A Comparison of Tissue Doses from Colloidal Sn-117m, P-32, Y-90, Re-186 and Er-169 for Radiosynoviorthesis Using Monte Carlo Simulation Richard E. Wendt.

Slides:



Advertisements
Similar presentations
Numerical Analysis for Influence of Cascade Solidity on the Performances of Cavitating Inducers Xiaojun Li Research Center of Fluid.
Advertisements

The Vin č a Institute of Nuclear Sciences, Belgrade, Serbia * Universita degli studi di Bologna, DIENCA, Italia Radovan D. Ili}, Milan Pe{i}, Radojko Pavlovi}
Esteban Fabián Boggio 1 Lucas Provenzano 2 Sara Gonzalez 2,3 Sara Gonzalez 2,3 Juan Manuel Longhino 1 1 Bariloche Atomic Center, Atomic Energy National.
Alexander Brandl ERHS 630 Radiation and Tissue Weighting Factors Environmental and Radiological Health Sciences.
Signal Analysis and Processing for SmartPET D. Scraggs, A. Boston, H Boston, R Cooper, A Mather, G Turk University of Liverpool C. Hall, I. Lazarus Daresbury.
MONTE CARLO RADIATION DOSE SIMULATIONS AND DOSIMETRY COMPARISON OF THE MODEL 6711 AND I BRACHYTHERAPY SOURCES Mark J. Rivard Department of Radiation.
Tissue inhomogeneities in Monte Carlo treatment planning for proton therapy L. Beaulieu 1, M. Bazalova 2,3, C. Furstoss 4, F. Verhaegen 2,5 (1) Centre.
Radiation Dosimetry Dose Calculations D, LET & H can frequently be obtained reliably by calculations: Alpha & low – Energy Beta Emitters Distributed in.
At the position d max of maximum energy loss of radiation, the number of secondary ionizations products peaks which in turn maximizes the dose at that.
The brachytherapy advanced example Susanna Guatelli (CERN/INFN)
Radiation therapy is based on the exposure of malign tumor cells to significant but well localized doses of radiation to destroy the tumor cells. The.
Dose Distribution and Scatter Analysis
Geant4 simulation of the attenuation properties of plastic shield for  - radionuclides employed in internal radiotherapy Domenico Lizio 1, Ernesto Amato.
Introduction to Nuclear Medicine
TÍTULO DO TRABALHO NOMES DOS AUTORES ENDEREÇOS E DOS AUTORES INTRODUTION Gammacell 220 Series 39 is a irradiation device purchased by CDTN/CNEN in.
G. Bartesaghi, 11° ICATPP, Como, 5-9 October 2009 MONTE CARLO SIMULATIONS ON NEUTRON TRANSPORT AND ABSORBED DOSE IN TISSUE-EQUIVALENT PHANTOMS EXPOSED.
Ye, Sung-Joon, Ph.D. Ove, Roger, M.D., Ph.D.; Shen, Sui, Ph.D.
An Overview of Current and Propose Radioactive Nano- Particle Creation and Use L. Scott Walker Los Alamos National Laboratory 03/17/08.
SHINE SEP Campaign Events: Long-term development of solar corona in build-up to the SEP events of 21 April 2002 and 24 August 2002 A. J. Coyner, D. Alexander,
PHYSICAL BACKGROUND ATOMIC STRUCTURE, NUCLEONS AND ACTIVITY
Evaluation of absorbed fractions for beta- gamma radionuclides in ellipsoidal volumes of soft tissue through Geant4 Ernesto Amato 1, Domenico Lizio 2 and.
Li HAN and Neal H. Clinthorne University of Michigan, Ann Arbor, MI, USA Performance comparison and system modeling of a Compton medical imaging system.
Introduction The Radiological Physics Center (RPC) anthropomorphic quality assurance (QA) phantom program is one tool the RPC uses to remotely audit institutions.
SOES6002: Modelling in Environmental and Earth System Science CSEM Lecture 3 Martin Sinha School of Ocean & Earth Science University of Southampton.
Nuclear Decay. Radioactivity The emission of high-energy radiation or particles from the nucleus of a radioactive atom.
Thickness of CZT detector 110 MeV140 MeV DETECTOR A (1 mm CZT + 5 mm CZT) DETECTOR B (1 mm CZT + 10 mm CZT) DETECTOR C (1 mm CZT + 15 mm CZT) A. Generation.
Nature’s Clock.  When sedimentary rock is deposited in layers it is deposited horizontally.  Scientists use this “Principle of Original Horizontality”
Contents: Computer Code
HOW MUCH RADIOACTIVE WASTE COULD POTENTIALLY BE IMPORTED INTO TEXAS
Biot-Savart Law Performing various measures to study the magnetic field intensity variations around an inducting coil.
A Study of Reverse MC and Space Charge Effect Simulation with Geant4
J. Helsby, P. Ford, R. Hoch, K. Gnanvo, R. Pena, M. Hohlmann, D. Mitra
J Cho, G Ibbott, M Kerr, R Amos, and O Mawlawi
Methods & Materials (continued)
J Cho, G Ibbott, M Gillin, C Gonzalez-Lepera, U Titt and O Mawlawi
Louisiana State University Radiation Safety Office
Date of download: 10/11/2017 Copyright © ASME. All rights reserved.
Modulation-frequency dependency of optical measurements in turbid media: Phantom and simulation studies E L Maclin1, J Kimnach1, K A Low1 , M Fabiani1,
INTERCOMPARISON P3. Dose distribution of a proton beam
INTERACTION OF PARTICLES WITH MATTER
Characteristics and Comparison of RSO Isotopes including Sn-117m
Mouse Strain Modulates the Role of the Ciliated Cell in Acute Tracheobronchial Airway Injury-Distal Airways  Gregory W. Lawson, Laura S. Van Winkle, Elina.
Nuclear Chemistry.
Development and characterization of the Detectorized Phantom for research in the field of spatial fractionated radiation therapy. D. Ramazanov, V. Pugatch,
A Brachytherapy Treatment Planning Software Based on Monte Carlo Simulations and Artificial Neural Network Algorithm Amir Moghadam.
SIN502S Week 6.
Rutherford’s scattering experiment
Neutronics Studies for the Nab Experiment
Arghya Chattaraj, T. Palani Selvam, D. Datta
OCR Gateway 2016 Physics topic 6
Chapter 22 Nuclear Chemistry.
Radioactive Decay Section 21.2.
Radioactive material within the body
NanoBPM Status and Multibunch Mark Slater, Cambridge University
Acute inflammation with induction of anaphylatoxin C5a and terminal complement complex C5b-9 associated with multiple intra-articular injections of hylan.
MRI of articular cartilage in OA: novel pulse sequences and compositional/functional markers  Garry E. Gold, Deborah Burstein, Bernard Dardzinski, Phillip.
Osteoarthritis – a case for personalized health care?
Summary of alpha etc.
Uniform Sampling of Steady-State Flux Spaces: Means to Design Experiments and to Interpret Enzymopathies  Nathan D. Price, Jan Schellenberger, Bernhard.
Selected Bioavailability and Pharmacokinetic Calculations
Nuclear Chemistry Chapter 25.
Canadian Association of Nuclear Medicine
Canadian Association of Nuclear Medicine
Cost-effectiveness of oral phenytoin, intravenous phenytoin, and intravenous fosphenytoin in the emergency department  Maria I Rudis, PharmD, Daniel R.
Differences in structural and pain phenotypes in the sodium monoiodoacetate and meniscal transection models of osteoarthritis  P.I. Mapp, D.R. Sagar,
Volume 46, Issue 5, Pages (May 2007)
Atoms and Radioactivity
Assist. Prof. Dr. Ilker Ozsahin Oct
Matthew Rose - Emission Spectra of Bicron Scintillators
Matthew Rose - Emission Spectra of Bicron Scintillators
Presentation transcript:

A Comparison of Tissue Doses from Colloidal Sn-117m, P-32, Y-90, Re-186 and Er-169 for Radiosynoviorthesis Using Monte Carlo Simulation Richard E. Wendt III UT MD Anderson Cancer Center, Houston TX and Nigel R. Stevenson Serene, LLC, The Woodlands TX

Acknowledgment and Disclosure The work of REW was supported by an unrestricted grant from Serene, LLC. NRS is an officer and owner in Serene, LLC.

Radiosynoviorthesis Radionuclides Application e- Electron Range in ICRU 4-Component Tissue* (avg.; max. mm) Half-life (days) Y-90 (citrate) Large (knee) β (4.05; 11.4) 2.67 P-32 (Cr04P) (2.78; 8.3) 14.3 Re-186 (sulfide) Medium (elbow) (1.06; 4.79) 3.72 Er-169 (citrate) Small (fingers and toes) (0.14 [0.3†]; 1.07) 9.40 Sn-117m (6 μm colloid) Canine elbow (investigational) CE (0.241; 0.290 ) 14.0 In this study, we have considered five radionuclides for radiosynoviorthesis. Four of them, Y-90, P-32, Re-186 and Er-169 are used clinically to treat the range of human synovial joints. Sn-117m in a colloidal preparation is being developed as an alternative to the first four. Conventionally, the range of the emitted beta or conversion electrons has been used to define the appropriate radionuclide for a particular size of joint. However, the physical half-life of the radionuclide might also be an important consideration in determining the better applications of a particular radionuclide. *NIST ESTAR database for electron CSDA ranges: http://physics.nist.gov/PhysRefData/Star/Text/ESTAR.html †Numerous sources state that the average range of Er-169 in tissue is 0.3 mm

Premise and Hypothesis Conventional Premise: One should choose a radionuclide that has an electron range in tissue that is commensurate with the size of the joint synovium. Hypothesis: Migration by macrophages containing longer-lived, short-range radioactive particles into all of the layers of the synovial tissues delivers therapeutic absorbed doses throughout the synovium. In particular, we are studying the hypothesis that a radionuclide with a relatively long half-life and shorter range emissions can effectively treat larger joints, provided that it is taken up by the macrophages and transported into the deeper portions of the synovial tissue.

Model of the Synovial Joint The model of the synovial joint that we used was developed by Scott Johnson in the early 1990’s. It is for a mildly arthritic joint in which the synovial lining is about 300 microns thick. On the small scale of the range of beta particles, the rippling nature of the synovial membrane is approximated by parallel planes. The layers consist of bone, a millimeter of cartilage, 440 microns of capsular space containing the synovial fluid, 300 microns of synovial lining and then deeper synovial tissue. In Johnson’s work, the radioactivity was assumed to be distributed uniformly within the capsule and the cells of the synovial lining. We have investigated three distributions of the five radionuclides: stationary activity at the interface between the capsule and the lining, stationary activity uniformly distributed within the capsule and the lining, and activity that starts out in the capsule and the lining and migrates deeper and deeper into the synovial tissue over time. LS Johnson, Beta-Particle Dosimetry in Radiation Synovectomy and Use of the 10B(n,α) Nuclear Reaction to Examine the Pathology of Rheumatoid Arthritis, PhD, Massachusetts Institute of Technology, 1994, p. 65. Figure used with the permission of Dr. Johnson.

Monte Carlo Simulation GATE 8.0 Monte Carlo simulations The source definitions were built using the complete radionuclide emissions data from ICRP 107. Johnson’s model was built as a stack of 4 cm-diameter disks of the specified thicknesses for each layer. The spatial resolution perpendicular to the synovial tissue was 0.1 mm. The GATE materials were “Rib Bone” for the bone, “Cartilage” for the cartilage, “Water” for the capsule and “Muscle” for the synovium. The QBBC_EMY physics list was used. Two million events were simulated for each scenario. We used the GATE Monte Carlo software in order to perform these simulations. The source files for each radionuclide contain every emission in the ICRP 107 data base. We implemented Johnson’s model as a stack of 4 cm-diameter disks with the specified thicknesses. The spatial resolution of the dose actor was 0.1 mm perpendicular to the layers of the model. We used standard GATE material definitions and the QBBC_EMY physics list. Two million events were simulated for each scenario.

Stationary Activity on the Surface of the Synovial Lining When all of the activity is stationary at the plane separating the capsule from the lining, the spatial distributions of radiation absorbed dose of the various radionuclides are similar to their beta dose kernels. They have spatial extents that correspond to their average and maximum electron ranges since the dose is largely imparted by the non-penetrating emissions. In this plot, the activity of each radionuclide was chosen to deliver the same dose as 1 MBq/cm2 of Sn-117m.

Stationary Activity in Capsule and Lining When the stationary activity is uniformly distributed within the capsule and the synovial lining, there is a similar relative spatial distribution of radiation absorbed dose. Note that the lower energy radionuclides, Er-169 and Sn-117m, treat very little of the deeper synovial tissue in this scenario.

Macrophage Action Radioactive colloidal particles are collected on the synovial lining and then transported deeper into the synovial tissue. However, there is evidence that suitably sized radioactive colloidal particles are eventually transported deeper into the synovial tissue. These autoradiographs were made seven weeks after treatment with a Sn-117m colloid. 100× 400× The arrow (→) indicates an area of inflammation in the autoradiographs.

Model of Moving Radioactivity × We modeled this transportation and the resulting dose distribution in a discrete fashion. We assumed that the activity in the capsule would disappear within two weeks while the activity in the lining would increase slightly until the third week, after which it would remain steady. We assumed that the activity in the deeper layers of the synovial tissue would demonstrate delayed uptake curves that would level out to a uniform distribution by the end of the ninth week. We simulated the spatial distributions of dose per disintegration from each of the radionuclides uniformly distributed in each of six layers: the capsule, the lining, and four subintimal layers. These doses were then multiplied by the relative activity at their locations and the cumulated activity at those locations and times to produce a total dose distribution once the activity had completely decayed. =

Moving Source Dose Distributions The results of simulating moving distributions of the five radionuclides is shown with two normalizations. One is to deliver the same dose to the interface between the capsule and the lining and the other is to deliver the same dose to the center of the lining. In particular, note that the dose that is delivered to the deeper layers of the synovial tissue is very similar for Re-186, Er-169 and Sn-117m. At the same time, Er-169 and Sn-117m spare deliver a substantially lower dose to the cartilage and bone than do the other radionuclides. Nuclide Rel. Act. Sn-117m 1.00 Er-169 2.20 Y-90 2.65 Re-186 2.47 P-32 0.463 Nuclide Rel. Act. Sn-117m 1.00 Er-169 2.41 Y-90 4.10 Re-186 3.50 P-32 0.615

Discussion and Conclusion The relatively long half-lives of P-32, Er-169 and Sn-117m potentially allow them to be carried well into the synovial tissue before depositing all of their energy, assuming a suitable particle size. With the movement model in this study, the dose distributions of Er-169, Re-186 and Sn-117m are very similar. The further investigation of Sn-117m for the radiosynoviorthesis of medium-sized as well as smaller-sized joints is warranted. It is thus important to design a colloid that the macrophages will transport deeply into the synovial tissue. With such a colloid, Er-169, Re-186 and Sn-117m appear to deliver similar doses to the synovial tissue. We thus conclude that Sn-117m should be investigated for use in medium- as well as smaller-sized joints.