Energy response of an imaging plate exposed to standard beta sources.

Imaging plates (IPs) are a reusable media, which when exposed to ionizing radiation, store a latent image that can be read out with a red laser as photostimulated luminescence (PSL). They are widely used as a substitute for X-ray films for diagnostic studies. In diagnostic radiology this technology is known as computed radiography. In this work, the energy response of a commercial IP to beta-particle reference radiation fields used for calibrations at the National Institute of Standards and Technology was investigated. The absorbed dose in the active storage phosphor layer was calculated following the scaling procedure for depth dose for high Z materials with reference to water. It was found that the beta particles from Pm-147 and Kr-85 gave 68% and 24% higher PSL responses than that induced by Sr-90, respectively, which was caused by the different PSL detection efficiencies. In addition, normalized response curves of the IPs as a function of depth in polystyrene were measured and compared with the data measured using extrapolation chamber techniques. The difference between both sets of data resulted from the continuous energy change as the beta particle travels across the material, which leads to a different PSL response.

A dose-point-kernel model for a low energy gamma-emitting stent in a heterogeneous medium.

A computer dose model for a low energy gamma-emitting stent in a heterogeneous medium is described. The method is based on the Sievert model which is adapted to the dose-point-kernel (DPK) model to compute the dose distribution about filtered gamma sources (Sievert-DPK model). The new gamma stent model can take into account effects such as the metallic wire attenuation and the presence of dense calcified plaque in a stented artery. The Sievert-DPK model is tested against numerical simulations around cylindrical shell sources with dimensions comparable to those of a stent using a Monte Carlo transport code. For low energy gamma sources (Cs-131 and Pd-103), it is shown that the Sievert-DPK model is consistent with the Monte Carlo results to about 5%-10% for distances up to 5 mm from the cylindrical surface and 2.5 mm beyond the cylinder edges. These results indicate that the Sievert-DPK model may be useful to predict the dose in intravascular therapy applications for heterogeneous systems consisting of soft tissue, metal and dense plaque.

Dosimetry of the I-Plant Model 3500 iodine-125 brachytherapy source.

125I brachytherapy sources have been widely used for interstitial implants for a number of years in several tumor sites, especially the prostate. The design of the new I-Plant Model 3500 iodine source is novel, yet its characteristics are similar to those of two existing designs, Model 6711 and the Symmetra. Dosimetry parameters (including dose rate constant, radial dose function, and anisotropy function, as defined by AAPM Task Group 43) were measured with LiF thermoluminescent dosimeters in water-equivalent plastic phantoms. The dose rate constant was found by direct comparison of calibrated I-Plant Model 3500 and Model 6711 seeds in a solid water phantom, to be 1.01 (cGy/h)/U. The radial dose function and anisotropy function are similar to those of the Model 6711 and Symmetra seeds.

Dose model for a beta-emitting stent in a realistic artery consisting of soft tissue and plaque.

A model for the description of the near-field dose deposition from a 32p impregnated stent in an arterial system consisting of soft tissue and dense plaque is presented. The model is based on the scaling property of the dose-point-kernel (DPK) function which is extended to a heterogeneous medium consisting of a series of layers of different materials. It is shown that, for each point source originating from the stent surface, the DPK function for water can be scaled consistently along the path through the different layers of material to predict the dose at a given point in the heterogeneous medium. Radiochromic film dosimetry on actual 32p stents is used to test the new model. The experimental setup consists of a water-equivalent phantom in which a stent is deployed and on which a thin layer of polytetrafluoroethylene (PTFE) is deposited to simulate the presence of plaque. Layers of radiochromic films stacked over the phantom are used to measure the dose at distances varying from approximately 0.1 mm to approximately 3 mm from the stent surface with and without PTFE. It is shown that the proposed new DPK model for a heterogeneous medium agrees very well with the experimental data and that it compares favorably to the usual homogeneous DPK model. These results indicate that the new model can be used with confidence to predict the dose in a realistic artery in the presence of plaque.

Radiochromic film dosimetry of a high dose rate beta source for intravascular brachytherapy.

Good clinical physics practice requires that dose rates of brachytherapy sources be checked by the institution using them, as recommended by American Association of Physicists in Medicine Task Group 56 and The American College of Radiology. For intravascular brachytherapy with catheter-based systems, AAPM Task Group 60 recommends that the dose rate be measured at a reference point located at a radial distance of 2 mm from the center of the catheter axis. AAPM Task Group 60 also recommends that the dose rate along the catheter axis at a radial distance of 2 mm should be uniform to within +/- 10% in the center two-thirds of the treated length, and the relative dose rate in the plane perpendicular to the catheter axis through the center of the source should be measured at distances from 0.5 mm to R90 (the distance from a point source within which 90% of the energy is deposited) at intervals of 0.5 mm. Radiochromic film dosimetry has been used to measure the dose distribution in a plane parallel to and at a radial distance of 2 mm from the axis of a novel, catheter-based, beta source for intravascular brachytherapy. The dose rate was averaged along a line parallel to the catheter axis at a radial distance of 2 mm, in the centered 24.5 mm of the treated length. This average dose rate agreed with the dose rate measured with a well ionization chamber by the replacement method using source trains calibrated with an extrapolation chamber at the National Institute of Standards and Technology. All of the dose rates in the centered 24.5 mm of a line parallel to the axis at a distance of 2 mm were within +/-10% of the average.

Measurement of density and calcium in human atherosclerotic plaque and implications for arterial brachytherapy.

PURPOSE: To measure density of arterial plaque specimens for purposes of improving calculation of intravascular radiation dose. METHODS AND MATERIALS: In the described technique, the mass of the specimen submerged in water is compared with its mass in air. Thirty-three plaque specimens harvested from cadavers and subsequently histologically classified (18 coronary, 15 noncoronary) were subjected to density measurement, and were also assayed for calcium using inductively coupled plasma optical emission spectroscopy (ICPOES). A dose point kernel (DPK) computer model extended to heterogeneous media is used to determine delivered dose to tissues for stents labeled with 32P, 103Pd, and 131Cs, based on measured density values. RESULTS: Plaque specimens identified histologically as noncalcified (non-class VII) had an average density of 1.22 +/- 0.03 g/cm3 (n = 19). Plaque specimens identified as calcified (Class VII) had an average density of 1.45 +/- 0.06 g/cm3 (n = 13). Density of calcified portions of plaque may be even higher because plaque specimens are heterogeneous. Plaque density was found to be correlated with calcium weight percentage (R2 = 0.67) and histologic percent area calcification (R2 = 0.58). Significant variations in calculated dose were found according to isotope, plaque density, and plaque thickness. The assumption of an "all water density" dose model overestimates dose to tissues. For 1-mm thick calcified (class VII) plaque, computed dose to tissues (via DPK model) are decreased by 29%, 34%, and 15%, for 32P, 103Pd, and 131Cs stents, respectively, compared with an "all water density" assumption model, when density is taken into account. Similar decreases are expected for catheter-based brachytherapy systems using beta or low energy (< 100 keV) gamma sources. CONCLUSIONS: This work has importance for radioactive stents and catheter-based brachytherapy due to dependence of dose on density at distances between 0.1 mm and 3 mm away from the radiation source. This dependence is important for both beta- and gamma-based systems.

Small photon field dosimetry for stereotactic radiosurgery.

Performing and assuring the quality of the planning and delivery of stereotactic radiosurgery with photon beams requires accurate evaluation of beam parameters, usually including output factors, tissue-phantom ratios and off-axis ratios, and measurement of actual dose distributions from simulated treatments. For the small photon fields used in radiosurgery, these measurements require special equipment and techniques, which are described in this review.

Dose distribution for a 32P-impregnated coronary stent: comparison of theoretical calculations and measurements with radiochromic film.

PURPOSE: Restenosis, caused by proliferation of smooth-muscle cells, limits the efficacy of catheter-based revascularization of coronary arteries. Irradiation has been shown to inhibit growth of smooth-muscle cells in vitro and to prevent restenosis in animal models following stent placement. An intraarterial source of 32P, a pure beta emitter with a half-life of 14.28 days and a 90% range in water of 3.6 mm, is almost ideal for irradiating just arterial wall without exposing any other part of the patient's heart or any other organs, while posing minimal hazards to medical personnel. Two types of previously developed coronary stent impregnated with 32P were investigated. This study aimed to calculate and measure the dose outside of two types of 32P-impregnated beta-emitting coronary stents under conditions closely simulating clinical use. METHODS AND MATERIALS: The dose distributions in water surrounding these stents were calculated using a convolution method and measured by exposing radiochromic film in a solid-water phantom. RESULTS: Experimental results were in excellent agreement with theoretical calculations. CONCLUSIONS: Radiochromic dosimetry can be used to measure the dose distribution around a beta-emitting intraarterial stent at distances as small as 0.1 mm from the stent surface. A simple cylindrical shell model is adequate for calculating the dose at points farther than 0.5 mm from the stent surface.

Radiation dose from a phosphorous-32 impregnated wire mesh vascular stent.

The near field dose distribution of a realistic vascular stent impregnated with radioactive 32P is calculated employing the dose-point-kernel (DPK) method in a homogeneous and uniform medium. The cylindrical wire mesh geometry for the Palmaz-Schatz [Palmaz-Schatz is a tradename of Cordis (a Johnson & Johnson company)] stent is incorporated in the model calculation, and the dose distribution generated by the beta particles emitted from the decayed radioactive 32P is computed at distances ranging from 0.1 to 2 mm exterior to the stent surface. Dose measurements were obtained using radiochromic film dosimetry media on an actual Palmaz-Schatz half-stent impregnated with 32P using ion implantation, and compared to the DPK model predictions. The close agreement between the model calculation and the film dosimetry data confirms the validity of the model which can be adapted to a variety of different stent designs.

Use of a micro-ionization chamber and an anthropomorphic head phantom in a quality assurance program for stereotactic radiosurgery.

Quality assurance methods used in association with radiosurgery must include all aspects of the radiosurgery process: visualization and localization of the target, treatment and dose planning and dose delivery. Presented here is a quality assurance method that utilizes an anthromorphic head phantom and a micro-ionization chamber to demonstrate precise target localization and accurate dose delivery. This micro-ionization chamber method offers an immediate readout which is both accurate and reproducible. Additionally, this method allows unlimited repetition of the dose measurement process without repeated radiographic localization studies as is necessary with the conventional methods of TLD, film, and Fricke gels. The method and techniques presented can be used in the acceptance testing and routine quality assurance of both linac-based and Gamma Knife radiosurgery units.

Low-dose, beta-particle emission from 'stent' wire results in complete, localized inhibition of smooth muscle cell proliferation.

BACKGROUND: Restenosis after catheter-based revascularization has been demonstrated to be primarily caused by medial and/or intimal smooth muscle cell (SMC) proliferation. The objective of this study was investigate the ability of local emission of beta-particles from a 32P-impregnated titanium "stent" wire source to inhibit vascular SMC and endothelial cell proliferation in cell culture and to determine the dose-response characteristics of this inhibition. METHODS AND RESULTS: A series of experiments were performed using 0.20-mm-diameter titanium wires that were impregnated with varying low concentrations of 32P (activity range, 0.002 to 0.06 microCi/cm wire, n = 47) or 31P (nonradioactive control, n = 28) in cultures of rat and human aortic SMCs and in cultured bovine aortic endothelial cells. The zone of complete cell growth inhibition (in millimeters from stent wire) was measured using light microscopy in the cultures exposed to the radioactive (32P) or control (31P) wires at 6 and 12 days after plating. In both rat and human SMC cultures there was a distinct 5.5- to 10.6-mm zone of complete SMC inhibition at wire activity levels > or = 0.006 microCi/cm. In contrast, there was no zone of inhibition surrounding the control (31P impregnated) wires (P < .001 versus 32P wires at all wire activities > or = 0.006 microCi/cm for human and rat SMCs). Proliferating bovine endothelial cells were more radioresistant than SMCs, with no zone of inhibition observed at wire activity levels up to 0.019 microCi/cm (P < .001 versus SMCs at 0.006 microCi/cm and 0.019 microCi/cm). CONCLUSIONS: We conclude that very low doses of beta-particle emission from a 32P-impregnated stent wire (activity levels as low as 0.006 microCi/cm of wire) completely inhibit the growth and migration of both rat and human SMCs within a range of 5.5 to 10.6 mm from the wire. Endothelial cells appear to be much more radioresistant than SMCs. These data suggest that an intra-arterial stent impregnated with a low concentration of 32P may have a salutary effect on the restenosis process. Whether this approach can be used successfully and safely to inhibit restenosis in vivo and in the clinical setting is under investigation.