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Related papers: Low Level RF Control for the PIP-II Accelerator

200 papers

The beam volume of the Pre-Production Single Spoke Resonator type 2 (ppSSR2) cryomodule [1] for the Proton Improvement Plan-II (PIP-II) [2] project will be protected against over-pressurization using a burst disk. This contribution focuses…

Accelerator Physics · Physics 2022-09-14 II Collaboration , M. Parise , D. Passarelli , J. Bernardini

The CMS Level-1 calorimeter trigger is being upgraded in two stages to maintain performance as the LHC increases pile-up and instantaneous luminosity in its second run. In the first stage, improved algorithms including event-by-event…

An upgrade of the Jefferson Lab IR FEL is now under construction. It will provide 10 kW output light power in a wavelength range of 2-10 microns. The FEL will be driven by a modest-sized 80-210 MeV, 10 mA energy-recovering superconducting…

Accelerator Physics · Physics 2014-11-18 D. Douglas , S. V. Benson , G. A. Krafft , R. Li , L. Merminga , B. C. Yunn

The proposed Next Linear Collider (NLC) contains linac systems operating at L,S,C, and X band. This paper describes a wideband modular low-level RF (LLRF) system applicable for all NLC pulsed RF systems. High speed digital IF techniques are…

Accelerator Physics · Physics 2007-05-23 P. Corredoura , C. Adolphsen

Fermilab is currently constructing a superconducting electron linac that will eventually serve as the backbone of a user-driven facility for accelerator science. This contribution describes the accelerator and summarizes the enabled…

Accelerator Physics · Physics 2013-04-02 P. Piot , V. Shiltsev , S. Nagaitsev , M. Church , P. Garbincius , S. Henderson , J. Leibfritz

Fermi National Accelerator Laboratory is constructing a superconducting 1.3 GHz cryomodule test facility located at the New Muon Lab building. The facility will be used for testing and validating cryomodule designs as well as support…

Accelerator Physics · Physics 2012-06-29 A. Martinez , A. L. Klebaner , J. C. Theilacker , B. D. DeGraff , J. Leibfritz

We have reported previously on the conditioning of the high-gradient accelerating cavities in the Fermilab Linac. Automated measurements of the sparking rate have been recorded since 1994 and are reported here. The sparking rate has…

Accelerator Physics · Physics 2008-11-26 E. McCrory , T. Kroc , A. Moretti , M. Popovic

Currently ALS is undergoing an upgrade to ALSU to produce 100 times brighter soft X-ray light. The LLRF system for Accumulator Ring (AR) is composed of two identical LLRF stations, for driving RF amplifiers. The closed loop RF amplitude and…

To improve RHIC luminosity for heavy ion beam energies below 10 GeV/nucleon, the Low Energy RHIC electron Cooler (LEReC) is currently under commissioning at BNL. The Linac of LEReC is designed to deliver a 1.6 MeV to 2.6 MeV electron beam,…

ANL and the National Science Center "Kharkov Institute of Physics Technology" (NSC KIPT, Kharkov, Ukraine) jointly proposed to design and build a 100MeV/100KW linear accelerator which will be used to drive the neutron source subcritical…

Accelerator Physics · Physics 2015-06-11 Mi Hou , Xiang He , Shilun Pei

Significant transient beam loading effects were observed during beam commissioning tests of prototype II of the injector for the Accelerator Driven Sub-critical (ADS) system, which took place at the Institute of Modern Physics, Chinese…

Accelerator Physics · Physics 2016-08-03 Zheng Gao , Yuan He , Xian-Wu Wang , Wei Chang , Rui-Feng Zhang , Zheng-Long Zhu , Sheng-Hu Zhang , Qi Chen , Tom Powers

Low Level RF (LLRF) control systems of linear accelerators (LINACs) are typically implemented with heterodyne based architectures, which have complex analog RF mixers for up and down conversion. The Gen 3 Radio Frequency System-on-Chip…

Accelerator Physics · Physics 2024-05-15 C. Liu , R. Herbst , B. Hong , L. Ruckman , E. A. Nanni

Project-X is a proposed project to be built at Fermi National Accelerator Laboratory with several potential missions. A primary part of the Project-X accelerator chain is a Superconducting linac, and In October 2009 a workshop was held to…

Accelerator Physics · Physics 2012-02-02 J. Galambos , R. Garoby , S. Geer

High precision Low-level RF (LLRF) control and monitoring systems for future particle accelerators will be a significant technical challenge as the requirements in performance, flexibility and affordability become increasingly stringent. We…

We propose an evolution of the Mu2e experiment, called Mu2e-II, that would leverage advances in detector technology and utilize the increased proton intensity provided by the Fermilab PIP-II upgrade to improve the sensitivity for…

Instrumentation and Detectors · Physics 2018-02-09 F. Abusalma , D. Ambrose , A. Artikov , R. Bernstein , G. C. Blazey , C. Bloise , S. Boi , T. Bolton , J. Bono , R. Bonventre , D. Bowring , D. Brown , D. Brown , K. Byrum , M. Campbell , J. -F. Caron , F. Cervelli , D. Chokheli , K. Ciampa , R. Ciolini , R. Coleman , D. Cronin-Hennessy , R. Culbertson , M. A. Cummings , A. Daniel , Y. Davydov , S. Demers , D. Denisov , S. Denisov , S. Di Falco , E. Diociaiuti , R. Djilkibaev , S. Donati , R. Donghia , G. Drake , E. C. Dukes , B. Echenard , A. Edmonds , R. Ehrlich , V. Evdokimov , P. Fabbricatore , A. Ferrari , M. Frank , A. Gaponenko , C. Gatto , Z. Giorgio , S. Giovannella , V. Giusti , H. Glass , D. Glenzinski , L. Goodenough , C. Group , F. Happacher , L. Harkness-Brennan , D. Hedin , K. Heller , D. Hitlin , A. Hocker , R. Hooper , G. Horton-Smith , C. Hu , P. Q. Hung , E. Hungerford , M. Jenkins , M. Jones , M. Kargiantoulakis , K. S. Khaw , B. Kiburg , Y. Kolomensky , J. Kozminski , R. Kutschke , M. Lancaster , D. Lin , I. Logashenko , V. Lombardo , A. Luca , G. Lukicov , K. Lynch , M. Martini , A. Mazzacane , J. Miller , S. Miscetti , L. Morescalchi , J. Mott , S. E. Mueller , P. Murat , V. Nagaslaev , D. Neuffer , Y. Oksuzian , D. Pasciuto , E. Pedreschi , G. Pezzullo , A. Pla-Dalmau , B. Pollack , A. Popov , J. Popp , F. Porter , E. Prebys , V. Pronskikh , D. Pushka , J. Quirk , G. Rakness , R. Ray , M. Ricci , M. Röhrken , V. Rusu , A. Saputi , I. Sarra , M. Schmitt , F. Spinella , D. Stratakis , T. Strauss , R. Talaga , V. Tereshchenko , N. Tran , R. Tschirhart , Z. Usubov , M. Velasco , R. Wagner , Y. Wang , S. Werkema , J. Whitmore , P. Winter , L. Xia , L. Zhang , R. -Y. Zhu , V. Zutshi , R. Zwaska

The latest generation of IPMs installed in the Fermilab Main Injector and Recycler incorporate a 1 kG permanent magnet, a newly designed high-gain, rad-tolerant preamp, and a control grid to moderate the charge that is allowed to arrive on…

Accelerator Physics · Physics 2015-02-11 J. R. Zagel , M. Alvarez , B. Fellenz , C. Jensen , C. Lundberg , E. McCrory , D. Slimmer , R. Thurman-Keup , D. Tinsley

As part of the PIP-II Injector Experiment (PXIE) accelerator, a four-vane radio frequency quadrupole (RFQ) accelerates a 30-keV, 1-mA to 10-mA H- ion beam to 2.1 MeV. It is designed to operate at a frequency of 162.5 MHz with arbitrary duty…

Accelerator Physics · Physics 2016-12-22 A. L. Edelen , S. G. Biedron , S. V. Milton , D. Bowring , B. E. Chase , J. P. Edelen , J. Steimel

The RF system for the Pohang Light Source (PLS) storage ring was greatly upgraded for PLS-II project of 400mA, 3.0GeV from 200mA, 2.5GeV. Three superconducting(SC) RF cavities with each 300kW maximum klystron amplifier were commissioned…

Accelerator Physics · Physics 2019-10-07 Inha Yu , Myunghwan Chun , Youngdo Joo , Insoo Park , Younguk Sohn , Mujin Lee , Sehwan Park , Seunghwan Shin

Phase-3 testing of the pHB650 cryomodule at the PIP-II Injector Test Facility was conducted to evaluate the effectiveness of heat load mitigations performed after earlier phases of testing and to continue pinpointing any sources of…

This paper outlines the RF design of the CLIC (Compact Linear Collider) 30 GHz main linac accelerating structure and gives the resulting longitudinal and transverse mode properties. The critical requirement for multibunch operation, that…

Accelerator Physics · Physics 2008-11-26 I. Wilson , W. Wuensch