What causes secondary photons in He-3 detectors?

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SUMMARY

The discussion focuses on the generation of secondary photons in He-3 detectors, specifically addressing whether protons produced from the He(n,p)t reaction emit secondary X-ray photons as they decelerate in matter. It is established that the combined energy of the proton and triton is 764 keV, with 573 keV allocated to the proton. The secondary photons emitted are low in energy, while more energetic gamma-rays and X-rays can originate from interactions with the detector's metal wall or anode. The discussion emphasizes the importance of understanding the emission spectra of hydrogen and helium in this context.

PREREQUISITES
  • Understanding of He-3 neutron detectors and their operational principles.
  • Knowledge of the He(n,p)t reaction and its energy dynamics.
  • Familiarity with ionization energies of hydrogen and helium.
  • Basic concepts of gas-filled proportional counters and their sensitivity to X-rays and gamma-rays.
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  • Research the emission spectra of hydrogen and helium to understand photon generation.
  • Learn about the operational principles of gas-filled proportional counters.
  • Investigate the effects of neutron interactions with detector materials on photon emission.
  • Explore advanced topics in gamma-ray and X-ray detection technologies.
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Physicists, radiation detection engineers, and researchers in nuclear science focusing on neutron detection and photon emission phenomena.

Neutroniclad
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Does all the signals detected by He-3 detector caused by neutrons?
When the He(n,p)t reaction occurs, will proton cause any secondary x-ray photons since it de-accelerates in matter.
 
Neutroniclad said:
When the He(n,p)t reaction occurs, will proton cause any secondary x-ray photons since it de-accelerates in matter.
Think about the ionization energies of hydrogen (13.6 eV) and helium (1st 24.6 eV, 2nd 54.4 eV) so they will be UV or very soft X-rays, which would not ionize He atoms. Look at the emission or line spectra of H and He.

The combined energy of the p and t is the Q-value, 764 keV, with 573 keV to the proton and 191 keV to the triton). When they neutralize, the photons from them (t,p) are quite low in energy. More energetic gamma-rays and X-rays can originate in the metal wall or anode of the detector, if the t or p hit the anode or wall, and of course, they can originate from outside the detector.

Neutron detectors, including He-3: http://web.mit.edu/8.13/www/JLExperiments/38/tgm-neutron-detectors.pdf

Read up on gas-filled proportional counters and their sensitivity, or insensitivity, to X-rays and gamma-rays.

http://www.lanl.gov/orgs/n/n1/panda/00326408.pdf
http://large.stanford.edu/courses/2012/ph241/lam1/
https://www.gemeasurement.com/radia...etectors/helium-3-filled-proportional-counter
http://www.ncnr.nist.gov/staff/hammouda/distance_learning/chapter_13.pdf
http://www.whoi.edu/fileserver.do?id=166724&pt=2&p=155629

http://arxiv.org/pdf/1212.4724.pdf

Gamma-ray detectors - http://www.lanl.gov/orgs/n/n1/panda/00326398.pdf
http://www.canberra.com/literature/fundamental-principles/pdf/Gamma-Xray-Detection.pdf
 
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