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Program - Brookhaven National Laboratory

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J. P. Lestone, E. F. Shores<br />

Los Alamos <strong>National</strong> <strong>Laboratory</strong><br />

The neutron experiment (NUEX) was a common diagnostic on nuclear device tests conducted at the<br />

Nevada Test Site (NTS). In these experiments neutrons from a device pass up a collimated line of site,<br />

and in the case of a Faraday cup (FC) NUEX, the neutrons pass through a thin CH2 foil. Some of these<br />

neutrons interact with the nuclei in the foil, generating light charged particles (predominantly protons)<br />

which are collected in a Faraday cup. The time dependence of the Faraday cup current is a measure of the<br />

energy spectrum of the neutrons that leak from the device. With good device models and accurate neutrontransport<br />

codes, the leakage spectrum can be converted into a prompt fast-neutron-induced fission-neutron<br />

energy spectrum (PFNS) from ∼1 to 11 MeV. This has been done for one of our last events containing<br />

a plutonium primary, where the NUEX data were of a particularly high quality, and for an earlier event<br />

containing a uranium primary. The fission-neutrons in these devices were produced by fission events<br />

induced by neutrons over a broad range of energies. We have inferred 2 MeV n + 239Pu and n + 235U<br />

fission-neutron spectra for outgoing neutron energies from 1.5 to 10.5 MeV, in 1-MeV steps. These spectra<br />

are in good agreement with the Los Alamos fission model [1].<br />

[1] D. G. Madland and J. R. Nix, Nucl. Sci. and Eng. 81, 213 (1982), and http://t2.lanl.gov/data/fspect.<br />

LA 2 4:00 PM<br />

A New Measurement of the Neutron Capture Cross Section of 235 U Below 5 keV<br />

David Williams, Yaron Danon, Rian Bahran<br />

Gaerttner LINAC Center, Rensselaer Polytechnic Institute, Department of Mechanical, Aerospace and<br />

Nuclear Engineering, 110 8th St, Troy, NY 12180<br />

Devin Barry, Greg Leinweber, Robert Block, Michael Rapp<br />

Bechtel Marine Propulsion Corporation, Knolls Atomic Power, <strong>Laboratory</strong>, P.O. Box 1072, Schenectady,<br />

New York 12301-1072<br />

The neutron microscopic capture cross section for 235 U is a critical parameter for the design and operation<br />

of nuclear reactors. The evaluated nuclear data libraries of ENDF/B-VII.1 and JENDL-4.0 have nearly<br />

identical values for the neutron capture cross section for neutron energies below 0.5 keV. In the most recent<br />

release of the JENDL library the onset of the unresolved resonance region (URR) was changed from 2.25 keV<br />

to 0.5 keV, and in this region the average neutron capture cross section from ENDF/B-VII.1 is about 10%<br />

higher than that from JENDL-4.0. In an attempt to address the discrepancies between the libraries, a<br />

new measurement of the neutron capture cross section of 235 U was conducted at the Gaerttner LINAC<br />

Center located at Rensselaer Polytechnic Institute. This measurement used a 16 segment γ-multiplicity<br />

NaI(Tl) detector to detect the prompt gammas emitted from neutron interactions with a highly enriched<br />

235 U sample. Using the time-of-flight method, detected events were recorded and grouped based on the<br />

total gamma energy per interaction and observed multiplicity. A method was developed to separate fission<br />

from capture based on total energy deposition and gamma multiplicity. Application of this method in<br />

the thermal and resonance region below 0.5 keV for both the fission and capture cross section produced<br />

cross sections in excellent agreement with both the ENDF/B-VII.1 and JENDL-4.0 evaluations. The<br />

measurements support the conclusion to lower the 235 U neutron capture cross section below the ENDF<br />

values in the energy range 0.5-2.25 keV.<br />

LA 3 4:20 PM<br />

164

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