Neutrino oscillation physics potential of the T2K experiment
The observation of the recent electron neutrino appearance in a muon neutrino beam and the high-precision measurement of the mixing angle $\theta _{13}$ have led to a re-evaluation of the physics potential of the T2K long-baseline neutrino oscillation experiment. Sensitivities are explored for CP vi...
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creator | Abe, K. Aoki, S. Ariga, A. Barbi, M. Berardi, V. Berkman, S. Blondel, A. Bojechko, C. Bordoni, S. Bronner, C. Coleman, J. Coleman, S.J. Connolly, K. Das, R. Densham, C. Duffy, K. Escudero, L. Finch, A.J. Garcia, A. Giganti, C. Gilje, K. Hadley, D.R. Hansen, D. Hayato, Y. Himmel, A. Hiraki, T. Holeczek, J. Horikawa, S. Ieva, M. Imber, J. Ishii, T. Johnson, S. Kajita, T. Kameda, J. Katori, T. Kielczewska, D. Kikawa, T. Kobayashi, T. Kutter, T. Laihem, K. Laveder, M. Lister, C. Litchfield, R.P. Lopez, J.P. Ludovici, L. Marino, A.D. Marteau, J. Martin, J.F. Martins, P. Martynenko, S. McFarland, K.S. Missert, A. Nakahata, M. Nakamura, K.G. Nakamura, K. Nakaya, T. Nielsen, C. Nishimura, Y. O’Keeffe, H.M. Okumura, K. Okusawa, T. Ovsyannikova, T. Oyama, Y. Palladino, V. Palomino, J.L. Paolone, V. Perevozchikov, O. Perkin, J.D. Petrov, Y. Reeves, M. Rondio, E. Rubbia, A. Ruterbories, D. Schoppmann, S. Shaker, F. Shustrov, Y. Sobczyk, J.T. Stamoulis, P. Steinmann, J. Still, B. Suda, Y. Takahashi, S. Takeuchi, Y. Tanaka, H.K. Tanaka, H.A. Tanaka, M.M. Terhorst, D. Tobayama, S. Tomura, T. Touramanis, C. Vasseur, G. Warzycha, W. Weber, A. Williamson, Z. Yamamoto, K. Yen, S. Yoshida, K. Yu, M. Zambelli, L. Ziembicki, M. |
description | The observation of the recent electron neutrino appearance in a muon neutrino beam and the high-precision measurement of the mixing angle $\theta _{13}$ have led to a re-evaluation of the physics potential of the T2K long-baseline neutrino oscillation experiment. Sensitivities are explored for CP violation in neutrinos, non-maximal $\sin ^22\theta _{23}$, the octant of $\theta _{23}$, and the mass hierarchy, in addition to the measurements of $\delta _{{\rm CP}}$, $\sin ^2\theta _{23}$, and $\Delta m^2_{32}$, for various combinations of $\nu$-mode and $\bar {\nu }$-mode data-taking.With an exposure of $7.8\times 10^{21}$ protons-on-target, T2K can achieve 1$\sigma$ resolution of 0.050 (0.054) on $\sin ^2\theta _{23}$ and $0.040\ (0.045)\times 10^{-3}\,\rm {eV}^2$ on $\Delta m^2_{32}$ for 100% (50%) neutrino beam mode running assuming $\sin ^2\theta _{23}=0.5$ and $\Delta m^2_{32} = 2.4\times 10^{-3}\,\hbox {eV}^2$. T2K will have sensitivity to the CP-violating phase $\delta _{\rm {CP}}$ at 90% C.L. or better over a significant range. For example, if $\sin ^22\theta _{23}$ is maximal (i.e. $\theta _{23}=45^\circ$) the range is $-115^\circ \lt \delta _{\rm {CP}}\lt -60^\circ$ for normal hierarchy and $+50^\circ \lt \delta _{\rm {CP}}\lt +130^\circ$ for inverted hierarchy. When T2K data is combined with data from the NO$\nu$A experiment, the region of oscillation parameter space where there is sensitivity to observe a non-zero $\delta _{{\rm CP}}$ is substantially increased compared to if each experiment is analyzed alone. |
doi_str_mv | 10.1093/ptep/ptv031 |
format | Article |
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Sensitivities are explored for CP violation in neutrinos, non-maximal $\sin ^22\theta _{23}$, the octant of $\theta _{23}$, and the mass hierarchy, in addition to the measurements of $\delta _{{\rm CP}}$, $\sin ^2\theta _{23}$, and $\Delta m^2_{32}$, for various combinations of $\nu$-mode and $\bar {\nu }$-mode data-taking.With an exposure of $7.8\times 10^{21}$ protons-on-target, T2K can achieve 1$\sigma$ resolution of 0.050 (0.054) on $\sin ^2\theta _{23}$ and $0.040\ (0.045)\times 10^{-3}\,\rm {eV}^2$ on $\Delta m^2_{32}$ for 100% (50%) neutrino beam mode running assuming $\sin ^2\theta _{23}=0.5$ and $\Delta m^2_{32} = 2.4\times 10^{-3}\,\hbox {eV}^2$. T2K will have sensitivity to the CP-violating phase $\delta _{\rm {CP}}$ at 90% C.L. or better over a significant range. For example, if $\sin ^22\theta _{23}$ is maximal (i.e. $\theta _{23}=45^\circ$) the range is $-115^\circ \lt \delta _{\rm {CP}}\lt -60^\circ$ for normal hierarchy and $+50^\circ \lt \delta _{\rm {CP}}\lt +130^\circ$ for inverted hierarchy. When T2K data is combined with data from the NO$\nu$A experiment, the region of oscillation parameter space where there is sensitivity to observe a non-zero $\delta _{{\rm CP}}$ is substantially increased compared to if each experiment is analyzed alone.</description><identifier>ISSN: 2050-3911</identifier><identifier>ISSN: 0033-068X</identifier><identifier>EISSN: 2050-3911</identifier><identifier>DOI: 10.1093/ptep/ptv031</identifier><language>eng</language><publisher>Oxford University Press</publisher><subject>High Energy Physics - Experiment ; Physics</subject><ispartof>Progress of theoretical and experimental physics, 2015-04, Vol.2015 (4)</ispartof><rights>The Author(s) 2015. Published by Oxford University Press on behalf of the Physical Society of Japan. 2015</rights><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c502t-30c713933c3014b6047b44ef9a38657e6acaadc527c284a5e800ad199d1eee003</citedby><cites>FETCH-LOGICAL-c502t-30c713933c3014b6047b44ef9a38657e6acaadc527c284a5e800ad199d1eee003</cites><orcidid>0000-0003-2743-4741 ; 0000-0002-9543-2345 ; 0000-0001-5416-9301</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,860,881,1598,27901,27902</link.rule.ids><backlink>$$Uhttps://in2p3.hal.science/in2p3-01069288$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Abe, K.</creatorcontrib><creatorcontrib>Aoki, 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A.D.</creatorcontrib><creatorcontrib>Marteau, J.</creatorcontrib><creatorcontrib>Martin, J.F.</creatorcontrib><creatorcontrib>Martins, P.</creatorcontrib><creatorcontrib>Martynenko, S.</creatorcontrib><creatorcontrib>McFarland, K.S.</creatorcontrib><creatorcontrib>Missert, A.</creatorcontrib><creatorcontrib>Nakahata, M.</creatorcontrib><creatorcontrib>Nakamura, K.G.</creatorcontrib><creatorcontrib>Nakamura, K.</creatorcontrib><creatorcontrib>Nakaya, T.</creatorcontrib><creatorcontrib>Nielsen, C.</creatorcontrib><creatorcontrib>Nishimura, Y.</creatorcontrib><creatorcontrib>O’Keeffe, H.M.</creatorcontrib><creatorcontrib>Okumura, K.</creatorcontrib><creatorcontrib>Okusawa, T.</creatorcontrib><creatorcontrib>Ovsyannikova, T.</creatorcontrib><creatorcontrib>Oyama, Y.</creatorcontrib><creatorcontrib>Palladino, V.</creatorcontrib><creatorcontrib>Palomino, J.L.</creatorcontrib><creatorcontrib>Paolone, V.</creatorcontrib><creatorcontrib>Perevozchikov, O.</creatorcontrib><creatorcontrib>Perkin, J.D.</creatorcontrib><creatorcontrib>Petrov, Y.</creatorcontrib><creatorcontrib>Reeves, M.</creatorcontrib><creatorcontrib>Rondio, E.</creatorcontrib><creatorcontrib>Rubbia, A.</creatorcontrib><creatorcontrib>Ruterbories, D.</creatorcontrib><creatorcontrib>Schoppmann, S.</creatorcontrib><creatorcontrib>Shaker, F.</creatorcontrib><creatorcontrib>Shustrov, Y.</creatorcontrib><creatorcontrib>Sobczyk, J.T.</creatorcontrib><creatorcontrib>Stamoulis, P.</creatorcontrib><creatorcontrib>Steinmann, J.</creatorcontrib><creatorcontrib>Still, B.</creatorcontrib><creatorcontrib>Suda, Y.</creatorcontrib><creatorcontrib>Takahashi, S.</creatorcontrib><creatorcontrib>Takeuchi, Y.</creatorcontrib><creatorcontrib>Tanaka, H.K.</creatorcontrib><creatorcontrib>Tanaka, H.A.</creatorcontrib><creatorcontrib>Tanaka, M.M.</creatorcontrib><creatorcontrib>Terhorst, D.</creatorcontrib><creatorcontrib>Tobayama, S.</creatorcontrib><creatorcontrib>Tomura, T.</creatorcontrib><creatorcontrib>Touramanis, C.</creatorcontrib><creatorcontrib>Vasseur, G.</creatorcontrib><creatorcontrib>Warzycha, W.</creatorcontrib><creatorcontrib>Weber, A.</creatorcontrib><creatorcontrib>Williamson, Z.</creatorcontrib><creatorcontrib>Yamamoto, K.</creatorcontrib><creatorcontrib>Yen, S.</creatorcontrib><creatorcontrib>Yoshida, K.</creatorcontrib><creatorcontrib>Yu, M.</creatorcontrib><creatorcontrib>Zambelli, L.</creatorcontrib><creatorcontrib>Ziembicki, M.</creatorcontrib><creatorcontrib>The T2K Collaboration</creatorcontrib><title>Neutrino oscillation physics potential of the T2K experiment</title><title>Progress of theoretical and experimental physics</title><description>The observation of the recent electron neutrino appearance in a muon neutrino beam and the high-precision measurement of the mixing angle $\theta _{13}$ have led to a re-evaluation of the physics potential of the T2K long-baseline neutrino oscillation experiment. Sensitivities are explored for CP violation in neutrinos, non-maximal $\sin ^22\theta _{23}$, the octant of $\theta _{23}$, and the mass hierarchy, in addition to the measurements of $\delta _{{\rm CP}}$, $\sin ^2\theta _{23}$, and $\Delta m^2_{32}$, for various combinations of $\nu$-mode and $\bar {\nu }$-mode data-taking.With an exposure of $7.8\times 10^{21}$ protons-on-target, T2K can achieve 1$\sigma$ resolution of 0.050 (0.054) on $\sin ^2\theta _{23}$ and $0.040\ (0.045)\times 10^{-3}\,\rm {eV}^2$ on $\Delta m^2_{32}$ for 100% (50%) neutrino beam mode running assuming $\sin ^2\theta _{23}=0.5$ and $\Delta m^2_{32} = 2.4\times 10^{-3}\,\hbox {eV}^2$. T2K will have sensitivity to the CP-violating phase $\delta _{\rm {CP}}$ at 90% C.L. or better over a significant range. For example, if $\sin ^22\theta _{23}$ is maximal (i.e. $\theta _{23}=45^\circ$) the range is $-115^\circ \lt \delta _{\rm {CP}}\lt -60^\circ$ for normal hierarchy and $+50^\circ \lt \delta _{\rm {CP}}\lt +130^\circ$ for inverted hierarchy. When T2K data is combined with data from the NO$\nu$A experiment, the region of oscillation parameter space where there is sensitivity to observe a non-zero $\delta _{{\rm CP}}$ is substantially increased compared to if each experiment is analyzed alone.</description><subject>High Energy Physics - Experiment</subject><subject>Physics</subject><issn>2050-3911</issn><issn>0033-068X</issn><issn>2050-3911</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><sourceid>TOX</sourceid><recordid>eNp9kE1LAzEQQIMoWGpP_oGcvMjqTLJfAS-lqBWLXuo5pOksjaybsEmL_fduqagnLzMD82aGeYxdItwgKHkbEoUh7EDiCRsJKCCTCvH0T33OJjG-AwBCVUGOI3b3QtvUu85zH61rW5Oc73jY7KOzkQefqEvOtNw3PG2IL8Uzp89AvfsYGhfsrDFtpMl3HrO3h_vlbJ4tXh-fZtNFZgsQKZNgK5RKSisB81UJebXKc2qUkXVZVFQaa8zaFqKyos5NQTWAWaNSayQiADlm18e9G9PqMNw2_V574_R8utCuE0Hq4aNSibre4S9tex9jT83PCII-mNIHU_poaqCvjrTfhn_BL-A5aRo</recordid><startdate>20150401</startdate><enddate>20150401</enddate><creator>Abe, 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O.</creator><creator>Perkin, J.D.</creator><creator>Petrov, Y.</creator><creator>Reeves, M.</creator><creator>Rondio, E.</creator><creator>Rubbia, A.</creator><creator>Ruterbories, D.</creator><creator>Schoppmann, S.</creator><creator>Shaker, F.</creator><creator>Shustrov, Y.</creator><creator>Sobczyk, J.T.</creator><creator>Stamoulis, P.</creator><creator>Steinmann, J.</creator><creator>Still, B.</creator><creator>Suda, Y.</creator><creator>Takahashi, S.</creator><creator>Takeuchi, Y.</creator><creator>Tanaka, H.K.</creator><creator>Tanaka, H.A.</creator><creator>Tanaka, M.M.</creator><creator>Terhorst, D.</creator><creator>Tobayama, S.</creator><creator>Tomura, T.</creator><creator>Touramanis, C.</creator><creator>Vasseur, G.</creator><creator>Warzycha, W.</creator><creator>Weber, A.</creator><creator>Williamson, Z.</creator><creator>Yamamoto, K.</creator><creator>Yen, S.</creator><creator>Yoshida, K.</creator><creator>Yu, M.</creator><creator>Zambelli, L.</creator><creator>Ziembicki, M.</creator><general>Oxford University Press</general><general>Publication Office of Progress of Theoretical Physics</general><scope>TOX</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>1XC</scope><orcidid>https://orcid.org/0000-0003-2743-4741</orcidid><orcidid>https://orcid.org/0000-0002-9543-2345</orcidid><orcidid>https://orcid.org/0000-0001-5416-9301</orcidid></search><sort><creationdate>20150401</creationdate><title>Neutrino oscillation physics potential of the T2K experiment</title><author>Abe, K. ; Aoki, S. ; Ariga, A. ; Barbi, M. ; Berardi, V. ; Berkman, S. ; Blondel, A. ; Bojechko, C. ; Bordoni, S. ; Bronner, C. ; Coleman, J. ; Coleman, S.J. ; Connolly, K. ; Das, R. ; Densham, C. ; Duffy, K. ; Escudero, L. ; Finch, A.J. ; Garcia, A. ; Giganti, C. ; Gilje, K. ; Hadley, D.R. ; Hansen, D. ; Hayato, Y. ; Himmel, A. ; Hiraki, T. ; Holeczek, J. ; Horikawa, S. ; Ieva, M. ; Imber, J. ; Ishii, T. ; Johnson, S. ; Kajita, T. ; Kameda, J. ; Katori, T. ; Kielczewska, D. ; Kikawa, T. ; Kobayashi, T. ; Kutter, T. ; Laihem, K. ; Laveder, M. ; Lister, C. ; Litchfield, R.P. ; Lopez, J.P. ; Ludovici, L. ; Marino, A.D. ; Marteau, J. ; Martin, J.F. ; Martins, P. ; Martynenko, S. ; McFarland, K.S. ; Missert, A. ; Nakahata, M. ; Nakamura, K.G. ; Nakamura, K. ; Nakaya, T. ; Nielsen, C. ; Nishimura, Y. ; O’Keeffe, H.M. ; Okumura, K. ; Okusawa, T. ; Ovsyannikova, T. ; Oyama, Y. ; Palladino, V. ; Palomino, J.L. ; Paolone, V. ; Perevozchikov, O. ; Perkin, J.D. ; Petrov, Y. ; Reeves, M. ; Rondio, E. ; Rubbia, A. ; Ruterbories, D. ; Schoppmann, S. ; Shaker, F. ; Shustrov, Y. ; Sobczyk, J.T. ; Stamoulis, P. ; Steinmann, J. ; Still, B. ; Suda, Y. ; Takahashi, S. ; Takeuchi, Y. ; Tanaka, H.K. ; Tanaka, H.A. ; Tanaka, M.M. ; Terhorst, D. ; Tobayama, S. ; Tomura, T. ; Touramanis, C. ; Vasseur, G. ; Warzycha, W. ; Weber, A. ; Williamson, Z. ; Yamamoto, K. ; Yen, S. ; Yoshida, K. ; Yu, M. ; Zambelli, L. ; Ziembicki, M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c502t-30c713933c3014b6047b44ef9a38657e6acaadc527c284a5e800ad199d1eee003</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>High Energy Physics - Experiment</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Abe, K.</creatorcontrib><creatorcontrib>Aoki, S.</creatorcontrib><creatorcontrib>Ariga, A.</creatorcontrib><creatorcontrib>Barbi, M.</creatorcontrib><creatorcontrib>Berardi, V.</creatorcontrib><creatorcontrib>Berkman, S.</creatorcontrib><creatorcontrib>Blondel, A.</creatorcontrib><creatorcontrib>Bojechko, C.</creatorcontrib><creatorcontrib>Bordoni, S.</creatorcontrib><creatorcontrib>Bronner, C.</creatorcontrib><creatorcontrib>Coleman, J.</creatorcontrib><creatorcontrib>Coleman, S.J.</creatorcontrib><creatorcontrib>Connolly, K.</creatorcontrib><creatorcontrib>Das, R.</creatorcontrib><creatorcontrib>Densham, C.</creatorcontrib><creatorcontrib>Duffy, K.</creatorcontrib><creatorcontrib>Escudero, L.</creatorcontrib><creatorcontrib>Finch, A.J.</creatorcontrib><creatorcontrib>Garcia, A.</creatorcontrib><creatorcontrib>Giganti, C.</creatorcontrib><creatorcontrib>Gilje, K.</creatorcontrib><creatorcontrib>Hadley, D.R.</creatorcontrib><creatorcontrib>Hansen, D.</creatorcontrib><creatorcontrib>Hayato, Y.</creatorcontrib><creatorcontrib>Himmel, A.</creatorcontrib><creatorcontrib>Hiraki, T.</creatorcontrib><creatorcontrib>Holeczek, J.</creatorcontrib><creatorcontrib>Horikawa, S.</creatorcontrib><creatorcontrib>Ieva, M.</creatorcontrib><creatorcontrib>Imber, J.</creatorcontrib><creatorcontrib>Ishii, T.</creatorcontrib><creatorcontrib>Johnson, S.</creatorcontrib><creatorcontrib>Kajita, T.</creatorcontrib><creatorcontrib>Kameda, J.</creatorcontrib><creatorcontrib>Katori, T.</creatorcontrib><creatorcontrib>Kielczewska, D.</creatorcontrib><creatorcontrib>Kikawa, T.</creatorcontrib><creatorcontrib>Kobayashi, T.</creatorcontrib><creatorcontrib>Kutter, T.</creatorcontrib><creatorcontrib>Laihem, K.</creatorcontrib><creatorcontrib>Laveder, M.</creatorcontrib><creatorcontrib>Lister, C.</creatorcontrib><creatorcontrib>Litchfield, R.P.</creatorcontrib><creatorcontrib>Lopez, J.P.</creatorcontrib><creatorcontrib>Ludovici, L.</creatorcontrib><creatorcontrib>Marino, A.D.</creatorcontrib><creatorcontrib>Marteau, J.</creatorcontrib><creatorcontrib>Martin, J.F.</creatorcontrib><creatorcontrib>Martins, P.</creatorcontrib><creatorcontrib>Martynenko, S.</creatorcontrib><creatorcontrib>McFarland, K.S.</creatorcontrib><creatorcontrib>Missert, A.</creatorcontrib><creatorcontrib>Nakahata, M.</creatorcontrib><creatorcontrib>Nakamura, K.G.</creatorcontrib><creatorcontrib>Nakamura, K.</creatorcontrib><creatorcontrib>Nakaya, T.</creatorcontrib><creatorcontrib>Nielsen, C.</creatorcontrib><creatorcontrib>Nishimura, Y.</creatorcontrib><creatorcontrib>O’Keeffe, H.M.</creatorcontrib><creatorcontrib>Okumura, K.</creatorcontrib><creatorcontrib>Okusawa, T.</creatorcontrib><creatorcontrib>Ovsyannikova, T.</creatorcontrib><creatorcontrib>Oyama, Y.</creatorcontrib><creatorcontrib>Palladino, V.</creatorcontrib><creatorcontrib>Palomino, J.L.</creatorcontrib><creatorcontrib>Paolone, V.</creatorcontrib><creatorcontrib>Perevozchikov, O.</creatorcontrib><creatorcontrib>Perkin, J.D.</creatorcontrib><creatorcontrib>Petrov, Y.</creatorcontrib><creatorcontrib>Reeves, M.</creatorcontrib><creatorcontrib>Rondio, E.</creatorcontrib><creatorcontrib>Rubbia, A.</creatorcontrib><creatorcontrib>Ruterbories, D.</creatorcontrib><creatorcontrib>Schoppmann, S.</creatorcontrib><creatorcontrib>Shaker, F.</creatorcontrib><creatorcontrib>Shustrov, Y.</creatorcontrib><creatorcontrib>Sobczyk, J.T.</creatorcontrib><creatorcontrib>Stamoulis, P.</creatorcontrib><creatorcontrib>Steinmann, J.</creatorcontrib><creatorcontrib>Still, B.</creatorcontrib><creatorcontrib>Suda, Y.</creatorcontrib><creatorcontrib>Takahashi, S.</creatorcontrib><creatorcontrib>Takeuchi, Y.</creatorcontrib><creatorcontrib>Tanaka, H.K.</creatorcontrib><creatorcontrib>Tanaka, H.A.</creatorcontrib><creatorcontrib>Tanaka, M.M.</creatorcontrib><creatorcontrib>Terhorst, D.</creatorcontrib><creatorcontrib>Tobayama, S.</creatorcontrib><creatorcontrib>Tomura, T.</creatorcontrib><creatorcontrib>Touramanis, C.</creatorcontrib><creatorcontrib>Vasseur, G.</creatorcontrib><creatorcontrib>Warzycha, W.</creatorcontrib><creatorcontrib>Weber, A.</creatorcontrib><creatorcontrib>Williamson, Z.</creatorcontrib><creatorcontrib>Yamamoto, K.</creatorcontrib><creatorcontrib>Yen, S.</creatorcontrib><creatorcontrib>Yoshida, K.</creatorcontrib><creatorcontrib>Yu, M.</creatorcontrib><creatorcontrib>Zambelli, L.</creatorcontrib><creatorcontrib>Ziembicki, M.</creatorcontrib><creatorcontrib>The T2K Collaboration</creatorcontrib><collection>Oxford Journals Open Access Collection</collection><collection>CrossRef</collection><collection>Hyper Article en Ligne (HAL)</collection><jtitle>Progress of theoretical and experimental physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Abe, K.</au><au>Aoki, S.</au><au>Ariga, A.</au><au>Barbi, M.</au><au>Berardi, V.</au><au>Berkman, S.</au><au>Blondel, A.</au><au>Bojechko, C.</au><au>Bordoni, S.</au><au>Bronner, C.</au><au>Coleman, J.</au><au>Coleman, S.J.</au><au>Connolly, K.</au><au>Das, R.</au><au>Densham, C.</au><au>Duffy, K.</au><au>Escudero, L.</au><au>Finch, A.J.</au><au>Garcia, A.</au><au>Giganti, C.</au><au>Gilje, K.</au><au>Hadley, D.R.</au><au>Hansen, D.</au><au>Hayato, Y.</au><au>Himmel, A.</au><au>Hiraki, T.</au><au>Holeczek, J.</au><au>Horikawa, S.</au><au>Ieva, M.</au><au>Imber, J.</au><au>Ishii, T.</au><au>Johnson, S.</au><au>Kajita, T.</au><au>Kameda, J.</au><au>Katori, T.</au><au>Kielczewska, D.</au><au>Kikawa, T.</au><au>Kobayashi, T.</au><au>Kutter, T.</au><au>Laihem, K.</au><au>Laveder, M.</au><au>Lister, C.</au><au>Litchfield, R.P.</au><au>Lopez, J.P.</au><au>Ludovici, L.</au><au>Marino, A.D.</au><au>Marteau, J.</au><au>Martin, J.F.</au><au>Martins, P.</au><au>Martynenko, S.</au><au>McFarland, K.S.</au><au>Missert, A.</au><au>Nakahata, M.</au><au>Nakamura, K.G.</au><au>Nakamura, K.</au><au>Nakaya, T.</au><au>Nielsen, C.</au><au>Nishimura, Y.</au><au>O’Keeffe, H.M.</au><au>Okumura, K.</au><au>Okusawa, T.</au><au>Ovsyannikova, T.</au><au>Oyama, Y.</au><au>Palladino, V.</au><au>Palomino, J.L.</au><au>Paolone, V.</au><au>Perevozchikov, O.</au><au>Perkin, J.D.</au><au>Petrov, Y.</au><au>Reeves, M.</au><au>Rondio, E.</au><au>Rubbia, A.</au><au>Ruterbories, D.</au><au>Schoppmann, S.</au><au>Shaker, F.</au><au>Shustrov, Y.</au><au>Sobczyk, J.T.</au><au>Stamoulis, P.</au><au>Steinmann, J.</au><au>Still, B.</au><au>Suda, Y.</au><au>Takahashi, S.</au><au>Takeuchi, Y.</au><au>Tanaka, H.K.</au><au>Tanaka, H.A.</au><au>Tanaka, M.M.</au><au>Terhorst, D.</au><au>Tobayama, S.</au><au>Tomura, T.</au><au>Touramanis, C.</au><au>Vasseur, G.</au><au>Warzycha, W.</au><au>Weber, A.</au><au>Williamson, Z.</au><au>Yamamoto, K.</au><au>Yen, S.</au><au>Yoshida, K.</au><au>Yu, M.</au><au>Zambelli, L.</au><au>Ziembicki, M.</au><aucorp>The T2K Collaboration</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Neutrino oscillation physics potential of the T2K experiment</atitle><jtitle>Progress of theoretical and experimental physics</jtitle><date>2015-04-01</date><risdate>2015</risdate><volume>2015</volume><issue>4</issue><issn>2050-3911</issn><issn>0033-068X</issn><eissn>2050-3911</eissn><abstract>The observation of the recent electron neutrino appearance in a muon neutrino beam and the high-precision measurement of the mixing angle $\theta _{13}$ have led to a re-evaluation of the physics potential of the T2K long-baseline neutrino oscillation experiment. Sensitivities are explored for CP violation in neutrinos, non-maximal $\sin ^22\theta _{23}$, the octant of $\theta _{23}$, and the mass hierarchy, in addition to the measurements of $\delta _{{\rm CP}}$, $\sin ^2\theta _{23}$, and $\Delta m^2_{32}$, for various combinations of $\nu$-mode and $\bar {\nu }$-mode data-taking.With an exposure of $7.8\times 10^{21}$ protons-on-target, T2K can achieve 1$\sigma$ resolution of 0.050 (0.054) on $\sin ^2\theta _{23}$ and $0.040\ (0.045)\times 10^{-3}\,\rm {eV}^2$ on $\Delta m^2_{32}$ for 100% (50%) neutrino beam mode running assuming $\sin ^2\theta _{23}=0.5$ and $\Delta m^2_{32} = 2.4\times 10^{-3}\,\hbox {eV}^2$. T2K will have sensitivity to the CP-violating phase $\delta _{\rm {CP}}$ at 90% C.L. or better over a significant range. For example, if $\sin ^22\theta _{23}$ is maximal (i.e. $\theta _{23}=45^\circ$) the range is $-115^\circ \lt \delta _{\rm {CP}}\lt -60^\circ$ for normal hierarchy and $+50^\circ \lt \delta _{\rm {CP}}\lt +130^\circ$ for inverted hierarchy. When T2K data is combined with data from the NO$\nu$A experiment, the region of oscillation parameter space where there is sensitivity to observe a non-zero $\delta _{{\rm CP}}$ is substantially increased compared to if each experiment is analyzed alone.</abstract><pub>Oxford University Press</pub><doi>10.1093/ptep/ptv031</doi><orcidid>https://orcid.org/0000-0003-2743-4741</orcidid><orcidid>https://orcid.org/0000-0002-9543-2345</orcidid><orcidid>https://orcid.org/0000-0001-5416-9301</orcidid><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 2050-3911 |
ispartof | Progress of theoretical and experimental physics, 2015-04, Vol.2015 (4) |
issn | 2050-3911 0033-068X 2050-3911 |
language | eng |
recordid | cdi_hal_primary_oai_HAL_in2p3_01069288v1 |
source | Oxford Journals Open Access Collection; DOAJ Directory of Open Access Journals; Oxford University Press Open Access Books; Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals |
subjects | High Energy Physics - Experiment Physics |
title | Neutrino oscillation physics potential of the T2K experiment |
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