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Radioactivity is a spontaneous disintegration of an unstable nuclide and is a random process, as all the nuclei in the sample do not decay simultaneously. The number of disintegrations per unit time is called the activity (A), which is directly proportional to the number of nuclei in the sample. The decay constant (λ) is an average probability of decay per nucleus in unit time.
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The 40Ar(d,p)41Ar cross section between 3-7 MeV.

D L Bleuel1, S G Anderson1, L A Bernstein2

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|October 28, 2022
PubMed
Summary
This summary is machine-generated.

This study measured the argon-40 (d,p) argon-41 cross section to assess argon as a deuteron beam stopping material. Results indicate a higher cross section than previously reported, impacting safety assessments.

Keywords:
Argon cross section γray activation

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Area of Science:

  • Nuclear physics
  • Materials science

Background:

  • Argon is a potential material for stopping deuteron beams in accelerators.
  • Accurate cross-section data is crucial for safety evaluations and beam control.

Purpose of the Study:

  • To measure the 40Ar(d,p)41Ar cross section at specific deuteron energies.
  • To evaluate the safety and feasibility of using argon as a deuteron beam stopping material.

Main Methods:

  • Activation method using a 16-MeV deuteron beam from a cyclotron.
  • Deuteron energy degradation using nickel foils and an aluminum gas chamber.
  • Measurement of 41Ar activation using a high-purity germanium detector.

Main Results:

  • Cross sections for the 40Ar(d,p)41Ar reaction were determined at 3.6, 5.5, and 7.0 MeV.
  • Measured cross sections were approximately 40% larger than a prior experimental value.

Conclusions:

  • The measured cross-section data provides critical information for the safe use of argon.
  • Higher cross-section values necessitate a re-evaluation of argon's suitability as a beam stopping material.