Posts Tagged ‘neutron’

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HPGe Detector, Part II: Neutron Activation with a Weak AmBe Source

September 21, 2011

Activation of antimony, indium, and aluminum is possible using a homemade neutron source containing ~5.6 millicuries of Am-241 in sealed smoke detector sources pressed against beryllium.  Although the source is weak (at best about 2000 n/s) and the activities induced by it even weaker, an HPGe detector can convincingly sniff out the telltale signs of neutron exposure in certain materials that have been nearby.  (Read Part I in this series for details about the HPGe detector.  Successful detection hinges on the high resolution of the HPGe in these three cases, but see my video here for an example of activation detected by a NaI:Tl scintillator.) 

Below are the three test specimens: 200-mesh antimony powder, an old piece of 0.01″ indium foil, and some little scrap pieces of 6061 aluminum:

When manufacturing artificial radioactivity by neutron capture, it’s important to optimize both the irradiation conditions and the detection conditions according to the physics of the experiment—tailoring the neutron energy spectrum to the reaction cross-section with moderators, choosing irradiation and counting durations according to product lifetime, and using an appropriate detector for the expected activities (in these cases, all expected products are strong gamma emitters).  My goal with the antimony is to detect Sb-122 from radiative capture of low-energy neutrons on the natural isotope Sb-121, i.e. Sb-121(n,g)Sb-122.  With indium, I’m seeking the In-115(n,g)In-116m1/In-116m2 reactions, also favored by low-energy neutrons.  The aluminum presents an opportunity to perform a fast neutron reaction, Al-27(n,p)Mg-27.  I will discuss the challenges particular to this reaction in more detail later.

I elected to use polyethylene as a moderator and reflector for all three irradiations.  The AmBe source emits a broad spectrum of fast neutrons with a mean energy near 5 MeV, so the indium and antimony activations benefit from having those neutrons slowed down.  The Al(n,p) reaction does not benefit from slow neutrons; however, the mean free path of fast neutrons in Al metal exceeds the thickness of my pieces, and the plastic will serve to reflect many neutrons back into the sample that would otherwise be wasted.  Below are a couple ad-hoc contraptions to surround samples with plastic.  At left is my black HDPE “neutron oven,” originally part of a “Snoopy” neutron detector.  At right is a more versatile concept—HDPE bricks.  For no particular reason the antimony and aluminum went in the “neutron oven” and the indium was cooked inside the stack of bricks.

The half life of Sb-122 is 2.72 days, so ideally the antimony would cook next to the neutron source for more than a week to bring it up toward saturation activity.  I’m not that patient, so it cooked for only two days.  In-116m1 (half-life 54m) saturates in a few hours, so I cooked the indium in contact with the neutron source for two hours.  Mg-27 from the Al(n,p) reaction (half-life 9.5m) is expected at exceedingly low activity and a special technique of repetitive irradiating and counting was adopted: irradiate (1800 s), count (700 s), wait (700 s), count background (700 s), and repeat this sequence two more times.

After irradiation, I counted the samples with the HPGe detector (left, its electronics at right).  My approach is generally to count for at least one half-life if practical, but no longer than two.  The count times (detector “live times”) are noted in each collected spectrum in the gallery below.  Background spectra for subtraction are best obtained by allowing the sample to remain in position near the detector for several half-lives to decay, then counting again for as long as possible.  I used this general approach with indium and aluminum, but with the 2.7-day antimony, it would have been somewhat impractical.  An alternative is to simply remove the sample entirely and count as I ended up doing; a better alternative would have been to count the background before irradiation.

Each experiment resulted in radioactivity of the type expected.  Or did it?  Check out the results (click any image for full size):

The radiation from antimony has a simple spectrum that matches expectations of a 564.2-keV gamma ray accompanying 71% of decays.

The indium spectrum offers a robust and distinct fingerprint of multiple gamma energies that are a textbook match to the expected values from In-116m1; other possible radiations from other isomers of In-116  or In-114 are not in evidence.

And then we come to a genuine interpretive challenge with the aluminum.  I expect a major peak at 843.8 keV (72%) and a minor peak at 1014.4 keV (28%) from Mg-27.  Obviously there’s a peak in the immediate vicinity of the former value—its centroid is calculated to be 841.9 keV based on calibration of the energy scale with Cs-137 and Co-60.  Close enough to be conclusive?  Well, there’s a hitch.  Manganese is an important contaminant in 6061 alloy.  Its (n,g) reaction has a high cross section and results in 2.6-hour Mn-56, which emits an 846.8-keV gamma ray.  There are just two channels of separation between 846.8 keV and 843.8 keV in my pulse height spectrum.  Further infusing doubt into the Mg-27 hypothesis is the absence of a significant peak at 1014.4 keV, although only 12±4 counts are expected there—well into the noise.  But if, on the other hand, Mn-56 is responsible for this peak, we can look to additional evidence to corroborate that hypothesis.  First, Mn-56 emits an 1811-keV gamma ray (27%) in addition to the 846.8-keV gamma ray (99%).  There is the noisy suggestion of a peak at 1764 keV that could be Mn-56’s 1811-keV radiation if the detector’s energy calibration is poor, but this could also plausibly be Al-28 (1779 keV), or radon daughter Bi-214 (1764 keV).  Second, Mn-56’s half life is much longer than Mg-27’s and longer than the duration of the experimental sequence, so the “background” spectra for this experiment should show  many counts at this energy if Mn-56 is the culprit.   In fact, the background has just 8 counts in this channel.  In conclusion: I’m willing to put faith in my three-point linear energy calibration and attribute the 1764-keV peak to ambient Bi-214, and from examination of the background spectrum in this experiment, attribute the 841.9-keV peak to Mg-27.  Sometimes these analyses aren’t straightforward!

Reference information from the National Nuclear Data Center:

  • Energy-dependent cross-section for the (n,g) reaction in Sb-121; decay radiation from Sb-122
  • Energy-dependent cross-section for the (n,g) reaction in In-115; decay radiation from In-116
  • Energy-dependent cross-sections for the (n,g) and (n,p) reactions in Al-27; decay radiation from Mg-27, Al-28, Mn-56, Bi-214
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Farnsworth Fusor (“Carl’s Jr.”)

February 17, 2008

This post will serve as a documentation hub for my Farnsworth fusor hobby projects. I have used these devices as neutron generators for doing activation experiments at home and at college. The fusor is a simple spherical ion source / accelerator / collider that can be built on a shoestring budget with a minimum of technical background, enabling hobbyists to access some nuclear fusion reactions. This blog post isn’t intended to provide an adequate overview of the fusor’s physics or serve as a base for technical discussion–there are already some good websites out there with those purposes. Readers with questions or interest in this technology are encouraged to engage in the discussions on the Fusor Forum.

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“Carl’s Jr.” is my current fusor project, first operated in 2006.

Star dischargeCarl’s JrCathodeFusor systemModeratorCockroft-Walton

Specifications of “Carl’s Jr.” are provided below, with links to more detail and commercial suppliers for some components.

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While a student at Guilford College, I built the predecessor to Carl’s Jr., a larger but less innovative fusor with which I did some novel neutron activation experiments.

OldFusorPoissor OldFusorTopViewxray machine sparking

Specifications of my Guilford fusor are provided below.

  • Typical operating conditions: 67 kVp, 15 mA, 10 mtorr, ~3E+06 neutrons / sec.
  • Vacuum chamber: 2 x 8″ 304SS hemispheres, 10″ equatorial CF flanges
  • Chamber ports: 2 x QF25, 1 x 2.75″ CF, 1 x special feedthrough solder lip
  • Cathode: 6 x 2.5″ loops of 0.025″ dia. 316SS wire, construction by spot welding
  • Ion source: none
  • HV feedthrough: surplus 100 kV vacuum-rated feedthrough, air-insulated
  • Gas system: 5o-liter LB cylinder of deuterium, 2 series needle valves
  • High voltage system: 135 kVp x-ray supply, controlled by Variac and magnetic amplifier
  • Vacuum system: Varian 50 LPS baby turbopump system
  • Cooling system: forced-convection air cooling (ShopVac)
  • Neutron irradiator: Water in VHS cases; paraffin canning wax

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Fusor Experiments

Documents

  • My undergraduate thesis for the physics department of Guilford College, entitled “Neutron Activation Using a Farnsworth Fusor” (2003) can be downloaded here. An accompanying PowerPoint presentation can be downloaded here.

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