Transition magnetic moments of JP=(3/2)+ decuplet to JP=(1/2)+ octet baryons in the chiral constituent quark model

Harleen Dahiya

doi:10.1088/1674-1137/42/9/093102

Chinese Physics C> 2018, Vol. 42> Issue(9) : 093102 DOI: 10.1088/1674-1137/42/9/093102

Transition magnetic moments of J^P=(3/2)⁺ decuplet to J^P=(1/2)⁺ octet baryons in the chiral constituent quark model

Harleen Dahiya

1.
Department of Physics, Dr. B. R. Ambedkar National Institute of Technology, Jalandhar, 144011, India

Abstract
HTML
Reference
Related

PDF

Abstract：
In light of the developments of the chiral constituent quark model (χCQM) in studying low energy hadronic matrix elements of the ground-state baryons, we extend this model to investigate their transition properties. The magnetic moments of transitions from the J^P=(3/2)⁺ decuplet to J^P=(1/2)⁺ octet baryons are calculated with explicit valence quark spin, sea quark spin and sea quark orbital angular momentum contributions. Since the experimental data is available for only a few transitions, we compare our results with the results of other available models. The implications of other complicated effects such as chiral symmetry breaking and SU(3) symmetry breaking arising due to confinement of quarks are also discussed.
- baryon magnetic moments ,
- quark model ,
- chiral symmetries

References

[1]	J. Ashman et al (EMC Collaboration), Phys. Lett. B, 206:364 (1988); J. Ashman et al (EMC Collaboration), Nucl. Phys. B, 328:1 (1989)
[2]	B. Adeva et al (SMC Collaboration), Phys. Rev. D, 58:112001 (1998)
[3]	P.L. Anthony et al (E142 Collaboration), Phys. Rev. Lett., 71:959 (1993); K. Abe et al (E143 Collaboration), Phys. Rev. Lett., 76:587 (1996); K. Abe et al (E154 Collaboration), Phys. Rev. Lett., 79:26 (1997); P. Adams et al, Phys. Rev. D, 56:5330 (1997)
[4]	E.A. Hawker et al (E866/NuSea Collaboration), Phys. Rev. Lett., 80:3715 (1998); J.C. Peng et al, Phys. Rev. D, 58:092004 (1998); R.S. Towell et al, Phys. Rev. D, 64:052002 (2001)
[5]	A. Airapetian et al (HERMES Collaboration), Phys. Rev. D, 71:012003 (2005)
[6]	C. Patrignani et al (Particle Data Group), Chin. Phys. C, 40:100001 (2016)
[7]	D. B. Lichtenberg, Phys. Rev. D, 15:345 (1977); A. L. Choudry and V. Joshi, Phys. Rev. D, 13:3115 (1976)
[8]	M. Gupta, S. K. Sood, and A. N. Mitra, Phys. Rev. D, 16:216 (1977); M. Gupta and A. N. Mitra, Phys. Rev. D, 18:1585 (1978); M. Gupta, S. K. Sood, and A. N. Mitra, Phys. Rev. D, 19:104 (1979); M. Gupta and N. Kaur, Phys. Rev. D, 28:534 (1983); P. N. Pandit, M. P. Khanna, and M. Gupta, J. Phys. G, 11:683 (1985)
[9]	A. Faessler, T. Gutsche, M. A. Ivanov, J. G. Korner, and V. E. Lyubovitskij, Phys. Rev. D, 73:094013 (2006)
[10]	F. Schlumpf, Phys. Rev. D, 48:4478 (1993); B. Julia-Diaz, and D. O. Riska, Nucl. Phys. A, 739:69 (2004); G. Ramalho, K. Tsushima, and F. Gross, Phys. Rev. D, 80:033004 (2009)
[11]	P. Ha, Phys. Rev. D, 58:113003 (1998); C. S. An, Q. B. Li, D. O. Riska, and B. S. Zou, Phys. Rev. C, 74:055205 (2006)
[12]	M.D. Slaughter, Phys. Rev. C, 82:015208 (2010); M. D. Slaughter, Phys. Rev. D, 84:071303 (2011)
[13]	A. Bernotas, and V. Simonis, Phys. Rev. D, 87:074016 (2013)
[14]	B. O. Kerbikov and Y. A. Simonov, Phys. Rev. D, 62:093016 (2000)
[15]	T. M. Aliev, A. Ozpineci, and M. Savci, Phys. Rev. D, 62:053012 (2000); T. M. Aliev, A. Ozpineci, M. Savc, Phys. Rev. D, 65:056008 (2002); T. M. Aliev, K. Azizi, A. Ozpineci, Phys. Rev. D, 77:114006 (2008); T. M. Aliev, K. Azizi, M. Savc, Nucl. Phys. B, 895:59 (2012); T. M. Aliev, K. Azizi, M. Savc, JHEP, 1304:042 (2013); T. M. Aliev, K. Azizi, M. Savc, J. Phys. G, 40:065003 (2013); T. M. Aliev, A. Ozpineci, V.S. Zamiralov, Phys. Atom. Nucl., 73:1754 (2010)
[16]	F. X. Lee, Phys. Rev. D, 57:1801 (1998); S. L. Zhu, W. Y. P. Hwang, and Z. S. P. Yang, Phys. Rev. D, 57:1527 (1998); A. Iqubal, M. Dey, and J. Dey, Phys. Lett. B, 477:125 (2000)
[17]	B. Patel, A. K. Rai, and P. C. Vinodkumar, J. Phys. G, 35:065001 (2008)
[18]	B. Schwesinger and H. Weigel, Nucl. Phys. A, 540:461 (1992); Y. Oh, Phys. Rev. D, 75:074002 (2007)
[19]	T. Ledwig, A. Silva, and M. Vanderhaeghen, Phys. Rev D, 79:094025 (2009)
[20]	H-C. Kim, M. Praszalowicz, and K. Goeke, Phys. Rev. D, 57:2859 (1998); G. S. Yang, H-C. Kim, M. Praszalowicz, and K. Goeke, Phys. Rev. D, 70:114002 (2004); S. Scholl, and H. Weigel, Nucl. Phys. B, 735:163 (2004)
[21]	E. E. Jenkins and A.V. Manohar, Phys. Lett. B, 335:452 (1994); M. A. Luty, J. March-Russell, and M. J. White, Phys. Rev. D, 51:2332 (1995); A. J. Buchmann, J. A. Hester, and R. F. Lebed, Phys. Rev. D, 66:056002 (2002); A. J. Buchmann and R. F. Lebed, Phys. Rev. D, 67:016002 (2003); R. Flores-Mendieta, Phys. Rev. D, 80:094014 (2009); L. S. Geng, J. M. Camalich, and M. J. V. Vacas, Phys. Rev D, 80:034027 (2009)
[22]	S. Boinepalli, D. B. Leinweber, P. J. Moran, A. G. Williams, J. M. Zanotti, and J. B. Zhang, Phys. Rev. D, 80:054505 (2009); C. Aubin, K. Orginos, V. Pascalutsa, and M. Vanderhaeghen, Phys. Rev. D, 79:051502 (2009); P. E. Shanahan et al (CSSM and QCDSF/UKQCD Collaborations), Phys. Rev. D, 89:074511 (2014)
[23]	F. X. Lee, R. Kelly, L. Zhou, and W. Wilcox, Phys. Lett. B, 627:71 (2005)
[24]	A. J. Buchmann, E. Hernandez, and A. Faessler, Nucl. Phys. A, 569:661 (1994); G. Wagner, A. J. Buchmann, and A. Faessler, Phys. Lett. B, 359:288 (1995); A. J. Buchmann, E. Hernandez, and A. Faessler, Phys. Rev. C, 55:448 (1997); G. Wagner, A. J. Buchmann, and A. Faessler, Phys. Rev. C, 58:3666 (1998); G. Wagner, A. J. Buchmann, and A. Faessler, J. Phys. G, 26:267 (2000); A. J. Buchmann and E. M. Henley, Phys. Rev. C, 63:015202 (2000); A. J. Buchmann, Phys. Rev. Lett., 93:212301 (2004)
[25]	M. N. Butler, M. J. Savage and R. P. Springer, Phys. Lett. B, 304:353 (1993); H-S. Li, Z-W. Liu, X-L. Chen, W-Z. Deng, and S-L. Zhu, arXiv:1706.06458
[26]	T. M. Aliev, A. Ozpineci, and M. Savc, Phys. Rev. D, 65:096004 (2002)
[27]	E. E. Jenkins, Phys. Rev. D, 85:065007 (2012)
[28]	R. F. Lebed and D. R. Martin, Phys. Rev. D, 70:016008 (2004)
[29]	G. Ramalho and K. Tsushima, Phys. Rev. D, 87:093011 (2013)
[30]	G. Kaelbermann and J. M. Eisenberg, Phys. Rev. D, 28:71 (1983); K. Bermuth, D. Drechsel, L. Tiator, and J. B. Seaborn, Phys. Rev. D, 37:89 (1988); D. H. Lu, A. W. Thomas and A. G. Williams, Phys. Rev. C, 55:3108 (1997)
[31]	A. Wirzba and W. Weise, Phys. Lett. B, 188:6 (1987); A. Abada, H. Weigel, and H. Reinhardt, Phys. Lett. B, 366:26 (1996); H. Walliser and G. Holzwarth, Z. Phys. A, 357:317 (1997)
[32]	S. T. Hong, Phys. Rev. D, 76:094029 (2007)
[33]	L. Wang and F. X. Lee, AIP Conf. Proc., 1182:532 (2009)
[34]	D. B. Leinweber, T. Draper and R.M. Woloshyn, Phys. Rev. D, 48:2230 (1993); C. Alexandrou et al, Phys. Rev. D, 69:114506 (2004); C. Alexandrou, P. de Forcrand, H. Neff, J. W. Negele, W. Schroers, and A. Tsapalis, Phys. Rev. Lett., 94:021601 (2005); G. Ramalho and M. T. Pena, Phys. Rev. D, 80:013008 (2009)
[35]	H. C. Kim, M. Polyakov, M. Praszalowicz, G. S. Yang, and K. Goeke, Phys. Rev. D, 71:094023 (2005)
[36]	R. Dhir and R. C. Verma, Eur. Phys. J. A, 42:243 (2009)
[37]	G. Ramalho and K. Tsushima, Phys. Rev. D, 88:053002 (2013)
[38]	D. Keller and K. Hicks, Eur. Phys. J. A, 49:53 (2013)
[39]	S. Weinberg, Physica A, 96:327 (1979); A. Manohar and H. Georgi, Nucl. Phys. B, 234:189 (1984)
[40]	E. J. Eichten, I. Hinchliffe, and C. Quigg, Phys. Rev. D, 45:2269 (1992)
[41]	T. P. Cheng and L. F. Li, Phys. Rev. Lett., 74:2872 (1995); T. P. Cheng and L. F. Li, Phys. Rev. D, 57:344 (1998); T. P. Cheng and L. F. Li, Phys. Rev. Lett., 80:2789 (1998)
[42]	J. Linde, T. Ohlsson, and H. Snellman, Phys. Rev. D, 57:452 (1998); J. Linde, T. Ohlsson, and H. Snellman, Phys. Rev. D, 57:5916 (1998)
[43]	X. Song, J. S. McCarthy, and H. J. Weber, Phys. Rev. D, 55:2624 (1997); X. Song, Phys. Rev. D, 57:4114 (1998)
[44]	H. Dahiya and M. Gupta, Phys. Rev. D, 64:014013 (2001); H. Dahiya and M. Gupta, Int. Jol. of Mod. Phys. A, 19(29):5027 (2004); H. Dahiya, M. Gupta and J. M. S. Rana, Int. Jol. of Mod. Phys. A, 21(21):4255 (2006); H. Dahiya and M. Randhawa, Phys. Rev. D, 90:074001 (2014)
[45]	H. Dahiya and M. Gupta, Eur. Phys. J. C, 52:571 (2007); H. Dahiya and M. Gupta, Phys. Rev. D, 78:014001 (2008)
[46]	N. Sharma, H. Dahiya, P.K. Chatley, and M. Gupta, Phys. Rev. D, 79:077503 (2009); N. Sharma, H. Dahiya and P. K. Chatley, Eur. Phys. J. A, 44:125 (2010); N. Sharma and H. Dahiya, Phys. Rev. D, 81:114003 (2010)
[47]	H. Dahiya and M. Randhawa, Phys. Rev. D, 93:114030 (2016)
[48]	H. Dahiya and M. Randhawa, Int. Jol. of Mod. Phys. A, 32(31):1750185 (2017)
[49]	N. Sharma and H. Dahiya, Pramana,, 81:449 (2013); N. Sharma and H. Dahiya, Pramana, 80:237 (2013)
[50]	H. Dahiya and M. Gupta, Phys. Rev. D, 66:051501(R) (2002)
[51]	A. Girdhar, H. Dahiya and M. Randhawa, Phys. Rev. D, 92:033012 (2015)
[52]	N. Sharma, A. M. Torres, K. P. Khemchandani, and H. Dahiya, Eur. Jol. Phys. A, 49:11 (2013)
[53]	A. M. Torres, K. P. Khemchandani, N. Sharma, and H. Dahiya, Eur. Jol. Phys. A, 48:185 (2012)
[54]	A. Le Yaouanc, L. Oliver, O. Pene, and J. C. Raynal, Phys. Rev. D, 12:2137 (1975); A. Le Yaouanc, L. Oliver, O. Pene, and J.C. Raynal, Phys. Rev. D, 15:844 (1977)

[1]	Jiazheng Ji , Yuheng Xing , Xinxing Wu , Ning Xu , Yue Tan . Dynamical study of T_ss systems using the chiral quark model. Chinese Physics C, 2025, 49(1): 013101. doi: 10.1088/1674-1137/ad7c28
[2]	Xiaoyun Chen , Fu-Lai Wang , Yue Tan , Youchang Yang . Double-heavy tetraquarks with strangeness in the chiral quark model. Chinese Physics C, 2023, 47(2): 023102. doi: 10.1088/1674-1137/ac9de9
[3]	Yue Tan , Jialun Ping . X(2900) in a chiral quark model. Chinese Physics C, 2021, 45(9): 093104. doi: 10.1088/1674-1137/ac0ba4
[4]	Wei-Jie Fu . Chiral criticality and glue dynamics. Chinese Physics C, 2019, 43(7): 074101. doi: 10.1088/1674-1137/43/7/074101
[5]	Zalak Shah , Ajay Kumar Rai . Spectroscopy of the Ω_ccb baryon in the hypercentral constituent quark model. Chinese Physics C, 2018, 42(5): 053101. doi: 10.1088/1674-1137/42/5/053101
[6]	Jia Chen , Chunsheng An , Hong Chen . Mixing of the lowest-lying qqq configurations with J^P=1/2^- in different hyperfine interaction models. Chinese Physics C, 2018, 42(3): 034104. doi: 10.1088/1674-1137/42/3/034104
[7]	Cui-Bai Luo , Song Shi , Yong-Hui Xia , Hong-Shi Zong . Dynamical chiral symmetry breaking in NJL Model with a strong background magnetic field and Lorentz-violating extension of the Standard Model. Chinese Physics C, 2017, 41(6): 063104. doi: 10.1088/1674-1137/41/6/063104
[8]	Chao Wang , Yujiang Bi , Hao Cai , Ying Chen , Ming Gong , Zhaofeng Liu . Quark chiral condensate from the overlap quark propagator. Chinese Physics C, 2017, 41(5): 053102. doi: 10.1088/1674-1137/41/5/053102
[9]	Yubing Dong , Fei Huang , Pengnian Shen , Zongye Zhang . On the decays of d^* in a constituent chiral quark model. Chinese Physics C, 2017, 41(10): 101001. doi: 10.1088/1674-1137/41/10/101001
[10]	Hui Li , Zong-Xiu Wu , Chun-Sheng An , Hong Chen . Low-lying 1/2^- hidden strange pentaquark states in the constituent quark model. Chinese Physics C, 2017, 41(12): 124104. doi: 10.1088/1674-1137/41/12/124104
[11]	LUAN Yi-Long , CHEN Xiao-Lin , DENG Wei-Zhen . Meson electro-magnetic form factors in an extended Nambu-Jona-Lasinio model including heavy quark flavors. Chinese Physics C, 2015, 39(11): 113103. doi: 10.1088/1674-1137/39/11/113103
[12]	CHEN Shao-Na , PING Jia-Lun . Radial excitation states of η and η' in the chiral quark model. Chinese Physics C, 2012, 36(8): 681-690. doi: 10.1088/1674-1137/36/8/001
[13]	LI Ming-Tao , DONG Yu-Bing , ZHANG Zong-Ye . A study of meson-meson potential in the chiral quark model. Chinese Physics C, 2011, 35(7): 622-628. doi: 10.1088/1674-1137/35/7/005
[14]	ZHONG Xian-Hui , ZHAO Qiang . K^－p scattering and hyperon excitations in a chiral quark model. Chinese Physics C, 2010, 34(9): 1428-1432. doi: 10.1088/1674-1137/34/9/062
[15]	. Lowest-lying spin-1/2 and spin-3/2 baryon magnetic moments in chiral perturbation theory. Chinese Physics C, 2010, 34(9): 1307-1311. doi: 10.1088/1674-1137/34/9/030
[16]	HE Jun . Study of nucleon resonances in a chiral quark model via η productions. Chinese Physics C, 2009, 33(12): 1389-1392. doi: 10.1088/1674-1137/33/12/062
[17]	ZHONG Xian-Hui , ZHAO Qiang . Λ resonances studied in K^－p→Σ⁰π⁰ in a chiral quark model. Chinese Physics C, 2009, 33(12): 1373-1376. doi: 10.1088/1674-1137/33/12/058
[18]	Pan Feng , Dai Lianrong . Magnetic Moments of Odd a Nuclei in q-Deformed Nuclear Shell Model. Chinese Physics C, 1996, 20(S2): 197-204.
[19]	Xu Xiaoming , Qiu Xijun . A Chiral Quark-Soliton Model Theory for Nuclear Force. Chinese Physics C, 1990, 14(S4): 381-389.
[20]	XIE YI-CHENG . THE BARYON MAGNETIC MOMENT IN A QUARK-DIQUARK MODEL. Chinese Physics C, 1982, 6(5): 653-656.

Access

Get Citation

Harleen Dahiya. Transition magnetic moments of J^P=(3/2)⁺ decuplet to J^P=(1/2)⁺ octet baryons in the chiral constituent quark model[J]. Chinese Physics C, 2018, 42(9): 093102. doi: 10.1088/1674-1137/42/9/093102

RIS(for EndNote,Reference Manager,ProCite)

BibTex

Txt

Milestone

Received: 2018-05-10

Article Metric

Article Views(1814)
PDF Downloads(20)
Cited by(0)

Policy on re-use

To reuse of Open Access content published by CPC, for content published under the terms of the Creative Commons Attribution 3.0 license (“CC CY”), the users don’t need to request permission to copy, distribute and display the final published version of the article and to create derivative works, subject to appropriate attribution.

通讯作者: 陈斌, bchen63@163.com

1.
沈阳化工大学材料科学与工程学院沈阳 110142

Transition magnetic moments of J^P=(3/2)⁺ decuplet to J^P=(1/2)⁺ octet baryons in the chiral constituent quark model

Abstract：

References

Access

Article Metrics

Metrics

通讯作者: 陈斌, bchen63@163.com

Email This Article

Transition magnetic moments of J^P=(3/2)⁺ decuplet to J^P=(1/2)⁺ octet baryons in the chiral constituent quark model

HTML

目录