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AbstractAbstract
[en] Beam stability issues of the VLHC rings in Phase 1 and Phase 2 are reviewed. For accelerator rings of circumference 232 km and beam pipe radius of the order of 1 cm, the impedance of the vacuum chamber is dominated by the resistive wall. The most dangerous instabilities are the single-bunch transverse mode coupling instability and the transverse coupled bunch instability driven by the resistive wall at sub-revolution frequency. Scaling is studied concerning the thresholds of these instabilities and the dominance of the resistive wall impedance as the size of the accelerator increases
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8 May 2001; 266 Kilobytes; AC02-76CH03000; Available from https://www.osti.gov/servlets/purl/780448-KQ66Dv/native/
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AbstractAbstract
[en] During polarized beam experiments, the 50 GeV proton synchrotron, proposed by the Institute of Nuclear Study of Japan, requires zero-dispersion straight sections. This will be implemented by turning on a special excitation of the quadrupoles resulting in a dispersion wave through the arcs of the machine. Aside from the inconvenience of the power supply, this special excitation also brings about unwanted high betatron functions and high dispersion functions, which will eventually limit the performance of the accelerator at high intensities. In this paper, dispersion suppressors are introduced. A new preliminary lattice that contains two straight sections with nonzero dispersion and two straight sections with zero dispersion is presented. The whole ring remains having a reasonable imaginary γt. The horizontal and vertical betatron functions have been kept to below 32.4 m and dispersion function between -0.52 and 1.86 m. The number of 6.2 m dipoles is reduced from 96 to 92, and the dipole field at 50 GeV will become slightly above 18 T. Some analysis of the new lattice is discussed. 10 refs., 9 figs., 1 tab
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Feb 1997; 27 p; CONTRACT AC02-76CH03000; Available from OSTI as DE97051895; NTIS; US Govt. Printing Office Dep
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AbstractAbstract
[en] Some issues are presented on the rf system in the future Fermilab prebooster, which accelerates 4 bunches each containing 0.25 x 1014 protons from 1 to 3 GeV kinetic energy. The problem of beam loading is discussed. The proposal of having a non-tunable fixed-frequency rf system is investigated. Robinson's criteria for phase stability are checked and possible Robinson instability growth is computed
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1 Jun 1998; 13 p; Workshop on Space Charge Physics in High Intensity Hadron Rings; Shelter Island, NY (United States); 4-7 May 1998; CONF--980567--; ON: DE98054542; BR: KA HEP; AC02-76CH03000; Also available from OSTI as DE00016630; PURL: https://www.osti.gov/servlets/purl/16630-gEIcUl/native/; Supercedes report DE98054542
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AbstractAbstract
[en] Space-charge effects on beam stabilities are studied for the proposed two-ring high-intensity Fermilab booster destined for the muon collider. This includes microwave instabilities and rf potential-well distortions. For the first ring, ferrite insertion is suggested to cancel the space-charge distortion of the rf wave form. To control the inductance of the ferrite during ramping and to minimize resistive loss, perpendicular biasing to saturation is proposed
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Apr 1998; 12 p; Front end of the muon colliders workshop; Batavia, IL (United States); 6-9 Nov 1997; CONF-971194--; CONTRACT AC02-76CH03000; ALSO AVAILABLE FROM OSTI AS DE98052816; NTIS; INIS; US GOVT. PRINTING OFFICE DEP
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Ng, K.-Y.; Trbojevic, D.
Fermi National Accelerator Lab., Batavia, IL (United States). Funding organisation: USDOE Office of Energy Research, Washington, DC (United States)1998
Fermi National Accelerator Lab., Batavia, IL (United States). Funding organisation: USDOE Office of Energy Research, Washington, DC (United States)1998
AbstractAbstract
[en] The lattice design of the 50-50 Gev muon collider is presented. Due to the short lifetime of the 50 GeV muons, the ring needs to be as small as possible. The 4 cm low betas in both planes lead to high betatron functions at the focusing quadrupoles and hence large chromaticities, which must be corrected locally. In order to maintain a low rf voltage of around 10 MV, the momentum-compaction factor must be kept to less than 10-2 , and therefore the flexible momentum-compaction modules are used in the arcs. The dynamical aperture is larger than 6 to 7 rms beam size for ±5 rms momentum offset. Comments are given and modifications are suggested
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Feb 1998; 10 p; 4. international conference on physics potential and development of muon-muon colliders; San Francisco, CA (United States); 10-12 Dec 1997; CONF-971215--; CONTRACT AC02-76CH03000; ALSO AVAILABLE FROM OSTI AS DE98052126; NTIS; US GOVT. PRINTING OFFICE DEP
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Lambertson, G.R.; Ng, K-Y.
California Univ., Berkeley (USA)1988
California Univ., Berkeley (USA)1988
AbstractAbstract
[en] The miscellaneous components of an accelerator may contribute a substantial or even dominant part of the interaction between beam and surroundings. We have estimated the beam impedances of a few of these components. When needed, we have added our own conceptions to the descriptions available at the Workshop on the RHIC Performance in order to make definite the calculations of impedance. These assumed parameters, while not unique, hopefully illustrate feasible and typical designs. 8 refs., 4 figs., 2 tabs
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May 1988; 13 p; Workshop on the relativistic heavy ion collider performance; Upton, NY (USA); 21-26 Mar 1988; CONF-880335--7; Available from NTIS, PC A03/MF A01; 1 as DE88014866; Portions of this document are illegible in microfiche products.
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Ostiguy, J.-F.; Ng, K.-Y.
Fermi National Accelerator Lab., Batavia, IL (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2000
Fermi National Accelerator Lab., Batavia, IL (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2000
AbstractAbstract
[en] During the course of the last decade, traveling wave accelerating structures for a future Linear Collider have been the object of intense R and D efforts. An important problem is the efficient computation of the long range wakefield with the ability to include small alignment and tuning errors. To that end, SLAC has developed an RF circuit model with a demonstrated ability to reproduce experimentally measured wakefields. The wakefield computation involves the repeated solution of a deterministic system of equations over a range of frequencies. By taking maximum advantage of the sparsity of the equations, they have achieved significant performance improvements. These improvements make it practical to consider simulations involving an entire linac (approximately 103 structures). One might also contemplate assessing, in real time, the impact of fabrication errors on the wakefield as an integral part of quality control
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14 Sep 2000; 86 Kilobytes; 20. International Linac Conference (LINAC 2000); Monterey, CA (United States); 21-25 Aug 2000; AC02-76CH03000; Available from PURL: https://www.osti.gov/servlets/purl/762224-0VOe2z/webviewable/
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AbstractAbstract
[en] The longitudinal and transverse impedances of an off-centered beam in a rectangular beampipe are solved exactly using conformal mapping. The results are represented in each case by the product of the corresponding impedance due to a circular beampipe with the beam at the center and a form factor that takes into account that the beampipe is rectangular in shape and that the beam is off center. When the width to height ratio of the beampipe is large, the form factor is found to stay flat for a wide range of beam displacement. Both effects due to the resistivity of the beampipe wall and to space charge are considered. (author)
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Journal Article
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Numerical Data
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Particle Accelerators; ISSN 0031-2460; ; v. 16(1-2); p. 63-80
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Chou, W.; Capista, D.; Griffin, J.; Ng, K.-Y.; Wildman, D.; Fermilab
Fermi National Accelerator Laboratory FNAL, Batavia, IL (United States). Funding organisation: US Department of Energy (United States)2007
Fermi National Accelerator Laboratory FNAL, Batavia, IL (United States). Funding organisation: US Department of Energy (United States)2007
AbstractAbstract
[en] Two barrier RF systems were fabricated, tested and installed in the Fermilab Main Injector. Each can provide 8 kV rectangular pulses (the RF barriers) at 90 kHz. When a stationary barrier is combined with a moving barrier, injected beams from the Booster can be continuously deflected, folded and stacked in the Main Injector, which leads to doubling of the beam intensity. This paper gives a report on the beam experiment using this novel technology
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1 Jun 2007; 3 p; PAC 2007: 22. IEEE Particle Accelerator Conference; Albuquerque, NM (United States); 25-29 Jun 2007; AC02-76CH03000; Available from http://lss.fnal.gov/cgi-bin/find_paper.pl?conf-07-347.pdf; PURL: https://www.osti.gov/servlets/purl/917843-Y6h0n6/
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AbstractAbstract
[en] In order to maintain a reasonable r.f. system, it may be necessary for a collider with ultra-short bunches to operate with a small slippage factor, for example, η<1 x 10-6 for all the particles in the bunches. The buckets dominated by the zeroth order, first order, or second order of η are examined, and the required r.f. voltages are computed. The problem of microwave instability is addressed. The reliability of computing higher-order momentum-compaction factor using lattice codes is examined. (orig.)
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19 refs.
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Journal Article
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Nuclear Instruments and Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment; ISSN 0168-9002; ; CODEN NIMAER; v. 404(2-3); p. 199-216
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