Photolysis of 1-C4H9I and 2-C4H9I at 266 nm: Direct Observation of the Effect of Branching on the Photodissociation Mechanism
Velocity ion imaging (see figure) is used to analyze the photodissociation mechanism of 1‐C4H9I (left image) and 2‐C4H9I (right image) at 266 nm. For 2‐C4H9I, a new channel for formation of I and I* atoms is observed. It is attributed to the repulsive mode along the CI stretch, coupled with some be...
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Published in | Chemphyschem Vol. 10; no. 5; pp. 830 - 834 |
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Main Authors | , , , , , |
Format | Journal Article |
Language | English |
Published |
Weinheim
WILEY-VCH Verlag
23.03.2009
WILEY‐VCH Verlag Wiley |
Subjects | |
Online Access | Get full text |
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Summary: | Velocity ion imaging (see figure) is used to analyze the photodissociation mechanism of 1‐C4H9I (left image) and 2‐C4H9I (right image) at 266 nm. For 2‐C4H9I, a new channel for formation of I and I* atoms is observed. It is attributed to the repulsive mode along the CI stretch, coupled with some bending motions.
Photodissociation dynamics of 1‐C4H9I and 2‐C4H9I at 266 nm is investigated by velocity ion imaging. Photodissociation channels of 1‐C4H9I and 2‐C4H9I are analyzed and compared. For 1‐C4H9I the photodissociation dynamics only correlates with direct dissociation via repulsive surfaces. While for 2‐C4H9I, a new formation channel of I and I* atoms is observed. It is attributed to the repulsive mode along the CI stretch, coupled with some bending motions. As the alkyl group becomes more branched, the contribution of bending modes to I and I* is much more obvious in the photodissociation of 2‐C4H9I than in that of 1‐C4H9I. Additionally, the curve‐crossing probability between 3Q0 and 1Q1 increases greatly with branching, from 0.31 for 1‐C4H9I to 0.70 for 2‐C4H9I in the prompt dissociation channel; the relative quantum yield for I* decreases strongly with branching, from 0.65 for 1‐C4H9I to 0.28 for 2‐C4H9I.
Velocity ion imaging (see figure) is used to analyze the photodissociation mechanism of 1‐C4H9I (left image) and 2‐C4H9I (right image) at 266 nm. For 2‐C4H9I, a new channel for formation of I and I* atoms is observed. It is attributed to the repulsive mode along the CI stretch, coupled with some bending motions. |
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Bibliography: | ArticleID:CPHC200800742 ark:/67375/WNG-NG4ZC7PG-8 National Natural Science Foundation of China - No. 20703061 istex:5722D4FBCEAE5620A30BBB07DAB970774E7A4288 ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 1439-4235 1439-7641 |
DOI: | 10.1002/cphc.200800742 |