Two-dimensional ion-imaging of fragment angular distributions after photolysis of state-selected and oriented triatomic molecules

1997 ◽  
Author(s):  
J. M. Teule ◽  
M. H. Hilgeman ◽  
M. H. M. Janssen ◽  
D. W. Chandler ◽  
C. A. Taatjes ◽  
...  
2019 ◽  
Vol 21 (6) ◽  
pp. 3083-3091 ◽  
Author(s):  
Yuji Nakashima ◽  
Kenichi Okutsu ◽  
Keita Fujimoto ◽  
Yuri Ito ◽  
Manabu Kanno ◽  
...  

Velocity and angular distributions of photofragment CO2+ ions produced from mass-selected (CO2)2+ at 532 nm excitation were observed in an ion imaging experiment.


1990 ◽  
Vol 167 (6) ◽  
pp. 583-587 ◽  
Author(s):  
A. Hagemeyer ◽  
L. Brombacher ◽  
K. Schmidt-Rohr ◽  
H.W. Spiess

2003 ◽  
Vol 94 (3) ◽  
pp. 369-373 ◽  
Author(s):  
O. V. Elyukhina ◽  
O. S. Vasyutinskii ◽  
J. A. Beswick

2021 ◽  
Vol 2090 (1) ◽  
pp. 012048
Author(s):  
A Smirnov ◽  
N Kovalenko ◽  
O Riabushkin

Abstract The numerical model of the diffuse reflection of Gaussian beam from the surface of biological tissue is introduced. The two-dimensional fractional Brownian motion (fBm) with the Hurst index H and the scale parameter σ was used for the simulations of the tissue surface relief. For the surfaces described by fixed σ = 0.1 and H = 0.55, H = 0.803 (corresponds to the surface of a banana fruit), H = 0.9, the angular distributions of the reflected radiation intensity were calculated using a Kirchhoff integral approach. The resulting distributions considerably differ from each other. Therefore, the introduced model can be used for the solution of the inverse problem of finding the fBm parameters of tissue surfaces employing the experimentally measured distribution of the reflected radiation intensity.


1998 ◽  
Vol 17 (4) ◽  
pp. 185-190 ◽  
Author(s):  
Peter C. Samartzis ◽  
Theodosia Gougousi ◽  
Theofanis N. Kitsopoulos

The velocity distributions for the Cl(2P3/2) and Cl(2P1/2) photofragments produced by the photolysis of Cl2 at 308 nm are measured using ion imaging. The angular distributions yield anisotropy parameters of β(2P3/2)=−1.00±0.05,β(2P1/2)=−0.95±0.05, suggesting that Cl(2P3/2) and Cl(2P1/2) is essentially produced via non-adiabatic curve crossing between the lu and the 0u+ excited electronic states.


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