Nuclear Electric quadrapole moments Q in 58Ni for some selected levels have been investigated and calculated through Nuclear shell model and considering of 56Ni as an inert core with two active neutrons in a model space (2p3/2, 1f5/2 and 2p1/2) and the configuration mixing of the original states is also done. F5Pvh interaction has been utilized as a two body interaction to generate model space vectors with harmonic oscillator potential as a single particle wave function. OXBASH code is used to carry this calculations and the program of Core, Valence, Tassie (CVT) written in FORTRAN go language to calculate the Electric quadrapole moments between excited states themselves. All of these calculations have been carried through model space vectors only. One body density matrix elements (OBDM) for ground and Excited states is calculated in order to carry the calculations using single particle Transition matrix elements between excited states theme selves.
Published in | American Journal of Physics and Applications (Volume 6, Issue 4) |
DOI | 10.11648/j.ajpa.20180604.11 |
Page(s) | 80-84 |
Creative Commons |
This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited. |
Copyright |
Copyright © The Author(s), 2018. Published by Science Publishing Group |
Shell Model, E2, Q, 58Ni
[1] | P. J. Brussaard and P. W. M. Glademans "Shell-model Application in Nuclear Spectroscopy" North-Holland Publishing Company, Amsterdam (1977). |
[2] | M. Wang, G. Audi, A. H. Wapstra, F. G. Kondev, M. MacCormick, X. Xu and B. Pfeiffer Chinese Physics C36(2012) 1603-2014; http://people.physics.anu.edu.au/~ecs103/chart/ |
[3] | Http://ie.lbl.gov/education/isotopes.htm, “The Berkeley Laboratory Isotopes Project’s, Exploring the Table of Isotopes, Last updated May 22, 2000, Richard B. Firestone, e-mail: rbf@lbl.gov.”. |
[4] | Z. Wang and Z. Ren, Phys. Rev., Phys. Rev. C, vol. 71, 9 (2005). |
[5] | O. V. Bespalova, I. N. Boboshin, V. V. Varlamov, T. A. Ermakova, B. S. Ishkhanov, A. A. Klimochkina, S. Y. Komarov, H. Koura, E. A. Romanovsky, and T. I. Spasskaya, Bulletin of the Russian Academy of Sciences: Phys., vol. 74, no. 4, 542 (2010). |
[6] | B. A. Brown, J. M. Allmond, A. E. Stuchbery, A. Galindo-Uribarri, E. Padilla-Rodal, D. C. Radford, J. C. Batchelder, M. E. Howard, J. F. Liang, B. Manning, R. L. Varner, and C. H. Yu, Phys. Rev. C 90, 6 (2014). |
[7] | J. M. Yao, M. Bender, P-H. Heenen, Pys. Rev. C91, 023401(2014). |
[8] | G. Neyens; Rep. Prog. Phys., 66, 633 (2003). |
[9] | B. A. Brown, B. H. Wildenthal, C. F. Williamson, F. N. Rad, S. Kowisiki, H. crannell and J. T. O'Brien; Phys. Rev., C 324, 1127 (1985). |
[10] | L. R. B. Elton; "Nuclear Sizes", Oxford University Press (1961). |
APA Style
Huda A. Ruzuqy, Firas Z. Majeed. (2018). Nuclear Electric Quadrapole Moments (Q) in 58Ni. American Journal of Physics and Applications, 6(4), 80-84. https://doi.org/10.11648/j.ajpa.20180604.11
ACS Style
Huda A. Ruzuqy; Firas Z. Majeed. Nuclear Electric Quadrapole Moments (Q) in 58Ni. Am. J. Phys. Appl. 2018, 6(4), 80-84. doi: 10.11648/j.ajpa.20180604.11
AMA Style
Huda A. Ruzuqy, Firas Z. Majeed. Nuclear Electric Quadrapole Moments (Q) in 58Ni. Am J Phys Appl. 2018;6(4):80-84. doi: 10.11648/j.ajpa.20180604.11
@article{10.11648/j.ajpa.20180604.11, author = {Huda A. Ruzuqy and Firas Z. Majeed}, title = {Nuclear Electric Quadrapole Moments (Q) in 58Ni}, journal = {American Journal of Physics and Applications}, volume = {6}, number = {4}, pages = {80-84}, doi = {10.11648/j.ajpa.20180604.11}, url = {https://doi.org/10.11648/j.ajpa.20180604.11}, eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajpa.20180604.11}, abstract = {Nuclear Electric quadrapole moments Q in 58Ni for some selected levels have been investigated and calculated through Nuclear shell model and considering of 56Ni as an inert core with two active neutrons in a model space (2p3/2, 1f5/2 and 2p1/2) and the configuration mixing of the original states is also done. F5Pvh interaction has been utilized as a two body interaction to generate model space vectors with harmonic oscillator potential as a single particle wave function. OXBASH code is used to carry this calculations and the program of Core, Valence, Tassie (CVT) written in FORTRAN go language to calculate the Electric quadrapole moments between excited states themselves. All of these calculations have been carried through model space vectors only. One body density matrix elements (OBDM) for ground and Excited states is calculated in order to carry the calculations using single particle Transition matrix elements between excited states theme selves.}, year = {2018} }
TY - JOUR T1 - Nuclear Electric Quadrapole Moments (Q) in 58Ni AU - Huda A. Ruzuqy AU - Firas Z. Majeed Y1 - 2018/07/26 PY - 2018 N1 - https://doi.org/10.11648/j.ajpa.20180604.11 DO - 10.11648/j.ajpa.20180604.11 T2 - American Journal of Physics and Applications JF - American Journal of Physics and Applications JO - American Journal of Physics and Applications SP - 80 EP - 84 PB - Science Publishing Group SN - 2330-4308 UR - https://doi.org/10.11648/j.ajpa.20180604.11 AB - Nuclear Electric quadrapole moments Q in 58Ni for some selected levels have been investigated and calculated through Nuclear shell model and considering of 56Ni as an inert core with two active neutrons in a model space (2p3/2, 1f5/2 and 2p1/2) and the configuration mixing of the original states is also done. F5Pvh interaction has been utilized as a two body interaction to generate model space vectors with harmonic oscillator potential as a single particle wave function. OXBASH code is used to carry this calculations and the program of Core, Valence, Tassie (CVT) written in FORTRAN go language to calculate the Electric quadrapole moments between excited states themselves. All of these calculations have been carried through model space vectors only. One body density matrix elements (OBDM) for ground and Excited states is calculated in order to carry the calculations using single particle Transition matrix elements between excited states theme selves. VL - 6 IS - 4 ER -