2012
DOI: 10.1063/1.4743961
|View full text |Cite
|
Sign up to set email alerts
|

Differential cross sections for the electron impact excitation of pyrimidine

Abstract: We report on differential cross section (DCS) measurements for the electron-impact excitation of the electronic states of pyrimidine. The energy range of the present measurements was 15-50 eV with the angular range of the measurements being 10 • -90 • . All measured DCSs displayed forward-peaked angular distributions, consistent with the relatively large magnitudes for the dipole moment and dipole polarizability of pyrimidine. Excitations to triplet states were found to be particularly important in some energy… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

6
30
2

Year Published

2013
2013
2020
2020

Publication Types

Select...
7
1

Relationship

2
6

Authors

Journals

citations
Cited by 31 publications
(38 citation statements)
references
References 32 publications
(44 reference statements)
6
30
2
Order By: Relevance
“…At 50 eV, where both effects should be smallest within the overlapping energy range, a good agreement is found between the present σ expt (29.3 × 10 −20 m 2 ) and the sum of elastic integral CSs from Ref. [14] and ionization and electronic excitation CSs measured by Linert et al [18] and Jones et al [15], respectively (26.1 × 10 −20 m 2 ), especially when taking into account that in Ref. [15], electronic states are included up to an excitation energy of 10 eV and do thus represent rather a lower limit to the integral electronic excitation CS.…”
Section: Resultssupporting
confidence: 67%
See 2 more Smart Citations
“…At 50 eV, where both effects should be smallest within the overlapping energy range, a good agreement is found between the present σ expt (29.3 × 10 −20 m 2 ) and the sum of elastic integral CSs from Ref. [14] and ionization and electronic excitation CSs measured by Linert et al [18] and Jones et al [15], respectively (26.1 × 10 −20 m 2 ), especially when taking into account that in Ref. [15], electronic states are included up to an excitation energy of 10 eV and do thus represent rather a lower limit to the integral electronic excitation CS.…”
Section: Resultssupporting
confidence: 67%
“…[14] and ionization and electronic excitation CSs measured by Linert et al [18] and Jones et al [15], respectively (26.1 × 10 −20 m 2 ), especially when taking into account that in Ref. [15], electronic states are included up to an excitation energy of 10 eV and do thus represent rather a lower limit to the integral electronic excitation CS. Generally, it has to be kept in mind that the integral elastic CS derived in Ref.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…In the case of positron scattering, the experiments are also expected to encounter similar difficulties, plus some additional problems due to the significantly reduced incident positron fluxes. This is reflected in the available data for pyrimidine found in the literature: whereas electron collisions have been the subject of numerous studies, including the measurement of elastic differential cross sections [17,18], gas-phase electronic-state cross-section studies [19,20] and (e,2e) ionization studies [21], vibrational and electronic excitation cross sections in the condensed phase [22], and electron energy-loss spectra [23], little work on positron scattering from pyrimidine has been done. However, Zecca et al [24] measured total cross sections (TCSs) from 0.3 to 45 eV using a positron transmission beam technique.…”
Section: Introductionmentioning
confidence: 99%
“…[11][12][13][14][15][16][17][18] As a consequence, in this short paper, we report on our derivation of vibrational-mode and electronicstate ICSs from our previously published differential cross section measurements. 21,22 Phenol also possesses a range of physico-chemical properties which, from our experience with other collision systems, [24][25][26][27][28][29][30] are anticipated to play important roles in its scattering dynamics. Specifically, phenol has a permanent dipole moment of magnitude ∼1.42 D 3 and a significant average dipole polarisability of 10.53 Å 3 .…”
Section: Introductionmentioning
confidence: 99%