Journal List > Prog Med Phys > v.28(3) > 1098595

Prog Med Phys. 2017 Sep;28(3):92-99. English.
Published online September 30, 2017.  https://doi.org/10.14316/pmp.2017.28.3.92
Copyright © 2017 Korean Society of Medical Physics
Development of a Real-Time Internal and External Marker Based Gating System for Proton Therapy
Junsang Cho,* Wonjoong Cheon, Sanghee Ahn, Moonhee Lee, Hee Chul Park,* and Youngyih Han*
*Department of Radiation Oncology, Samsung Medical Center, SAIHST, Sungkyunkwan University School of Medicine, Seoul, Korea.
Department of Health Sciences and Technology, Samsung Advanced Institute for Health Sciences and Technology, Sungkyunkwan University, Seoul, Korea.

Corresponding author: Youngyih Han. (Email: youngyih@skku.edu ), Tel: 82-2-3410-2604, Fax: 82-2-3410-2619
Received August 24, 2017; Revised September 27, 2017; Accepted September 28, 2017.

This is an Open-Access article distributed under the terms of the Creative Commons Attribution Non-Commercial License (http://creativecommons.org/licenses/by-nc/4.0) which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited.


Abstract

In respiratory-induced proton therapy, the accuracy of tracking system and beam controlling is more important than photon therapy. Therefore, a high accuracy motion tracking system that can track internal marker and external surrogate is needed. In this research, our team has installed internal and external marker tracking system at our institution's proton therapy system, and tested the scanning with gating according to the position of marker. The results demonstrate that the developed in-house external/internal marker based gating system can be clinically used for proton therapy system for moving tumor treatment.

Keywords: Proton therapy; Respiratory gating; Internal/external fiducials; Marker tracking

Introduction

In recent years, Proton therapy become widely introduced in many hospitals because of the superiority of the protons in sparing normal tissues due to the characteristic of sharp dose fall off the Bragg-Peak.1, 2, 3) However, the drawback of the sharp dose fall off is that higher accuracy is required in the treatment than that in x-ray therapy.4, 5, 6) In the cases of tumors located in the thorax and abdomen, respiratory motion introduces uncertainties into the process of calculating the range of proton beams. Therefore, more precise gating or tracking methods are needed for proton therapy.7, 8)

In order to incorporate the organ motion into the proton treatment aiming at reduction of the motion induced uncertainty, an internal-external motion monitoring and gating system was developed. For the system, the internal marker tracking algorithm was applied to the images from the biplane flat panel detector (FPD). The external marker tracking was performed by the ‘Vicon’ (Vicon Motion Systems Ltd, U.K.) system.9) For the gating system with internal and external marker tracking, we merged each system's output data into one program, and named as ‘co-registration algorithm’.10) Through this algorithm, the proton beam could be activated when the external or internal markers were at the treatment range.

Materials and Methods

1. Internal marker tracking: biplane FPD and tracking software

The motion of an internal marker can be shown by fluoroscopic X-ray images. Our institution's proton therapy system has equipped the biplane FPD for verifying the position of the patients (Fig. 1). In this study, the FPD was used for capturing the image of internal marker with 8 frames/second in biplane direction and bypassing the images for marker tracking. The concept of finding the 3D coordinates of marker in biplane images was represented at Fig. 2. Through this concept internal marker tracking algorithm was developed. The derived 3D coordinates of internal marker were displayed on the right down of the monitor. A normal piece of clip was used for internal marker, because this was the phantom simulation.


Fig. 1
The flat panel detectors (FPD) at the gantry of our institution.
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Fig. 2
The concept of finding the 3D coordinates of marker in biplane images (The two blue rectangles represent FPD's biplane images).
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2. External surrogate tracking: the Vicon system

For the external surrogate tracking, Vicon tracking system was adopted.11) This system was used at our previous article.10) This system can find out real time 3-D coordinates of each reflective marker's position. The ‘Bonita 10’ infra-red camera (Bonita, Vicon, Los Angeles, USA) has high resolution (1024×1024 pixels) and frame rates (250 Hz) . Through the ‘Nexus’ software (Vicon Nexus, Vicon Motion Systems, Oxford Metrics Group, U.K.) every single position of each markers are captured and exported to another application (Fig. 3).


Fig. 3
The Bonita 10 camera (left) and the Nexus software (right).
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3. Integration of internal and external marker tracking data

For the real-time tracking of internal target and external surrogate, the integration of the two independent system was needed. Therefore, the internal marker's 3D coordinates and external surrogates' 3D coordinates were gathered in one PC and displayed at one window. This process was named as ‘co-registration’ system.10) For the co-registration, firstly the coordinates of the three external markers with the Vicon system were imported to the ‘co-registration computer’. Simultaneously, the internal marker data, captured with the FPD, were imported to the ‘co-registration computer’ through another TCP/IP socket, and thus, the ‘co-registration computer’ could import three external markers' coordinates data and internal marker's coordinate data simultaneously through the two TCP/IP socket. Here, every single position of one internal and three external markers can be exported to ASCII file, for further analysis. The display of monitoring of the ‘Co-registration Algorithm’ was presented (Fig. 4).


Fig. 4
The real time output status of the ‘Co-registration Algorithm’. The boxes on the left side of the monitor show the coordinates of the three external markers, and the box on the right shows the 3D coordinates of the internal marker in millimeter scale.
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The next issue was let the proton beam export when the location of the marker was within treatment range. Currently, our institution uses ‘Anzai AZ-733V external respiratory gating system’ (Anzai Medical, Tokyo, Japan) for scanning with gating treatment (Fig. 5). This system was modified to external and internal marker tracking system with adopting the developed algorithm (Fig. 6). To modify the system, some interface was made which can export the trigger signal from the ‘co-registration’ system to current treatment control system client (TCSC).


Fig. 5
Current proton therapy system at our institution.
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Fig. 6
Modified proton therapy system which is able to gate the beam based on external/internal marker's position.
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4. Phantom set-up

The experimental environment was set for scanning with gating at proton therapy room (Fig. 7). The ‘Octatvius detector 1500’ (PTW-Freiburg, Freiburg, Germany) is an air vented ionization chamber array with 1405 detectors in a 27×27 cm2 measurement area arranged in a chaeckerboard pattern with a chamber-to-chamber distance of 10 mm in each row. The Octavius detector was placed on moving phantom for simulating a patient's movement. The moving phantom was moved sliding motion with sine wave.


Fig. 7
A sliding motion phantom was placed on a couch for phantom simulation.
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For 2 liver cancer cases, the passing rate for 3%/3 mm gamma analysis were generated following the TG-119 instructions.12) The maximum energy was 172.4 MeV, and the minimum energy was 88 MeV. The Spread-out Bragg peak was used with 25 modulation layers. The snout position was 25.32 and the air gap was 16.3 cm. The gating window was opened for 10% of the total phase. Firstly, the ‘Anzai external respiratory gating system’ was used for reference, and then, the proposed system was used for gating. Finally, the gamma analysis was conducted for comparison.

Results and Discussion

The gamma analysis with anzai gating system was shown at Fig. 8. The low passing rate (89.0%) may be the effect of the moving phantom and gating mismatch. The gamma analysis with proposed gating system was shown at Fig. 9. The passing rate was 93.8% and it was a reasonable result for actual scanning with gating treatment.


Fig. 8
The gamma analysis result for case 1 with the anzai external respiratory gating.
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Fig. 9
The gamma analysis result for case 1 with the modified system's respiratory gating.
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The another case's results were shown at Fig. 10, 11. In this second case, anzai gating system showed better result. However, the proposed system was also affordable for using in gating treatment. The values of every cases were summarized at the Table 1.


Fig. 10
The gamma analysis result for case 2 with the anzai external respiratory gating.
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Fig. 11
The gamma analysis result for case 2 with the modified system's respiratory gating.
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Through these results, the scanning with gating performance was tested with our modified marker tracking system. In clinical usage, upper than 90% passing rate for 3%/3 mm gamma analysis is required. The proposed system meets the requirements and can be used for real treatment with further validation test.

In these experiments, external marker based gating was conducted. Actually, each internal/external marker based gating is available. However, the internal marker based tracking has some risk for damaging the proton therapy gantry. Therefore, we have plan for internal marker based gating experiment when spare FPD are ready (about next year). For the further study, intermittent internal marker position verification with FPD imagers, together with full-time external marker tracking is planned.

Conclusion

In this study, we developed a system that can track the internal and external marker simultaneously, and gating the proton beam according the position of the markers. The developed tracking software was interfaced to allow internal marker tracking with the images from a biplane FPD, while using the Vicon system to monitor external surrogates. With the continuous validation test, this gating system with internal and external marker tracking may be available for use in real treatment.

Notes

Conflicts of Interest:The authors have nothing to disclose.

Availability of Data and Materials:All relevant data are within the paper and its Supporting Information files.

Acknowledgements

This research was supported by the National Research Foundation of Korea (NRF) funded by The Ministry of Education (No. 2016R1A6A3A11932875) and of Science, ICT & Future Planning (Nos. 2012M3A9B6055201 and 2012R1A1A2042414) and by a grant from Samsung Medical Center (No. GFO1130081).

References
1. Pedroni E, Bacher R, Blattmann H, Böhringer HT, Coray A, Lomax A, et al. The 200 MeV proton therapy project at PSI: Conceptual design and practical realization. Med Phys 1995;22:37–53.
2. Chiba T, Tokuuye K, Matsuzaki Y, Sugahara S, Chunganji Y, Kagei K, et al. Proton beam therapy for hepatocellular carcinoma: a retrospective review of 162 patients. Clin Cancer Res 2005;11:3799–3805.
3. Chang JY, Zhang X, Wang X, Kang Y, Riley B, Bilton S, et al. Significant reduction of normal tissue dose by proton radiotherapy compared with proton radiotherapy with three-dimensional conformal or intensity modulated radiation therapy in stage I or stage III non-small cell lung cancer. Int J Radiat Oncol Biol Phys 2006;65:1087–1096.
4. Minohara S, Kanai T, Endo M, Noda K, Kanazawa M. Respiratory gated irradiat ion system for heavy-ion radiotherapy. Int J Radiat Oncol Biol Phys 2000;47:1097–1103.
5. Mori S, Chen GTY, Endo M. Effect of intrafractional motion on water equivalent path length in respiratory-gated heavy charged particle beam radiotherapy. Int J Radiat Oncol Biol Phys 2007;70:308–317.
6. Mori S, Yanagi T, Hara R, Sharp GC, Asakura H, Kumagai M, et al. Comparison of respiratory-gated and respiratory un-gated planning in scattered carbon ion treatment of the pancreas using four-dimensional computed tomography. Int J Radiat Oncol Biol Phys 2010;76:303–312.
7. Inada T, Tsujii H, Hayakawa Y, Maruhashi A, Tsujii H. Proton irradiation synchronized with respiratory cycle. Nihon Igaku Hoshasen Gakkai Zasshi 1992;52:1161–1167.
8. Kang Y, Zhang X, Chang JY, Wang H, Wei X, Liao Z, et al. 4D Proton treatment planning strategy for mobile lung tumors. Int J Radiat Oncol Biol Phys 2007;67:906–914.
9. Woolard A. In: Vicon 512 User Manual. Tustin CA: Vicon Motion Systems; 1999.
10. Cho J, Cheon W, Ahn S, Jung H, Sheen H, Park HC, et al. Development of a real-time internal and external marker tracking system for particle therapy: a phantom study using patient tumor trajectory data. J Radiat Res 2017;58:710–719.
11. Vicon Motion Systems Ltd. Bonita, UK:
12. Ezzell GA, Burmeister JW, Dogan N, LoSasso TJ, Mechalakos JG, Mihailidis D, et al. IMRT commissioning: multiple institution planning and dosimetry comparisons, a report from AAPM Task Group 119. Med Phys 2009;36:5359–5373.