Title: www.kayzero.com
1NAA using Kayzerofrom peak areas to element
concentration
- R. van Sluijs, k0-ware, Heerlen, the Netherlands
- D. Bossus, DSM Geleen, the Netherlands
- F. De Corte, RUG, Ghent, Belgium
2Problem? No problem!?
Simple? Perhaps not, but very well
documented! nowadays there
are many programs to help!
3No problem,but ..... (1)
- How to get the correct peak area?
- Use a perfect gamma spectrometry system and keep
it in the best possible condition! - Use the perfect gamma spectrum deconvolution
program! - However who has this perfect set-up?
4No problem, but......... (2)
- How to select the analytical line
- K0-library has data for 68 elements, 144 nuclides
and more than 700 gamma-lines - For a panoramic analysis you use preferably 2
irradiations (short and long) each followed by
2-3 measurements - A single element will give data for several
nuclides and probably tens of gamma lines. - All we want one single list
- Containing the all elements with their
concentrations and/or limits of detection.
5DSMs/Kayzeros method
User Input
Automatic
- Optimise the peak table!
- Peak Table Areas and Energies from gamma
spectrum deconvolution program - Calculation
- Concentrations for all lines in the k0- library
- Evaluation
- Identify the nuclides in the sample
- Correct for gamma interferences
- Calculate averages per nuclide and per element
- Average over all measurements
- Refine the results
6 Optimise the peak table!
- Peak Areas
- Broadened peaks (due to count rate effects, bad
pile-up correction, etc..) can be split by the
gammaspectrum deconvolution program into two
separate peaks. - Sum the false/artificial peaks for a correct
result - Peak locations
- Linear energy calibration, non-linear is often
better - Re-do the energy calibration
- Hypermet shifts data 1 channel to the left
- Shift back
7Measurement Input screen
8Peak summation screen
9Re-do energy calibration
10k0-calculations
- Calculate concentrations for all library lines
- Including Corrections for
- background,
- dead-time,
- gamma-absorption,
- burn-up,
- neutron self absorption,
- True-coincidence correction
- No matching peak the LD concentration is
calculated using the spectrum base line. - No result if calculated concentration gt100
11Evaluation of the results Check the presence of
a nuclide
12Evaluation of the resultsCheck the presence of
an element
13Evaluation of the resultsCorrect for gamma
interferences
- Nnumber of interfering
- nuclides on line E
14Evaluation of all results Calculate averages and
standard deviations
- over the lines of a nuclide
- weighing factor wi 1/s2i
- sobserved should be approx. equal to sexpected
15Refine the resultsselect the analytical lines
- Select by hand
- gammas to be used
- correct for threshold, fission, second-order
reaction interferences, - blank correction,
- Alarm for high epi-thermal self shielding
16Ba-131 large observed SD
17Deselect Ba-131 line
18Fission Correction for La-140
19Fission Correction
20Blank subtraction
21The goal of all our worka (digital) list of
concentrations
51 elements reported 30 with concentration, 21
only detection limit
Final result
51 elements reported - 30 concentrations - 21
only detection limit
22Conclusion
- k0-method (DeCorte/Simonits) is a very complete
method, all aspects of INAA are taken into
account, elaborate calculations are needed but
this is no problem nowadays - The method presented to handle k0-data is based
on almost 20 years of experience, analysing all
kinds of samples - Evaluation of the data of a panoramic elemental
analysis of an unknown sample takes less than
half an hour - Although very much automated the analyst is in
control - The competition in our lab is though, NAA is the
most expensive technique so quality and
reliability is a prerequisite