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Self-assembled Transition Metal Coordination Frameworks of ...

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Manganese(II) complexes<br />

D and E , etc. The g values other than that at ~2 <strong>of</strong> 19 and 20 were calculated from<br />

the spectra without simulations. For all complexes, EPR spectral simulation was done<br />

by considering them as mononuclear Mn(II) systems, i.e. under the investigation<br />

conditions. The simulations <strong>of</strong> 19 (Fig. 5.7) and 20 (Fig. 5.8) are not matching well<br />

with mononuclear Mn(H) models, as they doesn’t show g values other than at ~2;<br />

however, the simulation at the hyperfine sextet could yield precise values <strong>of</strong> g and<br />

A , though the D -term might be unreliable, due to wrong model usage. However, the<br />

simulations <strong>of</strong> 21 (Fig. 5.9) and 22 (Fig. 5.10) are in well agreement with<br />

experimental spectra and suggesting the possible decomposition <strong>of</strong> these complexes in<br />

DMF.<br />

All manganese complexes, except 23, exhibit a resonance at g '~“- 2, show a six<br />

line hyperfine structure, which is due to the interaction <strong>of</strong> electron spin <strong>of</strong> manganese<br />

ions with its own nuclear spin [=5/2. The g value for the hyperfine splitting is<br />

indicative <strong>of</strong> the nature <strong>of</strong> bonding in the matrix. The strength <strong>of</strong> the hyperfine<br />

splitting depends on the matrix into which the ion is dissolved and is mainly<br />

determined by the electronegativety <strong>of</strong> the neighbors. This means a qualitative<br />

measure <strong>of</strong> the covalency <strong>of</strong> the bonding in the matrix that can be determined from the<br />

value <strong>of</strong> A ; the smaller the splitting, the more covalent the bonding <strong>of</strong> the anion. In<br />

the spectra <strong>of</strong> all the complexes additional forbidden lines are observed in between<br />

each <strong>of</strong> the two lines <strong>of</strong> the central hyperfine sextet. These lines are arising by the<br />

violation <strong>of</strong> Am|= :k() <strong>of</strong> allowed transitions (Am,= il, Am|= :l:0).<br />

The EPR spectrum <strong>of</strong> 19 exhibits a well-defined hyperfine sextet at g =1 .995.<br />

Several additional features can be observed including five other ESR resonances at<br />

g=7.l6l, g=4.002, g=3.239, g= 2.473 and g=l.582 as small disturbances. A<br />

similar, but along with two sets <strong>of</strong> eleven lines are reported for a dinuclear Mn(H)<br />

system in X-band frozen solution spectrum [35]. The hyperfine coupling constant<br />

209

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