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

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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

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[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)

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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

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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

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

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