1 / 20

Fission cross section measurements with a coincidence method

Fission cross section measurements with a coincidence method. Measured isotopes : 233 U, 234 U, 232 Th, 237 Np, and 209 Bi, nat Pb References : 235 U and 238 U. Focus on isotopes with several targets : 234 U (2 targets), 232 Th (5 targets), 237 Np (4 targets). Detection layout.

Download Presentation

Fission cross section measurements with a coincidence method

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Fission cross section measurements with a coincidence method • Measured isotopes : 233U, 234U, 232Th, 237Np, and 209Bi, natPb • References : 235U and 238U • Focus on isotopes with several targets : 234U (2 targets), 232Th (5 targets), 237Np (4 targets)

  2. Detection layout

  3. Solid angle acceptance 237Np : 10 MeV < En < 15 MeV (2 targets) Target 1 Target 2

  4. f for 234U

  5. 238U/235U ratio

  6. f for 237Np

  7. Corrected counting rate of 237Np targets

  8. Raw counting rate of 237Np targets

  9. Raw counting rate of 232Th targets

  10. f for 237Np (raw)

  11. f for 232Th (raw)

  12. 238U/235U ratio (raw)

  13. Conclusion • The efficiency at 0° is lower than 1 when all localisation signals are • requested (unexpected) • The cross section based on anode signals is more reliable, and a • good reproducibility is obtained for different targets • Not protected against variations of angular distribution (between • 0.5 MeV and 50 MeV), and need of a normalisation factor. • A cross section accuracy better than 10% can probably be achieved

  14. Selection of fission Singles Coincidence

  15. Use of FADCs : pile up resolution 50 channels 500Ms/s Original signals - anode (black) - cathode right (red) - cathode left (green) Signals after filtered derivative (convolution)

  16. Use of FADCs : noise reduction Original signals Signals after filtered derivative (convolution)

  17. Energy resolution 235U around 10eV ( scaled and compared to ENDF) 234U around 570eV

  18. Targets • Thin layer (0.3mg/cm2) of 8cm in diameter • Electrodeposition on Al backing (2m thick) 234U Measured isotopes 237Np, 233U, 234U, 232Th, 209Bi, natPb Reference isotopes : 235U, 238U

  19. Emitting point distribution on the target 234U fission α activity Targets with Ø=8cm 209Bi natPb Extended targets

  20. Flux from 235U and 238U (JENDL above 20 MeV)

More Related