In order to study the bound-state structure of the Helium halo nuclei, the 8-nucleon Yakubovsky formalism has been implemented for 8He in a 5-body sub-cluster model, i.e. α+n+n+n+n. In this case, the 8-nucleon Yakubovsky equations have been obtained in the form of two coupled equations, based on the two independent components. In addition, by removing the contribution interactions of the 8 and 7’s bound nucleons in the formalism, the obtained equations explicitly reduce to the 6-nucleon Yakubovsky equations for 6He, in the case of effective 3-body model, i.e. α+n+n. In view of the expectation for the dominant structure of 8He, namely an inert α-core and four loosely-bound neutrons, Jacobi configurations of the two components in momentum space have been represented to provide technicalities which were considered useful for a numerical performance, such as bound-state calculations and momentum density distributions for halo-bound neutrons.
Published in | American Journal of Modern Physics (Volume 8, Issue 3) |
DOI | 10.11648/j.ajmp.20190803.12 |
Page(s) | 40-49 |
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), 2019. Published by Science Publishing Group |
8-Nucleon Yakubovsky Formalism, Halo Nucleus Helium-8, Effective α-core Structure, Jacobi Configurations, Bound State Problem, Halo-bound Neutrons
[1] | M. Brodeur, et. al. Phys. Rev. Lett. 108, 052504 –31 Jan (2012). |
[2] | M. V. Zhukov, et. al. Physics Reports, Volume 231, Issue 4, August (1993), Pages 151-199. |
[3] | S. Bacca, A. Schwenk, G. Hagen, et. al. Eur. Phys. J. A, 42: 553 (2009). |
[4] | L. B. Wang et al., Phys. Rev. Lett. 93, 142501 (2004). |
[5] | P. Mueller et al., Phys. Rev. Lett. 99, 252501 (2007). |
[6] | V. L. Ryjkov et al., Phys. Rev. Lett. 101, 012501 (2008). |
[7] | S. C. Pieper and R. B. Wiringa, Annu. Rev. Nucl. Part. Sci. 51, 53 (2001); S. C. Pieper, arXiv: 0711.1500. |
[8] | P. Navratil and W. E. Ormand, Phys. Rev. C 68, 034305 (2003). |
[9] | P. Navratil, V. G. Gueorguiev, J. P. Vary, W. E. Ormand and A. Nogga, Phys. Rev. Lett. 99, 042501 (2007). |
[10] | 10. H. Kamada and W. Glӧckle, Nucl. Phys. A 548, 205 (1992). |
[11] | A. Nogga, H. Kamada and W. Glöckle, Phys. Rev. Lett. 85, 944 (2000). |
[12] | W. Glӧckle and H. Witala, Few-Body Syst. 51, 27-44 (2011). |
[13] | E. Ahmadi Pouya and A. A. Rajabi, Acta, Phys, Pol, B 48: 1279 (2017). |
[14] | E. Ahmadi Pouya and A. A. Rajabi, Eur. Phys. J. Plus, 131: 240 (2016). |
[15] | A. C. Fonseca, Phys. Rev. C 30, 35 (1984). |
[16] | W. Glöckle: The Quantum Mechanical Few-Body Problem. Springer-Verlag, New York (1983). |
[17] | D. Huber, H. Witala, A. Nogga, W. Glӧckle and H. Kamada, Few-Body Syst. 22, 107 (1997). |
[18] | E. Ahmadi Pouya and A. A. Rajabi, Karbala Int. J. of Mod. Science, Vol. 3, 4 (2017). |
APA Style
Eskandar Ahmadi Pouya, Ali Akbar Rajabi. (2019). Implementation of the 8-Nucleon Yakubovsky Formalism for Halo Nucleus 8He. American Journal of Modern Physics, 8(3), 40-49. https://doi.org/10.11648/j.ajmp.20190803.12
ACS Style
Eskandar Ahmadi Pouya; Ali Akbar Rajabi. Implementation of the 8-Nucleon Yakubovsky Formalism for Halo Nucleus 8He. Am. J. Mod. Phys. 2019, 8(3), 40-49. doi: 10.11648/j.ajmp.20190803.12
AMA Style
Eskandar Ahmadi Pouya, Ali Akbar Rajabi. Implementation of the 8-Nucleon Yakubovsky Formalism for Halo Nucleus 8He. Am J Mod Phys. 2019;8(3):40-49. doi: 10.11648/j.ajmp.20190803.12
@article{10.11648/j.ajmp.20190803.12, author = {Eskandar Ahmadi Pouya and Ali Akbar Rajabi}, title = {Implementation of the 8-Nucleon Yakubovsky Formalism for Halo Nucleus 8He}, journal = {American Journal of Modern Physics}, volume = {8}, number = {3}, pages = {40-49}, doi = {10.11648/j.ajmp.20190803.12}, url = {https://doi.org/10.11648/j.ajmp.20190803.12}, eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajmp.20190803.12}, abstract = {In order to study the bound-state structure of the Helium halo nuclei, the 8-nucleon Yakubovsky formalism has been implemented for 8He in a 5-body sub-cluster model, i.e. α+n+n+n+n. In this case, the 8-nucleon Yakubovsky equations have been obtained in the form of two coupled equations, based on the two independent components. In addition, by removing the contribution interactions of the 8 and 7’s bound nucleons in the formalism, the obtained equations explicitly reduce to the 6-nucleon Yakubovsky equations for 6He, in the case of effective 3-body model, i.e. α+n+n. In view of the expectation for the dominant structure of 8He, namely an inert α-core and four loosely-bound neutrons, Jacobi configurations of the two components in momentum space have been represented to provide technicalities which were considered useful for a numerical performance, such as bound-state calculations and momentum density distributions for halo-bound neutrons.}, year = {2019} }
TY - JOUR T1 - Implementation of the 8-Nucleon Yakubovsky Formalism for Halo Nucleus 8He AU - Eskandar Ahmadi Pouya AU - Ali Akbar Rajabi Y1 - 2019/09/10 PY - 2019 N1 - https://doi.org/10.11648/j.ajmp.20190803.12 DO - 10.11648/j.ajmp.20190803.12 T2 - American Journal of Modern Physics JF - American Journal of Modern Physics JO - American Journal of Modern Physics SP - 40 EP - 49 PB - Science Publishing Group SN - 2326-8891 UR - https://doi.org/10.11648/j.ajmp.20190803.12 AB - In order to study the bound-state structure of the Helium halo nuclei, the 8-nucleon Yakubovsky formalism has been implemented for 8He in a 5-body sub-cluster model, i.e. α+n+n+n+n. In this case, the 8-nucleon Yakubovsky equations have been obtained in the form of two coupled equations, based on the two independent components. In addition, by removing the contribution interactions of the 8 and 7’s bound nucleons in the formalism, the obtained equations explicitly reduce to the 6-nucleon Yakubovsky equations for 6He, in the case of effective 3-body model, i.e. α+n+n. In view of the expectation for the dominant structure of 8He, namely an inert α-core and four loosely-bound neutrons, Jacobi configurations of the two components in momentum space have been represented to provide technicalities which were considered useful for a numerical performance, such as bound-state calculations and momentum density distributions for halo-bound neutrons. VL - 8 IS - 3 ER -