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Nucleus closed shells

The spin density defines the excess probability of finding spin-up over spin-down electrons at a point in space and is zero everywhere for closed-shell RHF situations. The spin density at the position of a nucleus is a prime determinant of electron spin resonance (ESR) spectra. [Pg.243]

A transition metal with the configuration t/ is an example of a hydrogen-like atom in that we consider the behaviour of a single (d) electron outside of any closed shells. This electron possesses kinetic energy and is attracted to the shielded nucleus. The appropriate energy operator (Hamiltonian) for this is shown in Eq. (3.4). [Pg.40]

The result of the electrostatic multipole interaction is to deplete primarily the 5p-shell electrons in the I ion. The number of electrons originally in the 5p closed shell are lost to excited states. Since the 5p excitation is primarily to the 65 shell, the direct effect on the 5 electron density at the nucleus will be much smaller than the 5 density. As a result of the depletion of 5p electrons, however, the nucleus will be less shielded, and the 5 electrons will have a greater probability of being at... [Pg.139]

The formation of a complex Species by the association of two or more chemical entities (having, in general, electronic closed shells) is one of the most fundamental molecular processes in biology, in chemistry and in physics. Such a super-molecule represents the next higher level of physical complexity after the nucleus, the atom and the molecule. Its formation involves bonding interactions which are much weaker than the usual well defined covalent bonds. [Pg.2]

As the size of an atom increases, its outer electrons move further away from the attractive force of the nucleus. The electrons are held less tightly and are said to be more polarizable. Fluoride is a nucleophile having hard or low polarizability, with its electrons held close to the nucleus, and it must approach the carbon nucleus closely before orbital overlap can occur. The outer shell of the soft iodide has loosely held electrons, and these can easily shift and overlap with the carbon atom at a relatively long distance. [Pg.237]

Atomic Number. The number of positive charges or the number of negative electrons around the nucleus was designated as the atomic number of the atom, These showed a close parallelism with the arrangement of atoms in the periodic system. Through the formulation of a number of rules based upon Bohr s picture of quantized orbits, the periodic system of tlie elements could be understood, Hydrogen was given one electron, and helium two, The two electrons in helinin constituted a closed shell which exhibited almost perfect spherical symmetry and chemical inactivity. [Pg.1209]

In a schematic presentation(see fig.2) of a single-closed shell nucleus, we take as the lowest intruder state (0+state) a proton (tt) 2p-2h configuration... [Pg.189]

A special situation occurs at Zr (Z=40), where the neutron subshell closure (N=56) gives this nucleus a double subshell closure. Thus, particle-hole pair excitations across both subshell gaps are possible. This could produce situations much like those in doubly closed shell 0, in which the lowest-lying intruder deformed band has been shown to arise due to such excitations [BR064]. [Pg.200]

The angle brackets remind us that these energy terms are quantum-mechanical average values or expectation values each is a functional of the ground-state electron density. Focussing first on the middle term, the one most easily dealt with the nucleus-electron potential energy is the sum over all 2n electrons (as with our treatment of ab initio theory, we will work with a closed-shell molecule which perforce has an even number of electrons) of the potential corresponding to attraction of an electron for all the nuclei A ... [Pg.452]


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See also in sourсe #XX -- [ Pg.12 , Pg.19 , Pg.21 , Pg.38 ]




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