摘要The SU(3) quadrupole−quadrupole interaction is replaced by the SO(6) cubic [Q(0)×Q(0)×Q(0)]0 interaction in fitting energy levels, some energy ratios and B(E2) ratios. It is shown that the alternative scheme can indeed be used to describe properties of the X(5) nuclei, for example, 150Nd, 152Sm, 154Gd. The results of the new scheme are compared with the corresponding experimental data and with those of the traditional U(5)−SU(3) transitional description. It is clearly shown that the results are better than those obtained from the traditional U(5)− SU(3) transitional description.
Abstract:The SU(3) quadrupole−quadrupole interaction is replaced by the SO(6) cubic [Q(0)×Q(0)×Q(0)]0 interaction in fitting energy levels, some energy ratios and B(E2) ratios. It is shown that the alternative scheme can indeed be used to describe properties of the X(5) nuclei, for example, 150Nd, 152Sm, 154Gd. The results of the new scheme are compared with the corresponding experimental data and with those of the traditional U(5)−SU(3) transitional description. It is clearly shown that the results are better than those obtained from the traditional U(5)− SU(3) transitional description.
DAI Lian-Rong**;TENG Wei-Xin;PAN Feng;WANG Sheng-Hua
. An Alternative Interacting Boson Model Description of The N =90 Nuclei[J]. 中国物理快报, 2011, 28(5): 52101-052101.
DAI Lian-Rong**, TENG Wei-Xin, PAN Feng, WANG Sheng-Hua
. An Alternative Interacting Boson Model Description of The N =90 Nuclei. Chin. Phys. Lett., 2011, 28(5): 52101-052101.
[1] Feng D H, Gilmore R and Deans S R 1981 Phys. Rev. C 23 1254
[2] Jolie J, Cejnar P, Casten R F, Heinze S, Linnemann A and Werner V 2002 Phys. Rev. Lett. 89 182502
[3] Iachello F and Zamfir N V 2004 Phys. Rev. Lett. 92 212501
[4] Zamfir N V, von Brentano P, Casten R F and Jolie J 2002 Phys. Rev. C 66 021304(R)
[5] Werner V, von Brentano P, Casten R F and Jolie J 2002 Phys. Lett. B 527 55
[6] Iachello F 2000 Phys. Rev. Lett. 85 3580
[7] Iachello F 2001 Phys. Rev. Lett. 87 052502
[8] van Isacker P 1999 Phys. Rev. Lett. 83 4269
[9] Thiamova G, Cejinar P 2006 Nucl. Phys. A 765 97
[10] Krücken R, Albanna B, Bialik C, Casten R F, Cooper J R, Dewald A, Zamfir N V, Barton C J, Beausang C W, Caprio M A, Hecht A A, Klug T, Novak J R, Pietralla N and von Brentano P 2002 Phys. Rev. Lett. 88 232501
[11] Casten R F and Zamfir N V 2001 Phys. Rev. Lett. 87 052503
[12] Tonev D, Dewald A, Klug T, Petkov P, Jolie J, Fitzler A, Möller O, Heinze S, von Brentano P and Casten R F 2004 Phys. Rev. C 69 034334
[13] Iachello F and Arima A 1987 The Interacting Boson Model (Cambridge University Press, Cambridge)
[14] Caprio M A, Zamfir N V, Casten R F, Barton C J, Beausang C W, Cooper J R, Hecht A A, Krücken R, Newman H, Novak J R, Pietralla N, Wolf A and Zyromski K E 2002 Phys. Rev. C 66 054310
[15] Dewald A, Möller O, Saha B, Jessen K, Fitzler A, Melon B, Pissulla T, Heinze S, Jolie J, Zell K O, von Brentano P, Petkov P, Harissopulos S, De Angelis G, Martinez T, Napoli D R, Marginean N, Axiotis M, Rusu C, Tonev D, Gadea A, Zhang Y H, Bazzacco D, Lunardi S, Ur C A, Menegazzo R and Farnea E 2005 J. Phys. G 31 S1427
[16] Dewald A, Möller O, Tonev D, Fitzler A and Saha B, Jessen K, Heinze S, Linnemann A, Jolie J and Zell K O et al 2004 Eur. Phys. J. A 20 173
[17] Möller O, Dewald A, Petkov P, Saha B, Fitzler A, Jessen K, Tonev D, Klug T, Heinze S, Jolie J, von Brentano P, Bazzacco D, Ur C A, Farnea E, Axiotis M, Lunardi S, de Angelis G, Napoli D R, Marginean N, Martinez T, Caprio M A and Casten R F 2006 Phys. Rev. C 74 024313
[18] Dermateosian E and Tuli J K 1995 Nuclear Data Sheets 75 827
[19] Artna-Cohen Agda 1996 Nuclear Data Sheets 79 1
[20] Reich C W 2009 Nuclear Data Sheets 110 2257