2013
DOI: 10.1016/j.cplett.2013.03.073
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On the excitation wavelength dependence and Arrhenius behavior of stilbene isomerization rates in solution

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Cited by 24 publications
(42 citation statements)
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“…Figure 2A shows the evolution of the transient absorption spectrum of trans-stilbene following excitation with one-photon at 310 nm (total energy of 4.0 eV). Consistent with earlier studies, 8,12,15,18,[60][61][62] the TA spectrum is dominated by an excited-state absorption (ESA) band centered near 585 nm and a weaker stimulated emission (SE) band near 365 nm. The asymmetry of the ESA band, including a weak shoulder near 550 nm, was previously assigned as a vibronic progression in the S n ←S 1 transition.…”
Section: Excited-state Dynamics Following One-and Two-photon Excitationsupporting
confidence: 88%
“…Figure 2A shows the evolution of the transient absorption spectrum of trans-stilbene following excitation with one-photon at 310 nm (total energy of 4.0 eV). Consistent with earlier studies, 8,12,15,18,[60][61][62] the TA spectrum is dominated by an excited-state absorption (ESA) band centered near 585 nm and a weaker stimulated emission (SE) band near 365 nm. The asymmetry of the ESA band, including a weak shoulder near 550 nm, was previously assigned as a vibronic progression in the S n ←S 1 transition.…”
Section: Excited-state Dynamics Following One-and Two-photon Excitationsupporting
confidence: 88%
“…The amplitude ratios of the two components Aa A b % 0:1 , which are approximately determined by k 1 k À1 , indicate that the equilibrium is strongly favored for the 1 t* state and that t À1 % t a and t 1 %10 t a . The much slower forward barrier crossing times in both solvents ($700 ps in CHX and $1300 ps in HXD) than those found for bare trans-stilbene in non-viscous solvents ($100 ps) [34,47] suggests a higher barrier for the ethylenic bond twisting in the trans form of the DMANS S 1 state. The slower barrier crossing rate in HXD than that in CHX is consistent with the fact that the former has a much higher viscosity.…”
Section: Excited-state Deactivation Mechanism In Nonpolar Solventsmentioning
confidence: 70%
“…Photoexcitation launches a wave packet on this potential energy surface based on the amount of vibrational energy deposited by excitation (above the 0−1 transition energy). The excitationwavelength dependence of stilbene photoisomerization is heavily influenced by vibrational motion along the isomerization coordinate 94 increasing the rate and quantum yield in solution compared to those in the gas phase. The barrierless isomerization in rhodopsin is also dependent on wavelength because of excited-state vibrational wave packets, 95 with a significant drop in yields above 500 nm.…”
Section: ■ Discussionmentioning
confidence: 99%