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We propose that Bayesian variable selection for linear parametrisations with Gaussian iid likelihoods be based on the spherical symmetry of the diagonalised parameter space. Our r-prior results in closed forms for the evidence for four…

Statistics Theory · Mathematics 2015-12-11 M. B. De Kock , H. C. Eggers

The determination of the ordering of the neutrino masses (the hierarchy) is probably a crucial prerequisite to understand the origin of lepton masses and mixings and to establish their relationship to the analogous properties in the quark…

High Energy Physics - Phenomenology · Physics 2008-11-26 Olga Mena , Hiroshi Nunokawa , Stephen Parke

We investigate the impact of light ($\sim$ eV) sterile neutrinos in the long-baseline experiment T2K. We show that, within the 3+1 scheme, for mass-mixing parameters suggested by the short-baseline anomalies, the interference among the…

High Energy Physics - Phenomenology · Physics 2015-06-11 N. Klop , A. Palazzo

A physically viable ansatz for quark mass matrices must satisfy certain constraints, like the constraint imposed by CP-violation. In this article we study a concrete example, by looking at some generic matrices with a nearly democratic…

High Energy Physics - Phenomenology · Physics 2026-03-10 A. Kleppe

We review the effect that the choice of a uniform or logarithmic prior has on the Bayesian evidence and hence on Bayesian model comparisons when data provide only a one-sided bound on a parameter. We investigate two particular examples: the…

Cosmology and Nongalactic Astrophysics · Physics 2021-06-16 Lukas T. Hergt , Will J. Handley , Michael P. Hobson , Anthony N. Lasenby

The model of the neutrino mass matrix which we proposed in 2000 is revisited in the light of the recent T2K experiments. This model has the special property that it predicts the maximal 2-3 mixing and CP violation under the some simple…

High Energy Physics - Phenomenology · Physics 2015-11-18 Eiichi Takasugi

Beam neutrino oscillation experiments typically employ only one detector at a certain baseline, apart from the near detector that measures the unoscillated neutrino flux at the source. Lately, there have been discussions of having detectors…

High Energy Physics - Phenomenology · Physics 2019-07-03 Minseok Cho , YeolLin ChoeJo , Hye-Sung Lee , Young-Min Lee , Sushant K. Raut

One of the most criticized features of Bayesian statistics is the fact that credible intervals, especially when open likelihoods are involved, may strongly depend on the prior shape and range. Many analyses involving open likelihoods are…

Cosmology and Nongalactic Astrophysics · Physics 2020-07-15 S. Gariazzo

I study the weak basis CP-violating invariants in supersymmetric models, in particular those which cannot be expressed in terms of the Jarlskog--type invariants, and find basis--independent conditions for CP conservation. With an example of…

High Energy Physics - Phenomenology · Physics 2014-11-17 Oleg Lebedev

The T2K experiment presents new measurements of neutrino oscillation parameters using $19.7(16.3)\times10^{20}$ protons on target (POT) in (anti-)neutrino mode at the far detector (FD). Compared to the previous analysis, an additional…

High Energy Physics - Experiment · Physics 2023-09-12 The T2K Collaboration , K. Abe , N. Akhlaq , R. Akutsu , A. Ali , S. Alonso Monsalve , C. Alt , C. Andreopoulos , M. Antonova , S. Aoki , T. Arihara , Y. Asada , Y. Ashida , E. T. Atkin , M. Barbi , G. J. Barker , G. Barr , D. Barrow , M. Batkiewicz-Kwasniak , F. Bench , V. Berardi , L. Berns , S. Bhadra , A. Blanchet , A. Blondel , S. Bolognesi , T. Bonus , S. Bordoni , S. B. Boyd , A. Bravar , C. Bronner , S. Bron , A. Bubak , M. Buizza Avanzini , J. A. Caballero , N. F. Calabria , S. Cao , D. Carabadjac , A. J. Carter , S. L. Cartwright , M. G. Catanesi , A. Cervera , J. Chakrani , D. Cherdack , P. S. Chong , G. Christodoulou , A. Chvirova , M. Cicerchia , J. Coleman , G. Collazuol , L. Cook , A. Cudd , C. Dalmazzone , T. Daret , Yu. I. Davydov , A. De Roeck , G. De Rosa , T. Dealtry , C. C. Delogu , C. Densham , A. Dergacheva , F. Di Lodovico , S. Dolan , D. Douqa , T. A. Doyle , O. Drapier , J. Dumarchez , P. Dunne , K. Dygnarowicz , A. Eguchi , S. Emery-Schrenk , G. Erofeev , A. Ershova , G. Eurin , D. Fedorova , S. Fedotov , M. Feltre , A. J. Finch , G. A. Fiorentini Aguirre , G. Fiorillo , M. D. Fitton , J. M. Franco Patiño , M. Friend , Y. Fujii , Y. Fukuda , K. Fusshoeller , L. Giannessi , C. Giganti , V. Glagolev , M. Gonin , J. González Rosa , E. A. G. Goodman , A. Gorin , M. Grassi , M. Guigue , D. R. Hadley , J. T. Haigh , P. Hamacher-Baumann , D. A. Harris , M. Hartz , T. Hasegawa , S. Hassani , N. C. Hastings , Y. Hayato , D. Henaff , A. Hiramoto , M. Hogan , J. Holeczek , A. Holin , T. Holvey , N. T. Hong Van , T. Honjo , F. Iacob , A. K. Ichikawa , M. Ikeda , T. Ishida , M. Ishitsuka , H. T. Israel , K. Iwamoto , A. Izmaylov , N. Izumi , M. Jakkapu , B. Jamieson , S. J. Jenkins , C. Jesús-Valls , J. J. Jiang , P. Jonsson , S. Joshi , C. K. Jung , P. B. Jurj , M. Kabirnezhad , A. C. Kaboth , T. Kajita , H. Kakuno , J. Kameda , S. P. Kasetti , Y. Kataoka , Y. Katayama , T. Katori , M. Kawaue , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , H. Kikutani , S. King , V. Kiseeva , J. Kisiel , T. Kobata , H. Kobayashi , T. Kobayashi , L. Koch , S. Kodama , A. Konaka , L. L. Kormos , Y. Koshio , A. Kostin , T. Koto , K. Kowalik , Y. Kudenko , Y. Kudo , S. Kuribayashi , R. Kurjata , T. Kutter , M. Kuze , M. La Commara , L. Labarga , K. Lachner , J. Lagoda , S. M. Lakshmi , M. Lamers James , M. Lamoureux , A. Langella , J. -F. Laporte , D. Last , N. Latham , M. Laveder , L. Lavitola , M. Lawe , Y. Lee , C. Lin , S. -K. Lin , R. P. Litchfield , S. L. Liu , W. Li , A. Longhin , K. R. Long , A. Lopez Moreno , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , M. Malek , M. Mandal , S. Manly , A. D. Marino , L. Marti-Magro , D. G. R. Martin , M. Martini , J. F. Martin , T. Maruyama , T. Matsubara , V. Matveev , C. Mauger , K. Mavrokoridis , E. Mazzucato , N. McCauley , J. McElwee , K. S. McFarland , C. McGrew , J. McKean , A. Mefodiev , G. D. Megias , P. Mehta , L. Mellet , C. Metelko , M. Mezzetto , E. Miller , A. Minamino , O. Mineev , S. Mine , M. Miura , L. Molina Bueno , S. Moriyama , S. Moriyama , P. Morrison , Th. A. Mueller , D. Munford , L. Munteanu , K. Nagai , Y. Nagai , T. Nakadaira , K. Nakagiri , M. Nakahata , Y. Nakajima , A. Nakamura , H. Nakamura , K. Nakamura , K. D. Nakamura , Y. Nakano , S. Nakayama , T. Nakaya , K. Nakayoshi , C. E. R. Naseby , T. V. Ngoc , V. Q. Nguyen , K. Niewczas , S. Nishimori , Y. Nishimura , K. Nishizaki , T. Nosek , F. Nova , P. Novella , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , T. Odagawa , T. Ogawa , R. Okada , W. Okinaga , K. Okumura , T. Okusawa , N. Ospina , R. A. Owen , Y. Oyama , V. Palladino , V. Paolone , M. Pari , J. Parlone , S. Parsa , J. Pasternak , M. Pavin , D. Payne , G. C. Penn , D. Pershey , L. Pickering , C. Pidcott , G. Pintaudi , C. Pistillo , B. Popov , K. Porwit , M. Posiadala-Zezula , Y. S. Prabhu , F. Pupilli , B. Quilain , T. Radermacher , E. Radicioni , B. Radics , M. A. Ramírez , P. N. Ratoff , M. Reh , C. Riccio , E. Rondio , S. Roth , N. Roy , A. Rubbia , A. C. Ruggeri , C. A. Ruggles , A. Rychter , K. Sakashita , F. Sánchez , G. Santucci , C. M. Schloesser , K. Scholberg , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , A. Shaikhiev , F. Shaker , A. Shaykina , M. Shiozawa , W. Shorrock , A. Shvartsman , N. Skrobova , K. Skwarczynski , D. Smyczek , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , Y. Sonoda , A. J. Speers , R. Spina , I. A. Suslov , S. Suvorov , A. Suzuki , S. Y. Suzuki , Y. Suzuki , A. A. Sztuc , M. Tada , S. Tairafune , S. Takayasu , A. Takeda , Y. Takeuchi , K. Takifuji , H. K. Tanaka , Y. Tanihara , M. Tani , A. Teklu , V. V. Tereshchenko , N. Teshima , N. Thamm , L. F. Thompson , W. Toki , C. Touramanis , T. Towstego , K. M. Tsui , T. Tsukamoto , M. Tzanov , Y. Uchida , M. Vagins , D. Vargas , M. Varghese , G. Vasseur , C. Vilela , E. Villa , W. G. S. Vinning , U. Virginet , T. Vladisavljevic , T. Wachala , J. G. Walsh , Y. Wang , L. Wan , D. Wark , M. O. Wascko , A. Weber , R. Wendell , M. J. Wilking , C. Wilkinson , J. R. Wilson , K. Wood , C. Wret , J. Xia , Y. -h. Xu , K. Yamamoto , T. Yamamoto , C. Yanagisawa , G. Yang , T. Yano , K. Yasutome , N. Yershov , U. Yevarouskaya , M. Yokoyama , Y. Yoshimoto , N. Yoshimura , M. Yu , R. Zaki , A. Zalewska , J. Zalipska , K. Zaremba , G. Zarnecki , X. Zhao , T. Zhu , M. Ziembicki , E. D. Zimmerman , M. Zito , S. Zsoldos

Time reversal (T) symmetry violations in neutrino oscillations imply the presence of an $L$-odd component in the transition probability at fixed neutrino energy, with $L$ denoting the distance between neutrino source and detector. Within…

High Energy Physics - Phenomenology · Physics 2025-12-11 Sabya Sachi Chatterjee , Sudhanwa Patra , Thomas Schwetz , Kiran Sharma

Precision electroweak physics can provide fertile ground for uncovering new physics beyond the Standard Model (SM). One area in which new physics can appear is in so-called "oblique corrections", i.e., next-to-leading order expansions of…

High Energy Physics - Phenomenology · Physics 2015-03-17 Timothy Hobbs , Jonathan L. Rosner

The determination of the ordering of the neutrino masses (the hierarchy) is probably a crucial prerequisite to understand the origin of lepton masses and mixings and to establish their relationship to the analogous properties in the quark…

High Energy Physics - Phenomenology · Physics 2007-05-23 Olga Mena

T2K is a long baseline high intensity neutrino oscillation experiment employing an off-axis design to search for the as yet unobserved appearance of \nu_e neutrinos in a \nu_{\mu} beam. The neutrino beam originates at the J-PARC facility in…

High Energy Physics - Experiment · Physics 2019-08-14 Mark Hartz

We present a new method to analyze upcoming results in the search for CP violating neutrino oscillations. The CP violating amplitudes $\mathcal{A}_{\alpha\beta}^{kj}$ provide parametrization independent observables, which will be accessible…

High Energy Physics - Phenomenology · Physics 2017-04-12 Heinrich Päs , Philipp Sicking

Shrinkage prior has gained great successes in many data analysis, however, its applications mostly focus on the Bayesian modeling of sparse parameters. In this work, we will apply Bayesian shrinkage to model high dimensional parameter that…

Methodology · Statistics 2018-12-31 Qifan Song , Guang Cheng

The Bayesian formulation of inverse problems is attractive for three primary reasons: it provides a clear modelling framework; means for uncertainty quantification; and it allows for principled learning of hyperparameters. The posterior…

Statistics Theory · Mathematics 2019-05-14 Matthew M. Dunlop , Tapio Helin , Andrew M. Stuart

We study in detail the impact of a light sterile neutrino in the interpretation of the latest data of the long baseline experiments NO$\nu$A and T2K, assessing the robustness/fragility of the estimates of the standard 3-flavor parameters…

High Energy Physics - Phenomenology · Physics 2021-04-09 Sabya Sachi Chatterjee , Antonio Palazzo

T2K is a long baseline neutrino experiment which exploits a neutrino and antineutrino beam at JPARC to perform precision measurements of neutrino oscillation parameters $\Delta {\rm m}^2_{\rm 32}$, $\sin^2 \theta_{23}$ (besides the…

High Energy Physics - Experiment · Physics 2022-07-15 Ajmi Ali

CP violation in the lepton mass matrix will be probed with good precision in upcoming experiments. The amount of CP violation present in oscillations can be quantified in numerous ways and is typically parameterized by the complex phase…

High Energy Physics - Phenomenology · Physics 2021-05-20 Peter B. Denton , Rebekah Pestes