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As a part of the ongoing XIIth plan project titled "R&D activities for high energy proton linac based spallation neutron source", the work on physics design of various subsystems of the injector linac and accumulator ring has been taken up…

To maximize the physics potential of future neutrino oscillation experiments, it is proposed to build a 15-MW `proton driver' consisitng solely of a 3-GeV proton injector linac (PI) and a 17-GeV superconducting ILC-type linac (SCL). The…

Accelerator Physics · Physics 2019-03-25 Radoje Belusevic

The Pohang Accelerator Laboratory operates an electron linac for the pulsed neutron source as one of the long-term nuclear R&D programs at the Korea Atomic Energy Research Institute. The designed beam parameters are as follows; The nominal…

Accelerator Physics · Physics 2008-11-26 G. N. Kim , H. S. Kang , Y. S. Lee , M. H. Cho , I. S. Ko , W. Namkung

The demand for neutron production facilities is increasing, as the applications of neutron science are manifold. These applications drive the need for efficient and compact neutron sources. In this context, this paper explores the potential…

The China spallation neutron source (CSNS) linac is designed with beam energy of 81MeV and a peak current of 15mA in the first phase. The RF power system for the 81 MeV Linac requires 8 units of RF power sources, each unit has one…

Accelerator Physics · Physics 2019-09-26 Linyan Rong , Zhencheng Mu , Zhexin Xie , Bo Wang , Wenzhong Zhou , Maliang Wan , Meifei Liu , Jian Li , Xinan Xu

The Spallation Neutron Source (SNS) is being designed for operation in 2004. The SNS is a 1 GeV machine consisting of a combination normal-conducting and super-conducting linac as well as a ring and target area. The linac front end is a…

Accelerator Physics · Physics 2007-05-23 Amy Regan , Sung-il Kwon , Tony S. Rohlev , Yi-Ming Wang , Mark S. Prokop , David W. Thomson

New generation of neutron decay experiments, which can be done with high accuracy at new Spallation Neutron Sources, are very important for solution of current problems of fundamental physics and for tests of the Standard Model. The open…

Nuclear Theory · Physics 2016-09-08 Vladimir Gudkov

The Spallation Neutron Source (SNS) at Oak Ridge National Laboratory, Tennessee, provides an intense flux of neutrinos in the few tens-of-MeV range, with a sharply-pulsed timing structure that is beneficial for background rejection. In this…

The conception of High Power Linac developed in Russian accelerator centres is based on the use of independently phased SC resonators with quadrupole lenses between them. The type and parameters of the resonators as well as focusing…

Accelerator Physics · Physics 2007-05-23 A. Kolomiets , S. Yaramishev

Proposals exist and efforts are under way to construct pulsed spallation ultra-cold neutron (UCN) sources at accelerator laboratories around the world. At the Paul Scherrer Institut (PSI), Switzerland, and at the Los Alamos National…

Nuclear Experiment · Physics 2007-05-23 Klaus Kirch

Due to their high cost of acquisition and operation, there are still a limited number of high-yield, high-flux neutron source facilities worldwide. In this context, laser-driven neutron sources offer a promising, cheaper alternative to…

A muon collider (MC) would require a high-power proton driver to generate intense muon beams at the start of the accelerator chain. Like other high-power facilities, the driver would accumulate intense proton bunches via charge-exchange…

Accelerator Physics · Physics 2025-08-19 Austin Hoover , Vasiliy Morozov , Amith Narayan , Maurice Piller

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

Commissioning of the new high-intensity ultracold neutron (UCN) source at the Paul Scherrer Institut (PSI) has started in 2009. The design goal of this new generation high intensity UCN source is to surpass by a factor of ~100 the current…

Nuclear Experiment · Physics 2011-09-30 Bernhard Lauss

The cyclotron designed for the IsoDAR neutrino source represents a paradigm shift in cyclotron performance -- a factor of 10 increase in beam current. This performance is required to develop a neutrino source of sufficient strength for…

High Energy Physics - Experiment · Physics 2022-03-16 Jose Alonso

In the baseline design of the International Linear Collider (ILC) an undulator-based source is foreseen for the positron source in order to match the physics requirements. The recently chosen first energy stage with sqrt(s)=250 GeV requires…

The development of compact neutron sources for applications is extensive and features many approaches. Let alone ion-based approaches, several projects with different parameters exist. This article focuses on ion-based neutron production…

Instrumentation and Detectors · Physics 2023-07-13 Benedikt Schmitz , Stefan Scheuren

In order to dissipate long-lived radioactive waste, not only high ux proton accelerator but also electron linac have been proposed. A proton accelerator directly induces nuclear fission and mutation. On the other hand, electron beam has two…

Accelerator Physics · Physics 2021-04-20 Y. Kawashima , T. Asaka , H. Ego , M. Hara

A light source based on an Energy Recovered Linac (ERL) [1] consist of a superconducting linac and a transfer line that includes wigglers and undulators to produce the synchrotron light. The transfer line brings the electrons bunches back…

Adaptation and Self-Organizing Systems · Physics 2007-05-23 Andrew Hutton

Presently large efforts are conducted towards the development of highly brilliant gamma beams via Compton back scattering of photons from a high-brilliance electron beam, either on the basis of a normal-conducting electron linac or a…

Nuclear Experiment · Physics 2015-05-27 C. Hugenschmidt , K. Schreckenbach , D. Habs , P. G. Thirolf