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The MUonE experiment proposes a novel approach to determine the leading hadronic contribution to the muon g-2, from a precise measurement of the differential cross section of the $\mu-e$ elastic scattering, achievable by using the CERN SPS…

High Energy Physics - Experiment · Physics 2024-01-09 E. Spedicato

A silicon-tungsten (Si-W) sampling calorimeter, consisting of 19 alternate layers of silicon pad detectors (individual pad area of 1~cm$^2$) and tungsten absorbers (each of one radiation length), has been constructed for measurement of…

The Heating Neutral Beam Injectors (HNBs) for ITER will have to deliver 16.7 MW beams of H/D particles at 1 MeV energy. The beams will be produced from H-/D- ions, generated by a radiofrequency plasma source coupled to an ion acceleration…

Understanding the quark and gluon substructure of the nucleon has been a prime goal of both nuclear and particle physics for more than thirty years and has led to much of the progress in strong interaction physics. Still the flavor…

Deep--inelastic scattering events with a leading baryon have been detected by the H1 experiment at HERA using a forward proton spectrometer and a forward neutron calorimeter. Semi--inclusive cross sections have been measured in the…

High Energy Physics - Experiment · Physics 2008-11-26 C. Adloff

The European Research Council has recently funded HOLMES, a new experiment to directly measure the neutrino mass. HOLMES will perform a calorimetric measurement of the energy released in the decay of 163Ho. The calorimetric measurement…

An experiment to search for light sterile neutrinos was conducted at a reactor with a thermal power of 2.8 GW located at the Hanbit nuclear power complex. The search was done with a detector consisting of a ton of Gd-loaded liquid…

The newly built second experimental area EAR2 of the n_TOF spallation neutron source at CERN allows to perform (n, charged particles) experiments on short-lived highly radioactive targets. This paper describes a detection apparatus and the…

Instrumentation and Detectors · Physics 2016-06-01 L. Cosentino , A. Musumarra , M. Barbagallo , A. Pappalardo , N. Colonna , L. Damone , M. Piscopo , P. Finocchiaro , E. Maugeri , S. Heinitz , D. Schumann , R. Dressler , N. Kivel , O. Aberle , J. Andrzejewski , L. Audouin , M. Ayranov , M. Bacak , S. Barros , J. Balibrea-Correa , V. Beecares , F. Becvar , C. Beinrucker , E. Berthoumieux , J. Billowes , D. Bosnar , M. Brugger , M. Caamano , M. Calviani , F. Calvino , D. Cano-Ott , R. Cardella , A. Casanovas , D. M. Castelluccio , F. Cerutti , Y. H. Chen , E. Chiaveri , G. Cortes , M. A. Cortes-Giraldo , M. Diakaki , C. Domingo-Pardo , E. Dupont , I. Duran , B. Fernandez-Dominguez , A. Ferrari , P. Ferreira , W. Furman , S. Ganesan , A. Garcia-Rios , A. Gawlik , I. Gheorghe , T. Glodariu , K. Goebel , I. F. Goncalves , E. Gonzalez-Romero , E. Griesmayer , C. Guerrero , F. Gunsing , H. Harada , T. Heftrich , J. Heyse , D. G. Jenkins , E. Jericha , F. Kaeppeler , T. Katabuchi , P. Kavrigin , A. Kimura , M. Kokkoris , M. Krticka , E. Leal-Chidonca , J. Lerendegui , C. Lederer , H. Leeb , S. Lo Meo , S. Lonsdale , R. Losito , D. Macina , J. Marganiec , T. Martinez , C. Massimi , P. Mastinu , M. Mastromarco , F. Matteucci , A. Mazzone , E. Mendoza , A. Mengoni , P. M. Milazzo , F. Mingrone , M. Mirea , S. Montesano , R. Nolte , A. Oprea , N. Patronis , A. Pavlik , J. Perkowski , J. Praena , J. Quesada , K. Rajeev , T. Rauscher , R. Reifarth , A. Riego-Perez , P. Rout , C. Rubbia , J. Ryan , M. Sabate-Gilarte , A. Saxena , P. Schillebeeckx , S. Schmidt , P. Sedyshev , A. Stamatopoulos , G. Tagliente , J. L. Tain , A. Tarifeno-Saldivia , L. Tassan-Got , A. Tsinganis , S. Valenta , G. Vannini , V. Variale , P. Vaz , A. Ventura , V. Vlachoudis , R. Vlastou , J. Vollaire , A. Wallner , S. Warren , M. Weigand , C. Weiß , C. Wolf , P. J. Woods , T. Wright , P. Zugec , n_TOF collaboration

Over the last decades, the field of thermal neutron detection has overwhelmingly employed He-3-based technologies. The He-3 crisis together with the forthcoming establishment of the European Spallation Source have necessitated the…

A new measurement of the neutron EDM, using Ramsey's method of separated oscillatory fields, is in preparation at the new high intensity source of ultra-cold neutrons (UCN) at the Paul Scherrer Institute, Villigen, Switzerland (PSI). The…

The NOvA experiment has made a $4.4\sigma$-significant observation of $\bar\nu_{e}$ appearance in a 2 GeV $\bar\nu_{\mu}$ beam at a distance of 810 km. Using $12.33\times10^{20}$ protons on target delivered to the Fermilab NuMI neutrino…

High Energy Physics - Experiment · Physics 2023-02-18 M. A. Acero , P. Adamson , L. Aliaga , T. Alion , V. Allakhverdian , S. Altakarli , N. Anfimov , A. Antoshkin , A. Aurisano , A. Back , C. Backhouse , M. Baird , N. Balashov , P. Baldi , B. A. Bambah , S. Bashar , K. Bays , S. Bending , R. Bernstein , V. Bhatnagar , B. Bhuyan , J. Bian , T. Blackburn , J. Blair , A. C. Booth , P. Bour , C. Bromberg , N. Buchanan , A. Butkevich , S. Calvez , M. Campbell , T. J. Carroll , E. Catano-Mur , A. Cedeno , S. Childress , B. C. Choudhary , B. Chowdhury , T. E. Coan , M. Colo , J. Cooper , L. Corwin , L. Cremonesi , G. S. Davies , P. F. Derwent , P. Ding , Z. Djurcic , D. Doyle , E. C. Dukes , H. Duyang , S. Edayath , R. Ehrlich , M. Elkins , G. J. Feldman , P. Filip , W. Flanagan , M. J. Frank , H. R. Gallagher , R. Gandrajula , F. Gao , S. Germani , A. Giri , R. A. Gomes , M. C. Goodman , V. Grichine , M. Groh , R. Group , B. Guo , A. Habig , F. Hakl , J. Hartnell , R. Hatcher , A. Hatzikoutelis , K. Heller , V Hewes , A. Himmel , A. Holin , B. Howard , J. Huang , J. Hylen , F. Jediny , C. Johnson , M. Judah , I. Kakorin , D. Kalra , D. M. Kaplan , R. Keloth , O. Klimov , L. W. Koerner , L. Kolupaeva , S. Kotelnikov , A. Kreymer , Ch. Kulenberg , A. Kumar , C. D. Kuruppu , V. Kus , T. Lackey , K. Lang , S. Lin , M. Lokajicek , J. Lozier , S. Luchuk , K. Maan , S. Magill , W. A. Mann , M. L. Marshak , M. Martinez-Casales , V. Matveev , D. P. Mendez , M. D. Messier , H. Meyer , T. Miao , W. H. Miller , S. R. Mishra , A. Mislivec , R. Mohanta , A. Moren , L. Mualem , M. Muether , S. Mufson , K. Mulder , R. Murphy , J. Musser , D. Naples , N. Nayak , J. K. Nelson , R. Nichol , G. Nikseresht , E. Niner , A. Norman , T. Nosek , A. Olshevskiy , T. Olson , J. Paley , R. B. Patterson , G. Pawloski , D. Pershey , O. Petrova , R. Petti , D. D. Phan , R. K. Plunkett , B. Potukuchi , C. Principato , F. Psihas , A. Radovic , V. Raj , R. A. Rameika , B. Rebel , P. Rojas , V. Ryabov , O. Samoylov , M. C. Sanchez , S. Sanchez Falero , I. S. Seong , P. Shanahan , A. Sheshukov , P. Singh , V. Singh , E. Smith , J. Smolik , P. Snopok , N. Solomey , E. Song , A. Sousa , K. Soustruznik , M. Strait , L. Suter , A. Sutton , R. L. Talaga , B. Tapia Oregui , P. Tas , R. B. Thayyullathil , J. Thomas , E. Tiras , D. Torbunov , J. Tripathi , A. Tsaris , Y. Torun , J. Urheim , P. Vahle , J. Vasel , L. Vinton , P. Vokac , T. Vrba , M. Wallbank , B. Wang , T. K. Warburton , M. Wetstein , M. While , D. Whittington , S. G. Wojcicki , J. Wolcott , N. Yadav , A. Yallappa Dombara , K. Yonehara , S. Yu , S. Zadorozhnyy , J. Zalesak , B. Zamorano , R. Zwaska

The electro-magnetic calorimeter at the BaBar detector, part of the asymmetric B Factory at SLAC, measures photons in the energy range from 20 MeV to 8 GeV with good resolution. The calorimeter is calibrated at the low energy end with 6.13…

Instrumentation and Detectors · Physics 2019-08-14 Johannes M. Bauer

We present the design of a next-generation experiment, n2EDM, currently under construction at the ultracold neutron source at the Paul Scherrer Institute (PSI) with the aim of carrying out a high-precision search for an electric dipole…

We examine the reach of a Beta-beam experiment with two detectors at carefully chosen baselines for exploring neutrino mass parameters. Locating the source at CERN, the two detectors and baselines are: (a) a 50 kton iron calorimeter (ICAL)…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sanjib Kumar Agarwalla , Sandhya Choubey , Amitava Raychaudhuri

In addition to the common 3-body decay of the neutron $n\rightarrow p e^-\overline{\nu_e}$ there should exist an effective 2-body subset with the electron and proton forming a Hydrogen bound state with well defined total momentum, total…

In this paper, preliminary results are presented on high-$p_T$ inclusive neutral pion measurements in d-Au collisions at $\sqrt{s_{\rm NN}}$ = 200 GeV in the pseudo-rapidity range $0<\eta<1$. The photons of the decay $pi^0\to\gamma\gamma$…

Nuclear Experiment · Physics 2019-08-14 Andre Mischke

The EIC will deliver collisions of electrons with protons and nuclei at a wide variety of energies and at luminosities up to 1000 times higher than HERA. Precise measurement of both the scattered electron and the hadronic final state is…

Instrumentation and Detectors · Physics 2024-09-04 Henry T. Klest

HOLMES is a new experiment aiming at directly measuring the neutrino mass with a sensitivity below 2 eV. HOLMES will perform a calorimetric measurement of the energy released in the decay of $^{163}$Ho. The calorimetric measurement…

The quest for a non-zero electric dipole moment (EDM) of simple systems such as the electron, the neutron or atoms / molecules is a pow- erful way to search for physics beyond the standard model (SM) in par- ticular for new sources of CP…

Instrumentation and Detectors · Physics 2015-10-22 Yoann Kermaidic