Abstract
Keywords
1. Introduction
- Valentin J.
Honderden vrouwen onjuist bestraald in Maastricht. 2014 [cited 2018 13/11/2018]; Available from: https://www.rtlnieuws.nl/node/1807366.
Radiation equipment may not have correctly targeted cervical cancer in 25 patients. 2019 04/06/2019]; Available from: https://www.cbc.ca/news/canada/hamilton/radiation-equipment-juravinski-cancer-centre-1.4964780.
- Tanderup K.
- Beddar S.
- Andersen C.E.
- Kertzscher G.
- Cygler J.E.
2. Materials and methods
3. Deviations between delivery and treatment plan and their impact on dose and local tumor control
3.1 Deviations between delivery and treatment plan in brachytherapy
3.2 Impact of source position deviations
3.3 Detection sensitivity and false alarms
4. Methods for IVD

4.1 Time-integrated point/multipoint dosimetry
- Tanderup K.
- Beddar S.
- Andersen C.E.
- Kertzscher G.
- Cygler J.E.
4.2 Time-resolved point/multipoint dosimetry
- Smith R.L.
- Taylor M.L.
- McDermott L.N.
- Haworth A.
- Millar J.L.
- Franich R.D.
- Smith R.L.
- Taylor M.L.
- McDermott L.N.
- Haworth A.
- Millar J.L.
- Franich R.D.
- Espinoza A.
- Beeksma B.
- Petasecca M.
- Fuduli I.
- Porumb C.
- Cutajar D.
- et al.
- Watanabe Y.
- Muraishi H.
- Takei H.
- Hara H.
- Terazaki T.
- Shuto N.
- et al.
Year Authors [citation] | Detector | Geometry | Level of source tracking | Spatial resolution | Timing resolution | Additional info |
---|---|---|---|---|---|---|
2001 Duan et al. [81] | Film-pinhole camera | Polystyrene phantom | x, y, z for each dwell position | Dwell separations of 1 mm can be distinguished | None | Post treatment analysis |
2005 Nakano et al. [82] | One diamond detector on the skin | Anthropomorphic phantom | x, y, z for each dwell | 2.5 mm or 2% | None | Twelve measurements were performed with a single detector at 12 positions to simulate 12 detectors |
2010 Batic et al. [83] | Two pinhole detectors, 2 Si-pads for each pinhole | Air phantom with 2 needles | x, y, z for each dwell | 4.6 mm absolute, 2.8 mm relative | None | Focus on relative position between 2 positions inside a catheter |
2013 Smith et al. [28]
Source position verification and dosimetry in HDR brachytherapy using an EPID. Med Phys. 2013; 40111706https://doi.org/10.1118/1.4823758 | Flat panel | Solid water phantom | x, y, z for each dwell | <1.0 mm in the plane and 2.0 mm for the distance to the source | 0.1 s | Focus on a 4D measurement system and characterization of an EPID panel |
2013 Therriault-Proulx et al. [34]
On the use of a single-fiber multipoint plastic scintillation detector for 192Ir high-dose-rate brachytherapy. Med Phys. 2013; 40062101https://doi.org/10.1118/1.4803510 | Three plastic scintillators on a single fiber | Water phantom | z position only (along the catheter) | 0.3 mm | 3.0 s | The integration time was defined as a good trade-off between precision and temporal resolution |
2013 Espinoza et al. [30]
The feasibility study and characterization of a two-dimensional diode array in “magic phantom” for high dose rate brachytherapy quality assurance. Med Phys. 2013; 40111702https://doi.org/10.1118/1.4822736 | 11 × 11 Si diodes | Magic phantom: 3 × 30 × 30 cm solid water | x, y, z for each dwell | <0.5 mm for 75% of the positions | 0.001 s | They focus on a 4D measurement system that can also measure transit time |
2014 Kertzscher et al. [59]
Adaptive error detection for HDR/PDR brachytherapy: guidance for decision making during real-time in vivo point dosimetry. Med Phys. 2014; 41052102https://doi.org/10.1118/1.4870438 | Inorganic scintillators (Al2O3:C) | Simulation | Dosimeter position (x,y,z) | <0.8 mm | 1.0 s | The aim is to continuously update the position of the detector throughout a treatment based on the measured dose rates |
2014 Wang et al. [35] | Two inorganic scintillators (GaN) | PMMA cylinder phantom | x-position only (along the catheter) | <1.0 mm | 0.1 s | The study aimed to find a method for pretreatment Q |
2015 Safavi-Naeini et al. [40] | BrachyView prototype. Two 14 × 14-mm TimePix detectors in a specially designed probe with 6 cone pinholes | Plastic water | x, y, z for each dwell | <1.0 mm | None | Authors mention that they are developing a 4-detector system integrated with an ultrasound probe. The detector can acquire up to 400 fps, but dwell times larger than 0.5 s are preferable to reduce noise |
2016 Guiral et al. [26] | Four inorganic scintillators (GaN) | Plastic cylinder for QA and water phantom for probe | z for each dwell | <1.0 mm | 0.1 s | There were 2 systems: an expanded version of the QA phantom from Ref. [9] and a specially designed applicator |
2017 Fonseca et al. [38] | Flat panel | PMMA plate | x, y, and interdwell distance for each dwell | 0.2 mm | 0.1 s | Technique for commissioning of applicators using source tracking |
2017 Fonseca et al. [29] | Flat panel | Water phantom | x, y, z for each dwell | 0.2 mm for x and y. 0.6 mm for z | 0.1 s | Technique for pretreatment verification |
2018 Watanabe et al. [31]
Automated source tracking with a pinhole imaging system during high-dose-rate brachytherapy treatment. Phys Med Biol. 2018; 63145002https://doi.org/10.1088/1361-6560/aacdc9 | Pinhole camera with 2 holes; a scintillator plate and a CCD camera | Water phantom | x, y, z for each dwell | 0.7 mm | 2.0 s | The pixel intensity is directly proportional to the dwell time and could allow measurements with higher resolution than the shutter speed |
- Point detector: The measured dose rate by a point detector can be transformed into a distance between source and detector by using TG43 [32,33]. By adding the information from dose rate measurements at multiple positions, triangulation can be used to determine the actual position of the source or source catheter relative to the detector(s) [26,34,
- Therriault-Proulx F.
- Beddar S.
- Beaulieu L.
On the use of a single-fiber multipoint plastic scintillation detector for 192Ir high-dose-rate brachytherapy.Med Phys. 2013; 40062101https://doi.org/10.1118/1.480351035,36]. - Flat panel detector: The panel is placed close to the patient (e.g. in the treatment couch underneath the patient) so that it detects photons leaving the patient’s body. The panel response can be approximated by mathematical functions used to define the dwell positions [28,
- Smith R.L.
- Taylor M.L.
- McDermott L.N.
- Haworth A.
- Millar J.L.
- Franich R.D.
Source position verification and dosimetry in HDR brachytherapy using an EPID.Med Phys. 2013; 40111706https://doi.org/10.1118/1.482375829,37]. Panels are available with up to ≈0.1 mm spatial resolution and acquisition rates of more than 100 frames per second (fps). However, high acquisition rates usually limit the detection area and/or require pixel binning (combination of the response of adjacent pixels). An advantage of flat panel detectors is that they can be used for commissioning of brachytherapy applicators [[38]] and for imaging of the patient anatomy, which enables measurements relative to the anatomy [37,39].- Fonseca G.
- Podesta M.
- Reniers B.
- Verhaegen F.
MO-AB-BRA-03: development of novel real time in vivo EPID treatment verification for brachytherapy.Med Phys. 2016; 43 (3691-3691)https://doi.org/10.1118/1.4957155 - Slit cameras: A collimator is placed in front of a radiation detector. The collimator consists of a high-density plate, normally made of tungsten, with small holes at a fixed distance from each other. The radiation passes through the apertures and generates spots on high-resolution detectors. These can be pixelated Si-detectors [[40]] or charge-coupled device cameras [[31]].
- Watanabe Y.
- Muraishi H.
- Takei H.
- Hara H.
- Terazaki T.
- Shuto N.
- et al.
Automated source tracking with a pinhole imaging system during high-dose-rate brachytherapy treatment.Phys Med Biol. 2018; 63145002https://doi.org/10.1088/1361-6560/aacdc9

4.3 Clinical studies
- Anagnostopoulos G.
- Baltas D.
- Geretschlaeger A.
- Martin T.
- Papagiannis P.
- Tselis N.
- et al.
- Sharma R.
- Jursinic P.A.
Year | Site | Detector | No. Treated | MD | Additional info |
---|---|---|---|---|---|
2017 Wagner et al. [55] | PR | Alanine/ESR | 15 | ≈100.0% | Alanine strands were inserted into a Foley catheter. Needles and detector positions were measured using ultrasound images. The detector volume could not be clearly defined in some of the cases. Reported uncertainty 5.0% |
2017 Carrara et al. [47] | GYN | MOSkin | 26 | <14.0% | Dosimeters placed on top of the rectal probe. Large differences (>36.0%) were traced to a longitudinal probe displacement and not included in the analysis. Deviation between planned and measured doses increased with increasing time between imaging and treatment. Reported uncertainty 6.2% (k = 1 – MOSkin) and 7.1% (k = 1 – TPS). |
2017 Jaselske et al. [41] | HN, BR | TLD | >6 | ≈22.0% | Dosimeters inserted into catheters/needles. Reported an increased difference in every subsequent fraction. Reported uncertainty 17.9%. |
2017 Van Gellekom et al. [84] | GYN | MOSFET | 50 | >14.0% | Dosimeters inserted into a Fletcher or MUPIT applicator. Additional imaging should be performed for measured differences larger than 10.0%. Overall reported uncertainty 9.0% (k = 2). |
2018 Smith et al. [37] | *PR | Flat panel | 2 | 4.9 mm | EPID positioned under the patient couch used for imaging (additional X-ray source) and source tracking in 2D. Reported uncertainty 2.2 mm |
2018 Johansen et al. [36] | *PR | Opt. fiber (Al2O3:C) | 20 | ≈ 16.9% | Dosimeters inserted into catheters/needles. Time-resolved measurements. MR scans acquired just before and after the treatment. Reported uncertainty 5.0% (k = 1) |
2018 Melchert et al. [46] | BR, TH, HN | MOSFET | 12 | ≈ 56.0% | Dosimeters inserted into catheters/needles. A long interval between needle implantation and imaging can reduce positioning uncertainties due to edema. Reported uncertainty 4.0% (detector response) ± 1 mm positioning. |
2018 Belley et al. [85] | *GYN | Opt. fiber/TLD | 30 | < 20.0% | Dosimeters at the surface of a vaginal cylinder. Real-time dose rate monitoring. Reported uncertainty 13.9% (k = 2). |
2019 Jamalludin et al. [86] | SK | MOSkin | 5 | 24.0% (target) 32.0% (OAR) | MOSkin was placed between the arm and the chest of the patient (HDR Cobalt-60). The tumor was located at the medial aspect of the right arm. Differences were attributed to backscattering from lead shielding and TPS inaccuracies near the patient surface (TG43-based dose calculation). Reported uncertainty 8.4% (k = 1). |
2020 Jamalludin et al. [87] | GYN | MOSkin/diode | 48 | greater than 37.0% | MOSkin attached to diode during 18 sessions (HDR Cobalt-60). Doses measured with MOSkin were higher than planned for 44.0% of the cases, while doses measured with diodes were lower than planned for all the treatments. Reported uncertainty 5.2% (k = 1) and 6.6% (k = 1) for the detector and TPS, respectively. |
5. Requirements and future directions for research, development, and clinical practice
5.1 Estimates of required uncertainty limits
- Source tracking uncertainty: The uncertainty (1SD) of the detector system including post-processing (Section 5, items 2 and 4).
- Clinical threshold: A threshold level for a deviation to be considered of clinical relevance. For instance, if a 5 mm or 10 mm deviation in a source position is considered important for the quality of the treatment, these would be used as the clinical thresholds.
- Action level: The action level is the threshold at which an alarm should be set to indicate when a given deviation exceeds the threshold. Ideally, the action level should be equal to the clinical threshold, but the uncertainty from the detector might require a different action level, as will be described below.
- Sensitivity: The sensitivity is defined as the fraction of detected events occurring beyond a given clinical threshold. For example, if the clinical threshold is 10 mm and the system can identify 90% of 10 mm deviations, the sensitivity is 90%.
- False alarms: A false alarm is a measurement that is beyond the action level but for which the clinical threshold has not been reached. For example, 2 mm offsets are frequent deviations between delivery and treatment plan, but offsets of this magnitude normally have minor clinical impact. If, for instance, 10% of the 2 mm deviations trigger an alarm, the incidence of false alarms at 2 mm is 10%.

5.1.1 Point detector system uncertainty for source tracking
where is the relative dosimetric deviation and the geometric deviation [

5.1.2 Position of the detector for source tracking
- Kertzscher G.
- Andersen C.E.
- Tanderup K.
- Verhaegen F.
- Palefsky S.
- Rempel D.
- Poon E.
5.1.3 Dwell time measurements
5.1.4 Accuracy of current detector systems
5.2 Software and hardware integration
5.2.1 Integration with the brachytherapy afterloader
5.2.2 Integration with the TPS
- Shen C.
- Gonzalez Y.
- Klages P.
- Qin N.
- Jung H.
- Chen L.
- et al.
5.3 Resources and staffing
6. Discussion
6.1 Imaging
6.2 Electromagnetic tracking
- Damato A.L.
- Viswanathan A.N.
- Don S.M.
- Hansen J.L.
- Cormack R.A.
- Kallis K.
- Kreppner S.
- Lotter M.
- Fietkau R.
- Strnad V.
- Bert C.
6.3 Perspectives for clinical use of IVD
The Patient Safety in Radiotherapy Steering Group and Public Health England. 14/12/2019]; Available from: https://www.gov.uk/government/publications/radiotherapy-errors-and-near-misses-data-report.
Declaration of Competing Interest
Acknowledgments
Appendix A. Supplementary data
- Supplementary data 1
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☆During the 1st ESTRO Physics Workshop celebrated in November 2017 in Glasgow, Scotland, a task group was created to stimulate the wider adoption of in vivo dosimetry for radiotherapy. The members of this task group, authors of this report, were selected on the basis of their expertise to contribute relevant input to the area of study and their long-term experience in the clinical implementation of in vivo dosimetry systems.
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