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Journal articles on the topic 'Influence of electron'

Author: Grafiati

Published: 28 May 2022

Last updated: 31 July 2025

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1

Boiko, I. I. "Influence of electron-electron drag on piezoresistance of n-Si." Semiconductor Physics Quantum Electronics and Optoelectronics 14, no. 2 (2011): 183–87. http://dx.doi.org/10.15407/spqeo14.02.183.

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2

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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3

Myrvang, Margaretha, Carsten Baumann, and Ingrid Mann. "Modelling the influence of meteoric smoke particles on artificial heating in the D-region." Annales Geophysicae 39, no. 6 (2021): 1055–68. http://dx.doi.org/10.5194/angeo-39-1055-2021.

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Abstract. We investigate if the presence of meteoric smoke particles (MSPs) influences the electron temperature during artificial heating in the D-region. By transferring the energy of powerful high-frequency radio waves into thermal energy of electrons, artificial heating increases the electron temperature. Artificial heating depends on the height variation of electron density. The presence of MSPs can influence the electron density through charging of MSPs by electrons, which can reduce the number of free electrons and even result in height regions with strongly reduced electron density, so-

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4

Zhang, Shufeng. "Influence of electron relaxation on electron tunneling." Journal of Applied Physics 87, no. 9 (2000): 5218–20. http://dx.doi.org/10.1063/1.373300.

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5

Xiang, Ran, Xin Yu Tan, and Hui Li Wei. "Influence of Electron-Phonon Coupling Coefficient on Properties in Femtosecond Laser Ablation." Materials Science Forum 814 (March 2015): 144–49. http://dx.doi.org/10.4028/www.scientific.net/msf.814.144.

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Thermodynamics effects generated by femtosecond laser ablation are very important. In this work, the numerical simulation of high-energy femtosecond laser ablation especially the electro-phonon coupling coefficient influence of high-energy femtosecond laser ablation on metal target was studied. A new two-temperature model (TTM) which considered the effects of electron density of states (DOS) on electron-phonon coupling coefficient was first established, then the temperature evolvement for electron and lattice in different electro-phonon coupling coefficient G, and the effect of G on electron t

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6

Dedulewicz, S., and Ž. Kancleris. "Electron-Electron Scattering Influence on Hot Electron Transport in Semiconductors." Acta Physica Polonica A 80, no. 3 (1991): 353–56. http://dx.doi.org/10.12693/aphyspola.80.353.

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7

He, Li Jun. "Influence of Pressure of Electron Gas on Elastic Property of Metal." Advanced Materials Research 602-604 (December 2012): 857–60. http://dx.doi.org/10.4028/www.scientific.net/amr.602-604.857.

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A balloon filled with electron gas model was built to simulate metal for calculating its bulk elastic. Electron gas obeyed Fermi-Dirac distribution and satisfied with theory of ideal gas. Expression of metal bulk elastic modulus was derived, and the comparison between the new method given in this paper with current method according to theory of atom potential energy on calculation accuracy was also given. It showed that, pressure of electron gas closely related to bulk elastic modulus, and maybe it was the major factor in determining bulk elastic modulus of metal; not all of valence electrons

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8

Guerrero, A. H. "Influence of electron-electron interactions on the transfer of single electrons between quantum dots." Semiconductor Science and Technology 7, no. 3B (1992): B292—B294. http://dx.doi.org/10.1088/0268-1242/7/3b/072.

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9

Zhmurin, P. N. "Influence of electron-donor additive on properties of plastic scintillator." Functional Materials 21, no. 2 (2014): 195–99. http://dx.doi.org/10.15407/fm21.02.195.

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10

Pagonakis, Ioannis, Stefano Alberti, Konstantinos Avramidis, et al. "Overview on recent progress in magnetron injection gun theory and design for high power gyrotrons." EPJ Web of Conferences 203 (2019): 04011. http://dx.doi.org/10.1051/epjconf/201920304011.

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The magnetron injection gun (MIG) is one of the most critical subcomponents in gyrotrons. The electron beam, which has the primary role on the gyrotron operation, is generated and configured at this part of the tube. The electron beam properties determine the excitation mode in the cavity, the power of the generated microwaves and the gyrotron efficiency. The operation of MIGs could be influenced by several factors such as trapped electrons, manufacturing tolerances, roughness of the emitter ring, emitter temperature inhomogeneity, electron beam neutralization effect, etc. The influence of man

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11

Proto, Andrea, and Jon Gudmundsson. "The Influence of Secondary Electron Emission and Electron Reflection on a Capacitively Coupled Oxygen Discharge." Atoms 6, no. 4 (2018): 65. http://dx.doi.org/10.3390/atoms6040065.

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The one-dimensional object-oriented particle-in-cell Monte Carlo collision code oopd1 is applied to explore the role of secondary electron emission and electron reflection on the properties of the capacitively-coupled oxygen discharge. At low pressure (10 mTorr), drift-ambipolar heating of the electrons dominates within the plasma bulk, while at higher pressure (50 mTorr), stochastic electron heating in the sheath region dominates. Electron reflection has negligible influence on the electron energy probability function and only a slight influence on the electron heating profile and electron de

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12

Shang, Tianyi, and Weidong Ding. "Influence of gas pressure and gas type on pseudospark electron beam." Journal of Instrumentation 18, no. 09 (2023): P09045. http://dx.doi.org/10.1088/1748-0221/18/09/p09045.

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Abstract Pseudospark discharge is a discharge that occurs in the left band of the Paschen curve. According to previous studies, an electron beam will be generated in the initial stage of pseudospark discharge. This electron beam has the advantages of high energy, high current and self-confinement. It has a promising application in high-power microwave sources, surface treatment of metal materials, etc. To investigate the characteristics of this electron beam, a pseudospark discharge experimental platform is established in this paper. A pseudospark chamber is designed for pseudospark discharge.

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13

Lifa, A., S. Dilmi, and S. E. Bentridi. "The Influence of Hot Electrons on the Calculation of Ionization Rates." Engineering, Technology & Applied Science Research 12, no. 6 (2022): 9579–83. http://dx.doi.org/10.48084/etasr.5294.

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Electron-Impact Ionization (EII) is considered one of the most important ionization methods in dynamic systems, in which elements and ions are suddenly exposed to energetic electrons. In many plasma types, it has been observed that some electrons (hot) are governed by a non-Maxwellian energy distribution. This study illustrates the effects of a non-Maxwellian distribution on beryllium and Be+2 emission lines and their effective ionization rate coefficients. The focus on beryllium as an impacted material by electron flux aimed to evaluate the EII rates for Be and generate the corresponding data

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14

Schmidt, Tobias, and Stephan Kümmel. "The Influence of One-Electron Self-Interaction on d-Electrons." Computation 4, no. 3 (2016): 33. http://dx.doi.org/10.3390/computation4030033.

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15

Raghunathan, Ananthan, and John G. Hartley. "Influence of secondary electrons in high-energy electron beam lithography." Journal of Vacuum Science & Technology B, Nanotechnology and Microelectronics: Materials, Processing, Measurement, and Phenomena 31, no. 1 (2013): 011605. http://dx.doi.org/10.1116/1.4774114.

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16

Ovsyannikov, V. P., F. Ullmann, and G. Zschornack. "Influence of electron injection on electron cyclotron resonance plasma properties and reflected mode electrons (abstract)." Review of Scientific Instruments 71, no. 2 (2000): 859. http://dx.doi.org/10.1063/1.1150145.

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17

CRISAN, M. "MICROSCOPIC THEORY OF THE CONCENTRATION FLUCTUATIONS IN HIGH TEMPERATURE SUPERCONDUCTORS." Modern Physics Letters B 01, no. 11n12 (1988): 405–8. http://dx.doi.org/10.1142/s0217984988001478.

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We considered the influence of the concentration fluctuations of the electrons due to the doping, on the occurrence of the high temperature superconductivity. A microscopic model has beeen given and the influence of the concentration fluctuation on the attractive electron-electron interaction and on the Fermi energy was discussed.

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18

Sirenko, Yu M., and P. Vasilopoulos. "Coupled electron-electron and electron-hole transport: Influence of dimensionality and statistics." Superlattices and Microstructures 12, no. 3 (1992): 403–7. http://dx.doi.org/10.1016/0749-6036(92)90291-c.

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19

Deng, Chenhui, Jingyu Huang, Libing Zheng, Li Han, Geng Niu, and Pengfei Wang. "Study of the Effect of Magnetic Fields on the Secondary Electron Model." Electronics 14, no. 12 (2025): 2446. https://doi.org/10.3390/electronics14122446.

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Secondary electron emission (SEE), a common physical phenomenon, exhibits both prominent applications in various fields and concomitant adverse impacts. Secondary electron yield (SEY) is a parameter for characterizing SEE, which determines the effect of the application and is very sensitive to the surroundings, particularly the magnetic field. Previous studies mainly focused on the influence of the magnetic field on secondary electron trajectories rather than the SEY itself. In this work, a specialized experimental platform was established to measure SEY, through which the influences caused by

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20

Adamenko, I. N., A. V. Zhukov, and K. É. Nemchenko. "Influence of electron–electron interaction on the mobility of electrons on the surface of liquid helium." Low Temperature Physics 26, no. 7 (2000): 459–63. http://dx.doi.org/10.1063/1.1306398.

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21

Bessudnova, Nadezhda, Andrej Rozhnev, and Dmitriy Trubetskov. "Influence of thermal velocity distribution on electron beam - backward electromagnetic wave interaction." Izvestiya VUZ. Applied Nonlinear Dynamics 7, no. 5 (1999): 70–79. http://dx.doi.org/10.18500/0869-6632-1999-7-5-70-79.

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One—dimensional linear theory of interaction between electron beam and backward electromagnetic wave in transmission line is presented taking into account arbitrary velocity distribution of electrons and allowing correct consideration of finite length of interaction region. Influence of electron velocity spread оn start oscillation regime of low— voltage backward—wave oscillator is analysed. Calculations are carried out for rectangular, Lorentz and Maxwell distributions.

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22

Kralkina, Elena, Polina Nekludova, Aleksander Nikonov, Konstantin Vavilin, Ilya Zadiriev, and Vladimir Tarakanov. "Influence of external parameters on RF inductive discharge plasma characteristics." Plasma Sources Science and Technology 30, no. 11 (2021): 115020. http://dx.doi.org/10.1088/1361-6595/ac331a.

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Abstract Systematic experimental studies of the electron density and temperature, the efficiency of RF power coupling to the RF inductive discharge plasma have been carried out in the pressure range of helium, neon, argon, and krypton 0.1–133 Pa, at an RF generator power of 100–500 W and frequencies of 2, 4 and 13.56 MHz. It is shown that the electron density reaches a maximum, and the temperature reaches a minimum in the pressure range 1.33–13.3 Pa. Taking into account the presence of a parasitic capacitive coupling between the inductor and the plasma, which forms the capacitive channel of RF

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23

Stevanovic, Nenad, Vladimir Markovic, Momir Arsenijevic, and Dragoslav Nikezic. "Influence of electron motion in target atom on stopping power for low-energetic ions." Nuclear Technology and Radiation Protection 27, no. 2 (2012): 113–16. http://dx.doi.org/10.2298/ntrp1202113s.

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In this paper the stopping power was calculated, representing the electrons of the target atom as an assembly of quantum oscillators. It was considered that the electrons in the atoms have some velocity before interaction with the projectile, which is the main contribution of this paper. The influence of electron velocity on stopping power for different projectiles and targets was investigated. It was found that the velocity of the electron stopping power has the greatest influence at low energies of the projectile.

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24

Louksha O. I., Zuev A. S., Malkin A. G., Semenov E. S., Trofimov P. A., and Glyavin M. Yu. "Trajectory analysis in a collector with multistage energy recovery for a DEMO prototype gyrotron. Part III. Influence of the spent electron beam parameters." Technical Physics 68, no. 5 (2023): 670. http://dx.doi.org/10.21883/tp.2023.05.56075.14-23.

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The influence of the spent electron beam parameters on the possibilities of multistage energy recovery in the prototype gyrotron developed for the DEMO project is determined. The characteristics of electrodes and magnetic coils in a collector with four-stage recovery were optimized considering the distributions of electrons' coordinates and velocities obtained as a result of calculating the electron-wave interaction in the cavity. In the trajectory analysis in the collector, a sectioned electron beam was used to suppress the negative influence of the bundles of a toroidal solenoid used to crea

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25

Uehlein, Markus, Sebastian T. Weber, and Baerbel Rethfeld. "Influence of Electronic Non-Equilibrium on Energy Distribution and Dissipation in Aluminum Studied with an Extended Two-Temperature Model." Nanomaterials 12, no. 10 (2022): 1655. http://dx.doi.org/10.3390/nano12101655.

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When an ultrashort laser pulse excites a metal surface, only a few of all the free electrons absorb a photon. The resulting non-equilibrium electron energy distribution thermalizes quickly to a hot Fermi distribution. The further energy dissipation is usually described in the framework of a two-temperature model, considering the phonons of the crystal lattice as a second subsystem. Here, we present an extension of the two-temperature model including the non-equilibrium electrons as a third subsystem. The model was proposed initially by E. Carpene and later improved by G.D. Tsibidis. We introdu

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26

Yukhnovskii, I. R., and M. V. Vavrukh. "Many-body approach to the determination of the energy spectrum of multicomponent superconductors." Soviet Journal of Low Temperature Physics 13, no. 11 (1987): 693–94. https://doi.org/10.1063/10.0031832.

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An approach is proposed for the description of superconducting systems which takes into account the electron structure of the ions, correlations in a system of collectivized electrons, and electron-phonon interactions. The effective Hamiltonian of the subsystem of conduction electrons responsible for the transition to the superconducting state is obtained. A preliminary estimate of the influence of electron correlations on the transition temperature is carried out.

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27

ROMANENKO, A. I., O. B. ANIKEEVA, T. I. BURYAKOV, et al. "INFLUENCE OF CURVATURE OF GRAPHENE LAYERS OF MULTI-WALLED CARBON NANOTUBES ON ELECTRICAL PROPERTIES." International Journal of Nanoscience 08, no. 01n02 (2009): 1–4. http://dx.doi.org/10.1142/s0219581x09005608.

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We investigated temperature and magnetic field dependences of conductivity of multi-walled carbon nanotubes (MWNTs) with different average outer diameter. We separated out the quantum corrections to magnetoconductivity for interaction electrons and determined the dependence of constant of electron–electron interaction λ versus curvature of graphene layers in MWNTs.

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28

Panchenko, O. F., and L. K. Panchenko. "Relaxation of Highly Non Equilibrium Charge Carriers in Crystals by Low-Energy Electron Influence." Solid State Phenomena 115 (August 2006): 261–66. http://dx.doi.org/10.4028/www.scientific.net/ssp.115.261.

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The cascade process describing the energy loss and relaxation or multiplication of highly non-equilibrium secondary electrons and holes in crystalline platinum irradiated by lowenergy electrons is studied. The pair-creation scattering rates are evaluated in the framework of the statistical model taking into account the electron band structure of platinum. Kinetic equations for the excited electron and hole energy distributions are solved numerically in the isotropic scattering approximation for some primary (excitation) energies Ep which do not exceed the plasma energy.

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29

Vil’k, Yu M., and Yu P. Monarkha. "Influence of correlation effects on relaxation processes in a two-dimensional electron system on helium surface." Soviet Journal of Low Temperature Physics 15, no. 3 (1989): 131–37. https://doi.org/10.1063/10.0032129.

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Relaxation processes in a two-dimensional electron system are investigated without using the quasi-classical description under the conditions when the autocorrelation time τee, for the electron velocity is much shorter than the relaxation time of the system. A relation between the low-frequency conductivity and the energy loss rate of surface electrons, and the dynamic form factor of the two-dimensional electron liquid is established. It is shown that for the same values of the fundamental parameter Γ, equal to the ratio of the mean Coulomb energy to temperature, the contribution of correlatio

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30

Starodub, S. S., S. P. Roshchupkin, and V. V. Dubov. "Effective interaction of electrons in the field of two strong laser waves with phase shifts allowance." Laser and Particle Beams 36, no. 1 (2018): 55–59. http://dx.doi.org/10.1017/s0263034617000921.

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AbstractThe phase shift's influence of two strong-pulsed laser waves on effective interaction of electrons was studied. Considerable amplification of electron repulsion in the certain range of phase shifts and wave intensities is shown. That leads to electron scatter on greater distances than without an external field. The value of the distance can be greater on 2–3 order of magnitude. Considerable influence of the phase shift of pulses of waves on the possibility of effective attraction of electrons is also shown.

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31

Лукша, О. И., А. С. Зуев, А. Г. Малкин, Е. С. Семенов, П. А. Трофимов та М. Ю. Глявин. "Траекторный анализ в коллекторе с многоступенчатой рекуперацией энергии для прототипа гиротрона DEMO. Ч. III. Влияние параметров отработанного электронного потока". Журнал технической физики 93, № 5 (2023): 718. http://dx.doi.org/10.21883/jtf.2023.05.55468.14-23.

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The influence of the spent electron beam parameters on the possibilities of multistage energy recovery in the prototype gyrotron developed for the DEMO project is determined. The characteristics of electrodes and magnetic coils in a collector with four-stage recovery were optimized considering the distributions of electrons' coordinates and velocities obtained as a result of calculating the electron-wave interaction in the cavity. In the trajectory analysis in the collector, a sectioned electron beam was used to suppress the negative influence of the bundles of a toroidal solenoid used to crea

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32

Jablonski, A., and S. Tougaard. "Escape probability of electrons from solids. Influence of elastic electron scattering." Surface Science 432, no. 3 (1999): 211–27. http://dx.doi.org/10.1016/s0039-6028(99)00521-x.

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33

Boroński, Edward. "Influence of Electron-Electron Correlations and Lattice Effects on Positron-Electron Enhancement Factors." Materials Science Forum 666 (December 2010): 5–9. http://dx.doi.org/10.4028/www.scientific.net/msf.666.5.

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We present an approach taking into account the effect of electron-electron (e-e) correlations on electron-positron (e-p) momentum density distributions. The approach bases on the modification of the Bethe-Goldstone (B-G) equation for the positron in the electron gas due to self-energy effects. The example calculations have been performed for selected parameters corresponding to simple metals. The calculated dependencies exhibit the increase of the e-p enhancement factors below Fermi momentum, like Kahana enhancements, and a decrease above the Fermi sphere, leading to a many-body “tail” in the

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34

Liang, Li Min, Xin Jian Xie, Qiu Yan Hao, Yuan Tian, Wei Zhong Sun, and Cai Chi Liu. "Influence of Electron Irradiation on the Yellow Luminescence in Undoped n-GaN." Advanced Materials Research 571 (September 2012): 125–28. http://dx.doi.org/10.4028/www.scientific.net/amr.571.125.

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The yellow luminescence (YL) band in unintentional doped n-GaN irradiated by 10 MeV electrons has been investigated by means of photoluminescence (PL) spectroscopy. The YL intensity increased after electron irradiation and thermal annealing, indicating that the deep level defects are created by electron irradiation and thermal annealing. These deep level point defect complexes arising from the irradiation introduced Ga vacancies and oxygen donor impurities are responsible for the YL.

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35

Nikitovic, Zeljka, and Vladimir Stojanovic. "The influence of F, F2 on kinetics of electrons in BF3." Chemical Industry 65, no. 3 (2011): 229–32. http://dx.doi.org/10.2298/hemind110110014n.

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We present transport coefficients for electrons in mixtures of BF3 with its radicals (specifically F and F2) for ratios of the electric field to the gas number density E/N from 1 to 1000 Td (1 Td = 10-21 V m2). Our analysis of non-conservative collisions revealed a range of E/N where electron attachment to radicals significantly changes the electron kinetics compared to pure gaseous BF3. The results were obtained using simple solutions for Boltzmann?s equation and Monte Carlo simulation.

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36

Engström, K., J. Kinaret, R. I. Shekhter, M. Puska, and H. Saarikoski. "Influence of electron–electron interactions on supercurrent in SNS structures." Low Temperature Physics 29, no. 7 (2003): 546–50. http://dx.doi.org/10.1063/1.1596575.

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37

Lian, Hu, K. Y. Szeto, and Sun Xin. "Influence of Strong Electron-Electron Interaction on the Peierls Transition." Chinese Physics Letters 14, no. 1 (1997): 63–66. http://dx.doi.org/10.1088/0256-307x/14/1/017.

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38

Chuev, G. N., and N. L. Leonova. "Influence of electron–electron correlations on bipolaron in strong electrolytes." Physics Letters A 278, no. 1-2 (2000): 103–7. http://dx.doi.org/10.1016/s0375-9601(00)00759-3.

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39

Shi Han-Xu, Li Xin-Yang, Zhang Yu-Ru, and Wang You-Nian. "Numerical investigation of the secondary electron effect in capacitively coupled plasmas driven by ultra-low frequency/radio frequency sources." Acta Physica Sinica 74, no. 13 (2025): 0. https://doi.org/10.7498/aps.74.20250341.

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In recent years, capacitively coupled plasmas driven by ultra-low frequency source have garnered increasing attention, because they are beneficial for generating ions with high energy and small scattering angle, which aligns well with the current trend in high aspect ratio etching. Since the sheath becomes thicker when a ultra-low frequency source is applied, the secondary electron emission becomes significant. Indeed, these energetic secondary electrons could enhance the ionization process and even influence the discharge mode. In this work, a two-dimensional fluid model is employed to study

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40

Singh, Shiv, and Punit Kumar. "Ponderomotive effects in spin—polarized quantum plasma." Laser Physics 33, no. 7 (2023): 076004. http://dx.doi.org/10.1088/1555-6611/acd374.

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Abstract Analysis of ponderomotive effects exciting from propagation of an intense laser pulse through high density quantum plasma under the influence of an axial magnetic field taking into consideration the spin–spin (up and down) exchange interaction. The effects of electron Fermi pressure, quantum Bohm potential, and electron spin have been included in the analysis. Spin polarization is a result of the concentration difference of opposite spin electrons which is produced under the influence of the applied magnetic field. Axial gradient of the ponderomotive potential of laser has been applie

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41

Li, Kai, and Wen Yi Huo. "The nonlocal electron heat transport under the non-Maxwellian distribution in laser plasmas and its influence on laser ablation." Physics of Plasmas 30, no. 4 (2023): 042702. http://dx.doi.org/10.1063/5.0130888.

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The electron heat transport plays an important role in laser driven inertial confinement fusion. For the plasmas created by intense laser, the traditional Spitzer–Härm theory cannot accurately describe the electron heat transport process mainly due to two physical effects. First, the electron distribution function would significantly differ from the Maxwellian distribution because of the inverse bremsstrahlung heating. Second, the long mean free paths of heat carrying electrons relative to the temperature scale length indicate that the electron heat flux has the nonlocal feature. In 2020, we h

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42

Duras, J., R. Schneider, O. Kalentev, et al. "Influence of Electron Sources on the Near-field Plume in a Multistage Plasma Thruster." PLASMA PHYSICS AND TECHNOLOGY 3, no. 3 (2016): 126–30. http://dx.doi.org/10.14311/ppt.2016.3.126.

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n order to obtain a better understanding of the near-field plume of a multistage plasma thruster, the influence of an external electron source is investigated by Particle-In-Cell simulations. The variation of the source position showed a strong influence of the magnetic field configuration on the electron distribution and therefore on the plume plasma. In the second part of this work, higher energetic electrons were injected in order to model collision-induced diffusion in the plume. This broadens the electron distribution, which leads to a more pronounced divergence angle in the angular ion d

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43

Bonnaud, G. "Ion mobility influence on stimulated Raman scattering in homogeneous laser-irradiated plasma." Laser and Particle Beams 5, no. 1 (1987): 101–14. http://dx.doi.org/10.1017/s0263034600002524.

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1½ D computer simulations have been performed to illustrate the influence of ion dynamics on stimulated Raman scattering in laser irradiated plasmas. A flat density profile has been used. Backward and forward scatter and heated electron distribution have been studied as a function of ion mass and ion temperature. The results show clearly that the lighter the ions, the more inhibited the Raman scatter and associated fast electron production. Futhermore, when ions are cold enough to allow Brillouin scattering release, Raman scatter, as well as associated suprathermal electrons is even more reduc

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44

Zhao, J. C., L. H. Cao, J. H. Zheng та ін. "The model of the influence of the electron refluxing on the electron transport and Kα emission". Laser and Particle Beams 35, № 3 (2017): 483–91. http://dx.doi.org/10.1017/s0263034617000465.

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AbstractIn our previous research (Zhao et al., 2016), we focus on the transport processes from hot electrons to Kα X-ray emission in a copper foil and nanobrush target when the electron refluxing effect is not taken into account. In this work, considering the refluxing effect, the transport of hot electrons in a solid target is studied by adding the electric fields both at the front and rear surfaces of the target with Monte Carlo code Geant4. Simulation results show that the electron refluxing has an important influence on Kα photon yield and the size of Kα radiation source. Kα yield from the

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45

Niciejewski, R. J., and P. A. Forsyth. "Auroral influence on ionospheric electron content." Canadian Journal of Physics 66, no. 2 (1988): 175–81. http://dx.doi.org/10.1139/p88-026.

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A number of earlier investigations have established that regions of enhanced electron concentration in the ionosphere are often associated, both temporally and spatially, with optical auroral features. Attempts to determine whether these enhancements are completely accounted for by the same particle precipitation that causes the aurora have been only partially successful, largely because it is difficult to collect data over a sufficient time with sufficient spatial resolution to permit accurate modelling. This paper attempts to take one more step along this road by using photometer records, ta

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Horný, Vojtěch, та Ondřej Klimo. "Hot electron refluxing in the short intense laser pulse interactions with solid targets and its influence on K-α radiation". Nukleonika 60, № 2 (2015): 233–37. http://dx.doi.org/10.1515/nuka-2015-0045.

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Abstract Fast electrons created as a result of the laser beam interaction with a solid target penetrate into the target material and initialize processes leading to the generation of the characteristic X-ray K-α radiation. Due to the strong electric field induced at the rear side of a thin target the transmitted electrons are redirected back into the target. These refluxing electrons increase the K-α radiation yield, as well as the duration of the X-ray pulse and the size of the radiation emitting area. A model describing the electron refluxing was verified via particle-in-cell simulations for

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Nasirov, M. Z., S. D. Matbabayeva, and R. Aliev. "Influence of an Electric Field on the Electron Motion in Multilayer Quantum Nanostructures." Elektronnaya Obrabotka Materialov 61, no. 1 (2025): 65–72. https://doi.org/10.52577/eom.2025.61.1.065.

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The article uses an analytical solution to the Schrödinger equation for an electron in each layer and the boundary conditions between layers to simulate the behavior of electrons in multilayer quantum nanostructures, and also creates a Visual Basic program for the process under consideration. The program has the ability to change the effective mass of an electron in each layer, the height and width of the potential barrier in it, to calculate the coefficients of transmission and the return of electrons through barriers and the probability of being in them, and also to send the calculation resu

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Hsu, Shih-Ying, and J. M. Valles. "Electron tunneling into strongly disordered films: The influence of structure on electron-electron interactions." Physical Review B 49, no. 23 (1994): 16600–16604. http://dx.doi.org/10.1103/physrevb.49.16600.

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Bai, Jinzhou, Yonglin Bai, Xun Hou, et al. "The analysis of electron scattering among multiplying layer in EBAPS using optimized Monte Carlo method." Modern Physics Letters B 34, no. 34 (2020): 2050398. http://dx.doi.org/10.1142/s0217984920503984.

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Electron bombarded Active Pixel Sensor (EBAPS) is well known for its low noise in low-light level imaging, high mechanical integration, and a relatively low cost. It plays an important role in areas of the industrial process as well as the fundamental scientific research. However, the performance of EBAPS is intensively influenced by the structural parameters (i.e. the acceleration voltage between cathode and anode, thickness of the passivation layer, etc.). Due to the influence of these factors mentioned above, the performance of EBAPS is restricted to achieve its best condition. Herein, a mo

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WU Jiangcheng, YIN Yuting, and FANG Henan. "Theoretical study on the interlayer conductance of MoS<sub>2</sub> moiré superlattices." Acta Physica Sinica 74, no. 16 (2025): 0. https://doi.org/10.7498/aps.74.20250434.

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As a typical material of two-dimensional semiconductor transition metal chalcogenides, MoS<sub>2</sub> has excellent physical properties such as tunable band gap. Therefore, MoS<sub>2</sub> moirésuperlattice is an ideal system for investigating the electron transport in condensed matter and the design of optoelectronic devices. On the other hand, interlayer conductance serves as a significant indicator for analyzing coupling effects in moiré superlattice. Here, in order to clarify the influence of tunable band gap on the interlayer conductance, we have developed a tunne

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