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A novel low-energy neutrino-oscillation experiment NOSTOS, combining a strong tritium source and a high pressure spherical TPC detector (10 m in radius) has been recently proposed. The goal of the experiment is to measure the mixing angle…

High Energy Physics - Experiment · Physics 2009-11-11 I. Giomataris , S. Aune , P. Colas , I. Irastorza , B. Peyaud , J. Dolbeau , P. Gorodetzky , H. van der Graff , T. Patzak , P. Salin , V. Lepeltier , J. D. Vergados

By postulating the relation \theta_{23} \simeq 45^\circ + \eta\theta_{13}, we seek preferable correction terms to tri-bi-maximal mixing and discuss their origins. Global analyses of the neutrino oscillation parameters favor \eta=\pm…

High Energy Physics - Phenomenology · Physics 2014-05-07 Takeshi Araki

Under the assumption of Minimal Flavour Violation (MFV), the Unitarity Triangle (UT) can be determined by using only angle measurements and tree-level observables. In this respect, the most accurate quantities today available are sin 2…

High Energy Physics - Phenomenology · Physics 2009-01-06 Wolfgang Altmannshofer , Andrzej J. Buras , Diego Guadagnoli , Michael Wick

This Letter reports measurements of muon-neutrino disappearance and electron-neutrino appearance and the corresponding antineutrino processes between the two NOvA detectors in the NuMI neutrino beam. These measurements use a dataset with…

High Energy Physics - Experiment · Physics 2026-03-11 NOvA Collaboration , S. Abubakar , M. A. Acero , B. Acharya , P. Adamson , N. Anfimov , A. Antoshkin , E. Arrieta-Diaz , L. Asquith , A. Aurisano , D. Azevedo , A. Back , N. Balashov , P. Baldi , B. A. Bambah , E. F. Bannister , A. Barros , A. Bat , R. Bernstein , T. J. C. Bezerra , V. Bhatnagar , B. Bhuyan , J. Bian , A. C. Booth , R. Bowles , B. Brahma , C. Bromberg , N. Buchanan , A. Butkevich , S. Calvez , T. J. Carroll , E. Catano-Mur , J. P. Cesar , S. Chaudhary , R. Chirco , S. Choate , B. C. Choudhary , O. T. K. Chow , A. Christensen , M. F. Cicala , T. E. Coan , T. Contreras , A. Cooleybeck , D. Coveyou , L. Cremonesi , G. S. Davies , P. F. Derwent , P. Ding , Z. Djurcic , K. Dobbs , M. Dolce , D. Duenas Tonguino , E. C. Dukes , A. Dye , R. Ehrlich , E. Ewart , G. J. Feldman , P. Filip , M. J. Frank , H. R. Gallagher , F. Gao , A. Giri , R. A. Gomes , M. C. Goodman , R. Group , A. Habig , F. Hakl , J. Hartnell , R. Hatcher , J. M. Hays , M. He , K. Heller , V Hewes , A. Himmel , T. Horoho , X. Huang , A. Ivanova , B. Jargowsky , I. Kakorin , A. Kalitkina , D. M. Kaplan , A. Khanam , B. Kirezli , J. Kleykamp , O. Klimov , L. W. Koerner , L. Kolupaeva , R. Kralik , A. Kumar , C. D. Kuruppu , V. Kus , T. Lackey , K. Lang , J. Lesmeister , A. Lister , J. Liu , J. A. Lock , M. MacMahon , S. Magill , W. A. Mann , M. T. Manoharan , M. Manrique Plata , M. L. Marshak , M. Martinez-Casales , V. Matveev , A. Medhi , B. Mehta , M. D. Messier , H. Meyer , T. Miao , V. Mikola , W. H. Miller , S. R. Mishra , A. Mislivec , R. Mohanta , A. Moren , A. Morozova , W. Mu , L. Mualem , M. Muether , K. Mulder , C. Murthy , D. Myers , J. Nachtman , D. Naples , S. Nelleri , J. K. Nelson , O. Neogi , R. Nichol , E. Niner , A. Norman , A. Norrick , H. Oh , A. Olshevskiy , T. Olson , M. Ozkaynak , A. Pal , J. Paley , L. Panda , R. B. Patterson , G. Pawloski , R. Petti , R. K. Plunkett , L. R. Prais , A. Rafique , V. Raj , M. Rajaoalisoa , B. Ramson , B. Rebel , C. Reynolds , E. Robles , P. Roy , O. Samoylov , M. C. Sanchez , S. Sanchez Falero , P. Shanahan , P. Sharma , A. Sheshukov , A. Shmakov , W. Shorrock , S. Shukla , I. Singh , P. Singh , V. Singh , S. Singh Chhibra , D. K. Singha , E. Smith , J. Smolik , P. Snopok , N. Solomey , A. Sousa , K. Soustruznik , M. Strait , C. Sullivan , L. Suter , A. Sutton , S. K. Swain , A. Sztuc , N. Talukdar , P. Tas , T. Thakore , J. Thomas , E. Tiras , M. Titus , Y. Torun , D. Tran , J. Trokan-Tenorio , J. Urheim , B. Utt , P. Vahle , Z. Vallari , K. J. Vockerodt , A. V. Waldron , M. Wallbank , T. K. Warburton , C. Weber , M. Wetstein , D. Whittington , D. A. Wickremasinghe , J. Wolcott , S. Wu , W. Wu , W. Wu , Y. Xiao , B. Yaeggy , A. Yahaya , A. Yankelevich , K. Yonehara , S. Zadorozhnyy , J. Zalesak , R. Zwaska

The triplet or type-II seesaw mechanism is the simplest way to endow neutrinos with mass in the Standard Model (SM). Here we review its associated theory and phenomenology, including restrictions from $S$, $T$, $U$ parameters, neutrino…

High Energy Physics - Phenomenology · Physics 2022-06-01 Sanjoy Mandal , O. G. Miranda , G. Sanchez Garcia , J. W. F. Valle , Xun-Jie Xu

We show that the four high-energy Littlest Seesaw parameters in the flavour basis,namely two real Yukawa couplings plus the two right-handed neutrino masses, can be determined by an excellent fit to the seven currently constrained…

High Energy Physics - Phenomenology · Physics 2018-11-14 Stephen F. King , Susana Molina Sedgwick , Samuel J. Rowley

Diffusion Multi-modal Large Language Models (dMLLMs) have recently emerged as a novel architecture unifying image generation and understanding. However, developing effective and efficient Test-Time Scaling (TTS) methods to unlock their full…

Computer Vision and Pattern Recognition · Computer Science 2026-04-09 Yi Xin , Siqi Luo , Tianxiang Xu , Qi Qin , Haoxing Chen , Kaiwen Zhu , Zhiwei Zhang , Yangfan He , Rongchao Zhang , Jinbin Bai , Shuo Cao , Bin Fu , Junjun He , Yihao Liu , Yuewen Cao , Xiaohong Liu

3D object detection is a core component of automated driving systems. State-of-the-art methods fuse RGB imagery and LiDAR point cloud data frame-by-frame for 3D bounding box regression. However, frame-by-frame 3D object detection suffers…

Computer Vision and Pattern Recognition · Computer Science 2021-05-24 Emeç Erçelik , Ekim Yurtsever , Alois Knoll

The Standard Model Effective Field Theory (SMEFT) is a powerful tool to search for new physics in a model-independent way. We explore the synergies arising from different types of observables in a combined, global SMEFT fit. Specifically,…

High Energy Physics - Phenomenology · Physics 2023-07-13 Cornelius Grunwald , Gudrun Hiller , Kevin Kröninger , Lara Nollen

In this paper, we propose a $G_{L-R}\times U(1)_{L_\mu-L_\tau}$ gauge-symmetric model where $G_{L-R}$ is the left-right gauge symmetry and $L_i$ is the $i-$flavor lepton number. We use the spontaneous breaking (SSB) of $U(1)_{L_\mu-L_\tau}$…

High Energy Physics - Phenomenology · Physics 2018-01-31 Abhish Dev

A global fit to quark flavour-physics data disfavours the Standard Model with 3.6 standard deviations and points towards new CP-violating physics in meson-antimeson mixing amplitudes. Tevatron data call for a new Bs-Bs-bar mixing phase and…

High Energy Physics - Phenomenology · Physics 2011-07-05 Ulrich Nierste

In this paper, we give a model for understanding flavor physics in the lepton sector--mass hierarchy among different generations and neutrino mixing pattern. The model is constructed in the framework of supersymmetry, with a family symmetry…

High Energy Physics - Phenomenology · Physics 2012-12-03 Zhen-hua Zhao

Objective: Time-domain diffuse optical imaging (DOI) requires accurate forward models for photon propagation in scattering media. However, existing simulators lack comprehensive experimental validation, especially for non-contact…

In view of the recent neutrino oscillation data pointing to a non-vanishing value for the smallest mixing angle ($\theta_z$), we derive and find explicit realizations of the $(Z_2)^3$ flavor symmetry which characterizes, for the neutrino…

High Energy Physics - Phenomenology · Physics 2013-05-30 E. I. Lashin , M. Abbas , N. Chamoun , S. Nasri

We study the possibility of generating deviations from tri-bimaximal (TBM) neutrino mixing to explain the non-zero reactor mixing angle within the framework of both type I and type II seesaw mechanisms. The type I seesaw term gives rise to…

High Energy Physics - Phenomenology · Physics 2013-09-24 Debasish Borah

This study examines the precise measurement of the largest leptonic mixing angle $\theta_{23}$ through the analysis of neutrino oscillation data samples. Our findings indicate that, contrary to common understanding, the…

High Energy Physics - Phenomenology · Physics 2025-03-05 P. T. Quyen , Son Cao , N. T. Hong Van

We present a Froggatt-Nielsen flavor model that yields a minimal realization of the type-I seesaw mechanism. This seesaw model is minimal for three reasons: (i) It features only two rather than three right-handed sterile neutrinos: N_1 and…

High Energy Physics - Phenomenology · Physics 2016-12-30 Thomas Rink , Kai Schmitz , Tsutomu T. Yanagida

We present the first complete model of the Littlest Modular Seesaw, based on two right-handed neutrinos, within the framework of multiple modular symmetries, justifying the use of multiple moduli fields which take their values at 3 specific…

High Energy Physics - Phenomenology · Physics 2023-03-01 Ivo de Medeiros Varzielas , Steve F. King , Miguel Levy

We propose a simplified version of the inverse seesaw model, in which only two pairs of the gauge-singlet neutrinos are introduced, to interpret the observed neutrino mass hierarchy and lepton flavor mixing at or below the TeV scale. This…

High Energy Physics - Phenomenology · Physics 2009-09-28 Michal Malinsky , Tommy Ohlsson , Zhi-zhong Xing , He Zhang

Using the result of the three flavor analysis of the old Kamiokande data, the recent Superkamiokande data of atmospheric neutrinos and the CHOOZ reactor data, it is shown that the third mixing angle $\theta_{13}$ is small. It is proposed to…

High Energy Physics - Phenomenology · Physics 2011-04-15 Osamu Yasuda
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