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Self-assembled Transition Metal Coordination Frameworks of ...

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Chapter 5<br />

Broad signals above g=2, due to the S =5/2 ZFS has been reported for<br />

distorted mononuclear octahedral Mn(H) [38] and dimanganese(Il) complexes [39].<br />

So, here the presence <strong>of</strong> dinuclear species is hard to prove, as the same broad EPR<br />

features may also arise from ZF S <strong>of</strong> mononuclear species [3]. Alternatively, partial<br />

decomposition <strong>of</strong> the dimer to mononuclear species by the coordinating solvent may<br />

give same result [3].<br />

The spectra <strong>of</strong> 21 and 22 are more close to Mn(H) monomeric species, due to<br />

possible decomposition to monomeric units, and similar to each other. The six line<br />

manganese hyperfine pattem centered at g =l.995 for both compounds are in<br />

accordance with the Mn(H) ions in an environment close to octahedral symmetry and<br />

is known to arise from the transition between the energy levels <strong>of</strong> the lower doublet.<br />

This is usually observed with complexes <strong>of</strong> weak field ligands, which give only one<br />

g value close to 2.0023, the fiee electron g value.<br />

The magnitude <strong>of</strong> the hyperfine splitting A estimated to be approximately<br />

264 MHz (94.5 G) for complex 21 and 265 MHz (94.9 G) for 22 are consistent with<br />

octahedral coordination [36]. It is seen that the Am values are somewhat lower than<br />

those <strong>of</strong> the pure ionic compounds. The average separations <strong>of</strong> the forbidden<br />

hyperfine lines lying between each <strong>of</strong> the two main hyperfine lines in the spectra are<br />

approximately 55.8 MHz (20 G) for both compounds. For both the compounds, a D<br />

value <strong>of</strong> 400 MHZ (1.3343>

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