Fluorescence lifetime studies of NO2. IV. Temperature dependence of fluorescence spectra and of collisional quenching of fluorescence

1980 ◽  
Vol 73 (4) ◽  
pp. 1514-1520 ◽  
Author(s):  
D. G. Keil ◽  
V. M. Donnelly ◽  
F. Kaufman
Author(s):  
Peter P. Knox ◽  
Vladimir V. Gorokhov ◽  
Boris N. Korvatovsky ◽  
Nadezhda P. Grishanova ◽  
Sergey N. Goryachev ◽  
...  

2021 ◽  
Vol 498 (1) ◽  
pp. 170-176
Author(s):  
V. V. Gorokhov ◽  
B. N. Korvatovsky ◽  
P. P. Knox ◽  
N. P. Grishanova ◽  
S. N. Goryachev ◽  
...  

1988 ◽  
Vol 66 (3) ◽  
pp. 491-494 ◽  
Author(s):  
J. C. Scaiano ◽  
D. Weir

The fluorescence spectra of a series of ring-substituted diarylcarbenes have been examined. The solution spectra are generally red shifted by 25–30 nm with respect to the band positions in matrices at 77 K. The difference is believed to reflect emission from non-relaxed conformations at 77 K. Both electron-withdrawing and -donating substituents lead to red shifts in the emission. These shifts are essentially additive, and the carbene emission data show an excellent correlation with free radical fluorescence data for the corresponding diarylmethyl radicals. The temperature dependence of excited carbene lifetimes have been examined for a few representative examples.


2019 ◽  
Vol 9 (1) ◽  
Author(s):  
Avry Shirakov ◽  
Zeev Burshtein ◽  
Yehoshua Shimony ◽  
Eugene Frumker ◽  
Amiel A. Ishaaya

AbstractWe have measured the fluorescence quantum efficiency in Ti3+:sapphire single crystals between 150 K and 550 K. Using literature-given effective fluorescence lifetime temperature dependence, we show that the zero temperature radiative lifetime is (4.44 ± 0.04) μs, compared to the 3.85 μs of the fluorescence lifetime. Fluorescence lifetime thermal shortening resolves into two parallel effects: radiative lifetime shortening, and non-radiative transition rate enhancement. The first is due to thermally enhanced occupation of a ΔE = 1,700 cm−1 higher (top) electronic state of the upper multiplet, exhibiting a transition oscillator strength of f = 0.62, compared to only 0.013 of the bottom electronic state of the same multiplet. The non-radiative rate relates to multi-phonon decay transitions stimulated by the thermal phonon occupation. Thermal enhancement of the configuration potential anharmonicity is also observed. An empiric expression for the figure-of-anharmonicity temperature dependence is given as $$\hat{{\bf{H}}}$$Hˆ (T) = $$\hat{{\bf{H}}}$$Hˆ (0)(1 + β exp(−ℏωco /kBT )), where $$\hat{{\bf{H}}}$$Hˆ (0) = 0.276, β = 5.2, ℏωco = 908 cm−1, and kB is the Boltzmann constant.


2007 ◽  
Author(s):  
Martin Stark ◽  
Daniel Dörr ◽  
Alexander Ehlers ◽  
Daniel Sauer ◽  
Rainer Bückle ◽  
...  

2017 ◽  
Vol 25 (6) ◽  
pp. 6954 ◽  
Author(s):  
Harry Burton ◽  
Christopher Debardelaben ◽  
Wafa Amir ◽  
Thomas A. Planchon

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