Theory of the Spin Hamiltonian Parameters for Low Spin Cobalt(II) Complexes

1975 ◽  
Vol 53 (16) ◽  
pp. 2498-2511 ◽  
Author(s):  
B. R. McGarvey

The theory for the spin Hamiltonian parameters of low spin cobalt(II), d7, complexes has been developed to third order in perturbation theory for all reasonable ground states. Two extensions beyond previous treatments have been made: (1) the spin–orbit mixing of excited quartet states into the doublet ground state has been considered and (2) configuration interaction involving mixing of [Formula: see text]orbitals in lower symmetry has been included. In the case of axial complexes a more complete calculation has been made to assess the errors incurred in only going to third order in perturbation theory. The theory has been applied to porphyrin and phthalocyanine complexes and is shown to adequately account for the observed data on these complexes. The excited quartet states are much higher in energy than the ground state for the four coordinate porphyrin complexes but become much lower in energy when basic adducts are complexed along the z axis. Further there is mixing of the 4s orbital with the [Formula: see text]orbital for the four coordinate complexes which is completely removed when basic adducts are complexed to the porphyrin system. Application of equations to lower symmetry complexes is considered and it is shown that is is difficult to make an unambiguous assignment of ground state on the basis of g and 59Co hyperfine splitting values alone, although the relative values of gy and gz do seem to provide some clue as to the correct ground state.

2017 ◽  
Vol 31 (02) ◽  
pp. 1650262
Author(s):  
Chao Tu ◽  
Linhua Xie ◽  
Xiangrong Du

The spin Hamiltonian parameters of VO[Formula: see text] in KZnClSO[Formula: see text]3H2O single crystals are calculated from the third-order perturbation formulas based on the double spin–orbit coupling model for the tetragonal transition-ion clusters in crystals with the ground state [Formula: see text]. In the paper, both the crystal-field (CF) mechanism and the charge-transfer (CT) mechanism (double-mechanism model) are considered to calculate the spin Hamiltonian parameters. The calculated results are in agreement with the experimental data. Moreover, the calculated results show that the CT mechanism cannot be omitted for a high-valence state V[Formula: see text] ions in KZnClSO[Formula: see text]3H2O single crystals. The tetragonal field parameters are also acquired in the paper.


2003 ◽  
Vol 42 (17) ◽  
pp. 5293-5303 ◽  
Author(s):  
David Collison ◽  
Mark Murrie ◽  
Vasily S. Oganesyan ◽  
Stergios Piligkos ◽  
Nigel R. J. Poolton ◽  
...  

In Cs 2 NaHoCl 6 the Ho 3+ ion occupies a site of cubic symmetry, and the ground state produced by the crystal field splitting of the 4f 10 , 5 I 8 manifold is a ‘non-magnetic’ Γ 3 doublet. When a field B is applied, the doublet is split by the quadratic Zeeman effect, and transitions between the two levels of the doublet become allowed at a frequency and with an intensity each proportional to B 2. At a frequency of 9.6 GHz the e. s. r. spectrum of the Ho 3+ ion shows a single broad line, with the unusual anisotropic behaviour predicted for a Γ 3 doublet in cubic symmetry (see paper I). No hyperfine splitting is resolved, and the linewidth parameter ∆ v is of order 10 GHz, independent of orientation. The centre of the line occurs at a field consistent with that calculated from n. m. r. measurements (paper II), after a correction is applied for the anomalous line shape. The e. s. r. spectra of Gd 3+ , Dy 3+ , Er 3+ , Yb 3+ , present as impurities, also show cubic symmetry, with spin Hamiltonian parameters close to those observed in analogous compounds such as Cs 2 NaYCl 6 .


1964 ◽  
Vol 17 (4) ◽  
pp. 537 ◽  
Author(s):  
SP Burley

The allowed and forbidden paramagnetic resonance transitions of MnH ions in single crystals of apatite [CalO(PO.). (F, CI)] and smithsonite [ZnCO.] have been investigated. The spin Hamiltonian parameters, describing the spectra observedat 300oK, were found from a third-order perturbation-theory estimate of the eigenvalues, calculated for the cases in which the magnetic field was parallel and perpendicular to the trigonal axis. Since in the case of apatite the D term was not very small compared with the Zeeman term, it had to be included also in the zeroth-order Hamiltonian.


1998 ◽  
Vol 53 (9) ◽  
pp. 779-782
Author(s):  
F. Köksal ◽  
İ. Kartal ◽  
A. Gençten

Abstract The electron paramagnetic resonance spectra of Cu2+ doped Na2HAsO4 ·7H2O single crystals were studied at room temperature. The results indicate the substitutional entrance of Cu2+ in two magnetically inequivalent Na+ sites. Charge compensation is supposed to be fulfilled by proton vacancies. The spin Hamiltonian parameters were determined. The ground state for Cu2+ seems to indicate the dominance of the dz² orbital and therefore a compression of the distorted octahedron along its C4v axis.


1986 ◽  
Vol 39 (7) ◽  
pp. 1029 ◽  
Author(s):  
P Comba ◽  
AM Sargeson

An e.p.r . study of the cage complex [VIVdi(amH)sar-2H]4+ gives spin Hamiltonian parameters gX 1.974, gy 1.967, gZ 1.991, giso 1.977, AX 92×10-4 cm-1, Ay 100×10-4 cm-1, AZ 13×10-4 cm-1, Aiso 68×10-4 cm-1, viz. gX ≈ gy < gZ ≈ 2.0 and AX ≈ Ay > AZ. This is consistent with the metal centre approaching a trigonal prismatic environment and a 2A1 (D3) ground state, viz. ...d1/z2. Comparison of the spin Hamiltonian parameters from measurements in frozen and fluid solution, poly(vinyl alcohol) films and dilute powder [VIVdi(amH)sar-2H]4+ doped into the lattice of the protonated ZnII salt over a large temperature range indicates that the structures in solution and in the solid state are virtually identical. The results are discussed in relation to the known structure of the ion in the lattice [vIVdi(amH)sar -2H](S2O6)2, the sites of deprotonation of the coordinated amines and in relation to the trigonal and small rhombic distortions of the complex.


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