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Self-assembled Transition Metal Coordination Frameworks of ...

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5.3.2. EPR spectral studies<br />

Manganese(lI) complexes<br />

High spin Mn(II) ion with five unpaired electrons (S=5/2) have an orbitally<br />

non-degenerate 6A, ground state. Also, all the excited states are far removed and hence<br />

the spin-orbit coupling is expected to be very small or unimportant and the zero field<br />

splitting should be rather small. Due to this remoteness <strong>of</strong> excited states, the g<br />

factors <strong>of</strong> Mn(H) species lie very close to the free electron g value.<br />

The static spin Hamiltonian used to describe the energies <strong>of</strong> states <strong>of</strong> a<br />

paramagnetic species in the ground state with an effective electron spin S and m nuclei<br />

with nuclear spins I is given [29] by,<br />

Ho =H£z<br />

M<br />

+HZFS<br />

"I<br />

+HHF +H~z +HNQ<br />

!\4 F§J P'\l I{ §1<br />

k=l 1>l/2<br />

5,3 0gs+sDs+ZsA,1,_ p,Zg,_,,B01,,+Z1,_1>,,1 ‘/2. In the case <strong>of</strong><br />

Mn(lI) the zer<strong>of</strong>ield splitting, term become relevant, which is given by<br />

§Ds = D[Sf - s(s +1)/31+ E(sj - sf)<br />

B0 is a vector describing the direction and strength <strong>of</strong> the permanent<br />

Q<br />

%<br />

magnetic field. The transpose is denoted with . The zero-field splitting term here<br />

ignores second-order contributions, which are only different from zero for symmetries<br />

207

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