Big Chemical Encyclopedia

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

Articles Figures Tables About

Order external fields

The first two equations are equivalent, yielding the nonrelativistic first-order external field term,... [Pg.352]

The locations of the maxima of the -field and the E-field are different depending on the mode chosen for the EPR experuuent. It is desirable to design the cavity in such a way that the B field is perpendicular to the external field B, as required by the nature of the resonance condition. Ideally, the sample is located at a position of maxuuum B, because below saturation the signal-to-noise ratio is proportional to Simultaneously, the sample should be placed at a position where the E-field is a minimum in order to minimize dielectric power losses which have a detrimental effect on the signal-to-noise ratio. [Pg.1560]

The first-order eorreetion ean be thought of as arising from the response of the wavefunetion (as eontained in its ECAO-MO and Cl amplitudes and basis funetions Xv) plus the response of the Hamiltonian to the external field. Beeause the MCSCF energy funetional has been made stationary with respeet to variations in the Cj and Ci a amplitudes, the seeond and third terms above vanish ... [Pg.509]

If, as is eommon, the atomie orbital bases used to earry out the MCSCF energy optimization are not explieitly dependent on the external field, the third term also vanishes beeause (9xv/3)i)o = 0. Thus for the MCSCF ease, the first-order response is given as the average value of the perturbation over the wavefunetion with X=0 ... [Pg.509]

These concepts play an important role in the Hard and Soft Acid and Base (HSAB) principle, which states that hard acids prefer to react with hard bases, and vice versa. By means of Koopmann s theorem (Section 3.4) the hardness is related to the HOMO-LUMO energy difference, i.e. a small gap indicates a soft molecule. From second-order perturbation theory it also follows that a small gap between occupied and unoccupied orbitals will give a large contribution to the polarizability (Section 10.6), i.e. softness is a measure of how easily the electron density can be distorted by external fields, for example those generated by another molecule. In terms of the perturbation equation (15.1), a hard-hard interaction is primarily charge controlled, while a soft-soft interaction is orbital controlled. Both FMO and HSAB theories may be considered as being limiting cases of chemical reactivity described by the Fukui ftinction. [Pg.353]

Note that while the power-law distribution is reminiscent of that observed in equilibrium thermodynamic systems near a second-order phase transition, the mechanism behind it is quite different. Here the critical state is effectively an attractor of the system, and no external fields are involved. [Pg.441]

We consider first the polarizability of a molecule consisting of two or more polarizable parts which may be atoms, bonds, or other units. When the molecule is placed in an electric field the effective field which induces dipole moments in various parts is not just the external field but rather the local field which is influenced by the induced dipoles of the other parts. The classical theory of this interaction of polarizable units was presented by Silberstein36 and others and is summarized by Stuart in his monograph.40 The writer has examined the problem in quantum theory and finds that the same results are obtained to the order of approximation being considered. [Pg.79]

Let us in fact consider the expectation value of the current operator in the no-particle state in<0 (a ) 0>ln. In order to obtain an insight into this quantity, we first treat the case of a very weak external field so that only effects to first order in the external field need be... [Pg.587]

In order to interpret the above results, consider the expectation value of the total energy density in the vacuum state, i.e., of the hamiltonian density, Eq. (10-12). There is a contribution J u(x)Al(x) from the external field and a contribution m<0 j (a ) 0)ln 4 (a ) from the induced current, hence to lowest order... [Pg.597]

The third order contribution to the amplitude that the vacuum remain a vacuum under the influence of the external field is exhibited by the two diagrams of Fig. 10-7, and is given by... [Pg.623]

To second order in the external field, the scattering amplitude is given by... [Pg.628]

To lowest order in the external field, A%, the scattering is thus determined by the matrix element of the current operator ju(x) between the initial and final one-particle states, p, > and pV>. Let us consider this matrix element in greater detail. Translation invariance asserts... [Pg.712]

As a consequence of the time-averaging of the quasienergy Lagrangian, the derivative in the last equation gives only a nonvanishing result if the frequencies of the external fields fulfill the matching condition Wj = 0. In fourth order Eq. (29) gives the cubic response function ... [Pg.118]

When an electric field is applied, jumps of the ions in the direction of the field are somewhat preferred over those in other directions. This leads to migration. It should be noted that the absolute effect of the field on the ionic motion is small but constant. For example, an external field of 1 V m-1 in water leads to ionic motion with a velocity of the order of 50 nm s 1, while the instantaneous velocity of ions as a result of thermal motion is of the order of 100 ms-1. [Pg.132]

Note that in Eq. (9.11) the coefficient in the external field is factored out. A form very similar to Eq. (9.11) has been employed by Abell and Funabashi (1973) in which the expansion coefficients are expressed as products of incomplete gamma functions of order k,—that is,... [Pg.307]

Phase behavior in complex fluids such as polymer blends and block copolymers has been a rich area of the chemical sciences. Near-critical and other transitional phenomena are frequently prominent. Since molecular movement in viscous systems such as these is comparatively slow, phase transitions can be studied more easily in time, and manipulated by quenching and other external influences. Processes for controlled growth of ordered materials are often readily influenced by diffusion, a variety of external fields, and the influence of interacting boundaries, or flow. [Pg.50]


See other pages where Order external fields is mentioned: [Pg.461]    [Pg.461]    [Pg.635]    [Pg.718]    [Pg.575]    [Pg.878]    [Pg.289]    [Pg.12]    [Pg.195]    [Pg.202]    [Pg.588]    [Pg.605]    [Pg.624]    [Pg.655]    [Pg.710]    [Pg.711]    [Pg.756]    [Pg.85]    [Pg.202]    [Pg.126]    [Pg.129]    [Pg.208]    [Pg.282]    [Pg.404]    [Pg.178]    [Pg.229]    [Pg.287]    [Pg.68]    [Pg.260]    [Pg.267]    [Pg.285]    [Pg.287]    [Pg.308]    [Pg.249]    [Pg.91]    [Pg.122]   
See also in sourсe #XX -- [ Pg.482 ]

See also in sourсe #XX -- [ Pg.482 ]




SEARCH



External field

External ordered field

External ordered field

© 2024 chempedia.info