Dissociation dynamics of thiolactic acid at 193 nm: Detection of the nascent OH product by laser-induced fluorescence

2004 ◽  
Vol 120 (15) ◽  
pp. 6964-6972 ◽  
Author(s):  
Kumbil K. Pushpa ◽  
Hari P. Upadhyaya ◽  
Awadhesh Kumar ◽  
Prakash D. Naik ◽  
Paramanand Bajaj ◽  
...  
2009 ◽  
Vol 113 (30) ◽  
pp. 8462-8470 ◽  
Author(s):  
Yogesh N. Indulkar ◽  
Hari P. Upadhyaya ◽  
Awadhesh Kumar ◽  
Suresh B. Waghmode ◽  
Prakash D. Naik

1995 ◽  
Vol 102 (11) ◽  
pp. 4447-4460 ◽  
Author(s):  
Simon W. North ◽  
David A. Blank ◽  
J. Daniel Gezelter ◽  
Cheryl A. Longfellow ◽  
Yuan T. Lee

2019 ◽  
Vol 151 (17) ◽  
pp. 174303
Author(s):  
Erin N. Sullivan ◽  
Bethan Nichols ◽  
Stephen von Kugelgen ◽  
Gabriel da Silva ◽  
Daniel M. Neumark

ChemInform ◽  
2010 ◽  
Vol 22 (49) ◽  
pp. no-no
Author(s):  
M. EBBEN ◽  
M. VERSLUIS ◽  
J. J. TER MEULEN

1987 ◽  
Vol 101 ◽  
Author(s):  
P.D. Brewer ◽  
J.E. Jensen ◽  
G.L. Olson ◽  
L.W. Tutt ◽  
J.J. Zinck

ABSTRACTThe UV photodissociations of dimethyltelluride (CH3)2Te and diethyltelluride (C2Hs)2Te have been investigated by state-selective detection. Nascent populations of Te(5p Pjw) atoms produced by the photodissociation process were monitored using laser-induced fluorescence following excimer laser (248 nm and 193 nm) photolysis. Experimental results for both molecules indicate that the photolysis at 248 nm produces Te atoms via a single photon process and that the liberated Te atoms populate only the 5p3P2 state. The photolysis of diethyltelluride at 193 nm has also been found to be a single photon process producing Te atoms distributed over the 3P2, 3P1, and Pø states in a ratio of 13:2:1, respectively.


1993 ◽  
Vol 13 (1) ◽  
pp. 43-55 ◽  
Author(s):  
G. Wlnkelmann ◽  
R. Kuhls ◽  
R. Osmanow ◽  
E. Linke

KrF–laser-induced fluorescence from CF2-radicals was investigated during photolysis of CF2Cl2 and CF2HCl by 193 nm laserlight. In contrast to other publications, which postulated single-vibronic-level fluorescence, the fluorescence is caused by excitation from four closely situated absorption bands. These fluorescence bands of four series, are assigned to Ã1B1(v′1,6−2v′1,0) − X˜1A1(v″1,v″2,0) transitions with Δv1=0 and 0 ≤ v″2 ≤ 30. The Franck – Condon factors of the Ã1B1 (0, 6, 0) –X˜1A1 (0, v″2, 0) transitions, the frequencies of the bending vibration (ω″2 =673± 2cm–1) and the anharmonicity constants x″22 = –0.94 ± 0.08 cm-1 and x′22 = –0.44 ± 0.10 cm–1 were more precisely determined. For the first time higher anharmonicity constants are evaluated with x″12 + x″112 = –3.5 ± 1.0 cm–1 and x″122= –0.05 ± 0.02 cm–1.


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