摘要We analyse the recently published results from solar neutrino experiments SNO Phase-III and SAGE Part-III and show their constraints on solar neutrino oscillation parameters, especially for the mixing angle θ12. Through a global analysis using all existing data from SK, SNO, Ga&Cl radiochemical experiments and long base line reactor experiment KamLAND, we obtain the parameters Δm212=7.684+0.212-0.208×10-5,eV2, tan2θ12=0.440+0.059-0.057. We also find that the discrepancy between the KamLAND and solar neutrino results can be reduced by choosing a small non-zero value for the mixing angle θ13.
Abstract:We analyse the recently published results from solar neutrino experiments SNO Phase-III and SAGE Part-III and show their constraints on solar neutrino oscillation parameters, especially for the mixing angle θ12. Through a global analysis using all existing data from SK, SNO, Ga&Cl radiochemical experiments and long base line reactor experiment KamLAND, we obtain the parameters Δm212=7.684+0.212-0.208×10-5,eV2, tan2θ12=0.440+0.059-0.057. We also find that the discrepancy between the KamLAND and solar neutrino results can be reduced by choosing a small non-zero value for the mixing angle θ13.
YANG Ping;LIU Qiu-Yu. Solar Neutrino Oscillation Parameters after SNO Phase-III and SAGE Part-III[J]. 中国物理快报, 2009, 26(8): 81402-081402.
YANG Ping, LIU Qiu-Yu. Solar Neutrino Oscillation Parameters after SNO Phase-III and SAGE Part-III. Chin. Phys. Lett., 2009, 26(8): 81402-081402.
[1] Wolfenstein L 1978 Phys. Rev. D 17 2369 [2] Mikheyev S P and Smirnov A Y 1985 Sov. J. Nucl.Phys. 42 913 [3] Liu Q Y, Chen B L, Zhou J, Luo M J and Jing S C 2005 Commun. Theor. Phys. 44 505 [4] Yang P and Liu Q Y 2009 Chin. Phys. Lett. 26031401 [5] Hosaka J et al (Super-Kamkiokande Collaboration) 2006 Phys. Rev. D 73 112001 [6] Cravens J P et al (Super-Kamiokande Collaboration) 2008 Phys. Rev. D 78 032002 [7] Ahmad Q R et al (SNO Collaboration) 2002 Phys. Rev.Lett. 89 011302 [8] Aharmim B et al (SNO Collaboration) 2005 Phys. Rev.C 72 055502 [9] Cleveland B T et al 1998 Astrophys. J. 496 505 [10] Altmann M et al (GALLEX Collaboration) 2000 Phys.Lett. B 490 16 [11] Altmann M et al (GNO Collaboration) 2005 Phys.Lett. B 616 174 [12] Abdurashitov J N et al. (SAGE Collaboration) 1999 Phys. Rev. C 60 055801 [13] Abdurashitov J N et al (SAGE Collaboration) 2002 J.Exp. Theor. Phys. 95 181 [14] Abdurashitov J N et al. (SAGE Collaboration) 2009arXiv:nucl-ex/0901.2200v1 [15] Eguchi K et al (KamLAND Collaboration) 2003 Phys.Rev. Lett. 90 021802 [16] Araki T et al (KamLAND Collaboration) 2005 Phys.Rev. Lett. 94 081801 [17] Abe S et al (KamLAND Collaboration) 2008 Phys. Rev.Lett. 100 221803 [18] Aharmim B et al (SNO Collaboration) 2008 Phys. Rev.Lett. 101 111301 [19] For details see HOWTO Using the SNO Salt FluxResults http://sno.phy.queensu.ca. [20] Winter W T et al 2006 Phys. Rev. C 73 025503 [21] For details see HOWTO Using the SNO NCD FluxResults http://sno.phy.queensu.ca. [22] de Holanda P C, Liao W and Smirnov A Y 2004 Nucl.Phys. B 702 307 [23] Liu Q Y, Maris M and Petcov S T 1997 Phys. Rev. D 56 5991 [24] Maris M and Petcov S T 1997 Phys. Rev. D 567444 [25] de Holanda P C and Smirnov A Y 2002 Phys. Rev. D 66 113005 [26] Bahcall J N, Pinsonneault M H and Basu S 2001 Astrophys. J. 555 990 [27] Gonzalez-Garcia M C and Nir Y 2003 Rev. Mod. Phys. 75 345