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AbstractAbstract
No abstract available
Original Title
Binding energies, rms radii, single-particle energies, deformations
Primary Subject
Record Type
Journal Article
Journal
Phys. Rev., C; v. 9(6); p. 2261-2271
Country of publication
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INIS VolumeINIS Volume
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AbstractAbstract
No abstract available
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Record Type
Journal Article
Journal
International Journal of Applied Radiation and Isotopes; v. 23(9); p. 407-413
Country of publication
ALPHA DECAY RADIOISOTOPES, ANTIMONY 122, ANTIMONY 124, ANTIMONY 125, ARGON 41, ARSENIC 74, ARSENIC 76, BARIUM 140, BETA PARTICLES, BETA SPECTRA, BIOLOGY, BROMINE 82, CALCIUM 46, CALCIUM 47, CARBON 11, CARBON 14, CERIUM 141, CERIUM 144, CESIUM 134, CESIUM 137, CHLORINE 36, CHROMIUM 49, COBALT 60, COPPER 61, COPPER 64, EUROPIUM 152, EUROPIUM 154, GALLIUM 68, GALLIUM 72, GERMANIUM 77, GOLD 194, INTERNAL CONVERSION RADIOISOTO, IODINE 130, IODINE 131, IODINE 132, IRIDIUM 192, IRON 59, KEV RANGE, KRYPTON 85, LANTHANUM 140, LEAD 210, LUTETIUM 176, LUTETIUM 177, MEDICINE, MERCURY 203, MEV RANGE 01-10, MOLYBDENUM 99, NIOBIUM 95, NITROGEN 13, OSMIUM 193, OXYGEN 15, PHOSPHORUS 32, POTASSIUM 43, PRASEODYMIUM 142, RUBIDIUM 86, SCANDIUM 47, SILVER 110, SILVER 111, SODIUM 22, SODIUM 24, STRONTIUM 90, SULFUR 35, TRITIUM, XENON 133, YTTRIUM 90, ZINC 65, ZIRCONIUM 96, ZIRCONIUM ISOTOPES
ANTIMONY ISOTOPES, ARGON ISOTOPES, ARSENIC ISOTOPES, BARIUM ISOTOPES, BETA DECAY RADIOISOTOPES, BETA-MINUS DECAY RADIOISOTOPES, BETA-PLUS DECAY RADIOISOTOPES, BROMINE ISOTOPES, CALCIUM ISOTOPES, CARBON ISOTOPES, CERIUM ISOTOPES, CESIUM ISOTOPES, CHARGED PARTICLES, CHLORINE ISOTOPES, CHROMIUM ISOTOPES, COBALT ISOTOPES, COPPER ISOTOPES, DAYS LIVING RADIOISOTOPES, ELECTRON CAPTURE RADIOISOTOPES, ENERGY RANGE, EUROPIUM ISOTOPES, EVEN-EVEN NUCLEI, EVEN-ODD NUCLEI, GALLIUM ISOTOPES, GERMANIUM ISOTOPES, GOLD ISOTOPES, HEAVY NUCLEI, HOURS LIVING RADIOISOTOPES, HYDROGEN ISOTOPES, INTERMEDIATE MASS NUCLEI, IODINE ISOTOPES, IRIDIUM ISOTOPES, IRON ISOTOPES, ISOMERIC TRANSITION ISOTOPES, ISOTOPES, KRYPTON ISOTOPES, LANTHANUM ISOTOPES, LEAD ISOTOPES, LIGHT NUCLEI, LUTETIUM ISOTOPES, MERCURY ISOTOPES, MEV RANGE, MINUTES LIVING RADIOISOTOPES, MOLYBDENUM ISOTOPES, NIOBIUM ISOTOPES, NITROGEN ISOTOPES, NUCLEI, ODD-EVEN NUCLEI, ODD-ODD NUCLEI, OSMIUM ISOTOPES, OXYGEN ISOTOPES, PHOSPHORUS ISOTOPES, POTASSIUM ISOTOPES, PRASEODYMIUM ISOTOPES, RADIOISOTOPES, RUBIDIUM ISOTOPES, SCANDIUM ISOTOPES, SECONDS LIVING RADIOISOTOPES, SILVER ISOTOPES, SODIUM ISOTOPES, SPECTRA, STABLE ISOTOPES, STRONTIUM ISOTOPES, SULFUR ISOTOPES, XENON ISOTOPES, YEARS LIVING RADIOISOTOPES, YTTRIUM ISOTOPES, ZINC ISOTOPES
Publication YearPublication Year
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Andres, R.Y.; Blattmann, H.
Eidgenoessisches Inst. fuer Reaktorforschung, Wuerenlingen (Switzerland)
Eidgenoessisches Inst. fuer Reaktorforschung, Wuerenlingen (Switzerland)
AbstractAbstract
[en] With the emergence of new, biological vehicles of great organ specificity (e.g. steroid hormones, antibodies) the concept of systemic tumor therapy with the aid of radiotherapeutica has gained new momentum. In order to assess the options open for optimal adaptation of the radiation properties to the pharmacocinetics of a vehicle, a search was done to identify potentially useful therapeutic radionuclides. Main criteria for selection were half life, low gamma-yield and stable daughter nuclide. The resulting possibilities fall into 4 categories: 1) alpha-emitters (At-211); 2) beta/sup -/-emitters that can be prepared in a carrierfree fashion (P-32, S-35, As-77, Y-90, Ag-111, Pm-149, Tb-161, Lu-177), 3) beta/sup -/-emitters with carrier added (Pd-109, Pr-142, Gd-159, Er-169, Tm-172, Yb-175, Re-188, Ir-194, Pt-197) and 4) electron capture nuclides, emitting Auger-cascades (Cr-51, Ga-67, Ge-71, Br-77, Ru-97, Sb-119, I-123, Cs-129, Nd-140, Er-165, Ta-177, Hg-197, Tl-201). Among the 4th group some well known, diagnostically used nuclides are found. Their therapeutic use necessitates the precise localisation in or very near the genetic material of the cell to be killed; only there the destructive power of the very short range Auger-electrons can be used. For each of the selected nuclides a summary of decay data, possibilities of preparation and chemical reactivity for labelling of vehicles is given. (author)
Original Title
Nuklide fuer nuklearmedizinische Therapie: Eine Uebersicht
Primary Subject
Secondary Subject
Source
Feb 1986; 81 p
Record Type
Report
Report Number
Country of publication
ANTIMONY 119, ARSENIC 77, ASTATINE 211, BROMINE 77, CESIUM 129, CHROMIUM 51, ERBIUM 165, ERBIUM 169, GADOLINIUM 159, GALLIUM 67, GERMANIUM 71, INTERNAL CONVERSION RADIOISOTO, IODINE 123, IRIDIUM 194, LUTETIUM 177, MERCURY 197, NEODYMIUM 140, NEOPLASMS, PALLADIUM 109, PHOSPHORUS 32, PLATINUM 197, PRASEODYMIUM 142, PROMETHIUM 149, RADIOISOTOPES, RADIOTHERAPY, RHENIUM 188, RUTHENIUM 97, SILVER 111, SULFUR 35, TANTALUM 177, TERBIUM 161, THALLIUM 201, THULIUM 172, YTTERBIUM 175, YTTRIUM 90
ALPHA DECAY RADIOISOTOPES, ANTIMONY ISOTOPES, ARSENIC ISOTOPES, ASTATINE ISOTOPES, BETA DECAY RADIOISOTOPES, BETA-MINUS DECAY RADIOISOTOPES, BETA-PLUS DECAY RADIOISOTOPES, BROMINE ISOTOPES, CESIUM ISOTOPES, CHROMIUM ISOTOPES, DAYS LIVING RADIOISOTOPES, DISEASES, ELECTRON CAPTURE RADIOISOTOPES, ERBIUM ISOTOPES, EVEN-EVEN NUCLEI, EVEN-ODD NUCLEI, GADOLINIUM ISOTOPES, GALLIUM ISOTOPES, GERMANIUM ISOTOPES, HEAVY NUCLEI, HOURS LIVING RADIOISOTOPES, INTERMEDIATE MASS NUCLEI, IODINE ISOTOPES, IRIDIUM ISOTOPES, ISOMERIC TRANSITION ISOTOPES, ISOTOPES, LIGHT NUCLEI, LUTETIUM ISOTOPES, MEDICINE, MERCURY ISOTOPES, MINUTES LIVING RADIOISOTOPES, NEODYMIUM ISOTOPES, NUCLEI, ODD-EVEN NUCLEI, ODD-ODD NUCLEI, PALLADIUM ISOTOPES, PHOSPHORUS ISOTOPES, PLATINUM ISOTOPES, PRASEODYMIUM ISOTOPES, PROMETHIUM ISOTOPES, RARE EARTH NUCLEI, RHENIUM ISOTOPES, RUTHENIUM ISOTOPES, SECONDS LIVING RADIOISOTOPES, SILVER ISOTOPES, SULFUR ISOTOPES, TANTALUM ISOTOPES, TERBIUM ISOTOPES, THALLIUM ISOTOPES, THERAPY, THULIUM ISOTOPES, YTTERBIUM ISOTOPES, YTTRIUM ISOTOPES
Publication YearPublication Year
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AbstractAbstract
[en] Complete text of publication follows. The shape isomers of light nuclei attract much attention from different structure studies, and provide a close connection to nuclear reactions as well. Superdeformed (SD) bands in 36Ar and 40Ca have been well-established through gamma-ray spectroscopy. In addition, candidate hyperdeformed states have been suggested from reaction studies. There has been considerable theoretical effort, recently, in considering superdeformed and other highly deformed configurations in 28Si. From the experimental side, there are a set of states in 28Si identified in the 12C(20Ne,α)28Si reaction which have been attributed to the superdeformed band by Kubono et al.. This sequence does not, however, have the smooth characteristics expected for such a band, and the moment of inertia is not in line with the result of a recent AMD calculation. Jenkins et al. have reviewed the available experimental data, and extended them with new γ-transitions. As a result they propose a new candidate for the SD band. Inspired by this exciting situation with open questions on the SD state, we have carried out an independent theoretical analysis of highly-deformed structures in 28Si. In particular we performed a Nilsson-calculation, combined with quasi-dynamical U(3) considerations, and determined the allowed binary clusterization of the shape isomers. We have found eight shape isomers ranging from the ground state up to a linear alphachain configuration (see Fig. 1). In searching for the allowed clusterizations the clusters were considered to have deformations, like the ground states of the corresponding nuclei, and no constraint was applied for their relative orientation. The alpha-like clusterizations proved to be energetically favoured. The hyperdeformed state allows only a single binary clusterization (of intrinsic ground state clusters): 20Ne+8Be, the ground state can have core+alpha, as well as core+8Be. The prolate and the superdeformed state allow several clusterizations. For the SD state, which is the focus of the present work, we find that the 4He+24Mg, and the 12C+16O cluster configurations are the most probable, taking account of both the selection rules and energetic preference. Our result on the SD state supports the new candidate state proposed by Jenkins et al.
Primary Subject
Source
4 refs.
Record Type
Journal Article
Journal
Country of publication
ALKALINE EARTH ISOTOPES, ALPHA DECAY RADIOISOTOPES, ARGON ISOTOPES, BERYLLIUM ISOTOPES, CALCIUM ISOTOPES, CARBON ISOTOPES, DEFORMATION, DEFORMED NUCLEI, EVEN-EVEN NUCLEI, HELIUM ISOTOPES, ISOTOPES, LIGHT NUCLEI, MAGNESIUM ISOTOPES, NEON ISOTOPES, NUCLEI, OXYGEN ISOTOPES, RADIOISOTOPES, SILICON ISOTOPES, SPECTROSCOPY, STABLE ISOTOPES
Publication YearPublication Year
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AbstractAbstract
[en] We propose a simple expression for nuclear densities, which brings out the following important nuclear properties: (i) shell effects in proton and neutron central densities, (ii) approximate global constancy of neutron central densities, (iii) approximate constancy of RNsup(-1/3) and Rsub(p)Zsup(-1/3) where R is the nuclear half-density radius and Rsub(p) is the rms radius of the proton density, (iv) larger surface thickness and rms radius for neutron density as compared to those for proton density. (orig.)
Primary Subject
Secondary Subject
Record Type
Journal Article
Literature Type
Numerical Data
Journal
Country of publication
CALCIUM 40, CHROMIUM 52, DENSITY, EVEN-EVEN NUCLEI, GOLD 197, INTERNAL CONVERSION RADIOISOTO, IRON 56, LEAD 208, MAGNESIUM 24, MILLISEC LIVING RADIOISOTOPES, NEODYMIUM 142, NEUTRON DENSITY, NICKEL 58, NIOBIUM 93, NUCLEAR MATTER, NUCLEAR RADII, NUCLEAR STRUCTURE, OXYGEN 16, PROTON DENSITY, SHELL MODELS, SILICON 28, SILVER 109, SPATIAL DISTRIBUTION, STRONTIUM 88, TELLURIUM 126, THEORETICAL DATA, TIN 116, TITANIUM 48, ZINC 64, ZIRCONIUM 90
CALCIUM ISOTOPES, CHROMIUM ISOTOPES, DATA, DISTRIBUTION, GOLD ISOTOPES, HEAVY NUCLEI, INFORMATION, INTERMEDIATE MASS NUCLEI, IRON ISOTOPES, ISOMERIC TRANSITION ISOTOPES, ISOTOPES, LEAD ISOTOPES, LIGHT NUCLEI, MAGNESIUM ISOTOPES, MATHEMATICAL MODELS, MATTER, NEODYMIUM ISOTOPES, NICKEL ISOTOPES, NIOBIUM ISOTOPES, NUCLEAR MODELS, NUCLEAR PROPERTIES, NUCLEI, NUMERICAL DATA, ODD-EVEN NUCLEI, OXYGEN ISOTOPES, PHYSICAL PROPERTIES, RADIOISOTOPES, RARE EARTH NUCLEI, SECONDS LIVING RADIOISOTOPES, SILICON ISOTOPES, SILVER ISOTOPES, STABLE ISOTOPES, STRONTIUM ISOTOPES, TELLURIUM ISOTOPES, TIN ISOTOPES, TITANIUM ISOTOPES, YEARS LIVING RADIOISOTOPES, ZINC ISOTOPES, ZIRCONIUM ISOTOPES
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Satyan, V.; Parikh, J.C.
Proceedings of the nuclear physics and solid state physics symposium, Chandigarh, 28 Dec 1972-1 Jan 1973
Proceedings of the nuclear physics and solid state physics symposium, Chandigarh, 28 Dec 1972-1 Jan 1973
AbstractAbstract
No abstract available
Primary Subject
Source
Department of Atomic Energy, Bombay (India). Physics Committee; p. 289-292; 1973; Department of Atomic Energy; Bombay; Nuclear physics and solid state physics symposium; Chandigarh, India; 28 Dec 1972
Record Type
Book
Literature Type
Conference
Country of publication
Publication YearPublication Year
Reference NumberReference Number
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INIS IssueINIS Issue
AbstractAbstract
[en] Electronic stopping powers of various light elements in Ti, Fe, Ni, Cu, Ag, and Au have been reported recently. Earlier, measurements were made for the stopping of 16O in Ni, Ag, and Au. With the aid of the Northcliffe-Schilling stopping-power tables these values were extrapolated to values of E/A equal to 0.0125 and 12.0 MeV/amu. Ranges calculated from these stopping-power values and the stopping powers themselves are presented
Primary Subject
Record Type
Journal Article
Journal
Atomic Data and Nuclear Data Tables; v. 20(5); p. 389-396
Country of publication
ALUMINIUM ISOTOPES, ARGON ISOTOPES, CALCIUM ISOTOPES, CHLORINE ISOTOPES, ELEMENTS, EVEN-EVEN NUCLEI, FLUORINE ISOTOPES, ISOTOPES, LIGHT NUCLEI, MAGNESIUM ISOTOPES, METALS, NEON ISOTOPES, NUCLEI, ODD-EVEN NUCLEI, OXYGEN ISOTOPES, PHOSPHORUS ISOTOPES, POTASSIUM ISOTOPES, RADIATION TRANSPORT, SILICON ISOTOPES, SODIUM ISOTOPES, STABLE ISOTOPES, SULFUR ISOTOPES, TRANSITION ELEMENTS
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Nichols, A.L.
UKAEA, Harwell. Atomic Energy Research Establishment
UKAEA, Harwell. Atomic Energy Research Establishment
AbstractAbstract
[en] An evaluation has been made of the decay data of 91 activation products and related nuclides. The resultant recommended data have been produced in ENDF/B-IV format for use in reactor calculation codes. The data include half-life, branching ratios, alpha, beta and gamma radiation energies and intensities, total decay energy, mean alpha, beta and gamma energies, internal conversion coefficients and associated uncertainties. Conversion electron, Auger electron, X-ray and internal bremsstrahlung data are also included. The alpha, beta and gamma radiation intensities are given as fractions, and all such data are the best estimate of the decay mode intensity per disintegration. In this report the data are presented in a clear form by means of an intermediary listing program. (author)
Secondary Subject
Source
Sep 1977; 235 p; ISBN 0 70 580388 0;
; Also available from H.M. Stationery Office, price Pound4.50

Record Type
Report
Report Number
Country of publication
ANTIMONY 122, ANTIMONY 124, ARGON 39, ARGON 41, BARIUM 133, BERYLLIUM 10, BROMINE 82, CALCIUM 41, CALCIUM 45, CARBON 14, CARBON 15, CESIUM 134, CESIUM 136, CHLORINE 36, CHLORINE 38, CHROMIUM 51, COBALT 57, COBALT 58, COBALT 60, COPPER 64, COPPER 66, DATA, DECAY, EUROPIUM 152, EUROPIUM 154, GOLD 198, HAFNIUM 175, HAFNIUM 181, INDIUM 115, INDIUM 116, INTERNAL CONVERSION RADIOISOTO, IODINE 126, IODINE 128, IRON 55, IRON 59, MAGNESIUM 27, MANGANESE 54, MANGANESE 56, MERCURY 197, MERCURY 203, MOLYBDENUM 93, NEUTRONS, NICKEL 59, NICKEL 63, NICKEL 65, NIOBIUM 93, NIOBIUM 94, NITROGEN 16, NUCLEAR DATA COLLECTIONS, OXYGEN 19, POTASSIUM 40, POTASSIUM 42, PROMETHIUM 145, RADIOACTIVATION, RADIOISOTOPES, REACTOR COMPONENTS, REACTOR MATERIALS, REACTORS, SCANDIUM 46, SCANDIUM 47, SCANDIUM 48, SILVER 110, SODIUM 22, SODIUM 24, SULFUR 35, TANTALUM 182, TERBIUM 157, TIN 121, TRITIUM, TUNGSTEN 181, TUNGSTEN 185, TUNGSTEN 187, YTTRIUM 88, ZINC 65
ANTIMONY ISOTOPES, ARGON ISOTOPES, BARIUM ISOTOPES, BARYONS, BERYLLIUM ISOTOPES, BETA DECAY RADIOISOTOPES, BETA-MINUS DECAY RADIOISOTOPES, BETA-PLUS DECAY RADIOISOTOPES, BROMINE ISOTOPES, CALCIUM ISOTOPES, CARBON ISOTOPES, CESIUM ISOTOPES, CHLORINE ISOTOPES, CHROMIUM ISOTOPES, COBALT ISOTOPES, COPPER ISOTOPES, DAYS LIVING RADIOISOTOPES, ELECTRON CAPTURE RADIOISOTOPES, ELEMENTARY PARTICLES, EUROPIUM ISOTOPES, EVEN-EVEN NUCLEI, EVEN-ODD NUCLEI, FERMIONS, GOLD ISOTOPES, HADRONS, HAFNIUM ISOTOPES, HEAVY NUCLEI, HOURS LIVING RADIOISOTOPES, HYDROGEN ISOTOPES, INDIUM ISOTOPES, INFORMATION, INTERMEDIATE MASS NUCLEI, IODINE ISOTOPES, IRON ISOTOPES, ISOMERIC TRANSITION ISOTOPES, ISOTOPES, LIGHT NUCLEI, MAGNESIUM ISOTOPES, MANGANESE ISOTOPES, MERCURY ISOTOPES, MINUTES LIVING RADIOISOTOPES, MOLYBDENUM ISOTOPES, NICKEL ISOTOPES, NIOBIUM ISOTOPES, NITROGEN ISOTOPES, NUCLEI, NUCLEONS, ODD-EVEN NUCLEI, ODD-ODD NUCLEI, OXYGEN ISOTOPES, POTASSIUM ISOTOPES, PROMETHIUM ISOTOPES, RARE EARTH NUCLEI, SCANDIUM ISOTOPES, SECONDS LIVING RADIOISOTOPES, SILVER ISOTOPES, SODIUM ISOTOPES, STABLE ISOTOPES, SULFUR ISOTOPES, TANTALUM ISOTOPES, TERBIUM ISOTOPES, TIN ISOTOPES, TUNGSTEN ISOTOPES, YEARS LIVING RADIOISOTOPES, YTTRIUM ISOTOPES, ZINC ISOTOPES
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AbstractAbstract
[en] Beams of 96- and 115-MeV α particles were used to study the giant resonance region in 27 nuclei ranging from 14N to 208Pb. A prominent broad (GAMMA=3--7 MeV) peak is present in the spectra at an excitation energy of approx.63/A1/3 MeV for all nuclei studied with A> or =36. No such prominent peak is apparent for A<32. The angular distributions of the peak are characterized by an oscillatory behavior which is quite different from the monotonic behavior of the background. Distorted wave calculations with L=2 reproduce the experimental angular distributions quite well for most of the nuclei. Energy-weighted sum rule fractions range from 30--50% for the lighter targets to near 100% for the heavier targets. Distorted wave calculations with a breathing mode (L=0) form factor fail to reproduce the observed resonance strength by about a factor of 3 for all targets. The width of the peak is smallest for the closed shell nuclei 40Ca, 90Zr, 144Sm, and 208Pb. A small but significant broadening is observed in the rare-earth region of deformed nuclei. The giant dipole resonance is not appreciably excited for any of the targets
Primary Subject
Record Type
Journal Article
Journal
Phys. Rev., C; v. 13(3); p. 994-1008
Country of publication
ALPHA REACTIONS, ALUMINIUM 27, ALUMINIUM 27 TARGET, ANGULAR DISTRIBUTION, ARGON 36, ARGON 36 TARGET, ARGON 40, ARGON 40 TARGET, CALCIUM 40, CALCIUM 40 TARGET, COBALT 59, COBALT 59 TARGET, ELASTIC SCATTERING, GIANT RESONANCE, IRON 56, IRON 56 TARGET, LEAD 208, LEAD 208 TARGET, MEV RANGE 10-100, MOLYBDENUM 100, MOLYBDENUM 100 TARGET, MOLYBDENUM 94, MOLYBDENUM 94 TARGET, MOLYBDENUM 96, MOLYBDENUM 96 TARGET, NEODYMIUM 142, NEODYMIUM 142 TARGET, NEON 20, NEON 20 TARGET, NICKEL 58, NICKEL 58 TARGET, NICKEL 60, NICKEL 60 TARGET, NITROGEN 14, NITROGEN 14 TARGET, OXYGEN 16, OXYGEN 16 TARGET, PRASEODYMIUM 141, PRASEODYMIUM 141 TARGET, SAMARIUM 144, SAMARIUM 144 TARGET, SAMARIUM 148, SAMARIUM 148 TARGET, SAMARIUM 154, SAMARIUM 154 TARGET, SILICON 28, SILICON 28 TARGET, SULFUR 32, SULFUR 32 TARGET, TERBIUM 159, TERBIUM 159 TARGET, TITANIUM 48, TITANIUM 48 TARGET, YTTERBIUM 174, YTTERBIUM 174 TARGET, ZINC 66, ZINC 66 TARGET, ZIRCONIUM 90, ZIRCONIUM 90 TARGET
ALUMINIUM ISOTOPES, ARGON ISOTOPES, CALCIUM ISOTOPES, COBALT ISOTOPES, DISTRIBUTION, ENERGY RANGE, EVEN-EVEN NUCLEI, HEAVY NUCLEI, INTERMEDIATE MASS NUCLEI, IRON ISOTOPES, ISOMERIC TRANSITION ISOTOPES, ISOTOPES, LEAD ISOTOPES, LIGHT NUCLEI, MEV RANGE, MOLYBDENUM ISOTOPES, NEODYMIUM ISOTOPES, NEON ISOTOPES, NICKEL ISOTOPES, NITROGEN ISOTOPES, NUCLEAR REACTIONS, NUCLEI, ODD-EVEN NUCLEI, ODD-ODD NUCLEI, OXYGEN ISOTOPES, PRASEODYMIUM ISOTOPES, RADIOISOTOPES, RARE EARTH NUCLEI, RESONANCE, SAMARIUM ISOTOPES, SCATTERING, SILICON ISOTOPES, STABLE ISOTOPES, SULFUR ISOTOPES, TARGETS, TERBIUM ISOTOPES, TITANIUM ISOTOPES, YTTERBIUM ISOTOPES, ZINC ISOTOPES, ZIRCONIUM ISOTOPES
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DeWitt, R.
Mound Facility, Miamisburg, OH (USA)
Mound Facility, Miamisburg, OH (USA)
AbstractAbstract
[en] The recognized need for high purity radionuclides and the need for organ specific radiopharmaceuticals will stimulate the demand for large quantities of stable isotopes. Stable isotopes currently under investigation for use as targets for radionuclide production include: 9598100Mo, 203205Tl, 201Hg, 6667Zn, 122123Te, 112Sn, 111112Cd, 50Cr, 50V, 82Kr, 197Au, 7274Ge, 5458Fe, 63Cu, 64Ni, 69Ga, 4346Ca, 41K, 35Cl, 23Na, 81Br, 84Sr, 85Rb, 75As, 76Se, 81Br, 31P, 29Si, 156Dy, 152Sm, 170Er, 175Lu, 178Lu, 168Yb, 11B, 14N, 16O, 20Ne, and 124Xe. As isotope production and radiopharmaceutical preparation costs are lowered and FDA approvals are secured, increased demand could develop for most of the stable isotopes listed. Requirements appear to be increasing for isotopes of those elements which are considered biologically essential (currently 25 elements) or for those which have an effect on the life processes. Demand is currently developing for the isotopes of the elements; K, Ca, Mg, Fe, Cu, Zn, Ni, Cd, and Cr. High isotope costs, however, and the scarcity of some metal isotopes have severely limited biomedical research programs
Original Title
New stable isotopes for clinical use and use in beomedical research
Primary Subject
Secondary Subject
Source
18 Apr 1979; 63 p; Available from NTIS., PC A04/MF A01
Record Type
Report
Report Number
Country of publication
ARSENIC 75, BIOCHEMISTRY, BIOLOGY, BORON 11, BROMINE 81, CADMIUM 111, CADMIUM 112, CALCIUM 43, CALCIUM 46, CHEMICAL PREPARATION, CHLORINE 35, CHROMIUM 50, COPPER 63, DYSPROSIUM 156, ERBIUM 170, GALLIUM 69, GERMANIUM 72, GERMANIUM 74, GOLD 197, INTERNAL CONVERSION RADIOISOTO, IRON 54, IRON 58, ISOTOPE APPLICATIONS, ISOTOPE PRODUCTION, KRYPTON 82, LUTETIUM 175, LUTETIUM 178, MEDICINE, MERCURY 201, MOLYBDENUM 100, MOLYBDENUM 95, MOLYBDENUM 98, NEON 20, NICKEL 64, NITROGEN 14, NUCLEAR MEDICINE, OXYGEN 16, PHOSPHORUS 31, PHYSIOLOGY, POTASSIUM 41, RADIOPHARMACEUTICALS, RUBIDIUM 85, SAMARIUM 152, SELENIUM 76, SILICON 29, SODIUM 23, STRONTIUM 84, TELLURIUM 122, TELLURIUM 123, THALLIUM 203, THALLIUM 205, TIN 112, USES, VANADIUM 50, XENON 124, YTTERBIUM 168, ZINC 66, ZINC 67
ARSENIC ISOTOPES, BETA DECAY RADIOISOTOPES, BETA-MINUS DECAY RADIOISOTOPES, BORON ISOTOPES, BROMINE ISOTOPES, CADMIUM ISOTOPES, CALCIUM ISOTOPES, CHEMISTRY, CHLORINE ISOTOPES, CHROMIUM ISOTOPES, COPPER ISOTOPES, DAYS LIVING RADIOISOTOPES, DRUGS, DYSPROSIUM ISOTOPES, ELECTRON CAPTURE RADIOISOTOPES, ERBIUM ISOTOPES, EVEN-EVEN NUCLEI, EVEN-ODD NUCLEI, GALLIUM ISOTOPES, GERMANIUM ISOTOPES, GOLD ISOTOPES, HEAVY NUCLEI, INTERMEDIATE MASS NUCLEI, IRON ISOTOPES, ISOMERIC TRANSITION ISOTOPES, ISOTOPES, KRYPTON ISOTOPES, LABELLED COMPOUNDS, LIGHT NUCLEI, LUTETIUM ISOTOPES, MERCURY ISOTOPES, MINUTES LIVING RADIOISOTOPES, MOLYBDENUM ISOTOPES, NEON ISOTOPES, NICKEL ISOTOPES, NITROGEN ISOTOPES, NUCLEI, ODD-EVEN NUCLEI, ODD-ODD NUCLEI, OXYGEN ISOTOPES, PHOSPHORUS ISOTOPES, POTASSIUM ISOTOPES, RADIOACTIVE MATERIALS, RADIOISOTOPES, RARE EARTH NUCLEI, RUBIDIUM ISOTOPES, SAMARIUM ISOTOPES, SECONDS LIVING RADIOISOTOPES, SELENIUM ISOTOPES, SILICON ISOTOPES, SODIUM ISOTOPES, STABLE ISOTOPES, STRONTIUM ISOTOPES, SYNTHESIS, TELLURIUM ISOTOPES, THALLIUM ISOTOPES, TIN ISOTOPES, VANADIUM ISOTOPES, XENON ISOTOPES, YTTERBIUM ISOTOPES, ZINC ISOTOPES
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