57 research outputs found
146Gd and 144Sm excited by the (p,t) reaction on radioactive targets
The (p,t) reaction has been used to study the closed-shell nuclei 146Gd and 144Sm, the former exhibiting some characteristics of a doubly closed shell. Exotic radioactive targets of 148Gd (t1/2 = 75 yr) and 146Sm (t1/2 = 7×10^7 yr) obtained from chemical and isotope separation of irradiated beam-stop material were employed. The ground-state mass excess of 146Gd was measured as being Δu = -76.083(15) MeV and the first excited state is confirmed as being a 3- state at 1.580-MeV excitation energy. Thirteen states were observed in 146Gd and 23 in 144Sm. The pairing-monopole and pairing-quadrupole states in both nuclei are observed for the first time. These levels are higher than systematics would predict, confirming a proton-subshell closure in 146Gd, and are split in 144Sm, indicating a strong interaction between nuclear modes
A radium assay technique using hydrous titanium oxide adsorbent for the Sudbury Neutrino Observatory
As photodisintegration of deuterons mimics the disintegration of deuterons by
neutrinos, the accurate measurement of the radioactivity from thorium and
uranium decay chains in the heavy water in the Sudbury Neutrino Observatory
(SNO) is essential for the determination of the total solar neutrino flux. A
radium assay technique of the required sensitivity is described that uses
hydrous titanium oxide adsorbent on a filtration membrane together with a
beta-alpha delayed coincidence counting system. For a 200 tonne assay the
detection limit for 232Th is a concentration of 3 x 10^(-16) g Th/g water and
for 238U of 3 x 10^(-16) g U/g water. Results of assays of both the heavy and
light water carried out during the first two years of data collection of SNO
are presented.Comment: 12 pages, 4 figure
The Sudbury Neutrino Observatory
The Sudbury Neutrino Observatory is a second generation water Cherenkov
detector designed to determine whether the currently observed solar neutrino
deficit is a result of neutrino oscillations. The detector is unique in its use
of D2O as a detection medium, permitting it to make a solar model-independent
test of the neutrino oscillation hypothesis by comparison of the charged- and
neutral-current interaction rates. In this paper the physical properties,
construction, and preliminary operation of the Sudbury Neutrino Observatory are
described. Data and predicted operating parameters are provided whenever
possible.Comment: 58 pages, 12 figures, submitted to Nucl. Inst. Meth. Uses elsart and
epsf style files. For additional information about SNO see
http://www.sno.phy.queensu.ca . This version has some new reference
Measurement of the νe and total 8B solar neutrino fluxes with the Sudbury Neutrino Observatory phase-III data set
This paper details the solar neutrino analysis of the 385.17-day phase-III data set acquired by the Sudbury Neutrino Observatory (SNO). An array of 3He proportional counters was installed in the heavy-water target to measure precisely the rate of neutrino-deuteron neutral-current interactions. This technique to determine the total active 8B solar neutrino flux was largely independent of the methods employed in previous phases. The total flux of active neutrinos was measured to be 5.54-0.31+0.33(stat.)-0.34+0.36(syst.)×106 cm-2 s-1, consistent with previous measurements and standard solar models. A global analysis of solar and reactor neutrino mixing parameters yielded the best-fit values of Δm2=7.59-0.21+0.19×10 -5eV2 and θ=34.4-1.2+1.3degrees
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CALCULATED FRACTIONAL INDEPENDENT YIELDS OP PRODUCTS FORMED IN THE SPONTANEOUS FISSION OF 252Cf
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INTERPRETATION OF MASS ASYMMETRY IN FISSION BASED ON DEFORMATION ENERGY SURFACES
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CALCULATED FRACTIONAL INDEPENDENT YIELDS OP PRODUCTS FORMED IN THE SPONTANEOUS FISSION OF 252Cf
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DETERMINATION OF CHARGE AND MASS DISTRIBUTION IN THE FISSION OF 25ecf
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