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Capitani, G.P.; De Sanctis, E.; Di Giacomo, P.; Guaraldo, C.; Lucherini, V.; Polli, E.; Reolon, A.R.; Scrimaglio, R.
Perspectives in nuclear physics at intermediate energies1984
Perspectives in nuclear physics at intermediate energies1984
AbstractAbstract
[en] Differential cross sections for the /sup 2/H(γ,p)n reaction were measured at five laboratory angles, from 320 to 1300, for photon energies between 100 and 250 MeV. The LEALE quasi-monochromatic photon beam, obtained at Frascati by positron annihilation on liquid hydrogen target, was used; the photon beam spectrum was measured on-line by a pair spectrometer. Preliminary values of angular distributions and total cross sections at three laboratory photon energies are presented
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Source
Anon; p. 152-159; ISBN 9971-966-32-8; ; 1984; p. 152-159; World Scientific Pub. Co; Teaneck, NJ (USA); Workshop on perspectives in nuclear physics at intermediate energies; Trieste (Italy); 10-14 Oct 1983
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Book
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Conference
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AbstractAbstract
[en] A sensitive profile and position monitor for low intensity positron (approx.= 10-9 A) and photon (approx.= 108 ν/s) beams is described. It consists of a multiwire chamber with two sensitive planes and additional electronic circuits. The display of the beam profiles, which appears on a standard oscilloscope, is live and quantitative, the effect of adjustments of the beam transport is immediately and continuously visible. (orig.)
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Journal Article
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Nucl. Instrum. Methods Phys. Res; ISSN 0029-554X; ; v. 203(1-3); p. 63-68
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[en] The determination of photonuclear cross sections requires a knowledge of the primary photon spectrum. The intensity and the energy spectrum of the Frascati positron annihilation photon beam have been measured by a Komar et al. type quantameter and a pair spectrometer. The present paper concerns the study and the design of the pair spectrometer. In section 2 the general layout of the facility is reported. In section 3 the main characteristics of the magnet are given. Section 4 is concerned with the optical properties of the spectrometer. The detection system, with the associated electronics, is described in section 5. In section 6 the calculation of the spectrometer response function is reported. In section 7 the experimental photon energy spectrum, at positron energy Esub(+) = 200 MeV, compared with the calculated one, is given. (orig.)
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Journal Article
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Numerical Data
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Nuclear Instruments and Methods; ISSN 0029-554X; ; v. 178(1); p. 61-69
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[en] All the 2H(γ,p)n data in the energy range 20--440 MeV have been fitted to a simple phenomenological function. All differential cross-section data were used: The bremsstrahlung data were normalized to the total cross-section values obtained by fitting data provided by monochromatic photon beams. The results obtained give a good representation of the experimental points
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Journal Article
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[en] All existing data on the level densities, decay widths and lifetimes of excited nuclei have been analyzed in the framework of the statistical model in order to better determine the parameters of the phenomenological systematics of the nuclear level density. Data on level densities of several hundred nuclides obtained in the excitation energy range from 2 up to 20 MeV were used. The level densities of nuclei with large deformation (at the saddle point) have been studied by analyzing the data on the neutron emission and fission partial width ratio Γn/Γf, and the values of the fission barrier heights Bf, the level density parameters ratio af/an and the saddle point shell corrections δWs.p. have been extracted. The influence of shell and collective effects on the level density and the decay widths of nuclei which have different excitation energies and deformations has been studied. (orig.)
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Journal Article
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Numerical Data
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ANTIMONY 113, ASTATINE 213, ASYMPTOTIC SOLUTIONS, BERKELIUM 247, BRANCHING RATIO, CALCIUM 41, CALIFORNIUM 248, COLLECTIVE MODEL, COMPOUND NUCLEI, CORRECTIONS, CURIUM 244, DE-EXCITATION, DEFORMED NUCLEI, ENERGY DEPENDENCE, ENERGY-LEVEL DENSITY, FISSION BARRIER, GAMMA DECAY, INDIUM 107, IRIDIUM 189, IRON 56, LEVEL WIDTHS, LIFETIME, LIQUID DROP MODEL, LUTETIUM 173, MAGNESIUM 24, MANGANESE 55, MENDELEVIUM 256, MILLISEC LIVING RADIOISOTOPES, NANOSEC LIVING RADIOISOTOPES, NEPTUNIUM 239, NEUTRON EMISSION, NICKEL 60, NOBELIUM 258, NUCLEAR DECAY, NUCLEAR DEFORMATION, NUCLEAR STRUCTURE, OSMIUM 186, OSMIUM 188, PHOSPHORUS 30, PLUTONIUM 238, PLUTONIUM 239, PLUTONIUM 241, POLONIUM 210, POLONIUM 212, RESONANCE, ROTATIONAL STATES, SHELL MODELS, SILICON 28, SPONTANEOUS FISSION, SPONTANEOUS FISSION RADIOISOTO, STATISTICAL MODELS, STATISTICS, SULFUR 33, TANTALUM 179, THALLIUM 201, THEORETICAL DATA, URANIUM 239
ACTINIDE NUCLEI, ALPHA DECAY RADIOISOTOPES, ANTIMONY ISOTOPES, ASTATINE ISOTOPES, BERKELIUM ISOTOPES, BETA DECAY RADIOISOTOPES, BETA-MINUS DECAY RADIOISOTOPES, BETA-PLUS DECAY RADIOISOTOPES, CALCIUM ISOTOPES, CALIFORNIUM ISOTOPES, CURIUM ISOTOPES, DATA, DAYS LIVING RADIOISOTOPES, DECAY, DEFORMATION, ELECTRON CAPTURE RADIOISOTOPES, EMISSION, ENERGY, ENERGY LEVELS, ENERGY-LEVEL TRANSITIONS, EVEN-EVEN NUCLEI, EVEN-ODD NUCLEI, EXCITED STATES, FISSION, HEAVY ION DECAY RADIOISOTOPES, HEAVY NUCLEI, HOURS LIVING RADIOISOTOPES, INDIUM ISOTOPES, INFORMATION, INTERMEDIATE MASS NUCLEI, IRIDIUM ISOTOPES, IRON ISOTOPES, ISOMERIC TRANSITION ISOTOPES, ISOTOPES, LIGHT NUCLEI, LUTETIUM ISOTOPES, MAGNESIUM ISOTOPES, MANGANESE ISOTOPES, MATHEMATICAL MODELS, MATHEMATICS, MENDELEVIUM ISOTOPES, MINUTES LIVING RADIOISOTOPES, NEPTUNIUM ISOTOPES, NICKEL ISOTOPES, NOBELIUM ISOTOPES, NUCLEAR MODELS, NUCLEAR REACTIONS, NUCLEI, NUMERICAL DATA, ODD-EVEN NUCLEI, ODD-ODD NUCLEI, OSMIUM ISOTOPES, PHOSPHORUS ISOTOPES, PLUTONIUM ISOTOPES, POLONIUM ISOTOPES, POTENTIAL ENERGY, RADIOISOTOPES, RARE EARTH NUCLEI, SECONDS LIVING RADIOISOTOPES, SILICON 32 DECAY RADIOISOTOPES, SILICON ISOTOPES, STABLE ISOTOPES, SULFUR ISOTOPES, TANTALUM ISOTOPES, THALLIUM ISOTOPES, URANIUM ISOTOPES, YEARS LIVING RADIOISOTOPES
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AbstractAbstract
[en] A Monte Carlo computing program has been used to calculate the photon spectrum and emittance from positron annihilation and bremsstrahlung. The positron energy spread, the energy loss and the multiple scattering in the annihilation target have been taken into account. Moreover, the positron emittance, the positron incidence angle and the finite angular acceptance of the photon collimation channel have been explicitly considered. Experimental results, obtained with a pair spectrometer and a beam profile monitor are in good agreement with calculations. In particular, it is shown that the positron emittance has a crucial influence on the shape of the photon spectrum and on the absolute value of the photon flux. (orig.)
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Journal Article
Literature Type
Numerical Data
Journal
Nucl. Instrum. Methods Phys. Res; ISSN 0029-554X; ; v. 203(1-3); p. 353-358
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ANGULAR DISTRIBUTION, ANNIHILATION, ATOMS, BREMSSTRAHLUNG, DIFFERENTIAL CROSS SECTIONS, ELECTRON-POSITRON COLLISIONS, ELECTRON-POSITRON INTERACTIONS, ELECTRONS, ENERGY LOSSES, ENERGY SPECTRA, GAMMA SPECTRA, HYDROGEN, INELASTIC SCATTERING, LIQUIDS, MEV RANGE 100-1000, MOLECULES, MONTE CARLO METHOD, MULTIPLE SCATTERING, PHOTONS, POSITRON BEAMS, POSITRON COLLISIONS, POSITRON-ATOM COLLISIONS, POSITRON-MOLECULE COLLISIONS, POSITRONS, THEORETICAL DATA
ANTILEPTONS, ANTIMATTER, ANTIPARTICLES, ATOM COLLISIONS, BEAMS, COLLISIONS, CROSS SECTIONS, DATA, DISTRIBUTION, ELECTROMAGNETIC RADIATION, ELECTRON COLLISIONS, ELEMENTARY PARTICLES, ELEMENTS, ENERGY RANGE, FERMIONS, FLUIDS, INFORMATION, INTERACTIONS, LEPTON BEAMS, LEPTON-LEPTON INTERACTIONS, LEPTONS, MASSLESS PARTICLES, MATTER, MEV RANGE, MOLECULE COLLISIONS, NONMETALS, NUMERICAL DATA, PARTICLE BEAMS, PARTICLE INTERACTIONS, RADIATIONS, SCATTERING, SPECTRA
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AbstractAbstract
[en] The best experimental conditions to perform photofission measurements in the energy range 100-300 MeV by using the Frascati annihilation photon beam are deduced. For nuclei with very low fission threshold energies it is shown to be advantageous to collect the photon beam at an angle deltasub(ν) > 10. For nuclei with high fission threshold energies, the annihilation photon contribution to the yield already pre-dominates for 0.50 <= deltasub(ν) <= 10. (orig.)
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Journal Article
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Nucl. Instrum. Methods Phys. Res; ISSN 0029-554X; ; v. 203(1-3); p. 227-233
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Anghinolfi, M.; Battaglieri, M.; Corvisiero, P.; De Vita, R.; Golovach, E.; Longhi, A.; Mokeev, V.; Ricco, G.; Ripani, M.; Sapunenko, V.; Taiuti, M.; Avakian, H.; Bianchi, N.; De Sanctis, E.; Gyuriyan, V.; Muccifora, V.; Mirazita, M.; Polli, E.; Reolon, A.R.; Ronchetti, F.; Rossi, P., E-mail: taiuti@ge.infn.it2000
AbstractAbstract
[en] The measurement of the response of the large-angle electromagnetic shower calorimeter (LAC) of the CLAS detector to minimum ionizing particles is reported. The experimental set-up and the adopted procedures are described. The results of the light attenuation length in the calorimeter, the light output and the resolution of the interaction point reconstruction are discussed. The performances of the LAC match well with those required
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Source
S0168900299012875; Copyright (c) 2000 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: Ukraine
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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. 447(3); p. 424-431
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[en] We describe the performance of the readout of the Jet-Target internal tagging system. The apparatus and methods to test signal transmission and time dispersion of 3.5 m fiber optic light guides, and time drift, gain measurement and rate effect of the phototubes are presented. (orig.)
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Journal Article
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Nuclear Instruments and Methods in Physics Research. Section A; ISSN 0168-9002; ; CODEN NIMAE; v. 311(1/2); p. 173-178
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[en] Differential cross sections for the d(γ,p)n reaction were measured at five laboratory angles, from 32deg to 130deg, and for seven photon energies (100, 120, 140, 180, 200, 220 and 255 MeV). A quasi-monochromatic photon beam was used and the photon spectrum was measured on-line with a pair spectrometer. The absolute normalization uncertainty is within ±5%. Data agree, taking into account total errors, with results of recent experiments with monochromatic photons. (author)
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Secondary Subject
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3. international symposium on mesons and light nuclei; Bechyne (Czechoslovakia); 27 May - 1 Jun 1985
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Journal Article
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Conference; Numerical Data
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