In recent nanotechnology development, iron-based magnetic nanoparticles (MNPs) have been used in several
investigations on biomedical research for small animal experiments. Their important applications include targeted drug
delivery for therapeutic purpose, contrast agent for magnetic resonance imaging, and hyperthermia treatment for tumors.
These MNPs can be guided by an external magnetic field due to their physical characteristics of superparamagnetism. In
a recent report, authors indicated that covalently bound recombinant tissue plasminogen activator (rtPA) to MNP (MNPrtPA)
with preserved enzyme activity may be guided by a bar magnet and induce target thrombolysis in an embolic
model in rats. Delivery of rtPA by binding the thrombolytic drug to MNPs will improve the possibility of the drug to be
delivered under magnetic guidance and retained in a local targeted area in the circulation system. In this work, an ex vivo
intravascular thrombolysis model was developed to study the impact of external magnetic field on the penetration of
MNP-rtPA in the blood clot samples. The samples were then scanned by a micro CT system for quantification. Images of
MNPs show strong contrast with their surrounding blood clot materials. The optimum drug loading was found when 0.5
mg/ml rtPA is conjugated with 10 mg SiO2-MNP where 98% drug was attached to the carrier with full retention of its
thrombolytic activity. Effective thrombolysis with tPA bound to SiO2-MNP under magnetic guidance was demonstrated
in our ex vivo model where substantial reduction in time for blood clot lysis was observed compared with control groups
without magnetic field application.
In recent years, there has been a rapid research progress of molecular imaging technology. Many investigations in
molecular imaging such as the nanoparticle applications in targeted drug delivery have been widely studied in several
key small animal models. Various nanoparticles used as either the drug delivery carriers, imaging contrast mediums or
target-specific therapeutic agents have established a novel research platform for biomedical related scientists and
clinicians. Among these nanoparticles, gold nanoparticles have the unique non-toxic and stability properties. In this
work, a commercially-available micro CT imaging system was used to specifically study the imaging properties for 15
nm spherical-shaped gold particles. Imaging properties were quantified by the CT numbers obtained from a series of
photon energy levels in the micro CT scanner. We also compared the imaging results between gold nanoparticles and
iodinated contrast medium to study the potential impact of gold nanoparticles served as the contrast agent.
KEYWORDS: X-ray computed tomography, Imaging systems, Tumors, Animal model studies, Radiotherapy, Monte Carlo methods, Molecular imaging, X-rays, Scanners, Photon transport
In recent years, there has been an increasing number of integration for using the micro CT scanners, either home-built
bench-top or commercially made, as the small animal radiation therapy irradiator in several research groups. In this
paper, we study the x-ray beam physics such as the percentage depth dose distribution and their dose conformity
characteristics using Monte Carlo simulation method for a series of photon energy levels often found in the current
commercial micro CT imaging systems. Micro CT scanners have been one of the key imaging modalities in the current
state-of-the-art molecular imaging techniques and their applications in various biomedical research areas have been
increasing tremendously in recent years due to the ultra-high image quality. Tumor growth development and the
corresponding therapeutic response in the small animal model study can be evaluated by a micro CT imaging system. In
the most current advanced commercially available micro CT units, the nominal spatial resolution is typically at the scale
of 10.0 μm or less. In current research trend, there have been an increasing number of investigations for the applications
of x-ray units to organ-specific and whole-body radiation in dedicated small animal model study. In particular, scientists
have identified that the integrated micro CT imagers can be commissioned as the dual-purpose unit for the high spatial
resolution image acquisition and radiation delivery. As we all realized that small animal models are important and
critical in several studies of experimental (or pre-clinical) radiation therapy research. In this paper, a Monte Carlo code
(Penelope) was used to calculate the percentage depth dose distributions at different photon energy levels. Also the
corresponding iso-dose contour curves were computed and plotted from the circular CT scanning geometry to study the
desired dose conformity property. We note that the selected photon energy range that is included in this work is often
included in the current commercial micro CT systems.
CT numbers can be directly computed from the linear attenuation coefficients in the reconstructed CT images and are
correlated to the electron densities of the chemical elements with specific atomic numbers. However, the computed CT
numbers can be varied when different imaging parameters are used. Phantoms composed of clinically relevant and
tissue-equivalent materials (lung, bone, muscle, and adipose) were scanned with a commercial circular-scanning micro
CT imager. This imaging system is composed with a micro-focused x-ray tube and charged-coupled device (CCD)
camera as the detector. The mean CT numbers and the corresponding standard deviations in terms of Hounsfield units
were then computed from a pre-defined region of interest located within the reconstructed volumetric images. The
variations of CT number were then identified from a series of imaging parameters. Those parameters include imaging
acquisition modes (e.g., the metal filter used in the x-ray tube), reconstruction methods (e.g., Feldkamp and iterative
algorithm), and post-image processing techniques (e.g., ring artifact, beam-hardening artifact, and smoothing
processing). These variations of CT numbers are useful and important in tissue characterization, quantitative bone
structure analysis, bone marrow density evaluation, and Monte Carlo dose calculations for the pilot small animal study
when micro CT imaging systems are employed. Also these variations can be used as the quantification for the
performance of the micro CT imaging systems.
In this work, we investigated the effects of scattered radiation and beam quality on the low contrast performance
relevant to cone beam breast CT imaging. For experiments, we used our benchtop conebeam CT system and constructed
a phantom consisting of simulated fat and soft tissues. We varied the field of view (FOV) along the z direction to observe
its effect on scattered radiation. The beam quality was altered by varying the tube voltage from 50 to 100 kV. We
computed the contrast-to-noise ratio (CNR) from reconstructed images and normalized it to the square root of dose
measured at the center of the phantom. The results were used as the figure of merit (FOM). The effect of the beam
quality on the scatter to primary ratio (SPR) had minimal impact and the SPR was primarily dominated by the FOV. In
the central section of the phantom, increasing the FOV from 4 to 16 cm resulted in drop of CNR in the order of 15-20%
at any given kVp setting. For a given FOV, the beam quality had insignificant effect on the FOM in the central section of
the phantom. In the peripheral section, a 10 % drop in FOM was observed when the kVp setting was increased from 50
to 100. At lower kVp values, the primary x-ray transmission through the thicker parts of the phantom was severely
reduced. Under such circumstances, ring artifacts were observed due to imperfect flat field correction at very low signal
intensities. Higher kVp settings and higher SPRs helped to increase the signal intensity in highly attenuating regions and
suppressed the ring artifacts.
The half-scan cone beam technique, requiring a scan for 180° plus detector width only, can help achieve both shorter scan time as well as higher exposure in each individual projection image. This purpose of this paper is to investigate whether half-scan cone beam CT technique can provide acceptable images for clinical application. The half-scan cone beam reconstruction algorithm uses modified Parker's weighting function and reconstructs from slightly more than half of the projection views for full-scan, giving out promising results. A rotation phantom, stationary gantry bench top system was built to conduct experiments to evaluate half-scan cone beam breast CT technique. A post-mastectomy breast specimen, a stack of lunch meat slices embedded with various sizes of calcifications and a polycarbonate phantom inserted with glandular and adipose tissue equivalents are imaged and reconstructed for comparison study. A subset of full-scan projection images of a mastectomy specimen were extracted and used as the half-scan projection data for reconstruction. The results show half-scan reconstruction algorithm for cone beam breast CT images does not significantly degrade image quality when compared with the images of same or even half the radiation dose level. Our results are encouraging, emphasizing the potential advantages in the use of half-scan technique for cone beam breast imaging.
To investigate how the radiation dose level affects the detection of microcalcifications (MCs) in cone beam breast CT (CBCT), simulated MCs were embedded in simulated breast tissue and imaged with an experimental CBCT system. The system employs a 30 x 40 cm2 a-Si/CsI based flat panel detector with a pixel size of 194 microns. Three 5 x 5 clusters of simulated calcifications (212-224, 250-280, and 300-355 μm) were embedded in a stack of 11 cm diameter lunch meat and positioned at the center of each slice of lunch meat. 300 projection images over 360 degrees were acquired in the non-binning mode at various dose levels (4.2, 6, 12, 18, and 24 mGy) three times, and were reconstructed with the Feldkamp algorithm. After that, 767 x 767 x 9 volume data were extracted from the fifteen reconstructed images for each size group, resulting in 45 CBCT MC phantom images. An observer experiment was performed by counting the number of visible MCs for each MC phantom image. The phantom images were displayed on a review workstation with a 1600 x 1200 CRT monitor and reviewed by six readers independently. The order of the images was randomized for each reader. The ratios of the visible MCs were averaged over all readers and plotted as a function of the dose level. The CNR was calculated for each MC size and each doe level as well. The results showed that the performance of the reconstructed images acquired with 4.2 mGy was similar to the images acquired with 6 mGy, and the images acquired with 18 mGy performed similarly to those acquired with 24 mGy.
Purpose: To compare two detector systems - one based on the charge-coupled device (CCD) and image amplifier, the
other based on a-Si/CsI flat panel, for cone beam computed-tomography (CT) imaging of small animals.
A high resolution, high framing rate detector system for the cone beam CT imaging of small animals was developed. The
system consists of a 2048×3072×12 bit CCD optically coupled to an image amplifier and an x-ray phosphor screen. The
CCD has an intrinsic pixel size of 12 μm but the effective pixel size can be adjusted through the magnification
adjustment of the optical coupling systems. The system is used in conjunction with an x-ray source and a rotating stage
for holding and rotating the scanned object in the cone beam CT imaging experiments. The advantages of the system
include but are not limited to the ability to adjust the effective pixel size and to achieve extremely high spatial resolution
and temporal resolution. However, the need to use optical coupling compromises the detective quanta efficiency (DQE)
of the system. In this paper, the imaging characteristics of the system were presented and compared with those of an a-
Si/CsI flat-panel detector system.
This paper investigates the feasibility of using a flat panel based cone-beam computer tomography (CT) system for 3-D breast imaging with computer simulation and imaging experiments. In our simulation study, 3-D phantoms were analytically modeled to simulate a breast loosely compressed into cylindrical shape with embedded soft tissue masses and calcifications. Attenuation coefficients were estimated to represent various types of breast tissue, soft tissue masses and calcifications to generate realistic image signal and contrast. Projection images were computed to incorporate x-ray attenuation, geometric magnification, x-ray detection, detector blurring, image pixelization and digitization. Based on the two-views mammography comparable dose level on the central axis of the phantom (also the rotation axis), x-ray kVp/filtration, transmittance through the phantom, detected quantum efficiency (DQE), exposure level, and imaging geometry, the photon fluence was estimated and used to estimate the phantom noise level on a pixel-by-pixel basis. This estimated noise level was then used with the random number generator to produce and add a fluctuation component to the noiseless transmitted image signal. The noise carrying projection images were then convolved with a Gaussian-like kernel, computed from measured 1-D line spread function (LSF) to simulated detector blurring. Additional 2-D Gaussian-like kernel is designed to suppress the noise fluctuation that inherently originates from projection images so that the reconstructed image detectability of low contrast masses phantom can be improved. Image reconstruction was performed using the Feldkamp algorithm. All simulations were performed on a 24 PC (2.4 GHz Dual-Xeon CPU) cluster with MPI parallel programming. With 600 mrads mean glandular dose (MGD) at the phantom center, soft tissue masses as small as 1 mm in diameter can be detected in a 10 cm diameter 50% glandular 50% adipose or fatter breast tissue, and 2 mm or larger masses are visible in a 100% glandular 0% adipose breast tissue. We also found that the 0.15 mm calcification can be detected for 100μm detector while only 0.2 μm or above are visible for 200 μm detector. Our simulation study has shown that the cone-beam CT breast imaging can provide reasonable good quality and
detectability at a dose level similar to that of two views\mammography. For imaging experiments, a stationary x-ray source and detector, a step motor driven rotating phantom system was constructed to demonstrate cone beam breast CT image. A breast specimen from mastectomy and animal tissue embedded with calcifications were imaged. The resulting images show that 355-425 μm calcifications were visible in images obtained at 77 kVp with a voxel size of 316 μm and a center dose of 600 mrads. 300-315 μm calcifications were visible in images obtained at 60 kVp with a voxel size of 158 μm and a center dose of 3.6 rads.
We have developed a computer simulation model for cone beam computed tomography (CT) chest imagingon a general-purpose personal computer cluster system. Our simulation model incorporates quantum noise, detector blurring, and additive system noise.The main objective is to study how x-ray dose would affect the detectabilityof nodules in simulated cone beam CT chest images. The Radon transforms formalism was used to calculate the projection views for an analytically modeled chest phantom. A parallel random number generator was then
used to simulate and add quantum noise whose level depends on the
incident x-ray fluence, detector quantum efficiency and pixel size (0.4 mm).We also simulated detector blurring by convolving the
noise added images with a Gaussian function matching the modulation transfer function measured for the flat panel x-ray detector studied.
Then we modeled the additive system noise and added to the final projection images.The noise level (σ=20) for the additive system noise was calculated from the noise power spectrum of the flat panel detector using the curve-fitting technique.The Feldkamp algorithm with a Gaussian pre-filtering processwas used to reconstruct 3D image data from the projection images.For nodule contrast, the linear attenuation coefficient difference between nodule and lung was set to 10.0%. The diameters for the spherical nodules ranged from 0.2 to 1.7 cm. It was found that our Gaussian pre-filtering process helped reduce the noise level in the reconstructed images and allowed the nodules to be better visualized significantly. At 100,000 photons per pixel (8000 mR total unattenuated exposure at the rotating center), nodules 0.3 mm or larger could be visualized; at 10,000 photons per pixel( 800 mR), nodules 0.5 mm or larger could be visualized; at 2000 photons per pixel (160 mR), only nodules 1.5 mm or larger could be visualized.
Slot scanning imaging techniques allow for effective scatter rejection without attenuating primary x-rays. The use of these techniques should generate better image quality for the same mean glandular dose (MGD) or a similar image quality for a lower MGD as compared to imaging techniques using an anti-scatter grid. In this study, we compared a slot scanning digital mammography system (SenoScan, Fisher Imaging Systems, Denver, CO) to a full-field digital mammography (FFDM) system used in conjunction with a 5:1 anti-scatter grid (SenoGraphe 2000D, General Electric Medical Systems, Milwaukee, WI). Images of a contrast-detail phantom (University Hospital Nijmegen, The Netherlands) were reviewed to measure the contrast-detail curves for both systems. These curves were measured at 100%, 71%, 49% and 33% of the reference mean glandular dose (MGD), as determined by photo-timing, for the Fisher system and 100% for the GE system. Soft-copy reading was performed on review workstations provided by the manufacturers. The correct observation ratios (CORs) were also computed and used to compare the performance of the two systems. The results showed that, based on the contrast-detail curves, the performance of the Fisher images, acquired at 100% and 71% of the reference MGD, was comparable to the GE images at 100% of the reference MGD. The CORs for Fisher images were 0.463 and 0.444 at 100% and 71% of the reference MGD, respectively, compared to 0.453 for the GE images at 100% of the reference MGD.
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