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Journal articles on the topic 'Electron scattering calculations'

Author: Grafiati

Published: 7 June 2025

Last updated: 2 August 2025

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1

Berrington, M. J., D. V. Fursa, I. Bray, R. P. McEachran, and A. D. Stauffer. "Calculations of electron scattering from cadmium." Journal of Physics: Conference Series 388, no. 4 (2012): 042026. http://dx.doi.org/10.1088/1742-6596/388/4/042026.

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2

McCarthy, IE, and X. Zhang. "Distorted-wave Born Approximation for the Ionisation of Hydrogen by Electrons." Australian Journal of Physics 43, no. 3 (1990): 291. http://dx.doi.org/10.1071/ph900291.

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Matrix elements for ionisation play an important part in electron-atom scattering calculations. Two methods for describing ionisation that can be incorporated into a scattering calculation are tested here against coplanar asymmetric experimental differential cross sections at 150 and 250 eV. They are the distorted-wave Born approximation and the coupled pseudostates method. A method that incorporates the exact boundary condition for three charged bodies describes the data significantly better and shows an important direction for improvement of scattering calculations.

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3

Mirteimour, M. m., and Mina Aliyeva. "Study of the structure of atomics by the method of electron scattering in the distorted-wave approximation: Atomic energy." Turkish Computational and Theoretical Chemistry 9, no. 3 (2024): 38–44. https://doi.org/10.33435/tcandtc.1451290.

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Using distorted-wave approximation obtained the differential cross-section (DCS) of elastic scattering at energy of 80 eV of electrons on 49In, 31Ga, 34Se and 70Yb atoms, and calculated accordingly on the proposed mathematical method. The electron density distribution in the atom is chosen as a function calculated in the Dirac-Hartree-Fock-Slater approximation, which is a superposition of the spherically symmetric Yukawa potential. In addition, the DCSs were calculated for the electron density in the 49 In and 20 Ca atoms expressed as a three-parameter Fermi function at incident electron energ

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4

William McCurdy, C. "Low-energy Electron Scattering from Polyatomic Molecules: The Role of Electron Correlation." Australian Journal of Physics 45, no. 3 (1992): 337. http://dx.doi.org/10.1071/ph920337.

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Until recently the principal barrier to the accurate theoretical description of electronic collisions with polyatomic molecules was the problem of scattering by a nonlocal potential which is arbitrarily asymmetric. The last five or six years have seen the development of numerical techniques capable of solving the potential scattering problem, and the first applications of methods for treating many-body aspects of collisions of electrons with polyatomic molecules are beginning to appear in the literature. We describe the complex Kohn method and the use, in scattering calculations, of methods fo

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5

Bettega, Márcio H. F. "Low-Energy Electron Scattering by CS2 Molecules." Australian Journal of Physics 53, no. 6 (2000): 785. http://dx.doi.org/10.1071/ph00083.

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We report the integral elastic cross section for low-energy electron scattering by CS2 molecules. To perform our calculations we used the Schwinger multichannel method with pseudopotentials.We have found, in a static-exchange calculation, a shape resonance around 1 eV that belongs to the Π u symmetry.With the inclusion of polarisation effects only in that symmetry, we show that the resonance becomes a bound state. This result is in agreement with other results available in the literature.

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6

Xu, Zhi Zhong, and D. Morris. "Electron–electron inter-subband scattering in GaAs quantum wells." Canadian Journal of Physics 74, S1 (1996): 252–55. http://dx.doi.org/10.1139/p96-869.

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The role of electron–electron scattering in the dynamics of inter-subband relaxation in GaAs quantum wells is investigated theoretically. The scattering rate is calculated using the Fermi golden rule, as a function of the carrier densities. The dependence of the inter-subband relaxation time on the quantum-well width is also investigated. Calculations are performed for multiple quantum-well structures with well widths varying from 80 to 240 Å (1 Å = 10−10 m). The hot electron distribution and the subband occupation function are taken into account in these calculations. Results show that the el

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7

Qiao, S., A. Kimura, A. Harasawa, and A. Kakizaki. "A new compact spin- and angle-resolving photoelectron spectrometer with a high efficiency." Journal of Synchrotron Radiation 5, no. 3 (1998): 741–43. http://dx.doi.org/10.1107/s0909049597019067.

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A portable spin- and angle-resolving photoelectron spectrometer has been constructed, equipped with a newly developed compact retarding-potential Mott-scattering electron spin polarimeter with an efficiency of 1.9 × 10−4 for a gold target. Based on Monte Carlo calculations for the spin-dependent electron-scattering process and electron ray-tracing calculations, a novel design of the retarding-field electron optics with 0.59 sr collection solid angle for scattered electrons has been accomplished. Utilizing this spectrometer, the spin- and angle-resolved photoelectron spectra have been measured

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8

Müller, D. A., B. Edwards, E. J. Kirkland, and J. Silcox. "Detailed Calculations of Thermal Diffuse Scattering." Microscopy and Microanalysis 3, S2 (1997): 1153–54. http://dx.doi.org/10.1017/s1431927600012654.

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Convergent beam electron diffraction (CBED) produces a diffraction pattern from a single point on the specimen using a focused probe in the scanning transmission electron microscope (STEM). Because the incident wavefunction is a focused probe, each diffraction spot is enlarged to a disk the size of the objective aperture. Thermal vibration in the specimen reduces the intensity of the diffraction disks and introduces scattering in between the disk. This normally forbidden scattering between the diffraction disks is referred to as thermal diffuse scattering (TDS). The effects are most pronounced

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9

Amusia, M. Ya, and A. S. Baltenkov. "Elastic scattering of slow electrons by carbon nanotubes." Journal of Physics B: Atomic, Molecular and Optical Physics 54, no. 24 (2021): 245201. http://dx.doi.org/10.1088/1361-6455/ac3c94.

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Abstract In this paper we calculate the cross sections for elastic scattering of slow electrons by carbon nanotubes. The corresponding electron–nanotube interaction is substituted by a zero-thickness cylindrical potential that neglects the atomic structure of real nanotubes, thus limiting the range of applicability of our approach to sufficiently low incoming electron energies. The strength of the potential is chosen to be the same as was used in describing the scattering of electrons by fullerene C60. We present results for total and partial electron scattering cross sections as well as their

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10

Fabrikant, I. I. "Semiempirical calculations of inelastic electron-methylchloride scattering." Journal of Physics B: Atomic, Molecular and Optical Physics 27, no. 18 (1994): 4325–36. http://dx.doi.org/10.1088/0953-4075/27/18/026.

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11

Bauer, Eduardo, and Antonio M. Lallena. "Effective interaction in quasielastic electron scattering calculations." Physical Review C 57, no. 4 (1998): 1681–85. http://dx.doi.org/10.1103/physrevc.57.1681.

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12

Sjakste, Jelena, Iurii Timrov, Paola Gava, Natalio Mingo, and Nathalie Vast. "FIRST-PRINCIPLES CALCULATIONS OF ELECTRON-PHONON SCATTERING." Annual Review of Heat Transfer 17, N/A (2014): 333–83. http://dx.doi.org/10.1615/annualrevheattransfer.2014007320.

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13

Zhou, Yiajun, Igor Bray, and Ian McCarthy. "Model calculations of electron scattering from copper." Journal of Physics B: Atomic, Molecular and Optical Physics 32, no. 4 (1999): 1033–39. http://dx.doi.org/10.1088/0953-4075/32/4/018.

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14

Plenkiewicz, B., P. Plenkiewicz, and J. P. Jay-Gerin. "Pseudopotential calculations of elastic scattering of electrons by helium atoms in the range 0–20 eV." Canadian Journal of Physics 68, no. 1 (1990): 104–10. http://dx.doi.org/10.1139/p90-016.

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Our earlier pseudopotential calculations on electrons colliding with argon and krypton are extended to consider the elastic electron–helium scattering system. In this paper, we present detailed results for phase shifts, differential, total, and momentum-transfer cross sections for this system for incident electron energies in the range from 0 to 20 eV. These agree very well with existing experimental data and with other theoretical calculations.

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15

Stevens, D., T. J. Babij, J. R. Machacek, and J. P. Sullivan. "Low energy electron scattering from pyridine using a Surko trap and beam." Journal of Physics B: Atomic, Molecular and Optical Physics 54, no. 23 (2021): 235202. http://dx.doi.org/10.1088/1361-6455/ac3fc0.

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Abstract This paper presents measurements of low energy electron scattering from pyridine. The low energy positron beamline at the Australian National University was used for these measurements, with a change in operational parameters allowing for the measurement of electron scattering processes. We have collected data for the low energy total cross section for electron scattering, as well as measurements of the differential cross sections for electrons up to 3 eV impact energy. The operation of the beamline will be briefly outlined and data are compared to R-matrix and Schwinger multichannel

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16

Malykhina, Tetiana, Stepan Karpus, Oleg Shopen, and Valerii Prystupa. "Simulation of a High-Energy Electron Beam Transmission Through Titanium and Kapton® Thin Films." 4, no. 4 (December 10, 2021): 124–29. http://dx.doi.org/10.26565/2312-4334-2021-4-15.

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The results of computer simulation of the high-energy electrons passage through thin layers of titanium (Ti) and polyimide Kaptonâ (C22H10N2O5) in the energy range from 3 MeV to 20 MeV are presented. Simulation is carried out using the Geant4 toolkit. The number of primary electrons is 6.24×107 for each series of calculations. The thickness of the titanium foil in the model experiment is 50 µm, the thickness of the Kaptonâ film is 110 µm. The energies of primary electrons are chosen as following: 3 MeV, 5 MeV, 10 MeV, 15 MeV, and 20 MeV. The purpose of the calculations is to reveal the possibi

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17

Adibzadeh, Mehrdad, Constantine E. Theodosiou, and Nicholas J. Harmon. "Elastic Electron Scattering from Be, Mg, and Ca." Atoms 12, no. 6 (2024): 33. http://dx.doi.org/10.3390/atoms12060033.

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We present a comprehensive set of theoretical results for differential, integrated, and momentum transfer cross sections for the elastic scattering of electrons by beryllium, magnesium, and calcium at energies below 1 keV. In addition, we provide Sherman function values for elastic electron scattering from calcium in the same energy range. This study extends the application of our method of calculations, already employed for barium and strontium, to all stable alkaline-earth-metal atoms. Our semi-empirical approach to treating target polarization has produced in our earlier work a satisfactory

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18

DÍEZ MUIÑO, R., D. ROLLES, F. J. GARCÍA DE ABAJO, C. S. FADLEY, and M. A. VAN HOVE. "MULTIPLE SCATTERING THEORY OF PHOTOELECTRON ANGULAR DISTRIBUTIONS FROM ORIENTED DIATOMIC MOLECULES." Surface Review and Letters 09, no. 02 (2002): 1213–17. http://dx.doi.org/10.1142/s0218625x02003548.

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We use multiple scattering photoelectron diffraction (MSPD) theory to calculate the angular patterns of electrons photoemitted from the K-shell of CO and N 2 gas-phase oriented molecules, as recently measured by several groups. For low (E < 50 eV ) kinetic energies of the photoemitted electron, the electron scattering cannot be adequately represented by spherically symmetric potentials. We thus include nonspherical scattering potentials in our formalism through nondiagonal scattering matrices. We show that intramolecular scattering and interference are responsible for the experimentally mea

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19

Paris, Eleonora, Ziyu Wu, Annibale Mottana, and Augustο Marcelli. "Calcium environment in omphacitic pyroxenes: XANES experimental data versus one-electron multiple scattering calculations." European Journal of Mineralogy 7, no. 5 (1995): 1065–70. http://dx.doi.org/10.1127/ejm/7/5/1065.

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20

Salman, A. D., and D. R. Kadhim. "Longitudinal electron scattering form factors for 54,56Fe." International Journal of Modern Physics E 23, no. 10 (2014): 1450054. http://dx.doi.org/10.1142/s0218301314500542.

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In this paper, inelastic longitudinal electron scattering form factors for C2 transition have been studied in 54 Fe and 56 Fe with the aid of shell model calculations. The GX1 effective interaction for the fp-shell is used with the nucleon–nucleon realistic interaction Michigan three-range Yukawa and Modified surface delta interaction as a two-body interactions. The core polarization effects is taken into account through the first-order perturbation theory with the effective charge, which is taken to the proton and the neutron. The effective charge along with the core effects up to 6 ℏw enhanc

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21

ARABSHAHI, H., M. REZAEE ROKN-ABADI, and M. DASTRAS. "COMPARISON OF HIGH AND LOW FIELD ELECTRON TRANSPORT IN Al0.2Ga0.8N, AlN AND GaN." Modern Physics Letters B 22, no. 28 (2008): 2793–99. http://dx.doi.org/10.1142/s0217984908017370.

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We present a comprehensive study of the transport dynamics of electrons in the binary and ternary compounds AlN , GaN and Al 0.2 Ga 0.8 N . Calculations are made using a non-parabolic effective mass energy band model, Monte Carlo simulation that includes all of the major scattering mechanisms. The band parameters used in the simulation are extracted from optimized pseudopotential band calculations to ensure excellent agreement with experimental information and ab initio band models. The effects of alloy scattering on the electron transport physics are examined. The steady-state velocity field

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22

Позднеев, С. А. "Посвящается памяти выдающегося физика и математика --- Фаддеева Людвига Дмитриевича Применение квантовой теории рассеяния для расчетов простейших химических реакций --- диссоциативного прилипания, диссоциации и рекомбинации". Журнал технической физики 89, № 6 (2019): 803. http://dx.doi.org/10.21883/jtf.2019.06.47625.363-18.

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The quantum theory of few-body scattering based on the Faddeev-Yakubovsky equations is applied to the calculation of the main characteristics of different processes in laser, atomic, chemical and nuclear physics such as: the electron and atoms scattering with the diatomic initial rovibrational exiting molecules % $H_2$, $HD$, $D_2$, $N_2$, $Li_2$, $Na_2$, $HCl$, $HBr$ , simulation of bound and scattering states for nuclear physics %neutron-deuton, proton-deuton, positronium ion and so on. The results of this calculations are compared with available exsperimental data and other calculation.

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23

Poon, H. C., S. Y. Tong, W. F. Chung, and M. S. Altman. "Low Energy Electron Diffraction Analysis of Ultrathin Ag Films on W(110)." Surface Review and Letters 05, no. 06 (1998): 1143–49. http://dx.doi.org/10.1142/s0218625x9800147x.

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We have measured low energy electron diffraction data for clean W(110), ultrathin and thick Ag films on W(110). The data are analyzed by full dynamical multiple scattering calculations to determine the structure of the Ag-film/W(110) system. The multiple scattering calculation takes into account the incommensurate scattering between the non-pseudomorphic Ag films and the W(110) substrate. We have examined the effect of dynamical inputs used in the calculation. We find that for normally incident electrons, the surface barrier at the vacuum-film interface and the inelastic damping modify mainly

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24

KORTE, U. "MULTIPLE SCATTERING CALCULATIONS OF GBMEED." Surface Review and Letters 04, no. 05 (1997): 959–63. http://dx.doi.org/10.1142/s0218625x97001127.

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A method for computing grazing-incidence backscattering medium energy (1–3 keV) electron diffraction (GBMEED) is presented. The technique was recently proposed as a structural tool exhibiting diffraction effects resembling those of XPD. In GBMEED the intensity of quasielastically thermal diffuse scattering is measured at large scattering angles such that different atoms can be assumed to vibrate independently, and thus represent localized sources for diffuse scattering in the surface layers. The basis of the calculations is the multiple scattering theory of diffuse RHEED adopted to the medium

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25

Bostock, C., D. V. Fursa, and I. Bray. "RCCC calculations for electron scattering on quasi-two electron targets." Journal of Physics: Conference Series 388, no. 4 (2012): 042014. http://dx.doi.org/10.1088/1742-6596/388/4/042014.

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26

ROKN-ABADI, M. REZAEE, H. ARABSHAHI, and M. R. BENAM. "COMPARISON OF LOW FIELD ELECTRON TRANSPORT IN SiC AND GaN STRUCTURES FOR HIGH-POWER AND HIGH-TEMPERATURE DEVICE MODELING." Modern Physics Letters B 22, no. 13 (2008): 1357–66. http://dx.doi.org/10.1142/s0217984908015358.

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Temperature and doping dependencies of electron mobility in SiC and GaN structures have been calculated using an iteravive technique. The following scattering mechanisims, i.e. impurity, polar optical phonon, acoustic phonon, piezoelectric and electron–plasmon are included in the calculation. Ionized imurity scattering has been treated beyond the Born approximation using the phase-shift analysis. It is found that the electron mobility decreases monotonically as the temperature increases from 100 K to 600 K. The low temperature value of electron mobilty increases significantly with increasing d

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27

Bernardi, Marco, Derek Vigil-Fowler, Chin Shen Ong, Jeffrey B. Neaton, and Steven G. Louie. "Ab initio study of hot electrons in GaAs." Proceedings of the National Academy of Sciences 112, no. 17 (2015): 5291–96. http://dx.doi.org/10.1073/pnas.1419446112.

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Hot carrier dynamics critically impacts the performance of electronic, optoelectronic, photovoltaic, and plasmonic devices. Hot carriers lose energy over nanometer lengths and picosecond timescales and thus are challenging to study experimentally, whereas calculations of hot carrier dynamics are cumbersome and dominated by empirical approaches. In this work, we present ab initio calculations of hot electrons in gallium arsenide (GaAs) using density functional theory and many-body perturbation theory. Our computed electron–phonon relaxation times at the onset of the Γ, L, and X valleys are in e

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28

Mirabutalybov, Mirteimour, and Mina Aliyeva. "Study of Average Characteristic Parameters of Isotopes, Isotones and Isobars by Electron and Proton Scattering." Quantum Beam Science 9, no. 2 (2025): 18. https://doi.org/10.3390/qubs9020018.

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By way of studying the difference of the proton and neutron distributions in isotopes, isotones and isobars, we used the results of theoretical calculations obtained from the scattering of protons and electrons on nuclei. To calculate the differential cross section of proton scattering, an expression was obtained for the distorted-wave formfactor of the nucleus, which, using the mathematical method proposed by us, is expressed through the plane-wave Born formfactor. In addition, using the data for elastic scattering of electrons on nuclei, the average characteristic parameters of C2040a, C2048

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29

Guo, Fei, Zhe Liu, Mingfeng Zhu, and Yisong Zheng. "Electron–phonon scattering limited hole mobility at room temperature in a MoS2 monolayer: first-principles calculations." Physical Chemistry Chemical Physics 21, no. 41 (2019): 22879–87. http://dx.doi.org/10.1039/c9cp04418c.

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30

Teubner, P. J. O., V. Karaganov, M. R. Law, and P. M. Farrell. "Superelastic electron scattering from calcium and lithium." Canadian Journal of Physics 74, no. 11-12 (1996): 984–90. http://dx.doi.org/10.1139/p96-818.

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Superelastic scattering experiment were performed on optically pumped calcium atoms at energies of 25.7 and 45 eV referred to the ground state. Orientation and alignment parameters derived from these experiments are compared with the predictions of several theories based on a distorted-wave formalism. The agreement between theory and experiment is unsatisfactory at the lower energy at all scattering angles. At the higher energy agreement improves at small scattering angles but is poor at middle angles. The results of our quantum electrodynamical calculation on optical pumping in lithium are co

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31

Gorelik, Tatiana E., Reinhard Neder, Maxwell W. Terban, et al. "Towards quantitative treatment of electron pair distribution function." Acta Crystallographica Section B Structural Science, Crystal Engineering and Materials 75, no. 4 (2019): 532–49. http://dx.doi.org/10.1107/s205252061900670x.

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The pair distribution function (PDF) is a versatile tool to describe the structure of disordered and amorphous materials. Electron PDF (ePDF) uses the advantage of strong scattering of electrons, thus allowing small volumes to be probed and providing unique information on structure variations at the nano-scale. The spectrum of ePDF applications is rather broad: from ceramic to metallic glasses and mineralogical to organic samples. The quantitative interpretation of ePDF relies on knowledge of how structural and instrumental effects contribute to the experimental data. Here, a broad overview is

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32

Fursa, Dmitry V., and Igor Bray. "Convergent close-coupling calculations of electron - helium scattering." Journal of Physics B: Atomic, Molecular and Optical Physics 30, no. 4 (1997): 757–85. http://dx.doi.org/10.1088/0953-4075/30/4/003.

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33

Fursa, Dmitry V., and Igor Bray. "Convergent close-coupling calculations of electron - beryllium scattering." Journal of Physics B: Atomic, Molecular and Optical Physics 30, no. 8 (1997): L273—L277. http://dx.doi.org/10.1088/0953-4075/30/8/003.

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34

Bray, Igor, and Andris T. Stelbovics. "Convergent close-coupling calculations of electron-hydrogen scattering." Physical Review A 46, no. 11 (1992): 6995–7011. http://dx.doi.org/10.1103/physreva.46.6995.

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35

Bransden, B. H., I. E. McCarthy, J. D. Mitroy, and A. T. Stelbovics. "Extended coupled-channels calculations for electron-hydrogen scattering." Physical Review A 32, no. 1 (1985): 166–75. http://dx.doi.org/10.1103/physreva.32.166.

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36

Nesbet, R. K., C. J. Noble, and L. A. Morgan. "Calculations of elastic electron scattering byH2for fixed nuclei." Physical Review A 34, no. 4 (1986): 2798–808. http://dx.doi.org/10.1103/physreva.34.2798.

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37

Bray, Igor. "Calculations of spin asymmetries in electron-alkali scattering." Zeitschrift f�r Physik D Atoms, Molecules and Clusters 30, no. 2-3 (1994): 99–103. http://dx.doi.org/10.1007/bf01426056.

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38

Hannachi, M., Z. Rouabah, C. Champion, and N. Bouarissa. "Electron backscattering from solid targets: Elastic scattering calculations." Journal of Electron Spectroscopy and Related Phenomena 195 (August 2014): 155–59. http://dx.doi.org/10.1016/j.elspec.2014.07.006.

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39

Yassir, Ahlam K., and Alaa A. Khalaf. "Rotational excitation of methane molecule by electron impact." International Journal of Chemistry, Mathematics and Physics 8, no. 3 (2024): 01–08. https://doi.org/10.22161/ijcmp.8.3.1.

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Electron scattering by methane molecule plays a crucial role in understanding the interaction dynamics between electrons and molecules In this research we focus on investigating the elastic and rotational excitation process for electron scattering by CH_4 within the energy range of 530 eVThe main objective is to calculate the differential and total cross sections to provide insights into the scattering behavior and energy transfer mechanisms involved in these collisions To achieve this advanced theoretical model and computational method are employed Accurate potential energy and interaction po

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40

Luniov, S. V., V. V. Lyshuk, V. T. Maslyuk, and O. V. Burban. "Mechanisms of Electron Scattering in Uniaxially Deformed Silicon Single Crystals with Radiation Defects." Latvian Journal of Physics and Technical Sciences 56, no. 5 (2019): 45–57. http://dx.doi.org/10.2478/lpts-2019-0030.

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Abstract Temperature dependencies for Hall mobility of electrons for the uniaxially deformed n-Si single crystals, irradiated by the flow of electrons Ω=1·1017 el./cm2 with the energy of 12 MeV, are obtained on the basis of piezo-Hall effect measurements. From the analysis of these dependencies it follows that under the uniaxial pressure (0–0.42) GPa and (0–0.37) GPa along crystallographic directions [100] and [111], respectively, the deformation-induced increase of the Hall mobility has been observed. On the basis of the proposed theoretical model of mobility, this increase is explained by th

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41

Vandas, M. "Shock Drift Electron Acceleration and Pitch Angle Scattering." Symposium - International Astronomical Union 203 (2001): 577–79. http://dx.doi.org/10.1017/s0074180900220044.

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Spacecraft measurements of energetic electrons in the vicinity of the Earth's bow shock and interplanetary shocks are analyzed and compared with theoretical calculations. It is concluded that shock drift acceleration of electrons is very modified by an additional process, probably by strong pitch angle scattering. Calculations including this effect are presented.

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42

Potekhin, Alexander. "Heat and charge transport in envelopes of weakly and strongly magnetized neutron stars." International Astronomical Union Colloquium 177 (2000): 621–22. http://dx.doi.org/10.1017/s0252921100060796.

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AbstractThermal and electrical electron conductivities are calculated for a broad range of physical parameters typical for envelopes of neutron stars. An appropriate effective electron-ion scattering potential is used, based on calculations involving modified ion structure factors suggested recently for the treatment of the transport problems in dense Coulomb plasmas. These results are applied to calculation of the thermal structure of neutron-star envelopes.

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43

Vukalović, Jelena, Jelena B. Maljković, Francisco Blanco, Gustavo García, Branko Predojević, and Bratislav P. Marinković. "Absolute Differential Cross-Sections for Elastic Electron Scattering from Sevoflurane Molecule in the Energy Range from 50–300 eV." International Journal of Molecular Sciences 23, no. 1 (2021): 21. http://dx.doi.org/10.3390/ijms23010021.

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We report the results of the measurements and calculations of the absolute differential elastic electron scattering cross-sections (DCSs) from sevoflurane molecule (C4H3F7O). The experimental absolute DCSs for elastic electron scattering were obtained for the incident electron energies from 50 eV to 300 eV, and for scattering angles from 25° to 125° using a crossed electron/target beams setup and the relative flow technique for calibration to the absolute scale. For the calculations, we have used the IAM-SCAR+I method (independent atom model (IAM) applying the screened additivity rule (SCAR) w

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44

Zatsarinny, Oleg, Klaus Bartschat, and Michael Allan. "Electron scattering from krypton: High-resolution electron scattering experiments and B-spline R-matrix calculations." Journal of Physics: Conference Series 388, no. 4 (2012): 042017. http://dx.doi.org/10.1088/1742-6596/388/4/042017.

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45

Wang, Z. L., and Chen Zhang. "Absorption Potential for Dynamic Electron Diffraction - A Revisit." Microscopy and Microanalysis 4, S2 (1998): 340–41. http://dx.doi.org/10.1017/s1431927600021826.

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Quantitative analysis of structural information provided by transmission electron diffraction and imaging strongly relies on computer simulations. An important quantity in dynamic calculation is the “absorption” potential. The absorption here actually means that the electron is not absorbed by the specimen rather it is scattered out of the elastic state (or Bragg peaks) due to energy-loss and momentum transfer, resulting in a decrease in the intensity of the elastic wave. This is the effect of inelastic scattering (or diffuse scattering) on the Bragg reflected waves [1]. Almost all of the mode

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Tanuma, S., C. J. Powell, and D. R. Penn. "Calculations of electron inelastic mean free paths for carbides." Proceedings, annual meeting, Electron Microscopy Society of America 54 (August 11, 1996): 130–31. http://dx.doi.org/10.1017/s0424820100163113.

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Knowledge of the values of inelastic mean free paths (IMFPs) for low-energy electrons in solids is important for quantitative surface analysis by AES and XPS as well as for determining the surface sensitivity of other electron-spectroscopic methods of surface characterization. In previous papers, we have described the Penn algorithm for calculations of electron inelastic mean free paths in solids, and used this algorithm for calculations of IMFPs for 50 – 2000 eV electrons in a group of 27 elements, a group of 15 inorganic compounds, and a group of 14 organic compounds. We fitted the calculate

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Patterson, J. D., Wafaa A. Gobba, and S. L. Lehoczky. "Electron mobility in n-type Hg1−xCdxTe and Hg1−xZnx Te alloys." Journal of Materials Research 7, no. 8 (1992): 2211–18. http://dx.doi.org/10.1557/jmr.1992.2211.

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We have calculated the mobility of electrons in n-type Mercury Cadmium Telluride (MCT) and compared it to a calculation of the mobility of electrons in n-type Mercury Zinc Telluride (MZT) with nearly the same energy gap and with the same number of donors and acceptors. We also compared the results of the MZT calculation with experiment. We found for equivalent energy gaps that the mobilities in the two compounds (MCT, MZT) were nearly the same. The calculations for both MCT and MZT were based on the best set of material parameters that we could compile from the literature. Using these paramete

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Tyuterev, V. G. "Electron short-wave phonon scattering in crystals with chalcopyrite lattice." Canadian Journal of Physics 98, no. 8 (2020): 818–23. http://dx.doi.org/10.1139/cjp-2019-0523.

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Electron short-wavelength phonon scattering is an effective channel for energy relaxation in crystals with a pseudo-direct optical gap. The equilibrium parameters of crystal structures and spectra of electrons and phonons in the ternary chalcopyrite compounds ZnSiP2 and ZnGeP2 are calculated self-consistently in good agreement with available experimental and theoretical calculations. The ab initio probabilities of phonon-assisted intervalley scattering of electrons in the conduction bands of the pseudo-direct-gap compounds ZnSiP2 and ZnGeP2 between the central Γ minima and the lowest lateral m

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Salman, A. D., N. Al-Dahan, F. I. Sharrad, and I. Hossain. "Calculation of inelastic electron–nucleus scattering form factors of 29Si." International Journal of Modern Physics E 23, no. 09 (2014): 1450046. http://dx.doi.org/10.1142/s0218301314500463.

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Inelastic electron scattering form factors for 29 Si nucleus with total angular momentum and positive parity (Jπ) and excited energy (3/2+, 1.273 MeV; 5/2+, 2.028 MeV; 3/2+, 2.425 MeV and 7/2+, 4.079 MeV) have been calculated using higher energy configurations outside the sd-shell. The calculations of inelastic form factors up to the first- and second-order with and without core-polarization (CP) effects were compared with the available experimental data. The calculations of inelastic electron scattering form factors up to the first-order with CP effects are in agreement with the experimental

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Neumann, K. D., and J. C. H. Spence. "The electron energy loss near edge structure of MGO: Theory and experiment." Proceedings, annual meeting, Electron Microscopy Society of America 45 (August 1987): 126–27. http://dx.doi.org/10.1017/s0424820100125567.

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A similiarity between theoretical calculations of the differential scattering cross section for electron energy-loss near edge structure (ELNES) and the cross section for x-ray absorption near edge structure (XANES) has been demonstrated by several workers (see, e.g. Leapman et al). Since theoretical XANES calculations using band structure methods have often given impressive agreement with experimental results, it is expected hat these same methods can be used under certain experimental conditions to fit ELNES theory to experimental data. The interpretation of ELNES may however, be subject to

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