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Pauli exclusion principle and

The resolution of this issue is based on the application of the Pauli exclusion principle and Femii-Dirac statistics. From the free electron model, the total electronic energy, U, can be written as... [Pg.128]

Electrons occupy orbitals in such a way as to minimize the total energy of an atom by maximizing attractions and minimizing repulsions in accord with the Pauli exclusion principle and Hund s rule. [Pg.161]

We account for the ground-state electron configuration of an atom by using the building-up principle in conjunction with Fig. 1.41, the Pauli exclusion principle, and Hund s rule. [Pg.161]

The application of the quantum mechanics to the interaction of more complicated atoms, and to the non-polar chemical bond in general, is now being made (45). A discussion of this work can not be given here it is, however, worthy of mention that qualitative conclusions have been drawn which are completely equivalent to G. N. Lewis s theory of the shared electron pair. The further results which have so far been obtained are promising and we may look forward with some confidence to the future explanation of chemical valence in general in terms of the Pauli exclusion principle and the Heisenberg-Dirac resonance phenomenon. [Pg.60]

Before estabiishing the connection between atomic orbitals and the periodic table, we must first describe two additionai features of atomic structure the Pauli exclusion principle and the aufbau principle. [Pg.513]

The connection between the Pauli exclusion principle and the more general Pauli principle can be understood as follows. If two electrons with the same spin a were to occupy the same orbital ip, the total wave function for the system would be written yi, zO (/ "to, yi,... [Pg.69]

Further, if the wave function depends also on the electron spins, spin variables over all electrons should also be integrated we will see this below, in the calculation of exchange hole. The expression in the curly brackets above is exactly the XC hole PxCM(r, r ) defined in Equation 7.17. A comparison with Equation 7.19a shows that adding the hole to the density is similar to subtracting the density of one electron p(r )/N from it. The hole thus represents a deficit of one electron from the density. This is easily verified by integrating p tM(V, r ) over the volume dr, which gives a value of — 1. However, the structure of the hole is not simple and this is because of the motion of different electrons correlated due to the Pauli exclusion principle and the Coulomb interaction between them. Finally we note that the product p(r)p cM(r, r ) is symmetric with respect to an exchange in the variables... [Pg.88]

The XC energy represents the correction to the Coulomb energy for the self-energy of an electron in a many-electron system. The latter is due to both the direct self-energy of the electron as well as the redistribution of electronic density around each electron because of the Pauli exclusion principle and the Coulomb interaction. As an example, we now discuss the case of Fermi hole and the exchange energy in Hartree-Fock (HF) theory [16]. For brevity, we restrict ourselves to closed-shell cases. [Pg.89]

Of course, the Coulomb interaction appears in the Hamiltonian operator, H, and is often invoked for interpreting the chemical bond. However, the wave function, l7, must be antisymmetric, i.e., must satisfy the Pauli exclusion principle, and it is the only fact which explains the Lewis model of an electron pair. It is known that all the information is contained in the square of the wave function, 1I7 2, but it is in general much complicated to be analyzed as such because it depends on too many variables. However, there have been some attempts [3]. Lennard-Jones [4] proposed to look at a quantity which should keep the chemical significance and nevertheless reduce the dimensionality. This simpler quantity is the reduced second-order density matrix... [Pg.282]

Quantum mechanics may be used to determine the arrangement of the electrons within an atom if two specific principles are applied the Pauli exclusion principle and the Aufbau principle. The Pauli exclusion principle states that no two electrons in a given atom can have the same set of the four quantum numbers. For example, if an electron has the following set of quantum numbers n = 1, l = 0, m = 0, and ms= +1/2, then no other electron may have the same set. The Pauli exclusion principle limits all orbitals to only two electrons. For example, the ls-orbital is filled when it has two electrons, so that any additional electrons must enter another orbital. [Pg.111]

Lewis and many other chemists saw in the Pauli exclusion principle and the Uhlenbeck-Goudsmit spin hypothesis firm physical support for the chemical valence theory of the electron pair. In fact, the Pauli exclusion principle has to be postulated within the physics of the quantum theory.23 Accepting the Nobel Prize in physics for 1945, Pauli expressed regret that the principle cannot be derived ab initio. [Pg.249]

Quoted from R. Kronig and W. F. Weisskopf, eds., W. Pauli Collected Scientific Papers (New York John Wiley, 1964), II 1085, in Peter Joseph Hall, "The Pauli Exclusion Principle and the Foundations of Chemistry," Synthese 69 (1986) 267272, on 270. [Pg.249]

Short-range repulsive forces are a direct result of the Pauli exclusion principle and are thus quantum mechanical in nature. Kitaigorodskii (1961) has emphasized that such short-range repulsive forces play a major role in determining the packing in molecular crystals. The size and shape of molecules is determined by the repulsive forces, and the molecules pack as closely as is permitted by these forces. [Pg.203]

Notice the similarities between the two parts of Table 1.1 and the form of the Periodic Table given in Figure 1.3. The quantum rules, the Pauli exclusion principle and the aufbau principle combine to explain the general structure of the Periodic Table. [Pg.8]

THE PAULI EXCLUSION PRINCIPLE AND THE PERIODIC SYSTEM OF THE ELEMENTS... [Pg.47]

See also Pauli Exclusion Principle and Quantum Mechanics. [Pg.1220]

The nuclei of the atoms in a solid and the inner electrons form ion cores with energy levels little different from corresponding levels in free atoms. The characteristics of the valence electrons arc modified greatly, however. The stale functions of these outer electrons greatly overlap those of neighboring atoms. Restrictions of the Pauli Exclusion Principle and the Uncertainty Principle force modification of the state functions, and the development of a set of split energy levels becomes a quasi-continuous band of levels of width, which are several electron volts for most solids. Importantly, unoccupied levels of the atoms are also split into bands. The electronic characteristics of solids are determined by the relative position in energy of the occupied and unoccupied levels as well as by die characteristics of the electrons within a band. [Pg.1518]

COVALENT BONDING involves a pair of electrons with opposite electron spin. The bond (or electron charge distribution) is essentially localized between nearest neighbor atoms that contribute electrons for the bonding. Since these electron pairs follow Bose-Einstein statistics, therefore they are known as boson. In this case the paired particles do not obey the Pauli Exclusion Principle and many electron pairs in the system may occupy the same energy level. [Pg.1]

The theoretical treatment of a solid-state transition involving covalent (localized) vs. conduction (delocalized) electronic transformation was first enunciated by Mott [44], By considering the Pauli Exclusion Principle and the electron-electron interaction during the transformation, it was shown that such transition will be critically dependent upon the inter-atomic distances. The number of electrons already existing in the conduction state will in turn influence the critical inter-atomic distances and the transition therefore, it is necessarily a cooperative phenomenon. Later, in a theoretical treatment of the same subject, but based on a different context, Goodenough [45] has shown that the transition is likely to be second-order if the number of electrons per like atom is non-integral. Further, a crystallographic distortion is a prominent manifestation of such a transition. [Pg.137]

Thus, the triplet repulsion arises due to the Pauli exclusion principle and is often referred to as Pauli repulsion. [Pg.52]

According to the Pauli Exclusion Principle, and Hund s Rule for filling electron orbitals, each orbital of the same type must fill with two electrons, spinning in opposite directions, before a new type of orbital is occupied. However, before electrons can double up in an orbital, all orbitals on the same energy level of the same type must have one electron in it, all spinning in the same direction. [Pg.72]

Obviously two particles cannot overlap significantly (the Pauli Exclusion Principle and our experience tells us this). Thus, we have the boundary condition... [Pg.553]


See other pages where Pauli exclusion principle and is mentioned: [Pg.176]    [Pg.177]    [Pg.19]    [Pg.51]    [Pg.76]    [Pg.18]    [Pg.63]    [Pg.89]    [Pg.281]    [Pg.257]    [Pg.140]    [Pg.37]    [Pg.407]    [Pg.79]    [Pg.648]    [Pg.625]    [Pg.215]    [Pg.679]    [Pg.1101]    [Pg.1]    [Pg.7]    [Pg.342]    [Pg.74]   
See also in sourсe #XX -- [ Pg.132 , Pg.142 ]




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