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相关论文: Single/Few Bunch Space Charge Effects at 8-GeV in …

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For Project X, the Fermilab Main Injector will be required to operate with 3 times higher bunch intensity. The plan to study the space charge effects at the injection energy with intense bunches will be discussed.

加速器物理 · 物理学 2012-08-17 K. Seiya , B. Chase , J. Dey , P. Joireman , I. Kourbanis , A. Yagodnitsyna

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…

加速器物理 · 物理学 2013-02-01 D. J. Scott , D. Capista , B. Chase , J. Dye , I. Kourbanis , K. Seiya , M. -J. Yang

Detrimental beam dynamics effects limit performance of high intensity rapid cycling synchrotrons (RCS) such as the 8 GeV proton Fermilab Booster. Here we report the results of comprehensive experimental studies of various beam intensity…

加速器物理 · 物理学 2021-04-14 Jeff Eldred , Valeri Lebedev , Kiyomi Seiya , Vladimir Shiltsev

Fermilab has been working with the international particle physics and nuclear physics communities to explore and develop research programs possible with a new high intensity proton source known as "Project-X". Project X will provide…

高能物理 - 实验 · 物理学 2011-09-19 R. Tschirhart

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…

加速器物理 · 物理学 2012-08-17 J. Dey , I. Kourbanis

Currently, Fermilab Booster accelerates ~4.5E12 protons per pulse (ppp) in 81 bunches from 400 MeV to 8 GeV at 15 Hz to provide beam to multiple HEP experiments and is being upgraded to handle higher beam intensity >6.7E12 ppp at a…

加速器物理 · 物理学 2021-10-20 C. M. Bhat , N. Eddy

The next generation of high-energy physics experiments requires high intensity protons in the multi-GeV energy range for efficient production of secondary beams. The Fermilab long-term future requires an 8 GeV proton source to feed the Main…

加速器物理 · 物理学 2012-03-09 L. Jenner , C. Johnstone , D. Neuffer , J. Pasternak

The A0 Photoinjector at Fermilab can produce high charge (10-14 nC) electron bunches of low emittance (20 pi mm-mrad for 12 nC). We have undertaken a study of the optimal compression conditions. Off-crest acceleration in the 9-cell capture…

加速器物理 · 物理学 2007-05-23 M. J. Fitch , A. C. Melissinos , N. Barov , J. -P. Carneiro , H. T. Edwards , W. H. Hartung

Fermilab Booster synchrotron requires an intensity upgrade from 4.5x1012 to 6.5x1012 protons per pulse as a part of Fermilabs Proton Improvement Plan-II (PIP-II). One of the factors which may limit the high-intensity performance is the fast…

加速器物理 · 物理学 2022-08-10 S. A. K. Wijethunga , J. Eldred , C. Y. Tan , E. Pozdeyev

An overview is given of the methods and preliminary results from dedicated beam studies on three topics conducted over five days in July 2023. In the first study, the Fermilab Booster magnets were held constant at magnetic fields…

加速器物理 · 物理学 2024-08-20 Jeffrey Eldred , Michael Balcewicz , Frank Schmidt , Benjamin Simons

From 2005 through 2012, the Fermilab Main Injector provided intense beams of 120 GeV protons to produce neutrino beams and antiprotons. Hardware improvements in conjunction with improved diagnostics allowed the system to reach sustained…

The next generation of accelerators for Megawatt proton and heavy-ion beams moves us into a completely new domain of extreme specific energies of up to 0.1 MJ/g (Megajoule/gram) and specific power up to 1 TW/g (Terawatt/gram) in beam…

加速器物理 · 物理学 2014-09-02 N. V. Mokhov , S. R. Childress , A. I. Drozhdin , V. S. Pronskikh , D. Reitzner , I. S. Tropin , K. Vaziri

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,…

加速器物理 · 物理学 2013-02-01 D. J. Scott , D. Capista , I. Kourbanis , K. Seiya , M. -J. Yan

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…

加速器物理 · 物理学 2024-06-03 A. Pathak , O. Napoly , J. -F. Ostiguy

The Fermilab Booster - built more than 40 years ago - operates well above the design proton beam intensity of 4x10**12 ppp. Still, the Fermilab neutrino experiments call for even higher intensity of 5.5x10**12 ppp. A multitude of intensity…

加速器物理 · 物理学 2013-02-01 Y. Alexahin , N. Eddy , E. Gianfelice-Wendt , V. Lebedev , W. Marsh , W. Pellico , K. Triplett

The Project X Injector Experiment (PXIE), a test bed for the Project X front end, will be completed at Fermilab at FY12-16. One of the challenging goals of PXIE is demonstration of the capability to form a 1 mA H- beam with an arbitrary…

This paper presents the modeling of time-structured multiturn injection for an upgraded Main Injector with the 8-GeV Superconducting RF proton driver, or an ILC-style linac, or a Project-X linac. The Radio-Frequency mismatch between a linac…

加速器物理 · 物理学 2012-08-07 Phil S. Yoon , David E. Johnson , Weiren Chou

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…

加速器物理 · 物理学 2007-05-23 R. Zwaska , S. Kopp , W. Pellico , R. Webber

Fermilab Booster synchrotron requires an intensity upgrade from 4.5x1012 to 6.5x1012 protons per pulse as a part of Fermilab's Proton Improvement Plan-II (PIP-II). One of the factors which may limit the high-intensity performance is the…

加速器物理 · 物理学 2023-07-21 S. A. K. Wijethunga , N. Eddy , J. Eldred , C. Y. Tan , B. Fellenz , E. Pozdeyev , R. V. Sharankova

We discuss the progress made on a new installation in Fermilab's Main Injector that will help investigate the electron cloud phenomenon by making direct measurements of the secondary electron yield (SEY) of samples irradiated in the…

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