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Program - Brookhaven National Laboratory

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differential yield data at requested energy and angular range, the MCNPX calculations need to be validated<br />

against the independent experiments. Recently, the dosimetry-foils method was successfully used to the<br />

validation of the MCNPX prediction of spectral flux characteristics for the p+D2O (thick) source. In the<br />

present work, this method was employed to determine the spectrum of the Be(p,xn) source reaction at<br />

the position of irradiated samples. The wide set of dosimetry foils (Al, Sc, Mn, Fe, Co, Ni, Ti, Y, In, Lu,<br />

Ta, Au, Nb, and Bi) was selected to cover the energy range under interest. In the experiment, the thick<br />

beryllium target was bombarded by the 35 MeV protons at beam current of 9 µA. Activated foils were<br />

investigated by the nuclear gamma-spectrometry technique (the HPGe detector). To unfold the neutron<br />

spectrum from resulting reaction rates, a modified version of the SAND-II code was used. Results and<br />

uncertainty of the validation are discussed in details.<br />

PR 33<br />

A CVD Diamond Detector for (n, α) Cross-section Measurements<br />

C. Weiss, E. Griesmayer,C. Guerrero, The n TOF collaboration, Vienna University of Technology,<br />

Vienna, Austria, CERN, Geneva, Switzerland, https://ntof-exp.web.cern.ch/ntof-exp/.<br />

In the last years, the experimental program at the n TOF facility at CERN has been extended to (n,<br />

cp) cross section measurements of astrophysical and medical interest. These measurements require using<br />

thin samples and often feature small cross sections, which results in small yields and thus call for a highresolution<br />

and low-background detector. In this context, we have developed a dedicated device, based on<br />

the chemical vapor deposition (CVD) diamond technology. The high performance of the detector, an array<br />

of 9 sCVD diamonds, tested in 2011 and used in 2012 for a 59 Ni(n, α) 56 Fe measurement, is presented here.<br />

CIVIDEC Instrumentation GmbH, Vienna, Austria, sponsored this work.<br />

PR 34<br />

Gas-filled Parallel-Plate Avalanche Counters for Fission Studies<br />

C.Y. Wu, A. Chyzh, E. Kwan, R.A. Henderson, J.M. Gostic, D. Carter, Lawrence Livermore <strong>National</strong><br />

<strong>Laboratory</strong>. T.A. Bredeweg, A. Couture, M. Devlin, R.C. Haight, M. Jandel, H.Y. Lee, B. A. Perdue, T.<br />

N. Taddeucci, J.L. Ullmann, Los Alamos <strong>National</strong> <strong>Laboratory</strong>.<br />

To study the prompt gamma and neutron emission in either spontaneous or neutron-induced fission using<br />

the DANCE [1] or Chi-Nu [2] arrays respectively requires a starter detector to identify uniquely the fission<br />

event by detecting the fission fragments. A gas-filled parallel-plate avalanche counter (PPAC) has many<br />

advantages for this application such as fast timing ( 1 ns), resistance to radiation damage, and tolerance of<br />

high counting rate. Therefore, a new generation of PPAC was developed at Lawrence Livermore <strong>National</strong><br />

<strong>Laboratory</strong> specifically for those arrays, located at Los Alamos Neutron Science Center (LANSCE), to<br />

make the needed measurements possible. For DANCE, a compact PPAC was fabricated with two anodes<br />

placed at 3 cm away on either side of the cathode [3]. The anodes are made of the 1.4 µm thick aluminized<br />

mylar. The cathode holds a 3 µm titanium foil with the electrodeposited target material that is sandwiched<br />

between two mylar foils of the same thickness. The target is double-sided using the electrodeposition cell<br />

described in Ref. [4]. For the Chi-Nu array, a low-mass multi-foil fission chamber was fabricated to<br />

accommodate 10 sets of PPAC [5]. Each one has the same geometrical arrangement of the anodes and<br />

cathode as the PPAC for DANCE. The targets were fabricated in a similar way except for the active areas:<br />

4 cm in diameter for Chi-Nu and 0.7 cm diameter for DANCE. The design details and performances of these<br />

PPACs will be presented. This work performed under the auspices of the U.S. Department of Energy by<br />

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