2016
DOI: 10.1140/epjd/e2016-60473-6
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Measuring electron-impact cross sections of water: elastic scattering and electronic excitation of the ã3B1 and Ã1B1 states

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Cited by 26 publications
(39 citation statements)
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“…Note that this modifies substantially the derived integral cross section as well as the momentum transfer cross section values which tend to be much higher when dipole interactions are included. It is also noteworthy that the backward peaking below 6.0 eV, which was found in other polar molecular targets, 36,37 is not evident from the present measurements. This larger angle region also contributes to the determination of the ICS and the MTCS and therefore calculated and extrapolated values can be again crucial.…”
Section: A Elastic Dcss For E − + Pf 3 From 20 To 200 Evcontrasting
confidence: 76%
“…Note that this modifies substantially the derived integral cross section as well as the momentum transfer cross section values which tend to be much higher when dipole interactions are included. It is also noteworthy that the backward peaking below 6.0 eV, which was found in other polar molecular targets, 36,37 is not evident from the present measurements. This larger angle region also contributes to the determination of the ICS and the MTCS and therefore calculated and extrapolated values can be again crucial.…”
Section: A Elastic Dcss For E − + Pf 3 From 20 To 200 Evcontrasting
confidence: 76%
“…Measurements of electronic excitation cross-sections are usually restricted to some particular channels. 18,19,21,74 However, data for many more transitions are provided in ref. 20, which is the most complete information currently available to the best of our knowledge.…”
Section: Energy Distributions Of Secondary Electrons and Total Electrmentioning
confidence: 99%
“…10,11 Plenty of experimental information is available on electronimpact ionisation cross-sections (total probabilities as well as energy spectra of ejected electrons) of relevant biomolecules (such as water or DNA nucleobases), however it is usually limited to the gas phase, [12][13][14][15][16][17] without taking into account the condensed-phase nature of living organisms. Experimental data on electronic excitations are much scarcer and scattered 16,[18][19][20][21] and also limited just to molecules in the gas phase, with only a few exceptions. 22 An alternative for gathering all relevant cross-sections resorts into theoretical calculations, where some very successful ab initio approaches are available for calculating both excitation and ionisation cross-sections.…”
Section: Introductionmentioning
confidence: 99%
“…Previous literature attributes a shoulder at 7.1 eV to theã 3 B 1 transition. [52][53]57 Computationally, the second excited state in the TDDFT calculation was observed at 10.02 eV and the molecular orbital diagram for this valence transition is seen in Fig. 5b.…”
Section: Watermentioning
confidence: 93%