|Year : 2020 | Volume
| Issue : 2 | Page : 123-129
Simultaneous measurement of In vivo and transit mid-plane doses with ionization chambers in gynecological malignancy patients undergoing three-dimensional conformal radiotherapy
Putha Suman Kumar1, Challapalli Srinivas1, BM Vadhiraja2, Sourjya Banerjee1, R Shreyas1, PU Prakash Saxena1, Ramamoorthy Ravichandran1, Dilson Lobo1
1 Department of Radiation Oncology, Kasturba Medical College (A constituent institution of Manipal Academy of Higher Education, Manipal), Mangalore, Karnataka, India
2 Department of Radiation Oncology, Manipal Hospitals, Bengaluru, Karnataka, India
|Date of Submission||14-Jan-2020|
|Date of Decision||05-May-2020|
|Date of Acceptance||05-May-2020|
|Date of Web Publication||20-Jul-2020|
Dr. Challapalli Srinivas
Department of Radiation Oncology, Kasturba Medical College, (A constituent Institution of Manipal Academy of Higher Education, Manipal), Mangalore - 575 001, Karnataka
Source of Support: None, Conflict of Interest: None
| Abstract|| |
Purpose: The aim of this study is to estimate delivered radiation doses inside planning tumor volume (PTV) using the in vivo (mid-plane dose) measurement and transit measurement methods in gynecological malignancy patients undergoing three-dimensional conformal radiotherapy (3DCRT) using calibrated ionization chambers. Materials and Methods: Six patients with histopathologically proven carcinoma of the cervix or endometrium were planned with four-field 3DCRT to the pelvic site. Isocenter was at the geometric mid-plane of PTV with a dose prescription of 50 Gy in 25 fractions. Clinical mid-plane dose (Diso,Transit) estimates were done in one method (transit) using the FC-65 positioned at electronic portal imaging device level. In another method, a repeat computerized tomography scan was performed (at the 11th fraction) using CC-13 having a protective cap in the vaginal cavity for in vivo measurements (Din vivo). Simultaneous measurements were performed with the two chambers from the 11th fraction onward at least 3–4 times during the remaining course of treatment. Results: The agreement of mean doses from these two described methods and treatment planning system reference doses was in the range of −4.4 ± 1.1% (minimum) to −0.3 ± 2.0% (maximum) and −4.0 ± 1.7% (minimum) to 1.9 ± 2.4% for Dinvivoand Diso,Transit, respectively, which are an acceptable range of daily radiation dose delivery. Conclusion: The fundamental importance of this study lies in simultaneous validation of delivered dose in real time with two methods. A study in this small number of patients has given the confidence to apply transit measurements for quality assurance on a routine basis as an accepted clinical dosimetry for the selected patients.
Keywords: In vivo dosimetry, quality assurance, real-time dose estimate, transit dosimetry
|How to cite this article:|
Kumar PS, Srinivas C, Vadhiraja B M, Banerjee S, Shreyas R, Prakash Saxena P U, Ravichandran R, Lobo D. Simultaneous measurement of In vivo and transit mid-plane doses with ionization chambers in gynecological malignancy patients undergoing three-dimensional conformal radiotherapy. J Med Phys 2020;45:123-9
|How to cite this URL:|
Kumar PS, Srinivas C, Vadhiraja B M, Banerjee S, Shreyas R, Prakash Saxena P U, Ravichandran R, Lobo D. Simultaneous measurement of In vivo and transit mid-plane doses with ionization chambers in gynecological malignancy patients undergoing three-dimensional conformal radiotherapy. J Med Phys [serial online] 2020 [cited 2020 Oct 23];45:123-9. Available from: https://www.jmp.org.in/text.asp?2020/45/2/123/290220
| Introduction|| |
In vivo dosimetry in external-beam radiotherapy plays a vital role in ensuring the delivery of prescribed dose to the patient at the treatment site. In the individual departments, regular quality assurance (QA) checks such as beam output and quality, isocenter, field congruence, and reproducibility in treatment executions are performed in the treatment machines on a routine basis. Apart from these, however, errors are known to occur during the course of treatment (both inter- and intra-treatments) (e.g., setup positions, source to the skin distance, and morphological changes resulting in variations in patient contour), necessitating the implementation ofin vivo dosimetry.
An effective way of checking the status of the entire dosimetric procedures, starting from the performance of the treatment machine to accurate positioning of the patient, is to make absorbed dose measurements in the patient and when possible, in body cavities. Several studies have demonstrated quantification of mid-plane dose during real-time treatment deliveries (e.g., entrance, exit and transit dose measurements) with different detectors (e.g., thermoluminescence detectors, diodes, metal–oxide–semiconductor field-effect transistor, ionization chambers, chemical dosimetry, and/or electronic portal imaging device [EPID]).,,, Ionization chambers have always been the gold standard for reference dosimetry in radiation therapy; several documents, textbook chapters, and clinical studies have demonstrated their important role inin vivo dosimetry in patients treated by megavoltage radiotherapy with different techniques, for example, parallel-opposed three-dimensional conformal radiotherapy (3DCRT) and intensity-modulated radiotherapy (IMRT).,,,,,,
Typically, these chambers are placed in a central region of a phantom or in a region corresponding to the uniform high-dose area, which is then irradiated by all of the treatment beams. Ionization chambers are limited by the fact that they can only report dose to a point or averaged over a small area. In some of the studies, thein vivo dose was measured by inserting an ionization chamber directly into the natural body cavity (e.g., esophagus, rectum, or vagina) with a protective cap which comes in the region of the treatment portals.,,, The temperature of the cavity (which is the surrogate of the body temperature) where the chamber is placed is taken into account for temperature correction factor that needs to be applied to the charge collected by the chamber. The dose is then calculated by application of all chamber-related correction factors (e.g., calibration factor, temperature, pressure, and beam quality) to the collected charge. The estimated dose is compared to the planned dose by the computerized treatment planning system (TPS). Few studies described methods to assessin vivo mid-plane dose in patients through transit signal measured by an ionization chamber positioned at the EPID level while actual treatment is going on.,,,,,,
Angelo Piermattei et al. reported the results of the application of a practical method to determine thein vivo dose at the isocenter point of the brain, thorax, and pelvic treatments using a transit signal “St” (X-ray beam transmitted through the patient) measured with an ionization chamber which is positioned at the EPID level. By this method, the disadvantages associated with the use of solid-state detectors positioned on the patient and their positioning time are minimized. Simultaneous measurements ofin vivo and mid-plane dose through transit method were performed using two ionization chambers, one placed intraluminally in patients who are undergoing esophagus treatment and the other one kept at a transit level, which was reported in the literature. A method was described to estimate mid-plane dose by measuring transit signal (Diso-transit) in pelvic and thorax patients which was correlated with TPS-calculated values., In these studies, simultaneous measurements ofin vivo and mid-plane dose were also carried out on pelvic and thorax phantoms using two ionization chambers, one kept at the mid-plane level and the another one at EPID level which were compared with the TPS-calculated values. In such new treatment plans in the department, there is a need for documentation of daily dose delivered to the planning target volume (PTV). To confirm delivered doses in a protocol group of pelvic radiotherapy, we need to standardize a method and we investigated simultaneous measurement within vivo and transit dosimetry.
| Materials and Methods|| |
Subjects of study
A medical linear accelerator (Model: Compact, Elekta Ltd, Crawley, UK) with 6 MV photons, equipped with motorized wedge, 40 pairs multileaf collimator (MLCi2) having leaf thickness of 1 cm at 100 cm isocenter, and camera-based portal imaging was used for 3DCRT treatments. The machine was calibrated to deliver 1cGy/MU with a dose rate of 350MU/min under the calibration conditions stated in the International Atomic Energy Agency (IAEA) dosimetry code of practice (TRS-398). In this study, onlinein vivo mid-plane dose estimates are made using two calibrated ionization chambers (Models: CC13 and FC65, IBA Dosimetry, Germany) simultaneously in patients with gynecological malignancy (endometrium and cervix), who have received the 3DCRT course schedule. Both the chambers are connected to dual-channel electrometer (Dose2, IBA Dosimetry, Germany) for charge collection, and the absolute dose measurements are arrived in a water phantom using TRS-398 protocol and the doses accepted within 0.2%. Estimates of onlinein vivo mid-plane doses were correlated with the TPS-calculated values at reference point inside the PTV. We got approval from a small number of gynecological malignant patients from institutional ethics committee (approval letter number: IEC KMC MLR 11-14/224) to conduct thisin vivo dosimetric study. Six patients had participated in this study. After the explanation of the nature of procedure, informed consent was obtained from all patients before the treatment process began.
Treatment planning (immobilization, simulation, and contouring)
All patients were immobilized in the supine treatment position using “Vacloc” device keeping their hands above the head; institution-specific bladder and rectal protocol was followed during simulation and treatment. Transverse images of 5 mm slice thickness acquired from computerized tomography (CT) scanner (Wipro GE, Model: High Speed) were exported to a contouring station (Focal Sim, M/s Elekta Ltd., Crawley, UK) for the generation of the clinical target volume (CTV) and marking organs at risk (OAR). A 5 mm margin was created around the CTV which forms PTV, to account for inter-fractional and geometric positional uncertainties. The contoured image data set was exported to the TPS (CMS XiO®, version 5.0, Elekta Ltd, Crawley, UK) for dose calculations using a superposition algorithm.
Four-field box technique treatment plans were used in all patients with beams directed through gantry angles of 0°, 90°, 180°, and 270°. The isocenter of all beams coincides with the intersecting point of anterior–posterior and lateral portals, along with the central axis corresponding to the center of PTV. The generated 3DCRT treatment plan with MLC covers PTV along with an additional margin of 5 mm. Depending on the requirement, either field-in-field (subfields) and/or wedge technique was used, for better homogeneity of the dose around the target region. A dose prescription of 50 Gy in 25 fractions (at 2.0 Gy per fraction) was normalized to 100% isodose line covered to PTV. It was ensured that the dose at the isocenter (i.e., Diso,TPS) is identical to the homogeneous prescribed dose in 3DCRT plan. This “template” treatment plan was saved to locate the detector location in vivo, in future fractions. Plan evaluation, approval, scheduling, and patient treatment verification before the execution of the first fraction were carried out in a similar way as followed by Putha et al.
Transit dose estimates
At the EPID level, a 0.65 cc ionization chamber (Model FC65-G from IBA Dosimetry, Germany) with vendor provided acrylic buildup cap (for 6 MV photon beam) of thickness 3.0 cm diameter was placed on the mounting assembly along the central axis. Source to chamber center distance was maintained approximately 1.463 m. The chamber was connected to the channel 1 of Dose2 electrometer for the measurement of transit signals for all conformal fields during “real-time” treatment for all patients. The mid-plane dose at isocenter by transit signal (i.e., Diso,Transit) was calculated using the method described by Putha et al. and was compared with the values of “Diso,TPS” of all the respective patients' conformal fields.
Transit andin vivo dose estimates
After 10 fractions were done, a repeat CT scan was performed in all patients by placing a CC13 ionization chamber (which is covered with a custom made acrylic cylindrical cap, extending to the stem level) in the vaginal cavity without changing immobilization device and patient orientation. In addition, a removable latex rubber sleeve is used to overcome the risk of fluid intrusion into the cap. As per the technical manual of CC13 ion chamber, the outer electrode is at earth potential along with the cable. Therefore, along with a rubber sleeve, it was confirmed that there is no risk to the patient during the collection of signals in nano Coulombs (nC). In this way,in vivo detector positioning was performed in all patients after 10 fractions. Three fiducial markers (one marker representing the anterior entry beam and the other two at left and right lateral sides indicating lateral beam entry) were placed along the patient's ongoing transverse iso-center plane. Repeat serial CT images were imported to the contouring station for chamber localization and exported them to TPS for dose calculations. Confirmation of CTV and treatment area has been reconfirmed by the radiation oncologist using the first collection of CT images in the repeat CT images. The point of calculation corresponds to the point of intersection of all three “fiducial” markers (visualized on the repeated transverse CT slice). Chamber location was ensured in all conformal treatment portals. The mean dose of the chamber (i.e., Din vivo,TPS) to the location of the sensitive volume is noted from the dose–volume histogram of TPS.
At the 11th fraction of the treatment,in vivo detector was positioned into the vaginal cavity of the patient for real-timein vivo dose measurements. The temperature of the patient's body is recorded. Verification of patient's treatment setup under Linac was checked with camera-based EPID (iViewC). A 3 mm margin of translational (x, y, and z) errors was permitted and appropriate couch changes were applied as needed. Once the treatment setup is verified, the transit stand is fixed at the level of EPID. The fixation of the stand (with FC65 ionization chamber in transit position) at the level of EPID of the Linac is well explained in our earlier work by Putha et al.
Both the chambers (i.e., FC65 [transit] and CC13 [in vivo]) were connected to the Dose2 electrometer in channel 1 and 2, respectively. The scheduled treatment plan was executed on the patient. With this measurement setup, chamber readings in nano Coulombs were recorded simultaneously during real-time treatment delivery. The readings of the detector (CC13) are converted to absorbed dose by incorporating necessary correction factors (calibration factor, body temperature, pressure, polarity, beam quality, and saturation) at chamber location, designated asin vivo dose (i.e., “Din vivo”). The chamber reading obtained from FC65 (transit signal) is used to estimate the mid-plane dose at isocenter (i.e., Diso,Transit) using the method described by Putha et al. This procedure was repeated at least 3–4 times with a gap of 3–4 fractions during the remaining course of treatment. The measured value ofin vivo dose, i.e., Din vivo, is correlated with the value obtained from TPS i.e., Din-vivo,TPS. [Figure 1] shows the position of CC13 ionization chamber with contour inside the patient's body in transverse, coronal, and sagittal sections of CMS XiO TPS. The [Figure 2]a and 2b shows the anterior conformal RT field in a patient (in supine position) with Coronal and Transverse planes where the estimates of mid-plane dose through transit signal with FC65 (i.e., Diso, Transit) and in vivo dose measurement with CC13 (i.e., Din vivo), respectively, by dual-channel electrometer is obtained.
|Figure 1: Position of CC13 ionization chamber with contour inside the patient's body in transverse, coronal, and sagittal sections of CMS XiO TPS|
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|Figure 2: (a and b) Represents the perspective views of anterior field of three-dimensional conformal radiotherapy treatment to the pelvic site of a patient under linac, showing the transverse and coronal planes containing (a) the treatment isocenter for estimation of transit mid-plane dose (Diso,transit) through transit signal obtained from FC65 chamber with buildup cap, which was kept at EPID level, and (b) the location of CC13 chamber (with protective cap) in vaginal cavity for measurement of “Din vivo”. Both the measurements were done simultaneously with chambers during real-time treatment delivery, for all four conformal fields (0°, 90°, 180°, and 270°) on at least 3–5 occasions (after having taken the repeat computerized tomography) during the course of treatment. Chambers' signals were measured with “Dose2” dual channel electrometer. The lower right side of the figure represents the patient orientation icon for treatment|
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| Results|| |
[Table 1] outlines the TPS reference doses correlated to the measured doses by the both (in vivo [Din vivo] and transit [Diso,Transit]) methods. Last four columns compare the agreement of delivered dose, confirmed by these two methods. In [Figure 3]a, [Figure 3]b, [Figure 3]c, [Figure 3]d, the percentage deviations of measuredin vivo and estimated mid-plane dose through transit signal as against TPS planned dose for 6 patients can be seen. The variations inin vivo measurements from these two described methods differed with TPS doses with a mean deviation in the range −4.4 ± 1.1% (min) to −0.3 ± 2.0% (max) and −4.0 ± 1.7% (min) to 1.9 ± 2.4% (max) for Din vivo and Diso,Transit, respectively. Transit dose estimates appear to give more nearer estimates than in situ doses, as not much variation due to tissue involuntary motion encountered with dosimeter placed outside.
|Table 1: Comparison of estimated transit mid-plane and in-vivo doses for treatment planning system reference dose|
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|Figure 3: (a) Percentage deviation Din vivovs Din vivo,TPSof six patients taken through in vivo measurements. (b) Mean percentage deviation of Din vivovs Din vivo,TPSof six patients taken through in vivo measurements. (c) Percentage deviation Diso-Transitvs Diso,TPSof six patients taken through transit signal. (d) Mean percentage deviation of Diso-Transitvs Diso,TPSof six patients taken through transit signal measurements|
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| Discussion|| |
It is easier to implement thein vivo dosimetry in sites with regular body contours such as the pelvis and for simple techniques not involving high-dose gradients. In a coordinated research project initiated by IAEA, the importance of exit/transit dosimetry is was highlighted, though the entrance dose measurements detect most of the human errors in treatment setup and error in the treatment equipment, but they could not account for inaccuracies taking place owing to morphological changes in the patients.
Srinivas et al., studied thein vivo dose measurements in the vaginal cavity by inserting the different detectors. An ion chamber (0.6 cc Farmer type with protective cap) in 12 cervical carcinoma patients undergoing 3DCRT treatment to the pelvic site demonstrated good agreement between planned vs prescribed dose which was within 3%.
Wertz et al. showed the feasibility to verify the actual dose measured with a small ionization chamber directly inserted in the rectum of eight patients, during the treatment for prostate with IMRT technique, and compared with TPS calculated values. In one patient, undergoing full pelvic treatment, the dose measurements in a homogeneous high-dose area resulted in a very small dose deviation between the measured and calculated doses. The mean deviation (± standard deviation) of 0.1% ± 2.1% relative to isocenter was reported in their study.
Goldenberg et al. has compared thein vivo dose (in the esophageal region) measured with an ionization chamber (the signal was corrected with the temperature of the body) with transit dose in the same patients and found it to be within 3%. In a clinical application ofin vivo dosimetry system used for transmission dosimetry, applied on 11 patients who were treated for the pelvic site, with and without bone correction done in TPS, the mean errors were between −5.20% and +2.20% for anteroposterior–posteranterior without bone correction and between −0.62% and +3.32% with bone correction. For lateral fields, the mean errors were between −10.80% and +3.46% without bone correction and between −0.55% and +3.50% with bone correction. It was brought out that the transmission method is a useful form ofin vivo dosimetry because of non-invasiveness and simplicity with no additional efforts. The above authors emphasized that if bone corrections are not applied, the variation in transmission measurement can be as much as 10%. Even without any patient involved, their dosimetry variation of output was 2% over the course of patient treatments. The algorithm used in our study takes care of the in-homogeneity corrections in TPS.
In two recent publications, dealing with 24 pelvic and 13 thorax patients undergoing 3DCRT, the role of transit dosimetry was highlighted in estimating the mid-plane doses using ionization chamber kept at EPID level. The percentage deviation in estimated doses against TPS values was −1.37% ± 2.03 and −0.73% ± 2.09, respectively. They also conducted simultaneous measurements with two ionization chambers (one kept at the mid-plane level and other one kept at EPID level) on locally fabricated pelvic and thorax phantoms: Measured/estimated values correlated well with TPS values. The mean percentage deviation of Diso,Transit with Diso,TPS and Diso,mid combined from all fields treated was 0.9 and 0.4% 2.7 and –2.6%, with the pelvic and thorax phantom, respectively.
In this study, we have reported only six patients' data. Our earlier work brought out the efficacy of on-line collection of signal during the actual treatment delivery. In our department, we treat more number of cancer cervix patients with radical treatment plans. As we knew the accuracy of our method, we wanted to correlate toin vivo dose estimates in the PTV region. Therefore, our physician co-authors felt that six patients are a sufficient number to validate the accuracy of this method. A beam therapy dosimeter based on “ion chamber measurement” gives more confidence to the inference. The measurement ofin vivo dose and estimation of mid-plane dose simultaneously by means of two ionization chambers may be possible in busy departments as a QA measure at least in protocol patients.
| Conclusion|| |
The efficacy of this transit dose estimation method is simultaneous validation of the delivered dose in real time. This will enable any corrective actions (if any) that may be applied during subsequent fraction of radiotherapy. Our presentation correlated the confidence limit on the transit dosimetry, with a simultaneous estimate of true dose “in situ” of the tumor. The transit dosimetry method can be routinely applied in clinical dosimetry because the present work has validated the estimated patient dose “in situ” simultaneously with “transit method with dosimeter outside.” As the patient does not have any detector, there is no inconvenience to the patients.
The authors would like to acknowledge all patients who participated and cooperated in this study. Authors thankfully acknowledge and appreciate the support & involvement of Mr. Prastuth and Ms. Sneha Abraham (Intern students of BSc RTT) during this study.
Financial support and sponsorship
Conflicts of interest
There are no conflicts of interest.
| References|| |
Human I, Series H. Development of procedures for in vivo
dosimetry in radiotherapy. IAEA Human Health Reports 2013;8:1-195.
Nijsten SM, Mijnheer BJ, Dekker AL, Lambin P, Minken AW. Routine individualised patient dosimetry using electronic portal imaging devices. Radiother Oncol 2007;83:65-75.
Putha SK, Saxena PU, Banerjee S, Srinivas C, Vadhiraja BM, Ravichandran R, et al
. On-line estimations of delivered radiation doses in three-dimensional conformal radiotherapy treatments of carcinoma uterine cervix patients in linear accelerator. J Med Phys 2016;41:224-33.
] [Full text]
Srinivas C, Shenoy KK, Dinesh M, Savitha KS, Kasturi DP, Supe S, et al
dosimetric study of carcinoma of uterine cervix with FBX solution in external beam therapy. J Med Phys 1999;24:47-50. [Full text]
Mans A, Wendling M, McDermott LN, Sonke JJ, Tielenburg R, Vijlbrief R, et al
. Catching errors within vivo
EPID dosimetry. Med Phys 2010;37:2638-44.
Galvin JM, Ezzell G, Eisbrauch A, Yu C, Butler B, Xiao Y, et al
. Implementing IMRT in clinical practice: A joint document of the American Society for Therapeutic Radiology and Oncology and the American Association of Physicists in Medicine. Int J Radiat Oncol Biol Phys 2004;58:1616-34.
Mijnheer B. State of the art ofin vivo
dosimetry. Radiat Prot Dosimetry 2008;131:117-22.
Low DA, Moran JM, Dempsey JF, Dong L, Oldham M. Dosimetry tools and techniques for IMRT. Med Phys 2011;38:1313-38.
Dong L, Antolak J, Salehpour M, Forster K, O'Neill L, Kendall R, et al
. Patient-specific point dose measurement for IMRT monitor unit verification. Int J Radiat Oncol Biol Phys 2003;56:867-77.
Srinivas C, Shenoy KK, Shetty J, Solomon JGR, Ravichandran R, Supe S, et al
. In vivo
dosimetry: Confirmation of dose delivery through transit dose measurements in carcinoma of uterine cervix patients undergoing teletherapy. J Med Phys 2004;29:177-78.
Mijnheer B, Georg D. Guidelines for the Verification of IMRT, ESTRO Booklet 9, Brussels: ESTRO; 2008.
Xia P, Verhey LJ. “Intensity modulated radiation therapy,” The Modern Technology of Radiation Oncology: A Compendium for Medical Physicists and Radiation Oncologists. 2nd
ed. Madison, WI: Medical Physics Publishing; 2005.
Goldenberg DB, Rao UV, Lott S, Digel J. Dosimetric considerations in cobalt 60 rotational therapy for esophageal lesions. A comparison of transit and intraluminal dose measurement. Am J Roentgenol Radium Ther Nucl Med 1969;105:518-22.
Wertz H, Boda-Heggemann J, Walter C, Dobler B, Mai S, Wenz F, et al
. Image-guidedin vivo
dosimetry for quality assurance of IMRT treatment for prostate cancer. Int J Radiat Oncol Biol Phys 2007;67:288-95.
Walter C, Boda-Heggemann J, Wertz H, Loeb I, Rahn A, Lohr F, et al
. Phantom and in-vivo
measurements of dose exposure by image-guided radiotherapy (IGRT): MV portal images vs. kV portal images vs. cone-beam CT. Radiother Oncol 2007;85:418-23.
Srinivas C, Kumar PS, Ravichandran R, Banerjee S, Saxena PU, Kumar ES, et al
. Dose verification in carcinoma of uterine cervix patients undergoing 3D conformal radiotherapy with Farmer type ion chamber. J Med Phys 2014;39:247-50. [Full text]
Piermattei A, Grimaldi L, D'Onofrio G, Cilla S, Viola P, Craus M, et al
portal dosimetry by an ionization chamber. Phys Med 2005;21:143-52.
Piermattei A, Fidanzio A, Stimato G, Azario L, Grimaldi L, D'Onofrio G, et al
dosimetry by an aSi-based EPID. Med Phys 2006;33:4414-22.
Piermattei A, Fidanzio A, Azario L, Grimaldi L, D'Onofrio G, Cilla S, et al
. Application of a practical method for the isocenter pointin vivo
dosimetry by a transit signal. Phys Med Biol 2007;52:5101-17.
Kumar PS, Banerjee S, Arun Kumar ES, Srinivas C, Vadhiraja BM, Saxena PU, et al
dose estimations through transit signal measured with thimble chamber positioned along the central axis at electronic portal imaging device level in medical linear accelerator in carcinoma of the middle-third esophagus patients undergoing three-dimensional conformal radiotherapy. J Cancer Res Ther 2018;14:300-7.
IAEA. Absorbed Dose Determination in External Beam Radiotherapy. Technical Report Series TRS 398. Vienna: International Atomic Energy Agency; 2000.
Kim BK, Chie EK, Huh SN, Lee HK, Ha SW. Clinical application ofin vivo
dosimetry system in radiotherapy of pelvis. J Radiat Prot Res 2002;27:37-49.
[Figure 1], [Figure 2], [Figure 3]