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Foelsche, H.; Hahn, H.
Brookhaven National Lab., Upton, N.Y. (USA)1972
Brookhaven National Lab., Upton, N.Y. (USA)1972
AbstractAbstract
No abstract available
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Source
24 Aug 1972; 6 p
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Pittman, R.N.
State Univ. of New York, Stony Brook (USA)1972
State Univ. of New York, Stony Brook (USA)1972
AbstractAbstract
No abstract available
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1972; 73 p; University Microfilms Order No. 72-16,967.; Thesis. (Ph.D.).
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Report
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Thesis/Dissertation
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Palmer, R.B.
Brookhaven National Lab., Upton, N.Y. (USA)1972
Brookhaven National Lab., Upton, N.Y. (USA)1972
AbstractAbstract
No abstract available
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Source
25 Aug 1972; 8 p
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AbstractAbstract
No abstract available
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Journal Article
Journal
Particles Nucl; v. 1(3); p. 220-227
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Lowenstein, D.I.
Brookhaven National Lab., Upton, N.Y. (USA)
Brookhaven National Lab., Upton, N.Y. (USA)
AbstractAbstract
[en] The typical AGS operating conditions are given, and the six antiproton beams and the one antineutron beam currently under test are described. Information on the following is given in tabular form: (1) the possible beam running configurations; (2) the status and availability of beams at the end of FY75; (3) a brief synopsis of the experiments that have gotten beam time during the present year; and (4) a description of new experiments which will use antiproton beams. (U.S.)
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nd; 19 p; 4. international symposium on nucleon-antinucleon interations; Syracuse, New York, USA; 2 May 1975; CONF-750547--3
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Conference
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Asseo, E.; Baird, S.; Bosser, J.; Chanel, M.; Lefevre, P.; Ley, R.; Maccaferri, R.; Manglunki, D.; Moehl, D.; Molinari, G.
Proceedings of the 3. European particle accelerator conference. V. 11992
Proceedings of the 3. European particle accelerator conference. V. 11992
AbstractAbstract
[en] A description is given of the recent performance of the LEAR storage ring. This includes the improvements made on the ultra-slow extraction (time structure, flux limitation), the progress on the semi-slow extraction (∼500 μs) at 61.2 MeV/c, and the results obtained from internal jet target operation at momenta higher than 800 MeV/c. (author) 8 refs.; 4 figs.; 1 tab
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Henke, H. (Technische Univ., Berlin (Germany). Inst. fuer Theoretische Elektrotechnik); Homeyer, H. (Hahn-Meitner-Institut Berlin GmbH (Germany)); Petit-Jean-Genaz, Ch. (eds.); [908 p.]; ISBN 2-86332-114-5;
; 1992; p. 447-449; Editions Frontieres; Paris (France); EPAC 92: 3. European particle accelerator conference; Berlin (Germany); 24-28 Mar 1992

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AbstractAbstract
[en] The CERN Antiproton Decelerator will deliver low energy beams to four experimental beam-lines installed within the accelerator circumference. The limited space available imposes tight constraints on the topology of the beam-lines needed by the experimental devices. In this paper, the general layout of the experimental area is reviewed. Furthermore, a discussion of the so-called measurement line for AD beam property measurements is included
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S0375947499002225; Copyright (c) 1999 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
Journal
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Johnson, C.D.; Jones, E.; Sherwood, T.R.
Proceedings of the 1987 IEEE particle accelerator conference: Accelerator engineering and technology1987
Proceedings of the 1987 IEEE particle accelerator conference: Accelerator engineering and technology1987
AbstractAbstract
[en] On completion of the ACOL project, the increased beam intensity in the Antiproton Accumulator, AA, will be derived from extensions to the transverse and longitudinal acceptances via the new Antiproton Collector ring being constructed around the AA. Each of these extensions should give a factor of 3 to 4 improvement, i.e. an overall gain of at least 10 in anti-proton yield. The increased transverse acceptance has necessitated a redesign of the antiproton target station, which will be equipped to function with various passive and active targets. The antiproton collector lens will be a lithium lens, but high-current magnetic horns and a plasma lens are also under development. At start-up in 1987 antiproton yields into the ACOL nominal acceptance, Δp/p=6%, Ah, AV = 200 mm-mrad, are expected to be as predicted. Target and collector lens lifetime limitations may make further gains more difficult than initially supposed, but if these can be overcome another factor of two is possible
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Lindstrom, E.R.; Taylor, L.S; 2030 p; 1987; p. 1749-1751; IEEE Service Center; Piscataway, NJ (USA); Particle accelerator conference; Washington, DC (USA); 16-19 Mar 1987; CONF-870302--
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AbstractAbstract
No abstract available
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Melissinos, A. C. (ed.); p. 214-225; 1971; American Inst. of Physics; New York; Meeting on particles and fields; Rochester, N. Y; 30 Aug 1971
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Book
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Krienen, F.
Proceedings of the workshop on producing high luminosity high energy proton-anti proton collisions1978
Proceedings of the workshop on producing high luminosity high energy proton-anti proton collisions1978
AbstractAbstract
[en] An electron cooling device is described in which the 100 MeV anti protons concentrate at the lower end of its momentum range. The spot size depends on the electron temperature
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California Univ., Berkeley (USA). Lawrence Berkeley Lab.; Fermi National Accelerator Lab., Batavia, IL (USA); p. 141-148; 1978; p. 141-148; p-p workshop; Berkeley, CA, USA; 27 - 31 Mar 1978
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