Probing non-unitary CP violation effects in neutrino oscillation experiments
Probing non-unitary CP violation effects in neutrino oscillation experiments
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探讨中微子振荡实验中的非酉CP破坏效应
DOI:
10.1007/s12648-018-1211-7
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发表时间:
2016
影响因子:
2
通讯作者:
Shankita Bhardwaj
中科院分区:
文献类型:
--
作者:
Surender Verma;Shankita Bhardwaj
In the present work, we have considered minimal unitarity violation scheme to obtain the general expression for νμ→ντ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\nu _{\mu }\rightarrow \nu _{\tau }$$\end{document} oscillation probability in vacuum and matter. For this channel, we have investigated the sensitivities of short baseline experiments to non-unitary parameters |ρμτ|\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$|\rho _{\mu \tau }|$$\end{document} and ωμτ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\omega _{\mu \tau }$$\end{document} for normal as well as inverted hierarchical neutrino masses and θ23\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\theta _{23}$$\end{document} being above or below maximality. We find that for normal hierarchy, the 3σ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$3\sigma$$\end{document} sensitivity of |ρμτ|\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$|\rho _{\mu \tau }|$$\end{document} is maximum for non-unitary phase ωμτ=0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\omega _{\mu \tau }=0$$\end{document} whereas it is minimum for ωμτ=±π\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\omega _{\mu \tau }=\pm \pi$$\end{document}. For inverted hierarchy, the sensitivity is minimum at ωμτ=0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\omega _{\mu \tau }=0$$\end{document} and maximum for ωμτ=±π\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\omega _{\mu \tau }=\pm \pi$$\end{document}. We observe that the sensitivity to measure non-unitarity remains unaffected for unitary CP phase δ=0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\delta =0$$\end{document} or δ=π/2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\delta =\pi /2$$\end{document}. We have, also, explored wide spectrum of L/E ratio to investigate the possibilities to observe CP-violation due to unitary (δ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\delta$$\end{document}) and non-unitary (ωμτ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\omega _{\mu \tau }$$\end{document}) phases. We find that the both phases can be disentangled, in principle, from each other for L/E<200\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$L/E<200$$\end{document} km/GeV.
影响因子:
8.6
作者:
P. Adamson;I. Anghel;I. Anghel;A. Aurisano;G. Barr;M. Bishai;A. Blake;A. Blake;G. Bock;D. Bogert;S. Cao;T. Carroll;C. Castromonte;R. Chen;S. Childress;J. Coelho;L. Corwin;L. Corwin;D. Cronin-Hennessy;J. D. Jong;S. Rijck;A. Devan;N. Devenish;M. Diwan;C. Escobar;J. Evans;E. Falk;G. Feldman;W. Flanagan;M. Frohne;M. Frohne;M. Gabrielyan;H. Gallagher;S. Germani;R. Gomes;M. Goodman;P. Gouffon;N. Graf;R. Gran;K. Grzelak;A. Habig;S. Hahn;J. Hartnell;R. Hatcher;A. Holin;J. Huang;J. Hylen;G. Irwin;Z. Isvan;C. James;D. Jensen;T. Kafka;S. Amcix;G. Koizumi;M. Kordosky;A. Kreymer;K. Lang;P. Litchfield;P. Litchfield;P. Lucas;W. A. Mann;M. Marshak;N. Mayer;C. Mcgivern;M. M. Medeiros-M.;R. Mehdiyev;J. Meier;M. Messier;W. Miller;S. Mishra;S. M. Sher;C. Moore;L. Mualem;J. Musser;D. Naples;J. Nelson;H. Newman;R. Nichol;J. Nowak;J. Nowak;J. O’Connor;M. Orchanian;R. Pahlka;J. Paley;R. Patterson;G. Pawloski;A. Perch;M. Pfützner;D. Phan;S. Phan-Budd;R. Plunkett;N. Poonthottathil;X. Qiu;A. Radovic;B. Rebel;C. Rosenfeld;H. Rubin;P. Sail;M. Sánchez;M. Sánchez;J. Schneps;A. Schreckenberger;P. Schreiner;R. Sharma;A. Sousa;N. Tagg;R. Talaga;J. Thomas;M. Thomson;X. Tian;A. Timmons;J. Todd;S. Tognini;R. Toner;D. Torretta;G. Tzanakos;J. Urheim;P. Vahle;B. Viren;A. Weber;A. Weber;R. Webb;C. White;L. Whitehead;L. Whitehead;S. Wojcicki;R. Zwaska
通讯作者:
P. Adamson;I. Anghel;I. Anghel;A. Aurisano;G. Barr;M. Bishai;A. Blake;A. Blake;G. Bock;D. Bogert;S. Cao;T. Carroll;C. Castromonte;R. Chen;S. Childress;J. Coelho;L. Corwin;L. Corwin;D. Cronin-Hennessy;J. D. Jong;S. Rijck;A. Devan;N. Devenish;M. Diwan;C. Escobar;J. Evans;E. Falk;G. Feldman;W. Flanagan;M. Frohne;M. Frohne;M. Gabrielyan;H. Gallagher;S. Germani;R. Gomes;M. Goodman;P. Gouffon;N. Graf;R. Gran;K. Grzelak;A. Habig;S. Hahn;J. Hartnell;R. Hatcher;A. Holin;J. Huang;J. Hylen;G. Irwin;Z. Isvan;C. James;D. Jensen;T. Kafka;S. Amcix;G. Koizumi;M. Kordosky;A. Kreymer;K. Lang;P. Litchfield;P. Litchfield;P. Lucas;W. A. Mann;M. Marshak;N. Mayer;C. Mcgivern;M. M. Medeiros-M.;R. Mehdiyev;J. Meier;M. Messier;W. Miller;S. Mishra;S. M. Sher;C. Moore;L. Mualem;J. Musser;D. Naples;J. Nelson;H. Newman;R. Nichol;J. Nowak;J. Nowak;J. O’Connor;M. Orchanian;R. Pahlka;J. Paley;R. Patterson;G. Pawloski;A. Perch;M. Pfützner;D. Phan;S. Phan-Budd;R. Plunkett;N. Poonthottathil;X. Qiu;A. Radovic;B. Rebel;C. Rosenfeld;H. Rubin;P. Sail;M. Sánchez;M. Sánchez;J. Schneps;A. Schreckenberger;P. Schreiner;R. Sharma;A. Sousa;N. Tagg;R. Talaga;J. Thomas;M. Thomson;X. Tian;A. Timmons;J. Todd;S. Tognini;R. Toner;D. Torretta;G. Tzanakos;J. Urheim;P. Vahle;B. Viren;A. Weber;A. Weber;R. Webb;C. White;L. Whitehead;L. Whitehead;S. Wojcicki;R. Zwaska
DOI:
10.1209/0295-5075/105/11001
发表时间:
2014
期刊:
Europhysics Letters
影响因子:
--
作者:
Basso L;Fischer O;van der Bij J. J.
通讯作者:
van der Bij J. J.