Upstate New York Association of Physicists in Medicine, Inc.
(A Chapter of the AAPM)
Spring Meeting – Thursday May 22, 2008
TWIG Auditorium, Rochester General Hospital,

1425 Portland Ave, Rochester, NY 14621

 

Major Meeting Sponsor: Elekta Inc.

 

12:00 pm – 5:00 pm    Sponsoring Vendor Exhibits:

 

Elekta Inc.                                                                     North American Scientific

Impac Medical Systems                                                       Upstate Linac Services, LLC

Tomotherapy Inc                                                            Sun Nuclear

Aktina, Inc

                                               

10:30 AM-11:30 AM    Business Meeting

12:00              Lunch   Sponsored by North American Scientific

 

12:30              Refreshment and Vendor Exhibit – Sengupta Room

Sponsored by Sun Nuclear

 

1:00

Meeting Introduction

Shivaji Deore

UNYAPM President

Vendor Session

1:05

EPID for Absolute Dose Based IMRT QA”

James Ernsberger, Sun Nuclear

1:20

Discussion of Volumetric Modulated Arc Therapy

Ed Hahn, Elekta, Inc.

Proffered Paper Session

1:35

A Genetic Algorithm and Distributed-Computing Approach to Beam Angle Optimization in IMRT

Daryl P. Nazareth1, Stephen T. Brunner2,  Matthew D. Jones3, Matthew B. Podgorsak1, Michael R. Kuettel1

1:50

Beam Weight and Angle Optimization in Radiation Therapy using Coupled Monte Carlo and Genetic Algorithm Codes

M Bakhtiari1, M D Jones2, H K Malhotra1, M B Podgorsak1, and D Nazareth.

2:05

Computer-aided detection of metastatic brain tumors using automated 3-D template matching

R. Ambrosini1,P. Wang2, B. Kolar3, W. O’Dell1

2:20

The Solid-State X-Ray Image Intensifier (SSXII): The Next Generation of X-Ray Imagers

Andrew Kuhls-Gilcrist, Amit Jain, Daniel R Bednarek, Stephen Rudin,

2:35

Estimating Effective Dose in Radiostereometric Analysis of the Lumbar Spine

Kerry Greene-Donnelly, Kent Ogden, Nat Ordway, Jerry Calabrese, Marsha Roskopf

2:50

Refreshment , Vendor Exhibits and Poster Viewing* – Sengupta Room Sponsored by

                                                  Sun Nuclear,

3:20

An IMRT planning method for limiting spinal cord to tolerable levels with unintended field overlaps at the supra-clavicular junction plane of head and neck radiotherapy

Steven de Boer,  Osama Hassad*,  Wainwright Jaggernauth

3:35

A Guidance System for Optical Patient Alignment during breast radiotherapy

Jonathan Schmitta, Kenneth Hoffmanb, Mohammad Bakhtiaria, Harish Malhotraa, Daryl Nazaretha

                                                          Invited Speaker Sessions

3:50

Experience in Development of clinical SBRT Program

Harish K Malhotra,

Roswell Park Cancer Institute, Bufflao,NY

4:10

The Past, Present, and Future in Medical Physics

Prof. Jake Van Dyk

University of Western Ontario

London, Ontario, Canada

4:50

Frederick Faw Memorial Award Presentation

Dan Bednarek & Steve de Boer

 

     

                       

*Poster Presentations:

     1.  Accuracy in the dose delivery of IMRT as a function of Gantry and Collimator Angles,

         Jubei Liu, Zhou Wang, Matthew B. Podgorsak, Steven F. de Boer, Lalith Kumaraswamy,          

         Harish Malhotra, Department of Radiation Medicine, Roswell Park Cancer Institute, Elm & Carlton      

         Streets, Buffalo, NY 14263

 

   2.  Dosimetric Analysis of the Effect of Tungsten Shields in a Fletcher-suit Delclos Applicator in High-         

        Dose-Rate brachytherapy using Gafchromic Film,

        Thomas R. Stanley, Mohammad Bakhtiari, M B,Podgorsak, Wainwright Jaggernauth &       

        Malhotra HK, Roswell Park Cancer Institute, Buffalo, NY 14263.

 

     ADJOURN

 

 

Driving Directions to Rochester General Hospital:

 

Directions (to Rochester General Hospital):

 

From the West:  New York State Thruway to Exit 47.  490 East to 390 North to 104 (Ridge Road) East to Carter Street exit.  Follow service road to Hospital entrance.  Parking is available in the Ramp Garage.

 

From Rochester Airport (ROC):  390 North to 104 (Ridge Road) East to Carter Street exit.  Follow service road to Hospital entrance.  Parking is available in the Ramp Garage.

 

From the East:  New York State Thruway to Exit 45. 490 West to 590 North to 104 West to Goodman Street/Portland Avenue exit. Follow service road to Portland Avenue and turn left. Hospital is on the right. Parking is available in the Ramp Garage.

 

From the South:  390 North to 590 North to 104 West to Goodman Street/Portland Avenue exit. Follow service road to Portland Avenue and turn left. Hospital is on the right. Parking is available in the Ramp Garage.

 

 

Parking is available on 3rd and 4th floors. After parking, please take Elevator to Hospital Main Entrance. The TWIG auditorium is located right after front desk.

 

  

                                               

 

UNYAPM SPRING MEETING PROCEEDINGS

Rochester General Hospital, Rochester, NY

May 22, 2008

 

EPID for Absolute Dose Based IMRT QA

Benjamin Nelms, James Ernsberger

Sun Nuclear Corporation, Melbourne FL

 

The Electronic Portal Imaging Device (EPID) has become a common linac accessory, and there is great interest in the adoption of the Mega-voltage (MV) EPID for use in routine IMRT QA.  There are several benefits to this technology, most particularly: high data density, good resolution (small pixels), large area, and workflow efficiency (online and electronic).  However, the EPID is not a dosimeter, it is essentially a camera, and it is paramount to keep IMRT QA in a “dose-based” strategy. In order to fully audit both the delivery system and the TPS calculation, a measured absolute dose plane must be compared with a TPS calculated absolute dose plane (i.e. image-to-predicted image strategies do not audit fully the TPS calculation). EPIDoseTM, part of the MapCHECKTM suite of QA tools, was recently commercialized, making it possible to convert, via an algorithm, EPID images into QA absolute dose planes. The EPIDose model is commissioned vs. absolute dose diode array planes, and then used thereafter for comparison directly with TPS calculated planar dose fields.  The EPIDose solution is highly efficient, planning system independent, allows calculation accuracy to be verified by a trusted dosimetry standard and no part of the planning delivery system is left out of the QA routine. In this presentation, clinical IMRT plans will be presented illustrating the accuracy and power of EPIDose.

__________________________________________________________________________________________________________________________________________________________________________

 

Discussion of Volumetric Modulated Arc Therapy

Ed Hahn, Elekta, Inc.

 

Volumetric Modulated Arc Therapy (VMAT) technology provides a simultaneous control of the linear accelerator gantry position and speed, the leaves and angle of the multileaf collimator and dose rate. This flexibility enables highly conformal cancer treatments, as well as optimal sparing of the healthy tissue around the target. In addition, VMAT significantly reduces patient treatment times, leading to greater patient comfort and stillness for a more efficient and precise treatment.

 

The clinical benefits of VMAT that are seen by our customers who are utilizing this technology with CE Designation in Europe are as follows: Smooth automatic delivery in one automatic sequence, fast, accurate and efficient beam delivery, optimal tumor conformity, increased patient through put, reduced interplane dose and the ability for treatment of pediatric tumors.

 

With VMAT from Elekta, customers are able to utilize non-coplanar techniques (up to 12 degrees) as we have the smallest Linac head diameter.  By being able to kick the table this further improves conformity to PTV and reduces dose to critical structures.

 

As Elekta has been working on this technology (beginning with Intensity Modulated Arc Therapy, IMAT) for ten years and holds the patent on multiple arc delivery.  This enables the option deliver with more than one arc.  Complicated head and neck IMRT plans may have much better plans if the first arc rotated around the table at 0 degrees, and then rotated back with the table shifted at a 10 degree angle.

 

*Elekta Volumetric Intensity Modulated Arc Therapy (VMAT) is pending regulatory approvals in certain markets, including 510(k) clearance in the US, and is not yet available for commercial sale in the US.

 

__________________________________________________________________________________________________________________________________________________________________________

 

A Genetic Algorithm and Distributed-Computing Approach to Beam Angle Optimization in IMRT

Daryl P. Nazareth1, Stephen T. Brunner2, Matthew D. Jones3, Matthew B. Podgorsak1, Michael R. Kuettel1

1Roswell Park Cancer Institute, Buffalo NY, 2Carnegie Mellon University, Pittsburgh, PA

3University at Buffalo, Buffalo NY

 

Purpose: IMRT treatment planning involves the selection of gantry angles, as well as the specification of structures and constraints employed in the optimization process.  Including these angles in the combinatorial search space vastly increases the computational burden, and therefore the gantry angle selection is normally performed manually by a clinician, based on clinical experience.  We have investigated the use of a genetic algorithm (GA) and distributed-computing platform to optimize the gantry angle parameters and to provide insight into additional structures which may be necessary in the dose optimization process to produce optimal IMRT treatment plans.

 

Method and Materials: For an IMRT prostate patient, we produced the first generation of 40 samples, each of five gantry angles, by selecting from a uniform random distribution, subject to certain adjacency and opposition constraints.  The dose optimization was performed by distributing the forty-plan workload over several machines running a commercial treatment planning system.  A score was assigned to each resulting plan, based on how well it satisfied clinically-relevant constraints.  The second generation of 40 samples was produced by combining the highest-scoring samples using the techniques of crossover and mutation.  The process was repeated until the sixth generation, and the results compared with a clinical (equally-spaced) gantry angle configuration

 

Results: In the sixth generation, 34 of the 40 GA samples achieved better scores than the clinical plan, with the best plan showing an improvement of 84%.  Moreover, the resulting configuration of beam angles tended to cluster toward the patient’s sides, indicating where the inclusion of additional structures in the dose optimization process may avoid dose hot spots.

 

Conclusion: Gantry angle optimization in IMRT involves a large-scale computational problem.  We have demonstrated that the GA combined with a distributed-computing platform can be applied to optimize gantry angle selection within a reasonable amount of time. 

 

__________________________________________________________________________________________________________________________________________________________________________

Beam Weight and Angle Optimization in Radiation Therapy using Coupled Monte Carlo and Genetic Algorithm Codes

 

M Bakhtiari1, M D Jones2, H K Malhotra1, M B Podgorsak1, and D Nazareth1

1Roswell Park Cancer Institute, Buffalo, NY 14263

2Center for Computational Research, University at Buffalo, Buffalo, NY 14203

 

Purpose:  Monte Carlo (MC) algorithms remain the gold standard in dose calculation routines.  However, their long calculation times generally make them infeasible for clinical implementation, especially for IMRT optimization which requires rapid pencil-beam dose computation. In a preliminary study, we are investigating how high-throughput computing may be employed to perform MC dose calculations, beam weight optimization, and in conjunction with a genetic algorithm (GA), beam orientation optimization.

 

Method and Materials: Two non-commercial software packages were used for this project, VMC++ and CERR.  VMC++ is an MC dose calculation package which is more efficient than general-purpose MC routines due to its use of variance reduction techniques, making it approximately 50 times faster than the BEAMnrc code.  CERR is an open-source environment for radiotherapy calculations.  We used the data-importation and beam-shaping features of CERR in conjunction with the dose-calculation routines of VMC++ to perform dose computation on a 5-field 3D CRT prostate case as the inner loop of our method. We then optimized the beam weights using DVH-based constraints and the Nelder-Mead simplex technique, a multidimensional unconstrained nonlinear minimization algorithm.  The results served as input for a GA run in the outer loop.  Each generation of the GA involved 40 plans.  The calculations were performed using the computational resources of the Center for Computational Research, an academic supercomputing facility.

 

Results: The dose calculation and optimization involved several million particle histories, and required about two hours for each generation of the genetic algorithm.  The resulting plan was optimal based on the constraints provided to the system. 

 

Conclusion: We have shown that, using a distributed-computing platform, MC and GA routines may be coupled and employed for treatment planning in a reasonable amount of time. This work will be extended to IMRT and beam-angle optimization by combining a variety of techniques.

 

__________________________________________________________________________________________________________________________________________________________________________

 

The Solid-State X-Ray Image Intensifier (SSXII): The Next Generation of X-Ray Imagers

Andrew Kuhls-Gilcrist, Amit Jain, Daniel R Bednarek, Stephen Rudin

University at Buffalo, Buffalo, NY.

 

Purpose:  The solid-state x-ray image intensifier (SSXII) is an EMCCD-based x-ray detector designed to satisfy an increasing need for high-resolution real-time images, while offering significant improvements over current flat panel detectors (FPDs) and x-ray image intensifiers (XIIs). FPDs are replacing XIIs because they reduce/eliminate veiling glare, pincushion or s-shaped distortions and are physically flat. However, FPDs suffer from excessive lag and ghosting and their performance has been disappointing for low-exposure-per-frame procedures due to excessive instrumentation-noise. XIIs and FPDs both have limited resolution capabilities of ~3 cycles/mm.

 

Method and Materials: To overcome these limitations a prototype SSXII module has been developed, consisting of a 1k x 1k, 8 µm pixel EMCCD with a fiber-optic input window, which views a 350 µm thick CsI(Tl) phosphor via a 4:1 magnifying fiber-optic-taper (FOT). Arrays of such modules will provide a larger field-of-view. Detector MTF, DQE, and instrumentation-noise equivalent exposure (INEE) were measured to evaluate the SSXIIs performance using a standard x-ray spectrum (IEC RQA5), allowing for comparison with current state-of-the-art detectors.

 

Results: The MTF was 0.20 at 3 cycles/mm, comparable to standard detectors, and better than 0.05 up to 7 cycles/mm, well beyond current capabilities. DQE curves indicate no degradation from high-angiographic to low-fluoroscopic exposures (< 2% deviation in overall DQE from 1.3 mR to 2.7 µR), demonstrating negligible instrumentation-noise, even with low input signal intensities. An INEE of < 0.2 µR was measured for the highest-resolution mode (32 µm effective pixel size). Comparison images between detector technologies qualitatively demonstrate these improved imaging capabilities provided by the SSXII.

 

Conclusion: Initial use of the solid-state x-ray image intensifier has shown that this technology has great promise to be the next generation dynamic x-ray imager, providing significant improvements over current state-of-the-art detectors for applications such as fluoroscopy and angiography requiring high frame rates, resolution, dynamic range and sensitivity while maintaining essentially no lag and very low INEE.

 

__________________________________________________________________________________________________________________________________________________________________________

 

Accuracy in the dose delivery of IMRT as a function of Gantry and Collimator Angles

Jubei Liu, Zhou Wang, Matthew B. Podgorsak, Steven F. de Boer, Lalith Kumaraswamy, Harish Malhotra

Department of Radiation Medicine, Roswell Park Cancer Institute, Elm & Carlton Streets, Buffalo, NY 14263

 

Purpose:  Sliding window IMRT is the most demanding in terms of quality assurance requirement because of the coordination of the MLC positioning with the machine output.  Because of their weight, MLC leaves may experience significant gravitational force particularly when moving against gravity.  Traditionally IMRT beam data as well as patient specific IMRT QA is performed with gantry in straight condition which does not reflect the actual beam and collimator angle used in a patient.  Thus it is important to study the accuracy in dose delivery due to MLC motions as a function of gantry and collimator angles.

 

Material & Methods:  We have taken 3 IMRT treatment fields representing minimally, moderately and heavily modulated fluences, respectively.  The dose plans were generated for a Varian Trilogy unit employing a millennium MLC.  All the treatment fields had 320 control points for IMRT delivery.  MapCHECK along with 3 cm buildup material, in its isocentric fixture, was mounted in the linac accessory tray to hold it precisely at 100 cm SAD.  Both gantry and collimator angle were varied in intervals of 30° though collimator angles were restricted from 270°-90°.  This resulted in 72 combinations of gantry and collimator measurements per fluence.  Plans were evaluated using standard 3%/3mm criteria. 

 

Results:  The pass rate of each measurement was calculated and normalized over the result of 0o gantry and 0o collimator.  The variation in the pass-rate was independently studied as function of gantry angle and collimator angle but no systematic dependence on either of them was seen.  Worst variation of 6% in moderately modulated field at 270o gantry and 90o collimator was observed.  The overall average and standard deviations were within 3%.

 

Conclusion:  Our study has given a confidence that the sliding window IMRT dose delivery technique does not demonstrate significant gantry and collimator angle dependence due to MLC for the linac studied.

__________________________________________________________________________________________________________________________________________________________________________

 

An IMRT planning method for limiting spinal cord to tolerable levels with unintended field overlaps at the supraclavicular junction plane of head and neck radiotherapy.

Steven de Boer,  Osama Hassad*,  Wainwright Jaggernauth

Department of Radiation Medicine, Roswell Park Cancer Institute, Bufflao, NY

 

Purpose:   Head and neck cancers can be treated with an upper intensity modulation radiation therapy (IMRT) plan matched with a lower supraclavicular anterior field.  A small spinal cord block is traditionally placed in the supraclavicular field to shield to protect the spinal cord from excess dose due to unintended field overlaps.  This block can shield targeted tissue.  This study describes a method that keeps the cord dose within tolerance and still delivers dose to targeted tissues.

 

Method and Materials:

Radiotherapy plans were created with 7 coplanar IMRT fields matched to the anterior supraclavicular field.  IMRT optimization is then used to reduce the dose to levels that would result in tolerable spinal cord doses when field misalignments occur. A structure, named “cord junction”, was defined as the spinal cord that extends 2.1 cm superiorly and inferiorly to the junction plane.  The IMRT plan was optimized junction cord tolerances of 5, 10, 20, and 45 Gy. Each of these plans were then summated with the supraclavicular field with field misalignments of 0, 2, 5, 10 and 20 mm.  

 

Results:  As the overlap increases the maximum “junction cord” dose increases.  Larger overlaps are tolerable when the junction cord was reduced.  The 45 Gy junction cord limit is exceeded for overlaps of 2 mm (junction constraint of 45 Gy), 10 mm (junction constraint of 20 Gy or 10 Gy) and an over 20 mm overlap was tolerable when the cord junction constraint was 5 Gy.  The planning target volume (PTV) coverage was maintained for each optimization with D95 values of 98%.

 

Conclusion:  This study has addressed a common concern among clinicians of the need to not shield areas of possible disease yet ensure a safe spinal cord dose in the case of small positional errors in the radiation beam.

 

__________________________________________________________________________________________________________________________________________________________________________

 

Estimating Effective Dose in Radiostereometric Analysis of the Lumbar Spine

Kerry Greene-Donnelly, Kent Ogden, Nat Ordway, Jerry Calabrese, Marsha Roskopf

SUNY Upstate Medical University, Syracuse NY

 

Purpose:  To determine the effective dose of patients undergoing radiostereometric analysis (RSA) of the lumbar spine

 

Method and Materials:  12 patients with total disk replacement prosthetic devices in the lumbar spine participated in an IRB approved study to follow the sagittal and coronal range of motion using RSA.  Image pairs were obtained at 6 weeks, and then 3, 6, 12, 18 and 24 months.  Five image pairs were acquired at each visit (neutral, flexion, extension, and left and right lateral bend).  Radiographic techniques were recorded for all acquired images.  Patient mass was used to estimate abdominal AP thickness.  Tube output and half value layers were measured at the appropriate tube accelerating potentials.  This information was used with the image geometry to calculate the entrance kerma-area product (KAP) incident on the patients.  The KAP and patient thickness were then used to estimate the energy imparted to the patients and the resulting effective dose.

 

Results:  The average technique used was 141 kVp and 11.6 mAs.  The mean effective dose per image pair was 0.304 mSv, and the mean per visit (5 image pairs) was 1.52 mSv with a standard deviation of 0.7 mSv.  The average for the entire two year study was approximately 9.1 mSv.  This compares very favorably with the value of 18 mSv reported in the 2000 UNSCEAR report for a single diagnostic lumbar spine study.

 

Conclusion:  Image quality requirements for RSA are not the same as for general diagnostic imaging.  The use of high kV techniques that would result in unacceptable low contrast images for general diagnostic purposes are adequate for visualizing fiducial beads used in RSA.  Low doses allow for the acquisition of multiple image sets to detect motion of prosthetic devices with total effective doses that are much lower than a typical diagnostic lumbar spine examination.

 

__________________________________________________________________________________________________________________________________________________________________________

 

Computer-aided detection of metastatic brain tumors using automated 3-D template matching

R. Ambrosini1, P. Wang2, B. Kolar3, and W. O’Dell1,4

Departments of 1Biomedical Engineering, 3Radiology, and 4Radiation Oncology, University of Rochester, Rochester, NY, USA,

2Department of Radiation Oncology, University of Michigan, Ann Arbor, MI, USA

 

Purpose:  The development of metastases to the brain is a common and frequently devastating complication for patients with extracranial primary tumors.  However, the generally poor prognosis of patients with brain metastases can be improved with early detection and treatment with stereotactic radiosurgery, as performed routinely at our institution.  We have developed a novel small tumor detection algorithm based on 3-D template matching that will enhance the accuracy and efficiency of radiologists by allowing them to focus upon locations of high suspicion for metastatic brain tumors without having to spend time reviewing every image slice. 

 

Methods and Materials:  Spherical tumor appearance models were created to match the expected geometry of the small tumors of interest and accounting for offsets due to the cut of MRI sampling planes.  A 3-D normalized cross-correlation coefficient (NCCC) between the brain volume and spherical templates was calculated using a fast frequency domain algorithm. 

 

Results:  The data collected on 22 patient datasets consisting of 1320 coronal MR slices containing 161 total nodules shows that we can achieve currently a sensitivity of 87.6% with a false positive rate of 0.58 per image slice. 

 

Conclusion:  Our results demonstrate that the 3-D template matching method can be an effective, fast, and accurate tool for automated detection of tumors in brain MRIs.  Through the optimization of parameters such as zero padding and NCCC thresholding, we believe our algorithm has the potential to develop into a clinically useful tool to assist radiologists in providing earlier and more definitive diagnoses of metastases within the brain.

 

__________________________________________________________________________________________________________________________________________________________________________

 

A Guidance System for Optical Patient Alignment During Breast Radiotherapy

Jonathan Schmitta, Kenneth Hoffmanb, Mohammad Bakhtiaria, Harish Malhotraa, Daryl Nazaretha

a.) Roswell Park Cancer Institute b.) Toshiba Stroke Center, University at Buffalo

 

Purpose: Breast radiotherapy, particularly IMRT, involves large dose gradients and difficult patient positioning problems.  A critical requirement for successful treatment is accurate reproduction of the patient’s position assumed during CT simulation and planning.  We have developed an image-guided technique, which assists in accurately and reproducibly positioning the patient, by displaying her real-time optical image superimposed on a perspective projection image of her 3D CT data.

 

Methods. The Single Projection Technique (SPT) accurately determines the 3-D position and orientation of a camera from a single image acquired of a known model.  A calibration jig, composed of ten identifiable points, was constructed and CT imaged to provide this model.  The 3D coordinates of each point were indicated and recorded using treatment planning software.  In a preliminary study, a regular digital camera was installed in the treatment suite and used to obtain an optical image of the jig.  The SPT then provided the coordinates and orientation of the camera.  Using this information, 3D CT patient data could then be projected onto the camera’s imaging plane, superimposed on the real-time patient image using standard graphical software and displayed on a monitor. This would enable the therapist to view both the patient’s current and desired positions, and guide the patient into assuming the correct position. 

 

Results: The SPT can determine the position and orientation of the camera to an accuracy of 0.2 cm and 0.3°, respectively, using an optical digital image of the calibration jig.  This allows an estimated accuracy of 5 mm in the fidelity of the patient’s external anatomy to the surface CT data.  This includes anatomical points not easily positioned properly, such as the raised arm and breast skin surface.

 

Conclusion: We have developed a method to superimpose a perspective projection of a CT image on a patient’s real-time optical image.  Displaying this visual information will assist in accurate setup during breast radiotherapy.

 

__________________________________________________________________________________________________________________________________________________________________________

 

Dosimetric Analysis of the Effect of Tungsten Shields in a Fletcher-suit Delclos Applicator in High-Dose-Rate brachytherapy using Gafchromic Film

Thomas R. Stanley, Mohammad Bakhtiari, M B Podgorsak, Wainwright Jaggernauth & Harish K Malhotra

Roswell Park Cancer Institute, Buffalo, NY 14263.

 

Purpose: To study the effect of tungsten shields in the radiation dose delivery in a Fletcher-Suit Delclos applicator in high-dose-rate (HDR) brachytherapy using gafchromic film dosimetry. 

 

Methods and Materials: A gadget for rigidly and reproducibly mounting a Fletcher-Suit Delclos (FSD) tandem and ovoid applicator along with an attachment to hold a set of gafchromic films in relation to the applicator in a conventional water phantom was designed and fabricated.  The gadget allowed placing 14 films anterior to the tandem and another 14 posterior to the ovoids at a distance of 6.025 mm from each other.  The gadget has a provision of 5 fiducial marks per film for spatial registration with the orthogonal films acquired in a simulator.  A treatment plan delivering 700 cGy to the pseudo point A was designed.  The plan does not account for tungsten shields in the ovoids.  After the films were put in place, lasers were used as guides to mark the central axis of each film with respect to the tandem (to establish spatial coordination between both).  Once the films were properly aligned, the water phantom was filled with water.  The applicator was connected to the Micorselectron HDR treatment unit and the treatment plan was delivered.  Each gafchromic film was removed, marked for its location in the pack, dried, and scanned using a Vidar VXR-16 scanner for analysis using RIT software.  Using a measured H&D curve for calibration of the gafchromic films, the dose distributions on each film was evaluated and compared to the corresponding distributions produced from the treatment planning system. 

 

Results:  An analysis of the data revealed a reduction in dose measured by the gafchromic film over the calculated values from the treatment planning system in the area covered by the solid angle subtended by the tungsten shields in the ovoids.  This seems to follow logically considering the treatment planning algorithm does not account for the tungsten shields within each ovoid.  The details of the results will be presented. 

 

Conclusion:  The growing trend in brachytherapy procedures of this nature is to use CT/MR compatible tandem and ovoid applicators which do not provide any shielding for the bladder and rectum within the ovoids.  Thus, it is very important to understand the true radiation doses being delivered to these critical structures when the original treatment has used a shielded applicator.

 

__________________________________________________________________________________________________________________________________________________________________________

 

Experience in the development of clinical SBRT Program

Harish K Malhotra

Asst. Professor, Dept. of Radiation Medicine, Roswell Park Cancer Institute, Buffalo, NY

 

Recently Stereotactic body radiotherapy [SBRT] has been finding wide clinical acceptance for certain type of tumors.  Though initially started only for non-operable tumors with a palliative intent, recent interest is also to use it with curative intent irrespective of the operable status of certain tumors.  The ablative nature of the high doses associated with SBRT necessitate that this rapidly evolving modality for cancer treatment is implemented in a manner which ensures safe delivery of radiation dose to patients.  The present talk will focus on the clinical implementation of a SBRT program using Varian’s Trilogy linear accelerator.  The linear accelerator is equipped with KV-imager and has ability to KV-KV, KV-MV and CBCT acquisitions including KV-fluoroscopy mode.  It also comes with an optical guidance platform to assist in the patient setup using infrared fiducial markers.  Both single slice CT scanner as well as 16-slice CT scanners were used for the CT simulation of these patients.  A number of additional quality assurance steps were added at each phase of the treatment including simulation, immobilization, initial setup verification, treatment planning, pre-treatment QA for the linear accelerator as well as the process to determine the setup shifts and during the actual treatment delivery.  More than 30 patients have been treated so far since the starting of the program at Roswell Park Cancer Institute since February’07.  Details of our experience in the development of our clinical SBRT program will be discussed.

 

__________________________________________________________________________________________________________________________________________________________________________

 

The Past, Present, and Future in Medical Physics

Jacob (Jake) Van Dyk

Manager, Physics and Engineering

London Regional Cancer Program/London Health Sciences Centre

Professor, Departments of Oncology, Medical Biophysics, Diagnostic Imaging and Nuclear Medicine, and Physics and Astronomy, University of Western Ontario

790 Commissioners Rd E, London, Ontario, Canada

 

The discovery of “a new kind of ray” by Roentgen in 1895 spawned a new era for medicine and a new discipline known as “Medical Physics”. With the evolution of new technologies, medical physics has developed subspecialties in Radiation Oncology, Diagnostic Radiology and Nuclear Medicine. Progress in radiation oncology can be divided into five distinct phases. The advances in the last four decades have largely been in parallel with advances in computer capabilities. In the last two decades, we have experienced a revolution in radiation delivery technologies such that intensity modulated radiation therapy (IMRT) has become routine. Furthermore, enhancement of imaging technologies with the use of CT simulation, MRI, PET and combined PET/CT allows for 3-D viewing of targets and critical structures, with the addition of functional, disease-related information. At the same time, new imaging capabilities on radiation therapy machines provide the location of the “target of the day” and are moving us towards the routine use of image-guided adaptive radiation therapy. With 4-D imaging and 4-D treatment capabilities now possible, we can expect, in the not too distant future, to get daily 4-D imaging of the patient in treatment position and real-time optimization of an updated treatment plan to deal with the anatomy of the day. With developments in new technologies, heavy particle therapy will become more economically viable. In addition, radiobiological modeling and optimization will become routine. A little further forward, nanotechnology and molecular biology will become significant components of both diagnostic imaging and therapy, not only for cancer but for other diseases as well. With these continuous advancements in technology and the increased information base, medical physics continues to have a bright future.

__________________________________________________________________________________________________________________________________________________________________________