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Title: A time projection chamber for high accuracy and precision fission cross-section measurements

Journal Article · · Nuclear Instruments and Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment
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  1. Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)
  2. Pacific Northwest National Lab. (PNNL), Richland, WA (United States)
  3. California Polytechnic State Univ. (CalPoly), San Luis Obispo, CA (United States)
  4. Idaho National Lab. (INL), Idaho Falls, ID (United States)
  5. Oregon State Univ., Corvallis, OR (United States)
  6. Ohio Univ., Athens, OH (United States)
  7. Colorado School of Mines, Golden, CO (United States)
  8. Idaho State Univ., Pocatello, ID (United States); Georgia Inst. of Technology, Atlanta, GA (United States)
  9. Idaho State Univ., Pocatello, ID (United States)
  10. Colorado School of Mines, Golden, CO (United States); Los Alamos National Lab. (LANL), Los Alamos, NM (United States); California Polytechnic State Univ. (CalPoly), San Luis Obispo, CA (United States)
  11. Georgia Inst. of Technology, Atlanta, GA (United States)
  12. Idaho National Lab. (INL), Idaho Falls, ID (United States); Los Alamos National Lab. (LANL), Los Alamos, NM (United States)
  13. Abilene Christian Univ., Abilene, TX (United States)
  14. Los Alamos National Lab. (LANL), Los Alamos, NM (United States)
  15. Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States); Colorado School of Mines, Golden, CO (United States)

The fission Time Projection Chamber (fissionTPC) is a compact (15 cm diameter) two-chamber MICROMEGAS TPC designed to make precision cross-section measurements of neutron-induced fission. The actinide targets are placed on the central cathode and irradiated with a neutron beam that passes axially through the TPC inducing fission in the target. The 4π acceptance for fission fragments and complete charged particle track reconstruction are powerful features of the fissionTPC which will be used to measure fission cross-sections and examine the associated systematic errors. This study provides a detailed description of the design requirements, the design solutions, and the initial performance of the fissionTPC.

Research Organization:
Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)
Sponsoring Organization:
USDOE
Grant/Contract Number:
AC52-07NA27344
OSTI ID:
1343003
Report Number(s):
LLNL-JRNL-651187
Journal Information:
Nuclear Instruments and Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment, Vol. 759, Issue C; ISSN 0168-9002
Publisher:
ElsevierCopyright Statement
Country of Publication:
United States
Language:
English
Citation Metrics:
Cited by: 32 works
Citation information provided by
Web of Science

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Cited By (7)

High quality actinide targets journal July 2015
Fission fragment yields and total kinetic energy release in neutron-induced fission of 235,238 U,and 239 Pu journal January 2018
Nuclear fission: a review of experimental advances and phenomenology journal November 2017
Prompt neutron multiplicity distributions inferred from γ -ray and fission fragment energy measurements journal November 2019
Fission fragment angular anisotropy in neutron-induced fission of U 235 measured with a time projection chamber journal June 2019
High Quality Actinide Targets text January 2017
1H(n,el) as a Cross Section Reference in a White Source Neutron Beam With the fissionTPC preprint January 2019

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