Back to Search
Start Over
Intersystem crossing rates of S1 state keto-amino cytosine at low excess energy.
- Source :
- Journal of Chemical Physics; 2015, Vol. 143 Issue 23, p1-12, 12p, 2 Diagrams, 4 Charts, 6 Graphs
- Publication Year :
- 2015
-
Abstract
- The amino-keto tautomer of supersonic jet-cooled cytosine undergoes intersystem crossing (ISC) from the v = 0 and low-lying vibronic levels of its S<subscript>1</subscript>(¹ππ*) state. We investigate these ISC rates experimentally and theoretically as a function of S<subscript>1</subscript> state vibrational excess energy E<subscript>exc</subscript>. The S<subscript>1</subscript> vibronic levels are pumped with a ~5 ns UV laser, the S<subscript>1</subscript> and triplet state ion signals are separated by prompt or delayed ionization with a second UV laser pulse. After correcting the raw ISC yields for the relative S<subscript>1</subscript> and T<subscript>1</subscript> ionization cross sections, we obtain energy dependent ISC quantum yields Q<subscript>ISC</subscript><superscript>corr</superscript>=1%-5%. These are combined with previously measured vibronic state-specific decay rates, giving ISC rates k<subscript>ISC</subscript> = 0.4-1.5 · 10<superscript>9</superscript> s<superscript>-1</superscript>, the corresponding S<subscript>1</subscript> ⇝S<subscript>0</subscript> internal conversion (IC) rates are 30-100 times larger. Theoretical ISC rates are computed using SCS-CC2 methods, which predict rapid ISC from the S<subscript>1</subscript>; v = 0 state with k<subscript>ISC</subscript> = 3. 10<superscript>9</superscript> s<superscript>-1</superscript> to the T<subscript>1</subscript>(3ππ*) triplet state. The surprisingly high rate of this El Sayed-forbidden transition is caused by a substantial admixture of ¹n<subscript>O</subscript>π* character into the S<subscript>1</subscript>(¹ππ*) wave function at its non-planar minimum geometry. The combination of experiment and theory implies that (1) below E<subscript>exc</subscript> = 550 cm<superscript>-1</superscript> in the S<subscript>1</subscript> state, S<subscript>1</subscript> ⇝S<subscript>0</subscript> internal conversion dominates the nonradiative decay with k<subscript>IC</subscript> ≥ 2 . 10<superscript>10</superscript> s<superscript>-1</superscript>, (2) the calculated S<subscript>1</subscript>⇝T<subscript>1</subscript> (¹π#960;*³ππ*) ISC rate is in good agreement with experiment, (3) being El-Sayed forbidden, the S<subscript>1</subscript> ⇝ T<subscript>1</subscript> ISC is moderately fast (k<subscript>ISC</subscript> = 3. 10<superscript>9</superscript> s<superscript>-1</superscript>), and not ultrafast, as claimed by other calculations, and (4) at E<subscript>exc</subscript> ~ 550 cm<superscript>-1</superscript> the IC rate increases by ~50 times, probably by accessing the lowest conical intersection (the C5-twist CI) and thereby effectively switching off the ISC decay channels. [ABSTRACT FROM AUTHOR]
Details
- Language :
- English
- ISSN :
- 00219606
- Volume :
- 143
- Issue :
- 23
- Database :
- Complementary Index
- Journal :
- Journal of Chemical Physics
- Publication Type :
- Academic Journal
- Accession number :
- 111947446
- Full Text :
- https://doi.org/10.1063/1.4937375