Electrons spin orbitals

The first three of these functions are symmetric with respect to Pn and constitute the three components of a spin triplet with IT = 1 the fourth spin function is antisymmetric with respect to Pn and represents a spin singlet. Recalling that the total wave function consists of factors for electron orbital, electron spin, vibrational, rotational and nuclear... 

Recall from Chapter 7 that the three quantum numbers n, I, and m, describe the size (energy), shape, and orientation, respectively, of an atomic orbital. However, an additional quantum number is needed to describe a property of the electron itself, called spin, which is not a property of the orbital. Electron spin becomes important when more than one electron is present. 

The data reported for the molecules in the X, X, and states have been analysed in terms of an effective Hamiltonian which refers to the rotational, spin and hyperfine levels of a particular vibronic state. The Hamiltonian is formulated in terms of the various angular momenta involved, namely TV, L, S, G, J, /, and F which are respectively the rotational, orbital, electron spin, vibrational, nuclear plus electronic, nuclear spin, and total angular momenta (strictly speaking, N = R + L where R is the angular momentum of the nuclear framework). The effective Hamiltonian can be written... 

Electric Field Induced Second Harmonic Extended Huckel Molecular Orbital Electron Spin Echo Envelope Modulation Extended X-ray Absorption Fine Structure Fourier-Transform-ESR hexamethylphosphoric acid triamide Magnetic Circular Dichroism mesityl... 

Chapter 1 Atomic Orbitals, Electron Spin, Linear Combinations... 

Initially, we neglect tenns depending on the electron spin and the nuclear spin / in the molecular Hamiltonian //. In this approximation, we can take the total angular momentum to be N(see (equation Al.4.1)) which results from the rotational motion of the nuclei and the orbital motion of the electrons. The components of. m the (X, Y, Z) axis system are given by ... 

It would appear that identical particle pemuitation groups are not of help in providing distinguishing syimnetry labels on molecular energy levels as are the other groups we have considered. However, they do provide very usefiil restrictions on the way we can build up the complete molecular wavefiinction from basis fiinctions. Molecular wavefiinctions are usually built up from basis fiinctions that are products of electronic and nuclear parts. Each of these parts is fiirther built up from products of separate uncoupled coordinate (or orbital) and spin basis fiinctions. Wlien we combine these separate fiinctions, the final overall product states must confonn to the pemuitation syimnetry mles that we stated above. This leads to restrictions in the way that we can combine the uncoupled basis fiinctions. 

These limitations lead to electron spin multiplicity restrictions and to differing nuclear spin statistical weights for the rotational levels. Writing the electronic wavefunction as the product of an orbital fiinction and a spin fiinction there are restrictions on how these functions can be combined. The restrictions are imposed by the fact that the complete function has to be of synnnetry... 

The simplest case arises when the electronic motion can be considered in temis of just one electron for example, in hydrogen or alkali metal atoms. That electron will have various values of orbital angular momentum described by a quantum number /. It also has a spin angular momentum described by a spin quantum number s of d, and a total angular momentum which is the vector sum of orbital and spin parts with... 

In equation (bl. 15.24), r is the vector coimecting the electron spin with the nuclear spin, r is the length of this vector and g and are the g-factor and the Boln- magneton of the nucleus, respectively. The dipolar coupling is purely anisotropic, arising from the spin density of the impaired electron in an orbital of non-... 

The simplest system exliibiting a nuclear hyperfme interaction is the hydrogen atom with a coupling constant of 1420 MHz. If different isotopes of the same element exhibit hyperfme couplings, their ratio is detemiined by the ratio of the nuclear g-values. Small deviations from this ratio may occur for the Femii contact interaction, since the electron spin probes the inner stmcture of the nucleus if it is in an s orbital. However, this so-called hyperfme anomaly is usually smaller than 1 %. 

As is well known, when the electronic spin-orbit interaction is small, the total electronic wave function v / (r, s R) can be written as the product of a spatial wave function R) and a spin function t / (s). For this, we can use either... 

The permutational symmetry of the rotational wave function is determined by the rotational angular momentum J, which is the resultant of the electronic spin S, elecbonic orbital L, and nuclear orbital N angular momenta. We will now examine the permutational symmetry of the rotational wave functions. Two important remarks should first be made. The first refers to the 7 = 0 rotational... 

You can order the molecular orbitals that arc a solution to etjtia-tion (47) accordin g to th eir en ergy, Klectron s popii late the orbitals, with the lowest energy orbitals first. normal, closed-shell, Restricted Hartree hock (RHK) description has a nia.xirnuin of Lw o electrons in each molecular orbital, one with electron spin up and one w ith electron spin down, as sliowm ... 

A restricted Hartrec-Fock description means that spin-up and spin -down electron socciipy the same spatial orbitals ip,—there is no allowance for different spatial orbitals for different electron spins. 

Introductory descriptions of Hartree-Fock calculations [often using Rootaan s self-consistent field (SCF) method] focus on singlet systems for which all electron spins are paired. By assuming that the calculation is restricted to two electrons per occupied orbital, the computation can be done more efficiently. This is often referred to as a spin-restricted Hartree-Fock calculation or RHF. 

Irons of benzene are distributed in pairs among its three bonding tt MOs giving a closed shell electron configuration All the bonding orbitals are filled and all the electron spins are paired... 

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