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Wave revival

More recently, electrostatic theory has been revived due to the concept of molecular electrostatic potentials. The potential of the solute molecule or ion was used successfully to discuss preferred orientations of solvent molecules or solvation sites 50—54). Electrostatic potentials can be calculated without further difficulty provided the nuclear geometry (Rk) and the electron density function q(R) or the molecular wave function W rxc, [Pg.14]

Released in phenomenal quantities, only 1 % of their energy need be communicated to the envelope in order to shatter it to smithereens. The revived shock wave reignites nuclear reactions in its wake and modifies the deep isotopic composition of the star (Fig. 7.5). [Pg.148]

Figure 7.2 The enlarged view of the wave packet motion given in Figure 7.1 around the quarter revival (T /4) region. The motion of the two counter-propagating packets is indicated with dotted lines. Figure 7.2 The enlarged view of the wave packet motion given in Figure 7.1 around the quarter revival (T /4) region. The motion of the two counter-propagating packets is indicated with dotted lines.
T. Seideman. Revival structure of ahgned rotational wave packets. Phys. Rev. Lett, 83(24) 4971 974 (1999). [Pg.412]

But even those who can t afford a trip on the new Zeppelin may benefit from airship technology. The Japanese are designing blimps, which will float at an altitude of 65,000 feet and will be used to reflect waves used in cellular phone communication. The blimp s skin will be made of pvc coated with polyethylene, and the ship will be kept aloft for years. So we may yet see a revival of the great airships — with various new safety features. But, contrary to popular opinion, these great ships... [Pg.210]

The interest in superluminal processes has been revived, due to some new experimental results (mainly based on electromagnetic wave propagation) that provided incontrovertible evidence for motions occurring at faster-than-light... [Pg.684]

Anharmonic effects lead to a destruction of the initially localized wave-packet with the consequence that the transient signal is damped. However, there is the possibility for the wavepacket to regain its initial shape after long times resulting in so-called revivals [see, for example, Alber and Zoller (1991)]. The revival period Trev contains additional information about the shape of the potential. [Pg.373]

Schrodinger and Bohm both accepted that quantum motion follows a wave pattern. To account for wave-particle dualism the interpretation of matrix mechanics, developed by Heisenberg and others, was extended on the assumption of probability densities. Schrodinger developed the notion of wave structures to simulate particle behaviour, but this model has been rejected almost universally and apparently irretrievably, in favour of proba-bities, arguably prematurely and for questionable reasons. Bohm s attempt to revive the wave interpretation advocated a literary interpretation of wave-particle dualism in the form of a classical particle accompanied and piloted by a quantum wave. [Pg.85]

Schrodinger, Einstein, Bohm and others who may have happened to support aspects of the model outlined here, were invariably accused of trying to revive a classical interpretation of non-classical events. The implied sin is that these individuals dared to recognize a causal structure where it is expressly forbidden by the Copenhagen doctrine. The exact opposite is probably closer to the truth What is more non-classical than a particle that consists of vibrations in the aether a particle with the ability to adapt its shape as dictated by the environment a particle that disappears into, or appears from, the wave structure of another particle a particle with continuous non-local mass and charge densities or a particle which is different from the mass points of classical mechanics However, this is an irrelevant argument. Whether a model is classical or quantal is of no consequence -what is important is that it leads to a reasonable interpretation of chemical phenomena. [Pg.108]

In terms of the quantum-potential formulation particle trajectories can be associated with the quantum HJ equation (6) in exactly the same way as in the classical case [34, 35]. As before, particle trajectories associated with the phase S may be obtained by constructing the normals to S, each one distinguished by its initial coordinates. By this procedure Bohm managed to revive the pilot-wave model of De Broglie. It means that a point particle of mass m on a trajectory x = x(t), is now associated with the physical... [Pg.65]

A typical space-time distribution of the spatial density of the inversion (the inversion per single QD) w x, t) =a[ A x, tf - B(x, <)p] is shown in Fig. lb. As follows from (5) the depicted space-time dynamics corresponds to the evolution of a Rabi wavepacket defined as a superposition of Rabi waves with continuous spectrum of h. Physical interpretation of the picture predicted to observe in the QD chain can be given on the base of the collapse-revivals concept [1]. [Pg.34]

The diffraction of H2 and He beams by the surfaces of alkali halide crystals was observed originally in 1930 and provided direct evidence for the wave-nature of matter. Interest in the technique has revived in recent years and considerable experimental advances have been made, particularly in the production of well-collimated and approximately mono-energetic beams for reviews, including experimental details, see refs. 231, 232. [Pg.78]

Fig. 9. Radial trajectories of several mass elements of the core of a 15 M star versus time after bounce. The trajectories are plotted for each 0.02 M up to 1 M , and for each 0.01 M outside this mass. The thick dashed line indicates the location of the shock wave. The prompt shock stalls within 100 ms after reaching 150 km, and recedes down to below 100 km. No sign of a revival of the shock that possibly leads to a successful D(elayed-)CCSN is seen either, even after 300 ms. Instead, a stationary accretion shock forms at several tens of km. A PNS is seen to form, reaching 1.6 M around 1 s after bounce (from [19])... Fig. 9. Radial trajectories of several mass elements of the core of a 15 M star versus time after bounce. The trajectories are plotted for each 0.02 M up to 1 M , and for each 0.01 M outside this mass. The thick dashed line indicates the location of the shock wave. The prompt shock stalls within 100 ms after reaching 150 km, and recedes down to below 100 km. No sign of a revival of the shock that possibly leads to a successful D(elayed-)CCSN is seen either, even after 300 ms. Instead, a stationary accretion shock forms at several tens of km. A PNS is seen to form, reaching 1.6 M around 1 s after bounce (from [19])...
Fig. 2. Time dependence of a hydrogen wave-packet with averaged principal quantum number h = 80 and FWHM An = 4. On top we show the autocorrelation junction l(tp(t)l ip(0)[) and on bottom the radial expectation value. Both values document the occurrence of periodic structures as well as revival and partial revival structures as indicated by vertical dotted lines. Fig. 2. Time dependence of a hydrogen wave-packet with averaged principal quantum number h = 80 and FWHM An = 4. On top we show the autocorrelation junction l(tp(t)l ip(0)[) and on bottom the radial expectation value. Both values document the occurrence of periodic structures as well as revival and partial revival structures as indicated by vertical dotted lines.
J.H. Eberly, N.B. Narozhny, J.J. Sanchez-Mondragon, Periodic spontaneous collapse and revival in a simple quantum model, Phys. Rev. Lett. 44 (1980) 1323. l.Sh. Averbukh, N.F. Perel man, Fractional revivals Universality in the long-term evolution of quantum wave packets beyond the correspondence principle dynamics, Phys. Lett. A 139 (1989) 449. [Pg.482]


See other pages where Wave revival is mentioned: [Pg.346]    [Pg.148]    [Pg.148]    [Pg.148]    [Pg.119]    [Pg.219]    [Pg.293]    [Pg.403]    [Pg.407]    [Pg.183]    [Pg.903]    [Pg.184]    [Pg.332]    [Pg.22]    [Pg.333]    [Pg.465]    [Pg.530]    [Pg.531]    [Pg.532]    [Pg.162]    [Pg.192]    [Pg.110]    [Pg.82]    [Pg.35]    [Pg.60]    [Pg.250]    [Pg.207]    [Pg.50]    [Pg.1052]    [Pg.465]    [Pg.16]    [Pg.183]    [Pg.43]    [Pg.21]    [Pg.317]   
See also in sourсe #XX -- [ Pg.51 ]




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