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Volumn 58, Issue 9, 1998, Pages

Three flavor neutrino oscillation analysis of the SuperKamiokande atmospheric neutrino data

Author keywords

[No Author keywords available]

Indexed keywords


EID: 1542575700     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.58.091301     Document Type: Article
Times cited : (54)

References (35)
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  • 2
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  • 3
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    • T. Kajita, talk presented at XVIII International Conference on Neutrino Physics and Astrophysics, 1998, Takayama, Japan, http://www-sk.icrr.u-tokyo.ac.jp/nu98/scan/063/;
    • T. Kajita, talk presented at XVIII International Conference on Neutrino Physics and Astrophysics, 1998, Takayama, Japan, http://www-sk.icrr.u-tokyo.ac.jp/nu98/scan/063/;
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    • Addison-Wesley, Reading, MA, J. N. Bahcall, R. Davis, Jr., P. Parker, A. Smirnov, R. Ulrich
    • See, e.g., SOLAR NEUTRINOS: The First Thirty Years, edited by J. N. Bahcall, R. Davis, Jr., P. Parker, A. Smirnov, and R. Ulrich (Addison-Wesley, Reading, MA, 1994), and references therein.
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    • 85038936847 scopus 로고    scopus 로고
    • If we lift the reactor constraint, the large (Formula presented) limit gives a reasonable fit to both the Kamiokande and SuperKamiokande data. This is because the matter effect (Formula presented) can account for the zenith angle dependence in case of three flavor oscillations with large (Formula presented)
    • If we lift the reactor constraint, the large (Formula presented) limit gives a reasonable fit to both the Kamiokande and SuperKamiokande data. This is because the matter effect (Formula presented) can account for the zenith angle dependence in case of three flavor oscillations with large (Formula presented) 910. The author would like to thank E. Lisi for discussions on this point.
  • 29
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    • Notice that Figs. 22 and 33 do not have an allowed region toward the right side even for (Formula presented) where the reactor experiments give no constraint.
    • Notice that Figs. 22 and 33 do not have an allowed region toward the right side even for (Formula presented) where the reactor experiments give no constraint.
  • 30
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    • The author has learned that it was found by M. C. Gonzalez-Garcia, H. Nunokawa, O. L. G. Peres, T. Stanev, and J. W. F. Valle, Phys. Rev. D 58, 033004 (1998), that pure (Formula presented) gives a poor fit to the Superkamiokande data. He would like to thank O. L. G. Peres and H. Nunokawa for pointing this out to him.
    • The author has learned that it was found by M. C. Gonzalez-Garcia, H. Nunokawa, O. L. G. Peres, T. Stanev, and J. W. F. Valle, Phys. Rev. D 58, 033004 (1998), that pure (Formula presented) gives a poor fit to the Superkamiokande data. He would like to thank O. L. G. Peres and H. Nunokawa for pointing this out to him.
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    • ICARUS experiment, http://www.aquila.infn.it/icarus/.
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    • KamLAND experiment, http://www.awa.tohoku.ac.jp/html/KamLAND/.
    • KamLAND experiment, http://www.awa.tohoku.ac.jp/html/KamLAND/.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.