IR multiphoton pumping of optically selected levels of the approx. A /sup 1/A/sub 2/ state of thiophosgene
Below approx. 3400 cm/sup -1/ of excess vibrational energy relative to the origin, the quantum yield of fluorescence is unity independent of vibronic level. Above approx. 3400 cm/sup -1/, the lifetime suddenly changes from 35.mu.s to < 100ns. The approx. A /sup 1/A/sub 2/ state absorbs IR photons...
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ftosti:oai:osti.gov:6502825 2023-07-30T04:02:55+02:00 IR multiphoton pumping of optically selected levels of the approx. A /sup 1/A/sub 2/ state of thiophosgene Brenner, D M 2013-08-26 application/pdf http://www.osti.gov/servlets/purl/6502825 https://www.osti.gov/biblio/6502825 unknown http://www.osti.gov/servlets/purl/6502825 https://www.osti.gov/biblio/6502825 37 INORGANIC ORGANIC PHYSICAL AND ANALYTICAL CHEMISTRY 42 ENGINEERING PHOSGENE OPTICAL PUMPING CARBON DIOXIDE LASERS FLUORESCENCE INFRARED RADIATION LASER RADIATION VIBRATIONAL STATES CARBONIC ACID DERIVATIVES ELECTROMAGNETIC RADIATION ENERGY LEVELS EXCITED STATES GAS LASERS LASERS LUMINESCENCE ORGANIC CHLORINE COMPOUNDS ORGANIC COMPOUNDS ORGANIC HALOGEN COMPOUNDS PUMPING RADIATIONS 2013 ftosti 2023-07-11T10:49:04Z Below approx. 3400 cm/sup -1/ of excess vibrational energy relative to the origin, the quantum yield of fluorescence is unity independent of vibronic level. Above approx. 3400 cm/sup -1/, the lifetime suddenly changes from 35.mu.s to < 100ns. The approx. A /sup 1/A/sub 2/ state absorbs IR photons, probably via the 2 .nu./sub 2/ mode, in the 10.6.mu. wavelength region of the CO/sub 2/ laser. There is no obvious dependence of the predissociation yield on the vibrational energy content of the initial state. At 2900 cm/sup -1/ where the density of states is approx. 1 cm/sup -1/, the predissociation yield is wavelength dependent and the oscillator strength is very low. With increasing vibrational energy of the initial state, the predissociation yield does not increase. There is no obvious dependence on fluence. The dependence on laser intensity is neither quartic nor linear. Other/Unknown Material Carbonic acid SciTec Connect (Office of Scientific and Technical Information - OSTI, U.S. Department of Energy) |
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37 INORGANIC ORGANIC PHYSICAL AND ANALYTICAL CHEMISTRY 42 ENGINEERING PHOSGENE OPTICAL PUMPING CARBON DIOXIDE LASERS FLUORESCENCE INFRARED RADIATION LASER RADIATION VIBRATIONAL STATES CARBONIC ACID DERIVATIVES ELECTROMAGNETIC RADIATION ENERGY LEVELS EXCITED STATES GAS LASERS LASERS LUMINESCENCE ORGANIC CHLORINE COMPOUNDS ORGANIC COMPOUNDS ORGANIC HALOGEN COMPOUNDS PUMPING RADIATIONS |
spellingShingle |
37 INORGANIC ORGANIC PHYSICAL AND ANALYTICAL CHEMISTRY 42 ENGINEERING PHOSGENE OPTICAL PUMPING CARBON DIOXIDE LASERS FLUORESCENCE INFRARED RADIATION LASER RADIATION VIBRATIONAL STATES CARBONIC ACID DERIVATIVES ELECTROMAGNETIC RADIATION ENERGY LEVELS EXCITED STATES GAS LASERS LASERS LUMINESCENCE ORGANIC CHLORINE COMPOUNDS ORGANIC COMPOUNDS ORGANIC HALOGEN COMPOUNDS PUMPING RADIATIONS Brenner, D M IR multiphoton pumping of optically selected levels of the approx. A /sup 1/A/sub 2/ state of thiophosgene |
topic_facet |
37 INORGANIC ORGANIC PHYSICAL AND ANALYTICAL CHEMISTRY 42 ENGINEERING PHOSGENE OPTICAL PUMPING CARBON DIOXIDE LASERS FLUORESCENCE INFRARED RADIATION LASER RADIATION VIBRATIONAL STATES CARBONIC ACID DERIVATIVES ELECTROMAGNETIC RADIATION ENERGY LEVELS EXCITED STATES GAS LASERS LASERS LUMINESCENCE ORGANIC CHLORINE COMPOUNDS ORGANIC COMPOUNDS ORGANIC HALOGEN COMPOUNDS PUMPING RADIATIONS |
description |
Below approx. 3400 cm/sup -1/ of excess vibrational energy relative to the origin, the quantum yield of fluorescence is unity independent of vibronic level. Above approx. 3400 cm/sup -1/, the lifetime suddenly changes from 35.mu.s to < 100ns. The approx. A /sup 1/A/sub 2/ state absorbs IR photons, probably via the 2 .nu./sub 2/ mode, in the 10.6.mu. wavelength region of the CO/sub 2/ laser. There is no obvious dependence of the predissociation yield on the vibrational energy content of the initial state. At 2900 cm/sup -1/ where the density of states is approx. 1 cm/sup -1/, the predissociation yield is wavelength dependent and the oscillator strength is very low. With increasing vibrational energy of the initial state, the predissociation yield does not increase. There is no obvious dependence on fluence. The dependence on laser intensity is neither quartic nor linear. |
author |
Brenner, D M |
author_facet |
Brenner, D M |
author_sort |
Brenner, D M |
title |
IR multiphoton pumping of optically selected levels of the approx. A /sup 1/A/sub 2/ state of thiophosgene |
title_short |
IR multiphoton pumping of optically selected levels of the approx. A /sup 1/A/sub 2/ state of thiophosgene |
title_full |
IR multiphoton pumping of optically selected levels of the approx. A /sup 1/A/sub 2/ state of thiophosgene |
title_fullStr |
IR multiphoton pumping of optically selected levels of the approx. A /sup 1/A/sub 2/ state of thiophosgene |
title_full_unstemmed |
IR multiphoton pumping of optically selected levels of the approx. A /sup 1/A/sub 2/ state of thiophosgene |
title_sort |
ir multiphoton pumping of optically selected levels of the approx. a /sup 1/a/sub 2/ state of thiophosgene |
publishDate |
2013 |
url |
http://www.osti.gov/servlets/purl/6502825 https://www.osti.gov/biblio/6502825 |
genre |
Carbonic acid |
genre_facet |
Carbonic acid |
op_relation |
http://www.osti.gov/servlets/purl/6502825 https://www.osti.gov/biblio/6502825 |
_version_ |
1772813810293276672 |