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Related papers: Cavity Simulator for European Spallation Source

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The data produced by the future space-based millihertz gravitational-wave detector LISA will require nontrivial pre-processing, which might affect the science results. It is crucial to demonstrate the feasibility of such processing…

Instrumentation and Methods for Astrophysics · Physics 2023-05-22 Jean-Baptiste Bayle , Olaf Hartwig , Marc Lilley , Aurélien Hees , Christian Chapman-Bird , Graham Woan , Peter Wolf

The NNBAR experiment for the European Spallation Source will search for free neutrons converting to antineutrons with a sensitivity improvement of three orders of magnitude compared to the last such search. This paper describes progress…

High-beta superconducting radiofrequency (SRF) elliptical cavities are being developed for several accelerator projects including Project X, the European XFEL, and the International Linear Collider (ILC). Fermilab has recently established…

Accelerator Physics · Physics 2009-10-23 C. M. Ginsburg

The European XFEL is a new research facility currently under construction at DESY in the Hamburg area in Germany. From 2015 on, it will generate extremely intense X-ray flashes that will be used by researchers from all over the world. The…

Accelerator Physics · Physics 2015-06-16 J. Schaffran , Y. Bozhko , B. Petersen , D. Meissner , M. Chorowski , J. Polinski

A superconducting Double Spoke Resonator (DSR) is the technology of choice in a low energy section of a high power proton linear accelerator. At the FREIA laboratory in Uppsala University, we have tested two DSRs in a prototype cryomodule…

Accelerator Physics · Physics 2020-05-05 A. Miyazaki , H. Li , K. Fransson , K. Gajewski , L. Hermansson , R. Santiago Kern , R. Wedberg , R. Ruber

The EUROnu project has studied three possible options for future, high intensity neutrino oscillation facilities in Europe. The first is a Super Beam, in which the neutrinos come from the decay of pions created by bombarding targets with a…

Accelerator Physics · Physics 2013-05-20 T. R. Edgecock , O. Caretta , T. Davenne , C. Densham , M. Fitton , D. Kelliher , P. Loveridge , S. Machida , C. Prior , C. Rogers , M. Rooney , J. Thomason , D. Wilcox , E. Wildner , I. Efthymiopoulos , R. Garoby , S. Gilardoni , C. Hansen , E. Benedetto , E. Jensen , A. Kosmicki , M. Martini , J. Osborne , G. Prior , T. Stora , T. Melo-Mendonca , V. Vlachoudis , C. Waaijer , P. Cupial , A. Chancé , A. Longhin , J. Payet , M. Zito , E. Baussan , C. Bobeth , E. Bouquerel , M. Dracos , G. Gaudiot , B. Lepers , F. Osswald , P. Poussot , N. Vassilopoulos , J. Wurtz , V. Zeter , J. Bielski , M. Kozien , L. Lacny , B. Skoczen , B. Szybinski , A. Ustrycka , A. Wroblewski , M. Marie-Jeanne , P. Balint , C. Fourel , J. Giraud , J. Jacob , T. Lamy , L. Latrasse , P. Sortais , T. Thuillier , S. Mitrofanov , M. Loiselet , Th. Keutgen , Th. Delbar , F. Debray , C. Trophine , S. Veys , C. Daversin , V. Zorin , I. Izotov , V. Skalyga , G. Burt , A. C. Dexter , V. L. Kravchuk , T. Marchi , M. Cinausero , F. Gramegna , G. De Angelis , G. Prete , G. Collazuol , M. Laveder , M. Mazzocco , M. Mezzetto , C. Signorini , E. Vardaci , A. Di Nitto , A. Brondi , G. La Rana , P. Migliozzi , R. Moro , V. Palladino , N. Gelli , D. Berkovits , M. Hass , T. Y. Hirsh , M. Schaumann , A. Stahl , J. Wehner , A. Bross , J. Kopp , D. Neuffer , R. Wands , R. Bayes , A. Laing , P. Soler , S. K. Agarwalla , A. Cervera Villanueva , A. Donini , T. Ghosh , J. J. Gómez Cadenas , P. Hernández , J. Martín-Albo , O. Mena , J. Burguet-Castell , L. Agostino , M. Buizza-Avanzini , M. Marafini , T. Patzak , A. Tonazzo , D. Duchesneau , L. Mosca , M. Bogomilov , Y. Karadzhov , R. Matev , R. Tsenov , E. Akhmedov , M. Blennow , M. Lindner , T. Schwetz , E. Fernández Martinez , M. Maltoni , J. Menéndez , C. Giunti , M. C. González García , J. Salvado , P. Coloma , P. Huber , T. Li , J. López-Pavón , C. Orme , S. Pascoli , D. Meloni , J. Tang , W. Winter , T. Ohlsson , H. Zhang , L. Scotto-Lavina , F. Terranova , M. Bonesini , L. Tortora , A. Alekou , M. Aslaninejad , C. Bontoiu , A. Kurup , L. J. Jenner , K. Long , J. Pasternak , J. Pozimski , J. J. Back , P. Harrison , K. Beard , A. Bogacz , J. S. Berg , D. Stratakis , H. Witte , P. Snopok , N. Bliss , M. Cordwell , A. Moss , S. Pattalwar , M. Apollonio

The European Spallation Source linear proton accelerator will have a uniquely high power of 5 MW. The modifications and additions to the accelerator that are required to enable the generation of a uniquely intense neutrino Super Beam…

Instrumentation and Detectors · Physics 2019-04-03 Tord Ekelof , Marcos Dracos

Using an atom-cavity platform, we propose to combine the effective gauge phase of rotated neutral atoms and the superradiant phase transition to build a highly sensitive and fast quantum rotation sensor. The atoms in a well-controlled array…

Quantum Physics · Physics 2023-03-24 Jim Skulte , Jayson G. Cosme , Ludwig Mathey

Fundamental neutron and neutrino physics at neutron sources, combining precision measurements and theory, can probe new physics at energy scales well beyond the highest energies probed by the LHC and possible future high energy collider…

Nuclear Experiment · Physics 2025-07-01 H. Abele , J. Amaral , W. R. Anthony , L. AAstrand , M. Atzori Corona , S. Baessler , M. Bartis , E. Baussan , D. H. Beck , J. Bijnens , K. Bodek , J. Bosina , E. Bossio , G. Brooijmans , L. J. Broussard , G. Brunetti , A. Burgman , M. Cadeddu , N. Cargioli , J. Cederkall , A. Chambon , T. W. Choi , P. Christiansen , V. Cianciolo , C. B. Crawford , S. Degenkolb , N. Delarosa , M. Demarteau , K. Dickerson , D. D. DiJulio , F. Dordei , Y. Efremenko , T. Ekelof , M. Eshraqi , R. R. Fan , M. Fertl , H. Filter-Pieler , B. Fornal , G. Fragneto , C. Gatto , P. Geltenbort , F. Ghazi Moradi , H. Gisbert , P. Golubev , M. Gonzalez-Alonso , G. Gorini , P. Heil , N. Hermansson-Truedsson , Y. Hicyilmaz , M. Holl , T. Ito , K. E. Iversen , T. Jenke , M. Jentschel , M. Juni Ferreira , S. Kawasaki , E. Kemp , P. Kinhult , M. Kitaguchi , J. Klenke , W. Korten , A. Kozela , B. Lauss , M. Lebert , W. Lee , T. Lesiak , C. Y. Liu , L. Lobell , A. Longhin , E. Lytken , B. Maerkisch , J. Marton , B. Meirose , N. Milas , D. Milstead , F. Monrabal , S. Moretti , P. Mueller , A. Nepomuceno , J. Newby , R. Nieuwenhuis , T. Palasz , R. Pasechnik , S. Penttila , M. Persoz , L. B. Persson , F. M. Piegsa , B. Plaster , I. Pradler , F. Pupilli , K. Pysz , T. Quirino , J. C. Ramsey , B. Rataj , J. Rathsman , S. Roccia , D. Rozpedzik , D. Rudolph , E. Salehi , V. Santoro , A. Saunders , H. Schober , K. Scholberg , W. Schreyer , A. Schubert , D. Silvermyr , O. Smirnova , W. M. Snow , T. Soldner , S. R. Soleti , Y. V. Stadnik , R. Strauss , F. Terranova , T. Tolba , N. Tsapatsaris , L. Vale Silva , W. Van Goethem , R. Wagner , M. Wolke , W. Yao , N. Yazdandoost , A. R. Young , L. Zanini , M. Zielinski

Transport calculations for neutronic design require accurate nuclear data and validated computational tools. In the Spallation Physics Group, at the European Spallation Source, we perform shielding and neutron beam calculations to help the…

Instrumentation and Detectors · Physics 2021-03-11 Jose Ignacio Marquez Damian , Douglas D. DiJulio , Günter Muhrer

Los Alamos National Laboratory (LANL) is designing a coupled cavity linac (CCL) for the Spallation Neutron Source (SNS) being built at Oak Ridge National Laboratory (ORNL). As part of the design process, a proto-type, Hot Model, consisting…

Accelerator Physics · Physics 2007-05-23 Chrisine A. Treml , Stanley K. Brown , John D. Bernardin

The SNS linac accelerates an average beam current of 2 mA to an energy of 968 MeV. The linac is pulsed at 60 Hz with an H- beam pulse of 1 ms. The first 185 Mev of the linac uses normal conducting cavities, and the remaining length of the…

Accelerator Physics · Physics 2007-05-23 Michael Lynch , William Reass , Daniel Rees , Amy Regan , Paul Tallerico

During 2014 the second experimental area EAR2 was completed at the n-TOF neutron beam facility at CERN. As the neutrons are produced via spallation, by means of a high-intensity 20 GeV pulsed proton beam impinging on a thick target, the…

Instrumentation and Detectors · Physics 2019-08-14 L. Cosentino , A. Musumarra , M. Barbagallo , N. Colonna , L. Damone , A. Pappalardo , M. Piscopo , P. Finocchiaro

SoLid, located at SCK-CEN in Mol, Belgium, is a reactor antineutrino experiment at a very short baseline of 5.5 -- 10m aiming at the search for sterile neutrinos and for high precision measurement of the neutrino energy spectrum of…

Instrumentation and Detectors · Physics 2019-05-03 Lukas On Arnold

The transport of neutrons in long beamlines at spallation neutron sources presents a unique challenge for Monte-Carlo transport calculations. This is due to the need to accurately model the deep-penetration of high-energy neutrons through…

Instrumentation and Detectors · Physics 2020-01-07 Douglas D. DiJulio , Isak Svensson , Xiao Xiao Cai , Joakim Cederkall , Phillip M. Bentley

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…

In this paper, we describe the design and implementation of a high precision real time NAND simulator called Copycat that runs on a commodity multi-core desktop environment. This NAND simulator facilitates the development of embedded flash…

Hardware Architecture · Computer Science 2016-12-22 Juyong Shin , Jongbo Bae , Ansu Na , Sang Lyul Min

Fraunhofer FIRST develops a computing service and collaborative workspace providing a convenient tool for simulation and investigation of quantum algorithms. To broaden the twenty qubit limit of workstation-based simulations to the next…

We have realised a semiconductor quantum structure that produces electroluminescence while operating in the light-matter strong coupling regime. The mid-infrared light emitting device is composed of a quantum cascade structure embedded in a…

The SoLid experiment aims to measure neutrino oscillation at a baseline of 6.4 m from the BR2 nuclear reactor in Belgium. Anti-neutrinos interact via inverse beta decay (IBD), resulting in a positron and neutron signal that are correlated…