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CMDITR Review of Undergraduate Research - Pluto - University of ...

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Figure 2: The experimental high-resolution EPR<br />

spectrum <strong>of</strong> (13) in benzene at room temperature<br />

is shown above the simulated best-fit spectrum<br />

obtained with the WinSim program<br />

shifted, appearing closer to 600 nm; accordingly,<br />

(13) forms a maroon-colored solution in<br />

benzene, whereas the parent BNN radical forms<br />

a lime-green solution in benzene. The<br />

bathochromic shift in the absorbance spectrum <strong>of</strong><br />

(13), together with its unique maroon color,<br />

signifies a smaller energy gap between the<br />

ground and excited states <strong>of</strong> (13) relative to the<br />

parent BNN radical, which is logical,<br />

considering that the bromine and thiophene<br />

moieties <strong>of</strong> (13) are significantly electron-rich<br />

moieties that increase the energy <strong>of</strong> the HOMO<br />

<strong>of</strong> (13). The X-band (9.3 GHz) EPR spectrum <strong>of</strong><br />

(13) was obtained at room temperature in an<br />

oxygen-free benzene solution (the EPR sample<br />

was degassed with nitrogen in order to avoid<br />

dipolar broadening that is caused by the presence<br />

<strong>of</strong> oxygen in solution). The EPR spectrum <strong>of</strong><br />

(13) is characterized by the hyperfine coupling <strong>of</strong><br />

the unpaired electron with two equivalent 14 N<br />

nuclei (I = 1); one bromine ( 79 Br / 81 Br) nucleus<br />

(I = 3/2); and aromatic protons (I = 1/2) in the<br />

benzimidazole ring, the 2-phenyl substituent, and<br />

the thiophene ring. The g-factor for (13) was<br />

found to be 2.0085. The experimental nitrogen<br />

(a N ), hydrogen (a H ), and bromine (a Br ) hyperfine<br />

coupling constants (hfccs) 9 are provided in Table<br />

1. The experimental hfccs, as well as the<br />

calculated spin densities for (13) show that the<br />

unpaired electron is only slightly delocalized<br />

onto the thiophene moiety – in fact, the phenyl<br />

substituent in the 2-position contains more spin<br />

density than the thiophene moiety. Overall, the<br />

majority <strong>of</strong> the spin density <strong>of</strong> (13) is found on<br />

the two NO groups and the bromine atom.<br />

Relative to the parent BNN radical, the nitrogen<br />

hfcc <strong>of</strong> (13), as well as the hydrogen hfccs <strong>of</strong> its<br />

annelated phenyl ring, is slightly smaller, thus<br />

signifying a reduction in the amount <strong>of</strong> spin<br />

density present on these moieties.<br />

Curiously, (13) is considerably less stable<br />

relative to the parent BNN radical: while BNN<br />

radicals are stable in solution for upwards <strong>of</strong> 2<br />

18 <strong>CMDITR</strong> <strong>Review</strong> <strong>of</strong> <strong>Undergraduate</strong> <strong>Research</strong> Vol. 1 No. 1 Summer 2004

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