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NEUTRON ACTIVATION
NEUTRON ACTIVATION
ANALYSIS
ANALYSIS
DR HARSH MOHAN
DR HARSH MOHAN
DEPARTMENT OF PHYSICS
DEPARTMENT OF PHYSICS
M.L.N.COLLEGE
M.L.N.COLLEGE
YAMUNA NAGAR
YAMUNA NAGAR
What is Neutron Activation Analysis
What is Neutron Activation Analysis
(NAA)?
(NAA)?
 NAA
NAA is a method for qualitative and
is a method for qualitative and
quantitative determination of elements based
quantitative determination of elements based
on the measurement of characteristic radiation
on the measurement of characteristic radiation
from radionuclide formed directly or indirectly
from radionuclide formed directly or indirectly
by neutron irradiation of the material.
by neutron irradiation of the material.
INTRODUCTION
INTRODUCTION
HISTORICAL PROSPECTIVE
HISTORICAL PROSPECTIVE
1936 HEVESY AND LEVI
1936 HEVESY AND LEVI
RARE EARTH ELEMENTS
RARE EARTH ELEMENTS
EMPLOY NUC. REACTION
EMPLOY NUC. REACTION
MEASURED GAMMA RAY
MEASURED GAMMA RAY
BASIC PRINCIPAL
BASIC PRINCIPAL
NAA Categories
NAA Categories
 According to type of emitted
According to type of emitted γ
γ-ray measured
-ray measured
 If the Prompt
If the Prompt γ
γ-ray is the measured radiation
-ray is the measured radiation
Prompt
Prompt γ
γ -ray neutron activation analysis
-ray neutron activation analysis
(PGNAA)
(PGNAA)
 The measurements take place during irradiation.
The measurements take place during irradiation.
 If Delayed
If Delayed γ
γ-ray is the measured radiation.
-ray is the measured radiation.
 Delayed
Delayed γ
γ -ray neutron activation analysis
-ray neutron activation analysis
(DGNAA)
(DGNAA)
The measurements take place after a certain decay
The measurements take place after a certain decay
period
period.
.
 (DGNAA) is more common.
(DGNAA) is more common.
I. PGNAA
I. PGNAA
 The PGNAA technique is generally performed by using a beam of
The PGNAA technique is generally performed by using a beam of
neutrons extracted through a reactor beam port.
neutrons extracted through a reactor beam port.
 detectors are placed very close to the sample compensating for
detectors are placed very close to the sample compensating for
much of the loss in sensitivity due to flux.
much of the loss in sensitivity due to flux.
 The PGNAA technique is most applicable to elements with
The PGNAA technique is most applicable to elements with
extremely high neutron capture cross-sections (B, Cd, Sm, and
extremely high neutron capture cross-sections (B, Cd, Sm, and
Gd); elements which decay too rapidly to be measured by
Gd); elements which decay too rapidly to be measured by
DGNAA; elements that produce only stable isotopes; or elements
DGNAA; elements that produce only stable isotopes; or elements
with weak decay gamma-ray intensities.
with weak decay gamma-ray intensities.
II. DGNAA
II. DGNAA
 DGNAA (sometimes called conventional NAA)
DGNAA (sometimes called conventional NAA)
is useful for the
is useful for the vast majority of elements
vast majority of elements that
that
produce radioactive nuclides.
produce radioactive nuclides.
 The technique is flexible with respect to time
The technique is flexible with respect to time
such that the sensitivity for a long-lived
such that the sensitivity for a long-lived
radionuclide that suffers from an interference by
radionuclide that suffers from an interference by
a shorter-lived radionuclide can be improved by
a shorter-lived radionuclide can be improved by
waiting for the short-lived radionuclide to decay
waiting for the short-lived radionuclide to decay.
.
 This selectivity
This selectivity is a key advantage of DGNAA
is a key advantage of DGNAA
over other analytical methods.
over other analytical methods.
Prompt vs. Delayed NAA
Prompt vs. Delayed NAA
 The PGNAA technique is generally performed by
The PGNAA technique is generally performed by
using a beam of neutrons extracted through a
using a beam of neutrons extracted through a
reactor beam port. Fluxes on samples irradiated in
reactor beam port. Fluxes on samples irradiated in
beams are on the order of one million times lower
beams are on the order of one million times lower
than on samples inside a reactor but detectors can
than on samples inside a reactor but detectors can
be placed very close to the sample compensating
be placed very close to the sample compensating
for much of the loss in sensitivity due to flux. The
for much of the loss in sensitivity due to flux. The
PGNAA technique is most applicable to elements
PGNAA technique is most applicable to elements
with extremely high neutron capture cross-
with extremely high neutron capture cross-
sections B, Cd, Sm, and Gd
sections B, Cd, Sm, and Gd
Prompt vs. Delayed NAA
Prompt vs. Delayed NAA
 DGNAA (sometimes called conventional
DGNAA (sometimes called conventional
NAA) is useful for the vast majority of
NAA) is useful for the vast majority of
elements that produce radioactive nuclides.
elements that produce radioactive nuclides.
The technique is flexible with respect to
The technique is flexible with respect to
time such that the sensitivity for a long-
time such that the sensitivity for a long-
lived radionuclide that suffers from an
lived radionuclide that suffers from an
interference by a shorter-lived radionuclide
interference by a shorter-lived radionuclide
can be improved by waiting for the short-
can be improved by waiting for the short-
lived radionuclide to decay
lived radionuclide to decay
Instrumental vs. Radiochemical
Instrumental vs. Radiochemical
NAA
NAA
 The application of purely instrumental
The application of purely instrumental
procedures is commonly called instrumental
procedures is commonly called instrumental
neutron activation analysis (INAA)
neutron activation analysis (INAA)
If chemical separations are done to samples after
irradiation to remove interferences or to
concentrate the radioisotope of interest, the
technique is called radiochemical neutron
activation analysis (RNAA). The latter technique is
performed infrequently due to its high labor cost.
Instrumental vs. Radiochemical
Instrumental vs. Radiochemical
NAA
NAA
 It is generally possible to simultaneously measure more
It is generally possible to simultaneously measure more
than thirty elements in most sample types without
than thirty elements in most sample types without
chemical processing.
chemical processing.
 The application of purely instrumental procedures is
The application of purely instrumental procedures is
commonly called instrumental neutron activation analysis
commonly called instrumental neutron activation analysis
(INAA) and is one of NAA's most important advantages
(INAA) and is one of NAA's most important advantages
over other analytical techniques.
over other analytical techniques.
 If chemical separations
If chemical separations are done to samples after
are done to samples after
irradiation to remove interferences or to concentrate the
irradiation to remove interferences or to concentrate the
radioisotope of interest, the technique is called
radioisotope of interest, the technique is called
radiochemical neutron activation analysis (RNAA).
radiochemical neutron activation analysis (RNAA).
NAA
NAA procedure
procedure
 Sampling;
Sampling;
 Pre-irradiation sample treatment (such as cleaning,
Pre-irradiation sample treatment (such as cleaning,
drying or ashing, pre-concentration of elements of
drying or ashing, pre-concentration of elements of
interest or elimination of interfering elements, sub-
interest or elimination of interfering elements, sub-
sampling and packing);
sampling and packing);
 Irradiation (and prompt gamma-ray counting in
Irradiation (and prompt gamma-ray counting in
PGNAA);
PGNAA);
 Radiochemical separation (
Radiochemical separation (only in RNAA
only in RNAA);
);
 Radioactivity measurement;
Radioactivity measurement;
 Elemental concentration calculation;
Elemental concentration calculation;
 Critical evaluation of results and preparation of the
Critical evaluation of results and preparation of the
NAA report.
NAA report.
Irradiation
Irradiation
 There are several types of neutron sources: reactors,
There are several types of neutron sources: reactors,
accelerators, and radioisotopic neutron emitters.
accelerators, and radioisotopic neutron emitters.
 Nuclear reactors with their
Nuclear reactors with their high fluxes of neutrons
high fluxes of neutrons
offer the highest available sensitivities for most
offer the highest available sensitivities for most
elements.
elements.
 Most neutron energy distributions are quite broad and
Most neutron energy distributions are quite broad and
consist of three principal components
consist of three principal components (thermal,
(thermal,
epithermal, and fast).
epithermal, and fast).
NEUTRON SOURCES
NEUTRON SOURCES
 NEUTRON GENERATORS
NEUTRON GENERATORS
 Accelerators
Accelerators
 14 MeV Neutrons
14 MeV Neutrons
NUCLEAR REACTORS
NUCLEAR REACTORS
maximum thermal power region of 100 kW-10 MW
NEUTRON SOURCES
NEUTRON SOURCES
ISOTOPIC NEUTRON SOURCES
ISOTOPIC NEUTRON SOURCES
Neutron emitter
Neutron emitter Average Neutron energy
Average Neutron energy
Ac
Ac 4 MeV
4 MeV
Ra
Ra 3.6MeV
3.6MeV
Pu
Pu 4.5 MeV
4.5 MeV
Po
Po 4.3 MeV
4.3 MeV
NEUTRON ENERGY
NEUTRON ENERGY
DISTRIBUTION
DISTRIBUTION
NEUTRON ENERGY
NEUTRON ENERGY
 THERMAL NEUTRON
THERMAL NEUTRON
 EPI-THERMAL NEUTRON
EPI-THERMAL NEUTRON
 FAST NEUTRON
FAST NEUTRON
I. Thermal Flux
I. Thermal Flux
 The thermal neutron component consists of low-
The thermal neutron component consists of low-
energy neutrons (energies below 0.5 eV) in
energy neutrons (energies below 0.5 eV) in
thermal equilibrium with atoms in the reactor's
thermal equilibrium with atoms in the reactor's
moderator.
moderator.
 At room temperature, the energy spectrum of
At room temperature, the energy spectrum of
thermal neutrons is best described by a Maxwell-
thermal neutrons is best described by a Maxwell-
Boltzmann distribution with a mean energy of
Boltzmann distribution with a mean energy of
0.025 eV
0.025 eV and a most probable velocity of
and a most probable velocity of 2200
2200
m/s
m/s.
.
 In most reactor irradiation positions,
In most reactor irradiation positions, 90-95%
90-95% of
of
the neutrons that bombard a sample are thermal
the neutrons that bombard a sample are thermal
neutrons.
neutrons.
II. Epithermal Flux
II. Epithermal Flux
 The epithermal neutron component consists of neutrons
The epithermal neutron component consists of neutrons
(energies from 0.5 eV to about 0.5 MeV) which have been only
(energies from 0.5 eV to about 0.5 MeV) which have been only
partially moderated.
partially moderated.
 A
A cadmium foil 1 mm thick
cadmium foil 1 mm thick absorbs all thermal neutrons but
absorbs all thermal neutrons but
will allow epithermal and fast neutrons above 0.5 eV in energy
will allow epithermal and fast neutrons above 0.5 eV in energy
to pass through.
to pass through.
 In a typical unshielded reactor irradiation position, the
In a typical unshielded reactor irradiation position, the
epithermal neutron flux represents about 2% the total neutron
epithermal neutron flux represents about 2% the total neutron
flux.
flux.
 Both thermal and epithermal neutrons induce (n,gamma)
Both thermal and epithermal neutrons induce (n,gamma)
reactions on target nuclei.
reactions on target nuclei.
 An NAA technique that employs only epithermal neutrons to
An NAA technique that employs only epithermal neutrons to
induce (n,gamma) reactions by irradiating the samples being
induce (n,gamma) reactions by irradiating the samples being
analyzed inside either cadmium or boron shields is called
analyzed inside either cadmium or boron shields is called
epithermal neutron activation analysis (ENAA).
epithermal neutron activation analysis (ENAA).
III. Fast Flux
III. Fast Flux
 The fast neutron component of the neutron spectrum
The fast neutron component of the neutron spectrum
(energies above 0.5 MeV) consists of the primary
(energies above 0.5 MeV) consists of the primary
fission neutrons which still have much of their original
fission neutrons which still have much of their original
energy following fission.
energy following fission.
 Fast neutrons
Fast neutrons contribute very little to the (n,gamma)
contribute very little to the (n,gamma)
reaction, but instead induce nuclear reactions where the
reaction, but instead induce nuclear reactions where the
ejection of one or more nuclear particles - (n,p), (n,
ejection of one or more nuclear particles - (n,p), (n,α
α),
),
and (n,2n) - are prevalent.
and (n,2n) - are prevalent.
 In a typical reactor irradiation position, about 5% of
In a typical reactor irradiation position, about 5% of
the total flux consists of fast neutrons.
the total flux consists of fast neutrons.
 An NAA technique that employs nuclear reactions
An NAA technique that employs nuclear reactions
induced by fast neutrons is called
induced by fast neutrons is called fast neutron
fast neutron
activation analysis (FNAA).
activation analysis (FNAA).
Radioactivity Measurement
Radioactivity Measurement
 The instrumentation used to measure
The instrumentation used to measure
gamma rays from radioactive samples
gamma rays from radioactive samples
generally consists of a semiconductor
generally consists of a semiconductor
detector, associated electronics, and a
detector, associated electronics, and a
computer-based, multi-channel analyzer
computer-based, multi-channel analyzer
(MCA/computer).
(MCA/computer).
 Most NAA labs operate one or more
Most NAA labs operate one or more hyper
hyper
pure germanium detector (HPGe).
pure germanium detector (HPGe).
Gamma-Spectroscopy System
Gamma-Spectroscopy System
Calibration
Calibration
 Energy Calibration
Energy Calibration
 FWHM Calibration
FWHM Calibration
 Efficiency Calibration
Efficiency Calibration
Measurement of Gamma Rays
Measurement of Gamma Rays
 . Other characteristics to consider are peak
. Other characteristics to consider are peak
shape, peak-to-Compton ratio, crystal
shape, peak-to-Compton ratio, crystal
dimensions or shape, and price.
dimensions or shape, and price.
Measurement of Gamma Rays
Measurement of Gamma Rays
 The detector's resolution is a measure of its ability
The detector's resolution is a measure of its ability
to separate closely spaced peaks in a spectrum. In
to separate closely spaced peaks in a spectrum. In
general, detector resolution is specified in terms of
general, detector resolution is specified in terms of
the full width at half maximum (FWHM) of the
the full width at half maximum (FWHM) of the
122-keV photopeak of Co-57 and the 1332-keV
122-keV photopeak of Co-57 and the 1332-keV
photopeak of Co-60. For most NAA applications,
photopeak of Co-60. For most NAA applications,
a detector with 1.0-keV resolution or below at 122
a detector with 1.0-keV resolution or below at 122
keV and 1.8 keV or below at 1332 keV is
keV and 1.8 keV or below at 1332 keV is
sufficient.
sufficient.
Measurement of Gamma Rays
Measurement of Gamma Rays
 Detector efficiency depends on the energy
Detector efficiency depends on the energy
of the measured radiation, the solid angle
of the measured radiation, the solid angle
between sample and detector crystal, and
between sample and detector crystal, and
the active volume of the crystal. A larger
the active volume of the crystal. A larger
volume detector will have a higher
volume detector will have a higher
efficiency
efficiency
 As detector volume increases, the detector
As detector volume increases, the detector
resolution gradually decreases
resolution gradually decreases
Gamma-ray spectrum from an
Gamma-ray spectrum from an
irradiated pottery specimen
irradiated pottery specimen
Gamma-ray spectrum from 0 to 800 keV
Gamma-ray spectrum from 0 to 800 keV
showing medium- and long-lived elements
showing medium- and long-lived elements
measured in a sample
measured in a sample
Kinetics of activation
Kinetics of activation
 R = N (
R = N (φ
φth
th·
·σ
σth
th +
+ φ
φe
e · I
· I0
0 )
)
R= reaction rate
R= reaction rate
 σ
σth
th:
: conventional thermal neutron flux [in cm
conventional thermal neutron flux [in cm2
2
]
]
 φ
φth
th :
: effective thermal neutron cross-section [in
effective thermal neutron cross-section [in
cm
cm2
2
]
]
 φ
φe
e:
: conventional epithermal neutron flux [in cm
conventional epithermal neutron flux [in cm-2
-2
s
s-
-
1
1
eV]
eV]
I
Io
o:
: resonance integral cross section (in epithermal
resonance integral cross section (in epithermal
region), for 1/E epithermal spectrum [in cm
region), for 1/E epithermal spectrum [in cm2
2
]
]

Kinetics of activation
Kinetics of activation
 The activity (A) of the isotopes depends on
The activity (A) of the isotopes depends on
time. During irradiation the activity of the
time. During irradiation the activity of the
radioactive isotope produced grows
radioactive isotope produced grows
according to a saturation characteristic
according to a saturation characteristic
governed by a saturation factor S=1-e
governed by a saturation factor S=1-e-
-λ
λt
t
i
i.
.
Subsequent to the irradiation the isotope
Subsequent to the irradiation the isotope
decays according to the exponential law:
decays according to the exponential law:
D=e
D=e-
-λ
λ t
t
d
d:
:
 Where t
Where ti
i : time of irradiation; t
: time of irradiation; td
d : time of
: time of
decay;
decay; λ
λ : decay constant
: decay constant
Kinetics of activation
Kinetics of activation
 A=
A= I
e
th
th ⋅
+
⋅ ϕ
σ
ϕ
D
S
A
N
f
m
rel
Av
i
⋅
⋅
⋅
⋅
NAv
= Avogadro number
fi
= isotopic abundance
m = the mass of the irradiated element
Arel
= atomic mass of target element
Kinetics of activation
Kinetics of activation
 The intensity of the measured gamma line is
The intensity of the measured gamma line is
proportional to the activity. The measured
proportional to the activity. The measured
parameter is the total energy peak area (N
parameter is the total energy peak area (NP
P)
)
at a particular energy given by the
at a particular energy given by the
following equation (x)
following equation (x)
N A f t
P m
= ⋅ ⋅ ⋅
γ γ
ε
Kinetics of activation
Kinetics of activation
 The efficiency (
The efficiency (ε
εγ
γ) of a semiconductor
) of a semiconductor
detector varies with gamma energy. The
detector varies with gamma energy. The
emission probability of a gamma photon at
emission probability of a gamma photon at
a given energy is the f
a given energy is the fγ
γ, t
, tm
m is the measuring
is the measuring
time.
time.
Measurement and evaluation
Measurement and evaluation
 The modern gamma measuring systems consist of
The modern gamma measuring systems consist of
a gamma detector, usually a HPGe type and
a gamma detector, usually a HPGe type and
sometimes NaI(Tl) scintillation crystals. The
sometimes NaI(Tl) scintillation crystals. The
detectors are connected to a multichannel analyzer
detectors are connected to a multichannel analyzer
(MCA) by an appropriate electronic system
(MCA) by an appropriate electronic system
(preamlifier, spectroscopy amplifier, etc.).
(preamlifier, spectroscopy amplifier, etc.).
Nowadays, the MCAs are computer based systems
Nowadays, the MCAs are computer based systems
with the ability of an automatic spectrum
with the ability of an automatic spectrum
evaluation.
evaluation.
Analysis of the gamma spectra
Analysis of the gamma spectra
 The usual objective of the measurements
The usual objective of the measurements
by gamma ray spectrometers is the
by gamma ray spectrometers is the
determination of the number and energy
determination of the number and energy
of the photons emitted by the source.
of the photons emitted by the source.
The peak location and the peak area in
The peak location and the peak area in
the spectra have to be determined. The
the spectra have to be determined. The
peak location is a measure of the gamma
peak location is a measure of the gamma
energy, while the peak area is
energy, while the peak area is
proportional to the photon emission rate
proportional to the photon emission rate
Analysis of the gamma spectra
Analysis of the gamma spectra
 For the energy measurement the pulse
For the energy measurement the pulse
height scale must be calibrated with
height scale must be calibrated with
standard sources emitting photons of
standard sources emitting photons of
known energies
known energies
 In order to calculate the activities, the full-
In order to calculate the activities, the full-
energy-peak efficiencies of the source-
energy-peak efficiencies of the source-
detector system have to be determined by
detector system have to be determined by
using sources of known activities.
using sources of known activities.
Analysis of the gamma spectra
Analysis of the gamma spectra
 For the determination of the peak areas the
For the determination of the peak areas the
background under the peak interval has to be
background under the peak interval has to be
subtracted. The net count (Np) results from N
subtracted. The net count (Np) results from NP
P =
=
N
Nint
int - N
- NB
B, (N
, (Nint
int integral under the peak and N
integral under the peak and NB
B refers
refers
to the background).
to the background).
 The peak area can also be calculated by computer
The peak area can also be calculated by computer
programs which fit an analytical function to the
programs which fit an analytical function to the
peak. The shape is described basically by a
peak. The shape is described basically by a
Gaussian function, modified by suitable auxiliary
Gaussian function, modified by suitable auxiliary
functions. Thus all the peaks including also the
functions. Thus all the peaks including also the
multiplets can be automatically analysed.
multiplets can be automatically analysed.
Quantitative Analysis
Quantitative Analysis
 Absolute method
Absolute method
 The quantitative measurement can be
The quantitative measurement can be
effected by determining the neutron flux
effected by determining the neutron flux
and counting the absolute gamma rays.
and counting the absolute gamma rays.
The direct calculation of concentration is
The direct calculation of concentration is
made by applying nuclear constants
made by applying nuclear constants
according to Eq
according to Eq (x)
(x)
Quantitative Analysis
Quantitative Analysis
 Classic relative method
Classic relative method
 The method is based on the simultaneous
The method is based on the simultaneous
irradiation of the sample with standards of known
irradiation of the sample with standards of known
quantities of the elements in question in identical
quantities of the elements in question in identical
positions, followed by measuring the induced
positions, followed by measuring the induced
intensities of both the standard and the sample in a
intensities of both the standard and the sample in a
well known geometrical position.
well known geometrical position.
 A relative standardisation can be performed by
A relative standardisation can be performed by
means of individual monoelement standards, or
means of individual monoelement standards, or
by using synthetic or natural multielement
by using synthetic or natural multielement
standards.
standards.
Classic relative method
Classic relative method
 The equation used to calculate the mass of
The equation used to calculate the mass of
an element in the unknown sample relative
an element in the unknown sample relative
to the comparator standard
to the comparator standard
Classic relative method
Classic relative method
 Where A = activity of the sample (sam) and
Where A = activity of the sample (sam) and
standard (std),
standard (std),
M = mass of the element,
M = mass of the element,
= decay constant for the
= decay constant for the
isotope and =
isotope and =
decay time
decay time
Classic relative method
Classic relative method
 When performing short irradiations, the
When performing short irradiations, the
irradiation, decay and counting times are
irradiation, decay and counting times are
normally fixed the same for all samples and
normally fixed the same for all samples and
standards such that the time dependent
standards such that the time dependent
factors cancel. Thus the equation
factors cancel. Thus the equation
simplifies into
simplifies into
Classic relative method
Classic relative method
 Where C = concentration of the element
Where C = concentration of the element
W= weight of the sample and standard
W= weight of the sample and standard
Counting statistics
Counting statistics
 The nuclear decay processes occur at random, and
The nuclear decay processes occur at random, and
follow a Poisson distribution, where the standard
follow a Poisson distribution, where the standard
deviation (
deviation (σ)
σ) equals to N
equals to N1/2
1/2
(N is the observed
(N is the observed
number of events). In gamma spectrometry, the
number of events). In gamma spectrometry, the
peak area is the measured parameter. The standard
peak area is the measured parameter. The standard
deviation is:
deviation is: σ
σ = (N+2N
= (N+2NB
B)
)1/2
1/2
where the
where the
confidence level is 68%.
confidence level is 68%.
 The counting statistic is only one of the possible
The counting statistic is only one of the possible
sources of errors in NAA, the overall value
sources of errors in NAA, the overall value
depending on a number of different factors (e.g.
depending on a number of different factors (e.g.
sample preparation, weighing, and uncertainty of
sample preparation, weighing, and uncertainty of
standardisation).
standardisation).
Equipment and materials
Equipment and materials
 - sample for analysis hair sample, soil or
- sample for analysis hair sample, soil or
steel etc.
steel etc.
 - analytical balance
- analytical balance
 - micropipette
- micropipette
 - reactor for irradiation
- reactor for irradiation
 - HPGe detector, spectrometer
- HPGe detector, spectrometer
Procedure
Procedure
 1 .Choose the proper -nuclear reaction
1 .Choose the proper -nuclear reaction
-analytical gamma
-analytical gamma
line
line
-irradiation, decay
-irradiation, decay
and measuring time
and measuring time
Procedure
Procedure
 2.
2. Sample preparation:
Sample preparation:
 - weigh the samples into polyethylene
- weigh the samples into polyethylene
bags using analytical balance
bags using analytical balance
 - prepare standards using micropipettes
- prepare standards using micropipettes
Procedure
Procedure
 3.
3. Irradiation of the samples using pneumatic
Irradiation of the samples using pneumatic
system of the reactor
system of the reactor
 4.
4. Measure the gamma-spectra, evaluate the
Measure the gamma-spectra, evaluate the
spectra (determine the peak areas at the given
spectra (determine the peak areas at the given
gamma-lines)
gamma-lines)
 5.
5. Identify the isotopes in the spectra using
Identify the isotopes in the spectra using
gamma library. Determine the elemental
gamma library. Determine the elemental
concentrations and their uncertainties using
concentrations and their uncertainties using
standard method
standard method
Sensitivities Available by NAA
Sensitivities Available by NAA
 The sensitivities for NAA are dependent upon the
The sensitivities for NAA are dependent upon the
irradiation parameters (i.e., neutron flux,
irradiation parameters (i.e., neutron flux,
irradiation and decay times), measurement
irradiation and decay times), measurement
conditions (i.e., measurement time, detector
conditions (i.e., measurement time, detector
efficiency), nuclear parameters of the elements
efficiency), nuclear parameters of the elements
being measured (i.e., isotope abundance, neutron
being measured (i.e., isotope abundance, neutron
cross-section, half-life, and gamma-ray
cross-section, half-life, and gamma-ray
abundance). The accuracy of an individual NAA
abundance). The accuracy of an individual NAA
determination usually ranges between 1 to 10
determination usually ranges between 1 to 10
percent of the reported value.
percent of the reported value.
Detection Limits
Detection Limits
 The detection limit represents the ability of a
The detection limit represents the ability of a
given NAA procedure to determine the
given NAA procedure to determine the
minimum amounts of an element reliably.
minimum amounts of an element reliably.
 The detection limit depends on the:
The detection limit depends on the:
(1)The amount of material to be irradiated and to be counted.
(1)The amount of material to be irradiated and to be counted..
.
(2)
(2) The neutron fluxes.
The neutron fluxes.
(3)
(3) The duration of the irradiation time.
The duration of the irradiation time.
(4)
(4) The total induced radioactivity that can be
The total induced radioactivity that can be
(5)The duration of the counting time
(5)The duration of the counting time
(6)
(6) The detector size, counting geometry and background
The detector size, counting geometry and background
shielding.
shielding.
Advantages of NAA
Advantages of NAA
 Very low detection limits for 30–40 elements,
Very low detection limits for 30–40 elements,
 Significant matrix independence,
Significant matrix independence,
 The possibility of non-destructive analysis
The possibility of non-destructive analysis
(instrumental NAA or INAA),
(instrumental NAA or INAA),
 The use of radiochemical separation to overcome
The use of radiochemical separation to overcome
interference in complex gamma-ray spectra
interference in complex gamma-ray spectra
(radiochemical NAA or RNAA),
(radiochemical NAA or RNAA),
 An inherent capability for high levels of accuracy
An inherent capability for high levels of accuracy
compared to other trace element analysis
compared to other trace element analysis
techniques.
techniques.
NAA Applications
NAA Applications
 Archaeology
Archaeology
 Biomedicine
Biomedicine
 Environmental science and related fields
Environmental science and related fields
 Geology and geochemistry
Geology and geochemistry
 Industrial products
Industrial products
 Nutrition
Nutrition
 Quality assurance of analysis and reference
Quality assurance of analysis and reference
materials
materials
Applications for NAA
Applications for NAA
 1.
1. Archaeology
Archaeology
 The use of neutron activation analysis to
The use of neutron activation analysis to
characterize archaeological specimens (e.g.,
characterize archaeological specimens (e.g.,
pottery, obsidian, chert, basalt and
pottery, obsidian, chert, basalt and
limestone) and to relate the artifacts to
limestone) and to relate the artifacts to
sources through their chemical signatures is
sources through their chemical signatures is
a well-established application of the
a well-established application of the
method.
method.
Neutron activation of paintings
Neutron activation of paintings
Applications for NAA
Applications for NAA
 Geological science
Geological science
 Analysis of rock specimens by neutron activation
Analysis of rock specimens by neutron activation
analysis assists geochemists in research on the
analysis assists geochemists in research on the
processes involved in the formation of different
processes involved in the formation of different
rocks through the analysis of the rare earth
rocks through the analysis of the rare earth
elements (REEs) and other trace elements. About
elements (REEs) and other trace elements. About
thirty elements can be measured routinely in
thirty elements can be measured routinely in
almost any geological sample. An additional 15-
almost any geological sample. An additional 15-
20 elements can be measured by applying
20 elements can be measured by applying
specialized procedures
specialized procedures
Applications for NAA
Applications for NAA
 Semiconductor materials and other high-purity
Semiconductor materials and other high-purity
materials
materials
 Neutron Activation Analysis (NAA)
Neutron Activation Analysis (NAA) is used to
is used to
measure trace- and ultra trace-element
measure trace- and ultra trace-element
concentrations of impurities and/or dopants in
concentrations of impurities and/or dopants in
semiconductors and other high-purity materials.
semiconductors and other high-purity materials.
The behavior of semiconductor devices is strongly
The behavior of semiconductor devices is strongly
influenced by the presence of impurity elements
influenced by the presence of impurity elements
either added intentionally (doping with B, P, As,
either added intentionally (doping with B, P, As,
Au, etc.) or contaminants remaining due to
Au, etc.) or contaminants remaining due to
incomplete purification of the semiconductor
incomplete purification of the semiconductor
material during device manufacture.
material during device manufacture.
Applications for NAA
Applications for NAA
 Soil Science
Soil Science
 Many agricultural processes and their
Many agricultural processes and their
consequences, such as fertilization and herbicidal
consequences, such as fertilization and herbicidal
and pesticidal control, are influenced by surface
and pesticidal control, are influenced by surface
and sub-surface movement, percolation and
and sub-surface movement, percolation and
infiltration of water. Stable activatable tracers,
infiltration of water. Stable activatable tracers,
such as bromide, analyzed by NAA, have allowed
such as bromide, analyzed by NAA, have allowed
the soil scientist to quantify the distribution of
the soil scientist to quantify the distribution of
agricultural chemicals under a wide variety of
agricultural chemicals under a wide variety of
environmental and land use influences
environmental and land use influences
Obtain plant sample. Wash the sample to
Obtain plant sample. Wash the sample to
remove possible contaminants
remove possible contaminants
Dehydrate the sample.
Dehydrate the sample.
 Dehydration methods
Dehydration methods
use heat or freeze-
use heat or freeze-
drying.
drying.
 A lyophilizer is frequently
A lyophilizer is frequently
used for the freeze-dry
used for the freeze-dry
method.
method.
 A plant sample is then
A plant sample is then
placed in the chamber
placed in the chamber
atop the lyophilizer to the
atop the lyophilizer to the
right.
right.
The dehydrated sample is then prepared for
The dehydrated sample is then prepared for
testing. A small amount of dehydrated plant
testing. A small amount of dehydrated plant
material is removed from this bag.
material is removed from this bag.
A portion of the dried plant material is ground into a powder
A portion of the dried plant material is ground into a powder
using a mortar and pestle. Sterile technique is required
using a mortar and pestle. Sterile technique is required
to avoid cross contamination
to avoid cross contamination.
.
Bag the sample. Some of the ground plant powder
Bag the sample. Some of the ground plant powder
is bagged into a small plastic envelope. The sample
is bagged into a small plastic envelope. The sample
is double-bagged and labeled
is double-bagged and labeled.
.
Select a standard for comparison.
Select a standard for comparison.
 When looking for arsenic in
When looking for arsenic in
plant material, you would need
plant material, you would need
to prepare a sample of a
to prepare a sample of a
standard containing arsenic.
standard containing arsenic.
 The “standard” contains a
The “standard” contains a
known quantity of the element
known quantity of the element
you are looking for.
you are looking for.
 Containers of certified
Containers of certified
standards are pictured.
standards are pictured.
Place packages of both the prepared sample and
Place packages of both the prepared sample and
standard sample in a capsule.
standard sample in a capsule.
Take sample to the rabbit system apparatus.
Take sample to the rabbit system apparatus.
 The rabbit system works much
The rabbit system works much
like the system used by banks at
like the system used by banks at
drive-through windows. A
drive-through windows. A
canister carries items back and
canister carries items back and
forth between the customer and
forth between the customer and
teller.
teller.
 The sample is sent through the
The sample is sent through the
wall in a mini canister into the
wall in a mini canister into the
nuclear reactor located behind the
nuclear reactor located behind the
wall.
wall.
 Once inside the reactor, the
Once inside the reactor, the
sample is irradiated with
sample is irradiated with
neutrons.
neutrons.
After irradiation of the sample in the capsule, and before removing
After irradiation of the sample in the capsule, and before removing
it from the reactor site, it must be determined if the capsule is safe
it from the reactor site, it must be determined if the capsule is safe
for transfer. A Geiger counter is used to assess whether the
for transfer. A Geiger counter is used to assess whether the
radioactive decay has reached low enough levels to be safe.
radioactive decay has reached low enough levels to be safe.
The prepared sample and standard sample are placed
The prepared sample and standard sample are placed
in a “detector” one at a time.
in a “detector” one at a time.
 The detector system
The detector system
counts and records
counts and records
gamma radiation
gamma radiation
emissions for a period
emissions for a period
of time.
of time.
 Time varies, but is
Time varies, but is
usually in the range of 5
usually in the range of 5
minutes to an hour.
minutes to an hour.
Counts recorded by the detector system is sent
Counts recorded by the detector system is sent
to a computer.
to a computer.
12. Specialized software analyzes radiation peaks.
12. Specialized software analyzes radiation peaks.
Peak data is correlated to specific elements for
Peak data is correlated to specific elements for
identification and quantification.
identification and quantification.
Computer data is compared to a nuclide chart
Computer data is compared to a nuclide chart
to evaluate the results.
to evaluate the results.
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soil analysis with different techinques.

  • 1. NEUTRON ACTIVATION NEUTRON ACTIVATION ANALYSIS ANALYSIS DR HARSH MOHAN DR HARSH MOHAN DEPARTMENT OF PHYSICS DEPARTMENT OF PHYSICS M.L.N.COLLEGE M.L.N.COLLEGE YAMUNA NAGAR YAMUNA NAGAR
  • 2. What is Neutron Activation Analysis What is Neutron Activation Analysis (NAA)? (NAA)?  NAA NAA is a method for qualitative and is a method for qualitative and quantitative determination of elements based quantitative determination of elements based on the measurement of characteristic radiation on the measurement of characteristic radiation from radionuclide formed directly or indirectly from radionuclide formed directly or indirectly by neutron irradiation of the material. by neutron irradiation of the material. INTRODUCTION INTRODUCTION
  • 3. HISTORICAL PROSPECTIVE HISTORICAL PROSPECTIVE 1936 HEVESY AND LEVI 1936 HEVESY AND LEVI RARE EARTH ELEMENTS RARE EARTH ELEMENTS EMPLOY NUC. REACTION EMPLOY NUC. REACTION MEASURED GAMMA RAY MEASURED GAMMA RAY
  • 5. NAA Categories NAA Categories  According to type of emitted According to type of emitted γ γ-ray measured -ray measured  If the Prompt If the Prompt γ γ-ray is the measured radiation -ray is the measured radiation Prompt Prompt γ γ -ray neutron activation analysis -ray neutron activation analysis (PGNAA) (PGNAA)  The measurements take place during irradiation. The measurements take place during irradiation.  If Delayed If Delayed γ γ-ray is the measured radiation. -ray is the measured radiation.  Delayed Delayed γ γ -ray neutron activation analysis -ray neutron activation analysis (DGNAA) (DGNAA) The measurements take place after a certain decay The measurements take place after a certain decay period period. .  (DGNAA) is more common. (DGNAA) is more common.
  • 6. I. PGNAA I. PGNAA  The PGNAA technique is generally performed by using a beam of The PGNAA technique is generally performed by using a beam of neutrons extracted through a reactor beam port. neutrons extracted through a reactor beam port.  detectors are placed very close to the sample compensating for detectors are placed very close to the sample compensating for much of the loss in sensitivity due to flux. much of the loss in sensitivity due to flux.  The PGNAA technique is most applicable to elements with The PGNAA technique is most applicable to elements with extremely high neutron capture cross-sections (B, Cd, Sm, and extremely high neutron capture cross-sections (B, Cd, Sm, and Gd); elements which decay too rapidly to be measured by Gd); elements which decay too rapidly to be measured by DGNAA; elements that produce only stable isotopes; or elements DGNAA; elements that produce only stable isotopes; or elements with weak decay gamma-ray intensities. with weak decay gamma-ray intensities.
  • 7. II. DGNAA II. DGNAA  DGNAA (sometimes called conventional NAA) DGNAA (sometimes called conventional NAA) is useful for the is useful for the vast majority of elements vast majority of elements that that produce radioactive nuclides. produce radioactive nuclides.  The technique is flexible with respect to time The technique is flexible with respect to time such that the sensitivity for a long-lived such that the sensitivity for a long-lived radionuclide that suffers from an interference by radionuclide that suffers from an interference by a shorter-lived radionuclide can be improved by a shorter-lived radionuclide can be improved by waiting for the short-lived radionuclide to decay waiting for the short-lived radionuclide to decay. .  This selectivity This selectivity is a key advantage of DGNAA is a key advantage of DGNAA over other analytical methods. over other analytical methods.
  • 8. Prompt vs. Delayed NAA Prompt vs. Delayed NAA  The PGNAA technique is generally performed by The PGNAA technique is generally performed by using a beam of neutrons extracted through a using a beam of neutrons extracted through a reactor beam port. Fluxes on samples irradiated in reactor beam port. Fluxes on samples irradiated in beams are on the order of one million times lower beams are on the order of one million times lower than on samples inside a reactor but detectors can than on samples inside a reactor but detectors can be placed very close to the sample compensating be placed very close to the sample compensating for much of the loss in sensitivity due to flux. The for much of the loss in sensitivity due to flux. The PGNAA technique is most applicable to elements PGNAA technique is most applicable to elements with extremely high neutron capture cross- with extremely high neutron capture cross- sections B, Cd, Sm, and Gd sections B, Cd, Sm, and Gd
  • 9. Prompt vs. Delayed NAA Prompt vs. Delayed NAA  DGNAA (sometimes called conventional DGNAA (sometimes called conventional NAA) is useful for the vast majority of NAA) is useful for the vast majority of elements that produce radioactive nuclides. elements that produce radioactive nuclides. The technique is flexible with respect to The technique is flexible with respect to time such that the sensitivity for a long- time such that the sensitivity for a long- lived radionuclide that suffers from an lived radionuclide that suffers from an interference by a shorter-lived radionuclide interference by a shorter-lived radionuclide can be improved by waiting for the short- can be improved by waiting for the short- lived radionuclide to decay lived radionuclide to decay
  • 10. Instrumental vs. Radiochemical Instrumental vs. Radiochemical NAA NAA  The application of purely instrumental The application of purely instrumental procedures is commonly called instrumental procedures is commonly called instrumental neutron activation analysis (INAA) neutron activation analysis (INAA) If chemical separations are done to samples after irradiation to remove interferences or to concentrate the radioisotope of interest, the technique is called radiochemical neutron activation analysis (RNAA). The latter technique is performed infrequently due to its high labor cost.
  • 11. Instrumental vs. Radiochemical Instrumental vs. Radiochemical NAA NAA  It is generally possible to simultaneously measure more It is generally possible to simultaneously measure more than thirty elements in most sample types without than thirty elements in most sample types without chemical processing. chemical processing.  The application of purely instrumental procedures is The application of purely instrumental procedures is commonly called instrumental neutron activation analysis commonly called instrumental neutron activation analysis (INAA) and is one of NAA's most important advantages (INAA) and is one of NAA's most important advantages over other analytical techniques. over other analytical techniques.  If chemical separations If chemical separations are done to samples after are done to samples after irradiation to remove interferences or to concentrate the irradiation to remove interferences or to concentrate the radioisotope of interest, the technique is called radioisotope of interest, the technique is called radiochemical neutron activation analysis (RNAA). radiochemical neutron activation analysis (RNAA).
  • 12. NAA NAA procedure procedure  Sampling; Sampling;  Pre-irradiation sample treatment (such as cleaning, Pre-irradiation sample treatment (such as cleaning, drying or ashing, pre-concentration of elements of drying or ashing, pre-concentration of elements of interest or elimination of interfering elements, sub- interest or elimination of interfering elements, sub- sampling and packing); sampling and packing);  Irradiation (and prompt gamma-ray counting in Irradiation (and prompt gamma-ray counting in PGNAA); PGNAA);  Radiochemical separation ( Radiochemical separation (only in RNAA only in RNAA); );  Radioactivity measurement; Radioactivity measurement;  Elemental concentration calculation; Elemental concentration calculation;  Critical evaluation of results and preparation of the Critical evaluation of results and preparation of the NAA report. NAA report.
  • 13. Irradiation Irradiation  There are several types of neutron sources: reactors, There are several types of neutron sources: reactors, accelerators, and radioisotopic neutron emitters. accelerators, and radioisotopic neutron emitters.  Nuclear reactors with their Nuclear reactors with their high fluxes of neutrons high fluxes of neutrons offer the highest available sensitivities for most offer the highest available sensitivities for most elements. elements.  Most neutron energy distributions are quite broad and Most neutron energy distributions are quite broad and consist of three principal components consist of three principal components (thermal, (thermal, epithermal, and fast). epithermal, and fast).
  • 14. NEUTRON SOURCES NEUTRON SOURCES  NEUTRON GENERATORS NEUTRON GENERATORS  Accelerators Accelerators  14 MeV Neutrons 14 MeV Neutrons NUCLEAR REACTORS NUCLEAR REACTORS maximum thermal power region of 100 kW-10 MW
  • 15. NEUTRON SOURCES NEUTRON SOURCES ISOTOPIC NEUTRON SOURCES ISOTOPIC NEUTRON SOURCES Neutron emitter Neutron emitter Average Neutron energy Average Neutron energy Ac Ac 4 MeV 4 MeV Ra Ra 3.6MeV 3.6MeV Pu Pu 4.5 MeV 4.5 MeV Po Po 4.3 MeV 4.3 MeV
  • 17. NEUTRON ENERGY NEUTRON ENERGY  THERMAL NEUTRON THERMAL NEUTRON  EPI-THERMAL NEUTRON EPI-THERMAL NEUTRON  FAST NEUTRON FAST NEUTRON
  • 18. I. Thermal Flux I. Thermal Flux  The thermal neutron component consists of low- The thermal neutron component consists of low- energy neutrons (energies below 0.5 eV) in energy neutrons (energies below 0.5 eV) in thermal equilibrium with atoms in the reactor's thermal equilibrium with atoms in the reactor's moderator. moderator.  At room temperature, the energy spectrum of At room temperature, the energy spectrum of thermal neutrons is best described by a Maxwell- thermal neutrons is best described by a Maxwell- Boltzmann distribution with a mean energy of Boltzmann distribution with a mean energy of 0.025 eV 0.025 eV and a most probable velocity of and a most probable velocity of 2200 2200 m/s m/s. .  In most reactor irradiation positions, In most reactor irradiation positions, 90-95% 90-95% of of the neutrons that bombard a sample are thermal the neutrons that bombard a sample are thermal neutrons. neutrons.
  • 19. II. Epithermal Flux II. Epithermal Flux  The epithermal neutron component consists of neutrons The epithermal neutron component consists of neutrons (energies from 0.5 eV to about 0.5 MeV) which have been only (energies from 0.5 eV to about 0.5 MeV) which have been only partially moderated. partially moderated.  A A cadmium foil 1 mm thick cadmium foil 1 mm thick absorbs all thermal neutrons but absorbs all thermal neutrons but will allow epithermal and fast neutrons above 0.5 eV in energy will allow epithermal and fast neutrons above 0.5 eV in energy to pass through. to pass through.  In a typical unshielded reactor irradiation position, the In a typical unshielded reactor irradiation position, the epithermal neutron flux represents about 2% the total neutron epithermal neutron flux represents about 2% the total neutron flux. flux.  Both thermal and epithermal neutrons induce (n,gamma) Both thermal and epithermal neutrons induce (n,gamma) reactions on target nuclei. reactions on target nuclei.  An NAA technique that employs only epithermal neutrons to An NAA technique that employs only epithermal neutrons to induce (n,gamma) reactions by irradiating the samples being induce (n,gamma) reactions by irradiating the samples being analyzed inside either cadmium or boron shields is called analyzed inside either cadmium or boron shields is called epithermal neutron activation analysis (ENAA). epithermal neutron activation analysis (ENAA).
  • 20. III. Fast Flux III. Fast Flux  The fast neutron component of the neutron spectrum The fast neutron component of the neutron spectrum (energies above 0.5 MeV) consists of the primary (energies above 0.5 MeV) consists of the primary fission neutrons which still have much of their original fission neutrons which still have much of their original energy following fission. energy following fission.  Fast neutrons Fast neutrons contribute very little to the (n,gamma) contribute very little to the (n,gamma) reaction, but instead induce nuclear reactions where the reaction, but instead induce nuclear reactions where the ejection of one or more nuclear particles - (n,p), (n, ejection of one or more nuclear particles - (n,p), (n,α α), ), and (n,2n) - are prevalent. and (n,2n) - are prevalent.  In a typical reactor irradiation position, about 5% of In a typical reactor irradiation position, about 5% of the total flux consists of fast neutrons. the total flux consists of fast neutrons.  An NAA technique that employs nuclear reactions An NAA technique that employs nuclear reactions induced by fast neutrons is called induced by fast neutrons is called fast neutron fast neutron activation analysis (FNAA). activation analysis (FNAA).
  • 21. Radioactivity Measurement Radioactivity Measurement  The instrumentation used to measure The instrumentation used to measure gamma rays from radioactive samples gamma rays from radioactive samples generally consists of a semiconductor generally consists of a semiconductor detector, associated electronics, and a detector, associated electronics, and a computer-based, multi-channel analyzer computer-based, multi-channel analyzer (MCA/computer). (MCA/computer).  Most NAA labs operate one or more Most NAA labs operate one or more hyper hyper pure germanium detector (HPGe). pure germanium detector (HPGe).
  • 23. Calibration Calibration  Energy Calibration Energy Calibration  FWHM Calibration FWHM Calibration  Efficiency Calibration Efficiency Calibration
  • 24. Measurement of Gamma Rays Measurement of Gamma Rays  . Other characteristics to consider are peak . Other characteristics to consider are peak shape, peak-to-Compton ratio, crystal shape, peak-to-Compton ratio, crystal dimensions or shape, and price. dimensions or shape, and price.
  • 25. Measurement of Gamma Rays Measurement of Gamma Rays  The detector's resolution is a measure of its ability The detector's resolution is a measure of its ability to separate closely spaced peaks in a spectrum. In to separate closely spaced peaks in a spectrum. In general, detector resolution is specified in terms of general, detector resolution is specified in terms of the full width at half maximum (FWHM) of the the full width at half maximum (FWHM) of the 122-keV photopeak of Co-57 and the 1332-keV 122-keV photopeak of Co-57 and the 1332-keV photopeak of Co-60. For most NAA applications, photopeak of Co-60. For most NAA applications, a detector with 1.0-keV resolution or below at 122 a detector with 1.0-keV resolution or below at 122 keV and 1.8 keV or below at 1332 keV is keV and 1.8 keV or below at 1332 keV is sufficient. sufficient.
  • 26. Measurement of Gamma Rays Measurement of Gamma Rays  Detector efficiency depends on the energy Detector efficiency depends on the energy of the measured radiation, the solid angle of the measured radiation, the solid angle between sample and detector crystal, and between sample and detector crystal, and the active volume of the crystal. A larger the active volume of the crystal. A larger volume detector will have a higher volume detector will have a higher efficiency efficiency  As detector volume increases, the detector As detector volume increases, the detector resolution gradually decreases resolution gradually decreases
  • 27. Gamma-ray spectrum from an Gamma-ray spectrum from an irradiated pottery specimen irradiated pottery specimen
  • 28. Gamma-ray spectrum from 0 to 800 keV Gamma-ray spectrum from 0 to 800 keV showing medium- and long-lived elements showing medium- and long-lived elements measured in a sample measured in a sample
  • 29. Kinetics of activation Kinetics of activation  R = N ( R = N (φ φth th· ·σ σth th + + φ φe e · I · I0 0 ) ) R= reaction rate R= reaction rate  σ σth th: : conventional thermal neutron flux [in cm conventional thermal neutron flux [in cm2 2 ] ]  φ φth th : : effective thermal neutron cross-section [in effective thermal neutron cross-section [in cm cm2 2 ] ]  φ φe e: : conventional epithermal neutron flux [in cm conventional epithermal neutron flux [in cm-2 -2 s s- - 1 1 eV] eV] I Io o: : resonance integral cross section (in epithermal resonance integral cross section (in epithermal region), for 1/E epithermal spectrum [in cm region), for 1/E epithermal spectrum [in cm2 2 ] ] 
  • 30. Kinetics of activation Kinetics of activation  The activity (A) of the isotopes depends on The activity (A) of the isotopes depends on time. During irradiation the activity of the time. During irradiation the activity of the radioactive isotope produced grows radioactive isotope produced grows according to a saturation characteristic according to a saturation characteristic governed by a saturation factor S=1-e governed by a saturation factor S=1-e- -λ λt t i i. . Subsequent to the irradiation the isotope Subsequent to the irradiation the isotope decays according to the exponential law: decays according to the exponential law: D=e D=e- -λ λ t t d d: :  Where t Where ti i : time of irradiation; t : time of irradiation; td d : time of : time of decay; decay; λ λ : decay constant : decay constant
  • 31. Kinetics of activation Kinetics of activation  A= A= I e th th ⋅ + ⋅ ϕ σ ϕ D S A N f m rel Av i ⋅ ⋅ ⋅ ⋅ NAv = Avogadro number fi = isotopic abundance m = the mass of the irradiated element Arel = atomic mass of target element
  • 32. Kinetics of activation Kinetics of activation  The intensity of the measured gamma line is The intensity of the measured gamma line is proportional to the activity. The measured proportional to the activity. The measured parameter is the total energy peak area (N parameter is the total energy peak area (NP P) ) at a particular energy given by the at a particular energy given by the following equation (x) following equation (x) N A f t P m = ⋅ ⋅ ⋅ γ γ ε
  • 33. Kinetics of activation Kinetics of activation  The efficiency ( The efficiency (ε εγ γ) of a semiconductor ) of a semiconductor detector varies with gamma energy. The detector varies with gamma energy. The emission probability of a gamma photon at emission probability of a gamma photon at a given energy is the f a given energy is the fγ γ, t , tm m is the measuring is the measuring time. time.
  • 34. Measurement and evaluation Measurement and evaluation  The modern gamma measuring systems consist of The modern gamma measuring systems consist of a gamma detector, usually a HPGe type and a gamma detector, usually a HPGe type and sometimes NaI(Tl) scintillation crystals. The sometimes NaI(Tl) scintillation crystals. The detectors are connected to a multichannel analyzer detectors are connected to a multichannel analyzer (MCA) by an appropriate electronic system (MCA) by an appropriate electronic system (preamlifier, spectroscopy amplifier, etc.). (preamlifier, spectroscopy amplifier, etc.). Nowadays, the MCAs are computer based systems Nowadays, the MCAs are computer based systems with the ability of an automatic spectrum with the ability of an automatic spectrum evaluation. evaluation.
  • 35. Analysis of the gamma spectra Analysis of the gamma spectra  The usual objective of the measurements The usual objective of the measurements by gamma ray spectrometers is the by gamma ray spectrometers is the determination of the number and energy determination of the number and energy of the photons emitted by the source. of the photons emitted by the source. The peak location and the peak area in The peak location and the peak area in the spectra have to be determined. The the spectra have to be determined. The peak location is a measure of the gamma peak location is a measure of the gamma energy, while the peak area is energy, while the peak area is proportional to the photon emission rate proportional to the photon emission rate
  • 36. Analysis of the gamma spectra Analysis of the gamma spectra  For the energy measurement the pulse For the energy measurement the pulse height scale must be calibrated with height scale must be calibrated with standard sources emitting photons of standard sources emitting photons of known energies known energies  In order to calculate the activities, the full- In order to calculate the activities, the full- energy-peak efficiencies of the source- energy-peak efficiencies of the source- detector system have to be determined by detector system have to be determined by using sources of known activities. using sources of known activities.
  • 37. Analysis of the gamma spectra Analysis of the gamma spectra  For the determination of the peak areas the For the determination of the peak areas the background under the peak interval has to be background under the peak interval has to be subtracted. The net count (Np) results from N subtracted. The net count (Np) results from NP P = = N Nint int - N - NB B, (N , (Nint int integral under the peak and N integral under the peak and NB B refers refers to the background). to the background).  The peak area can also be calculated by computer The peak area can also be calculated by computer programs which fit an analytical function to the programs which fit an analytical function to the peak. The shape is described basically by a peak. The shape is described basically by a Gaussian function, modified by suitable auxiliary Gaussian function, modified by suitable auxiliary functions. Thus all the peaks including also the functions. Thus all the peaks including also the multiplets can be automatically analysed. multiplets can be automatically analysed.
  • 38. Quantitative Analysis Quantitative Analysis  Absolute method Absolute method  The quantitative measurement can be The quantitative measurement can be effected by determining the neutron flux effected by determining the neutron flux and counting the absolute gamma rays. and counting the absolute gamma rays. The direct calculation of concentration is The direct calculation of concentration is made by applying nuclear constants made by applying nuclear constants according to Eq according to Eq (x) (x)
  • 39. Quantitative Analysis Quantitative Analysis  Classic relative method Classic relative method  The method is based on the simultaneous The method is based on the simultaneous irradiation of the sample with standards of known irradiation of the sample with standards of known quantities of the elements in question in identical quantities of the elements in question in identical positions, followed by measuring the induced positions, followed by measuring the induced intensities of both the standard and the sample in a intensities of both the standard and the sample in a well known geometrical position. well known geometrical position.  A relative standardisation can be performed by A relative standardisation can be performed by means of individual monoelement standards, or means of individual monoelement standards, or by using synthetic or natural multielement by using synthetic or natural multielement standards. standards.
  • 40. Classic relative method Classic relative method  The equation used to calculate the mass of The equation used to calculate the mass of an element in the unknown sample relative an element in the unknown sample relative to the comparator standard to the comparator standard
  • 41. Classic relative method Classic relative method  Where A = activity of the sample (sam) and Where A = activity of the sample (sam) and standard (std), standard (std), M = mass of the element, M = mass of the element, = decay constant for the = decay constant for the isotope and = isotope and = decay time decay time
  • 42. Classic relative method Classic relative method  When performing short irradiations, the When performing short irradiations, the irradiation, decay and counting times are irradiation, decay and counting times are normally fixed the same for all samples and normally fixed the same for all samples and standards such that the time dependent standards such that the time dependent factors cancel. Thus the equation factors cancel. Thus the equation simplifies into simplifies into
  • 43. Classic relative method Classic relative method  Where C = concentration of the element Where C = concentration of the element W= weight of the sample and standard W= weight of the sample and standard
  • 44. Counting statistics Counting statistics  The nuclear decay processes occur at random, and The nuclear decay processes occur at random, and follow a Poisson distribution, where the standard follow a Poisson distribution, where the standard deviation ( deviation (σ) σ) equals to N equals to N1/2 1/2 (N is the observed (N is the observed number of events). In gamma spectrometry, the number of events). In gamma spectrometry, the peak area is the measured parameter. The standard peak area is the measured parameter. The standard deviation is: deviation is: σ σ = (N+2N = (N+2NB B) )1/2 1/2 where the where the confidence level is 68%. confidence level is 68%.  The counting statistic is only one of the possible The counting statistic is only one of the possible sources of errors in NAA, the overall value sources of errors in NAA, the overall value depending on a number of different factors (e.g. depending on a number of different factors (e.g. sample preparation, weighing, and uncertainty of sample preparation, weighing, and uncertainty of standardisation). standardisation).
  • 45. Equipment and materials Equipment and materials  - sample for analysis hair sample, soil or - sample for analysis hair sample, soil or steel etc. steel etc.  - analytical balance - analytical balance  - micropipette - micropipette  - reactor for irradiation - reactor for irradiation  - HPGe detector, spectrometer - HPGe detector, spectrometer
  • 46. Procedure Procedure  1 .Choose the proper -nuclear reaction 1 .Choose the proper -nuclear reaction -analytical gamma -analytical gamma line line -irradiation, decay -irradiation, decay and measuring time and measuring time
  • 47. Procedure Procedure  2. 2. Sample preparation: Sample preparation:  - weigh the samples into polyethylene - weigh the samples into polyethylene bags using analytical balance bags using analytical balance  - prepare standards using micropipettes - prepare standards using micropipettes
  • 48. Procedure Procedure  3. 3. Irradiation of the samples using pneumatic Irradiation of the samples using pneumatic system of the reactor system of the reactor  4. 4. Measure the gamma-spectra, evaluate the Measure the gamma-spectra, evaluate the spectra (determine the peak areas at the given spectra (determine the peak areas at the given gamma-lines) gamma-lines)  5. 5. Identify the isotopes in the spectra using Identify the isotopes in the spectra using gamma library. Determine the elemental gamma library. Determine the elemental concentrations and their uncertainties using concentrations and their uncertainties using standard method standard method
  • 49. Sensitivities Available by NAA Sensitivities Available by NAA  The sensitivities for NAA are dependent upon the The sensitivities for NAA are dependent upon the irradiation parameters (i.e., neutron flux, irradiation parameters (i.e., neutron flux, irradiation and decay times), measurement irradiation and decay times), measurement conditions (i.e., measurement time, detector conditions (i.e., measurement time, detector efficiency), nuclear parameters of the elements efficiency), nuclear parameters of the elements being measured (i.e., isotope abundance, neutron being measured (i.e., isotope abundance, neutron cross-section, half-life, and gamma-ray cross-section, half-life, and gamma-ray abundance). The accuracy of an individual NAA abundance). The accuracy of an individual NAA determination usually ranges between 1 to 10 determination usually ranges between 1 to 10 percent of the reported value. percent of the reported value.
  • 50. Detection Limits Detection Limits  The detection limit represents the ability of a The detection limit represents the ability of a given NAA procedure to determine the given NAA procedure to determine the minimum amounts of an element reliably. minimum amounts of an element reliably.  The detection limit depends on the: The detection limit depends on the: (1)The amount of material to be irradiated and to be counted. (1)The amount of material to be irradiated and to be counted.. . (2) (2) The neutron fluxes. The neutron fluxes. (3) (3) The duration of the irradiation time. The duration of the irradiation time. (4) (4) The total induced radioactivity that can be The total induced radioactivity that can be (5)The duration of the counting time (5)The duration of the counting time (6) (6) The detector size, counting geometry and background The detector size, counting geometry and background shielding. shielding.
  • 51. Advantages of NAA Advantages of NAA  Very low detection limits for 30–40 elements, Very low detection limits for 30–40 elements,  Significant matrix independence, Significant matrix independence,  The possibility of non-destructive analysis The possibility of non-destructive analysis (instrumental NAA or INAA), (instrumental NAA or INAA),  The use of radiochemical separation to overcome The use of radiochemical separation to overcome interference in complex gamma-ray spectra interference in complex gamma-ray spectra (radiochemical NAA or RNAA), (radiochemical NAA or RNAA),  An inherent capability for high levels of accuracy An inherent capability for high levels of accuracy compared to other trace element analysis compared to other trace element analysis techniques. techniques.
  • 52. NAA Applications NAA Applications  Archaeology Archaeology  Biomedicine Biomedicine  Environmental science and related fields Environmental science and related fields  Geology and geochemistry Geology and geochemistry  Industrial products Industrial products  Nutrition Nutrition  Quality assurance of analysis and reference Quality assurance of analysis and reference materials materials
  • 53. Applications for NAA Applications for NAA  1. 1. Archaeology Archaeology  The use of neutron activation analysis to The use of neutron activation analysis to characterize archaeological specimens (e.g., characterize archaeological specimens (e.g., pottery, obsidian, chert, basalt and pottery, obsidian, chert, basalt and limestone) and to relate the artifacts to limestone) and to relate the artifacts to sources through their chemical signatures is sources through their chemical signatures is a well-established application of the a well-established application of the method. method.
  • 54. Neutron activation of paintings Neutron activation of paintings
  • 55.
  • 56.
  • 57.
  • 58.
  • 59.
  • 60.
  • 61.
  • 62.
  • 63. Applications for NAA Applications for NAA  Geological science Geological science  Analysis of rock specimens by neutron activation Analysis of rock specimens by neutron activation analysis assists geochemists in research on the analysis assists geochemists in research on the processes involved in the formation of different processes involved in the formation of different rocks through the analysis of the rare earth rocks through the analysis of the rare earth elements (REEs) and other trace elements. About elements (REEs) and other trace elements. About thirty elements can be measured routinely in thirty elements can be measured routinely in almost any geological sample. An additional 15- almost any geological sample. An additional 15- 20 elements can be measured by applying 20 elements can be measured by applying specialized procedures specialized procedures
  • 64. Applications for NAA Applications for NAA  Semiconductor materials and other high-purity Semiconductor materials and other high-purity materials materials  Neutron Activation Analysis (NAA) Neutron Activation Analysis (NAA) is used to is used to measure trace- and ultra trace-element measure trace- and ultra trace-element concentrations of impurities and/or dopants in concentrations of impurities and/or dopants in semiconductors and other high-purity materials. semiconductors and other high-purity materials. The behavior of semiconductor devices is strongly The behavior of semiconductor devices is strongly influenced by the presence of impurity elements influenced by the presence of impurity elements either added intentionally (doping with B, P, As, either added intentionally (doping with B, P, As, Au, etc.) or contaminants remaining due to Au, etc.) or contaminants remaining due to incomplete purification of the semiconductor incomplete purification of the semiconductor material during device manufacture. material during device manufacture.
  • 65. Applications for NAA Applications for NAA  Soil Science Soil Science  Many agricultural processes and their Many agricultural processes and their consequences, such as fertilization and herbicidal consequences, such as fertilization and herbicidal and pesticidal control, are influenced by surface and pesticidal control, are influenced by surface and sub-surface movement, percolation and and sub-surface movement, percolation and infiltration of water. Stable activatable tracers, infiltration of water. Stable activatable tracers, such as bromide, analyzed by NAA, have allowed such as bromide, analyzed by NAA, have allowed the soil scientist to quantify the distribution of the soil scientist to quantify the distribution of agricultural chemicals under a wide variety of agricultural chemicals under a wide variety of environmental and land use influences environmental and land use influences
  • 66. Obtain plant sample. Wash the sample to Obtain plant sample. Wash the sample to remove possible contaminants remove possible contaminants
  • 67. Dehydrate the sample. Dehydrate the sample.  Dehydration methods Dehydration methods use heat or freeze- use heat or freeze- drying. drying.  A lyophilizer is frequently A lyophilizer is frequently used for the freeze-dry used for the freeze-dry method. method.  A plant sample is then A plant sample is then placed in the chamber placed in the chamber atop the lyophilizer to the atop the lyophilizer to the right. right.
  • 68. The dehydrated sample is then prepared for The dehydrated sample is then prepared for testing. A small amount of dehydrated plant testing. A small amount of dehydrated plant material is removed from this bag. material is removed from this bag.
  • 69. A portion of the dried plant material is ground into a powder A portion of the dried plant material is ground into a powder using a mortar and pestle. Sterile technique is required using a mortar and pestle. Sterile technique is required to avoid cross contamination to avoid cross contamination. .
  • 70. Bag the sample. Some of the ground plant powder Bag the sample. Some of the ground plant powder is bagged into a small plastic envelope. The sample is bagged into a small plastic envelope. The sample is double-bagged and labeled is double-bagged and labeled. .
  • 71. Select a standard for comparison. Select a standard for comparison.  When looking for arsenic in When looking for arsenic in plant material, you would need plant material, you would need to prepare a sample of a to prepare a sample of a standard containing arsenic. standard containing arsenic.  The “standard” contains a The “standard” contains a known quantity of the element known quantity of the element you are looking for. you are looking for.  Containers of certified Containers of certified standards are pictured. standards are pictured.
  • 72. Place packages of both the prepared sample and Place packages of both the prepared sample and standard sample in a capsule. standard sample in a capsule.
  • 73. Take sample to the rabbit system apparatus. Take sample to the rabbit system apparatus.  The rabbit system works much The rabbit system works much like the system used by banks at like the system used by banks at drive-through windows. A drive-through windows. A canister carries items back and canister carries items back and forth between the customer and forth between the customer and teller. teller.  The sample is sent through the The sample is sent through the wall in a mini canister into the wall in a mini canister into the nuclear reactor located behind the nuclear reactor located behind the wall. wall.  Once inside the reactor, the Once inside the reactor, the sample is irradiated with sample is irradiated with neutrons. neutrons.
  • 74. After irradiation of the sample in the capsule, and before removing After irradiation of the sample in the capsule, and before removing it from the reactor site, it must be determined if the capsule is safe it from the reactor site, it must be determined if the capsule is safe for transfer. A Geiger counter is used to assess whether the for transfer. A Geiger counter is used to assess whether the radioactive decay has reached low enough levels to be safe. radioactive decay has reached low enough levels to be safe.
  • 75. The prepared sample and standard sample are placed The prepared sample and standard sample are placed in a “detector” one at a time. in a “detector” one at a time.  The detector system The detector system counts and records counts and records gamma radiation gamma radiation emissions for a period emissions for a period of time. of time.  Time varies, but is Time varies, but is usually in the range of 5 usually in the range of 5 minutes to an hour. minutes to an hour.
  • 76. Counts recorded by the detector system is sent Counts recorded by the detector system is sent to a computer. to a computer.
  • 77. 12. Specialized software analyzes radiation peaks. 12. Specialized software analyzes radiation peaks. Peak data is correlated to specific elements for Peak data is correlated to specific elements for identification and quantification. identification and quantification.
  • 78. Computer data is compared to a nuclide chart Computer data is compared to a nuclide chart to evaluate the results. to evaluate the results.