A review of nuclear data for the k₀-based neutron activation analysis
Nuclear Science and Technology, Vol.9, No. 1 (2019), pp. 28-33
A review of nuclear data
for the k0-based neutron activation analysis
Ho Manh Dung1*, Phonesavanh Lathdavong2
1Center for Nuclear Techniques, 217 Nguyen Trai Street, District 1, Ho Chi Minh City, Vietnam
2Department of Science, Ministry of Science and Technology, Vientiane, Laos P.D.R.
(Received 28 June 2019, accepted 07 September 2019)
Abstract: Nuclear data for the k0-based neutron activation analysis (k0-NAA) including: k0-factors –
combination of nuclear constants (atomic mass, isotopic abundance, gamma-ray yield and thermal
neutron capture cross section); Q0 – the ratio of the resonance integral to thermal neutron capture cross
section; and
E
– effective resonance energy, along with the related nuclear data are presented and
r
evaluated in the presentation. Accuracy and capability of k0-NAA depends considerably on the
reliability of the above mentioned nuclear data. In general, the evaluation of nuclear data is essential
and necessary in the field of nuclear science and technology, and this work is conducted by the
nuclear data centers on the world as well as the research institutions where the nuclear data are used
for R&D. Therefore, the evaluation of the nuclear data used in k0-NAA should also be performed so
that some of data may no longer be appropriate should be redetermined. The evaluation of nuclear
data in k0-NAA would contribute to the improvement of accuracy and reliability of the method,
moreover, it would also contribute to the establishment a nuclear database in Vietnam in the future.
Keywords: Nuclear data, neutron activation analysis, k0-standardized method.
reviewed the nuclear data of interest, but their
findings have not been included in the library
of new database, and so on. Therefore, this
presentation reviews all of the nuclear data (k0,
I. INTRODUCTION
The k0-based neutron activation analysis
(k0-NAA) is based on the k0 factors – the
combined constant of nuclear data, determined
by experiment. Therefore, the accuracy of the
method depends on reliability of the k0 factors.
In addition, there are other related nuclear data
such as thermal neutron capture cross section
(0), integral resonance (I0) (or Q0= I0/0) and
Q0 and
E
) for the elements of interest in k -
r
0
NAA. After reviewing, some data will be
chosen for re-determining and then the
experimental determination of selected data
should be carried out.
The nuclear data (k0, Q0 and
E
) has
r
the effective resonance energy
( ).
E
r
been determined by experiment mainly in the
laboratories of Europe: Belgium, Hungary and
the Netherlands. Then, some other laboratories
in the US, Canada and Japan have been
involved in the implementation.
Currently, the first version of database and the
updated version [1,2] has widely used.
However, recent references show that some
data have only been determined just once 30
years ago but they have never been verified or
updated. Some k0 factors are considered as “not
yet approved”. Moreover, some of data of first
version have not yet been verified [3,4]. A
number of laboratories around the world have
Recently, the international scientific
committee of k0-NAA has recommended for
re-determining of a number of k0 factors and
related nuclear data. It should be
©2019 Vietnam Atomic Energy Society and Vietnam Atomic Energy Institute
HO MANH DUNG, PHONESAVANH LATHDAVONG
immplemented a review the k0 factors and
then use the HPGe detector based-spectrometer
to measure the gamma-ray spectrum. Finally,
using computer software to process the data
and calculate the results.
related nuclear data in k0-NAA, aiming to
evaluate and re-determine some nuclear data of
interest. Nuclear data including 300 gamma
energy levels, 55 radionuclides, with 17 types
of reactions and decays of nuclear states in k0-
NAA should be reviewed. Choose the
necessary data to re-determine by experiment
based on the updated criteria. The
establishment of the nuclear database includes,
Isotopes under investigation and
chosen convention
For all the determinations use was made
of the standards to which these materials,
mostly foils and wires, are especially suited
because of the minimum preparation required,
i.e. k0, Q0 and
E
for the elements with
r
negligible
chances
of
mass
losses,
relevance radionuclides of interest in k0-NAA,
homogeneity, stability and low uncertainty in
the certified content. Furthermore, several of
the diluted Al alloys or spiked paper filters can
be regarded as free from strong neutron self-
shielding effects during irradiations. The use of
the much simpler Høgdahl convention [5] over
the Westcott formalism [6] was chosen since
from Holden [7] it can be seen that only the
rhenium isotopes deviate slightly from the
1/v expected behavior. Their deviations are
so is essential and necessary.
The re-determination some of nuclear
data in k0-NAA will contribute to the world‟s
nuclear database. Experimental methods used
in the nuclear research reactor are
characterized such as neutron flux, energy
spectrum deviation, coefficient of cadmium,
and so on measured by the spectrometers based
on HPGe detectors and the data processing by
specialized software. To evaluate the new
nuclear data and apply to real samples using k0-
NAA. Compare the results using the new data
and the old data to prove the improvement of
the new data.
0
0.8 % at 60 C, while the temperature of our
0
channels is estimated to be 30 C. Table 1
displays the k0,Au factors and related nuclear
data for use in k0-NAA.
Experimentally measured k0,Au factors
and related nuclear data for use in k0-
standardized neutron activation analysis (k0-
NAA) are given. Data for which the percent
uncertainty (relative standard error, s, in %) is
denoted as (–) bear an uncertainty estimated to
be about 5% (for k0) or about 10% (for Q0).
The symbols in Table 1 are explained as
followings:
II. METHODOLOGY
Review of reference documents related
to nuclear data in k0-NAA problem, from
which the nuclear data are summarized for
reviewing and choosing the appropriate cases
to re-determine by experiment in consideration
of ability of the laboratories the nuclear
research reactor as a neutron source causing
nuclear
reactions
for
research
and
El - Chemical symbol of the element;
Target isotope - Isotope of the target element;
Q0=I0/0 - resonance integral to 2200-m/s
cross-section ratio; The relative standard error,
measurement systems as well as computer
software for data processing.
Experimental nuclear physics methods
used by bombarding the targets using pure
standards of the elements of interest in the
neutron field of the nuclear research reactor,
S, in %;
E
- Effective resonance energy, in
r
keV; Formed isotope Isotope formed in the
reaction, together with the activation/decay
29
A REVIEW OF NUCLEAR DATA FOR THE K0-BASED NEUTRON ACTIVATION ANALYSIS
further columns it is also indicated if the value
is affected by true coincidence summing or is
derived from summing a multiplet. The
revision dates and the relevant references are
also shown (see Table I). Neutron capture
cross-sections, resonance integrals and the
ratios of the two (Q0), as well as the effective
code; T1=2 - Half-life; E- Gamma-ray energy,
in keV, adopted from Isotope Explorer (1999);
k0,Au
- Measured k0,Au ratio, with the relative
standard error, S, in %; In our notation, 9.98E-
4 = 9.98 10-4 , etc.
III. RESULTS AND DISCUSSION
resonance energies (
E
) for the nuclides
r
The recommended nuclear data are
based on the data published in Refs. [8–10].
The values, references and comments have
been verified carefully and corrected where
typographical errors, data-handling (e.g.
rounding) errors, inconsistencies, or other
mistakes were found. All questionable data
were discussed one by one, and were modified
after a common agreement. All modifications
to the data and the rationale behind the
modification are traceable in the tables.
appearing in the table (see Table II).
Decay modes of the radioactive nuclides
formed during the activation can be found:
either decays or isomeric transitions. The
branching ratios between decays and
isomeric transitions also appear in the table.
Nuclides, the properties of the target and
product nuclides can be seen in the table. The
target nuclides are stable and their isotopic
abundances are given, while the products are
radioactive and their half-lives are shown in
the traditional units (see Table III).
In this work, the access version of the
IUPAC database [9] has been used in a table.
The obvious rounding errors (smaller than 0.1
%) were corrected and the all k0 factors are
written in the scientific format. Thus the values
listed in the tables contain the proper number
of significant digits. The present data contains
the followings:
Decay codes, most decays are type I,
where the radioactive state decays directly to
the very-short-lived gamma-emitting state.
Decays through several steps have the codes
from II to VII, which can be seen as “decay
code (n, )” and “decay code (n, f)” in Ref
[10]. There are data, which contain the most
important k0 and decay code for nuclides
produced by the neutron-induced fission of
uranium (see Table IV).
k0 – values, it lists the elements, their
isotopes and the gamma-ray energies together
with the k0 values and their uncertainties. In
Table I. Changes in the “k0” values of the recommended data.
dk
(%)
E
(keV)
0
k
0
El
A
S
Revised
Revision information
F
20
1
1
1
1,633.6 9.98E 04
1,345.8 4.98E 04
2,507.9 7.29E 03
1.2 2002-08-28
0.9 2002-08-28
Old revision on 2001-06-14. Published [7]
Removed Ref. [3], old k0 = 4.91E 4. Published [7]
Cu 64
Ga 72
1.3 2021-08-28* Published in Ref. [7]
*Type error, should be 2002-08-28.
Se
Se
Se
Zr
75
75
75
95
1
1
1
1
1
264.7 7.11E 03
279.5 3.00E 03
400.7 1.43E 03
756.7 1.10E 04
555.8 6.92E 02
0.7 2002-08-28
1.2 2002-08-28
0.8 2002-08-28
1.3 2011-12-07
Removed Ref. [3], old k0
Removed Ref. [3], old k0
Removed Ref. [3], old k0
=
=
=
7.25E 3. Published [7]
3.06E 3. Published [7]
1.45E 3. Published [7]
Eror in Ref. [7] for k0, E-5 instead of E-4. Published [8].
Rh 104
1.5 2011-12-07* Type error in Ref. [7] for c555.8(m/F2g), 0.0691 instead of
*The last publication Ref. [10] is also incorrect, with type error 0.651 instead of 0.0651. The correct value of
0.0651
30
HO MANH DUNG, PHONESAVANH LATHDAVONG
Pd 111
Sn 117
Tm 170
Ta 182
2
2
1
1
172.2 1.07E 05 1.4 2002-08-28
158.6 1.33E 05 2002-08-28
Removed Ref. [3], old k0
Removed Ref. [3], old k0
Removed Ref. [3], old k0
Removed Ref. [3], old k0
=
=
=
=
9.04E 6. Published in Ref. [7]
1.35E 5. Published in Ref. [7]
4.30E 2. Published in Ref. [7]
1.61E 2. Published in Ref. [7]
1
84.3 3.26E 02 1.7 2000-12-31
152.4 1.62E 02 0.7 2011-12-07
Table I I . Changes in the “Capture‟‟ data of the recommended k0 database.
dQ
dE
r
(%)
El
1
0
Q
E , eV
r
A
1
S
El
A
S
Revised
1
Comments to revision
0
(%)
Na 23 10 0.59
Cl 37 10 0.69
3,380 11 Na 24
13,700 14 Cl 38
1
1
1
2011-12-14 dQ
2011-12-14 dQ
=
=
4.7 is removed
4.1 is removed
0
0
K
41 10 0.87
3.0 2,960 7.1
K
42
2011-12-14 New Q and dQ from Ref. [7]. Removed Ref.
0
0
[3], old. Q
=
0.97 and no data for dQ
0
0
Sc 45 10 0.43
Cr 50 10 0.53
5,130 17 Sc 46
7,530 11 Cr 51
1
1
1
2011-12-14 Add dE from Ref. [2]
r
2011-12-14 dQ
=
2.4 is removed
0
Mn 55 10 1.053 3.0 468
11 Mn 56
2011-12-14 New dQ from Ref. [7]. Removed Ref. [3], old
0
dQ
=
2.6
0
Co 59 10
2
136
766
5.1 Co 60
17 Cu 66
2
1
1
2011-12-14 Add dE from Ref. [2]
r
Cu 65 10 1.06
2011-12-14 dQ
=
4.9 is removed
0
Zn 64 10 1.908 5.0 2,560 10 Zn 65
2011-12-14 New dQ from Ref. [7]. Removed Ref. [3], old
0
dQ
=
4.9
0
Sb 123 10 19.9
Au 197 10 15.7
28.2
1.8 5.65 7.1 Au 198 1 2011-12-14 Kept dQ from Ref. [3]
6.4 Sb 124 2 2011-12-14 Add dE from Ref. [2]
r
0
Table I I I . Changes in the “Nuclides” data of the recommended k0 database.
El
A
S Abu (%)
T1/2
Unit
D
dT1/2
0.3
Revised
Comment
Co
Rb
Rb
60
86
1
2
0
0
1,925.3
1.017
2002-09-01
1993-03-15
T
T
=
5.271 Y in Ref. [7]
1/2
M
Y
0.003
= 1.02 M in Ref. [7]
1/2
87 11 27.835
4.8E+10
2.73
1E
09
1993-03-15 No info in Ref. [7]
1993-03-15 No info in Ref. [7]
1993-03-15 No info in Ref. [7]
1993-03-15 No info in Ref. [7]
1993-03-15 No info in Ref. [7]
Sb 125
Ba 140
1
1
0
0
Y
0.03
0.01
12.746
1.4E+10
4.5E+09
D
Th 232 11 100
238 11 99.28
Y
6
E
E
07
06
U
Y
3
Table IV. Changes in the „„k0 (n,f)‟‟ data of the recommended k0 database
dk Revised Revision information
El.
A
S
k
0
E,
0
Ru 103 1 610.3 6.05E 05
Rh 105 2 129.6 1.85E 05
2011-12-07 Removed Ref. [7], old k
2011-12-07 Removed Ref. [7], old k
=
=
9.87E 5.
2.29E 5. Ref. [10]
0
0
Nd 147 1
91.1
2.41E 04
2011-12-07 k -data, type error in Ref. [6]: E
3 instead of E 4
0
guaranteed only if data from well-documented
sources are used. Recommended data libraries
or at least data sets evaluated are the best
choice. Such are the neutron cross sections and
resonance parameters, half-lives and gamma-
ray data from the Evaluated Nuclear Structure
and Decay Data File (ENSDF), as well as the
IV. CONCLUSIONS
An attempt has been made here to
present the state of the art concerning nuclear
data for k0-NAA. In order to be on the safe
side, the experimentalist may follow a few
practical guidelines, which are given below.
Traceability of the experimental procedure is
31
A REVIEW OF NUCLEAR DATA FOR THE K0-BASED NEUTRON ACTIVATION ANALYSIS
[3]. F. De Corte, A. Simonits, k0-measurements
and related nuclear-data compilation for (n,c)
reactor neutron activation analysis. J.
Radioanal. Nucl. Chem. 133, p 43, 1989.
recommended set of gamma-ray standards for
detector calibration. Quality assurance
mandates that only data with clearly specified
uncertainties are used. The data sources that
are recommended here all satisfy this
requirement. On the other hand, some
frequently used books, tables of decay gamma-
rays, do not.
[4]. F. De Corte, A. Simonits, et al, Recent
advances in the k0-NAA: extensions,
applications, prospects. J. Radioanal. Nucl.
Chem. 169, p 125, 1993.
[5]. F. De Corte, S. Van Lierde, A. Simonits, et al, A
re-evaluation of k0 and related nuclear data for
the 555.8 keV gamma-line emitted by the Rh-
104m-Rh-104 mother-daughter pair for use in
NAA. J. Appl. Radiat. Isot. 51, p 701, 1999.
Old handbooks and compilations should
be used with precaution, or rather avoided
entirely, in that many of the data they contain
may have been superseded. (This does not
imply, however, that old data are wrong!)
Sometimes even widely used handbooks quote
data which should be disregarded as, for
instance, the Handbook of Radioanalytical
Chemistry reproducing the outdated tables.
[6]. F. De Corte, S. Van Lierde, Determination and
evaluation of fission k0-factors for correction
of the U-235 (n,f) interference in k0-NAA. J.
Radioanal. Nucl. Chem. 248, p 97, 2001.
[7]. F. De Corte, A. Simonits, Recommended
nuclear data for use in the k0 standardization
of neutron activation analysis. At. Data Nucl.
Data Tables 85, p 47, 2003.
The most up-to-date resources are usually
those available on the Internet home pages of
professional data evaluation and distribution
centres, such as the IAEA Nuclear Data Section,
the NEA Data Bank, and the US National
Nuclear Data Center. A caution is required,
however, concerning uncontrolled Internet sites
providing various kinds of nuclear data.
[8]. V.P. Kolotov, F. De Corte, An electronic
database with a compilation of k0 and related
data for NAA. J. Radioanal. Nucl. Chem. 257,
p 501, 2003.
[9]. M. Blaauw, F. De Corte, Consistency of the
nuclear data in the fundamental databases for
use in the k0-method. J. Nucl. Inst. Meth.
Phys. Res. A 622, p 377, 2010.
ACKNOWLEDGEMENT
This work was supported by the
National Foundation for Science and
[10].F. De Corte, The k0-standardization method: A
move to the optimization of neutron activation
analysis. Aggregate Thesis, Gent University,
Belgium, 1987.
Technology
Development
(NAFOSTED) project under Grant number
“103.04-2017.75”.
[11].F. De Corte. J. Radioanal. Nucl. Chem. 248, p
13, 2001.
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