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AbstractAbstract
[en] A new approach for lithium drifting in silicon is described where the silicon devices under drift are held at constant temperature and bias at normal air ambient, and the drift process is terminated at the end of an estimated time depending upon the thickness of wafers. A 4-channel lithium drifting unit with electronically controlled oven has been constructed for this purpose. Full details of the fabrication procedure are given. A sizable number of Si(Li) detectors have been fabricated using this approach. The quality of the detectors is tested with 241Am alphas and conversion electrons from 209Bi and 137Cs sources. The detectors are regularly used for nuclear physics experiments at this Centre. (author)
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8 refs., 9 figures, 3 tables.
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ACTINIDE NUCLEI, ALPHA DECAY RADIOISOTOPES, AMERICIUM ISOTOPES, BETA DECAY RADIOISOTOPES, BETA-MINUS DECAY RADIOISOTOPES, BISMUTH ISOTOPES, CESIUM ISOTOPES, HEAVY NUCLEI, INTERMEDIATE MASS NUCLEI, ION SOURCES, ISOTOPES, LI-DRIFTED DETECTORS, MEASURING INSTRUMENTS, NUCLEI, ODD-EVEN NUCLEI, PARTICLE SOURCES, RADIATION DETECTORS, RADIATION SOURCES, RADIOISOTOPES, SEMICONDUCTOR DETECTORS, SI SEMICONDUCTOR DETECTORS, SPECTRA, STABLE ISOTOPES, TESTING, YEARS LIVING RADIOISOTOPES
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AbstractAbstract
[en] Ion-implanted phosphors were prepared by implanting Sb in CaS at 25 keV with concentration ranging from 0-05 to 0.2 per cent by weight. Samples of similar concentration were also prepared using the conventioal technique. The spectral response under UV excitation of both types of samples is compared. (author). 6 refs., 3 figs
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[en] A model for N-N interaction proposed earlier by Bhasin and Gupta (1985), has been extended to incorporate the tensor component of the nuclear force. Based on the quark compound bag model (QCB), the nucleon-nucleon potential has a short range repulsive core which is non-local and has a characteristic energy dependence and is expressed in terms of the parameters relating to the six-quark compound bag. To account for the low energy properties, this repulsive core interaction is supplemented by a phenomenological non-local potential containing both central (S-wave) and tensor components and operates only outside the QCB. Using this model, the results are analysed and compared wi th the experimental data for the electromagnetic form factors of the deuteron, the D-st ate observables, such as the quadrupole moment, the D-state probability, and the D/S ratio along with the n-p scattering phase shifts up to about 400 MeV . (author). 23 refs., 7 figs., 2 tabs
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Journal Article
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Numerical Data
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AbstractAbstract
[en] Energy migration and transfer from acriflavine to rhodamine B and malachite green in poly (methylmethacrylate) have been investigated using the decay function analysis. It is found that the influence of energy migration in energy transfer can be described quite convincingly by making use of the theories of Loring, Andersen and Fayer (LAF) and Huber. At high acceptor concentration direct donor-acceptor transfer occurs through Forster mechanism. (author). 17 refs., 5 figs
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Journal Article
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ACRIDINES, AMINES, AZINES, CARBOXYLIC ACIDS, DYES, EMISSION, ENERGY-LEVEL TRANSITIONS, ESTERS, FLAVINES, HETEROCYCLIC ACIDS, HETEROCYCLIC COMPOUNDS, LUMINESCENCE, MATERIALS, ORGANIC ACIDS, ORGANIC COMPOUNDS, ORGANIC NITROGEN COMPOUNDS, ORGANIC OXYGEN COMPOUNDS, ORGANIC POLYMERS, PHOTON EMISSION, POLYACRYLATES, POLYMERS, POLYVINYLS, PYRIDINES, REAGENTS, SPECTRA
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AbstractAbstract
[en] Excitation functions for the production of 68Ga, 67Ga, 66Ga, 65Ga + 65Zn and 61Cu from α-induced reactions in natural copper have been measured in the energy range ∼10-40 MeV using the stacked foil technique. A stack of nine copper foils was irradiated by a 40 MeV α-beam. The γ-rays emitted from the irradiated samples were recorded. Excitation functions have also been calculated theoretically using a statistical model with and without the inclusion of pre-equilibrium emission of particles. Pre-equilibrium component simulated by exciton model shows that the inclusion of pre-equilibrium emission gives better agreement between experimental and theoretical excitation functions. Pre-equilibrium fraction depends on the incident energy and the target mass number. (author). 26 refs., 15 figs., 3 tables
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Journal Article
Literature Type
Numerical Data
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ALPHA PARTICLES, ALPHA REACTIONS, COPPER, COPPER 61, COPPER 63 TARGET, COPPER 65 TARGET, CROSS SECTIONS, EXCITATION FUNCTIONS, EXCITON MODEL, EXPERIMENTAL DATA, FOILS, GALLIUM 65, GALLIUM 66, GALLIUM 67, GALLIUM 68, GAMMA SPECTRA, MEV RANGE 10-100, NEUTRONS, STATISTICAL MODELS, THEORETICAL DATA, ZINC 65
BARYONS, BETA DECAY RADIOISOTOPES, BETA-PLUS DECAY RADIOISOTOPES, CHARGED PARTICLES, COPPER ISOTOPES, DATA, DAYS LIVING RADIOISOTOPES, ELECTRON CAPTURE RADIOISOTOPES, ELEMENTARY PARTICLES, ELEMENTS, ENERGY RANGE, EVEN-ODD NUCLEI, FERMIONS, GALLIUM ISOTOPES, HADRONS, HELIUM IONS, HOURS LIVING RADIOISOTOPES, INFORMATION, INTERMEDIATE MASS NUCLEI, IONIZING RADIATIONS, IONS, ISOTOPES, MATHEMATICAL MODELS, METALS, MEV RANGE, MINUTES LIVING RADIOISOTOPES, NUCLEAR MODELS, NUCLEAR REACTIONS, NUCLEI, NUCLEONS, NUMERICAL DATA, ODD-EVEN NUCLEI, ODD-ODD NUCLEI, RADIATIONS, RADIOISOTOPES, SPECTRA, TARGETS, TRANSITION ELEMENTS, ZINC ISOTOPES
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[en] The data on the θsub(lab)=7deg excitation functions of 12C(15N,4He)23Na reaction between Esub(cm)=9.42 and 17.33 MeV for 28 states upto an excitation energy of 8.940 MeV in 23Na have been subjected to statistical analysis. In addition to statistical fluctuations, the results of the analysis indicate the existence of non-statistical structures at Esub(cm)=10.66, 10.93, 10.38, 12.62, 13.16, 15.32 and 16.18 MeV. (author). 57 refs., 4 figs
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[en] Excitation functions for the reaction 181Ta(α,xn)sup(185-x)Re, sup(107,109)Ag(α,ypxn) and 59Co(α,ypxn) were obtained from measurements of residual activity of stacked foils from thresold to 60 MeV. The excitation functions for the production of 181Re, 182Re, 183Re, 184Re, 105Ag, 111In, 54Mn, 56Co, 58Co and 60Co, are being presented. The experimental data are compared with calculations considering equilibrium as well as pre-equilibrium reactions according to the hybrid model of Blann. High energy part of the excitation functions is dominated by the pre-equilibrium reaction mechanism. Calculations were done using a priori calculational method of Overlaid Alice Code of Blann. Most of the excitation functions in the energy range mentioned above could be very well fitted with the hybrid model calculation for exciton number n=4 with nsub(p)=2 and nsub(n)=2. The overall agreement with theory is good. Certain discrepancies, however, indicate the necessity to revise the hybrid model with respect to emission of complex particles. (author). 33 refs., 13 figures
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Journal Article
Literature Type
Numerical Data
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ALPHA REACTIONS, COBALT 56, COBALT 59 TARGET, COBALT 60, CROSS SECTIONS, EXCITATION FUNCTIONS, EXPERIMENTAL DATA, INDIUM 111, INTERNAL CONVERSION RADIOISOTO, MEV RANGE 01-10, MEV RANGE 10-100, NEUTRONS, PROTONS, RHENIUM 181, RHENIUM 182, RHENIUM 183, RHENIUM 184, SILVER 105, SILVER 107 TARGET, SILVER 109 TARGET, TANTALUM 181 TARGET, THEORETICAL DATA
BARYONS, BETA DECAY RADIOISOTOPES, BETA-MINUS DECAY RADIOISOTOPES, BETA-PLUS DECAY RADIOISOTOPES, CATIONS, CHARGED PARTICLES, COBALT ISOTOPES, DATA, DAYS LIVING RADIOISOTOPES, ELECTRON CAPTURE RADIOISOTOPES, ELEMENTARY PARTICLES, ENERGY RANGE, FERMIONS, HADRONS, HEAVY NUCLEI, HOURS LIVING RADIOISOTOPES, HYDROGEN IONS, HYDROGEN IONS 1 PLUS, INDIUM ISOTOPES, INFORMATION, INTERMEDIATE MASS NUCLEI, IONS, ISOMERIC TRANSITION ISOTOPES, ISOTOPES, MEV RANGE, MINUTES LIVING RADIOISOTOPES, NUCLEAR REACTIONS, NUCLEI, NUCLEONS, NUMERICAL DATA, ODD-EVEN NUCLEI, ODD-ODD NUCLEI, RADIOISOTOPES, RHENIUM ISOTOPES, SILVER ISOTOPES, TARGETS, YEARS LIVING RADIOISOTOPES
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[en] Poincare gauge theory is derived from a linear theory by the method suggested by Gupta for deriving Einstein's general relativity from the linear theory of a spin-2 field. Nonlinearity is introduced by requiring that a set of tensor fields be coupled to the Noether currents of the Poincare group (energy-momentum and spin). (author)
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[en] In addition to the Kerr-Newman metric with cosmological constant several other metrics are presented giving Kerr-Newman type solutions of Einstein-Maxwell field equations in the background of deSitter universe. The electromagnetic field in all the solutions is assumed to be source-free. A new metric of what may be termed as an electrovac rotating deSitter space-time- a space-time devoid of matter but containing source-free electromagnetic field and a null fluid with twisting rays-has been presented. In the absence of the electromagnetic field, these solutions reduce to those discussed by Vaidya (1984). 8 refs. (author)
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[en] Some subtleties regarding regularizations in computing the soliton energy of degenerate systems are discussed. (author)
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