Skip to main content
Journal of Biomedical Physics & Engineering logoLink to Journal of Biomedical Physics & Engineering
. 2019 Aug 1;9(4):395–408. doi: 10.31661/jbpe.v0i0.839

Dosimetric Evaluation of Volumetric Modulated Arc Therapy (VMAT) and Intensity Modulated Radiotherapy (IMRT) Using AAPM TG 119 Protocol

Nainggolan A 1,2, Pawiro S A 1*
PMCID: PMC6709355  PMID: 31531292

Abstract

Background:

The commissioning accuracy of Volumetric Modulated Arc Therapy (VMAT) need to be evaluated.

Objective:

To test and evaluate commissioning accuracy of VMAT based on the TG 119 protocols at local institution.

Material and Methods:

The phantom, structure sets, VMAT and IMRT beam parameter setup, dose prescriptions and planning objectives were following TG 119 guidelines to create local treatment plans of VMAT and IMRT. The local planning results were compared with the results of TG 119. Point measurement at high and low dose regions were measured using three ionization chambers with different active volumes (CC01, CC13, FC65G). The composite dose was measured by a 2D detector array and analyzed for the percentage of points passing the gamma criteria of 3 % dose difference (DD) and 3 mm distance-to-agreement (DTA) and 2 % DD and 2 mm DTA.

Results:

The local treatment plans of VMAT and IMRT capable to meet the dose goals criteria set by TG 119 except for C-shape hard. Three ionization chambers with various active volumes for point measurement showed an increase in the confidence limit (CL), the larger the active volume was found proportional to increase the value of CL. The results obtained from ion chambers CC01 and CC13 could met the dose criteria set by TG 119, but results obtained from ion chamber FC65G fail the criteria. All gamma evaluation results show more than 95% data points pass the criteria of 3% DD and 3 mm DTA and the gamma index CL results fall within the TG 119 criteria, which is below 12.4.

Conclusion:

TG 119 methodology and recommendations have successfully been used to evaluate commissioning accuracy of VMAT. The CL value of the study could be used as a reference and recommendation to evaluate the accuracy and integrity of treatment planning and treatment delivery systems of VMAT and IMRT.

Keywords: Radiotherapy, Intensity-Modulated ; Radiometry ; Phantoms ; Imaging Radiotherapy Planning ; Computer-Assisted

Introduction

Intensity modulated radiation therapy (IMRT) techniques reduce dose to critical structures compared to three dimensional conformal radiotherapy (3D CRT) while maintaining conformal and homogenous dose with target volume. IMRT is different from 2D or 3D CRT, it can deliver fields of non-uniform intensity [1]. However, in Volumetric Modulated Arc Therapy (VMAT) the gantry rotates around the patient while the radiation is being delivered. The dose distribution was shaped into three dynamic variables: MLC, gantry rotation speed, and dose rate. The quality of VMAT treatment delivery was comparable to IMRT with an advantage such as a shorter time and less monitor unit (MU). The initial concept of VMAT was introduced by Cedric Yu in 1995 [2]. He proposed radiation treatment delivery in rotational, while the field shapes and dose weighting are being modulated. The technology started commercials in the market when Otto introduced the concept of delivering the radiation dose in a single 360º arc [3]. Varian has progressive resolution optimizer (PRO) algorithm used in VMAT RapidArc treatment plan optimization, the process depends on constraints to planning target volume (PTV) and organ at risk (OAR). The algorithm will find the best solution for variation of dynamic variables such as dynamic MLC, gantry and dose rate, it has four phases with increasing resolution to deliver optimal dose distribution [4].

VMAT and IMRT are some of radiation therapy techniques used widely in modern radiotherapy. In order to ensure the quality and safety of these radiation therapy techniques, procedural guidelines [5], quality assurance of IMRT [6] and commissioning and QA of VMAT [7] are followed by some of the radiotherapy centers. The proposed procedure consists of three types of tests, the first is to test MLC position accuracy (picket fence test), the second is to evaluate the dose rate control with gantry rotation speed, and the last is to test MLC leaf speed control during VMAT delivery.

American Association of Physicists in Medicine (AAPM) Task Group (TG) 119 has been published as a guidance for testing IMRT commissioning. This document was published based on reports of Radiologic Physics Center (RPC), they showed around 28% of the institutions were involved in the head and neck (HN) IMRT dosimetry audit process failed. TG 119 describes confidence limit (CL) to evaluate treatment planning and treatment delivery for IMRT, it consists of two preliminary tests to check linac stability and five tests that similar to clinically cases [8]. TG 119 guidance can be used to test the VMAT technique commissioning; Mynampati applied TG 119 on VMAT and IMRT then compared with IMRT TG 119. VMAT planning shows results almost the same and it can be compared with IMRT, an average difference of planning by point dose measurement did not exceed 2% and gamma index above 96% for VMAT and IMRT. TG 119 were useful to have confidence in the new modalities such as VMAT, but they require more study from other institutions and vendors [9].

Kang evaluated patient specific quality assurance (QA) results of VMAT and IMRT following TG 119 criteria; the treatment plan evaluation VMAT is able to meet the dose goal of target volume and OARs. The evaluation of absolute and relative dose measurement, VMAT results indicate the value of point dose measurement below 3% and gamma index above 97% [10]. Wen evaluated overall accuracy of VMAT RapidArc and IMRT treatment delivery for both flattening filter-free (FFF) and with flattening filter (FF) based on report of TG 119. The CLs value for both techniques were below the baseline in compared to TG 119 report [11]. Thomas reported TG 119 test tool useful in order to assess the adequacy of VMAT and IMRT commissioning, it is also useful to gain confidence for physicists in the clinic while using a new modality such as VMAT and IMRT. The planning results show the dose constraint based on the measurements, clearly the CLs were well within the baseline specified in TG 119 [12]. The purpose of our study was to test and evaluate commissioning accuracy of VMAT, IMRT treatment planning and dose delivery using AAPM TG 119 recommendations, also generate confidence limits for local institutions.

Material and Methods

TG 119 recommendations were followed in the selection, scanning phantom, treatment planning, and treatment delivery. A solid water phantom with dimensions L x W x H (30 x 30 x 20 cm3) was set up to measure a point dose at 10 cm depth from the surface; it is shown in Figure 1, ionization chambers were put in the center of the phantom and it was scanned in CT simulator. A two-dimensional detector array MatriXX Evolution with MultiCube phantom in a sandwich position were also scanned for planar dose measurements. The phantom was scanned using Philips Brilliance CT Big Bore 16 slices (Philips Healthcare, USA). Both of phantom images were exported directly to the TPS Eclipse to be contoured for structure target (PTV) and organ at risk (OAR); TG 119 provides structure set and it can be imported to the phantom.

Figure1.

Figure1

(A) Solid water phantom and CT scan image (B) MatriXX and CT scan image.

Varian treatment planning system Eclipse (v11.0.47) and linear accelerator Clinac iX D-2300CD with 120 Millennium MLC (Varian Medical Systems, USA) were used in this study. All VMAT and IMRT treatment plans using 6 MV beam, Anisotropic Analytical Algorithm (v11.0.31) were used for 3D dose distributions calculation with 2.5 cm calculation grid size. Equipment used during measurement were an ion chamber with 3 different volumes, electrometer Dose1, 2D array MatriXX Evolution, and a water phantom (IBA Dosimetry, Germany). The AAPM TG 119 problem set consists of two preliminary tests and five commissioning tests that resemble five clinical cases.

Figure 2 shows an illustration of preliminary tests P1 and P2. Preliminary tests P1 consist of a simple AP-PA open field of 10 x 10 cm with a prescribed dose of 2 Gy at the isocenter of solid water phantom. Preliminary tests P2 consisting of a series of AP-PA open fields in different sizes are used to creating a stair-step dose pattern, with dose ranging from 40 cGy to 200 cGy and point dose measurements are made at isocenter using ionization chambers.

Figure2.

Figure2

Illustration of Preliminary (A) test P1 and (B) test P2.

Figure 3(A) shows the multi-target structures, which consist of three cylindrical targets that were stacked along the axis of rotation, each target with a length of approximately 4 cm and diameter 4 cm. Each of these targets has a different dose objective. Figure 3(B) demonstrates the mock prostate structures. The prostate structure is approximately ellipsoidal, with posterior concavity, with right-left (RL), anterior-posterior (AP), and superior-inferior (SI) dimensions of 4.0 x 2.6 x 6.5 cm3, respectively. The prostate PTV is defined as a uniform expansion of 0.6 cm around the prostate. The rectum is a cylinder with diameter of 1.5 cm, and the bladder is 5.0 x 4.0 x 5.0 cm3 in the RL, AP, and SI dimensions, respectively.

Figure3.

Figure3

Mock of (a) multi target, (b) prostate, (c) head and neck, and (d) C-shape structures in Eclipse.

Figure 3(C) shows the mock head and neck (H&N) structures, which consists of a large central PTV with parotid glands on both side and a spinal cord. The structures for H&N case were first drawn on a scanned of an anthropomorphic phantom and then transferred to the rectangular phantom, the gap between the PTV and the spinal cord is 1.5 cm. Finally, Figure 3(D) shows the C-shape structures, which consist of two structures, an outer target with radius of 3.7 cm and a central core with a 1 cm radius, the gap between the two structures is 0.5 cm.

A number of dose objectives or goals for each commissioning test were provided in TG 119. The first specific aim of this work was to develop VMAT and IMRT plans for the TG 119 structure sets. The dose objectives provided in TG 119 were used as guidelines in the treatment planning process in order to create plans that had complexity and modulation similar to the TG 119 institutions’ plans. Table 1 lists of the numbers and arrangements beam for each commissioning test, for IMRT following the recommendations in TG 119, while for VMAT 2 arc is more easier to meet the dose goal criteria.

Table 1.

Beam parameter setup for VMAT and IMRT.

Number of beam/arcs Beam arrangement Collimator Angle Prescribe dose (Gy) Dose per fraction (Gy)
IMRT
Multitarget 7 50º from anterior 50 2
Prostate 7 50º from anterior 80 2
Head and neck 9 40º from anterior 50 2
C-Shape 9 40º from anterior 50 2
VMAT
Multitarget 2 CCW 179-181, CW 181-179 15º 50 2
Prostate 2 CCW 179-181, CW 181-179 30º 80 2
Head and neck 2 CCW 179-181, CW 181-179 30º 50 2
C-Shape 2 CCW 179-181, CW 181-179 30º 50 2

Local VMAT and IMRT treatment planning results were compared with TG 119 dose goal criteria to obtain the ratio between local treatment planning and TG 119. Conformity and the homogeneity index are two analysis tools were used to evaluate dosimetric comparison of VMAT and IMRT plans. Conformity Index (CI) equal to 1 corresponds to the ideal dose coverage or high conformity. Homogeneity Index (HI) corresponds to uniformity of the absorbed-dose distribution within the target volume, usually the PTV as indicated in Equation (1), where D2% is near-maximum, D95% is near-minimum, and D50% is median absorbed doses [13].

CI=Vol 95% coverage doseVol PTV HI=D2%-D98%D50% (1)

TG 119 protocol recommended using ionization chamber and planar dose measurements to have point dose for 2D array. Three ionization chambers, each one with an active volume of 0.01, 0.13, and 0.65 cm3 (IBA dosimetry, Germany) calibrated by Secondary Standard Dosimetry Laboratory (SSDL) BATAN, were listed in Table 2. The dosimeter was used to perform a point dose measurement, a volume of 0.01, 0.13, and 0.65 cm3 chamber selected to measure a dose point. IAEA TRS 398 protocol was used for measuring dose at a certain depth, phantom with a thickness of 20 cm and the ionization chamber has been placed at a 10 cm depth from the phantom surface, positioned at the isocenter of the linear accelerator with SAD 100 cm. The readings of detector were corrected for polarity effects, ion recombination, pressure and room temperature. Point dose measurements were taken at two regions, high and low dose region. Point dose measurement was performed to measure the composite dose of VMAT and IMRT treatment delivery of five tests commissioning TG 119. Point doses were analyzed by using the Equation (2) where Dmeasured was measured dose, Dplan is a planned dose, and Dprescrip was a prescription dose. The dose differences are indicated as the ratio of dose subtraction between planned and measured dose to prescribed dose instead of the predicted local dose.

Table 2.

Technical specifications of the ionization chambers used in the study.

Ionization chamber FC65G, S/N: 2311 CC13, S/N: 9692 CC01, S/N: 9755
Active volume 0.65 cm3 0.13 cm3 0.01 cm3
Polarizing voltage 300 V 300 V 300 V
Wall material Aluminum + Graphite Shonka Steel + Shonka

dose diff=Dmeasured-DplanDprescrip (2)

MatriXX Evolution 2D array detector, MultiCube phantom, and OmniPro IMRT software were used to measure composite planar dose distribution and to compare it with a planar dose of the treatment planning. Gamma index analysis was established for composite planar dose distribution. The gamma index technique, which is the standard method for planar dose verification in IMRT QA, calculates the quantity gamma for each point of interest using preselected dose difference (DD) and distance to agreement (DTA) criteria and then uses the gamma value to determine the outcome (pass-fail) of the IMRT QA. Gamma index was examined for the composite planar dose distribution, the criteria were set for 3 % DD, 3 mm DTA and 2 % DD, 2 mm DTA for IMRT (7 field and 9 field) and VMAT treatment delivery (2 arc).

In addition, the confidence limit (CL) was used as recommended and defined by TG 119. In TG 119, the 95% CL were established by fitting the gamma passing rate results to an assumed Gaussian distribution, then calculating the limit in which about 95% of all datasets fall within. New clinics can use TG 119 as a reference while commissioning their own IMRT program by using the aggregate gamma passing rates from multiple clinics and their associated 95% CLs. The CL is the sum of the absolute value of the average differences and the standard deviation of the differences multiplied by a factor of 1.96 as indicated in Equation (3).

CL=|mean|+1.96 SD CL=|100-mea|+1.96 SD (3)

Results and Discussions

The VMAT and IMRT dose distribution for the multi target, prostate, head and neck, and C-shape cases were shown in Figure 4. It is shown that dose distribution in 95 % isodose line between VMAT and IMRT is comparable, whereas IMRT produce more dose distribution in 30 % isodose line than VMAT.

Figure4.

Figure4

VMAT and IMRT dose distributions for all test commissioning.

VMAT and IMRT treatment planning dose results for five clinical tests were tabulated in Table 3. The table demonstrates that VMAT and IMRT treatment planning system for four clinical tests were capable to meet the dose goals criteria set by TG 119 except for C-shape hard. For C-shape hard case, IMRT PTV D10, Core D10, and VMAT Core D10 dose criteria could not be achieved in a local clinic as per TG 119 protocol. Since the beginning the plan goal for Core D10˂1000 set by TG 119 would not probably be achievable, it is for testing a treatment planning system being pushed very hard. In each of table, DXX designates the minimum absorbed dose received by XX% of the total volume of interest, D30 of the rectum = 70 Gy. It means that 30% of the rectum volume receives at least 70 Gy. This is determined from the cumulative DVH and can be read off the cDVH.

Table 3.

VMAT and IMRT treatment plan dose goals results .

Test/Planning parameters Volume (cm3) Plan goal (cGy) IMRT VMAT AAPM TG 119 Mean (cGy) IMRT/ TG 119 VMAT/ TG 119
Mean (cGy) Mean (cGy)
Multi target
Central D99 51.6 ˃5000 5023 ± 3 5038 ± 23 4955 ± 162 1.01 1.02
Central D10 ˂5300 5286 ± 5 5279 ± 4 5455 ± 173 0.97 0.97
Superior D99 51.4 ˃2500 2514 ± 13 2527 ± 1 2516 ± 85 1.00 1.00
Superior D10 ˂3500 3431 ± 11 3422 ± 44 3412 ± 304 1.01 1.00
Inferior D99 51.5 ˃1250 1374 ± 3 1344 ± 57 1407 ± 185 0.98 0.96
Inferior D10 ˂2500 2250 ± 18 2445 ± 24 2418 ± 272 0.93 1.01
Prostate
PTV Prostate D95 107.9 ˃7560 7663 ± 36 7838 ± 17 7566 ± 21 1.01 1.04
PTV Prostate D5 ˂8300 8129 ± 10 8144 ± 38 8143 ± 156 0.97 1.00
Rectum D30 20.71 ˂7000 6266 ± 44 6308 ± 49 6536 ± 297 1.00 0.97
Rectum D10 ˂7500 7284 ± 27 7331 ± 43 7303 ± 15 1.01 1.00
Bladder D30 63.59 ˂7000 4624 ± 62 5103 ± 67 4394 ± 878 0.98 1.16
Bladder D10 ˂7500 5913 ± 64 6375 ± 97 6269 ± 815 0.93 1.02
Head and neck
PTV D90 721.01 5000 5072 ± 6 5037 ± 9 5028 ± 58 1.01 1.00
PTV D99 ˃4650 4856 ± 7 4880 ± 22 4704 ± 52 1.03 1.04
PTV D20 ˂5500 5247 ± 5 5195 ± 5 5299 ± 93 0.99 0.98
Cord maximum 19.18 ˂4000 3887 ± 4 3877 ± 34 3741 ± 250 1.04 1.04
Parotid LT D50 10.21 ˂2000 1927 ± 3 1874 ± 29 1798 ± 184 1.07 1.04
Parotid RT D50 9.98 ˂2000 1943 ± 2 1878 ± 6 1798 ± 184 1.08 1.04
C-shape easy
PTV D95 283.91 5000 5016 ± 4 5012 ± 7 5010 ± 17 1.00 1.00
PTV D10 ˂5500 5351 ± 2 5340 ± 5 5440 ± 52 0.98 0.98
Core D10 31.54 ˂2500 2237 ± 22 2234 ± 21 2200 ± 314 1.02 1.02
C-shape hard
PTV D95 283.91 5000 5057 ± 32 5024 ± 3 5011 ± 165 1.01 1.00
PTV D10 ˂5500 5596 ± 53 5447 ± 4 5702 ± 220 0.98 0.96
Core D10 31.54 ˂1000 1558 ± 19 1420 ± 4 1630 ± 307 0.96 0.87

Figure 4 shows axial plane dose distributions of VMAT and IMRT plans for multi target, prostate, head and neck, and C-shape cases. The dose distributions were 30% from total dose.

Table 4 shows comparison of VMAT and IMRT plan parameter results. It consists of conformity and homogeneity indexes, number of beams, total monitor units (MU), and MU ratio of different test cases planned for both modalities. Conformity index for VMAT and IMRT were comparable for multi-target and c-shape hard test, IMRT conformity index are higher than VMAT in prostate and c-shape easy test, the value is 0.980, 1,193 and 1.160, 1.349 for IMRT and VMAT, respectively. VMAT conformity index is higher than IMRT in the last test, with a value of 1,128 and 1,198. Homogeneity indexes (HI) show comparable results for all clinical tests, for all five test cases the HI shows value close to zero. HI indicates the ratio between the maximum and minimum dose in the target volume and the lower value indicates a more homogenous dose distribution within the target volume.

Table 4.

The results of treatment plan comparison between VMAT and IMRT.

Multi Target Prostate Head and Neck C-shape easy C-shape hard
IMRT VMAT IMRT VMAT IMRT VMAT IMRT VMAT IMRT VMAT
Conformity index 1.357 1.372 0.980 1.160 1.198 1.128 1.193 1.349 1.355 1.400
Homogeneity index 0.042 0.047 0.074 0.055 0.067 0.073 0.113 0.090 0.154 0.133
Number of beams 7 2 7 2 9 2 9 2 9 2
Dose per fraction 200 200 200 200 200 200 200 200 200 200
Total MU 532 372 469 560 1374 497 1174 902 1464 985
MU ratio 1.43 1 0.84 1 1.76 1 1.30 1 1.49 1

Total monitor unit (MU) comparison between volumetric modulated arc therapy and intensity-modulated radiation therapy treatment plans was made for all test cases. VMAT plans resulted in fewer MUs with the quality of treatment planning being similar or even better than IMRT for all test cases except in prostate case. Total MU for IMRT plan of all test cases were 532, 469, 1374, 1174 and 1464 for multi target, prostate, head and neck, C shape from easy one to hard respectively, while the total monitor unit in VMAT were 372, 560, 497, 902 and 985, respectively. If the total MU of VMAT plans becomes the reference; the ratios of total MU for both of plans were 1.43, 0.84, 1.76, 1.30, and 1.49 respectively for all test cases. The complexity of the plan was found to be proportional to the total MU ratio, but the increase number of total MU was lower in VMAT plan compared to IMRT plan.

The Linear accelerator output calibration for 6 MV energy was performed following IAEA TRS 398, the deviation value between the measurement and the reference value was 0.36 %. That value was within the acceptable tolerance, according to AAPM TG 142 the deviation tolerance for Linac output is 2 % [14]. The result from 6 MV output calibrations can be used for implementing VMAT and IMRT treatment plan.

Tables 5 and 6 show dose point measurements and dose variations results between planned and measured dose for preliminary test P1 and P2 using three different ion chambers: CC01, CC13, and FC65. The three chambers demonstrate dose variation below 2%. The range of dose variations in test P2: bands from - 0.03 % to 1.78 %, meanwhile the mean dose variations are 1.17 %, 0.22 % and 0.32 % for CC01, CC13, and FC65 respectively. Both of these preliminary tests revealed that the non-IMRT system was commissioned with adequate accuracy.

Table 5.

The point dose measurements for preliminary test P1.

Test Ion chamber Planned dose (cGy) Measured dose (cGy) Dose variation
P1 CC01 200 201.93 0.0096
CC13 200 202.39 0.0120
FC65G 200 202.78 0.0139

Table 6.

The point dose measurements for preliminary test P2.

Test Location Planned dose (cGy) CC01 CC13 FC65G
Measured dose (cGy) Dose variation Measured dose (cGy) Dose variation Measured dose (cGy) Dose variation
P2 1st band left of isocenter 40 40.71 0.0178 40.08 0.0019 40.09 0.0022
2st band left of isocenter 80 80.78 0.0098 80.02 0.0002 80.15 0.0019
Pita 3 di isocenter 120 121.39 0.0116 120.65 0.0054 120.83 0.0069
1st band right of isocenter 160 161.23 0.0077 159.96 -0.0003 160.19 0.0012
2nd band right of isocenter 200 202.32 0.0116 200.72 0.0036 200.78 0.0039
Mean dose variation 0.0117 0.0022 0.0032

Tables 7 and 8 demonstrate dose point measurements, mean dose variations, standard deviation, and confidence limit results at high dose and low dose area of five clinical test cases for VMAT and IMRT using ionization chambers CC01, CC13, and FC65G. The prescription dose at isocenter is 200 cGy per fraction for all targets. Table 7 shows the maximum dose variations at high dose area for IMRT are 0.87 %, -0.52 %, 0.06 % and minimum dose variations of -0.04 %, -1.1 %, -1.14 % for ion chambers CC01, CC13, FC65G were measured, respectively. The means of the dose variations of CC01, CC13 and FC65G for IMRT are 0.33 %, -0.75 %, -0.44 and standard deviations of all these measurements are 0.37 %, 0.23 %, 0.48 %, respectively. The confidence limit (CL) values related to these mean and standard deviations are 0.0106, 0.0119, and 0.0137 for CC01, CC13, and FC65G chamber respectively. For VMAT, high dose area measurements show maximum dose variations of 1.03 %, -0.003 %, -0.34 % and minimum dose variations of -0.05, -1.23, -0.157 for CC01, CC13, and FC65G chamber respectively. The confidence limit (CL) values for VMAT are 0.0147, 0.0171, and 0.0208 for CC01, CC13, and FC65G, respectively.

Table 7.

VMAT and IMRT doses variation, standard deviation, and CL at high dose area.

Test Location IMRT VMAT
CC01 CC13 FC65G CC01 CC13 FC65G
Multi target Isocenter 0.00003 -0.0052 0.0006 -0.0003 -0.0003 -0.0137
Prostate Isocenter -0.0004 -0.0060 -0.0013 0.0091 -0.0123 -0.0157
Head and neck Isocenter 0.0087 -0.0069 -0.0030 0.0052 -0.0110 -0.0125
C shape (easy) 2.5 cm anterior to isocenter 0.0047 -0.0082 -0.0067 0.0103 -0.0073 -0.0053
C shape (hard) 2.5 cm anterior to isocenter 0.0035 -0.0110 -0.0114 -0.0005 -0.0017 -0.0034
Mean of dose variations 0.0033 -0.0075 -0.0044 0.0048 -0.0065 -0.0101
Standard deviation σ 0.0037 0.0023 0.0048 0.0051 0.0054 0.0054
CL = |mean| + 1.96 σ 0.0106 0.0119 0.0137 0.0147 0.0171 0.0208

Table 8.

VMAT and IMRT doses variation, standard deviation, and CL at low dose area.

Test Location IMRT VMAT
CC01 CC13 FC65G CC01 CC13 FC65G
Multi target 4 cm inferior to isocenter 0.0041 -0.0042 -0.0110 0.0086 -0.0041 -0.0206
Prostate 2.5 cm posterior to isocenter 0.0072 -0.0146 -0.0154 0.0006 0.0142 0.0331
Head and neck 4 cm posterior to isocenter 0.0048 -0.0066 -0.0264 0.0055 -0.0049 -0.0082
C shape (easy) Isocenter 0.0067 -0.0030 -0.0029 0.0007 0.0089 0.0007
C shape (hard) Isocenter 0.0043 -0.0044 -0.0077 0.0072 -0.0047 -0.0057
Mean of dose variations 0.0054 -0.0065 -0.0127 0.0045 0.0019 -0.0002
Standard deviation σ 0.0014 0.0047 0.0089 0.0037 0.0090 0.0201
CL = |mean| + 1.96 σ 0.0082 0.0158 0.0302 0.0117 0.0195 0.0396

Table 8 corresponds to doses variation, standard deviation, and CL at the low dose area. The location of low dose area measurement for multi target structure sets is 4 cm inferior to the isocenter, for prostate, head and neck structure low dose area measurement are at 2.5 cm and 4 cm posterior to the isocenter, whereas the low dose area measurement for C shape easy and hard structure sets are located at isocenter. For IMRT measurements at low dose area the CL are 0.0082, 0.0158, and 0.0302, whereas for VMAT CL are 0.0117, 0.0195, and 0.0396 for ion chamber CC01, CC13, FC65G respectively.

Three ionization with various active volumes showed an increase in the CL, the larger the active volume of ion chamber was found proportional to increase the value of CL. For the target and avoidance structure, CC01 reveals the lowest CL (0.82 %, 1.06 % for IMRT and 1.17 %, 1.47 % for VMAT), whereas FC65G has the highest CL (3.02 %, 1.37 % for IMRT and 3.96 %, 2.08 % for VMAT) in low dose and high dose gradient regions. TG 119 recommended that the confidence limit value for this was 4.7 %, local CLs were within 0.047. Even though FC65G CL within TG 119 limit, there is dose variation in low dose area more than 3 % beyond the expectations set by TG 119. This volume effect of the FC65G chamber or Farmer chamber could lead to inaccurate conclusions upon clinical verification of VMAT and IMRT treatment planning, one of the causes is the lack of spatial resolution of the detector used [15].

Tables 9 and 10 show the composite gamma index analysis for all different test cases planned for both modalities in high dose and low dose area, measured a 2D array MatriXX Evolution, phantom multi cube, and analyzed OmniPro-I’MRT software, the composite gamma index analysis are compared between VMAT and IMRT in Figure 5. The table contains test name, location, and % pass rate of gamma analysis for VMAT and IMRT for each test commissioning. The mean percentage of 3 %/3 mm and 2 % DD/2 mm DTA criteria for IMRT are 98.59, 95.21 (high dose area) and 97.28, 90.75 (low dose area). The standard deviations of the gamma analysis for IMRT are 1.16, 3.53 (high dose area) and 1.63, 2.28 (low dose area). The corresponding CLs are 3.68, 11.71 (high dose area) and 5.93, 13.71 (low dose area). For VMAT CL of gamma evaluation with the same IMRT analyzing, criteria are 1.44, 6.33 (high dose area) and 3.89, 7.18 (low dose area).

Table 9.

Gamma evaluation for VMAT and IMRT at high dose area.

Test Location 3%, 3 mm gamma pass 2%, 2 mm gamma pass
IMRT VMAT IMRT VMAT
Multi target Isocenter 99.23 99.80 97.42 98.77
Prostate Isocenter 99.04 99.62 97.31 98.42
Head and neck Isocenter 99.44 99.57 96.81 96.30
C shape (easy) 2.5 cm anterior to isocenter 96.59 99.14 89.05 95.33
C shape (hard) 2.5 cm anterior to isocenter 98.65 98.77 95.46 95.50
Overall mean 98.59 99.38 95.21 96.86
Overall Standard deviation σ 1.16 0.42 3.53 1.63
CL = |mean| + 1.96 σ 3.68 1.44 11.71 6.33

Table 10.

Gamma evaluation for VMAT and IMRT at low dose area.

Test Location 3%, 3 mm gamma pass 2%, 2 mm gamma pass
IMRT VMAT IMRT VMAT
Multi target 4 cm inferior to isocenter 95.63 98.26 89.80 94.00
Prostate 2.5 cm posterior to isocenter 95.43 97.20 89.96 94.24
Head and neck 4 cm posterior to isocenter 98.71 98.66 88.89 94.04
C shape (easy) Isocenter 97.87 98.76 90.42 94.92
C shape (hard) Isocenter 98.75 96.69 94.71 93.14
Overall mean 97.28 97.91 90.75 94.07
Overall Standard deviation σ 1.63 0.92 2.28 0.64
CL = |mean| + 1.96 σ 5.93 3.89 13.71 7.18

Figure5.

Figure5

The comparison between the gamma index map of the dose distribution for VMAT and IMRT.

All gamma evaluation results show more than 95% data points pass the criteria of 3% DD and 3 mm DTA, but for more tight criteria 2 % DD and 2 mm DTA IMRT at the low dose area fail to meet the criteria. For the same 3 %, 3 mm criteria TG 119 result value is 12.4 (i.e. 87.6 % dose point pass the criteria) as a base line. Both of them were in line with the study of Kang et al., Wen et al., and Thomas et al. [10-12] that the AAPM TG 119 can be implemented on commissioning VMAT.

Conclusion

Comparing VMAT and IMRT by AAPM TG 119 protocol along with points and composite dose measurements demonstrates adequate accuracy in delivering treatments. The ionization chamber that is smaller than a Farmer type recommended by TG 119 with 0.01 cm3 and 0.13 cm3 for IMRT point dose measurement shows the confidence limit value of below 4.2 % and dose difference 3 %, while the Farmer type chamber could not meet dose criteria of 3 % dose difference. The two-dimension detector array shows CL gamma index with criteria of 3 % / 3 mm which is below 12.4 that is a limit set of TG 119 .

The CL value from the result of measurements could be used as a reference and recommendation to evaluate the accuracy and integrity of treatment planning and treatment delivery systems of VMAT and IMRT. Planning target set by TG 119 was helpful to determine baseline IMRT commissioning and it was useful for testing of new modalities such as VMAT before clinical implementation. This study focused to develop CL to evaluate the accuracy of VMAT commissioning and increase the confidence in the implementation of complex techniques.

Acknowledgement

We thanks to the management of MRCCC Siloam Hospitals Semanggi who has allowed us to do the research in Radiotherapy Facility. This study was supported by Universitas Indonesia Grant with contract number 540/UN2.R12/HKP.05.00/2015.

Conflict of Interest:None

References

  • 1.Webb S. The physical basis of IMRT and inverse planning. Br J Radiol. 2003;76:678–89. doi: 10.1259/bjr/65676879. [DOI] [PubMed] [Google Scholar]
  • 2.Yu C X. Intensity-modulated arc therapy with dynamic multileaf collimation: an alternative to tomotherapy. Phys Med Biol. 1995;40:1435–49. doi: 10.1088/0031-9155/40/9/004. [DOI] [PubMed] [Google Scholar]
  • 3.Otto K. Volumetric modulated arc therapy: IMRT in a single gantry arc. Med Phys. 2008;35:310–7. doi: 10.1118/1.2818738. [DOI] [PubMed] [Google Scholar]
  • 4.Vanetti E, Nicolini G, Nord J, Peltola J, Clivio A, Fogliata A, et al. On the role of the optimization algorithm of RapidArc® volumetric modulated arc therapy on plan quality and efficiency. Med Phys. 2011;38:5844–56. doi: 10.1118/1.3641866. [DOI] [PubMed] [Google Scholar]
  • 5.LoSasso T, Chui C S, Ling C C. Comprehensive quality assurance for the delivery of intensity modulated radiotherapy with a multileaf collimator used in the dynamic mode. Med Phys. 2001;28:2209–19. doi: 10.1118/1.1410123. [DOI] [PubMed] [Google Scholar]
  • 6.Alber M, Broggi S, De Wagter C, Eichwurzel I, Engström P, Fiorino C, et al. Guidelines for the verification of IMRT. ESTRO Booklet. 2008;7 [Google Scholar]
  • 7.Ling C C, Zhang P, Archambault Y, Bocanek J, Tang G, Losasso T. Commissioning and quality assurance of RapidArc radiotherapy delivery system. Int J Radiat Oncol Biol Phys. 2008;72:575–81. doi: 10.1016/j.ijrobp.2008.05.060. [DOI] [PubMed] [Google Scholar]
  • 8.Ezzell G A, Burmeister J W, Dogan N, LoSasso T J, Mechalakos J G, Mihailidis D, et al. IMRT commissioning: multiple institution planning and dosimetry comparisons, a report from AAPM Task Group 119. Med Phys. 2009;36:5359–73. doi: 10.1118/1.3238104. [DOI] [PubMed] [Google Scholar]
  • 9.Mynampati D K, Yaparpalvi R, Hong L, Kuo H C, Mah D. Application of AAPM TG 119 to volumetric arc therapy (VMAT) J Appl Clin Med Phys. 2012;13:108–16. doi: 10.1120/jacmp.v13i5.3382. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 10.Kang D J, Jung J Y, Kim H J, Park S, Lee K S, Sohn S C, et al. The Patient Specific QA of IMRT and VMAT Through the AAPM Task Group Report 119. Journal of the Korean Society of Radiological Technology. 2012;35:255–63. [Google Scholar]
  • 11.Wen N, Zhao B, Kim J, Chin-Snyder K, Bellon M, Glide-Hurst C, et al. IMRT and RapidArc commissioning of a TrueBeam linear accelerator using TG-119 protocol cases. J Appl Clin Med Phys. 2014;15:74–88. doi: 10.1120/jacmp.v15i5.4843. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 12.Thomas M, Chandroth M. Local confidence limits for IMRT and VMAT techniques: a study based on TG119 test suite. Australas Phys Eng Sci Med. 2014;37:59–74. doi: 10.1007/s13246-014-0241-5. [DOI] [PubMed] [Google Scholar]
  • 13.Vol I. Prescribing, recording, and reporting photon-beam intensity-modulated radiation therapy (IMRT): contents. J ICRU. 2010;10 [Google Scholar]
  • 14.Klein E E, Hanley J, Bayouth J, Yin F F, Simon W, Dresser S, et al. Task Group 142 report: quality assurance of medical accelerators. Med Phys. 2009;36:4197–212. doi: 10.1118/1.3190392. [DOI] [PubMed] [Google Scholar]
  • 15.Laub W U, Wong T. The volume effect of detectors in the dosimetry of small fields used in IMRT. Med Phys. 2003;30:341–7. doi: 10.1118/1.1544678. [DOI] [PubMed] [Google Scholar]

Articles from Journal of Biomedical Physics & Engineering are provided here courtesy of Shiraz University of Medical Sciences

RESOURCES