標(biāo)題: Titlebook: Computation of Atomic and Molecular Processes; Introducing the ATOM Miron Ya. Amusia,Larissa V. Chernysheva Book 2021 The Editor(s) (if app [打印本頁(yè)] 作者: affront 時(shí)間: 2025-3-21 19:28
書(shū)目名稱Computation of Atomic and Molecular Processes影響因子(影響力)
書(shū)目名稱Computation of Atomic and Molecular Processes影響因子(影響力)學(xué)科排名
書(shū)目名稱Computation of Atomic and Molecular Processes網(wǎng)絡(luò)公開(kāi)度
書(shū)目名稱Computation of Atomic and Molecular Processes網(wǎng)絡(luò)公開(kāi)度學(xué)科排名
書(shū)目名稱Computation of Atomic and Molecular Processes被引頻次
書(shū)目名稱Computation of Atomic and Molecular Processes被引頻次學(xué)科排名
書(shū)目名稱Computation of Atomic and Molecular Processes年度引用
書(shū)目名稱Computation of Atomic and Molecular Processes年度引用學(xué)科排名
書(shū)目名稱Computation of Atomic and Molecular Processes讀者反饋
書(shū)目名稱Computation of Atomic and Molecular Processes讀者反饋學(xué)科排名
作者: BOAST 時(shí)間: 2025-3-21 23:35 作者: 粗魯性質(zhì) 時(shí)間: 2025-3-22 02:59 作者: 直覺(jué)好 時(shí)間: 2025-3-22 08:00 作者: 討好女人 時(shí)間: 2025-3-22 12:34
Phenomenology of Neutrino Oscillationsle. This chapter describes how to calculate GOS for electrons in the one-particle Hartree–Fock and RPAE approximations that account for the interaction of various transitions. RPAE equations are presented for the matrix elements of GOS, which are solved by methods similar to those described in Chap.作者: enfeeble 時(shí)間: 2025-3-22 13:44 作者: enfeeble 時(shí)間: 2025-3-22 20:30
Jan de Boer,Asad Naqvi,Assaf Shomerarameters for secondary electrons in the scattering of fast particles for intermediate values of the momentum . transferred from the projectile to the target atom. For small values of ., the same parameters are calculated in the programs described in Chap. ..作者: incisive 時(shí)間: 2025-3-22 22:01
String Topology and Cyclic Homologyparticle in elastic scattering, as well as the shift in the energy of the atomic electron caused by correlation effects. Formulas for calculating the phase shifts of inelastic scattering are presented.作者: 東西 時(shí)間: 2025-3-23 03:17 作者: Foreshadow 時(shí)間: 2025-3-23 09:13
String Topology and Cyclic Homologyo account the dynamic polarization of the target atom by the incident particle in the collision process. Formulas are given for calculating the form factor, bremsstrahlung cross section, and matrix elements included in these expressions.作者: exceptional 時(shí)間: 2025-3-23 13:32 作者: 錯(cuò) 時(shí)間: 2025-3-23 17:57 作者: optional 時(shí)間: 2025-3-23 19:08 作者: nettle 時(shí)間: 2025-3-23 23:21
978-3-030-85145-3The Editor(s) (if applicable) and The Author(s), under exclusive license to Springer Nature Switzerl作者: 仲裁者 時(shí)間: 2025-3-24 06:17
Lucas Robidou,Pierre PeterlongoThis chapter describes the main programs of the ATOM-M system. Each program corresponds to an independent physical problem related to the study of the structure of atoms and the calculation of the probabilities of atomic processes. The choice of approach is described for each investigated problem.作者: atrophy 時(shí)間: 2025-3-24 07:21 作者: Intrepid 時(shí)間: 2025-3-24 12:57 作者: OTTER 時(shí)間: 2025-3-24 17:02 作者: Pageant 時(shí)間: 2025-3-24 19:10 作者: mighty 時(shí)間: 2025-3-25 02:49 作者: 軌道 時(shí)間: 2025-3-25 05:20 作者: FECT 時(shí)間: 2025-3-25 09:35 作者: 秘方藥 時(shí)間: 2025-3-25 15:40 作者: Jingoism 時(shí)間: 2025-3-25 17:39 作者: 石墨 時(shí)間: 2025-3-25 23:32
Choice of Wave Functions,Each specific physical problem requires the choice of the initial basis of wave functions for its consideration. Obtaining the characteristics of a physical process requires knowledge of the wave functions in the ground and excited states.作者: oracle 時(shí)間: 2025-3-26 00:47 作者: 溫和女孩 時(shí)間: 2025-3-26 06:25 作者: Ardent 時(shí)間: 2025-3-26 11:25 作者: 谷物 時(shí)間: 2025-3-26 12:41 作者: 和平主義者 時(shí)間: 2025-3-26 20:28 作者: SSRIS 時(shí)間: 2025-3-26 23:20 作者: Fabric 時(shí)間: 2025-3-27 02:16 作者: 協(xié)議 時(shí)間: 2025-3-27 06:28
Angular Distribution of Photoelectrons and Secondary Electrons Outside the Dipole Approximation,c scattering of fast electrons. Their general and specific features are investigated, demonstrating a significant difference in the corresponding characteristics of the two processes under consideration, namely photoionization and fast electron scattering.作者: 兵團(tuán) 時(shí)間: 2025-3-27 10:32
Angular Distribution of Secondary Electrons Arising from the Scattering of Fast Particles by Atoms,arameters for secondary electrons in the scattering of fast particles for intermediate values of the momentum . transferred from the projectile to the target atom. For small values of ., the same parameters are calculated in the programs described in Chap. ..作者: 違抗 時(shí)間: 2025-3-27 15:24
Scattering of Particles of Low and Medium Energies by Atoms,particle in elastic scattering, as well as the shift in the energy of the atomic electron caused by correlation effects. Formulas for calculating the phase shifts of inelastic scattering are presented.作者: 運(yùn)動(dòng)吧 時(shí)間: 2025-3-27 19:42 作者: legacy 時(shí)間: 2025-3-27 22:53
Bremsstrahlung Spectra in High and Intermediate Energy Collisions,o account the dynamic polarization of the target atom by the incident particle in the collision process. Formulas are given for calculating the form factor, bremsstrahlung cross section, and matrix elements included in these expressions.作者: 到婚嫁年齡 時(shí)間: 2025-3-28 05:17
Photoabsorption Cross Section with Account for Inelastic Photoelectron Scattering, with the residual ion, thus changing its own energy, angular momentum, and spin projection. Formulas are given for calculating the photoabsorption dipole matrix elements and the photoionization cross section taking this effect into account.作者: Initial 時(shí)間: 2025-3-28 06:52
Computation of Atomic and Molecular Processes978-3-030-85143-9Series ISSN 1615-5653 Series E-ISSN 2197-6791 作者: 寬大 時(shí)間: 2025-3-28 12:35 作者: Fortuitous 時(shí)間: 2025-3-28 14:39
https://doi.org/10.1007/978-3-540-74233-3 to solve these equations is determined by the fact that many of the processes under consideration are nonrelativistic, while the solution of relativistic equations for many calculations related to intermediate and outer atomic shells is much more complicated and, in fact, is not necessary, although it gives high accuracy.作者: Keratectomy 時(shí)間: 2025-3-28 21:40
Maurizio Gasperini,Jnan Maharanases the simplest approach to calculating one-particle wave functions in discrete and continuous spectra. In this case, as a rule, the so-called frozen core approximation is used, in which it is assumed that the excitation of one electron does not affect the wave functions of the rest.作者: HAWK 時(shí)間: 2025-3-29 01:17
The ,(1), Anomaly and QCD Phenomenologyited states. This chapter proposes the simplest approach to calculating one-particle wave functions in discrete and continuous spectra. In this case, as a rule, the frozen core approximation is used, in which it is assumed that the excitation of one electron does not affect the others.作者: Immortal 時(shí)間: 2025-3-29 05:20
https://doi.org/10.1007/1-4020-3733-3c scattering of fast electrons. Their general and specific features are investigated, demonstrating a significant difference in the corresponding characteristics of the two processes under consideration, namely photoionization and fast electron scattering.作者: 運(yùn)氣 時(shí)間: 2025-3-29 07:21 作者: Obstruction 時(shí)間: 2025-3-29 12:28 作者: evince 時(shí)間: 2025-3-29 19:16
https://doi.org/10.1007/3-7643-7388-1rections in this process in the framework of RPAE and perturbation theory. A method is presented to calculate the probability of double Auger decay, i.e., a process in which two vacancies decay with the transfer of their energy to one escaping electron. Formulas are given for the amplitude of the process and the Coulomb matrix elements.作者: Cardiac 時(shí)間: 2025-3-29 23:16
String Topology and Cyclic Homologyo account the dynamic polarization of the target atom by the incident particle in the collision process. Formulas are given for calculating the form factor, bremsstrahlung cross section, and matrix elements included in these expressions.作者: 平躺 時(shí)間: 2025-3-30 00:47 作者: 吞吞吐吐 時(shí)間: 2025-3-30 07:23
Miron Ya. Amusia,Larissa V. ChernyshevaPresents and makes available an entire Fortran software suite for calculating almost any atomic process.Teaches the reader how to build atomic and molecular systems from the ground up using the code p作者: 散開(kāi) 時(shí)間: 2025-3-30 09:32 作者: 討好女人 時(shí)間: 2025-3-30 16:13
Short Review,cules, fullerenes, and endohedrals are discussed, definitions of concepts that are used throughout the book are given, and a diagrammatic description of all the processes under consideration is presented.作者: Atheroma 時(shí)間: 2025-3-30 20:11
,Wave Functions of the Ground State of Atoms and Simple Molecules in the Hartree–Fock Approximation, to solve these equations is determined by the fact that many of the processes under consideration are nonrelativistic, while the solution of relativistic equations for many calculations related to intermediate and outer atomic shells is much more complicated and, in fact, is not necessary, although作者: Morsel 時(shí)間: 2025-3-31 00:26
,Wave Functions of Excited States of Atoms and Simple Molecules in the Hartree–Fock Approximation,ses the simplest approach to calculating one-particle wave functions in discrete and continuous spectra. In this case, as a rule, the so-called frozen core approximation is used, in which it is assumed that the excitation of one electron does not affect the wave functions of the rest.作者: Implicit 時(shí)間: 2025-3-31 01:08
,Wave Functions of an Excited State of an Atom in the Hartree–Fock–Dirac Approximation,ited states. This chapter proposes the simplest approach to calculating one-particle wave functions in discrete and continuous spectra. In this case, as a rule, the frozen core approximation is used, in which it is assumed that the excitation of one electron does not affect the others.作者: 適宜 時(shí)間: 2025-3-31 07:40
Scattering Cross Section of Fast Electrons, Generalized Oscillator Strengths, and the Compton Effecle. This chapter describes how to calculate GOS for electrons in the one-particle Hartree–Fock and RPAE approximations that account for the interaction of various transitions. RPAE equations are presented for the matrix elements of GOS, which are solved by methods similar to those described in Chap.作者: Formidable 時(shí)間: 2025-3-31 11:03 作者: 可以任性 時(shí)間: 2025-3-31 15:35 作者: Abrade 時(shí)間: 2025-3-31 18:58 作者: 個(gè)阿姨勾引你 時(shí)間: 2025-3-31 21:59
Non-radiative or Auger Vacancy Decay,rections in this process in the framework of RPAE and perturbation theory. A method is presented to calculate the probability of double Auger decay, i.e., a process in which two vacancies decay with the transfer of their energy to one escaping electron. Formulas are given for the amplitude of the pr作者: Ptosis 時(shí)間: 2025-4-1 05:53
Bremsstrahlung Spectra in High and Intermediate Energy Collisions,o account the dynamic polarization of the target atom by the incident particle in the collision process. Formulas are given for calculating the form factor, bremsstrahlung cross section, and matrix elements included in these expressions.作者: Corroborate 時(shí)間: 2025-4-1 06:44 作者: 值得 時(shí)間: 2025-4-1 11:16
Ionization and Excitation of an Atom by Electron Impact,elastically scattered electron, one can calculate the cross section for ionization and excitation of an atom by electron impact in the Born approximation with plane and distorted waves. In the latter case, the effect of the atomic field is accounted for within the Hartree–Fock approximation. It is s
