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Wave fields

Figure Cl.4.3. Schematic diagram of the Tin-periD-lin configuration showing spatial dependence of the polarization in the standing-wave field (after 1171). Figure Cl.4.3. Schematic diagram of the Tin-periD-lin configuration showing spatial dependence of the polarization in the standing-wave field (after 1171).
The construction of a TXRF system, including X-ray source, energy-dispersive detector and pulse-processing electronics, is similar to that of conventional XRF. The geometrical arrangement must also enable total reflection of a monochromatic primary beam. The totally reflected beam interferes with the incident primary beam. This interference causes the formation of standing waves above the surface of a homogeneous sample, as depicted in Fig. 4.1, or within a multiple-layered sample. Part of the primary beam fades away in an evanescent wave field in the bulk or substrate [4.28],... [Pg.184]

A.A. Kaufman and A.L. Levshin - Acoustic and Elastic Wave Fields in Geophysics, I... [Pg.249]

In general the spectral one-particle density matrix p(r, rE) describes the mutual coherence of the wave field of high-energy electrons at the points r and r. For the simplest case of time-independent interaction potential the diagonal elements of... [Pg.161]

Ed being the energy of the fast electron. To a good approximation, the effect of inelastically scattered electrons on the elastic electron wave field may be treated via a first order perturbation method. From Equation (4) we have... [Pg.162]

All tensor expressions (35)-(42) involve summation over Bloch waves, i.e. summation over j. For a dynamical diffraction calculation involving AT beams, the number of Bloch waves resulting from Equation (30) equals the number of beams, i.e. N. It should be noted, however, that not all of these Bloch waves will be strongly excited within the crystal and contribute to the electron wave field. The excitation amplitudes of the Bloch waves in the crystal are given by B 0J. Extensive numerical calculations show that in a typical dynamical diffraction calculation, although typically more than... [Pg.170]

The coalescence of bubbles is driven by the two mechanisms. One is the attractive radiation force between bubbles called secondary Bjerknes force. The other is the other radiation force called the primary Bjerknes force which drives active bubbles to the pressure antinode of a standing wave field, ft should be noted, however, too strong acoustic wave repels bubbles from the pressure antinode as described in the next section [29, 30]. [Pg.7]

Fig. 13.12 Photographs of sonoluminescence from sulfuric acid solution of Na2SC>4, illustrating the spatial separation of sodium (orange) and continuum (blue-white) emissions using a horn-type transducer at 20 kHz (a) [38] (Reprinted from American Chemical Society. With permission) and using standing-wave fields at 28 kHz in a cylindrical beaker (b) [39]... Fig. 13.12 Photographs of sonoluminescence from sulfuric acid solution of Na2SC>4, illustrating the spatial separation of sodium (orange) and continuum (blue-white) emissions using a horn-type transducer at 20 kHz (a) [38] (Reprinted from American Chemical Society. With permission) and using standing-wave fields at 28 kHz in a cylindrical beaker (b) [39]...
Figure 31. Depiction of the X-ray standing wave field formed by the interference between incident and Bragg reflected beams. Figure 31. Depiction of the X-ray standing wave field formed by the interference between incident and Bragg reflected beams.
A charge (q) is therefore associated with the wave field ip(x) and the charge density is given by... [Pg.166]

In order to obtain the particle description required for quantum statistics, it may therefore be necessary to quantize the quantum-mechanical wave field a second time. This procedure, known as second quantization, starts from the wave field once quantized ... [Pg.456]

In summary, a series of energy levels E is determined by the original Sehrodinger equation. These energy levels may be occupied by the nfl quanta, or particles. This conclusion shows that field quantization guarantees the corpuscular character even in the case of the Sehrodinger wave field. [Pg.459]

There is a close similarity with planar electromagnetic cavities (H.-J. Stockmann, 1999). The basic equations take the same form and, in particular, the Poynting vector is the analog of the quantum mechanical current. It is therefore possible to experimentally observe currents, nodal points and streamlines in microwave billiards (M. Barth et.al., 2002 Y.-H. Kim et.al., 2003). The microwave measurements have confirmed many of the predictions of the random Gaussian wave fields described above. For example wave function statistics, current flow and... [Pg.72]

Ebeling, K.J. Statistical properties of random wave fields in Physical Acoustics Principles and Methods. New York Academic Press, 1984. [Pg.77]

Spengler, J. F. Jekel, M. Christensen, K. T. Adrian, R. J. Hawkes, J. J. Coakley, W. T., Observation of yeast cell movement and aggregation in a small scale MHz ultrasonic standing wave field, Bioseparation 2000, 9, 329 341... [Pg.444]

T. H. Watts, H. E. Gaub, and H. M. McConnell, T-cell-mediated association of peptide antigen and major histocompatibility complex protein detected by energy transfer in an evanescent wave-field, Nature 320, 176-179 (1986). [Pg.342]

TF Systems A TF is a device whose spectral transmission can be controlled by applying a voltage or acoustic signal. There are two main TF devices acousto-optical TF (AOTF), based on diffraction, and liquid crystal TF (LCTF), based on birefringence. An AOTF is a transparent crystal in which an ultrasonic wave field is created,... [Pg.414]

Additional complications arise when the EM wave in a dissipative medium approaches a vacuum interface at an oblique angle [26]. The incident and reflected wave fields then become inhomogeneous (damped) in the direction of propagation. As a consequence the matching at the interface to a conventional undamped electromagnetic wave in vacuo becomes impossible. [Pg.24]

When finally reaching the regime 0 0 the EMS wave fields of... [Pg.59]

Finally a few words would be perhaps not superfluous about the relation of our results to the quantum mechanics of wave fields. It might appear that all calculations based on p.m. in the latter theory are not justifiable from the mathematical standpoint. But it must be remarked that even the operators themselves used in this theory are quite singular and at present do not accept rigorous mathematical taeatment. In such a state of affairs it would be premature to discuss the validity of p,m. in particular. [Pg.77]

Since the structure of the wave field also depends on the wind history and on the size and exposure of the water body, the wind speeds which separate the regimes vary between different water bodies. The above limits reflect average conditions for the ocean. [Pg.903]


See other pages where Wave fields is mentioned: [Pg.182]    [Pg.160]    [Pg.171]    [Pg.8]    [Pg.13]    [Pg.350]    [Pg.310]    [Pg.312]    [Pg.200]    [Pg.281]    [Pg.331]    [Pg.456]    [Pg.77]    [Pg.114]    [Pg.470]    [Pg.82]    [Pg.102]    [Pg.260]    [Pg.159]    [Pg.384]    [Pg.496]    [Pg.59]    [Pg.724]    [Pg.751]    [Pg.2]    [Pg.901]    [Pg.914]   


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Beltrami vector fields waves

Bond length field wave functions

Complete active space self-consistent field wave function

Complete active space self-consistent-field CASSCF) wave function

Crystal field theory wave numbers

Degenerate four-wave mixing electric field induced second

Dissociation energies field wave functions

Electromagnetic field theory wave mechanics

Electromagnetic field/wave

Electromagnetic fields vector wave equations

Electromagnetic wave electric field

Evanescent field wave, penetration depth

Evanescent field/wave

Field wave equations

Free-field blast waves

Guided wave field

Harmonic electric-field wave

INDEX wave field

Local plane waves evanescent fields

Magnetic field electromagnetic wave

Magnetic field light wave

Multi-configurational self-consistent fields wave functions

Multiconfiguration Self-Consistent-Field Wave Functions

Multiconfigurational self-consistent field MCSCF) wave functions

Multiconfigurational self-consistent field wave function

Plane Wave Optical Field

Radiation field space wave contribution

Rayleigh wave field

Response equations field wave functions

Schrodinger wave field

Schroedinger wave equation field

Self-consistent field Xa scattered wave

Self-consistent field Xa scattered wave calculations

Self-consistent field ground-state wave

Self-consistent field ground-state wave complexes

Self-consistent field wave functions

Self-consistent field wave functions molecules

Shock Wave Propagation in a Two-Dimensional Flow Field

Standing wave probe field

Standing-wave field

Trapping of Atoms in Optical Standing Wave Fields

Wave field decomposition

Wave-Function Quantum Field

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