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Postulates wavefunction

To extract infomiation from the wavefimction about properties other than the probability density, additional postulates are needed. All of these rely upon the mathematical concepts of operators, eigenvalues and eigenfiinctions. An extensive discussion of these important elements of the fomialism of quantum mechanics is precluded by space limitations. For fiirther details, the reader is referred to the reading list supplied at the end of this chapter. In quantum mechanics, the classical notions of position, momentum, energy etc are replaced by mathematical operators that act upon the wavefunction to provide infomiation about the system. The third postulate relates to certain properties of these operators ... [Pg.7]

By learning the solutions of the Schrodinger equation for a few model systems, the student can better appreciate the treatment of the fundamental postulates of quantum mechanics as well as their relation to experimental measurement because the wavefunctions of the known model problems can be used to illustrate. [Pg.7]

The number No of occupied valence SCF orbitals in a molecule is typically less than the total number Nmb of orbitals in the minimal valence basis sets of all atoms. The full valence MCSCF wavefunction is the optimal expansion in terms of all configurations that can be generated from N b molecular orbitals. Closely related is the full MCSCF wavefunction of all configurations that can be generated from Ne orbitals, where Nc is the number of valence electrons, i.e. each occupied valence orbital has a correlating orbital, as first postulated by Boys (48) and also presumed in perfect pairing models (49,50), We shall call these two types of frill spaces FORS 1 and FORS 2. In both, the inner shell remains closed. [Pg.106]

The time evolution of the wavefunction P is determined by solving the time-dependent Schrodinger equation (see pp 23-25 of EWK for a rationalization of how the Schrodinger equation arises from the classical equation governing waves, Einstein s E=hv, and deBroglie s postulate that A,=h/p)... [Pg.39]

This picture can qualitatively account for the g tensor anisotropy of nitrosyl complexes in which g = 2.08, gy = 2.01, and g == 2.00. However, gy is often less than 2 and is as small as 1.95 in proteins such as horseradish peroxidase. To explain the reduction in g from the free electron value along the y axis, it is necessary to postulate delocalization of the electron over the molecule. This can best be done by a complete molecular orbital description, but it is instructive to consider the formation of bonding and antibonding orbitals with dy character from the metal orbital and a p orbital from the nitrogen. The filled orbital would then contribute positively to the g value while admixture of the empty orbital would decrease the g value. Thus, the value of gy could be quite variable. The delocalization of the electron into ligand orbitals reduces the occupancy of the metal d/ orbital. This effectively reduces the coefficients of the wavefunction components which account for the g tensor anisotropy hence, the anisotropy is an order of magnitude less than might be expected for a pure ionic d complex in which the unpaired electron resides in the orbital. [Pg.105]

With increasing atomic volume, one approaches the free atom limit where Hund s first rule postulates maximum spin, so that the individual spins of the electrons in a shell are aligned parallel. More generally, Pauli s exclusion principle implies that electrons with parallel spins have different spatial wavefunctions, reduces the Coulomb repulsion and is seen as exchange interaction. When the atoms are squeezed into a solid, some of the electrons are forced into common spatial wavefunctions, with antiparallel spins and reduction of the overall magnetic moment. At surfaces and interfaces, the reduced coordination reverses this effect, and a part of the atomic moment is recovered. [Pg.20]

Nuclear Spin Effects on Rotation. There is an interesting effect on the rotational partition function, even for the hydrogen molecule, due to nuclear spin statistics. The Fermi postulate mandates that the overall wavefunction (including all sources of spin) be antisymmetric to all two-particle interchanges. A simple molecule like (1H1)2, made of two electrons (S = 1/2) and two protons (spin 7=1/2), will have two kinds of molecule ... [Pg.301]

One of the postulates of quantum mechanics tells us that the physical state of a particle can be fully described by an appropriate mathematical function which is known as its wavefunction. The variation theorem states that any wavefunction which obeys the same boundary conditions as the correct ground state wavefunction will give an expectation value E for the energy that is greater than or equal to the true ground state energy Eo, i.e. E > Eq. [Pg.43]

One of the postulates of quantum mechanics is that the state of a particle, in this case an electron, is described fully by a wavefunction fi, from which all its observable properties can be determined. If an orthogonal coordinate system is being used, 4 will be a function of x, y and z, and denoted more fully by T(x, y, z). [Pg.100]

Postulate 5. The wavefunction of a system evolves in time in accordance with the time-dependent Schrddinger equation... [Pg.32]

Postulate 1. The state of a quantum-mechanical system is completely specified by a wavefunction < that depends on the coordinates and time. The square modulus of this function I gives the probability density for finding the system with a specified set of coordinate values. [Pg.196]

Fig. 17 Energy Level diagram pertaining to the [11(0112)5] + cation, following the one-electron orbital energy level scheme postulated by Best [47]. The wavefunctions of the Eg ground term are defined in terms of the quantum numbers jMj, Ms)... Fig. 17 Energy Level diagram pertaining to the [11(0112)5] + cation, following the one-electron orbital energy level scheme postulated by Best [47]. The wavefunctions of the Eg ground term are defined in terms of the quantum numbers jMj, Ms)...
VB functions have been championed by Warshel and his co-workers for use in studying reactions in enzymes and in solution. The method, which they term the empirical VB (EVB) method, supposes that the wave-function for a particular problem, i/>,can be written as a linear combination of the wavefunctions of resonant forms, v i, which are postulated to be important in the process. For example, for a bond breaking reaction, AB — A+ + B, which produces ionic products, the contributing resonant forms could be the covalent, AB, and ionic, A B+,states that dissociate to atoms and ions respectively. The total wavefunction is ... [Pg.136]

The foremost impact of electronic spin is due to the Pauli principle, a fundamental postulate of quantum mechanics. It can be stated as follows The total wavefunction (Equation 1.10) must be antisymmetric with respect to the interchange of any electron pair et and ey, i.e. of their coordinates qe. and q j (Equation 1.12). [Pg.20]

The relationship between this wavefunction (sometimes called state function) and the location of particles in the system forms the basis for a second postulate ... [Pg.5]

It follows from the fifth postulate that the kinetic energy of each particle in the system (and therefore the total kinetic energy) is restricted to non-negative values. Therefore, the expectation value of the kinetic energy cannot be negative. The other possibility is that the wavefunction is non-vanishing only when V = For... [Pg.21]

Here, n is an integer, is the frequency of the vibration, and h is known as Planck s constant This quantization of energy, as it is known, was first postulated by Max Planck in 1900 as a key part of his theory to explain the frequency distribution of radiation emitted by a black body. It is found that energy is quantized whenever a particle is confined to a small space because of the need to match the wavefunction of the particle to the space available. This applies just as much to electrons travelling around an atomic nucleus as it does to atoms vibrating in a solid. [Pg.3]

This important equation is based on one of the basic postulates of quantum mechanics, and it cannot be derived from a more fundamental equation. However, we can carry out a check on the equation by replacing the trial wavefunction with one of the eigenfunctions of the Hamiltonian operator, yr. Application of equation (8.1) then leads to the correct result ... [Pg.138]


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See also in sourсe #XX -- [ Pg.166 ]




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The Wavefunction Postulate

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