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Electron cloud interaction with high energy positive beam are believed responsible for various undesirable effects such as vacuum degradation, collective beam instability and even beam loss in high power proton circular accelerator. An…

Accelerator Physics · Physics 2015-08-04 Yu-Dong Liu , Kai-Wei Li

The back-streaming neutrons from the spallation target at CSNS are very intense, and can pose serious damage problems for the devices in the accelerator-target interface region. To tackle the problems, a possible scheme for this region was…

Accelerator Physics · Physics 2013-06-04 Jing Han-Tao , Tang Jing-Yu , Yang Zheng

The SRS is a 2GeV synchrotron light source with 14 beamlines serving approximately 34 experimental stations. Control of the major elements of the beamlines (vacuum pumps, gauges, valves and radiation stops) is the responsibility of the main…

Instrumentation and Detectors · Physics 2007-05-23 B. G. Martlew , B. Corker , G. Cox , P. W. Heath , M. T. Heron , A. Oates , W. R. Rawlinson , C. D. Sharp

A new muon source has been proposed to conduct muon spin rotation/relaxation/resonance ($\mu$SR) measurements at China Spallation Neutron Source (CSNS). Only 1 Hz of the CSNS proton beams (25 Hz in total) will be allocated for muon…

Instrumentation and Detectors · Physics 2022-12-07 Jingyu Dong , Ziwen Pan , Tianyi Yang , Zebin Lin , Zhe Wang , Zhengyang He , Zhe Chen , Hantao Jing , Jingyu Tang , Jiandang Liu , Hongjun Zhang , Bangjiao Ye

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

Injected beam energy and energy spread are critical parameters affecting the performance of our rapid cycling synchrotron (RCS). A real-time energy monitoring system is being installed to examine the H- beam out of the Intense Pulsed…

Accelerator Physics · Physics 2009-09-25 J. C. Dooling , F. R. Brumwell , M. K. Lien , G. E. McMichael

A beam loss in the superconducting part of the SNS linac has been observed during its commissioning and operation. Although the loss does not prevent the SNS high power operation, it results in an almost uniform irradiation of linac…

Accelerator Physics · Physics 2012-07-24 V. Lebedev , N. Solyak , J. -F. Ostigy , A. Alexandrov , A. Shishlo

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

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

This paper describes the dose delivery system used at the Centro Nazionale di Adroterapia Oncologica (CNAO) for ion beam modulated scanning radiotherapy. CNAO Foundation, INFN and University of Torino have developed and commissioned a Dose…

The Super Proton Synchrotron (SPS) injection system plays a fundamental role to preserve the quality of injected high-brightness beams for the Large Hadron Collider (LHC) physics program and to maintain the maximum storable intensity. The…

The Front End of the Spallation Neutron Source (SNS) extends from the Ion Source (IS), through a 65 keV LEBT, a 402.5 MHz RFQ, a 2.5 MeV MEBT, ending at the entrance to the DTL. The diagnostics suite in this space includes stripline beam…

Accelerator Physics · Physics 2010-11-15 L. Doolittle , T. Goulding , D. Oshatz , A. Ratti , J. Staples

Beam loss is a critical issue in high-intensity accelerators, and much effort is expended during both the design and operation phases to minimize the loss and to keep it to manageable levels. As new accelerators become ever more powerful,…

Accelerator Physics · Physics 2016-08-09 M. A. Plum

Multiple types of high quality neutron detectors are proposed for the first phase of the China Spallation Neutron Source (CSNS), which will be commissioned in 2018. Considering the shortage of 3He supply, a detector module composed of 49…

Instrumentation and Detectors · Physics 2017-03-21 Zhaoyang Xie , Jianrong Zhou , Yushou Song , Liang Sun , Zhijia Sun , Bitao Hu , Yuanbo Chen

The 10 MeV accelerator-driven subcritical system (ADS) Injector-I test stand at Institute of High Energy Physics (IHEP) is a testing facility dedicated to demonstrate one of the two injector design schemes [Injector Scheme-I, which works at…

The ITER Heating Neutral Beam (HNB) injector is required to deliver 16.7 MW power into the plasma from a neutralised beam of H-/D- negative ions, produced by an RF source and accelerated up to 1 MeV. To enhance the H-/D- production, the…

Plasma Physics · Physics 2022-11-04 M. Barbisan , R. Pasqualotto , A. Rizzolo

In this paper, we study the detection of accelerator neutrinos produced at the China Spallation Neutron Source (CSNS). Using the code FLUKA, we have simulated the production of neutrinos in the proton beam on the tungsten target and…

High Energy Physics - Phenomenology · Physics 2016-03-29 Ming-Yang Huang

The CSR-LINAC injector has been proposed in Heavy Ion Research Facility in Lanzhou (HIRFL). The linac mainly consists of two parts, the RFQ and the IH-DTL. The KONUS (Kombinierte Null Grad Struktur) concept has been introduced into the DTL…

Accelerator Physics · Physics 2013-06-21 Zhang Xiao-Hu , Yuan You-Jin , Xia Jia-Wen , Yin Xue-Jun , Du Heng

A white neutron beam line using the back-streaming neutrons from the spallation target at China Spallation Neutron Source (CSNS) is under construction. Different spectrometers mainly for nuclear data measurements to be installed in the…

Instrumentation and Detectors · Physics 2017-11-15 L. Y. Zhang , H. T. Jing , J. Y. Tang , Q. Li , X. C. Ruan , J. Ren , C. J. Ning , Y. J. Yu , Z. X. Tan , P. C. Wang , Y. C. He , X. Q. Wang

The China Spallation Neutron Source (CSNS) beam power was successfully reached 125 kW with a low beam loss in February 2022. In order to increase beam power, during the summer in 2022, we employ magnetic-alloy (MA) cavity in the rapid…

Accelerator Physics · Physics 2023-10-24 Yang Liu , Xiang Li , Jian Wu