Atomic Lithium Excitation by Electron Impact

Rabab M. Abdul Hassan, A. Khalaf
{"title":"Atomic Lithium Excitation by Electron Impact","authors":"Rabab M. Abdul Hassan, A. Khalaf","doi":"10.31257/2018/jkp/2019/110205","DOIUrl":null,"url":null,"abstract":"Article history: Received:14 JUN, 2019 Accepted: 25 AUG, 2019 Available Online: 25 DEC, 2019 Bethe approximation had been used to compute the excitation cross section in term of the diploe oscillator strength for some allowed transitions between energy levels of Li-atom collide with electrons with impact energy range (2-2000) eV. We also compute the radiation transition probability and lifetime. Our results for all calculations we had done were compared with the available theoretical and experimental data. DOI: http://dx.doi.org/10.31257/2018/JKP/2019/110205 K e y w o r d s : Excitation Cross section Lithium atom Electron impact Bethe approximation نورتكللاا ريثأتب مويثيللا ةرذ ةراثا فلخ نسحلا دبع ءلاع نسحلا دبع ىفطصم بابر ءايسيفلا نسق مىلعلا تيلك ةرصبلا تعهاج :تيحاخفولا ثاولكلا لا ــــ خ ـــ صلا ـــ ت ةراثأ يضرع عطقه مىيثيللا ةرذ ىورخكللإا ريثأح ثيب بيرقح بميرقح مامخخمتا نمح Bethe يم ةرامثرل يمضرعلا عمطقولا امسحل ممح بمببه ةىمق ييامٌث بطقلا لاا ضعبل ثلااقخً يمه تمقاطلا ثايىخسه ييب اهب حىوسولا ممٌع مىميثيللا ةرذ همامصح اه عمه ريثأممخلا تممقا يمممه ثاذ ثاممًورخكللإا (2-2000) eV. و لاوخحا امم يأ بممسحً تممي لاا اممقخً عاعمشلإا ي و امقخًلاا يمهز ثامًايبلا عمه امااٌيرجأ يمخلا ثابامسحلا عميولل امٌلياخً تمًراقه جموح . تحاخولا تيبيرلخلاو تيرظٌلا . JOURNAL OF KUFA–PHYSICS | Vol. 11, No. 2 (2019) Rabab M. Abdul Hassan, Alaa A. Khalaf 30 oscillator strength for these lines done by Fock and Petrashen [2], where they used in their treatment the wave functions of self-consistent field. Also the excitation cross section is performed by Williams et. al [3], where they calculate the excitation cross section at a limited number of electron impact energies. In the experimental side, Leep and Gallagher [4], Zajonc and Gallagher [5] were measured the excitation cross section for 2s-state to 2p-state for neutral lithium collide with electrons. The importance of studying inelastic scattering is coming from that the need is increasing for reliable and accurate computational cross section data in many fields like astrophysics, physics of radiation, and plasma physics [6]. In the inelastic interactions of neutral atoms -in ground and excited stateswith electrons, the information of cross sections are very important and has fundamental interest. A database of theoretical cross sections for inelastic collision of lithium atoms with electrons in the ground and excited states have been proposed by Schwinzer et. al [7]. To derive accurate cross sections for all inelastic excitation processes for lithium atoms colliding with single electrons they used sophisticated theoretical methods of calculations. The results of these methods were tested critically against the available newest experimental measurements data. The computation of atomic transition probabilities for allowed electric dipole lines of Li-atom, were performed by Wiese et. al [8]. The critical data compilations were included transitions between ground state and some excited states and between excited states itself. The wave functions of Hartree-Fock for 2s, 2p, 3s, 3p, and 3d states of Li-atom were computed by a wide-range method. The followed procedure represented by depend the method of analytic self-consistent field. Oscillator strengths for some transitions between these states were calculated using the dipole length formula. In this paper, Bethe approximation which play as a correct for the behavior of the Born approximation at high energies was used to calculate the excitation cross section for the scattering of electrons from lithium atom. The generated cross section is based on the calculated oscillator strength which in turn was produced from the given Hartree-Fock wave functions. Also we calculate the transition probability and lifetime between the states under investigation. Our results for all the preceding calculations were compared with available theoretical and measurements data, and in general the comparison was good 2. THEORY In the excitation process for atoms by fast electrons from its initial (i) state to final (f) or excited state. The integral cross section which performed using Born approximation where the generalized oscillator strength (GOS) plays a crucial role [9-10], can be expressed as:","PeriodicalId":16215,"journal":{"name":"Journal of Kufa - Physics","volume":"48 1","pages":"29-33"},"PeriodicalIF":0.0000,"publicationDate":"2019-12-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Kufa - Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.31257/2018/jkp/2019/110205","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
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Abstract

Article history: Received:14 JUN, 2019 Accepted: 25 AUG, 2019 Available Online: 25 DEC, 2019 Bethe approximation had been used to compute the excitation cross section in term of the diploe oscillator strength for some allowed transitions between energy levels of Li-atom collide with electrons with impact energy range (2-2000) eV. We also compute the radiation transition probability and lifetime. Our results for all calculations we had done were compared with the available theoretical and experimental data. DOI: http://dx.doi.org/10.31257/2018/JKP/2019/110205 K e y w o r d s : Excitation Cross section Lithium atom Electron impact Bethe approximation نورتكللاا ريثأتب مويثيللا ةرذ ةراثا فلخ نسحلا دبع ءلاع نسحلا دبع ىفطصم بابر ءايسيفلا نسق مىلعلا تيلك ةرصبلا تعهاج :تيحاخفولا ثاولكلا لا ــــ خ ـــ صلا ـــ ت ةراثأ يضرع عطقه مىيثيللا ةرذ ىورخكللإا ريثأح ثيب بيرقح بميرقح مامخخمتا نمح Bethe يم ةرامثرل يمضرعلا عمطقولا امسحل ممح بمببه ةىمق ييامٌث بطقلا لاا ضعبل ثلااقخً يمه تمقاطلا ثايىخسه ييب اهب حىوسولا ممٌع مىميثيللا ةرذ همامصح اه عمه ريثأممخلا تممقا يمممه ثاذ ثاممًورخكللإا (2-2000) eV. و لاوخحا امم يأ بممسحً تممي لاا اممقخً عاعمشلإا ي و امقخًلاا يمهز ثامًايبلا عمه امااٌيرجأ يمخلا ثابامسحلا عميولل امٌلياخً تمًراقه جموح . تحاخولا تيبيرلخلاو تيرظٌلا . JOURNAL OF KUFA–PHYSICS | Vol. 11, No. 2 (2019) Rabab M. Abdul Hassan, Alaa A. Khalaf 30 oscillator strength for these lines done by Fock and Petrashen [2], where they used in their treatment the wave functions of self-consistent field. Also the excitation cross section is performed by Williams et. al [3], where they calculate the excitation cross section at a limited number of electron impact energies. In the experimental side, Leep and Gallagher [4], Zajonc and Gallagher [5] were measured the excitation cross section for 2s-state to 2p-state for neutral lithium collide with electrons. The importance of studying inelastic scattering is coming from that the need is increasing for reliable and accurate computational cross section data in many fields like astrophysics, physics of radiation, and plasma physics [6]. In the inelastic interactions of neutral atoms -in ground and excited stateswith electrons, the information of cross sections are very important and has fundamental interest. A database of theoretical cross sections for inelastic collision of lithium atoms with electrons in the ground and excited states have been proposed by Schwinzer et. al [7]. To derive accurate cross sections for all inelastic excitation processes for lithium atoms colliding with single electrons they used sophisticated theoretical methods of calculations. The results of these methods were tested critically against the available newest experimental measurements data. The computation of atomic transition probabilities for allowed electric dipole lines of Li-atom, were performed by Wiese et. al [8]. The critical data compilations were included transitions between ground state and some excited states and between excited states itself. The wave functions of Hartree-Fock for 2s, 2p, 3s, 3p, and 3d states of Li-atom were computed by a wide-range method. The followed procedure represented by depend the method of analytic self-consistent field. Oscillator strengths for some transitions between these states were calculated using the dipole length formula. In this paper, Bethe approximation which play as a correct for the behavior of the Born approximation at high energies was used to calculate the excitation cross section for the scattering of electrons from lithium atom. The generated cross section is based on the calculated oscillator strength which in turn was produced from the given Hartree-Fock wave functions. Also we calculate the transition probability and lifetime between the states under investigation. Our results for all the preceding calculations were compared with available theoretical and measurements data, and in general the comparison was good 2. THEORY In the excitation process for atoms by fast electrons from its initial (i) state to final (f) or excited state. The integral cross section which performed using Born approximation where the generalized oscillator strength (GOS) plays a crucial role [9-10], can be expressed as:
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电子冲击激发原子锂
历史:收到:2019年6月14日:25 AUG, 2019 Available Online: 12月25日我们还计算辐射概率和寿命。我们所考虑的所有计算结果都与可能的理论和数据实验相匹配。DOI: http://dx.dodisExcitation十字区锂原子电子冲击成为类似نورتكللااريثأتبمويثيللاةرذةراثافلخنسحلادبعءلاعنسحلادبعىفطصمبابرءايسيفلانسقمىلعلاتيلكةرصبلاتعهاج:تيحاخفولاثاولكلالاــــخـــصلاـــتةراثأيضرععطقهمىيثيللاةرذىورخكللإاريثأحثيببيرقحبميرقحمامخخمتانمح成为يمةرامثرليمضرعلاعمطقولاامسحلممحبمببهةىمقييامٌثبطقلالااضعبلثلااقخًيمهتمقاطلاثايىخسهييباهبحىوسولاممٌعمىميثيللاةرذهمامصحاهعمهريثأممخلاتممقايمممهثاذثاممًورخكللإا(2-2000) eV。ولاوخحاامميأبممسحًتمميلاااممقخًعاعمشلإايوامقخًلاايمهزثامًايبلاعمهامااٌيرجأيمخلاثابامسحلاعميوللامٌلياخًتمًراقهجموح。تحاخولاتيبيرلخلاوتيرظٌلا。KUFA——物理杂志》| Vol . 11、2号(2019年)公元Rabab阿卜杜勒·哈桑,Alaa A。哈拉夫30振荡器为这些线条完成由福克和拼搏,Petrashen[2],他们以前在哪里他们的治疗之浪潮functions self-consistent陆军。此外,威廉姆斯和海军展示的十字部分也是他们在一场有限的电电影响区calculate交叉曝光部分的地方。《实验,一边听加拉赫[4],Zajonc和加拉赫[5]是measured《excitation十字区2s-state来说2p-state为中立和electrons锂相碰。studying之重要性inelastic scattering来是来自那可靠和准确的需要是increasing computational交叉在很多领域像天体物理学数据区,辐射的物理、等离子体物理[6]。在内生原子和与电子兴奋的相互作用下,交叉部分的信息是非常重要的,具有基本的兴趣。A theoretical cross sections for inelastic相撞事件的数据库的锂原子electrons》地面和兴奋各州已被proposed by Schwinzer et al[7]。对于提出计算的计算方法,均为锂离子原子与单电子并列的所有相关扩展方案。这些方法的结果被严重驳斥了我们最新的可用数据实验。原子转换概率允许融合电缆线,由Wiese et. al表演。critical数据包括地表州和州兴奋州之间的转换。hartref - fock的小规模功能为2s, 2p, 3s, 3p和3d国家的Li-atom被一种大规模的方法计算出来。分析自我凝聚场的方法。用上紧的公式计算出这两种州之间的转换强度。在这篇论文中生成的交叉部分是建立在钙化骨制定器上的。我们还考虑了美国调查期间发生的概率和寿命的转变。我们所建议的所有先验的计算都是可替代的和可替代的数据,一般来说是好的。存在于处理原子的过程中,从初始状态到最终状态(f)或excited状态。用普通的骨镜用力(戈斯)演奏一种粗面包卷[9-10],可以表示:
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