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Schrodinger’s equations

C. Cerjan, ed., Numerical Grid Methods and their Application to Schrodinger s Equation, Kluwer Academic Publishers, Dordrecht, 1993,... [Pg.322]

The quantum degrees of freedom are described by a wave function /) = (x, t). It obeys Schrodinger s equation with a parameterized coupling potential V which depends on the location q = q[t) of the classical particles. This location q t) is the solution of a classical Hamiltonian equation of motion in which the time-dependent potential arises from the expectation value of V with regard to tp. For simplicity of notation, we herein restrict the discussion to the case of only two interacting particles. Nevertheless, all the following considerations can be extended to arbitrary many particles or degrees of freedom. [Pg.397]

In a first discretization step, we apply a suitable spatial discretization to Schrodinger s equation, e.g., based on pseudospectral collocation [15] or finite element schemes. Prom now on, we consider tjj, T, V and H as denoting the corresponding vector and matrix representations, respectively. The total... [Pg.397]

Zeller, R., 1987, Multiple-scattering solution of Schrodinger s equation for potentials of general shape, J. Phys. C Solid State Phys. 20 2347. [Pg.490]

We now regard Eq. (8-233) as analogous to Schrodinger s equation, and proceed to carry out the transformation to the interaction representation described in Chapter 7, Section 7.7. We define the transformed density matrix R and the transformed potential U by... [Pg.476]

Schrddinger s Equation as a Unitary Transformation.— We may write Schrodinger s equation in the form... [Pg.481]

The third solution to Schrodinger s equation produces the magnetic quantum number, usually designated as m. Allowable values of this quantum number range from -f to +f. A summary of... [Pg.45]

In the application of Schrodinger s equation (2.30) to specific physical examples, the requirements that (jc) be continuous, single-valued, and square-integrable restrict the acceptable solutions to an infinite set of specific functions (jc), n = 1, 2, 3,. .., each with a corresponding energy value E . Thus, the energy is quantized, being restricted to certain values. This feature is illustrated in Section 2.5 with the example of a particle in a one-dimensional box. [Pg.48]

This form of SchrOdinger s equation can be separated with the use of the substitution... [Pg.282]

No theoretical proof of the Pauli principle was given originally. It was injected into electronic structure theory as an empirical working tool. The theoretical foundation of spin was subsequently discovered by Dirac. Spin arises naturally in the solution of Dirac s equation, the relativistic version of Schrodinger s equation. [Pg.272]

Fig. 5.1 Sample IJs) curves for various vibrational states of carbon monosulfide, C = S. These curves were calculated2 in accordance with Eq. (5.2), using i )y(r) functions obtained by solving Schrodinger s equation with an experimental potential energy surface derived from molecular spectroscopy. Fig. 5.1 Sample IJs) curves for various vibrational states of carbon monosulfide, C = S. These curves were calculated2 in accordance with Eq. (5.2), using i )y(r) functions obtained by solving Schrodinger s equation with an experimental potential energy surface derived from molecular spectroscopy.
Suppose that the atom (or nucleus) initially in an eigenstate 1 is subjected to a small time-dependent potential V (t) on top of the unperturbed Hamiltonian Ho2 It is then possible to treat the coefficients an in Eq. (A3.12) as functions of time, with ai 2(r) 1 being the probability that it is still in state 1 after a time x and a2 2(t) < C 1 the probability that it has undergone a transition to another eigenstate 2 . Substituting in Schrodinger s equation (A3.8),... [Pg.409]

This gives the equation of motion (in one dimension), known as Schrodinger s equation ... [Pg.195]

Schrodinger s equation is widely known as a wave equation and the quantum formalism developed on the basis thereof is called wave mechanics. This terminology reflects historical developments in the theory of matter following various conjectures and experimental demonstration that matter and radiation alike, both exhibit wave-like and particle-like behaviour under appropriate conditions. The synthesis of quantum theory and a wave model was first achieved by De Broglie. By analogy with the dual character of light as revealed by the photoelectric effect and the incoherent Compton scattering... [Pg.196]

The KG equation is Lorentz invariant, as required, but presents some other problems. Unlike Schrodinger s equation the KG equation is a second order differential equation with respect to time. This means that its solutions are specified only after an initial condition on bothand d /dt has been given. However, in contrast to k, d /dt has no direct physical interpretation [61]. Should the KG equation be used to define an equation of continuity, as was done with Schrodinger s equation (4), it is found to be satisfied by... [Pg.221]

In order to preserve the resemblance to Schrodinger s equation Dirac obtained another relativistic wave equation by starting from the form... [Pg.221]

Awkward questions about the electromagnetic and gravitational fields of infinitely many particles in the vacuum remain unanswered. Also, the Dirac theory, amended by the hole proposition is certainly not a one-particle theory, and hence not a relativistic generalization of Schrodinger s equation. [Pg.228]

Although Dirac s equation does not directly admit of a completely self-consistent single-particle interpretation, such an interpretation is physically acceptable and of practical use, provided the potential varies little over distances of the order of the Compton wavelength (h/mc) of the particle in question. It allows, for instance, first-order relativistic corrections to the spectrum of the hydrogen atom and to the core-level densities of many-electron atoms. The latter aspect is of special chemical importance. The required calculations are invariably numerical in nature and this eliminates the need to investigate central-field solutions in the same detail as for Schrodinger s equation. A brief outline suffices. [Pg.228]

The second term is just the electronic binding energy of Schrodinger s equation. [Pg.230]

Schrodinger s equation has solutions characterized by three quantum numbers only, whereas electron spin appears naturally as a solution of Dirac s relativistic equation. As a consequence it is often stated that spin is a relativistic effect. However, the fact that half-integral angular momentum states, predicted by the ladder-operator method, are compatible with non-relativistic systems, refutes this conclusion. The non-appearance of electron... [Pg.237]

The belief that computational chemists obtain molecular structures by solving Schrodinger s equation is often dressed up in so much jargon that the essential arguments are obscured. The general basis of the belief may be examined by considering the simplest possible molecule as a test case5. [Pg.363]

Since these field amplitudes are known to be solutions of Schrodinger s equation, the solutions of... [Pg.457]


See other pages where Schrodinger’s equations is mentioned: [Pg.32]    [Pg.107]    [Pg.439]    [Pg.441]    [Pg.443]    [Pg.459]    [Pg.785]    [Pg.47]    [Pg.156]    [Pg.172]    [Pg.44]    [Pg.96]    [Pg.135]    [Pg.662]    [Pg.718]    [Pg.200]    [Pg.237]    [Pg.238]    [Pg.246]    [Pg.249]    [Pg.272]    [Pg.300]    [Pg.476]    [Pg.488]    [Pg.514]   
See also in sourсe #XX -- [ Pg.97 , Pg.102 , Pg.115 , Pg.125 , Pg.131 , Pg.174 , Pg.300 ]




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