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For Project X, it is planned to inject a beam of 3x10**11 particles per bunch into the Main Injector. Therefore, at 8-GeV, there will be increased space charge tune shifts and an increased incoherent tune spread. In preparation for these…

Accelerator Physics · Physics 2013-01-30 D. J. Scott , D. Capista , I. Kourbanis , K. Seiya , M. -J. Yang

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 2018-03-06 R. Thurman-Keup , M. Alvarez , J. Fitzgerald , C. Lundberg , P. Prieto , J. Zagel , W. Blokland

Fermilab is executing a technology development program to develop a compact yet powerful electron accelerator. We are leveraging R&D breakthroughs in SRF cavities, cost-effective radio-frequency sources, modern cryo-coolers, and high…

Accelerator Physics · Physics 2022-02-17 Jayakar Thangaraj

The IOTA Proton Injector (IPI), currently under installation at the Fermilab Accelerator Science and Technology facility (FAST), is a machine capable of delivering 20 mA pulses of protons at 2.5 MeV to the Integrable Optics Test Accelerator…

Accelerator Physics · Physics 2023-10-23 D. Edstrom , A. Romanov , D. Broemmelsiek , K. Carlson , J. -P. Carneiro , H. Piekarz , A. Shemyakin , A. Valishev

The Fermilab Accelerator Science and Technology (FAST) Facility at FNAL is a dedicated research and development center focused on advancing particle accelerator technologies for future applications worldwide. Currently, a key objective of…

Accelerator Physics · Physics 2025-11-26 Daniel R. MacLean , Dean R. Edstrom

We propose a low-cost and movable setup to probe minicharged particles (or milli-charged particles) using high-intensity proton fixed-target facilities. This proposal, FerMINI, consists of a milliQan-type detector, requiring…

High Energy Physics - Phenomenology · Physics 2019-08-07 Kevin J. Kelly , Yu-Dai Tsai

The Neutrinos at the Main Injector (NuMI) beam supplies an intense $\nu_{\mu}$ beam to the Main Injector Neutrino Oscillation Search (MINOS). The $\nu_{\mu}$'s are derived from a secondary $\pi^+$ beam that is allowed to decay within a 675…

The MINOS long baseline experiment has been collecting neutrino beam data since March 2005 and has accumulated 3 x 10^{20} protons-on-target (POT) to date. MINOS uses Fermilab's NuMI neutrino beam which is measured by two steel-scintillator…

High Energy Physics - Experiment · Physics 2007-06-13 Tobias M. Raufer

The Main Injector Particle Production (MIPP) experiment is a fixed target hadron production experiment at Fermilab. It measures particle production in interactions of 120 GeV/c primary protons from the Main Injector and secondary beams of…

High Energy Physics - Experiment · Physics 2019-08-15 Sonam Mahajan , Rajendran Raja

The MINOS Collaboration continues its search for $\nu_e$ appearance in the NuMI (Neutrinos at the Main Injector) beam at Fermilab. Neutrinos in the beam interact in the Near Detector, located 1 km from the beam source, allowing us to…

High Energy Physics - Experiment · Physics 2015-03-19 Mhair Orchanian

Over the next 6 years the CDF and D0 collaborations have the goal of collecting 15 fb-1 of data in collider Run II. This will require a number of ambitious upgrades to the Fermilab accelerator complex, some of which have been completed,…

High Energy Physics - Experiment · Physics 2007-05-23 Mike Church

Recent performance of Fermilab's Tevatron has exceeded this year's design goals and further accelerator upgrades are underway. The high-luminosity period which follows these improvements is known as Run IIb. The D0 experiment is in the…

High Energy Physics - Experiment · Physics 2019-08-14 Breese Quinn

I will present the status of the long baseline neutrino oscillation experiment MINOS at Fermi National Accelerator Laboratory (Fermilab). I will summarize the status of the detector and beam construction, the expected event rates and…

High Energy Physics - Experiment · Physics 2009-11-07 Milind V. Diwan

The Neutrinos at the Main Injector (NuMI) facility is a conventional horn-focused neutrino beam which produces muon neutrinos from a beam of mesons directed into a long evacuated decay volume. The relative alignment of the primary proton…

The Long Baseline Neutrino Experiment (LBNE) will utilize a beamline facility located at Fermilab to carry out a compelling research program in neutrino physics. The facility will aim a wide band beam of neutrinos toward a detector placed…

Accelerator Physics · Physics 2015-02-06 V. Papadimitriou , R. Andrews , J. Hylen , T. Kobilarcik , A. Marchionni , C. D. Moore , P. Schlabach , S. Tariq

The use of existing Fermilab facilities to provide beams for two muon experiments -- the Muon to Electron Conversion Experiment (Mu2e) and the New g-2 Experiment -- is under consideration. Plans are being pursued to perform these…

Accelerator Physics · Physics 2009-10-20 M. J. Syphers

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

Integrable optics is an innovation in particle accelerator design that provides strong nonlinear focusing while avoiding parametric resonances. One promising application of integrable optics is to overcome the traditional limits on…

Accelerator Physics · Physics 2017-03-20 Jeffrey Eldred , Alexander Valishev

MINOS is an accelerator neutrino oscillation experiment at Fermilab. An intense high energy neutrino beam is produced at Fermilab and sent to a near detector on the Fermilab site and also to a 5 kTon far detector 735 km away in the Soudan…

High Energy Physics - Experiment · Physics 2009-05-22 Milind V. Diwan

The difference between the rf voltage seen by the beam and the accelerating voltage required to match the rate of change of the Booster magnetic field is used to estimate the energy loss per beam turn. Because the rf voltage (RFSUM) and the…

Accelerator Physics · Physics 2007-05-23 Xi Yang , C. Ankenbrandt , J. Norem
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