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AbstractAbstract
[en] CRYRING, which was proposed in October 1983, aims at a facility for performing experimental atomic, molecular and nuclear structure physics using very heavy, highly charged ions. In particular the possibility to study the interaction between a circulating heavy ion beam (proportional(1-5).109 ions) and beams of ions, electrons or photons is foreseen. An extracted beam (10 Hz, 30% duty cycle, proportional(1-5) pnA) with an energy around or slightly above the Coulomb barrier will allow experiments in atomic and nuclear structure physics. (orig.)
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Poth, H. (ed.); Kernforschungszentrum Karlsruhe G.m.b.H. (Germany, F.R.). Inst. fuer Kernphysik; 451 p; Jul 1984; p. 429-436; Workshop on electron cooling and related applications (ECOOL 1984); Karlsruhe (Germany, F.R.); 24-26 Sep 1984
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ARGON IONS, BEAM BENDING MAGNETS, BEAM EXTRACTION, BEAM FOCUSING MAGNETS, BEAM INJECTION, BEAM TRANSPORT, GEV RANGE 01-10, HEXAPOLES, ION BEAMS, KRYPTON IONS, LEAD IONS, MAGNETIC DIPOLES, MEV RANGE 100-1000, MHZ RANGE 01-100, MULTICHARGED IONS, QUADRUPOLES, RF SYSTEMS, STORAGE RINGS, VACUUM SYSTEMS, XENON IONS
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AbstractAbstract
[en] The CRYRING project was put forward by the Research Institute of Physics (AFI), Stockholm, Sweden, as a proposal in October 1983 under the heading A facility with CRYSIS and other ion sources connected to a synchrotron ring intended for studies of atomic, molecular and nuclear collisions, in particular in experiments with interacting beams of ions, molecules, electrons and laser photons. In September 1985 funding was granted for the last subproject, comprising the actual ring structure to be completed by 1989-90. Thus started the third Swedish storage ring project, the first being the synchrotron radiation electron ring MAX at Lund and the second the nuclear and particle physics light ion ring CELSIUS at Uppsala. The present short contribution aims at a pedagogical (though necessarily somewhat superficial) presentation of CRYRING and its modes of operation. 21 references, 5 figures
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Brouillard, F. (ed.); p. 453-462; 1986; p. 453-462; Plenum Publishing Corporation; New York, NY (USA); NATO advanced study institute on physics of electron-ion and ion-ion collisions; Han sur Lesse (Belgium); 30 Sep - 12 Oct 1985
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AbstractAbstract
[en] A synchrotron-storage ring for very highly charged heavy ions is under construction at the Research Institute of Physics in Stockholm. A short technical description of the ring and its injector is given. (orig.)
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Workshop and symposium on the physics of low-energy stored and trapped particles; Stockholm (Sweden); 14-18 Jun 1987
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Journal Article
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Physica Scripta. T; ISSN 0281-1847; ; v. 22 p. 282-285
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BEAM BENDING MAGNETS, BEAM FOCUSING MAGNETS, BEAM MONITORING, BEAM TRANSPORT, CAMAC SYSTEM, CAVITY RESONATORS, CONTROL SYSTEMS, CRYOGENICS, ELECTRON BEAM ION SOURCES, ELECTRON COOLING, HEAVY ION ACCELERATORS, ION BEAM INJECTION, ION BEAMS, ION SOURCES, MAGNETIC DIPOLES, PDP COMPUTERS, POWER SUPPLIES, QUADRUPOLE LINACS, QUADRUPOLES, REMOTE CONTROL, RF SYSTEMS, STORAGE RINGS, SYNCHROTRONS, ULTRAHIGH VACUUM, VACUUM SYSTEMS
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AbstractAbstract
[en] Using the 204Hg(α, pn)-reaction and α-particles of energies 39-55 MeV, we have found an isomeric 3.6 min 12- state in 206Tl at 2,642.9 keV. The 12- state decays mainly by an E5 transition of energy 1,021.4 keV to a 7+ state at 1,621.5 keV. There is, in addition, evidence for a weak 565 keV M4 branch to an 8+ state at 2,078 keV. The 7+ state decays by a stretched cascade of γ-rays to states of the following values of Jsub(π) and excitation energy: 5+, 1,405.4 keV; 4-, 952.1 keV; 2-, 265.8 keV and 0-, 0 keV. From the nuclear masses of 208Pb, 207Pb, 207Tl, and 206Tl and the experimental excitation energies it is possible to obtain the proton hole - neutron hole interaction in 206Tl. This interaction is compared with the calculations of Kuo and Herling and the discrepancies are discussed. (orig./BJ)
[de]
Unter Verwendung der 204Hg(α, pn)-Reaktion und α-Teilchen von Energien von 39-55 MeV, haben wir einen isomeren 3,6 min 12- Zustand in 206Tl bei 2.642,9 KeV gefunden. Der 12- Zustand zerfaellt hauptsaechlich durch einen E5 Uebergang von 1.021,4 keV auf einen 7+ Zustand bei 1.621,5 keV. Zusaetzlich gibt es einen Beweis fuer einen schwachen 565 keV M4 Uebergang auf einen 8+ Zustand bei 2.078 keV. Der 7+ Zustand zerfaellt durch eine Kaskade von γ-Strahlen auf Zustaende mit folgenden Jsub(π) Werten und Anregungsenergien: 5+, 1.405,4 keV; 4-, 952,1 keV; 2-, 265,8 KeV und 0-, 0 keV. Aus den Kernmassen von 208Pb, 207Pb, 207Tl und 206 Tl und den experimentellen Anregungsenergien ist es moeglich die Proton Loch - Neutron Loch Wechselwirkung in 206Tl zu erhalten. Diese Wechselwirkung wird mit den Rechnungen von Kuo und Herling verglichen und die Abweichungen werden diskutiert. (orig./BJ)Primary Subject
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8 figs.; 3 tabs.; 20 refs.
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Journal Article
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Z. Phys., A; v. 278(3); p. 257-264
Country of publication
ANGULAR MOMENTUM, BARYONS, BETA DECAY RADIOISOTOPES, BETA-MINUS DECAY RADIOISOTOPES, CATIONS, CHARGED PARTICLES, ELEMENTARY PARTICLES, ENERGY LEVELS, ENERGY RANGE, ENERGY-LEVEL TRANSITIONS, FERMIONS, HADRONS, HEAVY NUCLEI, HYDROGEN IONS, HYDROGEN IONS 1 PLUS, IONS, ISOTOPES, MEV RANGE, MINUTES LIVING RADIOISOTOPES, NUCLEAR CASCADES, NUCLEAR REACTIONS, NUCLEI, NUCLEONS, ODD-ODD NUCLEI, PARTICLE PROPERTIES, RADIOISOTOPES, SPECTRA, TARGETS, THALLIUM ISOTOPES
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Herrlander, C.J.; Hildingsson, L.; Johnson, A.
International conference on nuclear behaviour at high angular momentum. Contributions, Strasbourg, 22-24 April 19801980
International conference on nuclear behaviour at high angular momentum. Contributions, Strasbourg, 22-24 April 19801980
AbstractAbstract
No abstract available
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Strasbourg-1 Univ., 67 (France). Centre de Recherches Nucleaires; 180 p; Apr 1980; p. 41-42; International conference on nuclear behaviour at high angular momentum; Strasbourg, France; 22 - 24 Apr 1980; Published in summary form only.
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Miscellaneous
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AbstractAbstract
[en] The status of the CRYRING project is reviewed. Parameters for the main rings, magnets, acceleration system, and the electron cooler are given
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International symposium on electron beam ion sources and their applications; Upton, NY (USA); 14-18 Nov 1988; CONF-881154--
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AbstractAbstract
[en] This paper reports on CRYRING a project aiming at a facility for research in atomic, molecular and nuclear physics using a cryogenic electron-beam ion source CRYSIS together with an RFQ linear accelerator as injector into a synchrotron-storage ring for very highly charged, heavy ions. (CRYSIS stands for Cryogenic Stockholm Ion Source and CRYRING for Crysis-Synchrotron-Storage-Ring). The lay-out of a first phase of the planned facility is presented. At the ring research programs on photon-ion, electron-ion and atom/ion-ion interactions will be possible over a wide range of relative energies and particle species. The quality of the beam of circulating ions will be improved by electron cooling. In a second phase CRYRING will be equipped with a high-voltage (around 300 kV) ion accelerator as an alternative injection but also as the second source needed for atom/ion-ion collision experiments. An extracted beam is also planned for this phase
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Tazzari, S; 1545 p; ISBN 9971-50-642-4; ; 1988; p. 350; World Scientific Pub. Co; Teaneck, NJ (USA); 1. European particle accelerator conference (EPAC-1); Rome (Italy); 7-11 Jun 1988; CONF-880695--; World Scientific Pub. Co., 687 Hartwell Street, Teaneck, NJ 07666 (USA)
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Book
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AbstractAbstract
[en] Using α-particles in the energy range 42-51 MeV, the 209Bi(α,4n)209At reaction was studied with the intention of investigating the properties of excited high spin states in 209At. In-beam prompt and delayed gamma-ray and conversion electron spectroscopy reveal two isomeric states at 2,429 and 1,428 keV having the half-lives of 875 +- 100 ns and 25 +- 1 ns, respectively. The spins and parities of these states are found to be 29/2+ and 21/2-, respectively. The g-factors of the isomeric states are 1.06 +- 0.02 and 0.88 +- 0.06, which, within the experimental errors, are the same as the g-factors of the corresponding states in 211At. This suggests that the isomeric states are due to the π(h2sub(9/2))sub(8+)isub(13/2)ν(j-2)sub(0+) and π(h3sub(9/2))ν(j-2)sub(0+) configurations, respectively. The deviation between the calculated and experimentally found excitation energies of the isomeric levels are -146 +- 26 and +72 +- 26 keV. This deviation which in cases of a 208Pb-core usually is smaller than 15 keV, is likely to be due to the neglect of the interaction between two particles via the exchange of virtual 2+ phonons in the 206Pb core. This two-particle polarization interaction is found to be approximately described by a P2-force. (orig.)
[de]
Die 209Bi(α,4n)209At-Reaktion wurde mit Hilfe von α-Teilchen im Energiebereich 42-51 MeV in der Absicht untersucht, neue Informationen ueber die Eigenschaften angeregter Hochspinzustaende in 209At zu gewinnen. Die sofortige und verzoegerte γ- und Konversionselektronenspektroskopie entdeckt zwei isomere Zustaende bei 2.429 und 1.428 keV mit den Halbwertzeiten 875 +- 100 ns und 25 +- 1 ns. Als Spins und Paritaeten dieser Zustaende werden 29/2+ und 21/2- ermittelt. Die g-Faktoren der isomeren Zustaende sind 1,06 +- 0,02 und 0,88 +- 0,06 und entsprechen damit innerhalb der experimentellen Fehler den g-Faktoren der entsprechenden Zustaende in 211At, was die Vermutung nahelegt, dass die isomeren Zustaende auf der Konfiguration π(h2sub(9/2)sub(8+))isub(13/2)ν(j-2)sub(0+) bzw. π(h3sub(9/2))ν(j-2)sub(0+) beruhen. Die Abweichung zwischen den berechneten und den experimentell festgestellten Anregungsenergien der isomeren Zustaende betraegt -146 +- 26 und +72 +- 26 keV. Diese Abweichung, die fuer einen 208Pb-Kern gewoehnlich weniger als 15 keV betraegt, beruht wahrscheinlich auf der Nichtberuecksichtigung der Wechselwirkung zwischen zwei Teilchen ueber den Austausch virtuell vorhandener 2+-Phononen im 206Pb-Kern. Es wird festgestellt, dass diese Zwei-Teilchen-Polarisationswechselwirkung annaeherungsweise durch ein P2-Kraft beschrieben werden kann. (orig./AK)Primary Subject
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14 figs.; 4 tabs.; 25 refs.
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Journal Article
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Z. Phys., A; v. 273(3); p. 291-304
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ALPHA DECAY RADIOISOTOPES, ANGULAR MOMENTUM, ASTATINE ISOTOPES, BARYONS, BETA DECAY RADIOISOTOPES, DISTRIBUTION, ELECTRON CAPTURE RADIOISOTOPES, ELEMENTARY PARTICLES, ENERGY LEVELS, ENERGY RANGE, ENERGY-LEVEL TRANSITIONS, FERMIONS, HADRONS, HEAVY NUCLEI, HOURS LIVING RADIOISOTOPES, ISOTOPES, MEV RANGE, NUCLEAR REACTIONS, NUCLEI, NUCLEONS, ODD-EVEN NUCLEI, PARTICLE PROPERTIES, RADIOISOTOPES, SPECTRA, TARGETS
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Herrlander, C.J.; Bagge, L.; Barany, A.; Borg, S.; Danared, H.; Heikkinen, P.; Hultberg, S.; Liljeby, L.; Lindblad, T.
IEEE Transactions on Nuclear Science, Volume NS-32, No. 5. 1985 Particle accelerator conference. Accelerator engineering and technology1985
IEEE Transactions on Nuclear Science, Volume NS-32, No. 5. 1985 Particle accelerator conference. Accelerator engineering and technology1985
AbstractAbstract
[en] CRYRING is a facility for research in atomic, molecular and nuclear physics using a cryogenic electron beam ion source, CRYSIS, together with a RFQ linear accelerator as injector into a synchrotron ring, which can be used both for acceleration, deceleration and storage of very highly charged, heavy ions. (CRYRING stands for CRYsis-synchrotron-RING, RFQ for Radio Frequency Quadrupole and CRYSIS for CRYogenic Stockholm Ion Source.) A lay-out of CRYRING in an available laboratory area is shown. In the ring itself experiments with a circulating heavy ion beam and merged or crossed beams of electrons, laser-photons, neutrals and ions will be possible. Crossed ion beams will be available from a 400 kV accelerator. Injectors for negative (hydrogen) ions and electrons (intended for cooling as well as experiments) are included in the project. Regarding the extraction of accelerated heavy ions for nuclear and atomic spectroscopy, it should be emphasized that the project aims at very heavy ions (Xe-U) which will be energetic enough to overcome the Coulomb barrier of heavy target nuclei. The different injectors can be separately used for experiments when not in operation for CRYRING. It should also be emphasized that since CRYSIS is a pulsed ion source, beam-sharing will be simplified, making it possible to run two or perhaps even three different experiments simultaneously
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Shea, R.F. (ed.); Institute of Electrical and Electronics Engineers, Inc., New York (USA); p. 2718-2720; 1985; p. 2718-2720; Particle accelerator conference; Vancouver (Canada); 13-16 May 1985; IEEE, 345 East 47th St., New York, NY 10017
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Bagge, L.; Danared, H.; Ehrnsten, K.; Herrlander, C.J.; Hilke, J.; Nilsson, A.; Rensfelt, K.G.
Proceedings of the 3. European particle accelerator conference. V. 21992
Proceedings of the 3. European particle accelerator conference. V. 21992
AbstractAbstract
[en] CRYRING (Sweden) is an accelerator facility (synchrotron/storage ring) dedicated to low-energy research mainly using highly charged, heavy ions. The features of the main UHV components in the accelerator/storage ring of CRYRING are described. Using ion-pumps and NEG-pump modules, but without baking, a vacuum in the low 10-11 mbar region has been achieved in the 52 m circumference ring. Following some modifications, it is expected that the design value, the low 10-12 mbar region, will be reached. (R.P.) 7 refs.; 6 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.); [941 p.]; ISBN 2-86332-115-3; ; 1992; p. 1570-1572; Editions Frontieres; Paris (France); EPAC 92: 3. European particle accelerator conference; Berlin (Germany); 24-28 Mar 1992
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