|Year : 2006 | Volume
| Issue : 2 | Page : 72-77
Optimization of the imaging protocol of an X-ray CT scanner for evaluation of normoxic polymer gel dosimeters
Brindha Subramanian1, Paul B Ravindran1, Clive Baldock2
1 Department of Radiotherapy, Christian Medical College, Vellore, Tamil Nadu, India
2 Institute of Medical Physics, School of Physics, University of Sydney, Sydney, Australia
Department of Radiotherapy, Christian Medical College, Vellore, Tamil Nadu, India
Source of Support: None, Conflict of Interest: None
| Abstract|| |
X-ray computer tomography (CT) has previously been reported as an evaluation tool for polymer gel (PAG) dosimeters. In this study, the imaging protocol of a Siemens Emotion X-ray CT scanner was optimized to evaluate PAGAT normoxic gel dosimeters. The scan parameters were optimized as 130 kV and 150 mA with a slice thickness of 3 mm for smaller fields and 5 mm for larger fields of irradiation. The number of images to be averaged to reduce noise to an acceptable level was concluded to be 25. It was also concluded that the total monomer concentration required is 7% with 10 mM THP to obtain a maximum change in CT number at dose levels up to 15 Gy for evaluation with X-ray CT. Optimal scan parameters may vary with X-ray CT scanner. Hence the imaging protocol of each scanner to be used for evaluating polymer gels requires individual optimization for the purposes of gel dosimetry evaluation.
Keywords: Normoxic polymer gels, X-ray CT, imaging protocol
|How to cite this article:|
Subramanian B, Ravindran PB, Baldock C. Optimization of the imaging protocol of an X-ray CT scanner for evaluation of normoxic polymer gel dosimeters. J Med Phys 2006;31:72-7
|How to cite this URL:|
Subramanian B, Ravindran PB, Baldock C. Optimization of the imaging protocol of an X-ray CT scanner for evaluation of normoxic polymer gel dosimeters. J Med Phys [serial online] 2006 [cited 2020 Dec 3];31:72-7. Available from: https://www.jmp.org.in/text.asp?2006/31/2/72/26692
In 1984 Gore et al . proposed a method for determining the spatial distribution of radiation dose in tissue equivalent phantom using nuclear magnetic resonance imaging. Since then studies have been undertaken to investigate the feasibility of using gel dosimetry as a 3-D dosimetry system in radiation oncology.,,
In Fricke gel dosimeters, ferrous ions (Fe 2sub+) are converted to ferric ions (Fe 3sub+) due to ionizing radiation. Fricke gels however have a major limitation due to loss of spatial integrity due to the diffusion of ferric ions.
In 1993, a polymer gel dosimeter based upon polymerization of acrylamide (AA) and N'N'- methylene-bis-acrylamide (BIS) monomers infused in an aqueous gel matrix was developed. This polymer gel dosimeter formulation, often described as a polyacrylamide gel or PAG is normally manufactured in an oxygen free or hypoxic atmosphere due to the inhibitory effect of oxygen on the polymerization process.,,,,
Normoxic polymer gel dosimeters are produced, stored and irradiated in a normal or normoxic atmosphere. The first suggested normoxic polymer gel dosimeter, known as MAGIC, an acronym for Methacrylic acid, Ascorbic acid, Gelatin Initiated by Copper was based upon the polymerization of methacrylic acid infused with copper (II) sulphate and the antioxidant ascorbic acid in a gel matrix. Subsequently, a number of other normoxic polymer gel dosimeter formulations were investigated including MAGAS. Tetrakis (hydroxy methyl) phosphonium chloride (THP) was found to be a very effective antioxidant. Polymer gel dosimeter compositions containing the THP antioxidant include MAGAT (methacrylic acid, gelatin and tetrakis) and PAGAT (polyacrylamide, hydroquinone, gelatin and tetrakis).
To date magnetic resonance imaging (MRI) has been most extensively used for the evaluation of absorbed dose distributions in polymer gel dosimeters (2-4 and references therein). Other evaluation techniques such as optical tomography, vibrational spectroscopy, X-ray computerized tomography (CT) and ultrasound have also been investigated.
X-ray CT has been used as an evaluation tool to measure dose distributions of irradiated polymer gel dosimeters. The resulting images have CT numbers or Hounsfield units (H) related to linear attenuation data, which is directly linked to physical density changes of irradiated polymer gel dosimeters. The post-irradiation changes in the linear attenuation coefficient, µ have been evaluated., Technical considerations for evaluating PAG gels with X-ray CT has already been reported. The feasibility of using X-ray CT has further been evaluated for normoxic polymer gel dosimeters by studying radiological attenuation properties as well as the dose response characteristics of normoxic gel dosimeters.,, In the current work, the imaging protocol of a Siemens Emotion single slice spiral CT scanner was optimized for evaluating PAGAT polymer gels in addition to the optimization of monomer concentration for obtaining an optimum change in CT number with radiation dose.
| Materials and Methods|| |
Preparation of PAGAT gel dosimeter
Normoxic PAGAT gel dosimeters were prepared under normal atmospheric conditions as per the recipe previously published., For preparing the PAGAT gel dosimeter for optimization the imaging protocol of the CT scanner, 5% by total weight of gelatin was mixed with 89% distilled water and allowed to soak for 10 minutes before heating to 50°C in a conical flask. Once the temperature reached 50°C, the gel mixture was removed from the heater and 3% BIS was added, stirred thoroughly and allowed to dissolve. After dissolving the BIS, 3% acrylamide was added and allowed to dissolve. When the dosimeter was ready to be poured into the vials, 10 mM of THP was added and mixed thoroughly. The gel was poured into two 200 ml plastic bottles.
In order to optimize the concentration of monomers for evaluation with X-ray CT, the total concentration of monomer was varied. The concentration of BIS and AA were varied from 3 to 4.5% by total weight of gel dosimeter required. Four sets of gels with concentration of BIS as 3, 3.5, 4 and 4.5% by total weight of required gel dosimeter and concentration of AA as 3, 3.5, 4 and 4.5% by total weight respectively of the gel required were prepared. The PAGAT gel dosimeter was then poured into cylindrical plastic vials of height 5.6 cm and diameter 2.4 cm for optimization of monomer concentration and refrigerated.
Irradiation of the PAGAT gel dosimeters
The gels that were in the plastic bottles were left un-irradiated to study the variation of standard deviation of averaged CT images. The PAGAT gel dosimeters in the vials were irradiated to 5, 10 and 15 Gy at dmax with 6 MV photons using a field size of 30 x 30 cm 2sub from a Siemens Mevatron MD linear accelerator at 100 cm SSD using parallel opposed fields to obtain a uniform dose in the vials. The irradiated gels were left in the refrigerator for 24 hours before imaging assuming the polymerization due to irradiation is completed since it has been considered that the post-irradiation polymerization was essentially completed after approximately 12 hours post-irradiation.
The irradiated gels were placed horizontally on the flat couch top of the Siemens Somatom CT scanner for imaging. To determine the number of images to be averaged, the imaging parameters of 80 kV and 130 kV were used with maximum mA and the un-irradiated sample of the PAGAT gel dosimeter in the plastic bottle was imaged 50 times at the same scan position. For the optimization of concentration of monomers, the highest available tube voltage of 130 kV and tube current of 110 mA were used with an imaging time of 0.8 s. For optimizing the imaging protocol of the CT scanner all the scan parameters such as the tube voltage, tube current and slice thickness were varied.
The CT images were transferred to a PC and evaluated with modified software coded in MATLABTM. The software enabled averaging of images obtained at the same scan position, marking circular regions of interest (ROI) of varying diameter within the circumference of the bottles or vials, conversion of data to standard Hounsfield units (H) or CT number in the selected ROI and calculation of standard deviation of H within the ROI. The variation in two factors namely the standard deviation in CT number (sNCT) and changes in CT number (DNCT) were evaluated.
Optimization of number of images to be averaged
The CT images of the PAGAT gel had a low signal to noise ratio (SNR) and this has been found to improve by image averaging (Hilts et al ., 2000). It is time consuming to obtain 50 scans in each slice while validating radiotherapy treatment plans in a clinical set up. Hence a study was carried out to obtain an optimal number of scans at the same scan position to reduce the noise as well as to be less time consuming.
The un-irradiated sample of the PAGAT gel dosimeter in the plastic bottle was imaged 50 times at the same scan position with the following settings: tube voltage - 80kV and 130 kV, tube current 150 mA, exposure time 0.8 s and slice thickness 5 mm. The data was transferred to a PC and evaluated. Different number of images up to 50 images was averaged and upon which a circular ROI was drawn. The ROI was 292.58 mm 2sub in 749 pixels with each pixel size of 0.3906 mm 2sub . The CT numbers were extracted by taking the mean ROI value on each of the averaged image and the standard deviation in CT number (sNCT) for all the averaged images over the selected ROI was calculated.
An investigation on the effect of image averaging on the CT number of the irradiated gel was also carried out. One set of plastic vials irradiated to doses of 5, 10 and 15 Gy was imaged 50 times at the same scan position. The images were transferred to a PC and evaluated.
The SNR for different number of images averaged was calculated for different number of images averaged from
SNR = NCT (irradiatedgel)- NCT (un-irradiatedgel)
where s is the standard deviation in the averaged CT number obtained from the selected ROI within the vial of the un-irradiated PAGAT gel dosimeter.
Optimization of scanner parameters
The first step in optimizing the scan parameters was to optimize the tube voltage and tube current at which the dosimeter was to be imaged. For this, the un-irradiated PAGAT gel dosimeter was imaged with the available tube voltages of 80 kV, 110 kV and 130 kV with minimum and maximum available tube current for each tube voltage. The imaging was carried out with slice thickness of 1, 2, 3, 5 and 10 mm respectively. Circular regions of interest of area 163 mm 2sub over 221 pixels were drawn at the central region of the vials in the averaged image. The software calculates the CT numbers by taking the mean of the CT numbers in each pixel in the ROI selected. The average CT number and the standard deviation in CT number (sNCT) for all the averaged images over the selected ROI were obtained.
Optimization of monomer concentration
For optimization of monomer concentration, the maximum change in CT number (DNCT) with absorbed dose was studied. The PAGAT gel for this study was prepared, irradiated and imaged as discussed in sections 2.1, 2.2 and 2.3. The images were transferred to a PC and analyzed. The average of 50 images for each dose was calculated using the software. Circular regions of interest of area 163 mm 2sub over 221 pixels were drawn at the central region of the vials in the averaged image and the CT numbers were obtained. The change in CT number with radiation dose was calculated by subtracting the CT number of the irradiated gel from that of the un-irradiated gel.
| Results and Discussion|| |
Optimization of the imaging protocol of the X-ray CT scanner
[Figure - 1] shows the variation in standard deviation (sNCT) obtained over a region of interest of the averaged images for both the lowest and highest tube voltage available in the X-ray CT scanner for which the imaging protocol was optimized. The sNCT decreased from 6.19 H to 1.22 H for a tube voltage of 80 kV and from 3.6 H to 0.7 H for 130 kV when the number of images averaged was increased from 1 to 25. This shows that the noise due to photon counting statistics can be reduced by image averaging. After this point, the decrease in sNCT was found to be 0.3 H when the number of images averaged increased from 25 to 50. The resulting total noise of 0.5 H when 50 images were averaged compares with the value of 0.6 H obtained by Trapp et al ., 2001. This is a known effect in CT imaging and is due to factors such as reconstruction noise, electronic noise and CT number quantization. At 80 kV the HU for the normoxic polymer gel dosimeters was lower than that for 130 kV indicating that the HU changes with tube potential. This was to be expected, as linear attenuation of the normoxic polymer gel dosimeter is energy dependent. Moreover, the load on the X-ray tube is directly proportional to the number of images averaged. Since the variation in sNCT was minimal when the number of images averaged increased from 25 to 50, it was decided to average 25 images to reduce the noise in the image and also keep the load on the X-ray tube at a lesser level when compared to averaging a large number of images.
[Figure - 2] represents the variation in CT number with number of images averaged. The CT number was found to decrease as the number of images averaged increased. The maximum variation observed in CT numbers due to image averaging was 1 H for a dose of 15 Gy while the decrease was 0.5 H for lesser doses. This decrease is due to the variation in CT numbers in the pixels within the ROI. But when the variation in change in CT number (DNCT) with number of images averaged was calculated as shown in [Figure - 3], it was found that the DNCT remained unchanged over the number of images averaged for all doses. The decrease in CT number observed in [Figure - 2] was removed when the difference between the irradiated and un-irradiated samples were calculated. From this it was concluded that the image averaging reduces the image noise alone without causing changes in the CT number.
The variation in signal to noise ratio with increase in number of images averaged is shown in [Figure - 4]. The SNR was found to increase asymptotically with averaged images as expected since theoretically the SNR increases by ÖN where N is the number of images averaged. The limitations in increasing the number of images in a single scan position are the load to the X-ray tube with increase in number of scans, polymerization in the gel phantom due to the radiation dose contribution during the scan as the number of images are increased and the time limitation in the availability of the an X-ray CT scanner in a clinical radiotherapy department. Obtaining a pre-irradiation scan and subtracting it from the post-irradiation scan could be used to correct the radiation dose contribution to the gel phantom during evaluation by X-ray CT. However, only decreasing the number of images averaged could decrease the load on the scanner as well as the time consumed on the scanner for imaging. From [Figure - 1] it was observed that the sNCT decreased substantially when the number of images averaged increased from 1 to 25. The decrease was found to be less than 1 H for further increase in the number of images averaged. Hence the optimal number of images to be averaged was concluded as 25 to result in a desired SNR.
It has been shown that CT imaging technique affects the noise levels and these could be decreased by increasing tube voltage (kV), tube current (mA) and slice scan time (s). [Figure - 5] showing the variation of sNCT with tube voltage followed exponential decay pattern with decrease in image noise level with increase in tube voltage. The sNCT decreased by 72% when the tube voltage increased from 80 kV to 130 kV. This reduction is found to be higher than the 60% reduction in doubling the tube voltage reported by Hilts et al ., 2005. It was observed that the sNCT decreased steeply by 1.23 H when the tube voltage increased from 80 kV to 110 kV. But beyond 110 kV, when the tube voltage was further increased to 130 kV, the change in standard deviation was only 0.6 H. sNCT was found to be greater at lower tube voltages when compared to higher tube voltages as the maximum number of photons reaches the detector at the highest tube voltage providing a better SNR than the lower voltages characterized by lower photon emission. Hence the optimum tube voltage at which the PAGAT polymer gel dosimeter is to be imaged was selected at the highest tube voltage of 130 kV available on the scanner being studied in spite of the increase in load to the tube taking into consideration the amount of noise in the images at a lower tube voltage of 80 kV.
[Figure - 6] shows sNCT for different tube voltage and tube current combination with different slice thickness. All the curves followed the exponential decay pattern following the equation Y = Y 0 +Ae x/t where x is the slice thickness in mm and Y is sNCT. However the standard deviation sNCT was found to be minimal for two curves, one with a tube voltage of 110 kV and tube current of 150 mA and the other with a tube voltage of 130 kV and tube current of 150 mA. The sNCT for the lower tube voltage of 110 kV was found to be lesser than that of the higher tube voltage of 130 kV for the lowest slice thickness of 1 mm. But beyond 1 mm, the sNCT was more than that of 130 kV. Similarly, the standard deviation in CT number (sNCT) was found to be the maximum for a slice thickness of 1 mm and decreased with increase in slice thickness. While the variation in sNCT was 0.6 H between 1 mm and 2 mm slice thickness, the change was found to be 0.2 H for further increase in slice thickness. There was a minimal change sNCT as slice thickness increased from 5 mm to 10 mm. However while verifying dose distributions with dose gradients a lesser slice thickness is preferable. Therefore it was decided to use a 3 mm slice thickness for verification of small fields and 5 mm slice thickness for verification of larger fields.
Optimization of monomer concentration
The dose response of the PAGAT polymer gel with 2 mM THP and 10 mM THP with various concentrations of BIS and acrylamide is shown in [Figure - 7]. For 2 mM THP, the change in CT number was found to be 12 H for a dose of 15 Gy for the total monomer concentration of 9% (4.5% BIS and 4.5% Acrylamide) when compared to other concentrations. The 7% total concentration of monomers was 9 H for a dose of 15 Gy while the others had a lower change in CT numbers when compared to 7 and 9% total monomer concentration.
With 10 mM concentration of THP, the change in CT number was 13 H for a dose of 15 Gy for a total monomer concentration of 7% (3.5% BIS, 3.5% Acrylamide). The 9% total monomer concentration had the lowest change in CT number of 9 H for the dose of 15 Gy while the other concentrations had a lesser change in CT number when compared to 7% total monomer concentration.
From these observations a comparison of dose response between the total concentrations of 7 and 9% was investigated. It was found that with 7% total monomer concentration and 10 mM THP, the dose response curve was linear up to 10 Gy, with a maximum difference of 13 H for the dose of 15 Gy. For 9% total monomer and 2 mM THP, the linearity of dose response was observed till 5 Gy with a maximum difference of 12 H for 15 Gy. Hence, it was decided to optimize the total monomer concentration as 7% with 10 mM THP with a higher linear dose range for evaluating the PAGAT with X-ray CT scanner.
| Conclusion|| |
The imaging protocol of the Siemens Emotion X-ray CT scanner was optimized to evaluate PAGAT normoxic gel dosimeters. Since the change in sNCT was minimal beyond 25 images at the same scan position, the number of images to be averaged to reduce sNCT in a region of interest thus reducing the noise was concluded to be 25. The scan parameters were optimized at the highest available tube voltage of 130kV and highest available tube current of 150mA to enable the maximum number of photons to reach the detector thereby reducing the noise in the image. The optimal slice thickness was determined to be 3 mm while evaluating small fields of irradiation and 5 mm for larger fields. The total concentration of monomers was optimized at 7 % with 10 mM THP to obtain a maximum change in CT number (DNCT) with absorbed dose for evaluating with X-ray CT. It has been shown that X-ray CT can be used as an evaluation tool for the PAGAT polymer gel dosimeter. Optimal scan parameters may vary with X-ray CT scanner. Hence each scanner to be used for evaluating polymer gels requires individual optimization for the purposes of gel dosimetry evaluation.
| References|| |
|1.||Gore JC, Kang YS, Schulz RJ. Measurement of radiation dose distributions by nuclear magnetic resonance (NMR) imaging. Phys Med Biol 1984;29:1189-97. [PUBMED] [FULLTEXT]|
|2.||DOSGEL. Proceedings of the 1st international workshop on radiation therapy gel dosimetry. in DosGel'99. Canadian Organization of Medical Physicists: Lexington, KY, USA; 1999. |
|3.||DOSGEL. Prelimanary Proceedings of DOSGEL 2001 2nd International Conference on Radiotherapy Gel Dosimetry. in DOSGEL 2001. Queensland University of Technology, Queensland University of Technology: Brisbane, Australia; 2001. |
|4.||DOSGEL. Proceedings of the 3rd international workshop on radiation therapy gel dosimetry. in DosGel'04. Ghent: Belgium; 2004. |
|5.||Baldock C, Harris PJ, Piercy AR, Healy B. Experimental determination of the diffusion coefficient in two-dimensions in ferrous sulphate gels using the finite element method. Aust Phys Eng Sci Med 2001;24:19-30. [PUBMED] |
|6.||Maryanski MJ, Gore JC, Kennan RP, Schulz RJ. NMR relaxation enhancement in gels polymerized and cross-linked by ionizing radiation: A new approach to 3D dosimetry by MRI. Magn Reson Imaging 1993;11:253-8. [PUBMED] |
|7.||Baldock C, Burford RP, Billingham N, Wagner GS, Patval S, Badawi RD, et al . Experimental procedure for the manufacture and calibration of polyacrylamide gel (PAG) for magnetic resonance imaging (MRI) radiation dosimetry. Phys Med Biol 1998;43:695-702. |
|8.||Maryanski MJ, Audet C, Gore JC. Effects of cross linking and temperature on the dose response of a BANG polymer gel dosimeter. Phys Med Biol 1997;42:303-11. [PUBMED] [FULLTEXT]|
|9.||Lepage M, Whittaker AK, Rintoul L, Back SA, Baldock C. The relationship between radiation-induced chemical processes and transverse relaxation times in polymer gel dosimeters. Phys Med Biol 2001;46:1061-74. [PUBMED] [FULLTEXT]|
|10.||De Deene Y. Dose-response and spatial stability of various polymer gel dosimeters. Phys Med Biol 2002;47:2459-70. |
|11.||De Deene Y, Hurley C, Venning A, Vergote M, Mather M, Healy BJ, et al . A basic study of some normoxic polymer gel dosimeters. Phys Med Biol 2002;47:3441-63. |
|12.||De Deene Y, Hanselaer P, De Wagter C, Achten E, De Neve W. An investigation of the chemical stability of a monomer/polymer gel dosimeter. Phys Med Biol 2000;45:859-78. [PUBMED] [FULLTEXT]|
|13.||Fong PM, Keil DC, Does MD, Gore JC. Polymer gels for magnetic resonance imaging of radiation dose distributions at normal room atmosphere. Phys Med Biol 2001;46:3105-13. [PUBMED] [FULLTEXT]|
|14.||Venning AJ, Hill B, Brindha S, Healy BJ, Baldock C. Investigation of the PAGAT polymer gel dosimeter using magnetic resonance imaging. Phys Med Biol 2005;50:3875-88. [PUBMED] [FULLTEXT]|
|15.||Hurley CA, Venning, Baldock C. A study of a normoxic polymer gel dosimeter comprising methacrylic acid, gelatin and tetrakis (hydroxymethyl) phosphonium chloride (MAGAT). Appl Radiat Isot 2005;63:443-56. |
|16.||Venning AJ, Hill B, Brindha S, Healy BJ, Baldock C. Investigation of the PAGAT polymer gel dosimeter using magnetic resonance imaging. Phys Med Biol 2005;50:3875-88. [PUBMED] [FULLTEXT]|
|17.||Oldham M, Siewerdsen JH, Shetty A, Jaffray DA. High resolution gel-dosimetry by optical-CT and MR scanning. Med Phys 2001;28:1436-45. [PUBMED] |
|18.||Rintoul LM, Lepage, Baldock C. Radiation dose distribution in p olymer gels by Raman spectroscopy. Appl Spectrosc 2003;57:51-7. |
|19.||Hilts M, Audet C, Duzenli C, Jirasek A. Polymer gel dosimetry using X-ray computed tomography: A feasibility study. Phys Med Biol 2000;45:2559-71. [PUBMED] [FULLTEXT]|
|20.||Mather ML, Baldock C. Ultrasound tomography imaging of radiation dose distributions in polymer gel dosimeters: Preliminary study. Med Phys 2003;30:2140-8. [PUBMED] |
|21.||Audet C, Hilts M, Jirasek A, Duzenli C. CT gel dosimetry technique: Comparison of a planned and measured 3D stereotactic dose volume. J Appl Clin Med Phys 2002;3:110-8. [PUBMED] |
|22.||Trapp JV, Michael G, De Deene Y, Baldock C. Attenuation of diagnostic energy photons by polymer gel dosimeters. Phys Med Biol 2002;47:4247-58. [PUBMED] [FULLTEXT]|
|23.||Trapp JV, Back SA, Lepage M, Michael G, Baldock C. An experimental study of the dose response of polymer gel dosimeters imaged with X-ray computed tomography. Phys Med Biol 2001;46:2939-51. [PUBMED] [FULLTEXT]|
|24.||Hilts M, Jirasek A, Duzenli C. Technical considerations for implementation of x-ray CT polymer gel dosimetry. Phys Med Biol 2005;50:1727-45. [PUBMED] [FULLTEXT]|
|25.||Brindha S, Venning AJ, Hill B, Baldock C. Experimental study of attenuation properties of normoxic polymer gel dosimeters. Phys Med Biol 2004;49:N353-61. [PUBMED] [FULLTEXT]|
|26.||Hill B, Venning AJ, Baldock C. A preliminary study of the novel application of normoxic polymer gel dosimeters for the measurement of CTDI on diagnostic X-ray CT scanners. Med Phys 2005;32:1589-97. [PUBMED] |
|27.||Hill BA, Venning, Baldock C. The dose response of normoxic polymer gel dosimeters measured using X-ray CT. Br J Radiol 2005;78:623-30. |
|28.||Murry P, Baldock C. Research software for MRI radiotherapy gel dosimetry. Aust Phys Engg Sci Med 2000;23:44-51. [PUBMED] |
|29.||Curry TS, Dowdey JE, Murry RC. Christensen's Physics of Diagnostic Radiology. Lea and Febiger: Malvern, PA; 1990. |
|30.||Swindell WA. X-ray transmission computed tomography. The Physics of Medical Imaging. Institute of Physics Publishing: Philadelphia, PA; 1993. p. 98-125. |
[Figure - 1], [Figure - 2], [Figure - 3], [Figure - 4], [Figure - 5], [Figure - 6], [Figure - 7]
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