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Related papers: Preliminary Study on the RF tuning of CSNS DTL

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Stabilization of the accelerating field in Drift Tube Linac(DTL) is obtained by inserting Post Couplers(PCs).On the basis of the circuit model equivalent for the DTL with and without asymmetrical PCs, stabilization is deduced…

Accelerator Physics · Physics 2015-06-15 Xiaoyu Jia , Shuxin Zheng

Based on the design requirements proposed by the Beijing On-Line Isotope Separation project (BISOL), four Sn$^{22+}$-based,81.25MHz continuous wave (CW) drift tube linac (DTL) cavities have been designed. These DTLs are capable of…

Accelerator Physics · Physics 2023-07-28 Meiyun Han , Tianhao Wei , Ying Xia , Austin Morris , Yuanrong Lu , Zhi Wang , Zhaohua Peng

The Fermilab Linac is a roughly 145 meter linear accelerator that accelerates H- beam from 750 keV to 400 MeV and provides beam for the Booster and the rest of the accelerator chain. The first section of the Linac is a Drift-Tube Linac…

Accelerator Physics · Physics 2023-05-25 J. Stanton , R. Sharankova , K. Seiya , M. Wesley

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 closed-off structure of the Fermilab Drift Tube Linac precludes a robust array of instrumentation from directly monitoring the H- beam that is accelerated from 750 keV to 116 MeV. To improve beam tuning and operational assessment of…

Accelerator Physics · Physics 2025-11-25 E. V. Chen , A. L. Saewert , R. V. Sharankova

Cluster counting dN/dx is a promising method to enhance particle identification for gaseous detectors, especially in next-generation collider experiments like the FCC-ee, where good pion-kaon separation over a broad momentum range is…

Instrumentation and Detectors · Physics 2026-05-21 Jiajin Ge , Chihao Li , Can Suslu , Yuxiang Guo , Emmett Salzer , Tiesheng Dai , Jianming Qian , Bing Zhou , Junjie Zhu

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

The LCLS-II RF system physically spans ~700m and has strict requirements -- on the order of 20 fs -- on the phase stability of the accelerating RF fields in its SRF linac. While each LLRF rack is crudely temperature-stabilized, the weather…

Accelerator Physics · Physics 2023-11-15 L. Doolittle , S. D. Murthy , A. Benwell , D. Chabot , J. Chen , B. Hong , S. Hoobler , J. Nelson , C. Xu

The parameters for a 30 GeV test beam are outlined for use with an undulator in the FFTB tunnel where the LCLS will eventually be housed. It is proposed to use the SLAC linac and damping rings in their present mode of operation for PEP II…

Accelerator Physics · Physics 2007-05-23 Patrick Krejcik

The front end of Los Alamos Neutron Science Center (LANSCE) linear accelerator uses four 201.25-MHz Drift-Tube Linacs (DTLs) to accelerate the H+ and H- beams to 100 MeV. Three of the 201.25-MHz DTLs are powered by diacrodes and the first…

Accelerator Physics · Physics 2022-11-15 Sungil Kwon , M. S. Barrueta , L. Castellano , J. M. Lyles , M. Prokop , P. Van Rooy , P. Torrez

Alignment of the ILC main linac will be more critical than for any currently existing accelerators due to its long length and the ultra low emittance required. There are several techniques for measuring the ILC reference network; in this…

Instrumentation and Detectors · Physics 2009-02-02 John Dale , Armin Reichold

LINAC 4 is a normal conducting H- linac proposed at CERN to provide a higher proton flux to the CERN accelerator chain. It should replace the existing LINAC 2 as injector to the Proton Synchrotron Booster and can also operate in the future…

Accelerator Physics · Physics 2007-05-23 M. Baylac , J. M. De Conto , E. Froidefond , E. Sargsyan

Configuration tuning is critical for database performance. Although recent advancements in database tuning have shown promising results in throughput and latency improvement, challenges remain. First, the vast knob space makes direct…

Databases · Computer Science 2025-11-10 Xinyue Yang , Chen Zheng , Yaoyang Hou , Renhao Zhang , Yinyan Zhang , Yanjun Wu , Heng Zhang

China Spallation Neutron Source(CSNS) target power will upgrade to 500 kW(CSNS-II) from 300kW, energy gain of H-Linac will up to 300 MeV from 80 MeV using about 50 superconductor cavities. LLRF is an important device for controlling the…

Accelerator Physics · Physics 2023-11-17 Zhexin Xie , Kai Guo , Zhencheng Mu , Xinpeng Ma , Nan Gan , Maliang Wan , Bo Wang , Linyan Rong , Hui Zhang , Hexin Wang

The off-frequency detune method is being considered for application in the LCLS-II-HE superconducting linac to produce multi-energy electron beams for supporting multiple undulator lines simultaneously [1]. Design of the tuner has been…

Accelerator Physics · Physics 2022-08-10 Y. Pischalnikov , T. Arkan , C. Contreras-Martinez , B. Hartsell , J. Kaluzny , R. Pilipenko , J. C. Yun , W. Lahmadi

Suppression of beam losses is essential for successful operation of high-intensity linac. Historically, the values of the field amplitudes and phases of the side-coupled, 805-MHz LANSCE linac modules are maintained using a well-known…

Accelerator Physics · Physics 2020-02-26 Y. K. Batygin , F. E. Shelley , H. A. Watkins

We propose a transfer learning-enabled Transformer framework to simultaneously realize accurate modeling and Raman pump design in C+L-band systems. The RMSE for modeling and peak-to-peak GSNR variation/deviation is within 0.22 dB and…

Signal Processing · Electrical Eng. & Systems 2025-10-21 Jiaming Liu , Rui Wang , JinJiang Li , Hong Lin , Jing Zhang , Kun Qiu

KONUS beam dynamics design of uranium DTL with LORASR code is presented. The 238U34+ beam, whose current is 5.0emA, is accelerated from injection energy of 0.35MeV/u to output energy of 1.3MeV/u by IH-DTL operated at 81.25MHz in HIAF…

Accelerator Physics · Physics 2013-08-07 W. P. Dou , Y. He , Y. R. Lu

In order to update the beam power from 100 kW to 250 kW in China spallation neutron source (CSNS) Phase II, one of the important measures is to replace the 80 meters long beam transport line between the present 80 MeV linac injector and the…

Accelerator Physics · Physics 2015-07-14 LI Zhi-Hui , FU Shi-Nian

The generation of the ultra-bright beams required by modern accelerators and drivers of free-electron lasers (FELs) has generally relied on chicane-based bunch compressions that often result in the microbunching instability. Following…

Accelerator Physics · Physics 2014-09-09 Alex H. Lumpkin
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