In this study, a two-level full factorial design was used to identify the effects of the interactions between compositions in an N-isopropylacrylamide (NIPAM) gel dosimeter involving the following variables: (A) gelatin, (B) NIPAM, (C) the crosslinker N, N′-methylene-bis-acrylamide (Bis), and (D) the antioxidant tetrakis (hydroxymethyl) phosphonium chloride (THPC). The dose range was from 0 Gy to 5 Gy. Optical computed tomography was used to scan the polymer gel dosimeter. Each component was set to two levels for all four variables, including (A) 4% and 6%, (B) 4% and 6%, (C) 2% and 4%, as well as (D) 5 and 15 mM. Response surface methodology and a central composite design were adopted for the quantitative investigation of the respective interaction effects on the dose response curve of the gel. The results showed that the contributions of the interaction effects, i.e., AB (6.22%), AC (8.38%), AD (7.74%), BC (9.44%), ABC (18.24%), BCD (12.66%), and ABCD (13.4%), were greater than those of the four main effects, accounting for over 76.08% of the total variability. These results also indicated that the NIPAM gel recipe with the highest sensitivity was at 40%C (mass fraction of Bis).
Citation: Chang Y-J, Hsieh B-T (2012) Effect of Composition Interactions on the Dose Response of an N-Isopropylacrylamide Gel Dosimeter. PLoS ONE 7(10): e44905. doi:10.1371/journal.pone.0044905
Editor: Salvatore V. Pizzo, Duke University Medical Center, United States of America
Received: April 16, 2012; Accepted: August 9, 2012; Published: October 12, 2012
Copyright: © Chang, Hsieh. This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.
Funding: This research was funded by the National Science Council of Taiwan (NSC 99-2632-B-166-001-MY3). The funders had no role in study design, data collection and analysis, decision to publish, or preparation of the manuscript.
Competing interests: The authors have declared that no competing interests exist.
The rise in the number of radiotherapies used in dosimetry cases with high-dose gradient distribution signifies the increasing challenges in dose verification . A significant development in gel dosimetry was seen when Fong proposed a new type of gel dosimeter . Without the drawback of ferric ion diffusion found in Fricke-type gel dosimeters, the polymer-gel dosimeter is considered the most promising among the newly developed dosimeters because of its superior spatial and temporal stability. Moreover, for high-energy photo irradiation, most polymer-gel dosimeters can be considered soft tissue equivalent , , . Indeed, polymer-gel dosimetry is a promising dosimeter for dose determination in radiation therapy . However, the spatial resolution and accuracy of absorbed dose measurements remain important issues in the identification of the best gel dosimetry system, i.e., the best gel and readout method to be used in medical applications. The main medical applications include high dose rate gradient radiation fields such as intensity modulated radiotherapy and stereotactic radiosurgery.
Several studies – have described the chemical reaction of radiation-induced polymerization in polymer-gel dosimeters. 1H and 13C-NMR spectroscopy and FT-Raman spectroscopy have been used to investigate the properties of polymer-gel dosimeter post-irradiation . Upon irradiation, the polymerization process is initiated by radical products of water. This process involves water radiolysis, initiation reactions, propagation reactions, and termination reactions. The gel components show various degrees of interaction depending on their concentration. Jirasek and Duzenli , as well as Koeva et al.  have investigated the effect of the crosslinker fraction in polymer gel. Hayashi  has studied the role of gelatin in methacrylic-acid-based gel dosimeters. Given that oxygen (O2) tends to react with the free radicals generated by water radiolysis, which in turn terminates the polymerization process, a number of studies have proposed that some antioxidant additions to the gel are needed to inhibit O2 reaction , –. Some researchers have revealed that the dose response curve show different sensitivities using different monomers –. However, a variety of chemical and physical phenomena influence the radiation-induced polymerization process, including crosslinking, oxygen participation, and interaction between compositions. Therefore, a comprehensive understanding of the complicated polymerization process and gel composition interactions using a systematic approach is necessary.
Various readout methods have been suggested, such as magnetic resonance imaging (MRI), optical-CT scanning, X-ray CT, and ultrasound. Most of the previous studies focused on MRI and laser-based optical-CT scanning. For gel dosimetry, optical-CT scanning has the advantage of simplicity and cheaper implementation. However, the accurate and economical 3-D measurement of optical density (OD) is a crucial step in 3-D polymer-gel dosimetry in conjunction with optical-CT scanning. Some effective OD calibration methodologies have been investigated for fast and high-resolution CCD-based optical-CT scanning –. To reduce the uncertainty of optical density measurement, related factors that affect measurement in cone-beam CT have been studied –.
Polymer-gel dosimeters become more opaque when irradiated. The characteristic curve of gel opaqueness to irradiation is the dose response, which is represented by two-gel parameters, i.e., linearity and sensitivity . One important step in 3-D dose distribution reconstructed from an optical laser scanner is sensitivity calibration . To accomplish this calibration, glass vials with different doses are used to obtain the linear equations of the unit length optical density value (OD/cm) corresponding to the doses delivered to each glass vial –. The linear equation can be used to calculate dose distribution during 3-D reconstruction. Based on the linear optical response of a gel with the dose, Wuu and Xu  have adopted the two-point calibration approach to obtain the relative dose distribution inside an irradiated gel. Combined with ion chamber measurements at two certain points along the central axis of treatment planning, the entire 3-D dose distribution can be obtained. Both parameters are obtained from a linear regression model of the dose response. The optical-computed tomography (optical-CT) coefficients are related to the true attenuation coefficients; thus, adopting the two-point calibration method or linear equation of the unit length optical density value may result in large errors in 3-D dose distribution if the linear relationship is inaccurate . To achieve a more accurate dose distribution using optical-CT, four potential uncertainties should be considered . The first and second uncertainties are the electronic and mechanical noises derived from the optical and mechanical signal acquisition processes, respectively. The third uncertainty is the image reconstruction algorithm. The final and most important uncertainty is the non-uniformities of the gel. To improve gel uniformities, chemical reactions and composition interactions in radiation-induced polymerization need to be scrutinized.
The dose response curve depend not only on initial gel compositions but also on different dose ranges , . The dose sensitivity is lower in low doses than in high doses , . To understand further the effects of chemical interactions between gel compositions, tetrahydroxyphenylchlorin (THPC), and gelatin, the current study examined the effects in the low-dose range, which is most commonly used in clinical applications. The quantitative contribution of each composition and its effects on the gel characteristics were investigated. The effects of the complicated chemical interaction of the composition on sensitivity and linearity during polymerization were also discussed.
Materials and Methods
2.1. N-isopropyl acrylamide (NIPAM) polymer gel preparation and irradiation
The NIPAM polymer gel used in this study was manufactured based on the procedures presented by De Deene et al.  and Senden et al. . The gel was manufactured on a bench-top under normal atmospheric conditions using tetrakis (hydroxymethyl) phosphonium chloride (THPC) as a free radical scavenger. The prepared gel solutions were poured into Pyrex screw test vials (Pyrex Model No. 9826; 13 mm in outer diameter, 100 mm long), as shown in Fig. 1. The vials were wrapped in aluminum foil to prevent photo-polymerization by environmental light. The polymer gels were then carefully stored in a refrigerator at a fixed temperature (7°C) until complete solidification. Each gel sample was irradiated at various doses (i.e., 0, 0.2, 0.5, 1, 1.5, 2, 3, and 5 Gy) using a 6 MV linear accelerator (Varian 21× Clinac, Varian Ltd., Palo Alto, CA, USA).
Irradiation was performed less than 6 h after gel fabrication to avoid oxygen diffusion. A 13 mm-diameter hole was punctured to accommodate the placement of Pyrex test vials in the center of the short side of a customized 30×30×4 cm3 acrylic phantom. The non-irradiated gel vial was placed in the hole in the acrylic phantom to provide adequate build-up and scattering conditions. To ensure accurate location, two 3.5 and 16.5 cm-long acrylic sticks were placed adjacent to the upper and lower sides of the test tube, respectively. The acrylic phantom was placed between two 3 cm-long solid water phantoms to ensure that the source surface distance was 5 cm. All samples were maintained at room temperature (22°C) before irradiation.
2.2. Readout process by optical laser scanning
Magnetic resonance imaging (MRI) gel dosimetry allows the imaging only of arbitrarily shaped gel dosimeters in phantoms. In comparison, optical-CT can provide a low-cost solution for many applications , . Gore et al.  has proposed an optical laser scanning system that incorporates a He-Ne laser, photodiode detectors, and a rotating gel platform. Their experimental results indicate better than 5% accuracy with a spatial resolution of approximately 2 mm using the current prototype scanner. Micro optical-CT has been used to study the characteristics of a high-dose gradient dosimeter . To improve scanning speed, a rotating mirror and Fresnel lenses were used –. A significant development in optical-CT scanning was proposed by Krstajic and Doran (2007) –. In their study, a pair of galvanometer-controlled mirrors was used to manipulate the laser beam and the scanning speed. The commercial optical-CT scanner called Vista, which was manufactured and distributed by Modus Medical Devices, Inc. (London, Ontario, Canada), was developed to provide fast scanning speed –.
Based on the experiment conducted by Gore et al. , the current study used an optical laser scanning system with a 632.8 nm He-Ne laser (20 mW). An optical power meter was used to obtain the optical density I of the irradiated gel, as shown in Fig. 2. A background optical intensity I0 was also obtained from non-irradiated gel vials using the same experimental parameters. Each testing vial was mounted on a precision three-axis stage and immersed in a 90×37×95 mm3 tank (Pyrex glass; 1 mm thick) filled with vegetable oil. To minimize refraction and reflection at the interface, the oil had a refractive index similar to that of Pyrex glass. Room temperature was maintained at 22°C using an air conditioner to avoid temperature-induced dose deviation . The attenuation coefficient α of the irradiated gel was determined by the following equation :(1)where x is the gel diameter. The optical dose response curve, measured in terms of the attenuation coefficient and absorbed dose for each polymer gel recipe, was then obtained. The linear correlation coefficient (R2) was evaluated from the dose response curve. The slope of the dose response curve denoted the sensitivity , , , .
(1) 632.8 nm He-Ne laser, (2) beam splitter, (3) mirror, (4) oil tank, (5) gel in vial, (6) optical power meter, (7) optical sensor head, (8) optical power meter, and (9) optical sensor head.
2.3. Central composite design (CCD)
The amounts of gel components and their interactions affect the dose response of the gel , . Chang et al.  have applied a statistical method using a two-level fractional factorial plan to determine the optimal composition of NIPAM gel. In the current study, a two-level factorial design of experiment in conjunction with response surface methodology and a CCD were adopted to differentiate the effects between each composition and their interactions. The basic CCD for k variables typically consists of a 2k factorial design with each factor at two levels, −1 and +1, superimposed on a star design, or 2k axial points and several repetitions at the design center points. The axial points are factors set to mid-values of the high and low level of the factors. Therefore, the 2k design of the experiment augmented with the center point is an excellent method that can be used to indicate curvature .
In this work, a 2k factorial design was used to investigate the dose response characteristics of a NIPAM gel dosimeter as a function of the following four factors: gelatin (A), NIPAM (B), Bis (C), and THPC (D). Each factor ran at two levels: gelatin, 4% and 6%; NIPAM, 4% and 6%; bis, 2% and 4%; and THPC, 5 and 15 mM (Table 1). The experimental design was a 24 factorial design. The variables A, B, C, and D were defined on a coded scale from −1 to +1 (the low and high levels of A–D). To consider the curvature effect in the response function, the test for curvature was performed by adding five center points to the 24 factorial designs. Finally, the regression model was represented by the terms of the coded factors . Two batches of gels of the same composition were produced to replicate the experiments. The CCD design matrix was then generated and analyzed to determine the dose range of optimal compositions using the DESIGN-EXPERT software.
Based on the CCD design with the four independent variables (gelatin, NIPAM, Bis, and THPC) and two levels of each variable, a 24 design augmented with two replicated batches and five center points yielded a total of 37 runs. The test results of the experiments are listed in Table 2. The sensitivity and linearity for the dose range of 0–5 Gy were computed. The gel composition had different effects on the sensitivity and linearity across various dose ranges.
Results and Discussion
3.1 Dose-response curve
Given that the gels gradually became more opaque upon increased irradiation dose, the light intensity decreased and led to increased attenuation coefficients (Eq. 1). The relationship of the attenuation coefficients with the dose is called the dose-response curve. Figure 3 shows the dose-response curve of NIPAM gel with 4% gelatin, 6% NIPAM, 4% bis, and 15 mM THPC. Two batches of experimental data are shown in the same graph. The graph shows that the experimental data can reproduce very well. The least square fit of the dose-response curve can be obtained as y = 0.0218x−0.0004, and the R2 value is 0.997. Previous studies have shown that the sensitivity is the slope of the dose-response curve, i.e., 0.0218 mm−1Gy−1. On the other hand, the linearity is the goodness of fit of this experimental data for this gel composition, i.e. 0.997 , , , . The linearity indicates the linear relationship to ensure accurate measurement. The sensitivity and linearity of all gel compositions were calculated and are listed in Table 2.
The error bars indicate and experimental uncertainty of 5%.
3.2 Statistical analysis of sensitivity and linearity
Linearity and sensitivity data were entered into the CCD design matrix, as shown in Table 2. Data were formulated using the Design-Expert software (Stat-Ease, Inc., Minneapolis, MN, USA) for the determination of significant variables. The characteristics of the dose response (linearity and sensitivity) for the dose range of 0–5 Gy are listed. In this study, a regression analysis was conducted to develop a best-fit model between the dose response (linearity and sensitivity) and the four significant variables for the dose range of 0–5 Gy. The regression analysis results showed that the regression models for linearity were significant for the dose range of 0–5 Gy (p<0.05) (Table 3). Thus, 24 – 1 effect estimates, including 4 main effects, 6 two-factor interactions, 4 three-factor interactions, and 1 four-factor interaction, were obtained for the dose range of 0–5 Gy (Table 4). The results also showed that the contributions of the interaction effects, such as AB (6.22%), AC (8.38%), AD (7.74%), BC (9.44%), ABC (18.24%), BCD (12.66%), and ABCD (13.4%), were greater than those of the four main effects, accounting for over 76.08% of the total variability. This finding indicated that the interaction effect between factors play a more important role in the gel dose response for the dose range of 0–5 Gy.
The regression model equations describing the relationship between sensitivity and linearity, as well as the four factors for the dose range of 0–5 Gy were as follows:(2)(3)For the dose range of 0–5 Gy, was 0.9697 and was 0.9470 for sensitivity, whereas was 0.9259 and was 0.8704 for linearity (Eqs. 2 and 3), indicating that these models very well explained the experimental data.
3.3 Confirmation experiments
From the regression models (Eqs. 2 and 3) proposed in the previous section, several recipes with linearities greater than 0.995 were suitable to meet the clinical usage requirements. However, two better recipes and one worse recipe were specifically selected for the confirmation experiments to verify the validity of the regression models and exclusion of relatively important factors. The experimental and predicted values for these recipes were compared, and Table 5 shows the results for the dose range of 0–5 Gy. The errors between the experimental and predicted values were found to be all less than 1%. Therefore, the predictions of the regression model were valid and adequate.
3.4 Effect of the interaction of gel compositions on the gel dose response
For a normoxic polymer gel, antioxidant additions to the gel are needed to inhibit O2 reaction , , . However, Jirasek et al.  have found that the amount of antioxidants must exceed a certain level of concentration to reach the O2 inhibition region. Equations. (2) and (3) indicate that the effect of THPC is positive for both sensitivity and linearity because of the positive algebraic sign for factor D. Hence, increasing the amount of THPC improves the sensitivity and linearity for the dose range of 0–5 Gy, similar to the conclusion of De Deene et al. (2002) –. A similar trend can be obtained for Bis because of the positive algebraic sign for factor C. Bis acts as a crosslinker to increase polymerization rates. Jirasek and Duzenli  have proposed that 30%C (mass fraction of Bis) PAGs are the most sensitive dosimeters for the low-dose range of 0–5 Gy. In the current study, gel samples 29–32 had a higher sensitivity of 40%C. Gel recipes with greater and less than 40%C showed decreased sensitivity at the same THPC concentration. A negative trend for both sensitivity and linearity was observed with increased gelatin (factor A). A similar conclusion about the effect of gelatin on sensitivity can be found in De Deene's studies –. This result can be explained by the interaction of gelatin with THPC, as shown in Figure 4. Increased gelatin level decreased the gel sensitivity because high-content gelatin resulted in a low polymerization rate. The gelatin also reacted with free radicals, thereby reducing the polymer reaction and decreasing the gel sensitivity, as explained by De Deene et al. , .
Figure 5 illustrates the response surfaces and contour plots of gelatin and THPC with sensitivity for the dose range of 0–5 Gy. Regarding the interaction effects, both sensitivities decreased with increased gelatin content at THPC concentrations of 5 and 15 mM (low and high levels, respectively). However, the sensitivity decreased to 29.1% (sensitivity from 0.0134 to 0.0095 with gelatin content from 4% to 6%) when THPC = 15 mM, which was lower than 64.2% (sensitivity from 0.0081 to 0.0029 with gelatin content from 4% to 6%) when THPC = 5 mM. Thus, THPC reacted with the gelatin and reduced the amount of free radicals consumed by the gelatin , .
3.5 Effects of linearity and sensitivity
Clinic applications require the use of gel dosimeters with appropriate sensitivity and linearity. For some readout methods (e.g., X-ray CT), a gel recipe with higher sensitivity may be chosen. For some other higher dose range applications , a gel recipe with lower sensitivity may be chosen so that samples do not become too opaque. Eq. (2) is an equation for predicting the gel sensitivity within the dose range of 0–5 Gy. While determining the sensitivity of a gel, Xu et al.  have proposed a method to obtain optimal image contrast in the optical-CT scanning of gel dosimeters. The optical density increment is limited by the effective dynamic range of the optical detector. When the optical density increment exceeds the limitation, an artifact arises in the reconstructed image and causes a larger uncertainty in the dose estimate. The distortions of the image caused by the artifact indicate that the signals in these regions are larger than their actual values; thus, the dose in this area is over estimated. To achieve more accurate dose distribution, the gel recipe can be adjusted in advance to obtain optimal scanning results.
In this study, an experimental design was adopted to investigate the characteristics of the dose-response curve in terms of sensitivity and linearity for the dose range of 0–5 Gy. The sensitivity and linearity were strongly affected by the interactions of gel composition. This study provided quantitative analyses of the interaction effects of gel compositions based on statistical analyses, and revealed that the effects on the dose-response curve were different. Based on the results, the suitable sensitivity and linearity of the gel should be adjusted in advance for different clinical applications to achieve more accurate dose distribution in 3-D image reconstruction. The error between the predicted and experimental values was also found to be less than 1% for the dose range of 0–5 Gy. The NIPAM gel recipe with the highest sensitivity was 40%C.
Authors would like to thank the assistance of photon-beam irradiation from Department of Radiation Oncology, China Medical University Hospital, Taichung, Taiwan, ROC.
Conceived and designed the experiments: YJC. Performed the experiments: YJC. Analyzed the data: YJC. Contributed reagents/materials/analysis tools: BTH. Wrote the paper: YJC.
- 1. Baldock C, De Deene Y, Doran S, Ibbott G, Jirasek A, et al. (2010) Polymer gel dosimetry. Phys Med Biol 55: R1–R63.
- 2. Fong PM, Keil DC, Does MD, Gore JC (2001) Polymer gels for magnetic resonance imaging of radiation dose distributions at normal room atmosphere. Phys Med Biol 46: 3105–3113.
- 3. De Deene Y, Vergote K, Claeys C, Wagter CD (2006) The fundamental radiation properties of normoxic polymer gel dosimeters: a comparison between a methacrylic acid based gel and acrylamide based gels. Phys Med Biol 51: 653–673.
- 4. Pak F, Farajollahi A, Miabi Z (2012) The Basic Dosimetric Properties of NIPAM Polymer Gel Dosimeter. 3. 54th Ann Meeting of the AAPM. SU-E-T-150.
- 5. Chen DC, Chung MB, Shih TC, Lian JA, Chen YS, et al. (2012) MAGAT Gel dosimetry validation in RapidArcTM treatment using Cone-beam CT. J Med Biol Eng In Press. Accessed: 2012 March 12.
- 6. Lepage M, Whittaker AK, Rintoul L, Baldock C (2001) 13C-NMR, 1H-NMR, and FT-Raman study of radiationinduced modifications in radiation dosimetry polymer gels. J Appl Polym Sci 79: 1572–81.
- 7. Jirasek A, Duzenli C (2001) Effect of crosslinker fraction in polymer gel dosimeters using FT Raman spectroscopy. Phys Med Biol 46: 1949–1961.
- 8. Koeva VI, Csaszar ES, Senden RJ, Imam AHM, McAuley KB, et al. (2008) Polymer gel dosimeters with increased solubility: a preliminary investigation of the NMR and optical dose–response using different crosslinkers and co-solvents. Macromol Symp 261: 157–66.
- 9. Hayashi SI, Yoshioka MS, Kiyofumi H, Takahiro K, McAuley KB, et al. (2010) A study on the role of gelatin in methacrylic-acid-based gel dosimeters. Radiat Phys Chem 79 ((7)) 803–808.
- 10. Brindha S, Venning A, Hill B, Baldock C (2004) Experimental study of attenuation properties of normoxic polymer gel dosimeters,. Phys Med Biol 49: N353–N361.
- 11. Jirasek A, Hilts M, Shaw C, Baxter P (2006) Investigation of tetrakis hydroxymethyl phosphonium chloride as an antioxidant for use in x-ray computed tomography polyacrylamide gel dosimetry. Phys Med Biol 51: 1891–1906.
- 12. De Deene Y, Hurley C, Venning A, Vergote K, Mather M, et al. (2002a) A basic study of some normoxic polymer gel dosimeters. Phys Med Biol 47: 3441–3463.
- 13. De Deene Y, Venning A, Hurley C, Healy BJ, Baldock C (2002b) Dose-response stability and integrity of the dose distribution of various polymer gel dosimeters. Phys Med Biol 47: 2459–2470.
- 14. Senden RJ, Jean PD, McAuley KB, Schreiner LJ (2006) Polymer gel dosimeters with reduced toxicity: a preliminary investigation of the NMR and optical dose response using different monomers. Phys Med Biol 51 ((14)) 3301–3314.
- 15. Krstajic N, Doran S (2006) Focusing optics of a parallel beam CCD optical tomography apparatus for 3D radiation gel dosimetry. Phys Med Biol 51: 2055–75.
- 16. Krstajic N, Doran S (2007) Fast laser scanning optical-CT apparatus for 3D radiation dosimetry. Phys Med Biol 52: N257–63.
- 17. Krstajic N, Doran S (2007) Characterization of a parallel-beam CCD optical-CT apparatus for 3D radiation dosimetry. Phys Med Biol 52: 3693–3713.
- 18. Olding T, Holmes O, Schreiner LJ (2010) Cone beam optical computed tomography for gel dosimetry I: scanner characterization. Phys Med Biol 55: 2819–2840.
- 19. Olding T, Schreiner LJ (2011) Cone-beam optical computed tomography for gel dosimetry II: imaging protocols. Phys Med Biol 55: 2819–2840.
- 20. De Deene Y, Hanselaer P, De Wagter C, Achten E, De Neve W (2000) An investigation of the chemical stability of a monomer/polymer gel dosimeter. Phys Med Biol 45: 859–878.
- 21. Wuu CS, Xu Y (2010) How to perform dosimetry with Optical CT. J Phys Conf Ser 250: 1–10.
- 22. Xu Y, Wuu CS, Maryanski MJ (2003) Determining optimal gel sensitivity in optical CT scanning of polymer gels. Med Phys 30: 2257–2263.
- 23. Xu Y, Wuu CS, Maryanski MJ (2004) Performance of optical CT scanning of polymer gels as a tool for 3D dose verification. Med Phys 31: 3024–3033.
- 24. Xu Y, Wuu CS, Maryanski MJ (2010) Sensitivity calibration procedures in optical-CT scanning of BANG 3 polymer gel dosimeters. Med Phys 37: 861–868.
- 25. Wuu CS, Xu Y (2006) Three-dimensional dose verification for intensity modulated radiation therapy using optical CT based polymer gel dosimetry. Med Phys 33: 1412–1419.
- 26. Guo P, Adamovics J, Oldham M (2006) A practical three-dimensional dosimetry system for radiation therapy. Med Phys 33: 3962–3972.
- 27. Chang YJ, Hsieh BT, Liang JA (2011) A systematic approach to determine optimal composition of gel used in radiation therapy. Nucl Instrum Methods Phys Res Sect A 652 ((1)) 783–785 Available: http://dx.doi.org/10.1016/j.nima.2010.09.097.
- 28. Gore JC, Ranade M, Maryanski MJ, Schulz RJ (1996) Radiation dose distributions in three dimensions from tomographic optical density scanning of polymer gels: I. Development of an optical scanner. Phys Med Biol 41: 2695–2704.
- 29. Oldham M, Siewerdsen JH, Shetty A, Jaffray DA (2001) High resolution gel-dosimetry by optical-CT and MR scanning. Med Phys 28: 1436–45.
- 30. Massillon-JL G, Minniti R, Soares CG, Maryanski MJ, Robertson S (2010) Characteristics of a new polymer gel for high-dose gradient dosimetry using a micro optical CT scanner. Appl Radiat Isot 68 ((1)) 144–154.
- 31. Wuu CS, Schiff P, Maryanski MJ, Liu T, Borzillary S, et al. (2003) Dosimetry study of Re-188 liquid balloon for intravascular brachytherapy using polymer gel dosimeters and laser-beam optical-CT scanner. Med Phys 30: 132–7.
- 32. Van Doorn T, Bhat M, Rutten TP, Tran T, Costanzo A (2005) A fast, high spatial resolution optical tomographic scanner for measurement of absorption in gel dosimetry Australas. Phys Eng Sci Med 28: 76–85.
- 33. Conklin J, Deshpande R, Battista J, Jordan K (2008) Fast laser optical CT scanner with rotating mirror and Fresnel lenses. J Phys: Conf Ser 56: 211–3.
- 34. De Deene Y, Pittomvils G, Visalatchi S (2007) The influence of cooling rate on the accuracy of normoxic polymer gel dosimeters. Phys Med Biol 52: 2719–2728.
- 35. Gore JC, Ranadex M, Maryanski MJ, Schulz RJ (1996) Radiation dose distributions in three dimensions from tomographic optical density scanning of polymer gels:I. Development of an optical scanner. P Phys Med Biol 41: 2695–2704.
- 36. Montgomery DC (2005) Design and Analysis of Experiments, sixth ed., John Wiley & Sons, New York, 203–281, 405–463.