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Following the PIP-II 800 MeV Linac, Fermilab will need an accelerator that extends from that linac to the MI injection energy of ~8 GeV, completing the modernization of the Fermilab high-intensity accelerator complex. This will maximize the…

The Proton Improvement Plan-II (PIP-II) is a superconducting linear accelerator being built at Fermilab that will provide 800 MeV proton beam for neutrino production. The linac consists of a total of twenty-three (23) cryomodules of five…

Accelerator Physics · Physics 2023-07-18 William Soyars , Tomasz Banaszkiewicz , Ram Dhuley

Fermilab is upgrading its Booster synchrotron to increase ramp rate and intensity. This is part of the Proton Improvement Plan (PIP-II) that will allow the Main Injector to achieve proton beam power of 1.2 MW within the next few years. This…

The Proton Improvement Plan II (PIP-II) project is a vital upgrade to the Fermilab accelerator complex. The magnet pulse rate of the PIP-II Injection system requires an increase from the current rate of 15 Hz to 20 Hz as well as a roughly…

The Proton Improvement Plan II (PIPII) is a superconducting linear accelerator being built at Fermilab that will provide 800 MeV proton beams for neutrino production. The Linac requires cooling at 80 K, 5 K, and 2 K temperatures, which will…

Accelerator Physics · Physics 2022-06-23 Ashish Kumar Shukla , Andrew Dalesandro , Ram Dhuley , William Soyars

This paper introduces a new method for stacking beams in the longitudinal phase space. It uses RF barriers to confine and compress beams in an accelerator, provided that the machine momentum acceptance is a few times larger than the…

Accelerator Physics · Physics 2007-05-23 Weiren Chou , Akira Takagi

Two pulsed power systems have been upgraded for the g-2 experiment at Fermilab. The Pbar Lithium Lens supply previously ran with a half sine pulsed current of 75 kA peak, 400 us duration and a repetition rate of 0.45 pps. For the g-2…

Accelerator Physics · Physics 2018-10-03 H. Pfeffer , D. Frolov , C. C. Jensen , M. E. Kufer , K. Quinn

The challenging High Luminosity LHC (HL-LHC) beam requirements will lead in the future to unprecedented beam parameters along the LHC injector chain. In the SPS accelerator these requests translate into about a factor two higher intensity…

Beam stoppers are installed in the transfer lines of the CERN accelerator complex; these components are used as part of the access safety system, which guarantees the safety of workers in the accelerators. They are designed to stop one or…

High Energy Physics - Experiment · Physics 2024-08-05 D. Baillard , E. Grenier-Boley , M. Dole , F. Deslande , R. Froeschl , T. Lorenzon , P. Moyret , R. Peron , A. Pilan Zanoni , C. Sharp , M. Timmins , M. Calviani

PIP-II beam transfer line (BTL) to transport the beam from PIP-II Linac to the Booster ring at Fermilab. One crucial aspect of the BTL design involved the implementation of collimators. These collimators play a vital role in removing large…

Accelerator Physics · Physics 2023-12-15 M. Xiao , F. Ostiguy , D. Johnson

The current program at Fermilab involves the construction of a new superconducting linear accelerator (LINAC) to replace the existing warm version. The new LINAC, together with other planned improvements, is in support of proton beam…

Accelerator Physics · Physics 2023-10-03 R. Thurman-Keup , T. Folan , M. Mwaniki , S. Sas-Pawlik

The Fermilab Proton Improvement Plan (PIP) was formed in late 2011 to address important and necessary upgrades to the Proton Source machines (Injector line, Linac and Booster). The goal is to increase the proton flux by doubling the Booster…

Accelerator Physics · Physics 2015-04-29 T. A. Butler , F. G. Garcia , M. R. Kufer , H. Pfeffer , D. Wolff

Increasing the Fermilab Main Injector (MI) beam power above ~1.2 MW requires replacement of the 8 GeV Booster by a higher intensity alternative. Earlier, rapid-cycling synchrotron and linac solutions were considered for this purpose. In…

Accelerator Physics · Physics 2023-08-15 D. Neuffer , S. Belomestnykh , M. Checchin , D. Johnson , S. Posen , E. Pozdeyev , V. Pronskikh , A. Saini , N. Solyak , V. Yakovlev

The MIP Timing Detector will provide additional timing capabilities for detection of minimum ionizing particles (MIPs) at CMS during the High Luminosity LHC era, improving event reconstruction and pileup rejection. The central portion of…

Instrumentation and Detectors · Physics 2021-07-19 R. Abbott , A. Abreu , F. Addesa , M. Alhusseini , T. Anderson , Y. Andreev , A. Apresyan , R. Arcidiacono , M. Arenton , E. Auffray , D. Bastos , L. A. T. Bauerdick , R. Bellan , M. Bellato , A. Benaglia , M. Benettoni , R. Bertoni , M. Besancon , S. Bharthuar , A. Bornheim , E. Brücken , J. N. Butler , C. Campagnari , M. Campana , R. Carlin , P. Carniti , N. Cartiglia , M. Casarsa , O. Cerri , P. Checchia , H. Chen , S. Chidzik , F. Chlebana , F. Cossutti , M. Costa , B. Cox , I. Dafinei , F. De Guio , P. Debbins , D. del Re , A. Dermenev , E. Di Marco , K. Dilsiz , K. F. Di Petrillo , G. Dissertori , S. Dogra , U. Dosselli , I. Dutta , F. Caleb , C. Fernandez Madrazo , M. Fernandez , M. Ferrero , Z. Flowers , W. Funk , M. Gallinaro , S. Ganjour , M. Gardner , F. Geurts , A. Ghezzi , S. Gninenko , F. Golf , J. Gonzalez , C. Gotti , L. Gray , F. Guilloux , S. Gundacker , E. Hazen , S. Hedia , A. Heering , R. Heller , T. Isidori , R. Isocrate , R. Jaramillo , M. Joyce , K. Kaadze , A. Karneyeu , H. Kim , J. King , G. Kopp , M. Korjik , O. K. Koseyan , A. Kozyrev , N. Kratochwil , M. Lazarovits , A. Ledovskoy , H. Lee , J. Lee , A. Li , S. Li , W. Li , T. Liu , N. Lu , M. Lucchini , W. Lustermann , C. Madrid , M. Malberti , I. Mandjavize , J. Mao , Y. Maravin , D. Marlow , B. Marsh , P. Martinez del Arbol , B. Marzocchi , R. Mazza , C. McMahon , V. Mechinsky , P. Meridiani , A. Mestvirishvili , N. Minafra , A. Mohammadi , F. Monti , C. S. Moon , R. Mulargia , M. Murray , Y. Musienko , J. Nachtman , S. Nargelas , L. Narvaez , O. Neogi , C. Neu , T. Niknejad , M. Obertino , H. Ogul , G. Oh , I. Ojalvo , Y. Onel , G. Organtini , T. Orimoto , J. Ott , I. Ovtin , M. Paganoni , F. Pandolfi , R. Paramatti , A. Peck , C. Perez , G. Pessina , C. Pena , S. Pigazzini , O. Radchenko , N. Redaelli , D. Rigoni , E. Robutti , C. Rogan , R. Rossin , C. Rovelli , C. Royon , M. Ö. Sahin , W. Sands , F. Santanastasio , U. Sarica , I. Schmidt , R. Schmitz , J. Sheplock , J. C. Silva , F. Siviero , L. Soffi , V. Sola , G. Sorrentino , M. Spiropulu , D. Spitzbart , A. G. Stahl Leiton , A. Staiano , D. Stuart , I. Suarez , T. Tabarelli de Fatis , G. Tamulaitis , Y. Tang , B. Tannenwald , R. Taylor , E. Tiras , M. Titov , S. Tkaczyk , D. Tlisov , I. Tlisova , M. Tornago , M. Tosi , R. Tramontano , J. Trevor , C. G. Tully , B. Ujvari , J. Varela , S. Ventura , I. Vila , T. Wamorkar , C. Wang , X. Wang , M. Wayne , J. Wetzel , S. White , D. Winn , S. Wu , S. Xie , Z. Ye , G. B. Yu , G. Zhang , L. Zhang , Y. Zhang , Z. Zhang , R. Zhu

The upcoming Proton Improvement Plan-II (PIP-II), designated for enhancements to the Fermilab accelerator complex, features a new 800 MeV superconducting linac and a Beam Transfer Line (BTL) to transport the beam to the existing Booster…

Accelerator Physics · Physics 2024-06-03 A. Pathak , O. Napoly , J. -F. Ostiguy

The DESY II Test Beam Facility is a key infrastructure for modern high energy physics detector development, providing particles with a small momentum spread in a range from 1 to 6 GeV to user groups e.g. from the LHC experiments and Belle…

In preparation for PIP-II, there has been interest in running the Fermilab Booster at a higher current more indicative of the PIP-II era operation. In July 2023, an experiment was performed to study collective instabilities over the…

Accelerator Physics · Physics 2024-06-24 M. Balcewicz , J. Eldred

Transverse 2D phase space distribution of a 2.1 MeV, 5 mA H$^-$ beam is measured at the PIPIT test accelerator at Fermilab with an Allison scanner. The paper describes the design, calibration, and performance of the scanner as well as the…

Accelerator Physics · Physics 2021-02-03 C. Richard , J. -P. Carneiro , B. Hanna , L. Prost , A. Saini , V. Scarpine , A. Shemyakin

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