Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Magnetic field operator

Dense-phase fluidization can also be conducted in the presence of force fields other than a gravitational field. Such force fields include vibrational, acoustic, centrifugal, and magnetic fields. Operations with applications of these fields are known, respectively, as vibrofluidized beds [Mori et al., 1992], acoustic fluidized beds [Montz et al., 1988 Chirone et al., 1992],... [Pg.377]

A third contribution to the susceptibility rises from matrix elements of the magnetic field operator to states lying outside the coupled set of (2Si+ 1) (2S2 + 1) states. We now show that this is approximately the same for all states and equal to the sum of the contributions from the two separate systems. Consider system 1. If we neglect energies due to spin-orbit, spin-spin coupling, etc., we can write the excited states as and because of the form of the magnetic field operator... [Pg.97]

Fourier series mode expansions for the multipolar electric displacement and magnetic field operators may be written in terms of fhe creation and destruction operators as... [Pg.8]

The nature of media effects relates to the fact that, since the microscopic displacement field is the net field to which molecules of the medium are exposed, it corresponds to a fundamental electric field dynamically dressed by interaction with the surroundings. The quantized radiation is in consequence described in terms of dressed photons or polaritons. A full and rigorous theory of dressed optical interactions using noncovariant molecular quantum electrodynamics is now available [25-27], and its application to energy transfer processes has been delineated in detail [10]. In the present context its deployment leads to a modification of the quantum operators for the auxiliary fields d and h, which fully account for the influence of the medium—the fundamental fields of course remain unchanged. Expressions for the local displacement electric and the auxiliary magnetic field operators [27], correct for all microscopic interactions, are then as follows... [Pg.611]

The magnetic field operator B(r) can be obtained in an analogous manner. Since B(r) = rot A, we obtain from (4.41)... [Pg.118]

Non-Equilibrium Microwave Discharge in Magnetic Field Operating in Conditions of Electron Cyclotron Resonance... [Pg.374]

A SQUID [2] provides two basic advantages for measuring small variations in the magnetic field caused by cracks [3-7]. First, its unsurpassed field sensitivity is independent of frequency and thus dc and ac fields can be measured with an resolution of better than IpT/VHz. Secondly, the operation of the SQUID in a flux locked loop can provide a more than sufficient dynamic range of up to 160 dB/VHz in a shielded environment, and about 140 dB/>/Hz in unshielded environment [8]. [Pg.255]

Sensitive parameters are necessary to compare several high resolution magnetic field sensors. Such parameters can be found with methods of signal theory for LTI-systems. The following chapter explains characteristic functions and operations of the signal analysis for linear local invariant systems and their use in non-destructive testing. [Pg.365]

Main system parameters are shown in table 1. The fine field resolution is important. When operating in an unshielded space, however, at least such important is the high common mode rejection and the gradient rejection in order to suppress parasitic magnetic fields. [Pg.989]

Conventional covermeters operating on the principle of electro-magnetic fields are capable of determining depth of cover to reinforcement down to about 100 mm with an accuracy of 5 % provided the bar diameter is known and the spacing between individual bars is greater than about 150 mm. If bars are spliced then the covermeter will underestimate the cover depth. [Pg.999]

Electrons and most other fiindamental particles have two distinct spin wavefunctions that are degenerate in the absence of an external magnetic field. Associated with these are two abstract states which are eigenfiinctions of the intrinsic spin angular momentum operator S... [Pg.28]

Another powerftil class of instmnientation used to study ion-molecule reactivity is trapping devices. Traps use electric and magnetic fields to store ions for an appreciable length of time, ranging from milliseconds to thousands of seconds. Generally, these devices mn at low pressure and thus can be used to obtain data at pressures well below the range in which flow tubes operate. [Pg.810]

The original method employed was to scan eitiier the frequency of the exciting oscillator or to scan the applied magnetic field until resonant absorption occiined. Flowever, compared to simultaneous excitation of a wide range of frequencies by a short RF pulse, the scanned approach is a very time-inefficient way of recording the spectrum. Flence, with the advent of computers that could be dedicated to spectrometers and efficient Fourier transfomi (FT) algoritluns, pulsed FT NMR became the nomial mode of operation. [Pg.1470]

For a quantum mechanical system pg is replaced by the appropriate operator, equation (bl.15.1) to obtain the Flamiltonian for a free electton in a magnetic field,... [Pg.1549]

Now, consider the case of spinless particles not subject to external electronic and magnetic fields. We may now choose the unitai7 operator U as the unit operator, that is, T = K. For the coordinate and momentum operators, one then obtains... [Pg.616]

Alternatively, ions of any one selected m/z value can be chosen by holding the magnetic field steady at the correct strength required to pass only the desired ions any other ions are lost to the walls of the instrument. The selected ions pass through the gas cell and are detected in the singlepoint ion collector. If there is a pressure of a neutral gas such as argon or helium in the gas cell, then ion-molecule collisions occur, with decomposition of some of the selected incident ions. This is the MS/MS mode. However, without the orthogonal TOF section, since there is no further separation by m/z value, the new ions produced in the gas cell would not be separated into individual m/z values before they reached the detector. Before the MS/MS mode can be used, the instrument must be operated in its hybrid state, as discussed below. [Pg.159]


See other pages where Magnetic field operator is mentioned: [Pg.272]    [Pg.350]    [Pg.162]    [Pg.13]    [Pg.144]    [Pg.609]    [Pg.53]    [Pg.162]    [Pg.371]    [Pg.58]    [Pg.139]    [Pg.330]    [Pg.231]    [Pg.28]    [Pg.709]    [Pg.126]    [Pg.272]    [Pg.350]    [Pg.162]    [Pg.13]    [Pg.144]    [Pg.609]    [Pg.53]    [Pg.162]    [Pg.371]    [Pg.58]    [Pg.139]    [Pg.330]    [Pg.231]    [Pg.28]    [Pg.709]    [Pg.126]    [Pg.342]    [Pg.172]    [Pg.802]    [Pg.1126]    [Pg.1179]    [Pg.1470]    [Pg.1472]    [Pg.1501]    [Pg.1553]    [Pg.119]    [Pg.524]    [Pg.156]    [Pg.158]    [Pg.158]    [Pg.211]    [Pg.308]    [Pg.194]   
See also in sourсe #XX -- [ Pg.80 ]




SEARCH



© 2024 chempedia.info