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Planarizing cytosine: The S1 state structure, vibrations, and nonradiative dynamics of jet-cooled 5,6-trimethylenecytosine.

Authors :
Trachsel, Maria A.
Lobsiger, Simon
Schär, Tobias
Blancafort, Lluís
Leutwyler, Samuel
Source :
Journal of Chemical Physics; 2017, Vol. 146 Issue 24, p1-12, 12p, 5 Diagrams, 5 Charts, 7 Graphs
Publication Year :
2017

Abstract

We measure the S<subscript>0</subscript>→S<subscript>1</subscript> spectrum and time-resolved S<subscript>1</subscript> state nonradiative dynamics of the 'clamped' cytosine derivative 5,6-trimethylenecytosine (TMCyt) in a supersonic jet, using two-color resonant two-photon ionization (R2PI), UV/UV holeburning, and ns time-resolved pump/delayed ionization. The experiments are complemented with spin-component scaled second-order approximate coupled cluster (SCS-CC2), time-dependent density functional theory, and multi-state second-order perturbation-theory (MS-CASPT2) ab initio calculations. While the R2PI spectrum of cytosine breaks off ~500 cm<superscript>1</superscript> above its 0<superscript>0</superscript><subscript>0</subscript> band, that of TMCyt extends up to +4400 cm<superscript>-1</superscript> higher, with over a hundred resolved vibronic bands. Thus, clamping the cytosine C<superscript>5</superscript>-C<superscript>6</superscript> bond allows us to explore the S<subscript>1</subscript> state vibrations and S<subscript>0</subscript>→S<subscript>1</subscript> geometry changes in detail. The TMCyt S<subscript>1</subscript> state out-of-plane vibrations v'<subscript>1</subscript>, v'<subscript>3</subscript>, and v'<subscript>5</subscript> lie below 420 cm<superscript>-1</superscript>, and the in-plane v'<subscript>11</subscript>, v'<subscript>12</subscript>, and v'<subscript>23</subscript> vibrational fundamentals apper at 450, 470, and 944 cm<superscript>-1</superscript>. S<subscript>0</subscript> → S<subscript>1</subscript> vibronic simulations based on SCS-CC2 calculations agree well with experiment if the calculated v'<subscript>1</subscript>, v'<subscript>3</subscript> , and v'<subscript>5</subscript> frequencies are reduced by a factor of 2-3. MS-CASPT2 calculations predict that the ethylene-type S<subscript>1</subscript> S<subscript>0</subscript> conical intersection (CI) increases from +366 cm<superscript>-1</superscript> in cytosine to >6000 cm<superscript>-1</superscript> in TMCyt, explaining the long lifetime and extended S<subscript>0</subscript>→S<subscript>1</subscript> spectrum. The lowest-energy S<subscript>1</subscript> S<subscript>0</subscript> CI of TMCyt is the "amino out-of-plane" (OP<subscript>X</subscript>) intersection, calculated at +4190 cm<superscript>-1</superscript>. The experimental S<subscript>1</subscript> S<subscript>0</subscript> internal conversion rate constant at the S<subscript>1</subscript>(v' = 0) level is k<subscript>IC</subscript> = 0.98-2.2 10<superscript>8</superscript> s<superscript>-1</superscript>, which is ~10 times smaller than in 1-methylcytosine and cytosine. The S<subscript>1</subscript>(v' = 0) level relaxes into the T<subscript>1</subscript>(<superscript>3</superscript>ππ*) state by intersystem crossing with k<subscript>ISC</subscript> = 0.41-1.6 10<superscript>8</superscript> s<superscript>-1</superscript>. The T<subscript>1</subscript> state energy is measured to lie 24 580 ± 560 cm<superscript>-1</superscript> above the S<subscript>0</subscript> state. The S<subscript>1</subscript>(v' = 0) lifetime is = 2.9 ns, resulting in an estimated fluorescence quantum yield of ϕ<subscript>fl</subscript> = 24%. Intense two-color R2PI spectra of the TMCyt amino-enol tautomers appear above 36 000 cm<superscript>-1</superscript>. A sharp S<subscript>1</subscript> ionization threshold is observed for amino-keto TMCyt, yielding an adiabatic ionization energy of 8.114 ± 0.002 eV. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
00219606
Volume :
146
Issue :
24
Database :
Complementary Index
Journal :
Journal of Chemical Physics
Publication Type :
Academic Journal
Accession number :
123826594
Full Text :
https://doi.org/10.1063/1.4989465