As currently implemented, magnetic resonance imaging (MRI) relies on the protons of water molecules in tissue to provide the NMR signal. Protons are, however, notoriously difficult to image in some biological environments of interest, notably the lungs and lipid bilayer membranes such as those in the brain. Here we show that 129Xe gas can be used for high-resolution MRI when the nuclear-spin polarization of the atoms is increased by laser optical pumping and spin exchange. This process produces hyperpolarized 129Xe, in which the magnetization is enhanced by a factor of about 10(5). By introducing hyperpolarized 129Xe into mouse lungs we have obtained images of the lung gas space with a speed and a resolution better than those available from proton MRI or emission tomography. As xenon (a safe general anaesthetic) is rapidly and safely transferred from the lungs to blood and thence to other tissues, where it is concentrated in lipid and protein components, images of the circulatory system, the brain and other vital organs can also be obtained. Because the magnetic behaviour of 129Xe is very sensitive to its environment, and is different from that of 1H2O, MRI using hyperpolarized 129Xe should involve distinct and sensitive mechanisms for tissue contrast.

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Contrast reagents (CRs) may enter the tissue interstitium for a period after a vascular bolus injection. As the amount of interstitial CR increases, the longitudinal relaxographic NMR "shutter-speed" (T

The bulk magnetic susceptibility (BMS) shift of a nuclear resonance frequency caused by a paramagnetic compound is of importance in vivo NMR, both magnetic resonance spectroscopy and magnetic resonance imaging. However, since it is a rather complicated phenomenon, it has been the source of many misinterpretations in the literature. We have reworked and organized the theory of the BMS shift. This includes accounting for the important effects of local susceptibility. We have conducted experiments on phantom samples in order to illustrate the principles involved. Our phantoms consist of capillaries and coaxial cylinders. They simulate the situations of blood vessels oriented parallel and perpendicular to the magnetic field and the interstitial spaces surrounding them. In most of our experiments, the paramagnetic compound was one of several different hyperfine shift reagents for cation resonances. These were chosen to cover a range of potencies, in both magnitude and sign, of the shifts they produce. However, we also used a reagent which was incapable of inducing a hyperfine shift and thus could cause only a BMS shift. Although we report only 23Na spectra in this paper, the latter samples simulate the cases where one observes the water 1H resonance in experiments employing hyperfine shift reagents for cations. There have been a number of such investigations recently reported in the literature. The principles considered in this paper allow us to offer new interpretations for the results of several experiments published in the last few years.

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An extensive protocol for the study of tissue resonances of spin 3/2 nuclei is described. The roles of the most relevant multiple pulse experiments are indicated. Their theory is organized in terms of irreducible tensor operators and the pulse and quadrupolar relaxation transfer functions which relate them for a type c spectrum. A systematic approach to the interpretation of the temperature and/or magnetic field dependences of all six of the relaxation rate constants of the resonance of a single population of isolated spins in fast exchange, and giving rise to a type c spectrum, is presented. An experimental calibration and an application of this protocol are presented in an accompanying paper. The comprehensive method we describe has a number of practical benefits in the interpretation of the physiological spectra obtained from conventional one pulse experiments. A consideration of the appropriate transverse relaxation transfer function leads to an analytical expression for the heretofore empirical NMR visibility factor. This includes factors which account for relaxation during the receiver 'dead' time and relaxation during the pulse itself. Also, consideration of realistic transverse relaxation times likely to be observed in tissue leads to a reasonable strategy for the quantitative resolution and integration of in vivo spectra obtained in the presence of hyperfine shift reagents.