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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Veröffentlicht in:Progress of theoretical and experimental physics 2015-04, Vol.2015 (4)
Hauptverfasser: 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.
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container_issue 4
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container_title Progress of theoretical and experimental physics
container_volume 2015
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
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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. 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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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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>
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subjects High Energy Physics - Experiment
Physics
title Neutrino oscillation physics potential of the T2K experiment
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