Lorentz relationship

Lorenz-Lorentz theory

Lorenz-Lorentz theory measurement

Magnetization Lorentz model

Maxwell-Lorentz equation

Modified Lorentz curve

Onsager-Lorentz theory

Peak Lorentz

Peak shape function Lorentz

Periodic Yukawa-potential Lorentz gas

Potential Lorentz invariant

Quantum Lorentz covariance

Refractive index Lorentz-Lorenz equation

Relative Lorentz factor

Retardation from Lorentz Transformation

Signal Lorentz

Special relativistic notation Minkowski space-time. Lorentz transformation

The Lorentz Factor

The Lorentz Model

The Lorentz Oscillator

The Lorentz transformation

The Lorentz-Lorenz Equation

Uniqueness of Lorentz transformations

Useful Trigonometric and Hyperbolic Formulae for Lorentz Transformations

Vector Lorentz

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