Jonathon Coleman
University of Liverpool
H-index: 135
Europe-United Kingdom
About Jonathon Coleman
Jonathon Coleman, With an exceptional h-index of 135 and a recent h-index of 59 (since 2020), a distinguished researcher at University of Liverpool, specializes in the field of Physics.
His recent articles reflect a diverse array of research interests and contributions to the field:
Scintillator ageing of the T2K near detectors from 2010 to 2021
Supernova Model Discrimination with Hyper-Kamiokande
Precision measurement of the ratio
Proposal for A Water Cherenkov Test Beam Experiment for Hyper-Kamiokande andFuture Large-scale Water-based Detectors
AEDGE: Atomic Experiment for Dark Matter and Gravity Exploration in Space
Measurements of and charged-current cross-sections without detected pions nor protons on water and hydrocarbon at mean antineutrino energy of 0.86 …
A simple method for estimating the major nuclide fractional fission rates within light water and advanced gas cooled reactors
The Hyper-Kamiokande Experiment--Snowmass LOI
Jonathon Coleman Information
University | University of Liverpool |
|---|---|
Position | ___ |
Citations(all) | 70546 |
Citations(since 2020) | 19225 |
Cited By | 57972 |
hIndex(all) | 135 |
hIndex(since 2020) | 59 |
i10Index(all) | 536 |
i10Index(since 2020) | 307 |
University Profile Page | University of Liverpool |
Jonathon Coleman Skills & Research Interests
Physics
Top articles of Jonathon Coleman
Scintillator ageing of the T2K near detectors from 2010 to 2021
Authors
K Abe,N Akhlaq,R Akutsu,A Ali,C Alt,C Andreopoulos,M Antonova,S Aoki,T Arihara,Y Asada,Y Ashida,ET Atkin,S Ban,M Barbi,GJ 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,SB Boyd,A Bravar,C Bronner,S Bron,A Bubak,M Buizza Avanzini,NF Calabria,S Cao,AJ Carter,SL Cartwright,MG Catanesi,A Cervera,J Chakrani,D Cherdack,G Christodoulou,M Cicerchia,J Coleman,G Collazuol,L Cook,A Cudd,Yu I Davydov,A De Roeck,G De Rosa,T Dealtry,CC Delogu,C Densham,A Dergacheva,F Di Lodovico,S Dolan,D Douqa,TA Doyle,O Drapier,KE Duffy,J Dumarchez,P Dunne,K Dygnarowicz,A Eguchi,S Emery-Schrenk,A Ershova,S Fedotov,P Fernandez,AJ Finch,GA Fiorentini Aguirre,G Fiorillo,M Friend,Y Fujii,Y Fukuda,K Fusshoeller,C Giganti,V Glagolev,M Gonin,EAG Goodman,A Gorin,M Grassi,M Guigue,DR Hadley,JT Haigh,P Hamacher-Baumann,DA Harris,M Hartz,T Hasegawa,S Hassani,NC Hastings,A Hatzikoutelis,Y Hayato,A Hiramoto,M Hogan,J Holeczek,A Holin,TJ Holvey,NT Hong Van,T Honjo,F Iacob,AK Ichikawa,M Ikeda,T Ishida,M Ishitsuka,HT Israel,SJ Ives,K Iwamoto,A Izmaylov,N Izumi,M Jakkapu,B Jamieson,SJ Jenkins,C Jesús-Valls,JJ Jiang,P Jonsson,CK Jung,PB Jurj,M Kabirnezhad,AC Kaboth,T Kajita,H Kakuno,J Kameda,SP Kasetti,Y Kataoka,Y Katayama,T Katori,M Kawaue,E Kearns,M Khabibullin,A Khotjantsev,T Kikawa,H Kikutani,S King,J Kisiel,A Knight,T Kobata,T Kobayashi,L Koch,G Kogan,A Konaka,LL Kormos,Y Koshio,A Kostin,K Kowalik,Y Kudenko,S Kuribayashi,R Kurjata,T Kutter,M Kuze,M La Commara
Journal
Journal of Instrumentation
Published Date
2022/10/17
T2K (Tokai-to-Kamioka) is a long-baseline neutrino oscillation experiment [1] located in Japan, measuring muon (anti-) neutrino disappearance and electron (anti-) neutrino appearance from a muon (anti-) neutrino beam produced by the J-PARC (Japan Proton Accelerator Research Complex) synchrotron [2]. The experiment consists of a far detector at a distance of 295 km from J-PARC, a near detector complex 280 m downstream of the proton beam target, and the beam facility itself. The far detector is Super-Kamiokande [3], a 50 kt water Cherenkov detector positioned 2.5◦ off the beam axis. The near detector complex contains the ND280 [4] and INGRID [5] detectors which started operation in 2010. In addition, WAGASCI-BabyMIND [6, 7] was installed in 2019. INGRID is located directly on the beam axis, while the ND280 is situated at the same off-axis angle as Super-Kamiokande. ND280 measures the rate of …
Supernova Model Discrimination with Hyper-Kamiokande
Authors
Ko Abe,P Adrich,H Aihara,R Akutsu,I Alekseev,A Ali,F Ameli,I Anghel,LHV Anthony,M Antonova,A Araya,Y Asaoka,Y Ashida,V Aushev,F Ballester,I Bandac,M Barbi,GJ Barker,G Barr,M Batkiewicz-Kwasniak,M Bellato,V Berardi,M Bergevin,L Bernard,E Bernardini,L Berns,S Bhadra,J Bian,A Blanchet,F d M Blaszczyk,A Blondel,A Boiano,S Bolognesi,L Bonavera,N Booth,S Borjabad,T Boschi,D Bose,SB Boyd,C Bozza,A Bravar,D Bravo-Berguño,C Bronner,L Brown,A Bubak,A Buchowicz,M Buizza Avanzini,FS Cafagna,NF Calabria,JM Calvo-Mozota,S Cao,SL Cartwright,A Carroll,MG Catanesi,S Cebriàn,M Chabera,S Chakraborty,C Checchia,JH Choi,S Choubey,M Cicerchia,J Coleman,G Collazuol,L Cook,G Cowan,S Cuen-Rochin,M Danilov,G Díaz López,E De la Fuente,P De Perio,G De Rosa,T Dealtry,CJ Densham,A Dergacheva,N Deshmukh,MM Devi,F Di Lodovico,P Di Meo,I Di Palma,TA Doyle,E Drakopoulou,O Drapier,J Dumarchez,P Dunne,M Dziewiecki,L Eklund,S El Hedri,J Ellis,S Emery,A Esmaili,R Esteve,A Evangelisti,M Feely,S Fedotov,J Feng,P Fernandez,E Fernández-Martinez,P Ferrario,B Ferrazzi,T Feusels,A Finch,C Finley,A Fiorentini,G Fiorillo,M Fitton,K Frankiewicz,M Friend,Y Fujii,Y Fukuda,G Galinski,J Gao,C Garde,A Garfagnini,S Garode,L Gialanella,C Giganti,JJ Gomez-Cadenas,M Gonin,J González-Nuevo,A Gorin,R Gornea,V Gousy-Leblanc,F Gramegna,M Grassi,G Grella,M Guigue,P Gumplinger,DR Hadley,M Harada,B Hartfiel,M Hartz,S Hassani,NC Hastings,Y Hayato,JA Hernando-Morata,V Herrero,J Hill,K Hiraide,S Hirota,A Holin,S Horiuchi,K Hoshina,K Hultqvist,F Iacob,AK Ichikawa,W Idrissi Ibnsalih,T Iijima,M Ikeda,M Inomoto,K Inoue
Journal
The Astrophysical Journal
Published Date
2021/7/20
Core-collapse supernovae are among the most magnificent events in the observable universe. They produce many of the chemical elements necessary for life to exist and their remnants—neutron stars and black holes—are interesting astrophysical objects in their own right. However, despite millennia of observations and almost a century of astrophysical study, the explosion mechanism of core-collapse supernovae is not yet well understood. Hyper-Kamiokande is a next-generation neutrino detector that will be able to observe the neutrino flux from the next galactic core-collapse supernova in unprecedented detail. We focus on the first 500 ms of the neutrino burst, corresponding to the accretion phase, and use a newly-developed, high-precision supernova event generator to simulate Hyper-Kamiokandeʼs response to five different supernova models. We show that Hyper-Kamiokande will be able to distinguish …
Precision measurement of the ratio
Authors
JP Lees,V Poireau,V Tisserand,E Grauges,A Palano,G Eigen,David Nathan Brown,Yu G Kolomensky,M Fritsch,H Koch,T Schroeder,R Cheaib,C Hearty,TS Mattison,JA McKenna,RY So,VE Blinov,AR Buzykaev,VP Druzhinin,VB Golubev,EA Kozyrev,EA Kravchenko,AP Onuchin,SI Serednyakov,Yu I Skovpen,EP Solodov,K Yu Todyshev,AJ Lankford,B Dey,JW Gary,O Long,AM Eisner,WS Lockman,W Panduro Vazquez,DS Chao,CH Cheng,B Echenard,KT Flood,DG Hitlin,J Kim,Y Li,DX Lin,TS Miyashita,P Ongmongkolkul,J Oyang,FC Porter,M Röhrken,Z Huard,BT Meadows,BG Pushpawela,MD Sokoloff,L Sun,JG Smith,SR Wagner,D Bernard,M Verderi,D Bettoni,C Bozzi,R Calabrese,G Cibinetto,E Fioravanti,I Garzia,E Luppi,V Santoro,A Calcaterra,R de Sangro,G Finocchiaro,S Martellotti,P Patteri,IM Peruzzi,M Piccolo,M Rotondo,A Zallo,S Passaggio,C Patrignani,BJ Shuve,HM Lacker,B Bhuyan,U Mallik,C Chen,J Cochran,S Prell,AV Gritsan,N Arnaud,M Davier,F Le Diberder,AM Lutz,G Wormser,DJ Lange,DM Wright,JP Coleman,E Gabathuler,DE Hutchcroft,DJ Payne,C Touramanis,AJ Bevan,F Di Lodovico,R Sacco,G Cowan,Sw Banerjee,CL Davis,AG Denig,W Gradl,K Griessinger,A Hafner,KR Schubert,RJ Barlow,GD Lafferty,R Cenci,A Jawahery,DA Roberts,R Cowan,SH Robertson,RM Seddon,N Neri,F Palombo,L Cremaldi,R Godang,DJ Summers,P Taras,G De Nardo,C Sciacca,G Raven,CP Jessop,JM LoSecco,K Honscheid,R Kass,A Gaz,M Margoni,M Posocco,G Simi,F Simonetto,R Stroili,S Akar,E Ben-Haim,M Bomben,GR Bonneaud,G Calderini,J Chauveau,G Marchiori,J Ocariz,M Biasini,E Manoni,A Rossi,G Batignani,S Bettarini,M Carpinelli,G Casarosa,M Chrzaszcz,F Forti
Journal
arXiv preprint arXiv:2005.01230
Published Date
2020/5/4
We report on a precision measurement of the ratio ${\cal R}_{\tau\mu}^{\Upsilon(3S)} = {\cal B}(\Upsilon(3S)\to\tau^+\tau^-)/{\cal B}(\Upsilon(3S)\to\mu^+\mu^-)$ using data collected with the BaBar detector at the SLAC PEP-II collider. The measurement is based on a 28 fb data sample collected at a center-of-mass energy of 10.355 GeV corresponding to a sample of 122 million mesons. The ratio is measured to be and is in agreement with the Standard Model prediction of 0.9948 within 2 standard deviations. The uncertainty in is almost an order of magnitude smaller than the only previous measurement.
Proposal for A Water Cherenkov Test Beam Experiment for Hyper-Kamiokande andFuture Large-scale Water-based Detectors
Authors
M Barbi,S Bhadra,SS Chinchanikar,L Ludovici,M Scott,KEI Fransson,M Wascko,G Collazuol,P Paganini,N McCauley,C Vilela,M Ziembicki,W Obrebski,C Garde,A Khotjantsev,J Walker,SH Seo,P de Perio,J Holeczek,T Nakadaira,M Hartz,LL Kormos,Y Zou,A Buchowicz,M Guigue,A Miyazaki,M Ishitsuka,M Buizza Avanzini,E O'Sullivan,T Lindner,PJ Rajda,J Coleman,T Dealtry,R Kurjata,M Kuze,E Rondio,K Zaremba,Y Uchida,E de la Fuente,N Kolev,A Waldron,M Pavin,A Konaka,AC Ruggeri,U Katz,AJ Finch,C Rott,M Mezzetto,P Dunne,B Quilain,K Zietara,G Santucci,T Mueller,F Di Lodovico,R Gornea,C van Eldik,G De Rosa,T Katori,S Zsoldos,A Klekotko,S Garode,G Galinski,C Giganti,J Cederkall,N Prouse,B Jamieson,J Marzec,K Stopa,A Rychter,Y Schnellbach,J Zalipska,J Reubelt,M Ostrowski,A Bubak,MG Catanesi,V Berardi,J Lagoda,G Zarnecki,M Shinoki,D Karlen,MJ Wilking,L Stawarz,K Long,A Shaykina,G Nieradka,K Kowalik,P Jonsson,J Wilson,S Cuen-Rochin,M Suchenek,T Ishida,HM O'Keeffe,M Olvegård,P Mijakowski,J Kisiel,S Boyd,C Metelko,N Yershov,A Ioannisyan,C Riccio,Y Kudenko,M Gonin,T Ekelof,M Posiadala-Zezula,A Longhin,K Porwit,O Drapier,S Suvorov,G Pastuszak,B Richards
Published Date
2020/3/9
Here we propose a 50 ton scale Water Cherenkov test experiment (WCTE) to be deployed in an East Area test beam line. The experiment will include a secondary target located just upstream of the experiment in order to produce very low energy particle fluxes, including charged pions. The WCTE program will be carried out with the following objectives. We will operate and understand the performance of new detector technologies such as multi-PMTs, and in a possible future phase, dichroicon wavelength-separating cones and water-based liquid scintillator in a fully integrated detector. We will study the performance of a< 1 kiloton scale water Cherenkov detector with known particle fluxes, and test and develop calibration systems necessary for accurate modeling of a detector of this size. We will measure important physics processes for the modeling of water Cherenkov detector responses, including high-angle Cherenkov light production, pion scattering and absorption, and secondary neutron production in hadron scattering. We aim to start operation of the water Cherenkov test experiment in 2022.
AEDGE: Atomic Experiment for Dark Matter and Gravity Exploration in Space
Authors
Yousef Abou El-Neaj,Cristiano Alpigiani,Sana Amairi-Pyka,Henrique Araújo,Antun Balaž,Angelo Bassi,Lars Bathe-Peters,Baptiste Battelier,Aleksandar Belić,Elliot Bentine,José Bernabeu,Andrea Bertoldi,Robert Bingham,Diego Blas,Vasiliki Bolpasi,Kai Bongs,Sougato Bose,Philippe Bouyer,Themis Bowcock,William Bowden,Oliver Buchmueller,Clare Burrage,Xavier Calmet,Benjamin Canuel,Laurentiu-Ioan Caramete,Andrew Carroll,Giancarlo Cella,Vassilis Charmandaris,Swapan Chattopadhyay,Xuzong Chen,Maria Luisa Chiofalo,Jonathon Coleman,Joseph Cotter,Yanou Cui,Andrei Derevianko,Albert De Roeck,Goran S Djordjevic,Peter Dornan,Michael Doser,Ioannis Drougkakis,Jacob Dunningham,Ioana Dutan,Sajan Easo,Gedminas Elertas,John Ellis,Mai El Sawy,Farida Fassi,Daniel Felea,Chen-Hao Feng,Robert Flack,Chris Foot,Ivette Fuentes,Naceur Gaaloul,Alexandre Gauguet,Remi Geiger,Valerie Gibson,Gian Giudice,Jon Goldwin,Oleg Grachov,Peter W Graham,Dario Grasso,Maurits Van der Grinten,Mustafa Gündogan,Martin G Haehnelt,Tiffany Harte,Aurélien Hees,Richard Hobson,Jason Hogan,Bodil Holst,Michael Holynski,Mark Kasevich,Bradley J Kavanagh,Wolf Von Klitzing,Tim Kovachy,Benjamin Krikler,Markus Krutzik,Marek Lewicki,Yu-Hung Lien,Miaoyuan Liu,Giuseppe Gaetano Luciano,Alain Magnon,Mohammed Attia Mahmoud,Sarah Malik,Christopher McCabe,Jeremiah Mitchell,Julia Pahl,Debapriya Pal,Saurabh Pandey,Dimitris Papazoglou,Mauro Paternostro,Bjoern Penning,Achim Peters,Marco Prevedelli,Vishnupriya Puthiya-Veettil,John Quenby,Ernst Rasel,Sean Ravenhall,Jack Ringwood,Albert Roura,Dylan Sabulsky,Muhammed Sameed,Ben Sauer,Stefan Alaric Schäffer,Stephan Schiller,Vladimir Schkolnik,Dennis Schlippert,Christian Schubert,Haifa Rejeb Sfar,Armin Shayeghi,Ian Shipsey,Carla Signorini,Yeshpal Singh,Marcelle Soares-Santos,Fiodor Sorrentino,Timothy Sumner,Konstantinos Tassis,Silvia Tentindo,Guglielmo Maria Tino,Jonathan N Tinsley,James Unwin,Tristan Valenzuela,Georgios Vasilakis,Ville Vaskonen,Christian Vogt,Alex Webber-Date,André Wenzlawski,Patrick Windpassinger,Marian Woltmann,Efe Yazgan,Ming-Sheng Zhan,Xinhao Zou,Jure Zupan
Published Date
2020/12
We propose in this White Paper a concept for a space experiment using cold atoms to search for ultra-light dark matter, and to detect gravitational waves in the frequency range between the most sensitive ranges of LISA and the terrestrial LIGO/Virgo/KAGRA/INDIGO experiments. This interdisciplinary experiment, called Atomic Experiment for Dark Matter and Gravity Exploration (AEDGE), will also complement other planned searches for dark matter, and exploit synergies with other gravitational wave detectors. We give examples of the extended range of sensitivity to ultra-light dark matter offered by AEDGE, and how its gravitational-wave measurements could explore the assembly of super-massive black holes, first-order phase transitions in the early universe and cosmic strings. AEDGE will be based upon technologies now being developed for terrestrial experiments using cold atoms, and will benefit from the space …
Measurements of and charged-current cross-sections without detected pions nor protons on water and hydrocarbon at mean antineutrino energy of 0.86 …
Authors
K Abe,N Akhlaq,R Akutsu,A Ali,C Alt,C Andreopoulos,L Anthony,M Antonova,S Aoki,A Ariga,T Arihara,Y Asada,Y Ashida,ET Atkin,Y Awataguchi,S Ban,M Barbi,GJ Barker,G Barr,D Barrow,C Barry,M Batkiewicz-Kwasniak,A Beloshapkin,F Bench,V Berardi,S Berkman,L Berns,S Bhadra,S Bienstock,A Blondel,S Bolognesi,T Bonus,B Bourguille,SB Boyd,D Brailsford,A Bravar,D Bravo Berguño,C Bronner,S Bron,A Bubak,M Buizza Avanzini,J Calcutt,T Campbell,S Cao,SL Cartwright,MG Catanesi,A Cervera,A Chappell,C Checchia,D Cherdack,N Chikuma,G Christodoulou,M Cicerchia,J Coleman,G Collazuol,L Cook,D Coplowe,A Cudd,A Dabrowska,G De Rosa,T Dealtry,PF Denner,SR Dennis,C Densham,F Di Lodovico,N Dokania,S Dolan,TA Doyle,O Drapier,J Dumarchez,P Dunne,A Eguchi,L Eklund,S Emery-Schrenk,A Ereditato,P Fernandez,T Feusels,AJ Finch,GA Fiorentini,G Fiorillo,C Francois,M Friend,Y Fujii,R Fujita,D Fukuda,R Fukuda,Y Fukuda,K Fusshoeller,K Gameil,C Giganti,T Golan,M Gonin,A Gorin,M Guigue,DR Hadley,JT Haigh,P Hamacher-Baumann,M Hartz,T Hasegawa,S Hassani
Journal
arXiv preprint arXiv:2004.13989
Published Date
2020/4/29
We report measurements of the flux-integrated and charged-current cross-sections on water and hydrocarbon targets using the T2K anti-neutrino beam with a mean beam energy of 0.86 GeV. The signal is defined as the (anti-)neutrino charged-current interaction with one induced and no detected charged pion or proton. These measurements are performed using a new WAGASCI module recently added to the T2K setup in combination with the INGRID Proton Module. The phase space of muons is restricted to the high-detection efficiency region, and , in the laboratory frame. An absence of pions and protons in the detectable phase spaces of , and , is required. In this paper, both the cross-sections and cross-sections on water and hydrocarbon targets and their ratios are provided by using the D’Agostini unfolding method. The results of the integrated cross-section measurements over this phase space are $\sigma_{\rm H_{2}O}=(1.082\pm0.068(\rm stat.)^{+0.145}_{-0.128}(\rm syst.)) \times 10^{-39}\,{\rm cm^{2} / nucleon}$, $\sigma_{\rm CH}=(1.096\pm0.054(\rm stat.)^{+0.132}_{-0.117}(\rm syst.)) \times 10^{-39}\,{\rm cm^{2} / nucleon}$, and . The cross-section is $\sigma_{\rm H_{2}O} = (1.155\pm0.064(\rm stat.)^{+0.148}_{-0.129}(\rm syst.)) \times 10^{-39}\,{\rm cm^{2} / nucleon}$, $\sigma_{\rm CH}=(1.159\pm0.049(\rm stat.)^{+0.129}_{-0.115}(\rm syst.)) \times 10^{-39}\,{\rm cm^{2} / nucleon}$, and .
A simple method for estimating the major nuclide fractional fission rates within light water and advanced gas cooled reactors
Authors
RW Mills,BM Slingsby,J Coleman,R Collins,G Holt,C Metelko,Y Schnellbach
Journal
Nuclear Engineering and Technology
Published Date
2020/3/7
The standard method for calculating anti-neutrino emissions from a reactor involves knowing the fractional fission rates for the most important fissioning nuclides in the reactor. To calculate these rates requires detailed reactor physics calculations based upon the reactor design, fuel design, burnup dependent fuel composition, location of specific fuel assemblies in the core and detailed operational data from the reactor. This has only been published for a few reactors during specific time periods, whereas to be of practical use for anti-neutrino reactor monitoring it is necessary to be able to predict these on the publicly available information from any reactor, especially if using these data to subtract the anti-neutrino signal from other reactors to identify an undeclared reactor and monitor its operation. This paper proposes a method to estimate the fission fractions for a specific reactor based upon publicly available …
The Hyper-Kamiokande Experiment--Snowmass LOI
Authors
K Abe,P Adrich,H Aihara,R Akutsu,I Alekseev,A Ali,F Ameli,LHV Anthony,A Araya,Y Asaoka,V Aushev,I Bandac,M Barbi,G Barr,M Batkiewicz-Kwasniak,M Bellato,V Berardi,L Bernard,E Bernardini,L Berns,S Bhadra,J Bian,A Blanchet,A Blondel,A Boiano,S Bolognesi,L Bonavera,S Borjabad,T Boschi,D Bose,SB Boyd,C Bozza,A Bravar,C Bronner,A Bubak,A Buchowicz,M Buizza Avanzini,FS Cafagna,NF Calabria,JM Calvo-Mozota,S Cao,MG Catanesi,S Chakraborty,JH Choi,S Choubey,M Cicerchia,J Coleman,G Collazuol,S Cuen-Rochin,M Danilov,E De la Fuente,P de Perio,G De Rosa,T Dealtry,CJ Densham,A Dergacheva,N Deshmukh,MM Devi,F Di Lodovico,P Di Meo,I Di Palma,TA Doyle,E Drakopoulou,O Drapier,J Dumarchez,L Eklund,S El Hedri,J Ellis,S Emery,A Esmaili,S Fedotov,J Feng,E Fernández-Martinez,P Ferrario,B Ferrazzi,A Finch,C Finley,G Fiorillo,M Fitton,M Friend,Y Fujii,Y Fukuda,G Galinski,J Gao,C Garde,A Garfagnini,S Garode,L Gialanella,C Giganti,JJ Gomez-Cadenas,M Gonin,J González-Nuevo,A Gorin,R Gornea,F Gramegna,M Grassi,G Grella,M Guigue,DR Hadley,M Harada,M Hartz,S Hassani,NC Hastings,Y Hayato,K Hiraide,K Hoshina,K Hultqvist,F Iacob,AK Ichikawa,W Idrissi Ibnsalih,M Ikeda,M Inomoto,A Ioannisian,T Ishida,K Ishidoshiro,H Ishino,M Ishitsuka,H Ito,S Ito,Y Itow,K Iwamoto,N Izumi,S Izumiyama,M Jakkapu,B Jamieson,JS Jang,HS Jo,P Jonsson,KK Joo,T Kajita,H Kakuno,J Kameda,Y Kano,D Karlen,Y Kataoka,A Kato,T Katori,N Kazarian,M Khabibullin,A Khotjantsev,T Kikawa,JY Kim,SB Kim,S King,T Kinoshita,J Kisiel,A Klekotko,T Kobayashi,L Koerich,N Kolev
Journal
arXiv preprint arXiv:2009.00794
Published Date
2020/9/2
Hyper-Kamiokande is the next generation underground water Cherenkov detector that builds on the highly successful Super-Kamiokande experiment. The detector which has an 8.4~times larger effective volume than its predecessor will be located along the T2K neutrino beamline and utilize an upgraded J-PARC beam with 2.6~times beam power. Hyper-K's low energy threshold combined with the very large fiducial volume make the detector unique, that is expected to acquire an unprecedented exposure of 3.8~Mtonyear over a period of 20~years of operation. Hyper-Kamiokande combines an extremely diverse science program including nucleon decays, long-baseline neutrino oscillations, atmospheric neutrinos, and neutrinos from astrophysical origins. The scientific scope of this program is highly complementary to liquid-argon detectors for example in sensitivity to nucleon decay channels or supernova detection modes. Hyper-Kamiokande construction has started in early 2020 and the experiment is expected to start operations in 2027. The Hyper-Kamiokande collaboration is presently being formed amongst groups from 19 countries including the United States, whose community has a long history of making significant contributions to the neutrino physics program in Japan. US physicists have played leading roles in the Kamiokande, Super-Kamiokande, EGADS, K2K, and T2K programs.
Search for electron antineutrino appearance in a long-baseline muon antineutrino beam
Authors
K Abe,R Akutsu,A Ali,C Alt,C Andreopoulos,L Anthony,M Antonova,S Aoki,A Ariga,Y Asada,Y Ashida,ET Atkin,Y Awataguchi,S Ban,M Barbi,GJ Barker,G Barr,D Barrow,C Barry,M Batkiewicz-Kwasniak,A Beloshapkin,F Bench,V Berardi,S Berkman,L Berns,S Bhadra,S Bienstock,A Blondel,S Bolognesi,B Bourguille,SB Boyd,D Brailsford,A Bravar,D Bravo Berguño,C Bronner,A Bubak,M Buizza Avanzini,J Calcutt,T Campbell,S Cao,SL Cartwright,MG Catanesi,A Cervera,A Chappell,C Checchia,D Cherdack,N Chikuma,G Christodoulou,J Coleman,G Collazuol,L Cook,D Coplowe,A Cudd,A Dabrowska,G De Rosa,T Dealtry,PF Denner,SR Dennis,C Densham,F Di Lodovico,N Dokania,S Dolan,TA Doyle,O Drapier,J Dumarchez,P Dunne,L Eklund,S Emery-Schrenk,A Ereditato,P Fernandez,T Feusels,AJ Finch,GA Fiorentini,G Fiorillo,C Francois,M Friend,Y Fujii,R Fujita,D Fukuda,R Fukuda,Y Fukuda,K Fusshoeller,K Gameil,C Giganti,T Golan,M Gonin,A Gorin,M Guigue,DR Hadley,JT Haigh,P Hamacher-Baumann,M Hartz,T Hasegawa,NC Hastings,T Hayashino,Y Hayato,A Hiramoto,M Hogan,J Holeczek,NT Hong Van,F Iacob,AK Ichikawa,M Ikeda,T Ishida,T Ishii,M Ishitsuka,K Iwamoto,A Izmaylov,M Jakkapu,B Jamieson,SJ Jenkins,C Jesús-Valls,M Jiang,S Johnson,P Jonsson,CK Jung,M Kabirnezhad,AC Kaboth,T Kajita,H Kakuno,J Kameda,D Karlen,SP Kasetti,Y Kataoka,T Katori,Y Kato,E Kearns,M Khabibullin,A Khotjantsev,T Kikawa,H Kim,J Kim,S King,J Kisiel,A Knight,A Knox,T Kobayashi,L Koch,T Koga,A Konaka,LL Kormos,Y Koshio,A Kostin,K Kowalik,H Kubo,Y Kudenko,N Kukita,S Kuribayashi,R Kurjata,T Kutter
Journal
Physical review letters
Published Date
2020/4/21
Electron antineutrino appearance is measured by the T2K experiment in an accelerator-produced antineutrino beam, using additional neutrino beam operation to constrain parameters of the Pontecorvo-Maki-Nakagawa-Sakata (PMNS) mixing matrix. T2K observes 15 candidate electron antineutrino events with a background expectation of 9.3 events. Including information from the kinematic distribution of observed events, the hypothesis of no electron antineutrino appearance is disfavored with a significance of 2.40 σ and no discrepancy between data and PMNS predictions is found. A complementary analysis that introduces an additional free parameter which allows non-PMNS values of electron neutrino and antineutrino appearance also finds no discrepancy between data and PMNS predictions.
Measurement of the charged-current electron (anti-) neutrino inclusive cross-sections at the T2K off-axis near detector ND280
Authors
K Abe,N Akhlaq,R Akutsu,A Ali,C Alt,C Andreopoulos,L Anthony,M Antonova,S Aoki,A Ariga,T Arihara,Y Asada,Y Ashida,ET Atkin,Y Awataguchi,S Ban,M Barbi,GJ Barker,G Barr,D Barrow,C Barry,M Batkiewicz-Kwasniak,A Beloshapkin,F Bench,V Berardi,L Berns,S Bhadra,S Bienstock,A Blondel,S Bolognesi,T Bonus,B Bourguille,SB Boyd,D Brailsford,A Bravar,D Bravo Berguño,C Bronner,S Bron,A Bubak,M Buizza Avanzini,J Calcutt,T Campbell,S Cao,SL Cartwright,MG Catanesi,A Cervera,A Chappell,C Checchia,D Cherdack,N Chikuma,G Christodoulou,M Cicerchia,J Coleman,G Collazuol,L Cook,D Coplowe,A Cudd,A Dabrowska,G De Rosa,T Dealtry,PF Denner,SR Dennis,C Densham,F Di Lodovico,N Dokania,S Dolan,TA Doyle,O Drapier,J Dumarchez,P Dunne,A Eguchi,L Eklund,S Emery-Schrenk,A Ereditato,P Fernandez,T Feusels,AJ Finch,GA Fiorentini,G Fiorillo,C Francois,M Friend,Y Fujii,R Fujita,D Fukuda,R Fukuda,Y Fukuda,K Fusshoeller,C Giganti,T Golan,M Gonin,A Gorin,M Guigue,DR Hadley,JT Haigh,P Hamacher-Baumann,M Hartz,T Hasegawa,S Hassani,NC Hastings,T Hayashino,Y Hayato,A Hiramoto,M Hogan,J Holeczek,NT Hong Van,T Honjo,F Iacob,AK Ichikawa,M Ikeda,T Ishida,T Ishii,M Ishitsuka,K Iwamoto,A Izmaylov,N Izumi,M Jakkapu,B Jamieson,SJ Jenkins,C Jesús-Valls,M Jiang,S Johnson,P Jonsson,CK Jung,X Junjie,PB Jurj,M Kabirnezhad,AC Kaboth,T Kajita,H Kakuno,J Kameda,D Karlen,SP Kasetti,Y Kataoka,Y Katayama,T Katori,Y Kato,E Kearns,M Khabibullin,A Khotjantsev,T Kikawa,H Kikutani,H Kim,S King,J Kisiel,A Knight,A Knox,T Kobata,T Kobayashi,L Koch,T Koga
Journal
Journal of High Energy Physics
Published Date
2020/10
The electron (anti-) neutrino component of the T2K neutrino beam constitutes the largest background in the measurement of electron (anti-) neutrino appearance at the far detector. The electron neutrino scattering is measured directly with the T2K off-axis near detector, ND280. The selection of the electron (anti-) neutrino events in the plastic scintillator target from both neutrino and anti-neutrino mode beams is discussed in this paper. The flux integrated single differential charged-current inclusive electron (anti-) neutrino cross-sections, dσ/dp and dσ/d cos (θ), and the total cross-sections in a limited phase-space in momentum and scattering angle (p> 300 MeV/c and θ≤ 45) are measured using a binned maximum likelihood fit and compared to the neutrino Monte Carlo generator predictions, resulting in good agreement.
Search for lepton-flavor-violating decays
Authors
Roel Aaij,C Abellan Beteta,T Ackernley,B Adeva,M Adinolfi,CA Aidala,Z Ajaltouni,S Akar,P Albicocco,J Albrecht,F Alessio,M Alexander,A Alfonso Albero,G Alkhazov,P Alvarez Cartelle,AA Alves Jr,S Amato,Y Amhis,L An,L Anderlini,G Andreassi,M Andreotti,JE Andrews,F Archilli,P d’Argent,J Arnau Romeu,A Artamonov,M Artuso,K Arzymatov,E Aslanides,M Atzeni,B Audurier,S Bachmann,JJ Back,S Baker,V Balagura,W Baldini,A Baranov,RJ Barlow,S Barsuk,W Barter,M Bartolini,F Baryshnikov,V Batozskaya,B Batsukh,A Battig,V Battista,A Bay,M Becker,F Bedeschi,I Bediaga,A Beiter,LJ Bel,V Belavin,S Belin,N Beliy,V Bellee,K Belous,I Belyaev,E Ben-Haim,G Bencivenni,S Benson,S Beranek,A Berezhnoy,R Bernet,D Berninghoff,E Bertholet,A Bertolin,C Betancourt,F Betti,MO Bettler,M Van Beuzekom,Ia Bezshyiko,S Bhasin,J Bhom,MS Bieker,S Bifani,P Billoir,A Birnkraut,A Bizzeti,M Bjørn,MP Blago,T Blake,F Blanc,S Blusk,D Bobulska,V Bocci,O Boente Garcia,T Boettcher,A Boldyrev,A Bondar,N Bondar,S Borghi,M Borisyak,M Borsato,JT Borsuk,M Boubdir,TJV Bowcock,C Bozzi,S Braun,A Brea Rodriguez,M Brodski,J Brodzicka,A Brossa Gonzalo,D Brundu,E Buchanan,A Buonaura,C Burr,A Bursche,JS Butter,J Buytaert,W Byczynski,S Cadeddu,H Cai,R Calabrese,S Cali,R Calladine,M Calvi,M Calvo Gomez,A Camboni,P Campana,DH Campora Perez,L Capriotti,A Carbone,G Carboni,R Cardinale,A Cardini,P Carniti,K Carvalho Akiba,A Casais Vidal,G Casse,M Cattaneo,G Cavallero,R Cenci,MG Chapman,M Charles,Ph Charpentier,G Chatzikonstantinidis,M Chefdeville,V Chekalina,C Chen,S Chen,A Chernov,S-G Chitic,V Chobanova,M Chrzaszcz,A Chubykin,P Ciambrone,MF Cicala,X Cid Vidal
Journal
Physical review letters
Published Date
2019/12/12
A search for the lepton-flavor violating decays B+→ K+ μ±e∓ is performed using a sample of proton-proton collision data, collected with the LHCb experiment at center-of-mass energies of 7 and 8 TeV and corresponding to an integrated luminosity of 3 fb− 1. No significant signal is observed, and upper limits on the branching fractions are set as B (B+→ K+ μ− e+)< 7.0 (9.5)× 10− 9 and B (B+→ K+ μ+ e−)< 6.4 (8.8)× 10− 9 at 90%(95)% confidence level. The results improve the current best limits on these decays by more than one order of magnitude.
Search for Rare or Forbidden Decays of the Meson
Authors
JP Lees,V Poireau,V Tisserand,E Grauges,A Palano,G Eigen,David Nathan Brown,Yu G Kolomensky,M Fritsch,H Koch,T Schroeder,R Cheaib,C Hearty,TS Mattison,JA McKenna,RY So,VE Blinov,AR Buzykaev,VP Druzhinin,VB Golubev,EA Kozyrev,EA Kravchenko,AP Onuchin,SI Serednyakov,Yu I Skovpen,EP Solodov,K Yu Todyshev,AJ Lankford,B Dey,JW Gary,O Long,AM Eisner,WS Lockman,W Panduro Vazquez,DS Chao,CH Cheng,B Echenard,KT Flood,DG Hitlin,J Kim,Y Li,TS Miyashita,P Ongmongkolkul,FC Porter,M Röhrken,Z Huard,BT Meadows,BG Pushpawela,MD Sokoloff,L Sun,JG Smith,SR Wagner,D Bernard,M Verderi,D Bettoni,C Bozzi,R Calabrese,G Cibinetto,E Fioravanti,I Garzia,E Luppi,V Santoro,A Calcaterra,R de Sangro,G Finocchiaro,S Martellotti,P Patteri,IM Peruzzi,M Piccolo,M Rotondo,A Zallo,S Passaggio,C Patrignani,BJ Shuve,HM Lacker,B Bhuyan,U Mallik,C Chen,J Cochran,S Prell,AV Gritsan,N Arnaud,M Davier,F Le Diberder,AM Lutz,G Wormser,DJ Lange,DM Wright,JP Coleman,E Gabathuler,DE Hutchcroft,DJ Payne,C Touramanis,AJ Bevan,F Di Lodovico,R Sacco,G Cowan,Sw Banerjee,CL Davis,AG Denig,W Gradl,K Griessinger,A Hafner,KR Schubert,RJ Barlow,GD Lafferty,R Cenci,A Jawahery,DA Roberts,R Cowan,SH Robertson,RM Seddon,N Neri,F Palombo,L Cremaldi,R Godang,DJ Summers,P Taras,G De Nardo,C Sciacca,G Raven,CP Jessop,JM LoSecco,K Honscheid,R Kass,A Gaz,M Margoni,M Posocco,G Simi,F Simonetto,R Stroili,S Akar,E Ben-Haim,M Bomben,GR Bonneaud,G Calderini,J Chauveau,G Marchiori,J Ocariz,M Biasini,E Manoni,A Rossi,G Batignani,S Bettarini,M Carpinelli,G Casarosa,M Chrzaszcz,F Forti,MA Giorgi,A Lusiani
Journal
Physical Review Letters
Published Date
2020/2/19
We present a search for nine lepton-number-violating and three lepton-flavor-violating neutral charm decays of the type D 0→ h′− h− ℓ′+ ℓ+ and D 0→ h′− h+ ℓ′±ℓ∓, where h and h′ represent a K or π meson and ℓ and ℓ′ an electron or muon. The analysis is based on 468 fb− 1 of e+ e− annihilation data collected at or close to the ϒ (4 S) resonance with the BABAR detector at the SLAC National Accelerator Laboratory. No significant signal is observed for any of the twelve modes, and we establish 90% confidence level upper limits on the branching fractions in the range (1.0–30.6)× 10− 7. The limits are between 1 and 3 orders of magnitude more stringent than previous measurements.
Measurements of the Absolute Branching Fractions of
Authors
Medina Ablikim,Mikhail N Achasov,P Adlarson,XC Ai,Riccardo Aliberti,Antonio Amoroso,MR An,Qi An,Yu Bai,Olga Bakina,I Balossino,Y Ban,V Batozskaya,K Begzsuren,N Berger,M Berlowski,M Bertani,D Bettoni,F Bianchi,E Bianco,A Bortone,I Boyko,RA Briere,A Brueggemann,H Cai,X Cai,A Calcaterra,GF Cao,N Cao,SA Cetin,JF Chang,TT Chang,WL Chang,GR Che,C Chen,Chao Chen,G Chen,HS Chen,ML Chen,SJ Chen,SM Chen,T Chen,XR Chen,XT Chen,YB Chen,YQ Chen,ZJ Chen,WS Cheng,SK Choi,X Chu,G Cibinetto,SC Coen,F Cossio,JJ Cui,HL Dai,JP Dai,A Dbeyssi,RE de Boer,D Dedovich,ZY Deng,A Denig,I Denysenko,M Destefanis,F De Mori,B Ding,XX Ding,Y Ding,J Dong,LY Dong,MY Dong,X Dong,MC Du,SX Du,ZH Duan,P Egorov,YHY Fan,YL Fan,J Fang,SS Fang,WX Fang,Y Fang,R Farinelli,L Fava,F Feldbauer,G Felici,CQ Feng,JH Feng,K Fischer,M Fritsch,C Fritzsch,CD Fu,JL Fu,YW Fu,H Gao,YN Gao,Yang Gao,S Garbolino,I Garzia,PT Ge,ZW Ge,C Geng,EM Gersabeck,A Gilman,K Goetzen,L Gong,WX Gong,W Gradl,S Gramigna,M Greco,MH Gu,CY Guan,ZL Guan,AQ Guo,LB Guo,MJ Guo,RP Guo,YP Guo,A Guskov,TT Han,WY Han,XQ Hao,FA Harris,KK He,KL He,FHH Heinsius,CH Heinz,YK Heng,C Herold,T Holtmann,PC Hong,GY Hou,XT Hou,YR Hou,ZL Hou,HM Hu,JF Hu,T Hu,Y Hu,GS Huang,KX Huang,LQ Huang,XT Huang,YP Huang,T Hussain,N Hüsken,W Imoehl,J Jackson,S Jaeger,S Janchiv,JH Jeong
Journal
Physical Review D
Published Date
2023/11/21
Based on a dataset of (27.12±0.10)× 10 8 ψ (3686) events collected at the BESIII experiment, the absolute branching fractions of the three dominant Ω− decays are measured to be B Ω−→ Ξ 0 π−=(25.03±0.44±0.53)%, B Ω−→ Ξ− π 0=(8.43±0.52±0.28)%, and B Ω−→ Λ K−=(66.3±0.8±2.0)%, where the first and second uncertainties are statistical and systematic, respectively. The ratio between B Ω−→ Ξ 0 π− and B Ω−→ Ξ− π 0 is determined to be 2.97±0.19±0.11, which is in good agreement with the PDG value of 2.74±0.15, but greater by more than four standard deviations than the theoretical prediction of 2 obtained from the Δ I= 1/2 rule.
First combined measurement of the muon neutrino and antineutrino charged-current cross section without pions in the final state at T2K
Authors
K Abe,N Akhlaq,R Akutsu,A Ali,C Alt,C Andreopoulos,L Anthony,M Antonova,S Aoki,A Ariga,T Arihara,Y Asada,Y Ashida,ET Atkin,Y Awataguchi,S Ban,M Barbi,GJ Barker,G Barr,D Barrow,C Barry,M Batkiewicz-Kwasniak,A Beloshapkin,F Bench,V Berardi,L Berns,S Bhadra,S Bienstock,A Blondel,S Bolognesi,T Bonus,B Bourguille,SB Boyd,D Brailsford,A Bravar,D Bravo Berguño,C Bronner,S Bron,Arkadiusz Bubak,M Buizza Avanzini,J Calcutt,T Campbell,S Cao,SL Cartwright,MG Catanesi,A Cervera,A Chappell,C Checchia,D Cherdack,N Chikuma,G Christodoulou,M Cicerchia,J Coleman,G Collazuol,L Cook,D Coplowe,A Cudd,A Dabrowska,G De Rosa,T Dealtry,PF Denner,SR Dennis,C Densham,F Di Lodovico,N Dokania,S Dolan,TA Doyle,O Drapier,J Dumarchez,P Dunne,A Eguchi,L Eklund,S Emery-Schrenk,A Ereditato,P Fernandez,T Feusels,AJ Finch,GA Fiorentini,G Fiorillo,C Francois,M Friend,Y Fujii,R Fujita,D Fukuda,R Fukuda,Y Fukuda,K Fusshoeller,C Giganti,T Golan,M Gonin,A Gorin,M Guigue,DR Hadley,JT Haigh,P Hamacher-Baumann,M Hartz,T Hasegawa,S Hassani,NC Hastings,T Hayashino,Y Hayato,A Hiramoto,M Hogan,Jacek Holeczek,NT Hong Van,T Honjo,F Iacob,AK Ichikawa,M Ikeda,T Ishida,T Ishii,M Ishitsuka,K Iwamoto,A Izmaylov,N Izumi,M Jakkapu,B Jamieson,SJ Jenkins,C Jesús-Valls,M Jiang,S Johnson,P Jonsson,CK Jung,X Junjie,PB Jurj,M Kabirnezhad,AC Kaboth,T Kajita,H Kakuno,J Kameda,D Karlen,SP Kasetti,Y Kataoka,Y Katayama,T Katori,Y Kato,E Kearns,M Khabibullin,A Khotjantsev,T Kikawa,H Kikutani,H Kim,S King,Jan Kisiel,A Knight,A Knox,T Kobata,T Kobayashi,L Koch,T Koga
Journal
Physical Review D
Published Date
2020/6/2
This paper presents the first combined measurement of the double-differential muon neutrino and antineutrino charged-current cross sections with no pions in the final state on hydrocarbon at the off-axis near detector of the T2K experiment. The data analyzed in this work comprise 5.8× 10 20 and 6.3× 10 20 protons on target in neutrino and antineutrino mode respectively, at a beam energy peak of 0.6 GeV. Using the two measured cross sections, the sum, difference, and asymmetry were calculated with the aim of better understanding the nuclear effects involved in such interactions. The extracted measurements have been compared with the prediction from different Monte Carlo generators and theoretical models showing that the difference between the two cross sections have interesting sensitivity to nuclear effects.
Resonances in annihilation near 2.2 GeV
Authors
JP Lees,V Poireau,V Tisserand,E Grauges,A Palano,G Eigen,DN Brown,Yu G Kolomensky,M Fritsch,H Koch,T Schroeder,R Cheaib,C Hearty,TS Mattison,JA McKenna,RY So,VE Blinov,AR Buzykaev,VP Druzhinin,VB Golubev,EA Kozyrev,EA Kravchenko,AP Onuchin,SI Serednyakov,Yu I Skovpen,EP Solodov,K Yu Todyshev,AJ Lankford,B Dey,JW Gary,O Long,AM Eisner,WS Lockman,W Panduro Vazquez,DS Chao,CH Cheng,B Echenard,KT Flood,DG Hitlin,J Kim,Y Li,TS Miyashita,P Ongmongkolkul,FC Porter,M Röhrken,Z Huard,BT Meadows,BG Pushpawela,MD Sokoloff,L Sun,JG Smith,SR Wagner,D Bernard,M Verderi,D Bettoni,C Bozzi,R Calabrese,G Cibinetto,E Fioravanti,I Garzia,E Luppi,V Santoro,A Calcaterra,R de Sangro,G Finocchiaro,S Martellotti,P Patteri,IM Peruzzi,M Piccolo,M Rotondo,A Zallo,S Passaggio,C Patrignani,BJ Shuve,HM Lacker,B Bhuyan,U Mallik,C Chen,J Cochran,S Prell,AV Gritsan,N Arnaud,M Davier,F Le Diberder,AM Lutz,G Wormser,DJ Lange,DM Wright,JP Coleman,E Gabathuler,DE Hutchcroft,DJ Payne,C Touramanis,AJ Bevan,F Di Lodovico,R Sacco,G Cowan,Sw Banerjee,CL Davis,AG Denig,W Gradl,K Griessinger,A Hafner,KR Schubert,RJ Barlow,GD Lafferty,R Cenci,A Jawahery,DA Roberts,R Cowan,SH Robertson,RM Seddon,N Neri,F Palombo,L Cremaldi,R Godang,DJ Summers,P Taras,G De Nardo,C Sciacca,G Raven,CP Jessop,JM LoSecco,K Honscheid,R Kass,A Gaz,M Margoni,M Posocco,G Simi,F Simonetto,R Stroili,S Akar,E Ben-Haim,M Bomben,GR Bonneaud,G Calderini,J Chauveau,G Marchiori,J Ocariz,M Biasini,E Manoni,A Rossi,G Batignani,S Bettarini,M Carpinelli,G Casarosa,M Chrzaszcz,F Forti,MA Giorgi,A Lusiani
Journal
Physical Review D
Published Date
2020/1/22
Using the initial-state radiation method, the e+ e−→ K S K L cross section from 1.98 to 2.54 GeV is measured in a data sample of 469 fb− 1 collected with the BABAR detector. The results are used in conjunction with previous BABAR results for the e+ e−→ K+ K−, e+ e−→ π+ π−, e+ e−→ π+ π− η, and e+ e−→ ω π π cross sections to investigate the nature of the resonance structure recently observed by the BESIII experiment in the e+ e−→ K+ K− cross section.
AION: An atom interferometer observatory and network
Authors
L Badurina,E Bentine,Diego Blas,K Bongs,D Bortoletto,T Bowcock,K Bridges,W Bowden,O Buchmueller,C Burrage,J Coleman,G Elertas,J Ellis,C Foot,Valerie Gibson,MG Haehnelt,T Harte,S Hedges,R Hobson,M Holynski,T Jones,M Langlois,S Lellouch,M Lewicki,Roberto Maiolino,P Majewski,S Malik,J March-Russell,C McCabe,D Newbold,B Sauer,Ulrich Schneider,I Shipsey,Y Singh,MA Uchida,T Valenzuela,M van der Grinten,V Vaskonen,J Vossebeld,D Weatherill,I Wilmut
Journal
Journal of Cosmology and Astroparticle Physics
Published Date
2020/5/6
We outline the experimental concept and key scientific capabilities of AION (Atom Interferometer Observatory and Network), a proposed experimental programme using cold strontium atoms to search for ultra-light dark matter, to explore gravitational waves in the mid-frequency range between the peak sensitivities of the LISA and LIGO/Virgo/KAGRA/INDIGO/Einstein Telescope/Cosmic Explorer experiments, and to probe other frontiers in fundamental physics. AION would complement other planned searches for dark matter, as well as probe mergers involving intermediate-mass black holes and explore early-universe cosmology. AION would share many technical features with the MAGIS experimental programme, and synergies would flow from operating AION in a network with this experiment, as well as with other atom interferometer experiments such as MIGA, ZAIGA and ELGAR. Operating AION in a network with …
Simultaneous measurement of the muon neutrino charged-current cross section on oxygen and carbon without pions in the final state at T2K
Authors
K Abe,N Akhlaq,R Akutsu,A Ali,C Alt,C Andreopoulos,L Anthony,M Antonova,S Aoki,A Ariga,T Arihara,Y Asada,Y Ashida,ET Atkin,Y Awataguchi,S Ban,M Barbi,GJ Barker,G Barr,D Barrow,M Batkiewicz-Kwasniak,A Beloshapkin,F Bench,V Berardi,L Berns,S Bhadra,S Bienstock,S Bolognesi,T Bonus,B Bourguille,SB Boyd,A Bravar,D Bravo Berguño,C Bronner,S Bron,A Bubak,M Buizza Avanzini,T Campbell,S Cao,SL Cartwright,MG Catanesi,A Cervera,D Cherdack,N Chikuma,G Christodoulou,M Cicerchia,J Coleman,G Collazuol,L Cook,D Coplowe,A Cudd,A Dabrowska,G De Rosa,T Dealtry,SR Dennis,C Densham,F Di Lodovico,N Dokania,S Dolan,TA Doyle,O Drapier,J Dumarchez,P Dunne,A Eguchi,L Eklund,S Emery-Schrenk,A Ereditato,AJ Finch,G Fiorillo,C Francois,M Friend,Y Fujii,R Fujita,D Fukuda,R Fukuda,Y Fukuda,K Fusshoeller,C Giganti,M Gonin,A Gorin,M Guigue,DR Hadley,JT Haigh,P Hamacher-Baumann,M Hartz,T Hasegawa,S Hassani,NC Hastings,Y Hayato,A Hiramoto,M Hogan,J Holeczek,NT Hong Van,T Honjo,F Iacob,AK Ichikawa,M Ikeda,T Ishida,M Ishitsuka,K Iwamoto,A Izmaylov,N Izumi,M Jakkapu,B Jamieson,SJ Jenkins,C Jesús-Valls,M Jiang,P Jonsson,CK Jung,X Junjie,PB Jurj,M Kabirnezhad,AC Kaboth,T Kajita,H Kakuno,J Kameda,D Karlen,SP Kasetti,Y Kataoka,Y Katayama,T Katori,Y Kato,E Kearns,M Khabibullin,A Khotjantsev,T Kikawa,H Kikutani,H Kim,S King,J Kisiel,A Knight,T Kobata,T Kobayashi,L Koch,T Koga,A Konaka,LL Kormos,Y Koshio,A Kostin,K Kowalik,H Kubo,Y Kudenko,N Kukita,S Kuribayashi,R Kurjata,T Kutter,M Kuze,L Labarga,J Lagoda,M Lamoureux
Journal
Physical Review D
Published Date
2020/6/16
This paper reports the first simultaneous measurement of the double differential muon neutrino charged-current cross section on oxygen and carbon without pions in the final state as a function of the outgoing muon kinematics, made at the ND280 off-axis near detector of the T2K experiment. The ratio of the oxygen and carbon cross sections is also provided to help validate various models’ ability to extrapolate between carbon and oxygen nuclear targets, as is required in T2K oscillation analyses. The data are taken using a neutrino beam with an energy spectrum peaked at 0.6 GeV. The extracted measurement is compared with the prediction from different Monte Carlo neutrino-nucleus interaction event generators, showing particular model separation for very forward-going muons. Overall, of the models tested, the result is best described using local Fermi gas descriptions of the nuclear ground state with RPA …
Measurement of the muon neutrino charged-current single production on hydrocarbon using the T2K off-axis near detector ND280
Authors
K Abe,R Akutsu,A Ali,C Alt,J Amey,C Andreopoulos,L Anthony,M Antonova,S Aoki,A Ariga,Y Ashida,ET Atkin,Y Awataguchi,Y Azuma,S Ban,M Barbi,GJ Barker,G Barr,C Barry,M Batkiewicz-Kwasniak,A Beloshapkin,F Bench,V Berardi,S Berkman,RM Berner,L Berns,S Bhadra,S Bienstock,A Blondel,S Bolognesi,S Bordoni,B Bourguille,SB Boyd,D Brailsford,A Bravar,C Bronner,M Buizza Avanzini,J Calcutt,RG Calland,T Campbell,S Cao,SL Cartwright,R Castillo,MG Catanesi,A Cervera,A Chappell,C Checchia,D Cherdack,N Chikuma,G Christodoulou,J Coleman,G Collazuol,L Cook,D Coplowe,A Cudd,A Dabrowska,G De Rosa,T Dealtry,PF Denner,SR Dennis,C Densham,F Di Lodovico,N Dokania,S Dolan,O Drapier,KE Duffy,J Dumarchez,P Dunne,L Eklund,S Emery-Schrenk,A Ereditato,P Fernandez,T Feusels,AJ Finch,GA Fiorentini,G Fiorillo,C Francois,M Friend,Y Fujii,R Fujita,D Fukuda,R Fukuda,Y Fukuda,K Gameil,A Garcia,C Giganti,F Gizzarelli,T Golan,M Gonin,A Gorin,M Guigue,DR Hadley,L Haegel,JT Haigh,P Hamacher-Baumann,D Hansen,J Harada,M Hartz,T Hasegawa,NC Hastings,T Hayashino,Y Hayato,A Hillairet,T Hiraki,A Hiramoto,S Hirota,M Hogan,J Holeczek,NT Hong Van,F Hosomi,K Huang,F Iacob,AK Ichikawa,M Ikeda,J Imber,T Inoue,J Insler,RA Intonti,T Ishida,T Ishii,M Ishitsuka,E Iwai,K Iwamoto,A Izmaylov,B Jamieson,SJ Jenkins,C Jesús-Valls,M Jiang,S Johnson,P Jonsson,CK Jung,M Kabirnezhad,AC Kaboth,T Kajita,H Kakuno,J Kameda,D Karlen,Y Kataoka,T Katori,Y Kato,E Kearns,M Khabibullin,A Khotjantsev,H Kim,J Kim,S King,J Kisiel,A Knight,A Knox,T Kobayashi
Journal
Physical Review D
Published Date
2020/1/21
We report the measurements of the single and double differential cross section of muon neutrino charged-current interactions on carbon with a single positively charged pion in the final state at the T2K off-axis near detector using 5.56× 10 20 protons on target. The analysis uses data control samples for the background subtraction and the cross section signal, defined as a single negatively charged muon and a single positively charged pion exiting from the target nucleus, is extracted using an unfolding method. The model-dependent cross section, integrated over the T2K off-axis neutrino beam spectrum peaking at 0.6 GeV, is measured to be σ=(11.76±0.44 (stat)±2.39 (syst))× 10− 40 cm 2 nucleon− 1. Various differential cross sections are measured, including the first measurement of the Adler angles for single charged pion production in neutrino interactions with heavy nuclei target.
Jonathon Coleman FAQs
What is Jonathon Coleman's h-index at University of Liverpool?
The h-index of Jonathon Coleman has been 59 since 2020 and 135 in total.
What are Jonathon Coleman's top articles?
The articles with the titles of
Scintillator ageing of the T2K near detectors from 2010 to 2021
Supernova Model Discrimination with Hyper-Kamiokande
Precision measurement of the ratio
Proposal for A Water Cherenkov Test Beam Experiment for Hyper-Kamiokande andFuture Large-scale Water-based Detectors
AEDGE: Atomic Experiment for Dark Matter and Gravity Exploration in Space
Measurements of and charged-current cross-sections without detected pions nor protons on water and hydrocarbon at mean antineutrino energy of 0.86 …
A simple method for estimating the major nuclide fractional fission rates within light water and advanced gas cooled reactors
The Hyper-Kamiokande Experiment--Snowmass LOI
...
are the top articles of Jonathon Coleman at University of Liverpool.
What are Jonathon Coleman's research interests?
The research interests of Jonathon Coleman are: Physics
What is Jonathon Coleman's total number of citations?
Jonathon Coleman has 70,546 citations in total.
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