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. Author manuscript; available in PMC: 2015 Jun 1.
Published in final edited form as: Int J Radiat Biol. 2014 Feb 10;90(6):433–445. doi: 10.3109/09553002.2014.884293

Figure 3.

Figure 3

Spectrum (A) of T(−H)• produced via annealing at 155 K owing to one-electron oxidation of the N3-deprotonated thymine base in 5′-TMP (3 mg/ml) by Cl2 in homogeneous aqueous glass (7.5 M LiCl/D2O) at pD ca. 10 in the presence of excess K2S2O8 ; (B) after photoexcitation of T(−H)• in 5′-TMP shown in (A) using 405 nm laser at 143 K for 40 min; (C) after photoexcitation of T(−H)• in a matched sample of 5′-TDP (3 mg/ml) using 405 nm laser at 143 K for 40 min; (D) after photoexcitation of T(−H)• -of T(−H)• in a matched sample of 5′-TTP (3 mg/ml) using 405 nm laser at 143 K for 40 min; (E) after visible illumination of T(−H)• formed in a similarly prepared sample of Thd (3 mg/ml) at pD ca. 11 at 143 K. (F) The simulated C3′• spectrum has been obtained using three isotropic β-proton HFCC (text). The line components of the C3′• spectrum is visible in spectra (B) to (E) as indicated by the dotted lines. Similar to the results found in Figure 2 and reaction (5), a small extent of Cl2 (ca. 10%) formed via one-electron oxidation of the matrix (LiCl) by (T(−H)•)* has been subtracted from each of the experimentally recorded spectra and the subtracted spectra have been presented in Figures 3(B) to 3(E).