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Journal articles on the topic 'Scattering electron'

Author: Grafiati

Published: 28 May 2022

Last updated: 31 July 2025

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1

Vijetha, T., P. S. Mallick, R. Karthik, and Kavitha Rajan. "Effect of Scattering Angle in Electron Transport of AlGaN and InGaN." Advances in Materials Science and Engineering 2022 (October 12, 2022): 1–4. http://dx.doi.org/10.1155/2022/3017040.

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The scattering angle between electrons plays a very important role for the calculation of scattering probability. The probability of scattering is an essential parameter for the simulation of electron paths. In this work, we calculated the scattering probability with scattering angle in AlGaN and InGaN at 77 K and found that the lower angle scatterings only dominate.

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2

Dedulewich, S., Z. Kancleris, A. Matulis, and Yu Pozhela. "Electron-electron scattering in hot electrons." Semiconductor Science and Technology 7, no. 3B (1992): B322—B323. http://dx.doi.org/10.1088/0268-1242/7/3b/081.

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3

Mallick, P. S., J. Kundu, and C. K. Sarkar. "Calculation of ionized impurity-scattering probability with scattering angles in GaN." Canadian Journal of Physics 86, no. 8 (2008): 1023–26. http://dx.doi.org/10.1139/p08-027.

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The probability of scattering by ionized impurities has been calculated as function of the scattering angle for various energy values of the electrons in gallium nitride at 77 K. It is found that for electron energies higher than 0.1 eV, almost-zero angle scatterings are most prevalent.PACS Nos.: 72.10.–d, 72.20.Fr

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4

Bariakhtar, I., and A. Nazarenko. "Potential Electron Scattering by Phosphorus Atom." Ukrainian Journal of Physics 59, no. 6 (2014): 596–600. http://dx.doi.org/10.15407/ujpe59.06.0596.

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5

Kotera, Masatoshi, Keiji Yamamoto, and Hiroshi Suga. "Applications of a direct simulation of electron scattering to quantitative electron-probe microanalysis." Proceedings, annual meeting, Electron Microscopy Society of America 50, no. 2 (1992): 1670–71. http://dx.doi.org/10.1017/s0424820100132984.

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A direct simulation of electron scatterings in solids is developed. The simulation takes into account elastic processes, and inelastic processes including inner-shell electron ionization, conduction electron ionization, bulk plasmon excitation, and bulk plasmon decay. After the ionization and the plasmon decay processes, the trajectories of hot electrons which are liberated from atomic electrons are calculated, and cascade multiplication of hot electrons is simulated in the solid. The theoretical equations used in the present simulation are in the following. For the elastic scattering of elect

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6

Wang, Heng, Kang Du, Ruibin Liu, et al. "Role of hot electron scattering in epsilon-near-zero optical nonlinearity." Nanophotonics 9, no. 14 (2020): 4287–93. http://dx.doi.org/10.1515/nanoph-2020-0266.

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AbstractThe physical origin of epsilon-near-zero (ENZ) optical nonlinearity lies in the hot-electron dynamics, in which electron scattering plays an important role. With the damping factor defined by hot electron scattering time, the Drude model could be extended to modeling ENZ optical nonlinearity completely. We proposed a statistical electron scattering model that takes into account the effect of electron distribution in a nonparabolic band and conducted the investigation on indium tin oxide (ITO) with femtosecond-pump continuum-probe experiment. We found that ionized impurity scattering an

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7

Nahar, Sultana N., and Bobby Antony. "Positron Scattering from Atoms and Molecules." Atoms 8, no. 2 (2020): 29. http://dx.doi.org/10.3390/atoms8020029.

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A review on the positron scattering from atoms and molecules is presented in this article. The focus on positron scattering studies is on the rise due to their presence in various fields and application of cross section data in such environments. Positron scattering is usually investigated using theoretical approaches that are similar to those for electron scattering, being its anti-particle. However, most experimental or theoretical studies are limited to the investigation of electron and positron scattering from inert gases, single electron systems and simple or symmetric molecules. Optical

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8

Sen, R., N. Vast, and J. Sjakste. "Hot electron relaxation and energy loss rate in silicon: Temperature dependence and main scattering channels." Applied Physics Letters 120, no. 8 (2022): 082101. http://dx.doi.org/10.1063/5.0082727.

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In this work, we revisit the density functional theory (DFT)-based results for electron–phonon scattering in highly excited silicon. Using the state-of-the-art ab initio methods, we examine the main scattering channels, which contribute to the total electron–phonon scattering rate and the energy loss rate of photoexcited electrons in silicon as well as their temperature dependence. Both temperature dependence and the main scattering channels are shown to strongly differ for the total electron–phonon scattering rate and the energy loss rate of photoexcited electrons. While the total electron–ph

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9

Shimizu, Ryuichi, and Hideki Yoshikawa. "Monte Carlo Simulation of Background in electron spectroscopies." Proceedings, annual meeting, Electron Microscopy Society of America 50, no. 2 (1992): 1664–65. http://dx.doi.org/10.1017/s0424820100132959.

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Recent progress in getting precise knowledge on inelastic scattering, particularly, on dielectric functions for various types of material has been enabling the electron spectroscopic spectra obtained by Auger electron spectroscopy (AES), X-ray photoelectron spectroscopy (XPS) and reflection electron energy loss spectroscopy (REELS) to be reproduced theoretically with considerable success. For this Monte Carlo simulation is probably most powerful tool, leading to more comprehensive understanding of not only the signal generation but also the background formation.In this paper we present a Monte

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10

Achenefe, Y., T. Senbeta, and V. N. Mal'nev. "Electron Scattering in Graphene by Remote Nanomagnets." Ukrainian Journal of Physics 61, no. 5 (2016): 393–99. http://dx.doi.org/10.15407/ujpe61.05.0393.

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11

Wang, Zan, Lei Quan, and Yi Wu Ruan. "Simulation of Electron Transport in Silicon using Monte Carlo Method." Advanced Materials Research 284-286 (July 2011): 871–74. http://dx.doi.org/10.4028/www.scientific.net/amr.284-286.871.

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A Monte Carlo method is employed to investigate the properties of electron transport with considerations of electron-phonon scattering including intervalley scattering and intravalley scattering. Under different electric fields, the coupling relations between electrons and phonons are studied, and the behaviors of absorbing and releasing phonons from electrons are also analyzed. The results show the scattering events of absorbing phonons from electrons decrease with the increasing simulation time. At the same temperature, the mean free path of electron increases initially and then decreases wi

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12

Cheng, S. C., Y. Y. Wang, and V. P. Dravid. "The measurements of the elastic-inelastic multiple scattering electron intensity in EELS." Proceedings, annual meeting, Electron Microscopy Society of America 53 (August 13, 1995): 300–301. http://dx.doi.org/10.1017/s0424820100137872.

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The Electron energy loss function in the low energy range is determined by collective excitation of valence electrons and charge carriers, i.e. plasmons, as well as interband and intraband excitations. The explicit dependence of the cross-section on the momentum transfer q allows the observation of nonvertical interband transition and a measurement of the dispersion of plasmon excitations. The drawback of the momentum resolved electron spectroscopy is the multiple scattering, which often obscure the single scattering events. Under relatively small scattering angles, both strong elasticinelasti

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13

Shimizu, Ryuichi, and Ze-Jun Ding. "Electron Scattering in Solids." Proceedings, annual meeting, Electron Microscopy Society of America 48, no. 2 (1990): 4–5. http://dx.doi.org/10.1017/s0424820100133618.

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Monte Carlo simulation has been becoming most powerful tool to describe the electron scattering in solids, leading to more comprehensive understanding of the complicated mechanism of generation of various types of signals for microbeam analysis.The present paper proposes a practical model for the Monte Carlo simulation of scattering processes of a penetrating electron and the generation of the slow secondaries in solids. The model is based on the combined use of Gryzinski’s inner-shell electron excitation function and the dielectric function for taking into account the valence electron contrib

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14

Wang, Z. L. "Coupled thermal diffuse-atomic inner shell scattering in electron diffraction." Proceedings, annual meeting, Electron Microscopy Society of America 52 (1994): 994–95. http://dx.doi.org/10.1017/s042482010017270x.

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In electron diffraction patterns, diffuse scattering at high angles is primarily generated by phonon, or thermal diffuse, scattering (TDS). Techniques were introduced to acquire the electron energy-loss spectra (EELS) of high-angle thermal-diffuse-scattered electrons (TDS-EELS) in a transmission electron microscope (TEM). With regards to the scattering mechanism, the TDS-EELS core ionization edge intensity was believed to be generated primarily by TDS - single electron, double-inelastic electron scattering processes. It was concluded from experimental data that the signal from coupled phonon -

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15

Jonas, P., P. Schattschneider, and P. Pongratz. "Removal of Bragg-Compton Channel Coupling in Electron Compton Scattering." Proceedings, annual meeting, Electron Microscopy Society of America 48, no. 2 (1990): 24–25. http://dx.doi.org/10.1017/s0424820100133710.

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Electron Compton scattering is inelastic scattering of fast electrons at large angles off core or valence electrons. The energy of the scattered electron is increasingly lowered with scattering angle; the energy distribution can be shown to be an image of the electron momentum density distribution in the ground state.The most dominant problem in ECOSS (Electron Compton Scattering from Solids), is the Bragg-Compton channel coupling. Bragg scattered electrons in the specimen act as new sources for Compton scattering. Since these Compton events correspond to various scattering angles a number of

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16

Walecka, J. D. "Electron scattering." Nuclear Physics A 574, no. 1-2 (1994): 271–96. http://dx.doi.org/10.1016/0375-9474(94)90050-7.

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17

Palenskis, Vilius. "New Insight into Electric Force in Metal and the Quadratic Electrical Resistivity Law of Metals at Low Temperatures." Metals 14, no. 5 (2024): 526. http://dx.doi.org/10.3390/met14050526.

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Considering that Einstein’s relation between the diffusion coefficient and the drift mobility of free randomly moving charge carriers in homogeneous materials including metals is always valid, it is shown that the effective electric force acting on free electrons in metal depends on the ratio between the kinetic free electron energy at the Fermi surface to the classical particle energy 3 kT/2. The electrical resistivity of elemental metals dependence on very low temperatures has the quadratic term, which has been explained by electron–electron scattering. In this paper, it is shown that the qu

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18

ZHANG, C. "EFFECT OF INELASTIC SCATTERING OF HOT ELECTRONS ON THERMIONIC COOLING IN A SINGLE-BARRIER STRUCTURE." International Journal of Modern Physics B 14, no. 14 (2000): 1451–57. http://dx.doi.org/10.1142/s0217979200001503.

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One of the important problems in thermionics using layered structures is the inelastic scattering of hot electrons in the electrodes and in the barrier region. Scattering in these systems is mainly via the electron–phonon interaction, or indirectly via the electron–electron interaction. In semiconductor heterostructures at room temperature, the LO-phonon plays a crucial role in thermalising electrons. In this work we study the effect of electron–phonon scattering on thermionic cooling in a single-barrier structure. Because of the asymmetry of the barrier under a bias, a larger fraction of the

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19

Lee, Geon-Woo, Young-Bok Lee, Dong-Hyun Baek, Jung-Gon Kim, and Ho-Seob Kim. "Raman Scattering Study on the Influence of E-Beam Bombardment on Si Electron Lens." Molecules 26, no. 9 (2021): 2766. http://dx.doi.org/10.3390/molecules26092766.

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Microcolumns have a stacked structure composed of an electron emitter, electron lens (source lens), einzel lens, and a deflector manufactured using a micro electro-mechanical system process. The electrons emitted from the tungsten field emitter mostly pass through the aperture holes. However, other electrons fail to pass through because of collisions around the aperture hole. We used Raman scattering measurements and X-ray photoelectron spectroscopy analyses to investigate the influence of electron beam bombardment on a Si electron lens irradiated by acceleration voltages of 0, 20, and 30 keV.

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20

VITKALOV, SERGEY, JING QIAO ZHANG, A. A. BYKOV, and A. I. TOROPOV. "NONLINEAR TRANSPORT OF 2D ELECTRONS IN MAGNETIC FIELD." International Journal of Modern Physics B 23, no. 12n13 (2009): 2689–92. http://dx.doi.org/10.1142/s0217979209062190.

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Electric field induced, spectacular reduction of longitudinal resistivity of two dimensional electrons placed in strong magnetic field is studied in broad range of temperatures. The data are in good agreement with theory, considering the strong nonlinearity of the resistivity as result of non-uniform spectral diffusion of 2D electrons induced by the electric field. Comparison with the theory gives inelastic scattering time τin of the 2D electrons. In temperature range T = 2 - 20 K for overlapping Landau levels, the inelastic scattering rate 1/τin is found to be proportional to T2, indicating d

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21

Rigler, Mark, and William Longo. "High Voltage Scanning Electron Microscopy Theory and Applications." Microscopy Today 2, no. 5 (1994): 12–13. http://dx.doi.org/10.1017/s1551929500066256.

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A variety of energy emissions occur as a result of primary beam interaction with the specimen surface. Secondary electrons, x-rays, visible photons, near IR photons, and Auger electrons are emitted during inelastic scattering of electrons. Backscattered electrons (BSE) are emitted during elastic scattering of primary electrons. Backscattered electrons are those electrons which pass through the electron cloud of an atom and change direction without much energy loss. BSEs may diffuse into the sample or may escape from the sample surface. In practice, the primary electron beam penetrates deeply i

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22

Wight, S. A., and C. J. Zeissler. "Phosphor Imaging Plate Measurement of Electron Scattering in the Environmental Scanning Electron Micrsoscope." Microscopy and Microanalysis 6, S2 (2000): 798–99. http://dx.doi.org/10.1017/s1431927600036485.

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In this work, phosphor imaging plate technology is applied to measure electron scattering directly in the environmental scanning electron microscope (ESEM) specimen chamber. The scattering of electrons from the primary electron beam, under relatively high-pressure conditions (266 Pa) in the ESEM sample chamber, degrades the analytical accuracy of elemental analysis. The degree of this degradation is poorly known. To date, attempts to measure experimentally the spatial distribution of the scattered electrons have been limited to observing secondary effects such as the intensity of x-rays produc

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23

Briones, J., H. C. Schneider, and B. Rethfeld. "Monte Carlo simulation of ultrafast nonequilibrium spin and charge transport in iron." Journal of Physics Communications 6, no. 3 (2022): 035001. http://dx.doi.org/10.1088/2399-6528/ac5873.

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Abstract Spin transport and spin dynamics after femtosecond laser pulse irradiation of iron (Fe) are studied using a kinetic Monte Carlo model. This model simulates spin dependent dynamics by taking into account two interaction processes during nonequilibrium: elastic electron–lattice scattering, where only the direction of the excited electrons changes, and inelastic electron–electron scattering processes, where secondary electrons are generated. An analysis of the spin dependent particle kinetics inside the material shows that a smaller elastic scattering time leads to a larger spatial sprea

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24

Vergados, J. D., Ch C. Moustakidis, Yeuk-Kwan E. Cheung, H. Ejiri, Yeongduk Kim, and Jeong-Yeon Lee. "Light WIMP Searches Involving Electron Scattering." Advances in High Energy Physics 2018 (2018): 1–14. http://dx.doi.org/10.1155/2018/6257198.

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In the present work we examine the possibility of detecting electrons in light dark matter searches. These detectors are considered to be the most appropriate for detecting dark matter particles with a mass in the MeV region. We analyze theoretically some key issues involved in such detection. More specifically we consider a particle model involving WIMPs interacting with fermions via Z-exchange. We find that for WIMPs with mass in the electron mass range the cross section for WIMP-atomic electron scattering is affected by the electron binding. For WIMPs more than 20 times heavier than the ele

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25

BARRANCO, J., A. BOLAÑOS, E. A. GARCÉS, O. G. MIRANDA, and T. I. RASHBA. "TENSORIAL NSI AND UNPARTICLE PHYSICS IN NEUTRINO SCATTERING." International Journal of Modern Physics A 27, no. 25 (2012): 1250147. http://dx.doi.org/10.1142/s0217751x12501473.

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We have analyzed the electron antineutrino scattering off electrons and the electron antineutrino–nuclei coherent scattering in order to obtain constraints on tensorial couplings. We have studied the formalism of nonstandard interactions (NSI) as well as the case of unparticle physics. For our analysis we have focused on the recent TEXONO collaboration results and we have obtained current constraints to possible electron antineutrino–electron tensorial couplings in both new physics formalisms. The possibility of measuring electron antineutrino–nucleus coherent scattering for the first time and

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26

Bronold, F. X., and H. Fehske. "Invariant embedding approach to secondary electron emission from metals." Journal of Applied Physics 131, no. 11 (2022): 113302. http://dx.doi.org/10.1063/5.0082468.

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Based on an invariant embedding principle for the backscattering function, we calculate the electron emission yield for metal surfaces at very low electron impact energies. Solving the embedding equation within a quasi-isotropic approximation and using the effective mass model for the solid experimental data are fairly well reproduced provided (i) incoherent scattering on ion cores is allowed to contribute to the scattering cascades inside the solid and (ii) the transmission through the surface potential takes into account Bragg gaps due to coherent scattering on crystal planes parallel to the

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27

Sanborn, B. A. "Total Dielectric Function Approach to the Electron Boltzmann Equation for Scattering from a Two-Dimensional Coupled Mode System." VLSI Design 6, no. 1-4 (1998): 69–72. http://dx.doi.org/10.1155/1998/70276.

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The nonequilibrium total dielectric function lends itself to a simple and general method for calculating the inelastic collision term in the electron Boltzmann equation for scattering from a coupled mode system. Useful applications include scattering from plasmon-polar phonon hybrid modes in modulation doped semiconductor structures. This paper presents numerical methods for including inelastic scattering at momentum-dependent hybrid phonon frequencies in the low-field Boltzmann equation for two-dimensional electrons coupled to bulk phonons. Results for electron mobility in GaAs show that the

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28

Frantsuzov, Viktor A., Anton Artemyev, Xiaofei Shi, and Anatoli A. Petrukovich. "Electron Heating by Magnetic Pumping and Whistler-mode Waves." Astrophysical Journal 963, no. 1 (2024): 16. http://dx.doi.org/10.3847/1538-4357/acfd2a.

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Abstract The investigation of mechanisms responsible for the heating of cold solar wind electrons around the Earth’s bow shock is an important problem in heliospheric plasma physics because such heating is vitally required to run the shock drift acceleration at the bow shock. The prospective mechanism for electron heating is magnetic pumping, which considers electron adiabatic (compressional) heating by ultralow-frequency waves and simultaneous scattering by high-frequency fluctuations. Existing models of magnetic pumping have operated with external sources of such fluctuations. In this study,

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29

VALERI, SERGIO. "MODULATED ELECTRON EMISSION." Surface Review and Letters 04, no. 05 (1997): 937–45. http://dx.doi.org/10.1142/s0218625x97001085.

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Basic aspects of energetic electron–atom scattering suffered by incident (primary) and/or excident (Auger, backscattered) electrons during propagation in (at least locally) ordered solids are reviewed. Scattering interference results in the dependence of total or partial electron yield on the incidence and/or takeoff angle. This paper is focused on processes experienced by incident electrons. The incident wave amplitude is spatially modulated within the solid by the interference of the unscattered wave portion and the wave portion scattered at the atomic sites. Interplay between forward focusi

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30

Maas, J. van der, R. Huguenin, and V. A. Gasparov. "Electron-electron scattering in tungsten." Journal of Physics F: Metal Physics 15, no. 11 (1985): L271—L278. http://dx.doi.org/10.1088/0305-4608/15/11/006.

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31

Zhao, J., J. Bass, W. P. Pratt, and P. A. Schroeder. "Electron-electron scattering in Li." Journal of Physics F: Metal Physics 16, no. 11 (1986): L271—L274. http://dx.doi.org/10.1088/0305-4608/16/11/003.

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32

Thomson, M. G. R. "Electron–electron scattering in microcolumns." Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures 12, no. 6 (1994): 3498. http://dx.doi.org/10.1116/1.587458.

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33

KHALILOV, V. R. "AHARONOV–BOHM EFFECT WITH SPIN-POLARIZED ELECTRONS." Modern Physics Letters A 21, no. 21 (2006): 1647–56. http://dx.doi.org/10.1142/s0217732306020962.

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The scattering of spin-polarized electrons in an Aharonov–Bohm vector potential is considered. The scattering cross-sections for spin-unpolarized and spin-polarized electron beams differ. It is shown that a bound electron state may occur if the interaction of electron spin with magnetic field having the form of two-dimensional delta function is included. The occurrence of bound state can modify the scattering states but the total cross-section does not change.

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34

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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35

Wang, Z. L. "Energy-filtered high-resolution Electron Microscopy of nanostructured materials." Proceedings, annual meeting, Electron Microscopy Society of America 53 (August 13, 1995): 176–77. http://dx.doi.org/10.1017/s0424820100137252.

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The interaction between an incident electron and the atoms in condensed matter results in various inelastic scattering processes. Thermal diffuse scattering or phonon scattering is the result of atomic vibrations in crystals. This process does not introduce any significant energy-loss (< 0.1 eV) but produces large momentum transfer. Valence-loss (or plasmon for metals and semiconductors) excitation, which characterizes the transitions of electrons from the valence band to the conduction band, involves an energyloss in the range of 1 -50 e V. Atomic inner-shell ionization is excited by the e

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Wang, L., J. Liu, and J. M. Cowley. "Zero-Loss Energy Filtered REM and RHEED Observations on Rutile (110) Surface." Proceedings, annual meeting, Electron Microscopy Society of America 51 (August 1, 1993): 968–69. http://dx.doi.org/10.1017/s0424820100150678.

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In reflection electron microscopy (REM), the surface reflection electrons undergo both elastic and inelastic scattering within a crystal. The dominant inelastic processes are phonon scattering, valence electron excitation, bulk and surface plasmon excitation and combinations of these processes. Multiple inelastic scattering processes are also probable as the mean traveling distance of surface reflection electrons is about 10 to 100 nm. In reflection high energy electron diffraction pattern (RHEED), 50% to 90% of the electrons contributing to surface reflection spots used for imaging have suffe

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DING, Z. J., X. D. TANG, and H. M. LI. "MONTE CARLO CALCULATION OF THE ENERGY DISTRIBUTION OF BACKSCATTERED ELECTRONS." International Journal of Modern Physics B 16, no. 28n29 (2002): 4405–12. http://dx.doi.org/10.1142/s0217979202015509.

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The full energy distribution of backscattered electrons from elastic peak down to true secondary electron peak has been calculated by a Monte-Carlo simulation method by including cascade secondary electrons production. The simulation method is based on the use of a dielectric function for describing electron inelastic scattering and secondary excitation, and the use of Mott cross section for electron elastic scattering. This calculation reproduces well the backscattering background observed in the direct mode of AES. The calculated absolute electron yields have been compared with the available

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38

Moodie, A. F., and J. C. H. Spence. "John Maxwell Cowley 1923 - 2004." Historical Records of Australian Science 17, no. 2 (2006): 227. http://dx.doi.org/10.1071/hr06012.

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John Cowley contributed significantly to all of the fields that relate to electron diffraction and electron microscopy, and helped to found not a few of them. His name is associated in particular with n-beam dynamical theory, high-resolution electron microscopy, scanning transmission electron microscopy, instrumental design, and the application of the techniques of electron scattering to structure analysis. His experimental work was not, however, confined to the scattering of electrons: to take but one instance, his seminal work on the theory of short-range order was stimulated initially by hi

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YANG, Y. H. "MAGNETIC SCATTERING EFFECTS IN A QUASI-TWO-DIMENSIONAL DISORDERED ELECTRON SYSTEM." Modern Physics Letters B 14, no. 27n28 (2000): 995–1000. http://dx.doi.org/10.1142/s0217984900001257.

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The weak-localization correction to the conductivity for a quasi-two-dimensional disordered electron system is calculated in the presence of magnetic impurity scatterings. The analytical result is obtained as a function of the magnetic scattering time, and the interesting magnetic-scattering-dependent crossover behavior from 3D to 2D is discussed.

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Marsiglio, F., and J. P. Carbotte. "Quasiparticle Lifetimes and the Conductivity Scattering Rate." Australian Journal of Physics 50, no. 6 (1997): 1011. http://dx.doi.org/10.1071/p97004.

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We compute the single-particle inverse lifetime, along with the conductivity-derived scattering rate, for a metallic system in an s-wave superconducting state. When both electron–phonon and electron-impurity scattering are included, we find that while these scattering rates are in qualitative agreement, in general quantitative agreement is lacking. We also derive results for the quasiparticle lifetime within the BCS framework with impurity scattering, which makes it clear that impurity scattering is suppressed for electrons near the Fermi surface in the superconducting state.

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Li, Zheng, Hailong Wang, Li Chen, Sha Chen, and Qian Gong. "The electron-longitudinal optical phonon scattering rate in GaInAsP/InP stepped quantum well." International Journal of Modern Physics B 30, no. 26 (2016): 1650196. http://dx.doi.org/10.1142/s0217979216501964.

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Within the framework of effective mass approximation, the scattering rate via longitudinal optical (LO) phonon emission for an electron and the mean scattering rate via LO phonons emission for electrons initially in the first excited sub-band and finally in the ground sub-band in [Formula: see text] stepped quantum well (QW) is calculated adopting the shooting method and Fermi’s golden rule. The results show that the scattering rate and the mean scattering rate are highly dependent on alloy compositions, well width, initial electron energy, electron temperature and sub-band separation [Formula

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42

Bezuglyi, E. V., N. G. Burma, A. L. Gaiduk, et al. "Electron sound in aluminum. Electron–electron scattering." Low Temperature Physics 24, no. 3 (1998): 169–81. http://dx.doi.org/10.1063/1.593567.

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43

Artamonov, O. M., S. N. Samarin, and J. F. Williams. "Electron screening and electron–electron scattering mechanisms." Journal of Electron Spectroscopy and Related Phenomena 191 (December 2013): 79–85. http://dx.doi.org/10.1016/j.elspec.2013.11.005.

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Milliman, T. E., J. P. Connelly, J. H. Heisenberg, F. W. Hersman, J. E. Wise, and C. N. Papanicolas. "Electron scattering fromMo92." Physical Review C 41, no. 6 (1990): 2586–604. http://dx.doi.org/10.1103/physrevc.41.2586.

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Glickman, J. P., W. Bertozzi, T. N. Buti, et al. "Electron scattering fromBe9." Physical Review C 43, no. 4 (1991): 1740–57. http://dx.doi.org/10.1103/physrevc.43.1740.

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Cichocki, A., J. Dubach, R. S. Hicks, et al. "Electron scattering fromB10." Physical Review C 51, no. 5 (1995): 2406–26. http://dx.doi.org/10.1103/physrevc.51.2406.

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47

Williams, I. D. "Electron-ion scattering." Reports on Progress in Physics 62, no. 10 (1999): 1431–69. http://dx.doi.org/10.1088/0034-4885/62/10/202.

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Kleinpoppen, H. "Electron-scattering experiments." Nature 330, no. 6143 (1987): 20. http://dx.doi.org/10.1038/330020a0.

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RÄDEL, GABY, and ROLF BEYER. "NEUTRINO ELECTRON SCATTERING." Modern Physics Letters A 08, no. 12 (1993): 1067–88. http://dx.doi.org/10.1142/s0217732393002567.

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Abstract:

This article reviews experimental results obtained from studies of neutrino electron scattering and shows in particular the important input from these experiments to the improved knowledge of weak neutral currents and the confirmation of the Standard Model at tree level. Special emphasis is put on recent high precision νe-experiments, whose results on electroweak parameters allow, in combination with precise results obtained at higher Q2, a test of the Standard Model at the level of higher order corrections.

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50

Sick, I. "Inclusive electron scattering." Progress in Particle and Nuclear Physics 34 (January 1995): 323–43. http://dx.doi.org/10.1016/0146-6410(95)00029-i.

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