Modern amorphous silicon flat panel-based electronic portal imaging devices that utilize thin gadolinium oxysulfide scintillators suffer from low quantum efficiencies (QEs). Thick two dimensionally (2D) pixelated scintillator arrays offer an effective but expensive option for increasing QE. To reduce costs, we have investigated the possibility of combining a thick one dimensional (1D) pixelated scintillator (PS) with an orthogonally placed 1D structured optical filter to provide for overall good 2D spatial resolution. In this work, we studied the potential for using a 1D video screen privacy film (PF) to serve as a directional optical attenuator and filter. A Geant4 model of the PF was built based on reflection and transmission measurements taken with a laser-based optical reflectometer. This information was incorporated into a Geant4-based x-ray detector simulator to generate modulation transfer functions (MTFs), noise power spectra (NPS), and detective quantum efficiencies (DQEs) for various 1D and 2D configurations. It was found that the 1D array with PF can provide the MTFs and DQEs of 2D arrays. Although the PF significantly reduced the amount of optical photons detected by the flat panel, we anticipate using a scintillator with an inherently high optical yield (e.g. cesium iodide) for MV imaging, where fluence rates are inherently high, will still provide adequate signal intensities for the imaging tasks associated with radiotherapy.
Flat panel imagers based on amorphous silicon technology (a-Si) for digital radiography are accepted by the medical
and industrial community as having several advantages over radiographic film-based systems. Use of Mega-voltage
x-rays with these flat panel systems is applicable to both portal imaging for radiotherapy and for nondestructive
testing (NDT) and security applications. In the medical field, one potential application that has not been greatly
explored is to radiotherapy treatment planning. Currently, such conventional computed tomographic (CT) data
acquired at kV energies is used to help delineate tumor targets and normal structures that are to be spared during
treatment. CT number accuracy is crucial for radiotherapy dose calculations. Conventional CT scanners operating at
kV X-ray energies typically exhibit significant image reconstruction artifacts in the presence of metal implants in
human body. Using the X-ray treatment beams, having energies typically ≥6MV, to acquire the CT data may not be
practical if it is desired to maintain contrast sensitivity at a sufficiently low dose. Nondestructive testing imaging
systems can expand their application space with the development of the higher energy accelerator for use in
pipeline, and casting inspection as well as certain cargo screening applications that require more penetration. A new
prototype x-band BCL designed to operate up to 1.75 MV has been designed built and tested. The BCL was tested
with a prototype portal imager and medical phantoms to determine artifact reductions and a PaxScan 2530HE
industrial imager to demonstrate resolution is maintained and penetration is improved.
Scintillating Fiber Optic Plates (SFOP) or Fiber Optic Scintillator (FOS) made with scintillating fiber-glass, were
investigated for x-ray imaging. Two different samples (T x W x L = 2cm x 5cm x 5cm) were used; Sample A: 10μm
fibers, Sample B: 50μm fibers both with statistically randomized light absorbing fibers placed in the matrix. A
customized holder was used to place the samples in close contact with photodiodes in an amorphous silicon flat panel
detector (AS1000, Varian), typically used for portal imaging. The detector has a 392μm pixel pitch and in the standard
configuration uses a gadolinium oxy-sulphide (GOS) screen behind a copper plate. X-ray measurements were performed
at 120kV (RQA 9 spectrum), 1MeV (5mm Al filtration) and 6MeV (Flattening Filter Free) for Sample A and the latter 2
spectra for Sample B. A machined edge was used for MTF measurements. The measurements showed the MTF
degraded with increased X-ray energies because of the increase in Compton scattering. However, at the Nyquist
frequency of 1.3lp/mm, the MTF is still high (FOS value vs. Cu+GOS): (a) 37% and 21% at 120kVp for the 10μm FOS
and the Cu+GOS arrays, (b) 31%, 20% and 20% at 1MeV and (c) 17%, 11% and 14% at 6MeV for the 10μm FOS,
50μm FOS and the Cu+GOS arrays. The DQE(0) value comparison were (a) at 120kV ~24% and ~13 % for the 10μm
FOS and the Cu+GOS arrays (b) at 1MV 10%, 10% and 7% and (c) at 6MV 12%, ~19% and 1.6% for the 10μm FOS ,
50μm FOS and Cu+GOS arrays.
In order to predict and improve the performance of pixelated detectors, it is important to understand the optical
properties of the basic unit of the scintillating structure in the detector. To measure one of the essential optical properties,
reflectance, we have used a device composed of a laser and photodiode array. We have also developed an analytical
model of the optical phenomena based on Snell's law and the Fresnel equations to simply analyze measured results and
reflectance parameters at the interface. The computed and experimentally measured results typically have good
agreement, validating the analytical model and measurements. The optical parameters are used as inputs to GEANT4 [1].
The simulations are then leveraged to optimize an imager design before a prototype is built.
The optical reflectance was measured by using relatively inexpensive samples. A sample has scintillator, glue, and
septum (reflector) layers, and each sample has a different scintillator surface (polished/rough) and/or reflector [ESR
film/aluminum-sputtered (coated) ESR film] condition. A high-refractive-index hemisphere was attached on the top
surface of a sample to increase the maximum incidence angle at the scintillator-glue interface from 27° to 52°. The
sample including ESR film demonstrated average reflectance approximately 1.3 times higher than that from the sample
with aluminum-sputtered ESR film as a reflector, and the polished surface condition showed higher reflectance than the
rough-cut surface condition.
The Modulation Transfer Function (MTF) is a quantitative function based on frequency resolution that characterizes
imaging system performance. In this study, a new MTF methodology is investigated for application to Radiography by
Selective Detection (RSD), an enhanced single-side x-ray Compton backscatter imaging (CBI) technique which detects
selected scatter components. The RSD imaging modality is a unique type of real-time radiography that uses a set of fin
and sleeve collimators to preferentially select different components of the x-ray backscattered field. Radiography by
selective detection has performed successfully in different non-destructive evaluation (NDE) applications. A customized
RSD imaging system was built at the University of Florida for inspection of the space shuttle external tank spray-on
foam insulation (SOFI). The x-ray backscatter RSD imaging system has been successfully used for crack and corrosion
detection in a variety of materials. The conventional transmission x-ray image quality characterization tools do not apply
for RSD because of the different physical process involved. Thus, the main objective of this project is to provide an
adapted tool for dynamic evaluation of RSD system image quality. For this purpose, an analytical model of the RSD
imaging system response is developed and supported. Two approaches are taken for the MTF calculations: one using the
Fourier Transform of a line spread function and the other one using a sine function pattern. Calibration and test targets
are then designed according to this proposed model. A customized Matlab code using image contrast and digital curve
recognition is developed to support the experimental data and provide the Modulation Transfer Functions for RSD.
A new Compton x-ray backscatter imaging technique, backscatter radiography by selective detection (RSD), has been used for inspection of the spray-on-foam-insulation (SOFI) on the space shuttle external tank. RSD employs detection of selected backscatter field components, by using specially designed detectors with movable detector collimators, to achieve high image contrast. The optimization study utilized test panels with simulated and natural defects in the spray-on foam insulation. Some of the test panels include structural features, stiffener-stringers and connection flanges, which were bolted to an aluminum base plate representative of the external tank. The SOFI was then layed down over the base plate and structural components with thicknesses varying from a few tens of mm up to a few hundred mm. The simulated defects range in cross-sectional size from 6 × 6 mm to 50 × 50 mm. Natural defects including roll-over voids and knit-line delaminations have a wide range of sizes, geometries, and orientations with a minimum critical cross-sectional size of 6 mm. Imaging registration is currently obtained at 0.05 seconds per 2 mm pixel, or about 19 minutes per 0.093 m2(1 ft2). The current system is being evaluated to enhance the detection of natural defects of a minimal critical size. Monte Carlo (MC) simulations with MCNP5 are being used to determine the history and corresponding spectrum of the detected photons that are responsible for improving defect image contrast. The simulation results are used in combination with experimental data to select optimal detector configurations. Detector configurations are sensitive not only to the type of defect being detected, but also the defect's depth in SOFI, distance from aluminum substrate, and defect orientation. Additional parameters including detector type, detection mode, and x-ray illumination beam size were also evaluated. Both NaI and plastic (BC404) scintillation detectors in pulse and integral mode were used to determine their effect on image quality and defect detection sensitivity. The x-ray illumination beam geometry (round versus square) and beam spot size were varied to determine resolution and the effect on defect contrast. The current system using pulse mode NaI detectors, and a 2 mm round x-ray illumination beam can detect the presence of the smallest critical size defects at a scan rate of 0.05 seconds per 2 mm pixel.
A new Compton x-ray backscatter imaging technique called lateral migration radiography (LMR) has been successfully applied to the detection of voids and delaminations in the foam thermal insulation used on the shuttle external tank. LMR employs detection of selected scatter field velocity components, by using specially designed detectors and detector collimators, to achieve high image contrast.
LMR is based on image contrast generated by migration of probe x-ray radiation in directions transverse to the illumination radiation beam. Because LMR is sensitive to electron density variations in these directions, thin, but large density variations, such as cracks and delaminations, generate signal-to-background ratios sufficient to produce images of features which are not even detectable in the usually interrogated thin dimension. The examined foam thermal insulation test panels consist of aluminum plates onto which the sprayed-on foam insulation (SOFI) is applied. Some of the test panels include structural features bolted to the base plate. The SOFI was layed down over the base plate and structure with a thickness varying from a few tens of mm up to a few hundred mm. The test panels included voids and simulated delaminations in the SOFI ranging in cross-sectional size from 6 x 6 mm to 50 x 50 mm. High quality images were acquired using pixels of 2 to 3 mm and irradiation times as low as 0.05 s per pixel.
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