03.08.2013 Views

Self-assembled Transition Metal Coordination Frameworks of ...

Self-assembled Transition Metal Coordination Frameworks of ...

Self-assembled Transition Metal Coordination Frameworks of ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Chapter 5<br />

value <strong>of</strong> 265 MI-lz (94.9 G) at g=l.995 is consistent with octahedral coordination<br />

[36]. The average separation <strong>of</strong> the forbidden hyperfine lines lying between each <strong>of</strong><br />

the two main hyperfine lines in the spectrum is approximately 55.8 Ml-lz (20 G). A D<br />

value <strong>of</strong> 460 MHz (1 .5344xl0'2 cm“, 164.74 G) was used for simulation.<br />

* i<br />

I<br />

I I I<br />

20 I20 220 Q0 420<br />

5, h\Tl<br />

L___ I _ l_ . . I _ _l_ L . I . ._ _I<br />

280 330 $0 340 $0 $0 430 420<br />

B, WT]<br />

Fig. 5.7. The sextet part at g=l.995 <strong>of</strong> EPR spectrum <strong>of</strong> 19 (black) and its<br />

simulation (blue). The inset shows the full spectrum.<br />

The EPR spectrum <strong>of</strong> 20 also shows some features including a well-defined<br />

sextet pattern at g =1.995 . Another g value at 5.074 is also clear in the spectrum. For<br />

a dinuclear coupled Mn(II) system an eleven-line hyperfine pattern<br />

[2n1+1=4(5/2)+l=l1] with additional features are expected. However, the origin <strong>of</strong><br />

210

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!