ChemInform ◽  
1987 ◽  
Vol 18 (8) ◽  
Author(s):  
C. KOSMIDIS ◽  
A. BOLOVINOS ◽  
P. TSEKERIS

1965 ◽  
Vol 42 (4) ◽  
pp. 1183-1198 ◽  
Author(s):  
Y. Tanaka ◽  
F. R. Innes ◽  
A. S. Jursa ◽  
M. Nakamura
Keyword(s):  

1972 ◽  
Vol 57 (7) ◽  
pp. 2964-2976 ◽  
Author(s):  
Y. Tanaka ◽  
K. Yoshino
Keyword(s):  

ChemInform ◽  
1989 ◽  
Vol 20 (28) ◽  
Author(s):  
P. BRINT ◽  
P. TSEKERIS ◽  
A. BOLOVINOS ◽  
C. KOSMIDIS

2004 ◽  
Vol 426 (1) ◽  
pp. 105-117 ◽  
Author(s):  
G. Malloci ◽  
G. Mulas ◽  
C. Joblin

1988 ◽  
Vol 102 ◽  
pp. 243-246
Author(s):  
J.T. Costello ◽  
W.G. Lynam ◽  
P.K. Carroll

AbstractThe dual laser-produced plasma technique for the study of ionic absorption spectra has been developed by the use of two Q-switched ruby lasers to enable independent generation of the absorbing and back-lighting plasmas. Optical pulse handling is used in the coupling cicuits to enable reproducible pulse delays from 250 nsec. to 10 msec, to be achieved. At delay times > 700 nsec. spectra of essentially pure neutral species are observed. The technique is valuable, not only for obtaining the neutral spectra of highly refractory and/or corrosive materials but also for studying behaviour of ionic species as a function of time. Typical spectra are shown in Fig. 1.


1988 ◽  
Vol 102 ◽  
pp. 71-73
Author(s):  
E. Jannitti ◽  
P. Nicolosi ◽  
G. Tondello

AbstractThe photoabsorption spectra of the carbon ions have been obtained by using two laser-produced plasmas. The photoionization cross-section of the CV has been absolutely measured and the value at threshold, σ=(4.7±0.5) × 10−19cm2, as well as its behaviour at higher energies agrees quite well with the theoretical calculations.


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