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During Nova operations it is planned to run the Fermilab Recycler in a 12 batch slip stacking mode. In preparation for this, measurements of the tune during a six batch injection and then as the beam is slipped by changing the RF frequency,…

Accelerator Physics · Physics 2013-02-01 D. J. Scott , D. Capista , I. Kourbanis , K. Seiya , M. -J. Yan

The extraction bucket position in the Fermilab Booster is controlled with a cogging process that involves the comparison of the Booster RF count and the Recycler Ring revolution marker. A one RF bucket jitter in the extraction bucket…

Accelerator Physics · Physics 2017-09-22 K. Seiya , C. Drennan , W. Pellico , S. Chaurize

In order to meet the needs of Fermilabs planned post-collider experimental program, the total proton throughput of the 8 GeV Booster accelerator must be nearly doubled within the next two years. A system of 48 ramped corrector magnets has…

Accelerator Physics · Physics 2012-03-09 M. McAteer , S. Kopp , E. Prebys

A VME-based data acquisition system for beam-loss monitors has been developed and is in use in the Tevatron and Main Injector accelerators at the Fermilab complex. The need for enhanced beam-loss protection when the Tevatron is operating in…

The kicker control system was used for beam extraction and injection between two cooling storage rings (CSRs) at the Heavy Ion Research Facility in Lanzhou (HIRFL). To meet the requirements of special physics experiments, the kicker…

For Project X Fermilab Main Injector will be required to provide up to 2.3 MW to a neutrino production target at energies between 60 and 120 GeV. To accomplish the above power levels 3 times the current beam intensity will need to be…

Accelerator Physics · Physics 2012-08-17 J. Dey , I. Kourbanis

For NOvA and future experiments requiring high intensity proton beams, Fermilab is in the process of upgrading the existing accelerator complex for increased proton production. One such improvement is to reduce the Main Injector cycle time,…

Accelerator Physics · Physics 2014-09-22 R. Madrak , D. Wildman

To date, the 120 GeV Fermilab Main Injector accelerator has accelerated a single batch of protons from the 8 GeV rapid-cycling Booster synchrotron for production of antiprotons for Run II. In the future, the Main Injector must accelerate 6…

Accelerator Physics · Physics 2007-05-23 R. Zwaska , S. Kopp , W. Pellico , R. Webber

The planned neutrino program at Fermilab requires large proton beam intensities in excess of 2 MW. Measuring the transverse profiles of these high intensity beams is challenging and often depends on non-invasive techniques. One such…

Accelerator Physics · Physics 2015-11-09 R. Thurman-Keup , M. Alvarez , J. Fitzgerald , C. Lundberg , P. Prieto , M. Roberts , J. Zagel , W. Blokland

The Fermilab Booster is being upgraded under the Proton Improvement Plan (PIP) to be capable of providing a proton flux of $2.25^{17}$ protons per hour. The intensity per cycle will remain at the present operational $4.3^{12}$ protons per…

Accelerator Physics · Physics 2015-11-05 K. Seiya , C. M. Bhat , D. E. Johnson , V. V. Kapin , W. A. Pellico , C. Y. Tan , R. J. Tesarek

The possibility of using electron beam phase space manipulations to support a free-electron laser accelerator design optimization has motivated our research. An on-going program demonstrating the exchange of transverse horizontal and…

Accelerator Physics · Physics 2012-08-10 A. H. Lumpkin , A. S. Johnson , J. Ruan , J. Santucci , Y. -E. Sun , R. Thurman-Keup , H. Edwards

Fermilab will continue to maintain its pre-eminent position in the world of High Energy Physics, with a unique opportunity to make unprecedented studies of the top quark and major discoveries, until the Large Hadron collider (LHC) at CERN…

High Energy Physics - Experiment · Physics 2009-11-10 Pushpalatha C. Bhat , William J. Spalding

This paper describes the hardware and operations of the Neutrinos at the Main Injector (NuMI) beam at Fermilab. It elaborates on the design considerations for the beam as a whole and for individual elements. The most important design…

Accelerator Physics · Physics 2015-12-09 P. Adamson , K. Anderson , M. Andrews , R. Andrews , I. Anghel , D. Augustine , A. Aurisano , S. Avvakumov , D. S. Ayres , B. Baller , B. Barish , G. Barr , W. L. Barrett , R. H. Bernstein , J. Biggs , M. Bishai , A. Blake , V. Bocean , G. J. Bock , D. J. Boehnlein , D. Bogert , K. Bourkland , S. V. Cao , C. M. Castromonte , S. Childress , B. C. Choudhary , J. A. B. Coelho , J. H. Cobb , L. Corwin , D. Crane , J. P. Cravens , D. Cronin-Hennessy , R. J. Ducar , J. K. de Jong , A. V. Devan , N. E. Devenish , M. V. Diwan , A. R. Erwin , C. O. Escobar , J. J. Evans , E. Falk , G. J. Feldman , T. H. Fields , R. Ford , M. V. Frohne , H. R. Gallagher , V. Garkusha , R. A. Gomes , M. C. Goodman , P. Gouffon , N. Graf , R. Gran , N. Grossman , K. Grzelak , A. Habig , S. R. Hahn , D. Harding , D. Harris , P. G. Harris , J. Hartnell , R. Hatcher , S. Hays , K. Heller , A. Holin , J. Huang , J. Hylen , A. Ibrahim , D. Indurthy , G. M. Irwin , Z. Isvan , D. E. Jaffe , C. James , D. Jensen , J. Johnstone , T. Kafka , S. M. S. Kasahara , G. Koizumi , S. Kopp , M. Kordosky , A. Kreymer , K. Lang , C. Laughton , G. Lefeuvre , J. Ling , P. J. Litchfield , L. Loiacono , P. Lucas , W. A. Mann , A. Marchionni , M. L. Marshak , N. Mayer , C. McGivern , M. M. Medeiros , R. Mehdiyev , J. R. Meier , M. D. Messier , D. G. Michael , R. H. Milburn , J. L. Miller , W. H. Miller , S. R. Mishra , S. Moed Sher , C. D. Moore , J. Morfin , L. Mualem , S. Mufson , S. Murgia , M. Murtagh , J. Musser , D. Naples , J. K. Nelson , H. B. Newman , R. J. Nichol , J. A. Nowak , J. O Connor , W. P. Oliver , M. Olsen , M. Orchanian , S. Osprey , R. B. Pahlka , J. Paley , A. Para , R. B. Patterson , T. Patzak , Z. Pavlovic , G. Pawloski , A. Perch , E. A. Peterson , D. A. Petyt , M. M. Pfutzner , S. Phan-Budd , R. K. Plunkett , N. Poonthottathil , P. Prieto , D. Pushka , X. Qiu , A. Radovic , R. A. Rameika , J. Ratchford , B. Rebel , R. Reilly , C. Rosenfeld , H. A. Rubin , K. Ruddick , M. C. Sanchez , N. Saoulidou , L. Sauer , J. Schneps , D. Schoo , A. Schreckenberger , P. Schreiner , P. Shanahan , R. Sharma , W. Smart , C. Smith , A. Sousa , A. Stefanik , N. Tagg , R. L. Talaga , G. Tassotto , J. Thomas , J. Thompson , M. A. Thomson , X. Tian , A. Timmons , D. Tinsley , S. C. Tognini , R. Toner , D. Torretta , I. Trostin , G. Tzanakos , J. Urheim , P. Vahle , K. Vaziri , E. Villegas , B. Viren , G. Vogel , R. C. Webber , A. Weber , R. C. Webb , A. Wehmann , C. White , L. Whitehead , L. H. Whitehead , S. G. Wojcicki , M. L. Wong-Squires , T. Yang , F. X. Yumiceva , V. Zarucheisky , R. Zwaska

For Project X, it is planned to inject a beam of 3 10**11 particles per bunch into the Main Injector. To prepare for this by studying the effects of higher intensity bunches in the Main Injector it is necessary to perform coalescing at 8…

Accelerator Physics · Physics 2013-02-01 D. J. Scott , D. Capista , B. Chase , J. Dye , I. Kourbanis , K. Seiya , M. -J. Yang

A two-year Large Aperture Quadrupole (WQB) Project was completed in the summer of 2006 at Fermilab. Nine WQBs were designed, fabricated and bench-tested by the Technical Division. Seven of them were installed in the Main Injector and the…

In this paper, we describe a harmonic kicker system used in the beam exchange scheme for the Circulator Cooling Ring (CCR) of the Jefferson Lab Electron Ion Collider(JLEIC). By delivering an ultra-fast deflecting kick, a kicker directs…

Accelerator Physics · Physics 2021-06-30 Gunn Tae Park , Jiquan Guo , Shaoheng Wang , Robert A. Rimmer , Haipeng Wang

A double kicker system which extracts the ultra-low emittance multi-bunch beam stably from ATF damping ring was developed. The performance of the system was studied comparing an orbit jitter with single kicker extraction in single bunch…

Accelerator Physics · Physics 2007-05-23 T. Imai , K. Nakai , H. Hayano , J. Urakawa , N. Terunuma

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 GSI Unilac was upgraded as a high current injector for the SIS in 1999. Therefore, the stripping section [1] at 1.4 MeV/u, where a beam transport under highest space charge conditions and multi beam operation had to be established, was…

Accelerator Physics · Physics 2007-05-23 W. Barth , P. Forck