Gamma_Ray_Spectroscopy_Using_a_NaI_TI_De.pdf

P a g e 1 | 11
Gamma-Ray Spectroscopy Using a NaI (TI) Detector and Multi-Channel Analyzer
Lab Report Prepared by Nnaemeka Ani
NUC E 450, Radiation Detection and Measurement
Section 003
Team Members:
Francois Ross
Luke Merski
Kirk Brown
Date performed: 03/15/2016
Report due: 03/29/2016
Report turned in: 03/29/2016

Nnaemeka Ani March 28th, 2016 Gamma Ray Spectroscopy using NAI
(TI) detector and MCA
P a g e 2 | 11
Abstract
The lab uses a Multi-channel analyzer and computer software Genie 2000 to identify an
unknown element. We are to calibrate the software using cobalt-60, cesium-137 and barium-133.
Gamma-ray spectroscopy using this setup was very effective.
Introduction
In Experiment 5, we utilized a Single Channel Analyzer to develop a gamma ray spectrum for
Cs137 and Co60. Taking each count at different voltage windows is a long and tedious task, and
is impractical for recording the spectrum using many points. In this experiment, we utilize a
Multi-Channel Analyzer (MCA) which allows us to take counts for several hundred channels at
once, creating a more reliable, more accurate spectrum plot. The software we used for this
experiment was Genie 2000, a spectroscopy software that allows for measurement of photo
peaks, and calculates data for specific user-specified regions. The MCA in conjunction with
Genie allows us to accurately identify unknown radio nuclides through measuring reference
samples and matching the photo peaks of the unknown nuclide with known sources.
Theory
The Multi-Channel Analyzer is a computer based spectroscopy tool that can be used to identify
photo peaks for a nuclide, and thus be able to identify what an element is. Whereas the Single-
Channel Analyzer can only measure the counts for a single window at a time, the Multi-Channel
Analyzer has the ability to measure several hundred channels at once while retaining a very low
dead time.
Equipment
The system illustrated in Figure 1 was used to conduct this experiment. It consists of a Nal (Tl)
detector connected to both the Amplifier and the High Voltage Power Supply. The Multi-
Channel Analyzer (MCA) and the Oscilloscope were both connected to the Amplifier, and the
MCA connected straight to the computer. Model and serial numbers for each piece of equipment
are labeled in Table 1.
Oscilloscope Personal Computer
Multiport II ADC/MCA
Amplifier
Shelf Box
NaI (Tl)
Detector
with
Preamp
High Voltage Power Supply
O
O
O
I
I
I
Preamp Power

P a g e 3 | 11
Figure 1- Block Diagram of Instrumentation Layout used to perform NaI (TI) Multichannel
Analysis
Table 1- System components and their respective serial and model numbers
Component Serial Number Model Number
Oscilloscope CO 830834 TDS 1002
Multiport II ADC/MCA 11065394 MP2_MCA1
Amplifier 10062079 Canberra 2022
NaI(Tl) Detector 10062743 802-2x2
Preamplifier 11064348 2007P
NIM Bin and Power Supply 2080 Ortec 4002D
Detector High Voltage
Supply
00226056 4001C
Procedure
The procedure used for this experiment followed Experiment 6 in the Spring 2016 NucE 450
Experiment 6 Laboratory Manual. Dr. Brenizer and Dr. Flaska did not make any changes during
the course of the experiment
Data:
Cesium-137 Data
Peak was found to be at channel 898 with 1056 counts
Table 2- X-ray and full energy photopeaks
X-Ray Photopeak Full Energy(662KeV) Photopeak
Peak Centroid (channel) 52 894
FWHM (channel) 14.557 62.507
FWTM (channel) 28.758 116.728
Area (counts) 12881 66266
Uncertainty: ±1.04 % ±0.56 %

P a g e 4 | 11
High Voltage= 00V Gain = 1.273 ±100
Deadtime = 7.69%
Table 3- Energy Calibration of radioactive sources given.
Peak
Centroid(ch)
FWHM(ch) FWTM(ch) Area
Cesium-137, Barium-
133 Combined
19 4.635 10.736 65599±0.42%
Barium-133 Gamma
rays 1
48 5.319 9.583 17366±1.23%
Barium-133 Gamma
rays 2
192 15.416 26.296 13355±2.02%
Cesium-137 Gamma
rays
345 24.231 46.438 30178±1.07%
Cobalt-60 Gamma rays
1
601 28.481 51.504 30456±0.87%
Cobalt-60 Gamma rays
2
682 31.121 55.204 29451±0.75%
Figure 2- Peak Analysis Report for calibration spectrum

P a g e 5 | 11
Figure 3- Gamma Spectrum Analysis Report of unknown Radionuclide

P a g e 6 | 11
Figure 4- Graph of cesium-137 taken by NaI detector using both Cesium-137 and Barium-133
Figure 5- Graph of Unknown radioisotope
0
1000
2000
3000
4000
5000
6000
7000
8000
9000
0 200 400 600 800 1000
Measured
Counts(cpm)
Detected Energy(KeV)
Cesium-137 Spectrum with Barium-133
0
500
1000
1500
2000
2500
0 200 400 600 800 1000
Measured
Counts
Calibrated Energy Level (KeV)
Unknown Radioisotope Measured Count

P a g e 7 | 11
Analysis of Data or Results
1. Describe the effects on the cesium-137 spectrum caused by varying the various
MCA controls, gain, and the high voltage settings.
Effects on Varying MCA controls: When the MCA controls are varied, some changes
can be noticed. When there was an increment on the vertical scale past its maximum
value, it “wrapped around” and started again at the smallest value (which is the LOG
scale).
Effects on gain setting: When the gain setting was varied, some changes are noticed.
When the gain is increased, there is a decrease in the number of counts and an
increase in the dead time. Calibration was also altered to some extent.
Effects on high voltage setting: When high voltage setting is varied, some changes are
visible noticed. Photopeaks moved up and down the channels.
2. Using the cesium-137 spectrum data produced in Section D of the Laboratory
Manual and printed out in Section E of the Laboratory Manual, evaluate the
NaI(Tl) detector used in your experiment. Include in this evaluation the detector
resolution, peak symmetry, and peak-to-Compton ratio. How do your results
agree with those obtained in Experiment 5 and with the theoretical values?
Experiment 6 results
�� =
��
��
=
79.285
39.25
= 2.02
�� =
��ℎ� �� − 137 �ℎ��
�� ℎ��ℎ� �� ℎ��
=
1262
180
= 7.01
�� =
��
��
∗ 100 =
925 − 855.75
834
∗ 100 = 8.3%
Experiment 5 results
�� =
��
��
=
3.95 − 3.35
3.85 − 3.55
= 2
�� =
��ℎ� �� − 137 �ℎ��
�� ℎ��ℎ� �� ℎ��
=
1184
179
= 6.61
�� =
��
��
∗ 100 =
3.85 − 3.55
3.75
∗ 100 = 8%

P a g e 8 | 11
Comparing with Experiment 5 results:
In comparison with the results in experiment 5, it can be noticed that the data is
slightly different in all aspects. The true Compton shoulder was hidden by barium -
133. This was due to the fact that the operators had to be changed to function in a
different way. Everything in the data set for this experiment was within the minimum
standards. It was noticed that experiment 5 had better data. For instance the peak to
Compton ratio was 6.61 but for this experiment it is 7.01. Detector resolution for
experiment 5 was 8% but on this experiment it is 8.3%
Comparing with Theoretical values:
In comparison with theoretical values, it can be noticed that the values from this
experiment looked a bit off range. Theoretically, the detector resolution should be
within 7-8% but for this experiment it was 8.3%. Theoretically, peak symmetry
should be equal or less than 2 but in this experiment it was 2.02
3. Using either the cesium-137 peak data obtained in Section D of the Laboratory
Manual or one of the cobalt-60 peaks obtained in Section F of the Laboratory
Manual, use the procedures given in class to calculate peak centroid location,
gross and net peak areas and their standard errors, FWHM, FWTM, and peak
symmetry. How well do your values compare with those obtained by the Genie
2000 program for these values? Explain any differences.
�� =
∑ ��
∑ ��
=
45919300
65599
= 700
�� =
∑ ��
�� ℎ
�=��
�
= 30178.107
�� =
∑ ��
�� ℎ
�=��
�
− �� = 30178.107 − 17366.123 = 12811.984
�� =
��
��
=
110.45
54.79
= 2.02

P a g e 9 | 11
�� =
�
√�
=
1010.2
√600
= ±41.241
�� = 925 − 885.75 = 39.25
�� = 946.78 − 867.50 = 79.29
Comparing with results from Genie 2000:
Using Genie 2000, all the results matched up well from question 2. There are some
changes in the cesium-137 and barium-133 data. These slight changes maybe as a result
of the auto-peak select on the Genie 2000
4. Using the peak channel centroid data determined in Section F of the Laboratory
Manual and actual peak energies, evaluate the accuracy of the energy
calibration curve obtained in Section F. This requires you to fit a curve or line to
your data
Figure 6- Line of best fit for the Cesium-137 graph of peak centroid and energy
5. Identify, by using a table, all the spectral features in cesium-137 from Section D
of the Laboratory Manual and the calibration spectrum in Section F. Include
such items, if seen, as full energy peaks, escape peaks, backscatter peaks,
Compton continuums, annihilation peaks, sum peaks, etc. Do their shapes and
approximate energy or channel locations agree with the theory given in class?

P a g e 10 | 11
Identification of Spectral features
Table 4 – Spectral features and their equivalent energies for the Cesium-137 spectrum
Spectral Feature Energy(KeV)
X-ray Peak 31.2
Full Energy Peak 650.12
Backscatter Peak 195.52
Compton Peak 440.28
Table 5 - Spectral features and their equivalent energies for the calibration spectrum
Spectral Feature Energy(KeV)
Cobalt-60 Photo peak 1 1333.28
Cobalt-60 Photo peak 2 1150.25
Cesium-137 photo peak 660.45
Barium-133 photo peak 250.45
Compton Edge 321.28
Backscatter Peak 228.48
Detector Material X-ray 81.52
Cesium-137, Barium-
133 combined X-ray
26.45

P a g e 11 | 11
6. What was the unknown radionuclide? How were the identifications established?
How well did the calibration energies agree with the actual peak energies?
Explain any discrepancies in these values.
The Unknown radionuclide was found to be Sodium-22. This was identified from its
1,115.6 KeV Gamma ray. There was actually another peak energy found which was
511 KeV but this peak is only there as a result of the annihilation process. This was
the only peak shown in the data. The closeness to the known value was reported for
because of the continual randomness of gamma-ray emission. This therefore caused
some slightly changed values.
Conclusions
The NaI detector used was extremely important. It produced accurate results. Gamma rays
remain the same over long ranges through the use of gamma-ray spectroscopy. One very
important use of this method is the ability to identify any radioisotopes using this method. Even
when the half-life measurements and the radioisotopes are found, we can easily still find the
initial amount of element that that decayed.
Suggestions for Future Work
There were some areas that were not clear to me. I believe that if we are all given a run-down of
the experiment just before we conduct it, it will be much appreciated. Sometimes we do not
know what to expect and what not.
References
Brenizer, J.S., and Jovanovic, I. et al, Radiation Detection and Measurement Laboratory
Manual, 2013.
Knoll, Glenn F., Radiation Detection and Measurement, 4 ed., John Wiley and Sons,
2010.
Shultis, J. Kenneth, and Faw, Richard E., Fundamentals of Nuclear Science and
Engineering, 2 ed., CRC Press, 2008.
Appendices
http://demoweb.physics.ucla.edu/content/experiment-6-radioactivity

Gamma_Ray_Spectroscopy_Using_a_NaI_TI_De.pdf

More Related Content

Similar to Gamma_Ray_Spectroscopy_Using_a_NaI_TI_De.pdf

Recently uploaded

Gamma_Ray_Spectroscopy_Using_a_NaI_TI_De.pdf