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Zero-field spin-orbit splitting

Zero-field Spin-Orbit Splitting of Electronic Energy Levels... [Pg.2652]

Lichten [3 5] studied the magnetic resonance spectrum of the para-H2, N = 2 level, and was able to determine the zero-field spin-spin and spin-orbit parameters we will describe how this was done below. Before we come to that we note, from table 8.6, that in TV = 2 it is not possible to separate Xo and X2. Measurements of the relative energies of the J spin components in TV = 2 give values of Xo + fo(iX2, and the spin-orbit constant A the spin rotation constant y is too small to be determined. In figure 8.18 we show a diagram of the lower rotational levels for both para- and ortho-H2 in its c3 nu state, which illustrates the difference between the two forms of H2. This diagram does not show any details of the nuclear hyperfine splitting, which we will come to in due course. [Pg.436]

Foyt et al. [137] interpreted the quadrupole-splitting parameters of low-spin ruthenium(II) complexes in terms of a crystal field model in the strong-field approximation with the configuration treated as an equivalent one-electron problem. They have shown that, starting from pure octahedral symmetry with zero quadrupole splitting, A q increases as the ratio of the axial distortion to the spin-orbit coupling increases. [Pg.280]

For vanadocene second-order perturbation calculations of the spin-orbit contribution to the zero field splitting, DLS, showed the II ( 2) level to lie below A ( - ), but the estimated value, 1.4 to 1.5 cm-1, constitutes only about half of the observed result. How-... [Pg.116]

The first term is characterized by a scalar, 7, and it is the dominant term. Be aware of a convention disagreement in the definition of this term instead of -27, some authors write -7, or 7, or 27, and a mistake in sign definition will turn the whole scheme of spin levels upside down (see below). The second and third term are induced by anisotropic spin-orbit coupling, and their weight is predicted to be of order Ag/ge and (Ag/ge)2, respectively (Moriya 1960), when Ag is the (anisotropic) deviation from the free electron -value. The D in the second term has nothing to do with the familiar axial zero-field splitting parameter D, but it is a vector parameter, and the x means take the cross product (or vector product) an alternative way of writing is the determinant form... [Pg.189]

The ligand field was parameterised in terms of ea only, and values of this parameter, together with the spin-orbit coupling constant X, the orbital reduction factor k and the Racah parameter B were obtained by fitting the d-d spectra, zero-field splittings, principal magnetic susceptibilities and e.s.r. g-values. [Pg.110]

D is the zero-field splitting tensor, a traceless, rank-two tensorial quantity. The ZFS tensor is a property of a molecule or a paramagnetic complex, with its origin in the mixing of the electrostatic and spin-orbit interactions (80). In addition, the dipole dipole interaction between individual electron spins can contribute to the ZFS (81), but this contribution is believed to be unimportant... [Pg.63]


See other pages where Zero-field spin-orbit splitting is mentioned: [Pg.104]    [Pg.115]    [Pg.45]    [Pg.193]    [Pg.226]    [Pg.126]    [Pg.127]    [Pg.490]    [Pg.436]    [Pg.907]    [Pg.226]    [Pg.2653]    [Pg.2662]    [Pg.159]    [Pg.211]    [Pg.122]    [Pg.123]    [Pg.177]    [Pg.277]    [Pg.441]    [Pg.105]    [Pg.107]    [Pg.111]    [Pg.116]    [Pg.117]    [Pg.269]    [Pg.94]    [Pg.225]    [Pg.209]    [Pg.88]    [Pg.490]    [Pg.127]    [Pg.41]    [Pg.69]    [Pg.125]    [Pg.127]    [Pg.111]    [Pg.117]    [Pg.123]    [Pg.165]    [Pg.77]    [Pg.327]   
See also in sourсe #XX -- [ Pg.4 , Pg.2652 ]




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Field Splittings

Orbit, splitting

Orbital splitting

Spin-orbit splitting

Spin-orbit splittings

Zero field splitting

Zero-field

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