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Related papers: Synchronization of the Fermilab Booster and Main I…

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The Main Injector (MI) was commissioned using data acquisition systems developed for the Fermilab Main Ring in the 1980s. New VME-based instrumentation was commissioned in 2006 for beam loss monitors (BLM)[2], which provided a more…

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

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 Neutrinos at the Main Injector (NuMI) facility at Fermilab began operations in late 2004. NuMI will deliver an intense muon neutrino beam of variable energy (2-20 GeV) directed into the Earth at 58 mrad for short (~1km) and long…

Accelerator Physics · Physics 2007-05-23 Sacha E. Kopp

The SPIN@FERMI collaboration has updated its 1991-95 Reports on the acceleration of polarized protons in Fermilab's Main Injector, which was commissioned by Fermilab. This Updated Report summarizes some updated Physics Goals for a 120-150…

One consequence of the application of superconductivity to accelerator construction is that the power consumption of accelerators will become much smaller. This raises the old possibility of using high energy protons to make neutrons which…

Accelerator Physics · Physics 2010-08-02 R. R. Wilson

The Neutrinos at the Main Injector (NuMI) facility at Fermilab is under construction and due to begin operations in late 2004. NuMI will deliver an intense $\nu_{\mu}$ beam of variable energy 2-20 GeV directed into the Earth at 58 mrad.…

High Energy Physics - Experiment · Physics 2008-11-26 Sacha E. Kopp

In synchrotron machines, the beam extraction is accomplished by a combination of septa and kicker magnets which deflect the beam from an accelerator into another. Ideally the kicker field must rise/fall in between the beam bunches. However,…

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

The Fermi National Accelerator Laboratory (Fermilab) Linac accepts 750 keV H- ions from the front end and accelerates them to 400 MeV for injection into the Booster rapid cycling synchrotron. Day-to-day drifts in the beam longitudinal…

Accelerator Physics · Physics 2024-07-25 R. Sharankova , A. Shemyakin , S. Rego

We have measured cross sections for forward neutron production from a variety of targets using proton beams from the Fermilab Main Injector. Measurements were performed for proton beam momenta of 58 GeV/c, 84 GeV/c, and 120 GeV/c. The cross…

The Neutrinos at the Main Injector (NuMI) beamline at Fermilab generates an intense muon neutrino beam for the NOvA (NuMI Off-axis $\nu_e$ Appearance) long-baseline neutrino experiment. Over the years, the NuMI beamline has been pivotal in…

Accelerator Physics · Physics 2024-12-18 D. A. A. Wickremasinghe , K. Yonehara

The Main Injector Neutrino Oscillation Search (MINOS) experiment's primary goal is the precision measurement of the neutrino oscillation parameters in the atmospheric neutrino sector. This long-baseline experiment uses Fermilab's NuMI beam,…

High Energy Physics - Experiment · Physics 2007-05-23 A. Habig , E. W. Grashorn

The measurement of the longitudinal behavior of the accelerated particle beams at Fermilab is crucial to the optimization and control of the beam and the maximizing of the integrated luminosity for the particle physics experiments.…

Instrumentation and Detectors · Physics 2011-10-19 R. Thurman-Keup , C. Bhat , W. Blokland , J. Crisp , N. Eddy , B. Fellenz , R. Flora , A. Hahn , S. Hansen , T. Kiper , A. Para , S. Pordes , A. V. Tollestrup

The Booster Neutrino Experiment (MiniBooNE) searches for numu-to-nue oscillations using the O(1 GeV) neutrino beam produced by the Booster synchrotron at the Fermi National Accelerator Laboratory (FNAL). The Booster delivers protons with 8…

High Energy Physics - Experiment · Physics 2013-05-29 MiniBooNE Collaboration

It is important to have experimental methods to estimate the maximum beam intensity for the Fermilab Booster as objective input into long term program commitments. An important existing limit is set by the available rf power. This limit is…

Accelerator Physics · Physics 2007-05-23 Xi Yang , James MacLachlan

The Neutrinos at the Main Injector (NuMI) beamline will deliver an intense muon neutrino beam by focusing a beam of mesons into a long evacuated decay volume. We have built 4 arrays of ionization chambers to monitor the neutrino beam…

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 Main Injector Neutrino Oscillation Search (MINOS) experiment uses an accelerator-produced neutrino beam to perform precision measurements of the neutrino oscillation parameters in the "atmospheric neutrino" sector associated with muon…

Instrumentation and Detectors · Physics 2010-05-12 MINOS Collaboration , D. G. Michael

The Main Injector Neutrino Oscillation search (MINOS) uses two detectors separated by 735km to measure a beam of neutrinos created by the Neutrinos at the Main Injector (NuMI) facility at Fermi National Accelerator Laboratory. The…

High Energy Physics - Experiment · Physics 2008-11-26 Michael Kordosky