Hyperpolarized helium3 encapsulated in microbubbles: a new class of blood pool MRI contrast agent

Biomedical imaging with hyperpolarized noble gases

Hyperpolarized noble gases (HNGs), polarized to approximately 50% or higher, have led to major advances in magnetic resonance (MR) imaging of porous structures and air-filled cavities in human subjects, particularly the lung. By boosting the available signal to a level about 100 000 times higher than that at thermal equilibrium, air spaces that would otherwise appear as signal voids in an MR image can be revealed for structural and functional assessments. This review discusses how HNG MR imaging differs from conventional proton MR imaging, how MR pulse sequence design is affected and how the properties of gas imaging can be exploited to obtain hitherto inaccessible information in humans and animals. Current and possible future imaging techniques, and their application in the assessment of normal lung function as well as certain lung diseases, are described.

Microbubbles in Imaging: Applications Beyond Ultrasound

Since their introduction as ultrasound contrast agents, microbubbles have demonstrated the potential to revolutionise the use of ultrasound at the bedside. Aside from clinical application, where microbubbles are used to enhance ultrasonic assessment of myocardial perfusion, they have demonstrated potential in an exciting host of pre-clinical ultrasound imaging and therapeutic applications. These include the ability to target specific cellular markers of disease, provide dynamic blood flow estimation, deliver localised chemotherapy, potentiate the mechanisms of gene therapy, enhance lesion ablation through cavitation, and spatiotemporally permeabilise the blood-brain barrier. The unique and flexible construction of microbubbles not only enables a variety of ultrasound applications, but also opens the door to detection of microbubbles with modalities other than ultrasound. In this review, non-ultrasound imaging applications utilizing microbubbles are discussed, including MRI, PET, and DEI. These various imaging approaches illustrate novel applications of microbubbles, and may provide the groundwork for future multi-modality imaging or image-guided therapeutics.

Lung MRI for experimental drug research

Current techniques to evaluate the efficacy of potential treatments for airways diseases in preclinical models are generally invasive and terminal. In the past few years, the flexibility of magnetic resonance imaging (MRI) to obtain anatomical and functional information of the lung has been explored with the scope of developing a non-invasive approach for the routine testing of drugs in models of airways diseases in small rodents. With MRI, the disease progression can be followed in the same animal. Thus, a significant reduction in the number of animals used for experimentation is achieved, as well as minimal interference with their well-being and physiological status. In addition, under certain circumstances the duration of the observation period after disease onset can be shortened since the technique is able to detect changes before these are reflected in parameters of inflammation determined using invasive procedures. The objective of this article is to briefly address MRI techniques that are being used in experimental lung research, with special emphasis on applications. Following an introduction on proton techniques and MRI of hyperpolarized gases, the attention is shifted to the MRI analysis of several aspects of lung disease models, including inflammation, ventilation, emphysema, fibrosis and sensory nerve activation. The next subject concerns the use of MRI in pharmacological studies within the context of experimental lung research. A final discussion points towards advantages and limitations of MRI in this area.

Perfusion assessment with bolus differentiation: A technique applicable to hyperpolarized tracers

A new technique for assessing tissue blood flow using hyperpolarized tracers, based on the fact that the magnetization of a hyperpolarized substance can be destroyed permanently, is described. Assessments of blood flow with this technique are inherently insensitive to arterial delay and dispersion, and allow for quantification of the transit time and dispersion in the arteries that supply the investigated tissue. Renal cortical blood flow was studied in six rabbits using a 13C-labeled compound (2-hydroxyethylacrylate) that was polarized by the parahydrogen-induced polarization (PHIP) technique. The renal cortical blood flow was estimated to be 5.7/5.4 +/- 1.6/1.3 ml/min per milliliter of tissue (mean +/- SD, right/left kidney), and the mean transit time and dispersion in the renal arteries were determined to be 1.47/1.42 +/- 0.07/0.07 s and 1.78/1.93 +/- 0.40/0.42 s2, respectively.