KEYWORDS: Temperature metrology, Ablation, Thermometry, Computed tomography, Reconstruction algorithms, X-ray computed tomography, Medical image reconstruction, Data modeling, Temperature sensors, X-rays
In this work, we aimed to investigate the sensitivity of spectral CT to changes in temperatures. Moreover, we assessed the accuracy and precision of spectral CT to provide temperature mapping within the treatment volume in CT-guided hypo- and hyper-thermal tumor ablations. Leveraging optical temperature sensors and a 3D printed phantom holder designed to precisely position metallic thermal ablation applicators and reduce the associated image artifacts, we collected spectral CT data spanning a wide range of temperatures (-100 to +90°C) and used a robust theoretical model to fit these distributions for both conventional and spectral CT data. From these expressions, look-up tables that map temperature to CT were generated within the temperature range of interest for cryoablation and hyperthermal ablations, respectively. Consistent with expectations from theoretical models for a water-based gel material, we demonstrated similar sensitivity for conventional and spectral results, with a 3-fold increase in sensitivity in the heating temperature range compared to frozen material. Next, we used repeated scans of a multi-energy phantom to determine the imaging protocol that yield the highest precision (standard deviation of average signal through repeated measurements) in CT signal at the radiation dose levels used in our practice for treatment monitoring during thermal ablation. Our data revealed the complex interplay among radiation dose, image noise, and material decomposition accuracy for spectral data. With a 5mGy CTDIvol limit, we obtained a standard deviation of the average value within a 33 mm3 VOI value of 0.85HU-equivalent for electron density images, corresponding to a precision of 7°C and 2°C for frozen and heated gel, respectively. Conventional image data, including with the application of an in-house CNN denoising algorithm, was unable to reduce the standard deviation of ROI measurements below 1HU. This information was used to develop a clinical-ready CT thermometry protocol that was subsequently independently tested on hyper-thermal measurements, demonstrating an accuracy (root mean square error) in temperature estimates of <8°C for heated gel.
Computed tomography (CT) is routinely used to guide cryoablation procedures. Notably, CT-guidance provides 3D localization of cryoprobes and can be used to delineate frozen tissue during ablation. However, metal-induced artifacts from ablation probes can make accurate probe placement challenging and degrade the ice ball conspicuity, which in combination could lead to undertreatment of potentially curable lesions. An image domain metal artifact simulation framework was developed and validated for deep-learning-based metal artifact reduction for interventional oncology (MARIO). Metal probes and resulting artifacts were segmented from 19 phantom image sets and inserted into 19 different sets of patient CT images to simulate artifacts. This dataset was used to optimize a U-Net type model. Due to unique traits of probe artifacts, we employed custom augmentation techniques and loss functions for model optimization. An ablation study compared performance with and without these additional factors. The combined strategies improved quantitative metrics by 40.95% over baseline training. Augmentations also increased generalizability. Patient cases showed MARIO substantially reduced artifacts while preserving anatomical details. In a reader study, scores from three board-certified radiologists were significantly higher for MARIO processed images compared to the original images across all metrics (all p<0.0001).
Purpose: This work aims to develop a framework to accurately and efficiently simulate metallic objects used during interventional oncology (IO) procedures and their artifacts in computed tomography (CT) images of different body regions.
Approach: A metal insertion framework based on an existing lesion insertion tool was developed. Noise and beam hardening models were incorporated into the model and validated by comparing images of real and artificially inserted metallic rods of known material composition and dimensions. The framework was further validated by inserting ablation probes into a water phantom and comparing image appearance to scans of real probes at matching locations in the phantom. Finally, a comprehensive library of metallic probes used in our IO practice was generated and a graphical user interface was built to efficiently insert any number of probes at arbitrary positions in patient CT data, including projection and image domain insertions.
Results: Metallic rod experiments demonstrated that noise and beam hardening were properly modeled. Phantom and patient data with virtually inserted probes demonstrated similar artifact appearance and magnitude compared with real probes. The developed user interface resulted in accurately co-registered virtual probes both with and without accompanying artifacts from projection and image domain insertions, respectively.
Conclusions: The developed metal insertion framework successfully replicates metallic object and artifact appearance with projection domain insertions and provides corresponding artifact-free images with the metallic object in the identical location through image domain insertion. This framework has potential to generate robust training libraries for deep learning algorithms and facilitate image quality optimization in interventional CT.
Numerous advances in CT imaging have led to improved image guidance for interventional oncology procedures. However, image artifacts stemming from metal devices used during procedures have remained a persistent problem. Severe artifacts introduced by metallic treatment devices significantly degrade image quality in anatomical regions of interest and can substantially reduce the confidence of the interventional radiologist in accurate probe placement. The purpose of this work is to develop a framework to accurately simulate the presence of metal objects in CT images, which could be used for image quality assessment and development of artifact mitigation strategies. The projection domain insertion framework was developed based on an existing lesion insertion tool. New noise and beam hardening models were developed and incorporated into the insertion algorithm to better replicate the artifactual signal produced by the metal objects. These models were validated by comparing images of real and artificially inserted metallic rods with known material composition and dimensions in head and body CT phantoms. The validated model was applied to a single cryoablation probe, which was imaged with routine clinical acquisition parameters and reconstructed with three different sets of reconstruction settings to evaluate their effects on probe segmentation and eventual insertion performance. To determine the optimal digital probe model derived from CT images, the segmented probes were inserted into the projection data from a water phantom and compared to the corresponding water images with the real probe. Additional phantom studies were conducted with two probes positioned such that they were coplanar with the imaging plane, to fully evaluate the severity of the simulated metal artifacts. Finally, a comprehensive library of metallic probes used in our clinical practice during cryoablation and microwave ablation procedures was generated, and an intuitive graphical user interface was built to facilitate efficient insertion of any number of different probes at arbitrary positions in patient CT data. Results from the metallic rod experiments demonstrated that quantum noise, electronic noise, and beam hardening were properly modeled. Further, digital probe models derived from probe images from high resolution reconstructions with an extended HU scale yielded simulated image artifacts consistent with presentation of real artifacts; whereas, using probe models derived from segmentations of clinical reconstructions or high resolution reconstruction without the extended HU scale did not. Extension of the insertion model to two coplanar probes demonstrated production of realistic artifacts with similar magnitude and texture to real probes. Lastly, the model was successfully applied to patient data and generated convincing artifacts as compared to patient images with real probes.
Multiple efforts have been made in x-ray angiography to transition from traditional image quality metrics to mathematical observer models. Recent works have successfully implemented the channelized Hotelling observer (CHO) model for x-ray angiography systems. However, in these works the channel selection process is ambiguous and limits to identifying a range of frequencies and other channel parameters that are believed to represent the most relevant features of the imaging tasks. This channel selection rationale can be sufficient for certain simple scenarios but it might not be enough for more complex ones. On the other hand, it has been shown that besides dealing with the well-known bias caused by a finite number of samples, there is also another source of bias in the estimation of the detectability index in x-ray angiography. Such source of bias has been attributed to nonrandom differences in noise between images acquired at different time points, also referred as temporally variable nonstationary noise. This work proposes a task-specific automated method for optimal channel selection and corrects for the influence of bias due to temporally variable nonstationary noise, particular from x-ray angiography systems. The proposed method is computationally inexpensive, provides time efficient selection of optimal channels, and contributes to minimize bias, all of these without significantly compromising the accuracy of the detectability index estimation. This method for channel optimization can be readily adapted to other imaging modalities.
The use of iterative reconstruction (IR) algorithms in CT generally decreases image noise and enables dose reduction. However, the amount of dose reduction possible using IR without sacrificing diagnostic performance is difficult to assess with conventional image quality metrics. Through this investigation, achievable dose reduction using a commercially available IR algorithm without loss of low contrast spatial resolution was determined with a channelized Hotelling observer (CHO) model and used to optimize a clinical abdomen/pelvis exam protocol. A phantom containing 21 low contrast disks—three different contrast levels and seven different diameters—was imaged at different dose levels. Images were created with filtered backprojection (FBP) and IR. The CHO was tasked with detecting the low contrast disks. CHO performance indicated dose could be reduced by 22% to 25% without compromising low contrast detectability (as compared to full-dose FBP images) whereas 50% or more dose reduction significantly reduced detection performance. Importantly, default settings for the scanner and protocol investigated reduced dose by upward of 75%. Subsequently, CHO-based protocol changes to the default protocol yielded images of higher quality and doses more consistent with values from a larger, dose-optimized scanner fleet. CHO assessment provided objective data to successfully optimize a clinical CT acquisition protocol.
Fundamental to the development and application of channelized Hotelling observer (CHO) models is the selection of the
region of interest (ROI) to evaluate. For assessment of medical imaging systems, reducing the ROI size can be
advantageous. Smaller ROIs enable a greater concentration of interrogable objects in a single phantom image, thereby
providing more information from a set of images and reducing the overall image acquisition burden. Additionally,
smaller ROIs may promote better assessment of clinical patient images as different patient anatomies present different
ROI constraints. To this end, we investigated the minimum ROI size that does not compromise the performance of the
CHO model. In this study, we evaluated both simulated images and phantom CT images to identify the minimum ROI
size that resulted in an accurate figure of merit (FOM) of the CHO’s performance. More specifically, the minimum ROI
size was evaluated as a function of the following: number of channels, spatial frequency and number of rotations of the
Gabor filters, size and contrast of the object, and magnitude of the image noise. Results demonstrate that a minimum
ROI size exists below which the CHO’s performance is grossly inaccurate. The minimum ROI size is shown to increase
with number of channels and be dictated by truncation of lower frequency filters. We developed a model to estimate the
minimum ROI size as a parameterized function of the number of orientations and spatial frequencies of the Gabor filters,
providing a guide for investigators to appropriately select parameters for model observer studies.
Channelized Hotelling observer (CHO) models have been shown to correlate well with human observers for several phantom-based detection/classification tasks in clinical computed tomography (CT). A large number of repeated scans were used to achieve an accurate estimate of the model’s template. The purpose of this study is to investigate how the experimental and CHO model parameters affect the minimum required number of repeated scans. A phantom containing 21 low-contrast objects was scanned on a 128-slice CT scanner at three dose levels. Each scan was repeated 100 times. For each experimental configuration, the low-contrast detectability, quantified as the area under receiver operating characteristic curve, Az, was calculated using a previously validated CHO with randomly selected subsets of scans, ranging from 10 to 100. Using Az from the 100 scans as the reference, the accuracy from a smaller number of scans was determined. Our results demonstrated that the minimum number of repeated scans increased when the radiation dose level decreased, object size and contrast level decreased, and the number of channels increased. As a general trend, it increased as the low-contrast detectability decreased. This study provides a basis for the experimental design of task-based image quality assessment in clinical CT using CHO.
The use of Fourier domain model observer is challenged by iterative reconstruction (IR), because IR
algorithms are nonlinear and IR images have noise texture different from that of FBP. A modified Fourier
domain model observer, which incorporates nonlinear noise and resolution properties, has been proposed for
IR and needs to be validated with human detection performance. On the other hand, the spatial domain model
observer is theoretically applicable to IR, but more computationally intensive than the Fourier domain
method. The purpose of this study is to compare the modified Fourier domain model observer to the spatial
domain model observer with both FBP and IR images, using human detection performance as the gold
standard. A phantom with inserts of various low contrast levels and sizes was repeatedly scanned 100 times
on a third-generation, dual-source CT scanner at 5 dose levels and reconstructed using FBP and IR
algorithms. The human detection performance of the inserts was measured via a 2-alternative-forced-choice
(2AFC) test. In addition, two model observer performances were calculated, including a Fourier domain non-prewhitening
model observer and a spatial domain channelized Hotelling observer. The performance of these
two mode observers was compared in terms of how well they correlated with human observer performance.
Our results demonstrated that the spatial domain model observer correlated well with human observers across
various dose levels, object contrast levels, and object sizes. The Fourier domain observer correlated well with
human observers using FBP images, but overestimated the detection performance using IR images.
Evaluation of flat-panel angiography equipment through conventional image quality metrics is limited by the scope of standard spatial-domain image quality metric(s), such as contrast-to-noise ratio and spatial resolution, or by restricted access to appropriate data to calculate Fourier domain measurements, such as modulation transfer function, noise power spectrum, and detective quantum efficiency. Observer models have been shown capable of overcoming these limitations and are able to comprehensively evaluate medical-imaging systems. We present a spatial domain-based channelized Hotelling observer model to calculate the detectability index (DI) of our different sized disks and compare the performance of different imaging conditions and angiography systems. When appropriate, changes in DIs were compared to expectations based on the classical Rose model of signal detection to assess linearity of the model with quantum signal-to-noise ratio (SNR) theory. For these experiments, the estimated uncertainty of the DIs was less than 3%, allowing for precise comparison of imaging systems or conditions. For most experimental variables, DI changes were linear with expectations based on quantum SNR theory. DIs calculated for the smallest objects demonstrated nonlinearity with quantum SNR theory due to system blur. Two angiography systems with different detector element sizes were shown to perform similarly across the majority of the detection tasks.
In previous investigations on CT image quality, channelized Hotelling observer (CHO) models have been shown to well represent human observer performance in several phantom-based detection/discrimination tasks. In these studies, a large number of independent images was necessary to estimate the expectation images and covariance matrices for each test condition. The purpose of this study is to investigate how the number of repeated scans affects the precision and accuracy of the CHO’s performance in a signal-known-exactly detection task. A phantom containing 21 low-contrast objects (3 contrast levels and 7 sizes) was scanned with a 128-slice CT scanner at three dose levels. For each dose level, 100 independent images were acquired for each test condition. All images were reconstructed using filtered-backprojection (FBP) and a commercial iterative reconstruction algorithm. For each combination of dose level and reconstruction method, the low-contrast detectability, quantified with the area under receiver operating characteristic curve (Az), was calculated using a previously validated CHO model. To determine the dependency of CHO performance on the number of repeated scans, the Az value was calculated for different number of channel filters, for each object size and contrast, and for different dose/reconstruction settings using all 100 repeated scans. The Az values were also calculated using randomly selected subsets of the scans (from 10 to 90 scans with an increment of 10 scans). Using the Az from the 100 scans as the reference, the accuracy of Az values calculated from a fewer number of scans was determined and the minimal number of scans was subsequently derived. For the studied signal-known-exactly detection task, results demonstrated that, the minimal number of scans depends on dose level, object size and contrast level, and channel filters.
The addition of photoacoustic endoscopy to conventional endoscopic ultrasound offers imaging capabilities that may improve diagnosis and clinical care of gastrointestinal tract diseases. In this study, using a 3.8-mm diameter dual-mode photoacoustic and ultrasonic endoscopic probe, we investigated photoacoustic and ultrasonic image features of rabbit esophagi. Specifically, we performed ex vivo imaging of intact rabbit esophagi and correlated the acquired images with histology. Without motion artifact-based limitations, we were able to utilize the full resolving power of the endoscopic device and acquire the first three-dimensional vasculature map of the esophagus and mediastinum, along with coregistered tissue density information. Here, we present the experimental results and discuss potential clinical applications of the technique.
External MRI fiducial marker devices are expected to facilitate robust, accurate, and efficient image fusion between MRI
and other modalities. Automating of this process requires careful selection of a suitable marker size and material visible
across a variety of pulse sequences, design of an appropriate fiducial device, and a robust segmentation algorithm. A set
of routine clinical abdominal MRI pulse sequences was used to image a variety of marker materials and range of marker
sizes. The most successfully detected marker was 12.7 mm diameter cylindrical reservoir filled with 1 g/L copper sulfate
solution. A fiducial device was designed and fabricated from four such markers arranged in a tetrahedral orientation.
MRI examinations were performed with the device attached to phantom and a volunteer, and custom developed
algorithm was used to detect and segment the individual markers. The individual markers were accurately segmented in
all sequences for both the phantom and volunteer. The measured intra-marker spacings matched well with the
dimensions of the fiducial device. The average deviations from the actual physical spacings were 0.45± 0.40 mm and
0.52 ± 0.36 mm for the phantom and the volunteer data, respectively. These preliminary results suggest that this general
fiducial design and detection algorithm could be used for MRI multimodality fusion applications.
Like ultrasound endoscopy, photoacoustic endoscopy (PAE) could become a valuable addition to clinical practice due
to its deep imaging capability. Results from our recent in vivo transesophageal endoscopic imaging study on rabbits
demonstrate the technique’s capability to image major organs in the mediastinal region, such as the lung, trachea, and
cardiovascular systems. Here, we present various features from photoacoustic images from the mediastinal region of
several rabbits and discuss possible clinical contributions of this technique and directions of future technology
development.
Photoacoustic (PA) microscopy (PAM) can image optical absorption contrast with ultrasonic spatial resolution in the optical diffusive regime. Conventionally, accurate quantification in PAM requires knowledge of the optical fluence attenuation, acoustic pressure attenuation, and detection bandwidth. We circumvent this requirement by quantifying the optical absorption coefficients from the acoustic spectra of PA signals acquired at multiple optical wavelengths. With the acoustic spectral method, the absorption coefficients of an oxygenated bovine blood phantom at 560, 565, 570, and 575 nm were quantified with errors of <3 % . We also quantified the total hemoglobin concentration and hemoglobin oxygen saturation in a live mouse. Compared with the conventional amplitude method, the acoustic spectral method provides greater quantification accuracy in the optical diffusive regime. The limitations of the acoustic spectral method was also discussed.
We have developed a 2.5-mm outer diameter photoacoustic endoscopic mini-probe to use in the instrument channel
(typically 2.8 or 3.7 mm in diameter) of standard video endoscopes. To achieve adequate signal sensitivity, we
fabricated a focused ultrasonic transducer using a highly-sensitive PMN-PT piezoelectric material. We quantified the
PMN-PT transducer's operating parameters and validated the
mini-probe's endoscopic imaging capability through an ex
vivo imaging experiment on a rat colon.
Photoacoustic (PA) tomography (PAT) can image optical absorption contrast with ultrasonic spatial resolution in the
optical diffusive regime. Multi-wavelength PAT can noninvasively monitor hemoglobin oxygen saturation (sO2) with
high sensitivity and fine spatial resolution. However, accurate quantification in PAT requires knowledge of the optical
fluence distribution, acoustic wave attenuation, and detection system bandwidth. We propose a method to circumvent
this requirement using acoustic spectra of PA signals acquired at two optical wavelengths. With the acoustic spectral
method, the absorption coefficients of an oxygenated bovine blood phantom at 560 and 575 nm were quantified with
errors of ><5%.
pH is a tightly regulated indicator of metabolic activity. In mammalian systems, imbalance of pH regulation may result
from or result in serious illness. Even though the regulation system of pH is very robust, tissue pH can be altered in many
diseases such as cancer, osteoporosis and diabetes mellitus. Traditional high-resolution optical imaging techniques, such
as confocal microscopy, routinely image pH in cells and tissues using pH sensitive fluorescent dyes, which change their
fluorescence properties with the surrounding pH. Since strong optical scattering in biological tissue blurs images at
greater depths, high-resolution pH imaging is limited to penetration depths of 1mm. Here, we report photoacoustic
microscopy (PAM) of commercially available pH-sensitive fluorescent dye in tissue phantoms. Using both opticalresolution
photoacoustic microscopy (OR-PAM), and acoustic resolution photoacoustic microscopy (AR-PAM), we
explored the possibility of recovering the pH values in tissue phantoms. In this paper, we demonstrate that PAM was
capable of recovering pH values up to a depth of 2 mm, greater than possible with other forms of optical microscopy.
Photoacoustic endoscopy (PAE) provides unique functional information with high spatial resolution at super depths.
The provision of functional information is predicated on its strong spectroscopic imaging ability, and its deep imaging
capability is derived from its ultrasonic detection of diffused photon absorption. To accurately image functional
physiological parameters, it is necessary to rapidly alternate laser pulses of sufficient energy and different wavelengths.
In this study, we developed peripheral optical systems for PAE based on two identical pulsed-laser systems to achieve
the fast laser wavelength switching that is essential for accurate functional imaging. Each laser system was comprised of
a tunable dye laser pumped by a solid-state, diode-pumped Nd:YLF laser. Both systems deliver adequate energy at the
scanning head of the endoscope for imaging biological tissue in the optically diffusive regime (~0.3-0.6 mJ per pulse
with a repetition rate of ~1 kHz). In this paper, we introduce the employed laser systems and design of the light delivery
optics, and present results from an ex vivo animal imaging experiment that validates the system's multi-wavelength
functional imaging capability.
pH is a tightly regulated indicator of metabolic activity. In mammalian systems, an imbalance of pH regulation may result from or result in serious illness. In this paper, we report photoacoustic microscopy (PAM) of a commercially available pH-sensitive fluorescent dye (SNARF-5F carboxylic acid) in tissue phantoms. We demonstrated that PAM is capable of pH imaging in absolute values at tissue depths of up to 2.0 mm, greater than possible with other forms of optical microscopy.
To image beyond the quasi-ballistic photon regime, photoacoustic tomography systems must rely on diffuse photons;
however, there still exists an optimal illumination pattern that results in the largest number of photons reaching a target
at a given depth. Many photoacoustic imaging systems incorporate weak optical focusing through oblique or dark-field
illumination, but these systems are not often optimized for deep light delivery. Multiple parameters and constraints,
particularly for in vivo imaging, need to be considered to determine the optimal illumination scheme for a given system:
beam diameter, incident angle, pulse repetition rate, laser fluence, and target depth. Monte Carlo simulations of varied
beam geometries and incident angles show the best optical illumination schemes for different imaging depths. Further an
analytic model based on the diffusion theory provides a rapid method of determining the optimal beam size and incident
angle for a given target depth and agrees well with the simulations. The results reveal the most efficient optical focal
position to maximize the number of photons delivered to a target depth, therein maximizing the PA signal. The
principles and results discussed here are not limited to the system investigated, but can be applied to other system
configurations to improve the photoacoustic signal strength.
Scalability is a key feature of photoacoustic microscopy (PAM). Reports have shown that PAM systems can be
designed to possess sub-micron resolution at shallow depths or penetrate centimeters deep at the expense of
resolution while the number of resolved pixels in the depth direction remains high. This capability to readily tune
the imaging parameters while maintaining the same inherent contrast could be extremely useful for a variety of
biomedical applications. Human skin, with its layered vascular structure whose dimensions scale with depth,
provides an ideal imaging target to illustrate this advantage. Here, we present results from in vivo human skin
imaging experiments using two different PAM systems, an approach which enables better characterization of the
cutaneous microvasculature throughout the imaging depth. Specifically, we show images from several distinct areas
of skin: the palm and the forearm. For each region, the same area was imaged with both an optical-resolution PAM
(OR-PAM) and an acoustic-resolution PAM (AR-PAM), and the subsequent images were combined into composite
images. The OR-PAM provides less than 5 μm lateral resolution, capable of imaging the smallest capillary vessels,
while the AR-PAM enables imaging at depths of several millimeters. Several structures are identifiable in the ORPAM
images which cannot be differentiated in AR-PAM images, namely thin epidermal and stratum corneum
layers, undulations in the dermal papillae, and capillary loops. However, the AR-PAM provides images of larger
vessels, deeper than the OR-PAM can penetrate. These results demonstrate how PAM's scalability can be utilized to
more fully characterize cutaneous vasculature, potentially impacting the assessment of numerous cardiovascular
related and cutaneous diseases.
We have successfully implemented a focused ultrasonic transducer for photoacoustic endoscopy. The photoacoustic
endoscopic probe's ultrasound transducer determines the lateral resolution of the system. By using a focused ultrasonic
transducer, we significantly improved the endoscope's spatial resolution and signal-to-noise ratio. This paper describes
the technical details of the ultrasonic transducer incorporated into the photoacoustic endoscopic probe and the
experimental results from which the transducer's resolution is quantified and the image improvement is validated.
Optical absorption is closely associated with many physiologically important parameters, such as the
concentration and oxygen saturation of hemoglobin, and it can be used to quantify the concentrations of non-fluorescent
molecules. We introduce a method to quantify the absolute optical absorption based upon the acoustic spectra of
photoacoustic (PA) signals. This method is self-calibrating and thus insensitive to variations in optical fluence. Factors
such as the detection system bandwidth and acoustic attenuation can affect the quantification but can be canceled by
measuring the acoustic spectra at two optical wavelengths. This method has been implemented on various PA systems,
including optical-resolution PA microscopy, acoustic-resolution PA microscopy, and reconstruction based PA array
systems. We quantified the optical absorption coefficients of phantom samples at various wavelengths. We also
quantified the oxygen saturation of hemoglobin in live mice.
Photoacoustic microscopy (PAM) utilizes short laser pulses to deposit energy into light
absorbers and sensitively detects the ultrasonic waves the absorbers generate in response.
PAM directly renders a three-dimensional spatial distribution of sub-surface optical absorbers.
Unlike other optical imaging technologies, PAM features label-free optical absorption contrast
and excellent imaging depths. Standard dental imaging instruments are limited to X-ray and
CCD cameras. Subsurface optical dental imaging is difficult due to the highly-scattering enamel
and dentin tissue. Thus, very few imaging methods can detect dental decay or diagnose dental
pulp, which is the innermost part of the tooth, containing the nerves, blood vessels, and other
cells. Here, we conducted a feasibility study on imaging dental decay and dental pulp with PAM.
Our results showed that PAM is sensitive to the color change associated with dental decay.
Although the relative PA signal distribution may be affected by surface contours and subsurface
reflections from deeper dental tissue, monitoring changes in the PA signals (at the same site)
over time is necessary to identify the progress of dental decay. Our results also showed that
deep-imaging, near-infrared (NIR) PAM can sensitively image blood in the dental pulp of an in
vitro tooth. In conclusion, PAM is a promising tool for imaging both dental decay and dental
pulp.
KEYWORDS: Capillaries, Photoacoustic microscopy, In vivo imaging, Photoacoustic spectroscopy, Oxygen, Blood circulation, Skin, Spatial resolution, 3D image processing, 3D acquisition
Microcirculation is an important component of the cardiovascular system and can be used to assess systemic cardiovascular health. Numerous studies have investigated cutaneous microcirculation as an indicator of cardiovascular related diseases. Such research has shown promising results; however, there are many limitations regarding the employed measurement techniques, such as poor depth and spatial resolution and measurement versatility. Here we show the results of functional cutaneous microvascular experiments measured with photoacoustic microscopy, which provides high spatial resolution and multiparameter measurements. In a set of experiments, microvascular networks located in the palms of volunteers were perturbed by periodic ischemic events, and the subsequent hemodynamic response to the stimulus was recorded. Results indicate that during periods of arterial occlusion, the relative oxygen saturation of the capillary vessels decreased below resting levels, and temporarily increased above resting levels immediately following the occlusion. Furthermore, a hyperemic reaction to the occlusions was measured, and the observation agreed well with similar measurements using more conventional imaging techniques. Due to its exceptional capability to functionally image vascular networks with high spatial resolution, photoacoustic microscopy could be a beneficial biomedical tool to assess microvascular functioning and applied to patients with diseases that affect cardiovascular health.
KEYWORDS: Skin, In vivo imaging, Photoacoustic microscopy, Blood vessels, Melanoma, Tumors, Photoacoustic spectroscopy, Capillaries, Signal detection, Signal generators
In several human volunteers, photoacoustic microscopy (PAM) has been utilized for noninvasive cutaneous imaging of the skin microvasculature and a melanocytic nevus. Microvascular networks in both acral and nonacral skin were imaged, and multiple features within the skin have been identified, including the stratum corneum, epidermal-dermal junction, and subpapillary vascular plexus. Several vascular and structural differences between acral and nonacral skin were also observed in the photoacoustic images. In addition, a nevus was photoacoustically imaged, excised, and histologically analyzed. The photoacoustic images allowed for in vivo measurement of tumor thickness, depth, and microvasculature-values confirmed by histologic examination. The presented images demonstrate the potential of PAM to aid in the study and evaluation of cutaneous microcirculation and analysis of pigmented lesions. Through its ability to three-dimensionally image the structure and function of the microvasculature and pigmented lesions, PAM can have a clinical impact in diagnosis and assessment of systemic diseases that affect the microvasculature such as diabetes and cardiovascular disease, cutaneous malignancies such as melanoma, and potentially other skin disorders.
Gold nanoparticles have received much attention due to their potential diagnostic and therapeutic applications. Gold
nanoparticles are attractive in many biomedical applications because of their biocompatibility, easily modifiable
surfaces for targeting, lack of heavy metal toxicity, wide range of sizes (35-100 nm), tunable plasmonic resonance
peak, encapsulated site-specific drug delivery, and strong optical absorption in the near-infrared regime. Specifically,
due to their strong optical absorption, gold nanoparticles have been used as a contrast agent for molecular photoacoustic
(PA) imaging of tumor. The plasmonic resonance peak of the gold nanocages (AuNCs) was tuned to the near-infrared
region, and the ratio of the absorption cross-section to the extinction cross-section was approximately ~70%, as
measured by PA sensing. We used PEGylated gold nanocages (PEG-AuNCs) as a passive targeting contrast agent on
melanomas. After 6-h intravenous injection of PEG-AuNCs, PA amplitude was increased by ~14 %. These results
strongly suggest PA imaging paired with AuNCs is a promising diagnostic tool for early cancer detection.
KEYWORDS: Photoacoustic microscopy, Skin, Transducers, Photoacoustic imaging, In vivo imaging, Oxygen, Blood circulation, Photoacoustic spectroscopy, 3D image processing, Temperature metrology
We report results of two in vivo functional human imaging experiments using photoacoustic microscopy. In Experiment
1, the hemodynamic response to an ischemic event was measured. The palm of a volunteer was imaged and a single
cross-section was monitored while periodic arterial occlusions were administered using a blood pressure cuff wrapped
around the upper arm and inflated to ~280 mmHg. Significant relative decreases in oxygen saturation (sO2) and total
hemoglobin (HbT) were observed during periods of ischemia. Upon release of the occlusion, significant relative
increases in sO2 and HbT due to post-occlusive reactive hyperemia were recorded. Experiment 2 explored the vascular
response to a local, external thermal stimulus. Thermal hyperemia is a common physiological phenomenon and
thermoregulation function in which blood flow to the skin is increased to more efficiently exchange heat with the
ambient environment. The forearm of a volunteer was imaged and a single cross-section was monitored while the
imaged surface was exposed to an elevated temperature of ~46°C. Due to thermal hyperemia, relative increases in sO2
and HbT were measured as the temperature of the surface was raised. These results may contribute as clinically relevant
measures of vascular functioning for detection and assessment of vascular related diseases.
Advances in the brain functional imaging greatly facilitated the understanding of neurovascular coupling. For monitoring
of the microvascular response to the brain electrical stimulation in vivo we used optical-resolution photoacoustic
microscopy (OR-PAM) through the cranial openings as well as transcranially. Both types of the vascular response,
vasoconstriction and vasodilatation, were clearly observed with good spatial and temporal resolution. Obtained results
confirm one of the primary points of the neurovascular coupling theory that blood vessels could present vasoconstriction
or vasodilatation in response to electrical stimulation, depending on the balance between inhibition and excitation of the
different parts of the elements of the neurovascular coupling system.
Previous studies on dewetting of ultrathin Co films by nanosecond pulsed laser melting have shown that the films dewet due to a thin film hydrodynamic instability and form a system of ordered nanoparticles with uniform average size and nearest neighbor particle spacing. For Co films less than 8 nm thick, the nanoparticle spacing, λNN was dependent on the initial film thickness, h, and varied as h2. For Co films thicker than 8 nm, the nanoparticle spacing decreased with increasing film thickness, due to a thermocapillary effect generated by the ns laser heating. Here we show the results from investigations on dewetting of Co films that had initially much rougher surfaces with root mean square roughness values, 0.9 < Rrms < 2.8 nm as compared to smoother films examined in prior investigations, for which Rrms ≤ 0.2 nm. Laser induced dewetting of Co films with much large Rrms values generated nanoparticles that were qualitatively similar to those created from smoother Co films. The size distribution of the nanoparticles was monodispersed and there was short range spatial order present in the system from the average nearest neighbor nanoparticle spacing; however, a drastic reduction in the characteristic length scales was observed in the nanoparticulate arrays created from the rougher Co films. This result suggests that knowledge of film thickness and roughness are important towards predicting characteristic length scales from metal film dewetting.
Metallic nanoparticles embedded in dielectrics permit enhanced capture absorption and/or scattering of light at specific wavelengths through excitation of plasmons, i.e. the quanta of coherent and collective oscillations of large concentrations of nearly free electrons. In order to maximize the potential of such enhanced absorption in useful tasks, such as the generation of carriers in photocatalysts and semiconductors, it is important to be able to predict and design plasmonic nanocomposites with desired wavelength-dependent optical absorption. Recently, a mixing approach formulated by Garcia and co-workers [Phys. Rev. B, 75, 045439 (2007)] has been successfully applied to model the experimentally measured broadband optical absorption for ternary nanocomposites containing alloys or mixtures of two metals (from Ag, Au or Cu) in SiO2 dielectric. In this work we present the broadband optical behavior of an important an optical coating dielectric, Si3N4, containing various configuration of nanoparticles of Al, Au, Ag, or Cu. The spectral behavior of various combinations of the metallic species in the dielectrics was optimized to show either broadband solar absorption or strong multiple plasmonic absorption peaks. The applications of such nanocomposite materials in solar energy harvesting and spectral sensing are also presented and discussed.
Robust nanomanufacturing methodologies are crucial towards realizing simple and cost-effective products. Here we
discuss nanofabrication of ordered metal nanoparticles through pulsed-laser-induced self-organization. When ultrathin
metal films are exposed to short laser pulses, spontaneous pattern formation results under appropriate conditions. Under
uniform laser irradiation two competing modes of self-organization are observed. One, a thin film hydrodynamic dewetting
instability due to the competition between surface tension and attractive van derWaals interactions, results in nanoparticles
with well-defined and predictable interparticle spacings and sizes with short range spatial order. The second, thermocapillary
flow due to interference between the incident beam and a scattered surface wave, results in laser induced periodic surface
structures. Non-uniform laser irradiation, such as by 2-beam laser interference irradiation, initiates a tunable thermocapillary
effect in the film giving rise to nanowires, and continued laser irradiation leads to a Rayleigh-like breakup of the nanowires
producing nanoparticles with spatial long-range and short-range order. These self-organizing approaches appear to be
applicable to a variety of metal films, including Co, Cu, Ag, Fe, Ni, Pt, Zn, Ti, V and Mn. These results suggest that
laser-induced self-organization in thin films could be an attractive route to nanomanufacture well-defined nanoparticle
arrangements for applications in optical information processing, sensing and solar energy harvesting.
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