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Program - Brookhaven National Laboratory

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DB 5 5:00 PM<br />

Thermal Neutron Capture Cross-Section Measurements of 50 Ti, 51 V and 98 Mo<br />

V. H. Tan<br />

Vietnam Agency for Radiation and Nuclear Safety (VARANS), 70-Tran Hung Dao, Ha Noi, Vietnam<br />

P. N. Son<br />

Nuclear Research Institute, 01-Nguyen Tu Luc, Dalat, Vietnam<br />

Thermal neutron capture cross sections for 50 Ti, 51 V and 98 Mo were measured by the activation method<br />

using the filtered thermal neutron beam at the Channel No.2 of Dalat research reactor. An optimal<br />

composition of Si and Bi single crystals has been used as neutron filters to create the high purity filtered<br />

thermal neutron beam with Cadmium ratio up to 700. The cyclic activation mode was applied for the cases<br />

of 50 Ti and 51 V because of short half lives of their neutron capture products. The induced activities in the<br />

irradiated samples were measured by a high resolution HPGe digital gamma-ray spectrometer. The present<br />

results of thermal neutron capture cross sections for 50 Ti, 51 V and 98 Mo have been obtained relative to<br />

the reference values of 197 Au standard, with σ0 = 98.65 ± 0.09 barn. The necessary correction factors for<br />

gamma-ray true coincidence summing, and thermal neutron self-shielding effects were taken into account<br />

in the determinations. The present results are discussed and compared with previous measurements.<br />

Corresponding author: P. N. Son<br />

DB 6 5:15 PM<br />

Measuring Light-Ion Production and Fission Cross Sections Versus Elastic np-Scattering at<br />

the Upcoming NFS Facility<br />

Kaj Jansson, Cecilia Gustavsson, Anders Hjalmarsson, Stephan Pomp, Giovanni Scian, Diego Tarrio<br />

Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden<br />

Alexander Prokofiev<br />

The Svedberg <strong>Laboratory</strong>, Uppsala University, Uppsala, Sweden<br />

The Medley setup has been used in many measurements at the Svedberg <strong>Laboratory</strong> (TSL) in Uppsala<br />

mainly with a quasi-mono-energetic neutron beam at 96 and 175 MeV [1,2]. Medley has eight detector<br />

telescopes each consisting of two silicon detectors and a CsI(Tl) detector at the back providing ∆E-∆E-E<br />

data. The whole telescope setup is rotatable and can be made to cover any angle. Medley is now planned<br />

to be moved to and used at the new, currently under construction, neutron facility NFS [3] in Ganil<br />

where measurements of light-ion production as well as fission cross-sections are planned at 1-40 MeV. The<br />

light-ion production plays an important role in e.g. single-events effects in electronics. The 238 U fission is<br />

particularly important as a standard for high-energy neutron monitoring but also in nuclear power related<br />

areas and to understand the fission phenomena itself. At low and high neutron energies these cross-sections<br />

are fairly well known but at intermediate energies, especially above 20 MeV, there are large discrepancies<br />

among reported cross-sections. Our measurements will thus provide data in a much needed energy region.<br />

Our main goal is measuring U-238 and Th-232. However, we plan to extend the measurements also to<br />

other actinides. The fission cross-section is planned to be measured relative the standard np-cross-section<br />

by simultaneously measure protons in the forward angles and fission fragments in the backwards angles.<br />

The energy dependent anisotropy factor can also be measured. To be able to do these new measurements<br />

at NFS, which will have a high intensity white neutron beam coming from a full stop Be-target, Medley<br />

needs to detect the reaction products with a high temporal resolution providing the ToF of the primary<br />

neutron. In this paper we discuss the design of the Medley upgrade and experiments along with simulations<br />

59

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