Peripheral dose measurements in cervical cancer radiotherapy: a comparison of volumetric modulated arc therapy and step-and-shoot IMRT techniques
© Jia et al.; licensee BioMed Central Ltd. 2014
Received: 12 August 2013
Accepted: 13 February 2014
Published: 21 February 2014
The aim of this study was to investigate the peripheral doses resulting from volumetric modulated arc therapy (VMAT) and intensity modulated radiotherapy (IMRT) techniques in cervical cancer radiotherapy.
Nine patients with cervical cancer had treatment planned with both VMAT and IMRT. A specially designed phantom was used for this study, with ion chambers placed at interest points approximating the position of the breast, thyroid, and lens. The peripheral doses at the phantom interest points were measured and compared between the VMAT and IMRT techniques.
VMAT provides a potential dosimetric advantage compared with IMRT. The mean (± standard deviation) peripheral dose to the breast point for 1 fraction (2 Gy) during VMAT measured 5.13 ± 0.96 mGy, compared with 9.04 ± 1.50 mGy for IMRT. At the thyroid and lens interest points, the mean (± standard deviation) peripheral dose during VMAT was 2.19 ± 0.33 and 2.16 ± 0.28 mGy, compared with 7.07 ± 0.76 and 6.97 ± 0.91 mGy for IMRT, respectively. VMAT reduced the monitor units used by 28% and shortened the treatment delivery time by 54% compared with IMRT.
While the dosimetric results are similar for both techniques, VMAT results in a lower peripheral dose to the patient and reduces the monitor-unit usage and treatment delivery time compared with IMRT.
Radiotherapy is an important treatment modality for patients with cervical cancer. Over the last decade, interest in the use of intensity modulated radiotherapy (IMRT) to treat cervical cancer has been increasing. The IMRT technique has the potential benefit over conventional whole-pelvis irradiation of improving target dose coverage, reducing the volume of the organs at risk (OARs) that receive irradiation, and reducing the toxicity to normal tissue [1–4]. Despite the significant benefits of IMRT, there are some disadvantages. The technique usually requires multiple fixed-angle radiation beams, which can increase treatment delivery time. This has an impact on patient comfort, reproducibility of the treatment position, and intra-fraction motion. Moreover, IMRT uses a larger number of monitor units (MUs) compared with conventional conformal radiotherapy (CRT), leading to an increase in the amount of low-dose radiation received by the rest of the body. This raises the concern of secondary radiation-induced malignancy, which is of particular relevance to young patients or those with long future life expectancies [5–8].
A novel radiation technique, volumetric modulated arc therapy (VMAT), has recently been introduced in an attempt to overcome some of the limitations associated with fixed-field IMRT. VMAT allows continuous delivery of radiation by simultaneously varying the dose rate, the positions of the multileaf collimator, and the gantry rotation speed. Some studies demonstrate that VMAT can achieve highly conformal dose distributions, with improved target-volume coverage and sparing of normal tissues, compared with conventional radiotherapy techniques and IMRT [9–15]. VMAT also has the potential to offer additional advantages over conventional fixed-field IMRT in treatment-delivery efficiency, as a result of the reduction in both treatment delivery time and MU usage.
The peripheral dose is of clinical interest; it allows for estimation of the damage risk to those organs that are sensitive to relatively low doses of radiation. Such damage includes cataract formation in the lens of the eye and carcinogenesis, particularly in the thyroid and breast. The concept of the peripheral dose is normally associated with IMRT treatment, due to the increased number of MUs employed. Many researchers have investigated peripheral doses in IMRT [16–20].
The VMAT and IMRT techniques have been used to treat cervical cancer in clinical, yet to date, almost no data have been published that specifically address the peripheral dose generated by VMAT in patients with cervical cancer. The implementation of VMAT or IMRT in the treatment of cervical cancer raises concerns regarding the peripheral dose exposure. The purpose of this study was to investigate and compare the relative peripheral doses in VMAT and IMRT, planning both treatments in study patients and measuring peripheral doses in a specially designed phantom, using ion chambers approximating the position of the breast, thyroid, and lens tissue.
Methods and materials
Computed tomography simulation and planning objectives
Nine patients with cervical cancer, treated with the VMAT technique at our department between February 2013 and May 2013, were enrolled in this study. Ages ranged from 36 to 62 years, with a median age of 47 years. All of the patients had squamous cell carcinoma. Staging was performed according to the International Federation of Gynecology and Obstetrics (FIGO) classification. 5 patients had StageIIA and 4 patients had StageIIB cervical cancer. The studies was approved by Shengjing hospital of China Medical University's ethics committee.
All patients were immobilized in the supine position using the HipFix hip and pelvis immobilization system (CIVCO, Orange City, IA, USA). Computed tomography (CT) simulation was performed for each patient using the AQUILION 16-slice spiral CT scanner (Toshiba Medical Systems Corp., Otawara, Japan) with oral and intravenous contrast. Contiguous 3-mm slices were taken from the iliac crest to the ischial tuberosities. Each patient’s images were transported to the treatment planning system (Oncentra 4.1, Elekta AB, Stockholm, Sweden) to design the plan for VMAT. Each patient also had a plan designed for IMRT, using the same images. Two plans (VMAT and IMRT) were therefore designed for each patient, for a total of 18 treatment plans.
The gross tumor volume (GTV), clinical target volume (CTV), rectum, bladder, small bowel, and femoral heads were delineated in all patients by a single radiation oncologist. The GTV measured the volume of the primary tumor. The CTV comprised the GTV and any potential microscopic disease, including the entire uterus, parametrial tissues, the upper half of the vagina, and the regional lymph nodes in its calculation. The CTV was expanded uniformly by 8 mm in all directions to produce the planning target volume (PTV).
According to our treatment protocol, and referring to other studies [3, 14, 21], the dose prescription to the pelvis was set at 50 Gy, administered in 2 Gy fractions. Treatment plans were normalized to provide the mean dose to the PTV, in order to avoid any bias or rescaling effects in the comparison. The planning goal for both VMAT and IMRT was to obtain 95% of the prescribed dose to 98% of the PTV and not to exceed 105% as maximum dose. For the OARs including the rectum, bladder and small bowel, the dose received by 2% of the tissue volume (D2%) defined as the maximum dose was limit to 50 Gy. The complementary constraints (listed as V40Gy, the volume receiving 40 Gy of radiation) were < 40% for the rectum, < 50% for the bladder, < 25% for the small bowel, and < 5% for the femoral heads.
IMRT and VMAT planning
In IMRT planning, 7 angles were used to evenly separate coplanar fields, and “step-and-shoot” delivery was used. A collapsed-cone convolution algorithm was used to calculate dosage, with a dose grid resolution of 3 mm. In VMAT planning, a collapsed-cone convolution algorithm was adopted, using 2 full arcs of a clockwise rotation from the initial angle of 182 degrees to the end angle of 178 degrees. For optimization between the calculation time and the accuracy of treatment planning, 4 degrees was set as the spacing unit. There were a total of 180 control points, with the collimator of 45 degrees. We used the Elekta Synergy linear accelerator (Elekta AB, Stockholm, Sweden) to implement both VMAT and IMRT plans. A high-energy 6-MV photon beam was used for both techniques.
Dosimetric evaluation of VMAT and IMRT techniques
The quantitative plan evaluation was performed with a standard dose-volume histogram. For the PTV, the dose received by 98% of the tissue volume (D98%) was defined as the minimum dose, and the dose received by 2% of the tissue volume (D2%) was defined as the maximum dose. In addition, the volumes receiving at least 95% and at least 105% of the prescribed dose (V95% and V105%) were reported. Treatment homogeneity was expressed as the difference between the doses covering 5% and 95% of the PTV (D5% - D95%). The conformity index (CI90%) was defined as the ratio between the volume receiving at least 90% of the prescribed dose and the volume of the PTV. For the OARs, analysis included the mean dose, D2% and V40Gy.
Phantom and peripheral dose measurements
The phantom was then used to simulate treatment. The phantom was positioned on the treatment couch so that the center of the “pelvis” coincided with the machine isocenter, and so that the longitudinal axis of the phantom was perpendicular to the plane of gantry rotation. The ion chambers (FC65-G, IBA Dosimetry GmbH, Schwarzenbruck, Germany) were placed within the phantom at the positions meant to represent the breast, thyroid, and lens. A single fraction of 2 Gy was then delivered to the isocenter, using either the VMAT or IMRT plan, as determined for each of the 9 patients; the peripheral doses at the 3 interest points were measured using the ion chambers. The number of MUs and the treatment delivery time were recorded separately for each plan. The treatment delivery time was calculated from beam-on to beam-off, including time for radiation delivery and gantry rotation. A total of 18 measurements were made (9 VMAT plans and 9 IMRT plans).
The peripheral dose was defined, for the purposes of this study, as the radiation dose anywhere outside the treatment field; it was composed of the scatter dose and the leakage dose. The leakage dose was defined as the dose at the more distant point (i.e., the lens dose), and the scatter dose was defined as the dose difference between the closest point outside the field edge and the most distant point (i.e., breast dose minus lens dose).
The ion chambers were calibrated by the dosimetry calibration laboratory of the National Institute of Standards, using a standard 60Co beam energy. The inherent uncertainty was ± 0.27% and the reproducibility was ± 0.13%. The total uncertainty associated with our dosimeter was estimated to be within 2.0%.
The paired, 2-tailed Student’s t-test was used to compare the differences between the VMAT and IMRT techniques. Statistical analyses were conducted using Statistical Package for the Social Sciences (SPSS), version 12.0 (SPSS, Inc., Chicago, IL, USA). Statistical significance was assigned to p-values of < 0.05.
Dosimetric comparison between VMAT and IMRT plans: planned target volume and organs at risk
51.9 ± 0.5
52.2 ± 0.3
47.4 ± 1.6
48.0 ± 0.3
98.7 ± 0.8
98.7 ± 0.4
0.5 ± 0.4
1.3 ± 1.1
D5% - D95% (Gy)
3.3 ± 1.1
3.0 ± 0.3
1.5 ± 0.3
1.7 ± 0.2
37.1 ± 1.5
38.1 ± 1.7
49.5 ± 0.6
49.4 ± 0.9
39.2 ± 5.1
40.7 ± 5.1
38.1 ± 1.4
38.8 ± 1.9
50.4 ± 0.9
50.3 ± 0.5
47.3 ± 4.0
46.6 ± 5.6
28.8 ± 2.5
30.1 ± 1.4
49.5 ± 0.8
49.9 ± 0.5
20.3 ± 3.3
21.3 ± 3.5
Left femoral head
39.8 ± 1.7
40.3 ± 4.1
2.3 ± 1.4
2.9 ± 1.9
Right femoral head
39.1 ± 3.5
39.2 ± 5.0
2.5 ± 1.7
2.6 ± 1.9
Peripheral dose comparison
Comparison of peripheral dose, monitor units, and treatment delivery time
5.13 ± 0.96
9.04 ± 1.50
2.19 ± 0.33
7.07 ± 0.76
2.16 ± 0.28
6.97 ± 0.91
784.9 ± 179.2
1086.1 ± 184.6
6.12 ± 1.51
13.15 ± 0.83
In order to estimate the total dose delivered over an entire treatment course, the single fraction mean values were multiplied by 25. For the VMAT technique, the calculated total dose to the breast, thyroid, and lens points was 128, 55, and 54 mGy, respectively. These were each lower than the calculated total dose obtained with IMRT, of 226, 177, and 174 mGy, respectively. The calculated scatter dose to the breast from VMAT and IMRT was approximately 74 and 52 mGy, respectively. The scatter dose was slightly higher for VMAT than for IMRT, but the magnitude of the dose was quite small. The leakage dose from VMAT and IMRT was about 54 and 174 mGy, respectively; the leakage dose was much lower for VMAT than for IMRT.
MU and treatment delivery time comparison
The MUs and treatment delivery time associated with VMAT and IMRT are also shown in Table 2. Both measurements were lower for VMAT than for IMRT. Compared with IMRT, which used 1086 ± 185 MUs, VMAT used only 785 ± 179 MUs, a reduction of 28%. The treatment delivery time in VMAT (6.12 min) was reduced by 54% compared with IMRT (13.15 min). These differences were statistically significant (p < 0.05).
The results of the present study indicate that, although VMAT and IMRT have similar target dose coverage, VMAT has improved homogeneity and conformality, and is able to treat cervical cancer more efficiently with less damage to the small bowel. Cozzi et al.  conducted a treatment planning study comparing volumetric arc modulation and fixed-field IMRT for cervix uteri radiotherapy. Their study showed that the treatments provide the same coverage but arc therapy offers better homogeneity and conformality to the PTV. Arc therapy also reduces the mean dose to the bladder and rectum, which ranges from about 4 to 6 Gy. Cozzi et al’s results are slightly better than ours in sparing the bladder and rectum, presumably because they have extensive experience with VMAT planning. However, a discussion of the dosimetric advantage of VMAT is not the focal point of our study; we have focused on the peripheral dose resulting from VMAT in cervical cancer radiotherapy.
The peripheral dose arises primarily from scatter, generated by the patient or phantom, the machine collimators, and the walls of the room, and from leakage through the machine’s shielding and collimators. Many studies have reported the peripheral doses resulting from various radiotherapy techniques [19, 20, 22–26]. Kase et al.  measured the peripheral dose from secondary radiation outside an open treatment field. They found that the peripheral dose can be described by a simple exponential function of distance from the central axis of the radiation field for all energies and field sizes. The peripheral dose depends on the machine collimators, the field size, and the distance from the field. Machine collimator scatter contributes between 20% and 40% of the dose outside the treatment field; leakage radiation contributes very little.
Sharma et al.  reported the peripheral dose resulting from a uniform dynamic multileaf collimation (DMLC) field. They measured the different doses in a phantom that compared static open fields to those using moving strip fields of varying width, in an attempt to simulate DMLC delivery. Their study showed that all dynamic fields deliver a higher relative peripheral dose compared with the corresponding static open fields. However, peripheral doses close to the field edge can be higher for static fields than for certain DMLC comparison fields. They also carried out a feasibility study that used peripheral dose data from uniform DMLC fields to estimate out-of-field organ doses from IMRT treatment .
Mansur et al.  compared peripheral doses between IMRT and 3-dimensional CRT techniques in pediatric radiotherapy. Their study showed that IMRT delivery results in lower peripheral doses at points near the target, presumably due to reduced internal scatter from the smaller effective field size used in sliding window DMLC. Conversely, IMRT delivery results in higher doses to more distant points, presumably due to the higher MUs involved and the resulting increased head leakage. Since the magnitude of the doses at the distant points is much smaller than that seen at the closer points, the overall absolute peripheral dose is similar for both techniques.
Some researchers have pointed out that a higher peripheral dose may occur with the IMRT technique [24, 25]; others have reported a similar peripheral dose for IMRT and 3-dimensional CRT, at least in selected cases ; still others have reported a lower peripheral dose for IMRT in some cases . These discrepancies may result from the fact that VMAT is a novel radiation therapy technique. It is important to investigate the peripheral dose and the OAR dose outside the treatment field in cervical cancer radiotherapy using VMAT and to compare these results with IMRT. A little data have been reported on the peripheral doses resulting from VMAT in cervical cancer radiotherapy. Qiu Y et al. described the peripheral doses for gynecological patients undergoing IMRT or RapidArc (Varian Medical Systems, Palo Alto, CA) with kilovoltage cone beam CT . This study shows that the IMRT leakage dose is approximately 6 cGy, uniformly distributed throughout the patient’s body, while the leakage dose from RapidArc is about 3 cGy, using a prescribed dose of 45 Gy. Scatter doses from IMRT and RapidArc are similar in magnitude, reportedly about 5 cGy at the breast. Cozzi et al. also carried out a study in cervix uteri radiotherapy showing that RapidArc had a better profile than IMRT concerning peripheral doses, and RapidArc can reduce the peripheral dose from about 8% at 5 cm to about 30% at 15 cm from the PTV surface compared with IMRT. This result is in full support to our measurements.
Our phantom measurements reveal that the peripheral dose is always lower for VMAT than for IMRT, decreasing with increasing distance of measurement for both techniques. The VMAT dose at points closer to the beam edge (i.e., the breast point) is lower than the IMRT dose by about half, and the dose at more distant points (i.e., thyroid and lens points) is about a third lower. These differences can be explained by considering the 2 components of the phantom’s peripheral dose: internal scatter and accelerator head leakage. Internal scatter primarily affects tissues or organs at points closer to the beam edge and is directly proportional to the field size. Accelerator head leakage affects the entire body equally and is directly proportional to the MUs employed.
In the VMAT technique, continuous delivery is achieved by simultaneously varying the dose rate, the positions of the multileaf collimator, and the gantry rotation speed. Compared with IMRT, VMAT reduces MU usage and treatment delivery time, and the modulated beam has a relatively large field size. This means that the leakage contribution to the peripheral dose becomes quite small and the peripheral dose at distant points is lower. While the scatter contribution to the peripheral dose becomes larger, the peripheral dose at points closer to the beam edge increases. The leakage dose and scatter dose contribute approximately 42% and 58%, respectively, of the total peripheral dose from VMAT.
With the IMRT technique, “step-and-shoot” delivery is administered at different gantry angles. Compared with VMAT, IMRT increases both the MU usage and treatment delivery time, and the modulated beam has a relatively small field size. This means that the leakage contribution to the peripheral dose becomes quite large and the peripheral dose at distant points is higher. While the scatter contribution to the peripheral dose becomes relatively small, the peripheral dose at points closer to the beam edge decreases. The leakage dose and scatter dose contribute approximately 77% and 23%, respectively, of the total peripheral dose from IMRT.
Our study found that the scatter dose predominates in the peripheral dose in VMAT, while the leakage dose predominates in IMRT. Our scatter doses to the breast from both VMAT and IMRT are similar to those reported by Qiu et al. , but our leakage doses are larger. The difference possibly results from the use of different study methods and prescribed doses.
Knowledge of the peripheral dose resulting from VMAT and IMRT techniques in cervical cancer radiotherapy is important and of clinical interest. Physicians must be able to estimate the dose to the non-treated organs and the resultant risk to patients. An understanding of the peripheral dose allows a more complete assessment of the radiation dose to long-term survivors.
The VMAT technique is able to treat cervical cancer more efficiently than the IMRT technique. VMAT provides a potential dosimetric advantage, results in a lower peripheral dose to the patient, and reduces the MU usage and treatment delivery time.
Written informed consent was obtained from the patient for the publication of this report and any accompanying images.
- Georg P, Georg D, Hillbrand M, Kirisits C, Poetter R: Factors influencing bowel sparing in intensity modulated whole pelvic radiotherapy for gynaecological malignancies. Radiother Oncol. 2006, 80: 19-26. 10.1016/j.radonc.2006.04.014.View ArticlePubMedGoogle Scholar
- Portelance L, Chao C, Grisby P, Benner H, Low D: Intensity modulated radiation therapy(IMRT) reduces small bowel, rectum and bladder doses in patients with cervical cancer receiving pelvic and para-aortic irradiation. Int J Radiat Oncol Biol Phys. 2001, 51: 261-266.View ArticlePubMedGoogle Scholar
- Mundt A, Lujan A, Rotmensch J, Waggner S, Yamada D, Fleming G, et al: Intensity modulated whole pelvic radiotherapy in women with gynaecologic malignancies. Int J Radiat Oncol Biol Phys. 2002, 52: 1330-1337. 10.1016/S0360-3016(01)02785-7.View ArticlePubMedGoogle Scholar
- Roeske J, Lujan A, Rotmensch J, Waggner S, Yamada D, Mundt A: Intensity modulated whole pelvic radiation therapy in patients with gynaecologic malignancies. Int J Radiat Oncol Biol Phys. 2000, 48: 1613-1621. 10.1016/S0360-3016(00)00771-9.View ArticlePubMedGoogle Scholar
- Sharma SD, Upreti RR, Laskar S, et al: Estimation of risk of radiation-induced carcinogenesis in adolescents with nasopharyngeal cancer treated using sliding window IMRT. Radiother Oncol. 2008, 86: 177-181. 10.1016/j.radonc.2007.11.019.View ArticlePubMedGoogle Scholar
- Hall EJ, Wuu CS: Radiation-induced second cancers: the impact of 3D-CRT and IMRT. Int J Radiat Oncol Biol Phys. 2003, 56: 83-88. 10.1016/S0360-3016(03)00073-7.View ArticlePubMedGoogle Scholar
- Verellen D, Vanhavere F: Risk assessment of radiation induced malignancies based on whole-body equivalent dose estimates for IMRT treatment in the head and neck region. Radiother Oncol. 1999, 53: 199-203. 10.1016/S0167-8140(99)00079-1.View ArticlePubMedGoogle Scholar
- Ruben JD, Davis S, Evans C, Jones P, Gagliardi F, Harnes M, Hunter A: The effect of intensity-modulated radiotherapy on radiation-induced second malignancies. Int J Radiat Oncol Biol Phys. 2008, 70: 1530-1536. 10.1016/j.ijrobp.2007.08.046.View ArticlePubMedGoogle Scholar
- Vanetti E, Clivio A, Nicolini G, Fogliata A, Ghosh-Laskar S, Agarwal JP, et al: Volumetric modulated arc radiotherapy for carcinomas of the oro-pharynx, hypo-pharynx and larynx: a treatment planning comparison with fixed field IMRT. Radiother Oncol. 2009, 92: 111-117. 10.1016/j.radonc.2008.12.008.View ArticlePubMedGoogle Scholar
- Lu SH, Cheng CH, Kuo SH, et al: Volumetric modulated arc therapy for nasopharyngeal carcinoma: a dosimetric comparison with TomoTherapy and step-and-shoot IMRT. Radiother Oncol. 2012, 104: 324-330. 10.1016/j.radonc.2011.11.017.View ArticlePubMedGoogle Scholar
- McGrath SD, Matuszak MM, Yan D, Kestin LL, Martinez AA, Grills IS: Volumetric modulated arc therap for delivery of hypofractionated stereotactic lung radiotherapy: a dosimetric and treatment efficiency analysis. Radiother Oncol. 2010, 97: 437-442. 10.1016/j.radonc.2010.09.027.View ArticleGoogle Scholar
- Palma D, Vollans E, James K, Nakano S, Moiseenko V, Shaffer R, et al: Volumetric modulated arc therapy for delivery of prostate radiotherapy: comparison with intensity-modulated radiotherapy and three-dimensional conformal radiotherapy. Int J Radiat Oncol Biol Phys. 2008, 72: 996-1001. 10.1016/j.ijrobp.2008.02.047.View ArticlePubMedGoogle Scholar
- Zhang P, Happersett L, Hunt M, Jackson A, Zelefsky M, Mageras G: Volumetric modulated arc therapy: planning and evaluation for prostate cancer cases. Int J Radiat Oncol Biol Phys. 2010, 76: 1456-1462. 10.1016/j.ijrobp.2009.03.033.View ArticlePubMedGoogle Scholar
- Cozzi L, Dinshaw KA, Shrivastava SK, et al: A treatment planning study comparing volumetric arc modulation with RapidArc and fixed field IMRT for cervix uteri radiotherapy. Radiother Oncol. 2008, 89: 180-191. 10.1016/j.radonc.2008.06.013.View ArticlePubMedGoogle Scholar
- Aznar MC, Petersen PM, Logadottir A, et al: Rotational radiotherapy for prostate cancer in clinical practice. Radiother Oncol. 2010, 97: 480-484. 10.1016/j.radonc.2010.09.014.View ArticlePubMedGoogle Scholar
- Mutic S, Klein EE: A reduction in the AAPM TG-36 reported peripheral dose distributions with tertiary multileaf collimation. American Association of Physicists in Medicine Task Group 36. Int J Radiat Oncol Biol Phys. 1999, 44: 947-953. 10.1016/S0360-3016(99)00092-9.View ArticlePubMedGoogle Scholar
- Stern RL: Peripheral dose from a linear accelerator equipped with multileaf collimation. Med Phys. 1999, 26: 559-563. 10.1118/1.598557.View ArticlePubMedGoogle Scholar
- Eric EK, Beth M, Roy W, David M: Peripheral doses from pediatric IMRT. Med Phys. 2006, 33 (7): 2525-2531. 10.1118/1.2207252.View ArticleGoogle Scholar
- Mansur DB, Klein EE, Maserang BP: Measured peripheral dose in pediatric radiation therapy: a comparison of intensity-modulated and conformal techniques. Radiother Oncol. 2007, 82: 179-184. 10.1016/j.radonc.2007.01.002.View ArticlePubMedGoogle Scholar
- Shamurailatpam DS, Ritu RU, Deepak DD: Use of peripheral dose data from uniform dynamic multileaf collimation fields to estimate out-of-field organ dose in patients treated employing sliding window intensity-modulated radiotherapy. Phys Med Biol. 2006, 51: 2987-2995. 10.1088/0031-9155/51/11/020.View ArticleGoogle Scholar
- Vrdoljak E, Prskalo T, Omrcen T, Situm K, Boraska T, Frleta I, et al: Concomitant chemobrachyradiotherapy with ifosfamide and cisplatin followed by consolidation chemotherapy in locally advanced squamous cell carcinoma of the uterine cervix. Results of a phase IIstudy. Int J Radiat Oncol Biol Phys. 2005, 61: 824-829. 10.1016/j.ijrobp.2004.06.248.View ArticlePubMedGoogle Scholar
- Kase KR, Svensson GK, Wolbarst AB, et al: Measurements of dose from secondary radiation outside a treatment field. Int J Radiat Oncol Biol Phys. 1983, 9: 1177-1183. 10.1016/0360-3016(83)90177-3.View ArticlePubMedGoogle Scholar
- Sharma DS, Deshpande SS, Animesh, et al: Peripheral dose from uniform dynamic multileaf collimation fields: implications for sliding window intensity modulated radiotherapy. Br J Radiol. 2006, 79: 331-335. 10.1259/bjr/16208090.View ArticlePubMedGoogle Scholar
- Followill D, Geis P, Boyer A: Estimates of whole-body dose equivalent produced by beam intensity modulated conformal therapy. Int J Radiat Oncol Biol Phys. 1997, 38: 667-672. 10.1016/S0360-3016(97)00012-6.View ArticlePubMedGoogle Scholar
- Hall EJ: Intensity modulated radiation therapy, protons, and the risk of second cancer. Int J Radiat Oncol Biol Phys. 2006, 65: 1-7.View ArticlePubMedGoogle Scholar
- Aoyama H, Westerly DC, Mackie TR, et al: Integral radiation dose to normal structures with conformal external beam radiation. Int J Radiat Oncol Biol Phys. 2006, 64: 962-967. 10.1016/j.ijrobp.2005.11.005.View ArticlePubMedGoogle Scholar
- SaIz H, Eichner R, Wiezorek T: Doses IMRT increase the peripheral radiation dose? A comparison of treatment plans 2000 and 2010. Z Med Phys. 2012, 22: 6-12. 10.1016/j.zemedi.2011.03.004.View ArticleGoogle Scholar
- Qiu Y, Moiseenko V, Aquino-Parsons C, et al: Equivalent doses for gynecological patients undergoing IMRT and RapidArc with kilovoltage cone beam CT. Radiother Oncol. 2012, 104: 257-262. 10.1016/j.radonc.2012.07.007.View ArticlePubMedGoogle Scholar
This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly credited.