Contrast agent stability: a continuous B-mode imaging approach

In situ conversion of porphyrin microbubbles to nanoparticles for multimodality imaging

Converting nanoparticles or monomeric compounds into larger supramolecular structures by endogenous or external stimuli is increasingly popular because these materials are useful for imaging and treating diseases. However, conversion of microstructures to nanostructures is less common. Here, we show the conversion of microbubbles to nanoparticles using low-frequency ultrasound. The microbubble consists of a bacteriochlorophyll-lipid shell around a perfluoropropane gas. The encapsulated gas provides ultrasound imaging contrast and the porphyrins in the shell confer photoacoustic and fluorescent properties. On exposure to ultrasound, the microbubbles burst and form smaller nanoparticles that possess the same optical properties as the original microbubble. We show that this conversion is possible in tumour-bearing mice and could be validated using photoacoustic imaging. With this conversion, our microbubble can potentially be used to bypass the enhanced permeability and retention effect when delivering drugs to tumours.

Ultrafast 2-dimensional image monitoring and array-based passive cavitation detection for ultrasound contrast agent destruction in a variably sized region

OBJECTIVES

A combined approach was proposed, based on programmable ultrasound equipment, to simultaneously monitor surviving microbubbles and detect cavitation activity during microbubble destruction in a variably sized region for use in ultrasound contrast agent (UCA)-enhanced therapeutic ultrasound applications.

METHODS

A variably sized focal region wherein the acoustic pressure was above the UCA fragmentation threshold was synthesized at frequencies of 3, 4, 5, and 6 MHz with a linear broadband imaging probe. The UCAs' temporal and spatial distribution during the microbubbles' destruction was monitored in a 2-dimensional imaging plane at 5 MHz and a frame rate of 400 Hz, and simultaneously, broadband noise emissions during the microbubbles' fragmentation were extracted by using the backscattered signals produced by the focused release bursts (ie, destruction pulses) themselves. Afterward, the temporal evolution of broadband noise emission, the surviving microbubbles in a region of interest (ROI), and the destruction area in a static UCA suspension were computed. Then the inertial cavitation dose, destruction rate of microbubbles in the ROI, and area of the destruction region were determined.

RESULTS

It was found that an increasing pulse length and a decreasing transmit aperture and excitation frequency were correlated with an increased inertial cavitation dose, microbubble destruction rate, and destruction area. Furthermore, it was obvious that the microbubble destruction rate was significantly correlated with the inertial cavitation dose (P < .05). In addition, the intensity decrease in the ROI was significantly correlated with the destruction area (P < .05).

CONCLUSIONS

By the proposed strategy, microbubbles could be destroyed in a variably sized region, and destruction efficiency as well as the corresponding inertial cavitation dose could be regulated by manipulating the transmission parameters.

Quantitative contrast-enhanced ultrasound imaging: a review of sources of variability

Ultrasound provides a valuable tool for medical diagnosis offering real-time imaging with excellent spatial resolution and low cost. The advent of microbubble contrast agents has provided the additional ability to obtain essential quantitative information relating to tissue vascularity, tissue perfusion and even endothelial wall function. This technique has shown great promise for diagnosis and monitoring in a wide range of clinical conditions such as cardiovascular diseases and cancer, with considerable potential benefits in terms of patient care. A key challenge of this technique, however, is the existence of significant variations in the imaging results, and the lack of understanding regarding their origin. The aim of this paper is to review the potential sources of variability in the quantification of tissue perfusion based on microbubble contrast-enhanced ultrasound images. These are divided into the following three categories: (i) factors relating to the scanner setting, which include transmission power, transmission focal depth, dynamic range, signal gain and transmission frequency, (ii) factors relating to the patient, which include body physical differences, physiological interaction of body with bubbles, propagation and attenuation through tissue, and tissue motion, and (iii) factors relating to the microbubbles, which include the type of bubbles and their stability, preparation and injection and dosage. It has been shown that the factors in all the three categories can significantly affect the imaging results and contribute to the variations observed. How these factors influence quantitative imaging is explained and possible methods for reducing such variations are discussed.

Imaging of the ovine corpus luteum microcirculation with contrast ultrasound

Ultrasound contrast agents have been the subject of microvascular imaging research. The sheep corpus luteum (CL) is a microvascular tissue that provides a natural angiogenic and antiangiogenic process, which changes during the luteal phase of the estrous cycle of the ewe. It can also be controlled and monitored endocrinologically, providing a very attractive in vivo model for the study and development of microvascular measurement. The perfusion of the fully developed CL between days 8 and 12 of the estrous cycle was studied in six ewes. A Philips iU22 ultrasound scanner (Bothell, WA, USA) with the linear array probe L9-3 was used to capture contrast-enhanced images after an intravenous bolus injection of 2.4 mL SonoVue (Bracco S.P.A., Milan, Italy). Time-intensity curves of a region of interest inside the CL were formed from linearized image data. A lagged-normal model to simulate the compartmental kinetics of the microvascular flow was used to fit the data, and the wash-in time was measured. Good contrast enhancement was observed in the CLs of all animals and the wash-in time averaged at 5.5 s with 9% uncertainty. The regression coefficient was highly significant for all fits. These data correlated with stained endothelial area in the histology performed postmortem. Two ewes were injected with prostaglandin F2alpha to induce CL regression, which resulted in an increase of wash-in time after a few hours. The CL of the ewe is thus proposed as an ideal model for the study and development of microvascular measurements using contrast ultrasound. Our initial results demonstrate a highly reproducible model for the study of the microvascular hemodynamics in a range of tissues and organs.

The assessment of microvascular flow and tissue perfusion using ultrasound imaging

Imaging microvascular flow is of diagnostic value for a wide range of diseases including cancer, inflammation, and cardiovascular disease. The introduction of microbubbles as ultrasound contrast agents offers significant signal enhancement to the otherwise weakly scattered signal from blood in the circulation. Microbubbles provide maximum impedance mismatch, but are not linear scatterers. Their complex response to ultrasound has generated research on both their behaviour and their scattered-signal processing. Nearly 20 years ago signal processing started with simple spectral filtering of harmonics showing contrast-enhanced images. More recent pulse encoding techniques have achieved good cancellation of tissue echoes. The good quality contrast-only images enabled ultrasound contrast-imaging applications to be established in microvascular measurements in the liver and the myocardium. The field promises to advance the quantification of microvascular flow kinetics.

Growth and dissolution of an encapsulated contrast microbubble: effects of encapsulation permeability

Gas diffusion from an encapsulated microbubble is modeled using an explicit linear relation for gas permeation through the encapsulation. Both the cases of single gas (air) and multiple gases (perfluorocarbon inside the bubble and air dissolved in surrounding liquid) are considered. An analytical expression for the dissolution time for an encapsulated air bubble is obtained; it showed that for small permeability the dissolution time increases linearly with decreasing permeability. A perfluorocarbon-filled contrast microbubble such as Definity was predicted to experience a transient growth because of air infusion before it dissolves in conformity with previous experimental findings. The growth phase occurs only for bubbles with a critical value of initial mole fraction of perfluorocarbon relative to air. With empirically obtained property values, the dissolution time of a 2.5-micron diameter (same as that of Definity), lipid-coated octafluoropropane bubble, with surface tension 25 mN/m, is predicted to be 42 min in an air-saturated medium. The properties such as shell permeability, surface tension and relative mole fraction of octafluoropropane are varied to investigate their effects on the time scales of bubble growth and dissolution, including their asymptotic scalings where appropriate. The dissolution dynamics scales with permeability, in that when the time is nondimensioanlized with permeability, curves for different permeabilities collapse on a single curve. Investigation of bubbles filled with other gases (nonoctafluoropropane perfluorocarbon and sulfur hexafluoride) indicates longer dissolution time because of lower solubility and lower diffusivity for larger gas molecules. For such micron-size encapsulated bubbles, lifetime of hours is possible only at extremely low surface tension (<1 mN/m) or at extreme oversaturation.

Effects of encapsulation elasticity on the stability of an encapsulated microbubble

A model for gas transport from an encapsulated microbubble into the surrounding medium is developed and investigated incorporating the effects of encapsulation elasticity. Encapsulation elasticity stabilizes microbubbles against dissolution and explains the long shelf life of microbubble contrast agent. We consider air bubbles as well as bubbles containing perfluorocarbon gas. Analytical conditions between saturation level, surface tension and interfacial dilatational elasticity are determined for attaining non-zero equilibrium radius for these microbubbles. Numerical solution of the equation verifies the stability of the equilibrium radii. In an undersaturated medium all encapsulated bubbles dissolve. In a saturated medium, an encapsulated bubble is found to achieve a long-time stable radius when interfacial dilatational elasticity is larger than equilibrium surface tension. For bubbles with interfacial dilatational elasticity smaller than the equilibrium surface tension, stable bubble of non-zero radius can be achieved only when the saturation level is greater than a critical value. Even if they initially contain a gas other than air, bubbles that reach a stable radius finally become air bubbles. The model is applied to an octafluoropropane filled lipid-coated 2.5 microm bubble, which displayed a transient swelling due to air intake before reaching an equilibrium size. Effects of elasticity, shell permeability, initial mole fraction, initial radius and saturation level are investigated and discussed. Shell permeability and mole fraction do not affect the final equilibrium radius of the microbubble but affect the time scale and the transient dynamics. Similarly, the ratio of equilibrium radius to initial radius remains unaffected by the variation in initial radius.

Single microbubble response using pulse sequences: initial results

The study of acoustic scattering by single microbubbles has the potential to offer improved signal processing techniques. A microacoustic system that employs a hydrodynamically-focused flow was used to detect radiofrequency (RF) backscatter from single microbubbles. RF data were collected using a commercial scanner. Results are presented for two agents, namely Definity (Lantheus Medical Imaging, N. Billerica, MA, USA) and biSphere (Point Biomedical Corp, San Carlos, CA, USA). The agents were insonified with amplitude-modulated pulses, and it was observed in both agents that a subpopulation of microbubbles did not produce a measurable echo from the first-half amplitude pulse, but did produce a response from the full amplitude pulse and from a subsequent half amplitude pulse. The number of microbubbles in this subpopulation was seen to increase with increasing transmit amplitude. These results do not bear out the simple theory of microbubble-pulse sequence interaction and invite a reassessment of signal processing approaches.

Response of contrast agents to ultrasound

Microbubbles are used as ultrasonic contrast agents that enhance the ultrasound signals of the vascular bed. The recent development of site-targeted microbubbles opened up the possibility for molecular imaging as well as localised drug and gene delivery. Initially the microbubbles' physical properties and their response to the ultrasound beam were not fully understood. However, the introduction of fast acquisition microscopy has allowed the observation of the microbubble behaviour in the presence of ultrasound. In addition, acoustical techniques can determine the scatter of single microbubbles. Sonoporation experiments promise high-specificity drug and gene delivery, but the responsible physical mechanisms, particularly for in vivo applications, are not fully understood. An improvement of microbubble technology may address variability related problems in both imaging and drug/gene delivery.

Quantitative measurement of ultrasound disruption of polymer-shelled microbubbles

The goal of this study was to assess the threshold of disruption and subsequent time-course of acoustic response of four experimental nitrogen-filled polymer-shelled microbubbles. Using an in vitro measurement system, a sequence of low-amplitude detection pulses measured the change in echo caused by a high-amplitude disruption pulse on a dilute suspension of bubbles. Detection pulses were transmitted 0.5 ms before disruption and between 1 and 200 ms after disruption. Separate transducers, aligned confocally and orthogonally, were used to transmit and receive bubble echoes. After disruption, all agents demonstrated a transient increase in scattered power. Above the disruption threshold, highly echogenic, nonlinear scatterers were observed. Their echoes slowly disappeared after disruption with median decay times from 7.4 to 13.6 ms, calculated by fitting to a mono-exponential decay. This is consistent with a process wherein the shell is disrupted, releasing the gas and generating free gas bubbles, which cause high-amplitude nonlinear scattering followed by relatively slow diffusion of the gas into solution. This picture has been observed optically with single bubbles and differs from the concept of "stimulated acoustic emission" from disrupted bubbles.

Ultrasound microbubble contrast agents: fundamentals and application to gene and drug delivery

This review offers a critical analysis of the state of the art of medical microbubbles and their application in therapeutic delivery and monitoring. When driven by an ultrasonic pulse, these small gas bubbles oscillate with a wall velocity on the order of tens to hundreds of meters per second and can be deflected to a vessel wall or fragmented into particles on the order of nanometers. While single-session molecular imaging of multiple targets is difficult with affinity-based strategies employed in some other imaging modalities, microbubble fragmentation facilitates such studies. Similarly, a focused ultrasound beam can be used to disrupt delivery vehicles and blood vessel walls, offering the opportunity to locally deliver a drug or gene. Clinical translation of these vehicles will require that current challenges be overcome, where these challenges include rapid clearance and low payload. The technology, early successes with drug and gene delivery, and potential clinical applications are reviewed.

Destruction thresholds of echogenic liposomes with clinical diagnostic ultrasound

Echogenic liposomes (ELIP) are submicron-sized phospholipid vesicles that contain both gas and fluid. With antibody conjugation and drug incorporation, these liposomes can be used as novel targeted diagnostic and therapeutic ultrasound contrast agents. The utility of liposomes for contrast depends upon their stability in an acoustic field, whereas the use of liposomes for drug delivery requires the liberation of encapsulated gas and drug payload at the desired treatment site. The objective of this study was twofold: (1) to characterize the stability of liposome echogenicity after reconstitution and (2) to quantitate the acoustic destruction thresholds of liposomes as a function of peak rarefactional pressure (P(r)), pulse duration (PD) and pulse repetition frequency (PRF). The liposomes were insonified in an anechoic sample chamber using a Philips HDI 5000 diagnostic ultrasound scanner with a L12-5 linear array. Liposome stability was evaluated with 6.9-MHz fundamental and 4.5-MHz harmonic B-mode pulses at various P(r) at a fixed PRF. Liposome destruction thresholds were determined using 6.0-MHz Doppler pulses, by varying the PD with a fixed PRF of 1.25 kHz and by varying the PRF with a fixed PD of 3.33 micros. Videos or freeze-captured images were acquired during each insonation experiment and analyzed for echogenicity in a fixed region of interest as a function of time. An initial increase in echogenicity was observed for fundamental and harmonic B-mode imaging pulses. The threshold for acoustically driven diffusion of gas out of the liposomes using 6.0-MHz Doppler pulses was weakly dependent upon PRF and PD. The rapid fragmentation thresholds, however, were highly dependent upon PRF and PD. The quantification of acoustic destruction thresholds of ELIP is an important first step in their development as diagnostic and drug delivery agents.

Quantitative contrast enhanced ultrasound and CT assessment of tumor response to antiangiogenic therapy in rats

Contrast-enhanced computed tomography (CECT) and contrast-enhanced destruction-replenishment subharmonic ultrasound (CEDRSU) were used to quantify blood flow and tumor viability during antiangiogenic therapy. SU11657 or placebo was administered to R3230AC tumor-baring rats over a two-week period. CEDRSU vascular volume (ASI) and volume flow (VF) and CECT perfusion (PR) and permeability (PM) measurements were made on day 0, 7 and 14. The percent change in imaging parameters was calculated between day 0 and 7 and 14. Serum drug level (SDL) was compared with imaging parameters. Imaging estimates of tumor viability were compared with histology images on day 14. The percent change in imaging measures for control and treated groups were significantly different on day 7(ASI, p = 0.02; VF, p = 0.008, PR, p = 0.0007; PM, p = 0.003) and 14 (ASI, p = 0.0004; VF, p = 0.002, PR, p = 0.003; PM, p = 0.005). Imaging identified animals with lower SDLs as having higher tumor vascularity and flow. Spatial estimates of tumor viability correlated with histology (CEDRSU, r(2) = 0.92, p << 0.001; CT, r(2) = 0.86, p << 0.001). CEDRSU and CECT provide measures of blood flow and viability in tumors during antiangiogenic therapy. Tumors with higher flow were identified in animals with lower SDL. SU11657 treatment results in decreased tumor flow and viability.

Classification of contrast ultrasound images using autoregressive model coupled to Gaussian mixture model

Contrast ultrasound images are not clear enough to be directly adopted in the diagnostic. In fact, the ultrasound agents enhance the vascular zones but unfortunately the signals backscattered from agent and tissues are still close. Therefore, it is necessary to implement image-processing techniques to enhance the contrast echo and thus have the capability of classification. In this article, we apply a new approach based on the autoregressive model coupled to the Gaussian mixture model to represent both agent and tissue behaviors. Then, we process the resultant image by a classification method based on a fixed window's size in order to obtain a satisfying differentiation of the ultrasound image into two classes. Finally, we adopt the Agent to Tissue Ratio (ATR) factor and the Fisher criterion to compare the performance of this method with existing techniques as harmonic and B mode.

Acoustic techniques for assessing the Optison destruction threshold

OBJECTIVE

The purpose of this study was to identify the pressure threshold for the destruction of Optison (octafluoropropane contrast agent; Amersham Health, Princeton, NJ) using a laboratory-assembled 3.5-MHz pulsed ultrasound system and a clinical diagnostic ultrasound scanner.

METHODS

A 3.5-MHz focused transducer and a linear array with a center frequency of 6.9 MHz were positioned confocally and at 90 degrees to each other in a tank of deionized water. Suspensions of Optison (5-8x10(4) microbubbles/mL) were insonated with 2-cycle pulses from the 3.5-MHz transducer (peak rarefactional pressure, or Pr, from 0.0, or inactive, to 0.6 MPa) while being interrogated with fundamental B-mode imaging pulses (mechanical index, or MI,=0.04). Scattering received by the 3.5-MHz transducer or the linear array was quantified as mean backscattered intensity or mean digital intensity, respectively, and fit with exponential decay functions (Ae-kt+N, where A+N was the amplitude at time 0; N, background echogenicity; and k, decay constant). By analyzing the decay constants statistically, a pressure threshold for Optison destruction due to acoustically driven diffusion was identified.

RESULTS

The decay constants determined from quantified 3.5-MHz radio frequency data and B-mode images were in good agreement. The peak rarefactional pressure threshold for Optison destruction due to acoustically driven diffusion at 3.5 MHz was 0.15 MPa (MI=0.08). Furthermore, the rate of Optison destruction increased with increasing 3.5-MHz exposure pressure output.

CONCLUSIONS

Optison destruction was quantified with a laboratory-assembled 3.5-MHz ultrasound system and a clinical diagnostic ultrasound scanner. The pressure threshold for acoustically driven diffusion was identified, and 3 distinct mechanisms of ultrasound contrast agent destruction were observed with acoustic techniques.

Anin vitrostudy of a microbubble contrast agent using a clinical ultrasound imaging system

Optimal insonation settings for contrast imaging are yet to be specified, mainly due to the lack of good understanding of the behaviour of the microbubbles. A satisfactory model that explains the behaviour of individual contrast agent scatterers has not yet been reported in the literature. An in vitro system based on a commercial scanner (ATL HDI3000) has been developed to investigate the backscatter of such agents. Suspensions of Definity were introduced in an anechoic tank. The frequency of transmitted ultrasound varied from 1 to 5 MHz, pulse period from 2 to 10 periods and peak negative acoustic pressure from 0.08 to 1.7 MPa. The backscatter at the fundamental and second harmonic frequency windows from the agent was normalized in terms of the corresponding components of backscatter from a blood mimicking fluid suspension. The agent provided a dominant resonance effect at 1.6 MHz transmit frequency. Second harmonic normalized backscatter averaged around 9 dB higher than the fundamental. The normalized fundamental backscatter intensity was linear with peak negative pressure. The second harmonic at resonance peaked at 0.5 MPa suggestive of bubble disruption above such pressure. The system proved capable of illustrating the ultrasonic behaviour of Definity in vitro, and the investigation suggested particular insonation conditions for optimal image enhancement using Definity.

The behaviour of individual contrast agent microbubbles

In recent years, our knowledge of the behaviour of ultrasonic microbubble contrast agents has improved substantially through in vitro experiments. However, there has been a tendency to use high concentrations of contrast agents in suspension, so that ultrasonic backscatter data are generated by a cloud of microbubbles. Such experiments involve a variety of assumptions with validity that is open to question. In addition, high concentrations of microbubbles cannot be used to understand the behaviour of individual microbubble scatterers. This paper proposes a technique that minimises the number of assumptions that need to be made to interpret in vitro experimental data. The basis of the technique is a dilute suspension of microbubbles that makes single scattering events distinguishable. A commercial scanner was used to collect radio frequency (RF) data from suspensions of two different contrast agents, Quantison and Definity. Backscatter data were collected over a range of acoustic pressures. It was found that Definity provided a constant number of scattering events per unit volume of suspension for almost all applied acoustic pressures. Quantison demonstrated an increasing number of scattering events per unit volume with increasing acoustic pressure. Below 0.6 MPa, Quantison scatterers were not individually detectable and provided levels of backscatter similar to those of a blood-mimicking fluid, which suggests that Quantison microbubbles had almost linear scattering behaviour. At acoustic pressures greater than 0.6 MPa, both agents appeared to provide echoes from free bubbles. The change in the number of scatterers per unit volume with acoustic pressure cannot be demonstrated using high concentrations of contrast agent.

Understanding the limitations of ultrasonic backscatter measurements from microbubble populations

Despite over ten years of in vitro investigations of ultrasound contrast agents, the level of understanding of their behaviour in ultrasound fields is limited. Several problems associated with these investigations, particular to the nature of contrast agents, are discussed. Using a commercial scanner the RF normalized backscatter of two different contrast agents (Definity and Quantison) was measured at different suspension concentrations and acoustic pressures. Both contrast agents scattered ultrasound nonlinearly and the backscatter showed a dependence on acoustic pressure. In order to assess the average behaviour of the agents across the range of acoustic pressures and microbubble concentrations the experimental data were fitted to a theoretically acceptable model using nonlinear regression analysis. The analysis showed that both the backscatter and the attenuation of the Quantison suspensions displayed a higher order of dependence on acoustic pressure than the Definity suspensions. It was also discovered that Quantison microbubbles did not demonstrate uniform behaviour across the acoustic pressure range. At lower acoustic pressures the behaviour could not follow a model similar to that which predicted the behaviour at higher acoustic pressures, which was mainly due to the fact that free bubbles were released in a fashion dependent on acoustic pressure. The fact that two different populations of scatterers exist in the same suspensions makes the assessment of the behaviour of the particular agent impossible with the high concentrations that are commonly used. Very low concentration suspensions whereby single scattering events can be monitored should be more useful. In conclusion, the approach of using high microbubble concentrations in order to investigate the properties of ultrasonic contrast agents is limited in that the results of such studies cannot be used to understand the behaviour of single microbubbles.

Contrast-assisted destruction-replenishment ultrasound for the assessment of tumor microvasculature in a rat model

Angiogenesis, the development of new blood vessels, is necessary for tumor growth. Anti-angiogenic therapies have recently received attention as a possible cancer treatment. The purpose of this study was to monitor the vascularity of induced tumors in rats using contrast-enhanced ultrasound during anti-angiogenic therapy. Six rats with subcutaneously implanted R3230 murine mammary adenocarcinomas were treated with an orally administered anti-angiogenic agent (SU11657) beginning 28 days after tumor implantation (20 mg/kg BW once daily). Three additional tumor-bearing control rats were treated with an equivalent volume of vehicle alone. Sonographic evaluation of tumor blood flow was performed using a modified Siemens Sonoline Elegra equipped with a 5.0 MHz linear transducer prior to drug administration, during the first 51 hours following initial drug administration, and on days 8 and 15 after initiation of therapy. Tumor volumes were estimated at each time point using a prolate ellipsoid method from linear dimensions measured on the B-mode ultrasound image in the three major axes. A destruction-replenishment technique was used for tumor blood flow evaluation using a constant rate infusion of intravenously delivered ultrasound contrast media (Definity). A destructive pulse was fired first, followed by a chain of non-destructive pulses that allowed for visualization of vascular contrast agent replenishment. Parametric maps of the time required for contrast agent replenishment and the time-integrated intensity were generated for both the tumor and kidney. Following ultrasound examination, contrast-enhanced computed tomography of each tumor was performed in the same imaging plane as that used to acquire the ultrasound images. Fifteen days after the start of treatment, tumors were excised, preserved in 10% formalin, and sectioned in a plane approximating the ultrasound and CT imaging planes. Sections were prepared for light microscopy with H & E, CD31 and factor VIII immunostain to evaluate overall morphology and vessel distribution. Ultrasound measurements of tumor volume, the spatial extent of contrast enhancement, and the time required for contrast replenishment within control tumors were significantly different from those of treated tumors. The time-integrated ultrasound contrast enhancement decreases and the time required for replenishment of the contrast agent within the tumor volume increases over the course of anti-angiogenic therapy. Parametric maps of integrated intensity are shown to correlate with the regions of viable tumor demonstrated on H & E and regions of elevated contrast intensity on CT. Contrast-enhanced ultrasound imaging of implanted tumors provides a tool to assess differences in the microcirculation of treated and control tumors in studies of anti-angiogenic agents.

In vitro acoustic characterisation of four intravenous ultrasonic contrast agents at 30 MHz

The acoustic properties of four ultrasonic contrast agents (Optison, Definity, SonoVue and Sonazoid) were studied at 30 MHz using a Boston Scientific ClearView Ultra intravascular ultrasound (US) scanner modified to allow access to the unprocessed US data. A range of contrast agent concentrations were studied using either saline or glucose as the diluent of choice. Mean backscatter power was measured over regions-of-interest (ROI) at distances of 1, 1.5, 2, 3, 4 and 5 mm from the centre of the intravascular probe and normalised to the US data collected from a standard glass reflector. For all of the agents, the mean backscatter power at 30 MHz varied in a linear manner with concentration between 0.01 million microbubbles/mL and 1 million microbubbles/mL. Furthermore, for two of the agents, mean backscatter enhancement was detectable at concentrations as low as 2 microbubbles/sample volume.