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
Shankita Bhardwaj
中科院分区:
物理与天体物理4区
文献类型:
--
作者:
Surender Verma;Shankita Bhardwaj

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在我们的工作中,我们考虑了最小么正违反方案,得到了νμ→ντ\DocumentClass[12pt]{Minimum}\Usepackage{amsath}\Usepackage{amsFonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathsfs}\usepackage{upgreek}\setlong{\oddsidemargin}{-69pt}\Begin{Document}$\nu_{\Tau}$\end{Document}在真空和物质中振荡概率的一般表达式。对于该频道,我们研究了短基线实验对非么正参数的敏感性|ρμτ|\DocumentClass[12pt]{Minimum}\Usepackage{amsath}\Usepackage{wa ysym}\usepackage{amsFonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{maThrsfs}\usepackage{upgreek}\setlong{oddsidemarin}{-69pt}\Begin{Document}$|\Rho_{\Mu\tau}|$$\End{Document{Document}和ωμτ\entClass[12pt]{Minimum}\usepackage{amssym}\usepackage{asysym}\usepackage{amsFonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathsfs}\usepackage{upgreek}\setlong{oddsidemargin}{-69pt}\Begin{Document}$$\omega_{\Mu\tau}$\end{Document}表示正常的和逆的分层中微子质量和θ23\DocumentClass[12pt]{Minimum}\usepackage{amsmath}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{masfs}\Usepackage{upgreek}\setlong{\oddsidemargin}{-69pt}\Begin{Document}$$\theta_{23}$$\end{Document}高于或低于最大值。我们发现,对于正常的等级制度,The 3σ\DocumentClass[12pt]{Minimum}\usepackage{amsath}\usepackage{wa ysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathsfs}\usepackage{upgreek}\setlong{\oddsidemargin}{-69pt}\Begin{Document}$$3\sigma$\end{Document}敏感度|ρμτ|\DocumentClass[12pt]{Minimum}\usepackage{amsath}\usepackage{wa ysym}\usepackage{amsfonts}\usepackage{amsb}\usepackage{amssy}\非统一阶段的Usepackage{mathrsfs}\usepackage{upgreek}\setlong{oddsidemargin}{-69pt}\Begin{Document}$$|\rho_{Mu\tau}|$$\end{Document}是非统一阶段的最大值ωμτ=0\DocumentClass[12pt]{Minimum}\usepackage{amsath}\usesackage{amsFonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{upgreek}\setLong{\odsidemargin}{-69pt}\Begin{Document}$\$Omega_{\u\tau}=0$$\end{Document},而ωμτ=±π\DocumentClass[12pt]{Minimal}\usepackage{amsath}\usepackage{waysym}\usepackage{amsFonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{upgreek}\setLong{\oddsidemarin}{-69pt}\Begin{Document}$$\omega_{\MU\tau}=\pm\pi$\end{Document}。对于倒置层次结构,敏感度在ωμτ=0\DocumentClass[12pt]{Minimum}\Usepackage{amsath}\Usepackage{amsFonts}\Usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathsfs}\usepackage{upgreek}\setLong{\oddsidemargin}{-69pt}\Begin{Document}$$\omega_{\Mu\tau}=0$$\End{Document}时最小,对于ωμτ=±π\DocumentClass[12pt]{Minimum}\Usepackage{amsath}\usepackage{wa ysym}\usepackage{amssts}最大\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathsfs}\usepackage{upgreek}\setlong{\oddsidemargin}{-69pt}\Begin{Document}$$\omega_{\MU\tau}=\pm\pi$$\end{Document}。我们观察到,对于么正CP阶段δ=0\DocumentClass[12pt]{Minimum}\Usepackage{amsath}\Usepackage{amsFonts}\Usepackage{amssymb}\Usepackage{amsbsy}\usepackage{mathsfs}\usepackage{upgreek}\setLong{oddsidemargin}{-69pt}\Begin{Document}$$\Delta=0$$\END{DocumentClass[12pt]{Minimum\usepackage{amsath}\usepackage{wa ysym}\usepackage{usepackage{amsFonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathsfs}\usepackage{upgreek}\setlong{\oddsidemargin}{-69pt}\Begin{Document}$$\Delta=\pi/2$$\end{Document}。我们也有,探索了L/E比率的广谱,以考察由于单一性(δ\DocumentClass[12pt]{Minimum}\usepackage{amsath}\Usepackage{waysym}\usepackage{amsFonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{maThrsfs}\usepackage{upgreek}\setlong{oddsidemargin}{-69pt}\Begin{Document}$\Delta$$\End{Document})和非单一性(ωμτ\DocumentClass[12pt]{Minimum\usepackage{amsath}\Usepackage{wa ysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlong{\oddsidemargin}{-69pt}\Begin{Document}$$\omega_{\MU\tau}$$\end{Document})阶段。我们发现,对于L/E<200\DocumentClass[12pt]{Minimum}\UsPack{amsath}\Usepackage{wa ysym}\Usepackage{amsFonts}\Usepackage{amssymb}\Usepackage{amsbsy}\usepackage{matrsfs}\usepackage{upgreek}\setLong{\oddsidemargin}{-69pt}\Begin{Document}$L/E<200$$\end{Document}KM/GeV,原则上这两个阶段可以彼此解缠。
In the present work, we have considered minimal unitarity violation scheme to obtain the general expression for νμ→ντ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\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.
DOI: 10.1103/physrevlett.117.151803
发表时间: 2016-07
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
轻子混合的幺正性精密测试
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.