{"title":"用OXBASH代码应用核壳模型研究18Ne的核结构","authors":"Hadeel H. Abed, A. K. Hasan","doi":"10.31257/2018/jkp/2019/110201","DOIUrl":null,"url":null,"abstract":"Article history: Received: 20 MAR., 2019 Accepted: 10 GUN, 2019 Available Online: 24 DEC, 2019 In this study, the shell model used to calculate energy levels and reduced electric quadruple transition probability B(E2) for 18 Ne isotope using OXBASH code within the sd shell and using the KUOSD effective interaction. 18 Ne isotope contain two proton outside 16 O core in shell (0d5/2, 1s1/2, and 0d3/2) .The results of the energy levels and values of B(E2) were reasonably consistent with the experimental data available. DOI: http://dx.doi.org/10.31257/2018/JKP/2019/110201 K e y w o r d s : OXBASH Code Ne isotope Energy Levels B(E2) ـل يوونلا بيكرتلا تساردل يوونلا ةرشقلا جذومنأ قيبطت 18 Ne شابسكوأ دوك لامعتساب نسح فلخ يلع دبع مكاح ليده ءاٌزٍفلا مسق ,خاىثلل حٍتزرلا حٍلك , حفوكلا حعماج :حٍحارفملا خاملكلا لا ــــ خ ـــ صلا ـــ ح شاثسكوا دوك زٍظو 18 Ne , حقاطلا خاٌورسم ً اةةةةةةةتز كلا اةةةةةةةهرواا حةةةةةةةٍلامرحا حلزرخملا ً اةتز كلا ةةطهلا ًااةتزل اةهرواا حةٍلامرحاو حقاطلا خاٌورسم باسح مذ حسارذلا يذه ًف حةلزرخملا B(E2) زةٍظىل 18 Ne دوةك امعرةسات OXBASH جزةرهلا همةض sd امعرةساو اعفلا لاافرلا KUOSD زٍظو نأ ثٍح 18 Ne ةةلهلا راةخ هٍووذوزت ىلا يورحٌ 16 O ) جزةرهلا ًةف 0 d5/2, 1s1/2, and 0d3/2 ) اةهرواا حةٍلامرحاو حةقاطلا خاٌورةسم مٍةق دةواك . B(E2) جزفورملا حٍلمعلا مٍهلا عم وهعم لكرت قفرذ . JOURNAL OF KUFA–PHYSICS | Vol. 11, No. 2 December (2019) Hadeel H. Abed, Ali k. Hasan 2 nucleus. Shell model is one of the most prominent and successful nuclear models[1]. One of the central challenges in nuclear physics understanding on the nuclear structure is choosing the correct effective interaction and model space that can lead to predicting a wide range of observation from the nuclear shell model systematically and correctly[2]. The nuclear shell model is one of the most powerful tools to give a quantitative interpretation of the empirical data. The two central ingredients of any calculation of the shell model are the N-N interaction and configuration space for valence particles. In principle, one can implement calculations of shell models with realistic N-N interaction in an indefinite configuration space or with effective renormalized interaction restricted configuration space[3]. The calculations of the shell model are made within a model space in which the nucleons are limited to a few orbits, when effective operators are used, taking into account the effect of the larger model space. This model offers a significant description of this issue [4]. Thus, the study of nuclei in the sd shell leads to a better understanding among the macroscopic (collective) description and the microscopic description of the core (shell model)[5]. In the current work, we focus a specific attention on the calculation of energy levels and the probability of transition within the shell model for 18 Ne isotope which has configurations of (0d5/2,1s1/2,0d3/2).","PeriodicalId":16215,"journal":{"name":"Journal of Kufa - Physics","volume":"105 1","pages":"1-5"},"PeriodicalIF":0.0000,"publicationDate":"2019-12-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Applying Nuclear Shell Model to Study Nuclear Structure for 18Ne by Using OXBASH Code\",\"authors\":\"Hadeel H. Abed, A. K. Hasan\",\"doi\":\"10.31257/2018/jkp/2019/110201\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Article history: Received: 20 MAR., 2019 Accepted: 10 GUN, 2019 Available Online: 24 DEC, 2019 In this study, the shell model used to calculate energy levels and reduced electric quadruple transition probability B(E2) for 18 Ne isotope using OXBASH code within the sd shell and using the KUOSD effective interaction. 18 Ne isotope contain two proton outside 16 O core in shell (0d5/2, 1s1/2, and 0d3/2) .The results of the energy levels and values of B(E2) were reasonably consistent with the experimental data available. DOI: http://dx.doi.org/10.31257/2018/JKP/2019/110201 K e y w o r d s : OXBASH Code Ne isotope Energy Levels B(E2) ـل يوونلا بيكرتلا تساردل يوونلا ةرشقلا جذومنأ قيبطت 18 Ne شابسكوأ دوك لامعتساب نسح فلخ يلع دبع مكاح ليده ءاٌزٍفلا مسق ,خاىثلل حٍتزرلا حٍلك , حفوكلا حعماج :حٍحارفملا خاملكلا لا ــــ خ ـــ صلا ـــ ح شاثسكوا دوك زٍظو 18 Ne , حقاطلا خاٌورسم ً اةةةةةةةتز كلا اةةةةةةةهرواا حةةةةةةةٍلامرحا حلزرخملا ً اةتز كلا ةةطهلا ًااةتزل اةهرواا حةٍلامرحاو حقاطلا خاٌورسم باسح مذ حسارذلا يذه ًف حةلزرخملا B(E2) زةٍظىل 18 Ne دوةك امعرةسات OXBASH جزةرهلا همةض sd امعرةساو اعفلا لاافرلا KUOSD زٍظو نأ ثٍح 18 Ne ةةلهلا راةخ هٍووذوزت ىلا يورحٌ 16 O ) جزةرهلا ًةف 0 d5/2, 1s1/2, and 0d3/2 ) اةهرواا حةٍلامرحاو حةقاطلا خاٌورةسم مٍةق دةواك . B(E2) جزفورملا حٍلمعلا مٍهلا عم وهعم لكرت قفرذ . JOURNAL OF KUFA–PHYSICS | Vol. 11, No. 2 December (2019) Hadeel H. Abed, Ali k. Hasan 2 nucleus. Shell model is one of the most prominent and successful nuclear models[1]. One of the central challenges in nuclear physics understanding on the nuclear structure is choosing the correct effective interaction and model space that can lead to predicting a wide range of observation from the nuclear shell model systematically and correctly[2]. The nuclear shell model is one of the most powerful tools to give a quantitative interpretation of the empirical data. The two central ingredients of any calculation of the shell model are the N-N interaction and configuration space for valence particles. In principle, one can implement calculations of shell models with realistic N-N interaction in an indefinite configuration space or with effective renormalized interaction restricted configuration space[3]. The calculations of the shell model are made within a model space in which the nucleons are limited to a few orbits, when effective operators are used, taking into account the effect of the larger model space. This model offers a significant description of this issue [4]. Thus, the study of nuclei in the sd shell leads to a better understanding among the macroscopic (collective) description and the microscopic description of the core (shell model)[5]. In the current work, we focus a specific attention on the calculation of energy levels and the probability of transition within the shell model for 18 Ne isotope which has configurations of (0d5/2,1s1/2,0d3/2).\",\"PeriodicalId\":16215,\"journal\":{\"name\":\"Journal of Kufa - Physics\",\"volume\":\"105 1\",\"pages\":\"1-5\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-12-24\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Kufa - Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.31257/2018/jkp/2019/110201\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Kufa - Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.31257/2018/jkp/2019/110201","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
摘要
历史:收到:2019年接受:10支枪,2019年可以在网上使用:24年12月,2019年的研究,外壳模型用于在sd壳中消耗能量和减少温室效应代码B(E2) 18年的异位应用18 Ne isotope contain 2个质子在壳内存在16个O核(0d5 2、1/2和0d3/2)。DOI: http://dx.dodisOXBASH代码Ne同位素能源水平B (E2)ـليوونلابيكرتلاتساردليوونلاةرشقلاجذومنأقيبط18 Neشتابسكوأدوكلامعتسابنسحفلخيلعدبعمكاحليدهءاٌزٍفلامسق,خاىثللحٍتزرلاحٍلح,كفوكلاحعماج:حٍحارفملاخاملكلالاــــخـــصلاـــحشاثسكوادوكزٍظو18 Ne,حقاطلاخاٌورسمًاةةةةةةةتزكلااةةةةةةةهروااحةةةةةةةٍلامرحاحلزرخملاًاةتزكلاةةطهلاًااةتزلاةهروااحةٍلامرحاوحقاطلاخاٌورسمباسحمذحسارذلايذهًفحةلزرخملB (E2)زاةٍظى18 NeدلوةكامعرةساتOXBASHجزةرهلاهمة小学ضامعرةساواعفلالاافرلاKUOSDزٍظونأثٍ18 Neةحةلهلاراةخهٍووذوزتىلايورحٌ16 O)جزةرهلاًةف0 d5/2、1s1/2 0d3/2)اةهروااحةٍلامرحاوحةقاطلاخاٌورةسممٍةقدةواك。B (E2)جزفورملاحٍلمعلامٍهلاعموهعملكرتقفرذ。KUFA——物理杂志》|卷。11、12月2号(2019)Hadeel H . k Abed,阿里哈桑两个原子核。壳牌模型是最成功的核模型之一[1]。核物理上的一个中心挑战是对核结构的精确影响和空间模型的选择,这些影响可能导致对核外壳系统和正确度的广泛观察[2]。核外壳模型是最强大的工具之一,可以对经验数据进行定量解读。这两个中心的内核,外壳的任何计算都是N-N相互作用和形成空间对于valence particles。在原理上,一个人可以实现外壳模型的现实与相互作用的空间或有效的相互作用限制空间[3]。外壳模型的计算结果是在核限制很少使用的空间中进行的,当有效操作被使用时,对大质量空间的影响进行了记录。这个模型对这个问题有很大的解释[4]。因此,在sd的核心研究导致更好地理解macroscopic和微scopic对核心的描述[5]。在目前的工作中,我们特别关注能量水平的计算和外壳模型18 Ne同位素的转换的可能性,这些变量有其相似性(0d5/2,1s1/2,0d3 - 2)。
Applying Nuclear Shell Model to Study Nuclear Structure for 18Ne by Using OXBASH Code
Article history: Received: 20 MAR., 2019 Accepted: 10 GUN, 2019 Available Online: 24 DEC, 2019 In this study, the shell model used to calculate energy levels and reduced electric quadruple transition probability B(E2) for 18 Ne isotope using OXBASH code within the sd shell and using the KUOSD effective interaction. 18 Ne isotope contain two proton outside 16 O core in shell (0d5/2, 1s1/2, and 0d3/2) .The results of the energy levels and values of B(E2) were reasonably consistent with the experimental data available. DOI: http://dx.doi.org/10.31257/2018/JKP/2019/110201 K e y w o r d s : OXBASH Code Ne isotope Energy Levels B(E2) ـل يوونلا بيكرتلا تساردل يوونلا ةرشقلا جذومنأ قيبطت 18 Ne شابسكوأ دوك لامعتساب نسح فلخ يلع دبع مكاح ليده ءاٌزٍفلا مسق ,خاىثلل حٍتزرلا حٍلك , حفوكلا حعماج :حٍحارفملا خاملكلا لا ــــ خ ـــ صلا ـــ ح شاثسكوا دوك زٍظو 18 Ne , حقاطلا خاٌورسم ً اةةةةةةةتز كلا اةةةةةةةهرواا حةةةةةةةٍلامرحا حلزرخملا ً اةتز كلا ةةطهلا ًااةتزل اةهرواا حةٍلامرحاو حقاطلا خاٌورسم باسح مذ حسارذلا يذه ًف حةلزرخملا B(E2) زةٍظىل 18 Ne دوةك امعرةسات OXBASH جزةرهلا همةض sd امعرةساو اعفلا لاافرلا KUOSD زٍظو نأ ثٍح 18 Ne ةةلهلا راةخ هٍووذوزت ىلا يورحٌ 16 O ) جزةرهلا ًةف 0 d5/2, 1s1/2, and 0d3/2 ) اةهرواا حةٍلامرحاو حةقاطلا خاٌورةسم مٍةق دةواك . B(E2) جزفورملا حٍلمعلا مٍهلا عم وهعم لكرت قفرذ . JOURNAL OF KUFA–PHYSICS | Vol. 11, No. 2 December (2019) Hadeel H. Abed, Ali k. Hasan 2 nucleus. Shell model is one of the most prominent and successful nuclear models[1]. One of the central challenges in nuclear physics understanding on the nuclear structure is choosing the correct effective interaction and model space that can lead to predicting a wide range of observation from the nuclear shell model systematically and correctly[2]. The nuclear shell model is one of the most powerful tools to give a quantitative interpretation of the empirical data. The two central ingredients of any calculation of the shell model are the N-N interaction and configuration space for valence particles. In principle, one can implement calculations of shell models with realistic N-N interaction in an indefinite configuration space or with effective renormalized interaction restricted configuration space[3]. The calculations of the shell model are made within a model space in which the nucleons are limited to a few orbits, when effective operators are used, taking into account the effect of the larger model space. This model offers a significant description of this issue [4]. Thus, the study of nuclei in the sd shell leads to a better understanding among the macroscopic (collective) description and the microscopic description of the core (shell model)[5]. In the current work, we focus a specific attention on the calculation of energy levels and the probability of transition within the shell model for 18 Ne isotope which has configurations of (0d5/2,1s1/2,0d3/2).