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Propagator, Fourth order

Fig. 2. The time evolution of the total energy of four water molecules (potential-energy details are given in [48]) as propagated by the symplectic Verlet method (solid) and the nonsymplectic fourth-order Runge-Kutta method (dashed pattern) for Newtonian dynamics at two timestep values. Fig. 2. The time evolution of the total energy of four water molecules (potential-energy details are given in [48]) as propagated by the symplectic Verlet method (solid) and the nonsymplectic fourth-order Runge-Kutta method (dashed pattern) for Newtonian dynamics at two timestep values.
It is still necessary to perform an order analysis of the correlation potential in the calculation of. The usual implementation of the electron propagator is performed up to the third or partial fourth orders (31,32,129,130), which needs... [Pg.68]

Hirose et al. [26] proposed a homodyne scheme to achieve the background-free detection of the fourth-order field. With pump irradiation in a transient grating configuration, the fourth-order field propagates in a direction different from that of the second-order field because of different phase match conditions. The fourth-order field is homodyned to make ffourth(td. 2 D) and spatially filtered from the second-order response hecond td, 2 D). [Pg.106]

The lowest order term 7 f °[n], the relativistic kinetic energy in the Thomas-Fermi limit, has first been calculated by Vallarta and Rosen [12], In the second order contribution (which is given in a form simplified by partial integration) explicit vacuum corrections do not occur after renormalisation. Finite radiative corrections, originating from the vacuum part of the propagator (E.5), first show up in fourth order, where the term in proportion ll to... [Pg.77]

Obviously, those are the same considerations as we went through in order to obtain Eqs (90) and (91) and the electron propagator method and the ADC are thus equivalent methods. Using n = 2 in Eq. (93) we determine and n — 3 gives The U matrix in Eq. (93) corresponds to the transition matrix (cf. Eq. (75)). Both and only contain C and D terms (see Eqs (87), (88), (90) and (91), i.e. hj = hj alone. From Eq. (63) we see that we may classify the operators in hj as 2p-lh (two-particle, one-hole) and 2h-lp operators, and the n = 3 ADC approach, corresponding to the third-order electron propagator method, is therefore referred to as the extended 2p-lh Tamm-Dancoff approximation (TDA) (Walter and Schirmer, 1981). A fourth-order approximation to the ADC equations has also been described (Schirmer et ai, 1983) but not yet tested in actual applications. [Pg.218]

Working in a similar way, it is found that there are 24 contributions arising from diagrams of the distributive type represented in Fig. 8(b), where both real photons are absorbed at center A, and a virtual photon conveys the energy mismatch to B the final 24 distributive contributions arises from the mirror-image case where both real photons are absorbed at B and the virtual photon propagates to A. The addition of all 96 matrix element contributions then produces the complete fourth-order result for M -j. [Pg.56]

T. Deveze, L. Beaulie, and W. Tabbara, A fourth order scheme for the FDTD algorithm applied to Maxwell equations, in Proc. IEEE Antennas Propag. Soc. Int. Symp., Chicago, IL, July 1992, vol. 1, pp. 346—349. [Pg.52]

P. G. Petropoulos, Phase error control for FD-TD methods of second and fourth order accuracy, IEEE Trans. Antennas Propag., vol. 42, no. 6, pp. 859-862, June 1994. doi 10.1109/8.301709... [Pg.52]

J. L. Young, D. Gaitonde, and J. S. Shang, Toward the construction of a fourth-order difference scheme for transient EM wave simulation Staggered grid approach, IEEE Trans. Antennas Propag., vol. 45, no. 11, pp. 1573—1580, Nov. 1997.doi 10.1109/8.650067... [Pg.52]

As an example, consider the original PML absorber in a 2-D computational space. Regarding the propagation of the TE case, the fourth-order electric field expression for Ex in the interior of the layer, becomes... [Pg.101]

FIGURE 5.1 (a) Ratio of numerical to physical phase velocity, umln1/u, versus propagation angle (p for second- and fourth-order FDTD implementations, (b) Electric field component (left axis) of analytic and FDTD solutions as well as their absolute errors (right axis) at an observation point 20Ax from the source... [Pg.123]

By the end of the 1980s, state of the art methods of quantum chemistry, such as coupled cluster, configuration interaction, fourth order perturbation theory (MP4), second-order polarization propagator (SOPPA, multiconfigu-rational linear response (MCLR) etc., had been applied to the calculation of... [Pg.251]

Two fourth-order polarization diagrams b, c (Fig. 12.1) should be considered further. The contributions being under consideration are gauge dependent, though the results of the exact calculation of any physical quantity must be gauge independent. All the non-invariant terms are multielectron by their nature. Let us take the photon propagator calibration as follows ... [Pg.241]

Fourth-order and partial fourth-order electron propagator... [Pg.144]

Without including the operator manifold hs, the full fourth-order propagator matrix can be expressed as... [Pg.144]

It is generally more important to include the contributions from the hs manifold before increasing the order of the expansion, and one therefore finds it justifiable to study the electron propagator through what has been coined the partial fourth-order , where only the terms formed from the matrices already obtained in third order are retained. [Pg.144]

In conclusion, one can again reaffirm what already has been established by many workers in the field, namely, that the propagator theory is an appropriate and practical approach to the interpretation and prediction of spectra. The results presented here also show that in order to contain truly quantitative agreement with experiment, it is necessary to consider electron propagator theory at the third and partial fourth order and to also be able to accommodate larger basis sets. [Pg.151]

Yamamoto, T.M. Path-integral virial estimate based on the scaling of fluctiration comdinates application to quantum clusters with fourth-order propagators. J. Chem. Phys. 123, 104101 (2005)... [Pg.105]

Understanding the electronic movement in physical atomic as being driven by the conneeted and correlated functions especially by the (temporally) causal Green-fimction/quantum propagators Describing the physical atom as a semiclassical description of quantum motion, i.e., merely quantum than classical yet with certain orders of Planck constant contributions in electronic orbits in atom Learning the difference between the second and the fourth order of path integral expansion of the quantum amplitude of electronic orbits as quantifies in the associated partition functions ... [Pg.159]

Introduces the quantum statistical version of path integral approach of quantum mechanics, while employing the developed quantum propagators/amplitudes in the second- and fourth-order semiclas-sical expansion, with innovative applications on electronegativity and chemical hardness scales of Periodic Table ... [Pg.534]


See other pages where Propagator, Fourth order is mentioned: [Pg.23]    [Pg.261]    [Pg.469]    [Pg.185]    [Pg.91]    [Pg.52]    [Pg.269]    [Pg.288]    [Pg.138]    [Pg.261]    [Pg.2]    [Pg.12]    [Pg.358]    [Pg.55]    [Pg.52]    [Pg.184]    [Pg.150]    [Pg.95]    [Pg.141]    [Pg.142]    [Pg.532]    [Pg.264]    [Pg.299]    [Pg.287]    [Pg.40]    [Pg.60]    [Pg.61]    [Pg.70]   
See also in sourсe #XX -- [ Pg.144 ]




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