2002
DOI: 10.1088/0953-4075/35/4/328
|View full text |Cite
|
Sign up to set email alerts
|

The molecular and dissociative photoionization of ethane in the inner and outer valence energy regions

Abstract: The molecular and dissociative photoionization of C2H6 has been studied using synchrotron radiation within the energy range 11-40 eV. Positive and negative photoion mass spectra and threshold photoelectron spectra have been obtained. These show that superexcited states, which can decay through ion pair formation, play an important role in the photodissociative ionization process. The positive photoion yield curves display significant and hitherto unobserved structures, which are unrelated to those prese… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
11
0

Year Published

2004
2004
2013
2013

Publication Types

Select...
5
2

Relationship

0
7

Authors

Journals

citations
Cited by 18 publications
(11 citation statements)
references
References 21 publications
0
11
0
Order By: Relevance
“…The m/z = 30 signal gives two ionization thresholds of 10.86 and 11.53 eV (Figure 4D) respectively corresponding to formaldehyde (HCHO) and ethane (C 2 H 6 ). The observed inflection at ~12.5 eV in Figure 4d corresponds to the 2 E g electronic state of C 2 H 6 + ion34. The m/z = 32 signal gives two ionization thresholds of 10.82 and 12.05 eV (Figure 4E) respectively corresponding to methanol (CH 3 OH) and oxygen (O 2 ).…”
Section: Resultsmentioning
confidence: 93%
“…The m/z = 30 signal gives two ionization thresholds of 10.86 and 11.53 eV (Figure 4D) respectively corresponding to formaldehyde (HCHO) and ethane (C 2 H 6 ). The observed inflection at ~12.5 eV in Figure 4d corresponds to the 2 E g electronic state of C 2 H 6 + ion34. The m/z = 32 signal gives two ionization thresholds of 10.82 and 12.05 eV (Figure 4E) respectively corresponding to methanol (CH 3 OH) and oxygen (O 2 ).…”
Section: Resultsmentioning
confidence: 93%
“…It is equal to the Langevin rate (2.36 × 10 −9 cm 3 s −1 ) within experimental uncertainties, so the rate constant at 150 K is most probably the same. Product branching ratios cannot be precisely derived from these experiments, as the derivation of such ratios would have required coincidence measurements between singly charged product ions as in the studies from Lockyear et al (2011) (Mackie et al 2002;Stockbauer 1973 (±25%) for electron recombination Absolute cross section measurements have been carried out by Seiersen et al (2003) using the heavy-ion storage ring ASTRID in the relative collision energy range 10 −4 to 10 eV. They studied the recombination of 14 N 15 N ++ and deduced from their data analysis a rate constant of k = (5.8 ± 2.9) × 10 −7 (T e /300) −0.5 cm 3 s −1 , which is about 2.5 times greater than the dissociative recombination of N + 2 at room temperature.…”
Section: Reactionsmentioning
confidence: 99%
“…Much is known about the decomposition of C 2 H 6 + and the ions derived from its dehydrogenation products, C 2 H 4 + and C 2 H 2 + . Mackie et al . have reported ion distribution data from photoionization of C 2 H 6 by 11–40 eV radiation followed by quadrupole mass spectrometry.…”
Section: Introductionmentioning
confidence: 99%