Optimized planning for intraoperative planar permanent-seed implant

Similar documents
A fast, independent dose check of HDR plans

Dose Distributions. Purpose. Isodose distributions. To familiarize the resident with dose distributions and the factors that affect them

The IORT Treatment Planning System. radiance. GMV, 2012 Property of GMV All rights reserved

Optimization in Brachytherapy. Gary A. Ezzell, Ph.D. Mayo Clinic Scottsdale

CHAPTER 9 INFLUENCE OF SMOOTHING ALGORITHMS IN MONTE CARLO DOSE CALCULATIONS OF CYBERKNIFE TREATMENT PLANS: A LUNG PHANTOM STUDY

Chapter 9 Field Shaping: Scanning Beam

Basic Radiation Oncology Physics

Prostate Detection Using Principal Component Analysis

Air Kerma Strength Measurements and Monte Carlo based Dosimetric Characterization of a directional Pd 103 planar source array.

Coverage based treatment planning to accommodate organ deformable motions and contouring uncertainties for prostate treatment. Huijun Xu, Ph.D.

Intraoperative Prostate Tracking with Slice-to-Volume Registration in MR

Interactive Treatment Planning in Cancer Radiotherapy

Optimization with Multiple Objectives

DUAL energy X-ray radiography [1] can be used to separate

Comprehensive treatment planning for brachytherapy. Advanced planning made easy

3DVH : SUN NUCLEAR On The Accuracy Of The corporation Planned Dose Perturbation Algorithm Your Most Valuable QA and Dosimetry Tools *Patent Pending

Dose Calculation and Optimization Algorithms: A Clinical Perspective

UNCOMPROMISING QUALITY

A fluence convolution method to account for respiratory motion in three-dimensional dose calculations of the liver: A Monte Carlo study

How would, or how does, the patient position (chin extended) affect your beam arrangement?

CBCT Equivalent Source Generation Using HVL and Beam Profile Measurements. Johnny Little PSM - Medical Physics Graduate Student University of Arizona

3D TRUS Guided Robot Assisted Prostate Brachytherapy

An experimental investigation on the effect of beam angle optimization on the reduction of beam numbers in IMRT of head and neck tumors

Brachytherapy dose-volume histogram commissioning with multiple planning systems

ICARO Vienna April Implementing 3D conformal radiotherapy and IMRT in clinical practice: Recommendations of IAEA- TECDOC-1588

Slide 1. Technical Aspects of Quality Control in Magnetic Resonance Imaging. Slide 2. Annual Compliance Testing. of MRI Systems.

Quantitative imaging for clinical dosimetry

Fiber Selection from Diffusion Tensor Data based on Boolean Operators

REAL-TIME ADAPTIVITY IN HEAD-AND-NECK AND LUNG CANCER RADIOTHERAPY IN A GPU ENVIRONMENT

Photon beam dose distributions in 2D

Monaco Concepts and IMRT / VMAT Planning LTAMON0003 / 3.0

Dosimetric impact of the 160 MLC on head and neck IMRT treatments

PyCMSXiO: an external interface to script treatment plans for the Elekta CMS XiO treatment planning system

A software tool for the quantitative evaluation of 3D dose calculation algorithms

Geant4 in Brachytherapy

Application of Multiobjective Genetic Algorithms in Anatomy Based Dose Optimization in Brachytherapy and its Comparation with Deterministic Algorithms

Current state of multi-criteria treatment planning

8/4/2016. Emerging Linac based SRS/SBRT Technologies with Modulated Arc Delivery. Disclosure. Introduction: Treatment delivery techniques

Determination of rotations in three dimensions using two-dimensional portal image registration

Filling Space with Random Line Segments

AN AUTOMATED SOFTWARE SYSTEM FOR BRACHYTHERAPY SOURCE LOCATION ISMAIL AHMET NALCACIOGLU

Design and performance characteristics of a Cone Beam CT system for Leksell Gamma Knife Icon

Generation of uniformly distributed dose points for anatomy-based three-dimensional dose optimization methods in brachytherapy

4 Measurement. and Analysis. 4.1 Overview and Underlying Principles 4-1

Basics for vector implantation schemes in HDR brachytherapy using a new linear programming model

Adaptive algebraic reconstruction technique

An optimization framework for conformal radiation treatment planning

The MSKCC Approach to IMRT. Outline

CARS 2008 Computer Assisted Radiology and Surgery

A DOSIMETRIC MODEL FOR SMALL-FIELD ELECTRON RADIATION THERAPY A CREATIVE PROJECT (3 SEMESTER HOURS) SUBMITTED TO THE GRADUATE SCHOOL

Integrated proton-photon treatment planning

ROBUST OPTIMIZATION THE END OF PTV AND THE BEGINNING OF SMART DOSE CLOUD. Moe Siddiqui, April 08, 2017

3D-printed surface mould applicator for high-dose-rate brachytherapy

Creating a Knowledge Based Model using RapidPlan TM : The Henry Ford Experience

3/27/2012 WHY SPECT / CT? SPECT / CT Basic Principles. Advantages of SPECT. Advantages of CT. Dr John C. Dickson, Principal Physicist UCLH

Using Pinnacle 16 Deformable Image registration in a re-treat scenario

Shadow casting. What is the problem? Cone Beam Computed Tomography THE OBJECTIVES OF DIAGNOSTIC IMAGING IDEAL DIAGNOSTIC IMAGING STUDY LIMITATIONS

Michael Speiser, Ph.D.

Helical Tomotherapy Qualitative dose Delivery Verification

Optimization of CT Simulation Imaging. Ingrid Reiser Dept. of Radiology The University of Chicago

Digital Imaging and Communications in Medicine (DICOM) Supplement 176: Second Generation Radiotherapy. Additional RT Treatment Modalities

7/29/2017. Making Better IMRT Plans Using a New Direct Aperture Optimization Approach. Aim of Radiotherapy Research. Aim of Radiotherapy Research

A hybrid framework for optimizing beam angles in radiation therapy planning

Generation of Hulls Encompassing Neuronal Pathways Based on Tetrahedralization and 3D Alpha Shapes

A simple method to test geometrical reliability of digital reconstructed radiograph (DRR)

Digital breast tomosynthesis: comparison of different methods to calculate patient doses

Automatic Quantification of DTI Parameters along Fiber Bundles

Investigation of tilted dose kernels for portal dose prediction in a-si electronic portal imagers

IMSURE QA SOFTWARE FAST, PRECISE QA SOFTWARE

IMRT and VMAT Patient Specific QA Using 2D and 3D Detector Arrays

Applied Optimization Application to Intensity-Modulated Radiation Therapy (IMRT)

Data. ModuLeaf Mini Multileaf Collimator Precision Beam Shaping for Advanced Radiotherapy

Dose Calculations: Where and How to Calculate Dose. Allen Holder Trinity University.

Three Dimensional Dosimetry Analyses In Radionuclide Therapy Using IDL And MCNP-based Software Tools

Influence of electron density spatial distribution and X-ray beam quality during CT simulation on dose calculation accuracy

A Fully-Automated Intensity-Modulated Radiation Therapy Planning System

Prostate Brachytherapy Seed Segmentation Using Spoke Transform

An EGSnrc generated TG-43 dosimetry parameter database

Improving the detection of excessive activation of ciliaris muscle by clustering thermal images

Automatic Quantification of DTI Parameters along Fiber Bundles

NEW TECHNIQUES FOR CALCULATING VOLUMES BY CROSS SECTIONS.

Implementation and evaluation of a fully 3D OS-MLEM reconstruction algorithm accounting for the PSF of the PET imaging system

Spectral analysis of non-stationary CT noise

FAST, precise. qa software

AAPM Standard of Practice: CT Protocol Review Physicist

CT Protocol Review: Practical Tips for the Imaging Physicist Physicist

Spiral CT. Protocol Optimization & Quality Assurance. Ge Wang, Ph.D. Department of Radiology University of Iowa Iowa City, Iowa 52242, USA

Monte Carlo Simulation for Neptun 10 PC Medical Linear Accelerator and Calculations of Electron Beam Parameters

C a t p h a n / T h e P h a n t o m L a b o r a t o r y

A new algorithm for autoreconstruction of catheters in computed tomography based brachytherapy treatment planning

CHAPTER 2 MEDICAL IMAGING WITH NON-IONIZING RADIATION

Commissioning and quality assurance of Calypso four dimensional target localization system in linear accelerator facility

ACE Advanced Collapsed cone Engine

Automatic measurement of air gap for proton therapy using orthogonal x ray imaging with radiopaque wires

Annales UMCS Informatica AI 1 (2003) UMCS. Registration of CT and MRI brain images. Karol Kuczyński, Paweł Mikołajczak

Monte Carlo methods in proton beam radiation therapy. Harald Paganetti

Validation of GEANT4 for Accurate Modeling of 111 In SPECT Acquisition

VCU Radiation Oncology

IMAGE RECONSTRUCTION AND THE EFFECT ON DOSE CALCULATION FOR HIP PROSTHESES

Projection-Based Needle Segmentation in 3D Ultrasound Images

Transcription:

JOURNAL OF APPLIED CLINICAL MEDICAL PHYSICS, VOLUME 3, NUMBER 3, SUMMER 2002 Optimized planning for intraoperative planar permanent-seed implant Albert Y. C. Fung,* Howard I. Amols, and Marco Zaider Department of Medical Physics, Memorial Sloan-Kettering Cancer Center, 1275 York Avenue, New York, New York 10021 Received 18 February 2002; accepted for publication 14 May 2002 We describe a fast, PC-based optimization planning system for a planar permanentseed implant. Sites where this system is applicable include brain, lung, and head and neck. The system described here allowsplacing ribbons of different strengths and of different lengths along and across the implant plane. The program takes full advantage of the availability of different source strengths in inventory, and attempts to find configurations of ribbons that result in optimal dose uniformity over the prescription plane. Dosimetry is based on the AAPM TG 43 Report R. Nath et al., Med. Phys. 22, 209 234 1995. Compared with TG 43 parameters, the classical tables underestimate the I-125 source strengths needed by 40%. The use of several source strengths improves the plan. Typical optimization yields dose uniformity of 10%, and computing times are within 2 3 min. No further enhancement is obtained if ribbons are placed in a grid pattern as opposed to the simpler arrangement along parallel lines. Nor is it valuable to have variable ribbon lengths. For an I-125 implant the optimization system described here is a practical alternative to the strictly speaking inapplicable classical systems. It calculates correctly the total source strengths, and most notably generates plans with optimal dose uniformity. The fast computing time is well suited for planning during surgery in the operating room. 2002 American College of Medical Physics. DOI: 10.1120/1.1491787 Key words: optimization intraoperative planar seed implant PACS number s : 87.53.Jw, 87.53.Tf INTRODUCTION The work described in this article stems from the observation that intraoperative permanent implants at sites of residual disease tumor bed, such as brain, lung, and head and neck, are regularly performed without any treatment plan. A typical case at Memorial Sloan-Kettering Cancer Center MSKCC is the interstitial implantation of skull base tumors: following surgical resection of the tumor, I-125 seeds, evenly spaced in Vicryl suture ribbons, are implanted by free hand at a distance of 0.5 1 cm from each other. The dose prescription is determined by obtaining CT scans of the volume implanted and then selecting an isodose surface that surrounds the region of interest, which is typically determined by the sources themselves. There exists no good published system for an I-125 planar permanent implant. Classical implant systems, such as the Manchester, Quimby, or the Anderson nomogram, were originally developed for radium-equivalent isotopes with high gamma energies. Implants with I-125 seeds, because of lower energies and greater absorption in tissue, require much higher source strength than those indicated in the classical tables for the same implant area. There are also important practical constraints for this kind of implant. For instance: i Treatment planning must be performed rapidly in the operating room. ii The area to be implanted is known only at the time of surgery. iii The physicist is not routinely in the position 221 1526-9914Õ2002Õ3 3 Õ221Õ6Õ$17.00 2002 Am. Coll. Med. Phys. 221

222 Fung, Amols, and Zaider: Optimized planning for intraoperative... 222 to select the source activity that will optimize the intended dose distribution. iv The plan may not be put into operation as designed because of anatomical constraints. We describe a fast, PC-based optimization planning system for a planar permanent-seed implant. In addition, the potential benefit of modifications to the classical implant systems, such as several ribbon strengths, variable ribbon lengths, and crossing ribbons, has never been studied, and these with a computer may significantly improve the quality of the plan while continuing to fulfill the inevitable need for speedy planning. The optimization system described below is meant to produce a maximally uniform dose in a plane a given distance away from the implanted area, in line with the current intent of such treatments. METHODS The optimization system assumes that the implant is rectangular, and that the dose is prescribed in a parallel plane located at a distance d above the plane of the sources. Thus, the target volume is a rectangular slab of thickness 2d. If the implant is not flat the dose on the concave side will be somewhat larger than that on the convex side. Because it is difficult to measure the implant curvature, at this time it appears impractical to attempt to compensate for its effects. The program takes as input the isotope type I-125 or Ir-192, a list of source strengths available in the inventory, the length L and width W of the implant, the prescription dose, D 0, and the prescription distance, d. The solution describes a pattern of ribbons placed equidistantly 1-cm apart along, or perpendicular to the sides of the target volume. It specifies also the source strength used in each ribbon. The program allows one to seek solutions with ribbons along one direction only X or Y and also of variable length. Only solutions that are symmetric with respect to both axes X and Y are considered since the prescription doses are always symmetric. The set of all possible solutions is limited, and the simplest method of identifying the best solution is to evaluate sequentially all possible ribbon patterns in terms of a cost function. For a more complicated situation, sophisticated techniques such as the genetic algorithm 1 and simulated annealing 2 may be used. Specifically, solutions are ranked according to the dose uniformity on the prescription plane. Thus, Uniformity i D i D 0 2 /D 0 / number of points, 1 where D i is the dose delivered at point i, and the summation is over a predefined configuration of grid points on the prescription plane. As defined, uniformity gives equal score to underdosage and overdosage. Should the physician prefer otherwise, it is very easy to adjust the weights. Dose points are spaced 0.5 cm apart and the gap between seeds is 1 cm; thus, dose points are either just above or in-between seeds. Since only symmetric solutions are considered, the grid only needs to span one quarter of the area. The total number of dose points is L and W assumed integers N d L 1 W 1. In addition to dose uniformity, the program calculates the target coverage V100, or the percentage of target volume covered by the prescribed dose. The target volume is defined as the slab of tissue bounded by the rectangular plane at distance d from the centers of the sources i.e., the slab thickness is 2d. To deduce the target coverage, doses are calculated at points in a threedimensional grid of 0.1-cm spacing inside the target volume. The software also calculates the dose-volume histogram DVH of the plan and isodose distributions in axial planes. Dosimetry is based on the AAPM TG 43 report recommendations. 3 Full 2D anisotropy functions are employed. The code first calculates, at every grid location, the dose due to ribbons with unit-strength seeds of any feasible length and orthogonal orientation. This dose matrix is calculated before evaluating actual solutions since the dose values in the matrix will be used repeatedly. The computing time is 2

223 Fung, Amols, and Zaider: Optimized planning for intraoperative... 223 FIG. 1. Optimized solutions for an 8 5 cm planar implant, with ribbons along a the long direction only, b the short direction only, and c both orthogonal directions. The seeds shown with larger diameters are each of 1 U, and those with smaller diameters are of 0.5 U. In reality, sources have the same diameters regardless of strength. proportional to the number of solutions evaluated. If all ribbon-arrangement options are turned on, the total number of possible solutions is N s A 1 U V U V V U, where U Integer W/2, V Integer L/2, and A is the number of available source strengths the expression A 1 appears in Eq. 3 since zero strength is always permissible for any ribbon. If solutions are restricted to full ribbon lengths from end to end of the target area then the number of solutions is reduced to (A 1) U V. It is obvious that the computing time increases rapidly with the available source strengths and also L and W. A typical solution is obtained in a few minutes on a Pentium III computer. RESULTS AND DISCUSSION The availability of seeds with several source strengths will obviously improve the plan. This may not be impractical if, given a large number of patients, unused seeds are stocked. At MSKCC, for instance, a standing order of seeds delivered once a month is in effect. New iodine suture seeds have usually air kerma strength of 1.2 U. After one month, this will decay to 70% of its original value half-life of 59.4 days. Therefore, it is commonly the case that a series of decreasing source strengths 70% of one another is obtainable. In the case of a planar implant, an important criterion for plan evaluation and optimization is dose uniformity over the prescription plane. By contrast, in a volume implant, such as the prostate, target coverage and conformity are also invoked. For a planar implant coverage alone without other constraints is not sufficient since one can always heat up the implant with high activity seeds and achieve 100% coverage, at the expense of conformity and/or excessive dose to the surrounding normal tissue. In the case of brain implant, the normal brain tissue is itself a critical organ to be spared as much as possible. Internal uniformity is important in a volume implant but is misleading in planar implant, since the volumes closest to the radioactive sources are inevitably hot, and such volumes constitute a large fraction of the planar target volume. Uniformity over the prescription plane automatically achieves a compromise between coverage and conformity. It is a single criterion instead of two and thus, no extra weighting factor needs to be used. The optimization allows for ribbons in either one of two orthogonal directions. We have also studied the benefit of laying ribbons concurrently in two directions instead of only one direction. It appears that in nearly every case studied, the resulting dose distributions using both directions and either direction are very similar. The example shown in Fig. 1 is for a 8 5 cm 2 planar implant 3

224 Fung, Amols, and Zaider: Optimized planning for intraoperative... 224 TABLE I. Comparison of plans allowing for ribbons parallel to a the long direction only, b the short direction only, and c both orthogonal directions. Ribbons parallel to Total source strength U Uniformity % Target coverage % Long direction only 4.5 11.6 98.97 Short direction only 4.5 10.4 99.92 Both orthogonal directions 4.8 9.6 99.93 in which 150 Gy is prescribed at 0.5 cm distance. The available iodine source strengths are 0.5 and 1.0 U. The figure shows the optimized solutions allowing for ribbons parallel to a long direction only, b short direction only, and c both orthogonal directions. The thick seeds have 1.0 U while the thin ones are of 0.5 U. The seed arrangements of the three solutions are obviously quite different. However, differences between the three solutions see Table I are unlikely to have any clinical significance. Figure 2 graphs the corresponding dose volume histograms. Another consideration in using ribbons in both directions is that two seeds at the same spot cannot be placed in exactly the same level, but have to be on top of each other, resulting in slight deviation from the intended dose distribution. Figure 3 is a cross-sectional plane A indicated in Figure 1 c showing the isodose of the optimal plan. Although pockets of cold spots appear within the target volume, the target coverage is in fact 99.93%, i.e., the total volume receiving less than the prescribed dose is only 0.07% of the target volume. The Ir-192 ribbons we order are of ten-seed length, with 1-cm seed separation that gives 9 cm length from end to end. We do not really stock ribbons of various lengths, but we can cut with scissors an original ribbon to any length dictated by the plan. The program does not tract the number of ribbons available. When an activity is put in, it assumes the number of ribbons will be enough. The option of different ribbon lengths, which our program permits, does not seem to be helpful in achieving a more uniform dose distribution. With variable lengths, the computing time for implants larger than 5 5 cm 2 and with two or more source strengths is prohibitively long much more than several minutes and for nearly every optimized plan full-length ribbons are used anyway. Therefore, we do not turn on this option at all in clinical use. For hospitals that do not have a standing order, single source strength will probably be ordered for each patient. Our optimization program can still generate the best plan achievable with the limited available source strength. Nevertheless, since orthogonal directions and variable length ribbons seem not worth the trouble, a nomogram or similar formula will suffice for a single strength implant. Although a nomogram for an I-125 implant was published in the literature, 4 it FIG. 2. Dose volume histograms of optimized solutions for a 8 5 cm planar implant.

225 Fung, Amols, and Zaider: Optimized planning for intraoperative... 225 FIG. 3. Cross-sectional plane A indicated in Fig. 1 c showing the isodose of the optimal plan for an 8 5 cm planar implant. The three isodose curves are 200 Gy, 150 Gy prescribed dose, thick line, and 110 Gy. The prescription plane is 0.5 cm from the implant plane. was for spheroidal and cylindrical volume only and not for planar volume, and it was derived from the Ir-192 nomogram and gave inappropriate source activities for I-125. 5 We use the optimization software to generate nomogram-like formulas for hospitals that only have single activity seeds. Specifically, we record the implant areas for 50 patients in the past to obtain a realistic distribution of treatment areas, and re-run the plans with the optimizer. All 50 implants were rectangular. The area of the implants ranged from 25 to 108 cm 2, and the lengths ranges from 3 to 12 cm. The aspect ratio length / width averaged 1.4, with a maximum of 2.0. The results for a prescription dose of 150 Gy are plotted in Fig. 4. The fitted lines for the total source strengths U are U 0.83 area 10.8 for 150 Gy, d 0.5 cm, 4a U 1.31 area 25.4 for 150 Gy, d 1.0 cm, 4b where area is in cm 2. The total source strength required is proportional to the prescription dose, therefore the total source strength for any dose can be deduced from these formulas. Strictly speaking, these formulas are good for only for Amersham I-125 model 6720 suture seeds same dosimetry as model 6711, and needs to be scaled by a different dose rate constant cgy/u for other brands of seeds. We have never treated a patient for distance other than 0.5 or 1.0 cm, hence we have not produced similar formulas for other distances. Note that these fitted lines are based on optimized plans, irrespective of our past actual implant plans, which may or may not be optimal. Among the 50 implants, only one had an aspect ratio of 2. We have run the optimization for aspect ratios as high as 3, and the source strengths from formulas have less than a 10% difference from the optimized FIG. 4. Total source strength U for an I-125 planar permanent implant as a function of area for a 150 Gy dose prescribed at a d 0.5cmand b d 1.0 cm.

226 Fung, Amols, and Zaider: Optimized planning for intraoperative... 226 values. When the aspect ratio went up to 4, the algorithm in general took too long to finish more than 10 min. Hence, up to an aspect ratio of 3, the formulas provide valid source strength values, and our program can generate an optimized result in reasonable time. To use the formulas, first obtain the single individual source strength available, the implant area, and the prescription dose and distance. Calculate the total source strengths needed with the appropriate formula. The total source strengths can be divided by the individual source strength and the number of seeds in one ribbon to obtain the number of ribbons required, and hence the ribbon spacing. As an example, if 0.6 U I-125 suture seeds are available for a 4 6 cm implant with 120 Gy prescribed at d 0.5 cm, the total source strength required will be 0.83 24 10.8 120 150 24.6 U. Since each ribbon has seven seeds 6 cm end-to-end, the number of ribbons needed will be 24.6 0.6 7 5.85. Hence, one should use six ribbons to the nearest integer, and the spacing between ribbons will be 4 (6 1) 0.8 cm. CONCLUSION To summarize, for I-125 implants the optimization system described here is a practical alternative to the by and large invalid classical systems. This is not surprising, since the classical plans are among those being evaluated during optimization. It calculates correctly the total source strengths, takes full advantage of the availability of different source strengths in the inventory and, most importantly, generates plans according to pre-assigned dose uniformity requirements. Because the computing time is of the order of a few minutes, it is well suited for planning during surgery in the operating room. *Email address: Albert.fung@verizon.net 1 A. Y. C. Fung, K. M. Alektiar, D. Silvern, and M. Zaider, Treatment-plan optimization for soft-tissue sarcoma brachytherapy using a genetic algorithm, Int. J. Radiat. Oncol., Biol., Phys. 47, 1385 1395 2000. 2 J. Pouliot, D. Tremblay, J. Roy, and S. Filice, Optimization of permanent 125 I prostate implants using fast simulated annealing, Int. J. Radiat. Oncol., Biol., Phys. 36, 711 720 1996. 3 R. Nath et al. Dosimetry of interstitial brachytherapy sources: Recommendations of the AAPM Radiation Therapy Committee Task Group No.43, Med. Phys. 22, 209 234 1995. 4 L. L. Anderson, B. S. Hilaris, and L. K. Wagner, A nomograph for planar implant planning, Endocurie Hypertherm. Oncol. 1, 9 15 1985. 5 L. L. Anderson private communication.