標(biāo)題: Titlebook: Collisions of Electrons with Atoms and Molecules; G. F. Drukarev Book 1987 Plenum Press, New York 1987 Cross section.Plasma.atomic collisi [打印本頁] 作者: Flippant 時(shí)間: 2025-3-21 18:06
書目名稱Collisions of Electrons with Atoms and Molecules影響因子(影響力)
書目名稱Collisions of Electrons with Atoms and Molecules影響因子(影響力)學(xué)科排名
書目名稱Collisions of Electrons with Atoms and Molecules網(wǎng)絡(luò)公開度
書目名稱Collisions of Electrons with Atoms and Molecules網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱Collisions of Electrons with Atoms and Molecules被引頻次
書目名稱Collisions of Electrons with Atoms and Molecules被引頻次學(xué)科排名
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書目名稱Collisions of Electrons with Atoms and Molecules讀者反饋
書目名稱Collisions of Electrons with Atoms and Molecules讀者反饋學(xué)科排名
作者: burnish 時(shí)間: 2025-3-21 20:46
Book 1987sed to those who by nature of their work need detailed information about the cross sections of various processes of electron collisions with atomic particles: experimentalists working in plasma physics, optics, quantum electronics, atmospheric and space physics, ‘etc. Some of the cross sections have作者: 好開玩笑 時(shí)間: 2025-3-22 00:34
Heiko Lippold,Paul Schmitz,Dietrich Seibtment in H., HD and D. near 3.7 eV is shown. The reaction proceeds via the .∑. state of H. (Figure 9.2). There is a very large isotope effect. The peak cross sections are: 1.6 ? 10. cm. for H.; 1.3?10.cm. for HD and 8 ? 10. cm. for D作者: Buttress 時(shí)間: 2025-3-22 05:35 作者: Phenothiazines 時(shí)間: 2025-3-22 12:11
https://doi.org/10.1007/978-3-322-90744-8y a set of quantum numbers. After the collision all momenta, spin projections and other quantum numbers will be changed (in general). Moreover the structure of the target can be changed (e.g., ionization).作者: 貨物 時(shí)間: 2025-3-22 16:12
Contra: Die IT-Sicherheitskriterien der ZSI many respects to begin with a study of a simplified model of the target which can exist in only two states: the normal or ground state and just one excited state. Correspondingly we will speak about the elastic and inelastic scattering channels. Moreover, we will not take spin into account.作者: 貨物 時(shí)間: 2025-3-22 20:38 作者: 殘暴 時(shí)間: 2025-3-22 23:45
The Simplest Two-Channel System, many respects to begin with a study of a simplified model of the target which can exist in only two states: the normal or ground state and just one excited state. Correspondingly we will speak about the elastic and inelastic scattering channels. Moreover, we will not take spin into account.作者: 政府 時(shí)間: 2025-3-23 02:44 作者: Concomitant 時(shí)間: 2025-3-23 07:03
the consistent interpretation of experimental results. The main constituents of the book are: 1. General theory with special emphasis on the topics most impor- tant for understanding and discussing electron collisions with atomic particles.978-1-4612-8997-5978-1-4613-1779-1作者: humectant 時(shí)間: 2025-3-23 11:59
Introduction,ve certain momenta and projection of their spin on some specified fixed direction, and the target is in a certain state of internal motion specified by a set of quantum numbers. After the collision all momenta, spin projections and other quantum numbers will be changed (in general). Moreover the str作者: Endoscope 時(shí)間: 2025-3-23 16:07
Scattering of a Particle by a Potential,ain initial form of it. This initial form corresponds to a particle localized at a given time in the source far from the target. The time evolution of the wave function is governed by the Schr?dinger equation作者: COST 時(shí)間: 2025-3-23 20:02 作者: BET 時(shí)間: 2025-3-23 22:51 作者: AORTA 時(shí)間: 2025-3-24 06:26
Ionization,the ejected) near threshold is low and the energy dependence of the cross section is determined mainly by the motion of the electron far away from the nucleus. In this case the motion of the electrons can be treated using classical mechanics. This was done by Wannier (1953) and later by Vinkaln and 作者: Rebate 時(shí)間: 2025-3-24 06:48
Dissociation of Molecules,of the incident electron exceeds the reaction threshold. Some characteristic features of this process can be demonstrated when the H. molecule is the target. The experimental data were summarized by Schulz (1973). In Figure 9.1 the energy dependence of the total cross section for dissociative attach作者: Inflated 時(shí)間: 2025-3-24 14:11 作者: 臆斷 時(shí)間: 2025-3-24 17:03 作者: FORGO 時(shí)間: 2025-3-24 22:03 作者: Concerto 時(shí)間: 2025-3-24 23:59
Inference Control for relational databasesthe ejected) near threshold is low and the energy dependence of the cross section is determined mainly by the motion of the electron far away from the nucleus. In this case the motion of the electrons can be treated using classical mechanics. This was done by Wannier (1953) and later by Vinkaln and Gailitis (1967).作者: Cardiac-Output 時(shí)間: 2025-3-25 04:52
Pro: Die IT-Sicherheitskriterien der ZSIThe theory considered in the previous chapter did not take into account the spin of the particle. We will discuss now how to incorporate spin in the description of the scattering. Since we will be considering electrons we will suppose that the spin of the scattered particle is equal to 1/2 (in the units of ?).作者: 合群 時(shí)間: 2025-3-25 08:37
Electronic Data Interchange und SicherheitIn this chapter some of the approximate methods for cross section calculations will be considered. We do not intend to consider all existing methods, but only those which are mostly used and can be applied to a variety of particular cases. We will compare the results of calculations by various methods and with the experimental data.作者: Altitude 時(shí)間: 2025-3-25 13:38
Sicherheit in Unix-Netzen (TCP/IP)In this region only elastic scattering is possible. There are a large number of phase shifts and scattering length calculations. One of the most accurate is based on the variational method (Schwartz, 1961) . The wave function of the “electron + atom” system is represented in the form作者: OFF 時(shí)間: 2025-3-25 15:54
Inference Control for relational databasesIn this energy region the excitation of rotation is mainly due. to the long range interaction of the electron with the electric multipole moments of the molecule. This was shown first by Gerjuoy and Stein (1955) who took into account only the quadrupole moment. Later their results were extended by Takayanagi and Itikawa (1970).作者: emission 時(shí)間: 2025-3-25 19:58
Scattering of a Particle with Spin: Polarization Phenomena,The theory considered in the previous chapter did not take into account the spin of the particle. We will discuss now how to incorporate spin in the description of the scattering. Since we will be considering electrons we will suppose that the spin of the scattered particle is equal to 1/2 (in the units of ?).作者: 繁榮中國 時(shí)間: 2025-3-26 01:54
Approximate Methods for Electron-Atom Collisions: Cross Section Calculations,In this chapter some of the approximate methods for cross section calculations will be considered. We do not intend to consider all existing methods, but only those which are mostly used and can be applied to a variety of particular cases. We will compare the results of calculations by various methods and with the experimental data.作者: FANG 時(shí)間: 2025-3-26 05:04
Elastic and Inelastic Scattering of Electrons by Atoms and Positive Ions,In this region only elastic scattering is possible. There are a large number of phase shifts and scattering length calculations. One of the most accurate is based on the variational method (Schwartz, 1961) . The wave function of the “electron + atom” system is represented in the form作者: Vulvodynia 時(shí)間: 2025-3-26 08:36
Rotational and Vibrational Excitation of Molecules,In this energy region the excitation of rotation is mainly due. to the long range interaction of the electron with the electric multipole moments of the molecule. This was shown first by Gerjuoy and Stein (1955) who took into account only the quadrupole moment. Later their results were extended by Takayanagi and Itikawa (1970).作者: 跟隨 時(shí)間: 2025-3-26 13:37 作者: Heart-Attack 時(shí)間: 2025-3-26 19:54
Collisions of Electrons with Atoms and Ions: General Theory,tric with respect to the permutation of any pair r.μ. and r.μ.. Denoting by one quantity x. all variables r.μ. and by P. the permutation operator, we have.The function Φ is an eigenfunction of the Hamiltonian operator H.where H in the nonrelativistic approximation has the form作者: esoteric 時(shí)間: 2025-3-27 00:14
Ionization,the ejected) near threshold is low and the energy dependence of the cross section is determined mainly by the motion of the electron far away from the nucleus. In this case the motion of the electrons can be treated using classical mechanics. This was done by Wannier (1953) and later by Vinkaln and Gailitis (1967).作者: fulcrum 時(shí)間: 2025-3-27 02:45 作者: defray 時(shí)間: 2025-3-27 08:32
978-1-4612-8997-5Plenum Press, New York 1987作者: 品嘗你的人 時(shí)間: 2025-3-27 10:26 作者: 熱情贊揚(yáng) 時(shí)間: 2025-3-27 16:45 作者: micturition 時(shí)間: 2025-3-27 18:13 作者: 品牌 時(shí)間: 2025-3-27 23:09
Pro: Die IT-Sicherheitskriterien der ZSItric with respect to the permutation of any pair r.μ. and r.μ.. Denoting by one quantity x. all variables r.μ. and by P. the permutation operator, we have.The function Φ is an eigenfunction of the Hamiltonian operator H.where H in the nonrelativistic approximation has the form作者: 值得尊敬 時(shí)間: 2025-3-28 04:44
Inference Control for relational databasesthe ejected) near threshold is low and the energy dependence of the cross section is determined mainly by the motion of the electron far away from the nucleus. In this case the motion of the electrons can be treated using classical mechanics. This was done by Wannier (1953) and later by Vinkaln and 作者: 亞麻制品 時(shí)間: 2025-3-28 09:52
Heiko Lippold,Paul Schmitz,Dietrich Seibtof the incident electron exceeds the reaction threshold. Some characteristic features of this process can be demonstrated when the H. molecule is the target. The experimental data were summarized by Schulz (1973). In Figure 9.1 the energy dependence of the total cross section for dissociative attach作者: debris 時(shí)間: 2025-3-28 14:24
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