Rydberg and valence state excitation dynamics: a velocity map imaging study involving the E–V state interaction in HBr

2015 ◽  
Vol 17 (16) ◽  
pp. 10468-10477 ◽  
Author(s):  
Dimitris Zaouris ◽  
Andreas Kartakoullis ◽  
Pavle Glodic ◽  
Peter C. Samartzis ◽  
Helgi Rafn Hróðmarsson ◽  
...  

Velocity map imaging and REMPI of HBr reveal multiphoton excitation mechanisms and the involvement of the Rydberg state in valence state interactions.

2019 ◽  
Vol 21 (41) ◽  
pp. 23017-23025 ◽  
Author(s):  
Sonia Marggi Poullain ◽  
David V. Chicharro ◽  
Alexandre Zanchet ◽  
Luis Rubio-Lago ◽  
Alberto García-Vela ◽  
...  

Photodissociation dynamics of the ethyl radical from the 3s vs. 3p Rydberg states studied by velocity map imaging and ab initio electronic structure calculations.


2011 ◽  
Vol 135 (3) ◽  
pp. 034308 ◽  
Author(s):  
W. Scott Hopkins ◽  
M. Laura Lipciuc ◽  
Sara H. Gardiner ◽  
Claire Vallance

ChemPhysChem ◽  
2006 ◽  
Vol 7 (8) ◽  
pp. 1682-1686 ◽  
Author(s):  
Jesús G. Izquierdo ◽  
Gabriel A. Amaral ◽  
Florian Ausfelder ◽  
F. Javier Aoiz ◽  
Luis Bañares

2001 ◽  
Vol 79 (2-3) ◽  
pp. 211-227 ◽  
Author(s):  
H -P Loock ◽  
B LG Bakker ◽  
D H Parker

Jet-cooled HI has been excited using a resonant three-photon excitation scheme to energies corresponding to 13.39 and 15.59 eV. Analysis of velocity mapping images of the iodine atom fragments allowed the identification of the HI excited states at these energies as the (4Σ–1/2) 6p superexcited state and the repulsive 4Σ–1/2 state of HI+, respectively. Following excitation at 13.39 eV, we observe formation of iodine atomic fragments through the H(2S) + I[(3PJ) 6p] (J = 0, 1, 2) fragment channels, as well as through the H(2S) + I[(1D2) 6p] channel. This observation is explained by extensive nonadiabatic interactions between the (4Σ–1/2) 6p state with the repulsive (4Π1/2) 6p state and the weakly bound (A 2Σ+) 6p state. In support for this proposed dissociation mechanism excitation of the corresponding ionic 4Σ–1/2 state at 15.59 eV also results in formation of comparable quantities of I+ in its 1D2, 3P0,1, and 3P2 levels indicating again extensive nonadiabatic interactions with other repulsive curves. A similar mechanism based on the local interaction of the 4Σ–1/2 state with the A 2Σ+ and the 4Π1/2 state is proposed. PACS Nos.: 82.50F, 32.80R


2012 ◽  
Vol 136 (7) ◽  
pp. 074303 ◽  
Author(s):  
G. Gitzinger ◽  
M. E. Corrales ◽  
V. Loriot ◽  
R. de Nalda ◽  
L. Bañares

2000 ◽  
Vol 113 (6) ◽  
pp. 2182-2187 ◽  
Author(s):  
P. O’Keeffe ◽  
T. Ridley ◽  
K. P. Lawley ◽  
R. J. Donovan ◽  
H. H. Telle ◽  
...  

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