USE OF A HYPERPOLARIZED GAS FOR MRI DETECTION OF REGIONAL VARIATIONS IN OXYGEN UPTAKE FROM THE LUNGS

Abstract: The invention provides a method of detecting regional variations in oxygen uptake from the lungs of an air-breathing animal subject, said method comprising administering into the lungs of said subject a diagnostically effective amount of a gaseous hyperpolarized magnetic resonance imaging agent, detecting the magnetic resonance signal from said agent in said lungs, determining the temporal variation in relaxation rate for said signal for at least one region of interest whitin said lungs, and from said variation generating a qualitative or quantitative value or image indicative of the oygen concentration in at least one region of interest, and if desired the time dependency of such concentration.

Description: USE OF A HYPERPOLARIZED GAS FOR MRI DETECTION OF REGIONAL VARIATIONS IN OXYGEN UPTAKE FROM THE LUNGS Field of the Invention This invention relates to a method of magnetic resonance imaging of the human or animal (e.g. mammalian, reptilian or avian) body by which lung function and, if desired, morphology may be investigated. Background of the Invention Lung function is of interest to physicians, especially when dealing with patients who may have abnormalities of ventilation or perfusion or other determinants of gas exchange in the lung. For proper lung function five conditions must be met: 1. gas (air) must flow into and out of the lungs; 2. the gas must be distributed evenly within the lungs ; 3. gases must be exchanged by diffusion between the blood and the alveolar space; 4. blood must be pumped through the lungs; and 5. the distribution of the blood in the lungs should match the distribution of gas in the alveolar space (i.e. where the gas penetrates to, blood should flow). All diseases and ailments relating to the lungs and airways affect one or more of the five conditions above. It has therefore been known to study lung ventilation and perfusion using various diagnostic techniques . The conventional technique is known as VQ imaging and involves the use of two different radiopharmaceuticals, one to study perfusion and the other to study ventilation. The perfusion agent is generally a particulate (e.g. 99m Tc-macroaggregated albumin) which is administered intravenously upstream of the lungs and lodges in the precapillary arterioles . Images are recorded with a gamma camera and the signal intensity may be used to detect local abnormalities in blood flow. The ventilation agent is generally a radioactive gas or aerosol or microparticulate, e.g. 133 Xe, 127 Xe or 81m Kr, or a 99m Tc-DTPA aerosol or 99m Tc-labelled carbon particles. The agent is inhaled and an image is recorded with a gamma camera. Signal intensity and distribution may be used to detect airway obstructions or regional abnormalities in ventilation. Where there is a mismatch between the ventilation and perfusion images (which are generated at different times) , various different lung malfunctions, diseases or abnormalities may be diagnosed, e.g. pulmonary embolism, pleural effusion/atelectasis, pneumonia, tumour/hilar adenopathy, pulmonary artery obstruction, AVM, CHF, and intravenous drug use. Heterogenous perfusion patterns may likewise be used to diagnose various disease states or disorders, e.g. CHF, lymphangitic carcinomatosis, non-thrombogenic emboli, vasculitis, chronic interstitial lung disease, and primary pulmonary hypertension. Decreased perfusion to one lung may be used to diagnose pulmonary embolism, pulmonary agenesis, hypoplastic lung (pulmonary artery stenosis) , Swyer- James syndrome, pneumothorax, massive pleural effusion, tumour, pulmonary artery sarcoma and shunt procedures for congenital heart disease. VQ imaging however involves exposing the patient to radiation doses from two radiopharmaceuticals in two temporally separate imaging procedures. Clearance of the injected particulate agent is relatively slow and the agent is taken up in other organs besides the lungs. Moreover, in patients with severe pulmonary hypertension, the injected particulate causes a risk of - 3 - acute right heart failure. For pregnant patients the radiation dose involved in VQ imaging results in undesirable levels of radiation exposure for the foetus. Furthermore, for most diagnostic purposes mentioned above the resolution of conventional VQ imaging is unsatisfactory. There is thus a need for a technique which permits lung function to be assessed without the drawbacks associated with VQ imaging. In magnetic resonance (mr) imaging, radiofrequency signals from non-zero spin nuclei which have a non- equilibrium nuclear spin state distribution are detected and may be manipulated to provide images of the subject under study. In conventional mr imaging the nuclei responsible for the detected signals are protons (usually water protons) and the non-equilibrium spin state distribution is achieved by placing the subject in a strong magnetic field (to enhance the population difference between the proton spin states at equilibrium) and by exposing the subject to pulses of rf radiation at the proton Larmor frequency to excite spin state transitions and create a non-equilibrium spin state distribution. However the maximum deviation from equilibrium is that achievable by spin state population inversion and, since the energy level difference between ground and excited states is small at the temperatures and magnetic field strengths accessible, the signal strength is inherently weak. An alternative approach that has been developed is to "hyperpolarize" (i.e. obtain a nuclear spin state population difference greater than the equilibrium population difference) an imaging agent containing nonzero nuclear spin nuclei (e.g. by optical pumping, by polarization transfer or by subjecting such nuclei ex vivo to much higher magnetic fields than those used in the mr imaging apparatus) , to administer the hyperpolarized agent to the subject, and to detect the mr signals from the hyperpolarized nuclei as they relax back to equilibrium. In this hyperpolarized mr imaging technique, described for example in W095/27438, the hyperpolarized material is conveniently in gaseous form, e.g. 3 He or 129 Xe, and it may thereby be administered by inhalation into the lung and the mr signal detected may be used to generate a morphological image of the lungs . Since the relaxation time T : for 3 He in the lungs is about 10 seconds it is feasible, using fast imaging techniques, to generate a morphological image of the lungs from the 3 He signal following inhalation of hyperpolarized 3 He gas and at any desired stage of the breathing cycle, e.g. during breathhold. Since the mr signal selected is from the 3 He atoms and since the helium is in the gas phase in the lungs, the image detected is essentially only of the airways into and within the lungs. By administering the hyperpolarized agent as a bolus followed or preceded by other gases or aerosols, e.g. by air, nitrogen or 4 He, the hyperpolarized agent can be positioned at any desired section of the airways or other aerated spaces in the body, e.g. it may be flushed from the trachiobronchial tree and the image generated is then essentially only of the alveolar space . We have now found that functional imaging of the lungs may be carried out effectively using mr imaging of an inhaled hyperpolarized agent by making use of the variation with time of the relaxation rate Tj_ of the hyperpolarized agent in conjunction with imaging of the regional and temporal distribution of ventilation using hyperpolarized gases. Summary of the Invention Viewed from one aspect therefore, the invention provides a method of detecting regional variations in oxygen uptake from the lungs of an air-breathing animal subject, e.g. a mammalian (human or non-human) , avian or reptilian subject, said method comprising administering into the lungs of said subject a diagnostically effective amount of a gaseous hyperpolarized magnetic resonance imaging agent, detecting the magnetic resonance signal from said agent in said lungs, determining the temporal variation in relaxation rate (e.g. Tj_ relaxation rate) for said signal for at least one region of interest within said lungs, and from said variation generating a qualitative or quantitative value or image indicative of the oxygen concentration in the alveolar space in said at least one region of interest, and if desired the time dependency of such concentration as a result for example of physiological process, e.g. oxygen uptake by perfusion. In a preferred embodiment, the method of the invention also involves generation of a temporal and/or spatial image of the distribution of the hyperpolarized agent in at least part of the lungs of the subject, preferably in the alveolar space within the lungs. In a further preferred embodiment, the method also involves generation of a magnetic resonance image of at least part of the lungs of the subject following administration into the subject's vasculature of a second mr agent, preferably an agent which affects proton relaxation (with the image generated being a proton mr image) or more preferably an agent containing non-proton mr active nuclei (e.g. 19 F, 13 C, 31 P, 17 0, etc.) in which case the mr image will be generated from mr signals from such non-proton mr active nuclei. The mr active nuclei in the second agent will preferably not be the same as those in the hyperpolarized agent unless the image generated using the second agent is generated at a time when the lungs contain substantially none of the hyperpolarized agent. Lung volume may also be estimated from the integrated 3 He mr signal (or by 3 He mrs) following inhalation of the 3 He without air, breathhold, and expiration where the expired volume is measured directly and the residual hyperpolarization of the retained 3 He is extrapolated from the hyperpolarization value (signal strength) monitored during breathhold. In the method of the invention, it is preferred that for at least part of the mr signal detection period (preferably at least 1 second, more preferably at least 5 seconds, still more preferably at least 10 seconds, e.g. 20 sec to 1 minute), there be substantially no flow of gas into or out of the lungs, e.g. that there should be a breathhold period, and that the indication of oxygen uptake be derived from mr signals detected during at least part of this period. However, in a preferred embodiment, the method of the invention will also involve mr signal detection during gas flow into and/or out of the lungs with or without a period of breathhold. In this way, spatial or temporal images or other indications of lung ventilation may be generated from the detected mr signals. Because the detected mr signal derives from the hyperpolarized agent, the signal strength is effectively independent of the primary field strength of the magnet in the mr imager. Accordingly low or high field, e.g. 0.05 to 3.5T, machines may be used. Description of the Drawings The method of the invention is illustrated by the attached drawings, in which: Figures la and lb show 3 He mr images showing the effect of oxygen and flip angle on the images obtained using a 40 mL bolus of 3 He; Figure 2 shows 3 He mr images of the airway; Figure 3 shows the 3 He mr signal strength in the trachea during inspiration and breathhold where a bolus of 3 He is estimated; - 7 - Figure 4 shows a plot of regional F ιp 0 2 against F et 0 2 (see Example 7) ; Figure 5 showe a plot of F ιp 0 2 versus time (see Example 7) ; Figure 6 shows a plot of D n against number of images (see Example 3) ; Figure 7 shows a plot of signal intensity evolution (see Example 3) ; Figure 8 shows a plot of signal against number of images (see Example 3) ; Figure 9 shows a plot of signal intensities as a function of time (see Example 5) ; Figure 10 shows a plot of p0 2 versus time (see Example 6) ; Figure 11 shows images from a healthy volunteer after inspiration of a single bolus (see Example 9) ; and Figure 12 shows a plot of signal versus time (see Example 9) . Detailed description of the Invention The method of the invention involves administration of a gaseous hyperpolarized mr agent. By a gaseous agent is meant a gas as such (e.g. 3 He or 129 Xe) or a particulate agent held in the gas phase, e.g. an aerosol of powder or droplets. In the latter case, the gaseous carrier preferably is substantially free of paramagnetic gases such as oxygen. The hyperpolarized agent will conveniently have a polarization degree P of 2 to 75%, e.g. 10 to 50%. The mr active (i.e. non-zero nuclear spin) nuclei which are hyperpolarized may be any mr active nuclei which can be hyperpolarized and which can be presented in a gaseous form (i.e. elemental or molecular form, e.g. SF 6 ) which is physiologically tolerable. Examples of appropriate nuclei include various noble gas, carbon, nitrogen and fluorine isotopes; however the noble gases, e.g. He and Xe, and most especially 3 He , are the most preferred. Accordingly, the discussion below will present the invention in terms of 3 He-mr imaging although it does as indicated above, extend to cover the use of other mr active nuclei. During steady state, oxygen transport within the functional units of the lung, i.e. the alveolocapillary unit is characterized by a relationship governed by mass conservation : The net amount of oxygen entering the alveolocapillary unit by the airways has to be equal to the net amount of oxygen leaving the alveolocapillary unit on the blood side. This may be expressed by the equation: V (FiO, F E 0 2 Q [c.O, c v 0. ( i : V = ventilation Q = perfusion F I 0 2 = fractional inspiratory concentration of oxygen F E 0 2 = fractional expiratory concentration of oxygen c a 0 2 = oxygen content of arterial blood c v 0 2 = oxygen content of mixed venous blood Rearrangement of equation (1) provides the following equation for the ventilation-perfusion ratio V'/Q: VI = c 3 0 - C..O-, (2) Q F x 0 2 - F E 0 2 Oxygen contents as well as fractional oxygen concentrations can both be written as functions of oxygen partial pressure, yielding the following equation: VI . _ kj^Q, - p v Q_ 2 l + f(p a 0 2 - p v 0 2 ) (3) Q {p τ 0 2 - p E 0 2 ) Assuming complete equilibration of oxygen partial pressures across the alveolocapillary membrane, p a 0 2 will be equal to p E 0 2 : V_L = k_p E 0 2 - p v 0 2 l + f(p a 0 2 - p v 0 2 ) (4) Q (p x 0 2 - p E 0 2 ) Both k and f depend on a variety of factors, e.g. on barometric pressure, the solubility constant of oxygen in plasma, the dissociation curve of oxygenated haemoglobin, etc., all of which are known. Until now, quantitative description of these oxygen transport processes was possible only on a global basis for the whole organism. With the present invention one is able to measure these processes regionally in the lung. The method may be used to measure regional ventilation, regional partial pressure of oxygen and its time course, with high spatial and temporal resolution. Regional oxygen partial pressure may be measured by hyperpolarized gas magnetic resonance imaging, e.g. hyperpolarised 3 He gas magnetic resonance imaging. To this end, ultrafast MRI sequences are preferably used allowing sequential measurements of the 3 He signal, and its decay, which is dependent both on oxygen and MR acquisition (see Figures 1 a and b) . Signal decay induced by the MR sequence is corrected for by variation of the flip angle and/or of the inter-scan delay. Oxygen concentration inspired into the alveolocapillary unit is not constant during a single inspiration, due to the contribution of deadspace . Therefore, mean inspiratory concentration may be calculated based upon determination of deadspace (from airway imaging by 3 He; see Figure 2) , and from the inspiratory concentration administered at the mouth. - 10 - Regional ventilation may be measured by quantitative analysis of temporal changes in hyperpolarization signal in the trachea, and parallel to this, in the alveolar space, following inspiration of a single bolus of hyperpolarized gas. This analysis is performed on the basis of a mass balance, which allows the determination of functional residual capacity and serial deadspace on a global and regional basis. These signal changes can be measured over several respiratory cycles by ultrafast pulse sequences (e.g., temporal resolution <150 ms) and flow flip angles (Fig. 2 and 3) . Knowing intraalveolar oxygen partial pressure and mean inspiratory oxygen partial pressure, the local V'/Q ratio can be calculated; the addition of local ventilation then allows calculation of regional perfusion. With the assumption that local arterial p0 2 equals alveolar p0 2 , local oxygen uptake can be derived. Thus, for the first time, a complete status of regional oxygen transport in the lung can be obtained. The preferred MRI sequences for use in the method of the invention are: for oxygen partial pressure determination, short repetition time gradient-recalled echo sequences with small flip angle; and - for determination of ventilation, ultra-short repetition time (< 2 ms) gradient-recalled echo sequences with small flip angle, or echo-planar pulse sequences, or ultra-fast sequences using low flip angle and free induction decay. The theory of 3 He-MR-based on p0 2 analysis will now be discussed briefly: The decay of longitudinal magnetization, and hence signal intensity, that occurs with any mr acquisition, follows a function given by: (r) = S n * cos r a (5) - 11 - where n is the number of image acquisition, r is the number of radiofrequency impulses (lines) per image acquired, and a is the flip angle imposed by each consecutive radiofrequency impulse upon the nuclear spin polarization of 3 He in the acquisition volume. Simultaneously, signal intensity (S n ) also begins to decay according to an exponential function, to arrive (within a given time interval Dt) at S n+1 : S n+l ι Dt ( t ) = S n * exp -Dt/Ti f t ) } ( 6 ) The time constant of this decay is determined by the longitudinal spin relaxation time of 3 He, T l r which is shortened in the presence of paramagnetic molecular oxygen . In in vi tro experiments, the following relationship between T λ and oxygen concentration [0 2 ] in a gas mixture containing hyperpolarized 3 He has already been established to be: T ! (0 2 ) = k/ [0 2 ] , where k = 2.27 amagat*s; (7) at temperature 37°C (T x in seconds; [0 2 ] in amagat ; 1 amagat = gas density (2.68675 x 10 13 molecules per cm 3 )) The combined effects of acquisition and time result in a decay function of (valid for constant Tj_) : S n+1 (a,t) = S n * cos r a * expj-Dt/Tj . } (8) More generally, signal of image n acquired at time t n (n = 0, 1, ... n max ) given by [O (t)]dt/k) (8a) S(t n ) = S D (cos a) nr exp ( -J 0 Thus two values (flip angle a and oxygen - 12 - concentration [0 2 (t)]) have to be extracted from image intensities. Therefore make use of imaging with variation of one parameter, e.g. time interval τ between images, or RF amplitude U RF . This can be done either in two separate imaging experiments ("double acquisition") or within one experiment with a more intricate sequence (see attached examples) . Thereby both values can be quantified simultaneously without additional input parameters . Hyperpolarized helium-3 ( 3 He) can be produced by means of direct optical pumping from the metastable state ls2s 3 S 1 at lmb with subsequent conversion to convenient pressures of 1-6 bar. Surkau et al . in Nucl . Inst . & Meth. A384 : 444-450 (1997) describe apparatus which can be used to produce 3 He with a polarization degree P of at least 50% at a flow of 3.5 xlO 18 atoms/sec. or 40% at a flow rate of 8xl0 18 atoms/sec. The hyperpolarized gas may then be filled into glass cylinders, e.g. made of glass which has a low iron content and no coating. These cylinders can be closed by a stop-cock and transported to the mr imaging site, preferably within a magnet, eg a 0.3mT magnet. Under such conditions, the 3 He has a relaxation time (T x ) of up to 70 hours. To perform 3 He mr imaging, the hyperpolarized gas is preferably administered in a bolus into an application unit through which the subject under study may breath freely or alternatively ventilation may be supported by artificial ventilation. For non-human subjects at least, artificial ventilation apparatus will preferably be used and the animals will preferably be anaesthetized and relaxed. For humans, with whom voluntary breathhold is feasible, free breathing through the ventilation unit will generally be preferred. In this way, the 3 He bolus, conveniently of 1 to 1000ml, may be administered at a desired point within the breathing cycle, generally at or close to the beginning of inspiration. The bolus - 13 - size used will depend on the lung size or tidal respiration volume of the subject and will thus vary with subject size or species. However a bolus of 2 to 50%, preferably 5 to 25%, of tidal respiration volume may be suitable. On inspiration the 3 He bolus passes into the airways within about one second with alveolar filling occurring rapidly thereafter for healthy/unobstructed tissue. If inspiration is followed by a period (e.g. of 1 to 60 seconds during which there is substantially no gas flow into or out of the lungs, e.g. a period of breathhold) , the 3 He-mr signal gradually decays at a relaxation rate of the order of 10 seconds. The relaxation rate however is not constant spatially or temporally. Three significant factors contribute to this: loss of polarization due to the magnetic field changes required for mr imaging; loss of polarization due to relaxation enhancement by gaseous oxygen present in the lungs ; and loss of polarization due to relaxation enhancement by the tissue/gas boundary. If the same imaging sequence (s) is used throughout the signal detection period, then the first and third of these factors are constant during a period of no gas flow to/from the lungs; however, 3 He filled volumes as well as oxygen concentration will vary due to physiological processes, e.g. as oxygen is taken up from the lungs in the alveolar space. As a result, in a region of interest where oxygen concentration drops the 3 He relaxation time will increase with time even though absolute signal intensity will continue to drop. While relaxation rate enhancement by lung tissue plays a subordinate role in terms of the overall contributions to the 3 He relaxation rate, it does have a non-uniform effect as different tissues or abnormalities have different effects on the relaxation rate. It is thus preferred not to estimate the oxygen contribution to the relaxation rate by simple reference to a phantom - 14 - undergoing the same field gradient changes as the subject's lung. Use of a phantom is similarly non- preferred due to the inhomogeneity in the applied field across the volume in which the 3 He distributes. Accordingly it is preferred to extract the oxygen contribution to the relaxation rate by mr signal detection during at least two different types of signal generation, e.g. with the different sequences being interleaved. Thus for example the different sequences may involve different RF excitation intensities and/or different sequence intervals (τ). The magnetic field change contribution to the relaxation is desirably minimized so as to prolong the period over which a signal with an acceptable signal to noise ratio can be detected. This is generally achieved by using small flip angles (e.g. less than 7°, preferably less than 4°) in the imaging sequences and in this way mr signals may be detected for up to 60 seconds following bolus 3 He administration. For 3 He-mr imaging, because of the relatively short duration of the hyperpolarization and because relaxation rate change over time is to be studied, it is of course appropriate to use rapid image generating techniques, e.g. fast gradient echo techniques or other techniques with an image acquisition time of less than 2 seconds, preferably 1 second or less. Such techniques are mentioned elsewhere in this specification. Images generated in this way may have a spatial resolution (i.e. voxel size) of less than 20 mm 2 , which is far superior to the scintigraphic ventilation images in conventional VQ imaging. The regions of interest studied in the method of the invention will generally be the alveolar space and thus it is generally preferable that the 3 He bolus be followed in the same gas intake by air or nitrogen to flush the 3 He from the tracheobronchial tree and into the alveolar space. - 15 - As mentioned above, the method of the invention may, and probably will, involve generation of ventilation images, showing spatial and/or temporal distribution of 3 He, thereby permitting ventilation and perfusion to be determined in the same imaging procedure (unlike VQ imaging) . On a morphological level, such ventilation images may identify airway obstructions simply by identifying regions to which the J He does not penetrate, penetrates slowly, or penetrates at lower than normal concentrations. Obstructions and associated hypoperfusion, normal perfusion or hyperperfusion can also be identified by following the time dependence of the 3 He relaxation rate for slowly penetrated alveolar space as the oxygen concentration in such areas may be abnormally low or high. Thus while the mr signal strength may initially be abnormally low, the local relaxation rate may be or become abnormally high or low. Thus if local perfusion does not match local ventillation, oxygen concentration in that part of the lung will be affected and measurable by the method of the invention due to the local abnormal relaxation rate. This would be important in the case of patients with lung malfunction due to smoking. As also mentioned above, 3 He mr imaging may be combined with perfusion imaging with or without administration of a contrast agent, using a second imaging agent administered into the vasculature, e.g. a blood pool agent such as a polymeric paramagnetic chelate, or a superparamagnetic agent or, more preferably because of its oxygen sensitivity, a 19 F fluorocarbon emulsion. In the former cases, imaging would be proton mr imaging, in the latter case 19 F mr imaging. However, the perfusion data collected in this way, although equivalent to the perfusion data collected in VQ imaging, is not absolutely equivalent to that generated in the method of the invention since the second imaging agent distribution merely identifies the - 16 - regions of the lung to which blood flows and not whether or not oxygen uptake by the blood occurs in such regions. Accordingly, the perfusion data from the method of the invention provides a more comprehensive portrayal of lung function. The method of the invention may be used as part of a method of diagnosis of lung malfunction, disease, etc. or indeed in combination with a method of treatment to combat, i.e. prevent or cure or ameliorate, a lung malfunction or disease, etc., e.g. a method involving surgery or administration of therapeutic agents or a method of diagnosis of one of the lung malfunctions or diseases mentioned above. Such methods form further aspects of the present invention as does the use of 3 He (or other mr active nuclei containing materials) for the preparation of a hyperpolarized imaging agent for use in methods of treatment or diagnosis involving performance of the method of the invention. All documents referred to herein are hereby incorporated by reference. The invention will now be illustrated further by reference to the following non-limiting Examples: Example 1 The objectives in this Example were to realize single-breath, single-bolus visualization of intrapulmonarily administered 3 He to analyse nuclear spin relaxation of 3 He in vivo and to determine the regional oxygen concentration, i.e. [0 2 ] , and its time dependent change by perfusion. A double acquisition technique is described which also permits estimation of regional gas transport . In these examinations, the source of the MR signal is the large non-equilibrium polarization of 3 He . This polarization is achieved by means of direct optical pumping from its metastable state ls2s 3 S 1 at lmb with - 17 - subsequent compression to a convenient pressure of 1-6 bar. The apparatus is described by Surkau et al . Nuc . Instr. & Meth. A 384 (1997) 444-450 and is capable of yielding P > 50% at flow of 3.5 x 10 18 atoms/s and 40% at flow 8 x 10 18 atoms/s. The gas is filled into glass cylinders with long relaxation times. Cylinders for medical application are made from "Supremax glass" with low iron content and no coating. They show relaxation times up to 70 h and can be closed by a stop cock and disflanged from the filling system. Transport from the filling site to the MR imaging unit takes place inside a dedicated 0.3 mT guiding field. To perform 3 He-MRI experiments reproducibly, an application system was used. Predefined quantities of 3 He gas at 1 bar pressure can be inserted into breath at a predefined position. Volunteers or patients can breathe freely through the application unit or ventilation can be supported by a commercial respiration machine with controlled pressure. For studies with anesthetized and relaxed animals ventilation is by a respiration machine. Relaxation of the non-equilibrium polarization of inhaled 3 He in vivo is mainly caused by NMR excitations and the presence of oxygen. Relaxation by lung tissue plays a subordinate role as shown by experiments below. The time evolution of the polarization P inside a two- dimensional partition inside ventilated lung spaces can be described by rate equations . Considering the flip angle α and the partial oxygen pressure po we define a time-averaged relaxation rate by NMR via the equation r* P =-rc max rln(cosα)/r (12) (where T tot = duration of measurement, n max = index number of last image, r = number of NMR excitations per image) and by oxygen via the equation - 18 - r c = [o 2 (t)]ik k = 2.27 amagat*s at temperature 37°C referring to 299 Kelvin [see Saam et al . in Phys . Rev. A J52 . (1995) 862-865] . Since [0 2 ] changes in vivo by oxygen consumption, [0 2 ] is taken as a function of time t. Gas exchange from neighbouring volumes with polarization P', e.g. by diffusion, is taken into account by an exchange rate γ, weighted with the polarization difference (P - P ' ) . Assuming only relaxation by oxygen and wall contact for P', the time dependence of P is integrated to: P. = ^~{T RF xp (- JoTo 2 (i)dήcxp (-(T ω + γ) )(cosα)" w + γexp (- ( ln T ( i)di)exp(-T ω t n ) ■ RF ' Experiments have been carried out to investigate the dependence of P (t) on the given parameters. Signal intensities were averaged and analysed over regions of interests (ROIs) . Since signal to noise ratios were always >3, an intensity correction for noise was performed following the method of Gudbjartsson et al . , MRM 3_4 (1995) 910-914. The noise corrected signals A n of the n th image (n = 0, 1, ...) are proportional to P n . The data are normalized and linearized by calculating E n = In (A π /A 0 ) . Imaging of thick and thin partitions is feasible: (a) all spins in the lung are equally excited. This greatly simplifies matters and is to be preferred in practical applications. In this case, the effect of gas exchange is rendered unobservable, i.e. (P - P') = 0 for all times. Experimentally, it can be achieved either by - 19 - use of thick slices in 2D techniques, or by 3D acquisitions covering the entire inhaled volume of 3 He . (b) The volume V of the imaged partition is thin compared to the surrounding volume V with which diffusive contact exists within the time scale of a typical imaging sequence. In this case Y and y' scale according to the ratio of the volumes involved, hence γ r = γ.V/V . Thus Y' may be neglected if V << V . The idea of double acquisition imaging is best illustrated by a simple example. Consider a set of images with a single thick slice (i.e. suppressing diffusion effects) . If images are taken in equidistant interscan times (hence, t n = n.τ) : E. = - f m T 02 (t)dt + N n In (cosα) [14] Jo Method 1 The second set of images is acquired retaining τ , but doubling . Assuming p 02 and its time development to be equal in a given ROI during both series, the E n values of corresponding images can be subtracted giving E n (α) - E„(2α) cosα =n In [15] N cos 2αJ If the left hand side of [15] is plotted against n, In (cos α/cos 2α) and furthermore α are obtained from the slope. In a second step, eq. [14] of either dataset is corrected for flip angle effects, and r 02 is extracted by a fit. Method 2 The second set of images is acquired with the same - 20 - RF amplitude, but with a different τ. In this case, subtraction of corresponding E n values results in elimination of the (cos α) term in eq. [14] : E n -E n ) = r 2 p 02 {τ) dt - f ml p 02 (t) dt [16] Thus, information about the temporal development of P 02 is obtained. By correcting eq. [14] for this relaxation effect, depolarization by RF excitations can be computed. Example 2 Wall relaxation by lung tissue is negligible. The effect of wall relaxation was measured in a deoxygenized lung of a dead pig by double acquisition sampling with varied flip angles (method 1) . Immediately after inducing cardiac arrest, oxygen was washed out by ventilating with pure nitrogen for about 15 mins . Subsequently, two series of 11 images each were taken, with RF amplitudes U RF = 10V in the first and U RF = 5V in the second series. Partition thickness was 120 mm in coronal orientation in order to excite 3 He spins in the entire lung volume. InterScan time τ was 7 sees. A ROI of 415 pixel (6.5 cm 2 ) within the cranial left lung was examined. A time constant of longitudinal relaxation T λ = 261(4) sees was fitted to the data. This is in accordance with a possible residual oxygen concentration of about 10 mb. The value should thus be understood as a lower limit of wall relaxation time. Assuming wall relaxation only, lung tissue shows a cm/hour rate of at least 1/22 cm/hour (assuming spherical alveoles with radius r = 200 μm) . This value is smaller than that of most bare glass surfaces (see Heil et al . , in Phys.Lett. A 201 337 (1995). It means that non-diseased broncho-alveolar surfaces contain practically no radicals nor other paramagnetic centers. - 21 - Example 3 One anaesthezied pig (27 kg) was normoventilated inside a MRI unit (Siemens Vision scanner with B = 1.5 T, equipped with one of two transmit/receive coils resonant to 3 He at 48.44 MHz) . After administering a = 100 cm 3 bolus of 3 He, two series of 2D FLASH (TE < 4 ms , TR 11 ms) , images in transversal orientation were taken during breathhold. Predefined RF excitation intensities U were 10 and 20 Volts and intervals τ of 1.5s were used. Partition thickness was 20 mm. Signal intensities were averaged and analyzed over regions of interest (ROIs) . An intensity correction for noise was performed following Gudbjartsson et al . MRM 3_4: 910-914 (1995) . A first postprocessing was performed calculating E n = ln(A n /A 0 ) for both series, where "In" denotes the natural logarithm function. Following the dependence E n [WV] - E n [20V] ( cos α \ n In [17] »- N I cos2α Figure 6 shows a linear graph (N total number of images taken, n the considered image number) . Solving equation (17) one determines the flip α = 3.4°. Knowing this value, one can fit the signal intensity evolution with the image number given in Figure 7. A linear dependency of the regional partial oxygen pressure proved by other experiments is assumed: p(t) = p 0 - mt with time t, coefficient m and pressure p 0 at the beginning of the measurement. By method 1, [0 2 ] = 0.108(3) amagat and its change with time by m = 0.0026(5) amagat/s are extracted (see Figure 8) . Two more theoretical curves indicate the temporal evolution, if no change of partial oxygen pressure takes place (m = 0 amagat/s, p 0 = 0.108 amagat) and if no - 22 - relaxation by oxygen would be present (m = 0 amagat/s, p 0 = 0 amagat) . Both curves indicate, the significant change of partial oxygen pressure. The low value for regional p 0 found seems to be real from comparison with other analyses which yield the same flip angles for such excitation intensities. Example 4 In this example, we present an example of in vivo oxygen determination, as obtained from double acquisition with varied interscan time τ (method 2) . An anaesthetized pig underwent controlled ventilation with room air (oxygen concentration 21%) . After He bolus injection, a series of 8 images with τ x = 7 s was acquired during inspiratory apnea (~ 50 s) . After a short interval to ensure stability of vital parameters, a second series of 8 images with τ 2 = 1 s was taken. RF amplitude was 10 V in both series, partition thickness was 120 mm in coronal orientation. The oxygen density p 02 (t) is determined from the sequence of normalised logarithmic intensities E lf E 2 ...E n . The procedure is simplified if it is assumed a priori that the time dependence of p 02 be linear p 02 (t) = p 0 - Rt, [18] where R is the rate of oxygen decrease. One then computes E (τ.) - E ( x~) n [19] n(τ 2 - τ,) 12 Comparison with eq. [18] shows that the experimental quantities y n just equal the searched for oxygen density 23 y n = P02 (t n ) [20] at mean times t n = n(τ x + τ 2 )/2. The time course of p 02 (t n ) was obtained via eq. [20] within a ROI in the middle section of the right lung which comprises 89 pixel and covers an area of 1.39 cm 2 . A linear decrease of p 02 with time was observed, thus confirming the assumption a posteriori. A linear fit to the data yields p 0 = 0.168(5) amagat and R = 0.0034(2) amagat/s with a x 2 of 1.00 p.d.f. Consistent with physiology, the initial oxygen concentration is found to be lower in the functional residual capacity (FRC) of the lung than in inspired air . Once the temporal evolution of p 02 is determined, the flip angle α remains the only unknown parameter in eq. [8a] . Considering the uncertainties of intensities as statistical and those of p 0 and R as additional systematic errors, the τ = Is series yields α = 3.36 (10)° and the τ = 7s series α = 3.1(3)°. - 24 - Example 5 Effects of Gas Transport Phenomena in the lung on the MR Signal According to eq. [14] , the dynamics of intrapulmonary 3 He polarization are changed significantly when diffusive and/or convective gas transport is taken into account . This is necessarily the case when the imaged partition is thin compared to the total lung volume. In this example, a 20mm slice of a porcine lung was imaged in transversal orientation. Images were taken after cardiac arrest to ensure a time-constant p 02 (i.e. m = 0) . The inspiratory oxygen concentration was set to (30+1)%. Two series of nine images each were acquired with RF amplitudes of 10 and 20 V respectively. InterScan delays τ were alternating 1.2s and 1.8s. A ROI of 510 pixel, placed in the left lung, was analyzed in this example. The procedure in this case is as follows. As long as the polarization difference P-P ' between the imaged partition and non-imaged surrounding is small, the effect of gas exchange is considered negligible, hence P-P'~0 is approximated in the first three images. Thus, α and p 0 are computed in the same way as in example 3. Using γ=0 and linear fitting of subtracted logarithmic intensities E n (n=0,l,2), we obtain a flip angle α- 2.9(1)° for 10 V excitation. Subsequently, flip angle corrected intensities of these first images are fitted to determine p 0 =0.31(2) amagat. In a third step, the entire dataset of one acquisition is utilized to fit γ according to eq. [14] . Fig. 9 depicts the signal intensities A n (U HF =10 V) as a function of time. The upper curve refers to a fit with r RF =0.070s "1 and p 02 =p 0 =0.31 amagat as input parameters. The fit yields γ=0.056 (26) s "1 . Also shown is a curve for identical flip angle and oxygen - 25 - concentration, but with γ=0. Clearly this curve tends to increasingly disagree with the data points after about 5s, whereas only a small discrepancy is detected for the first three images, justifying the said method of analysis . Example 6 Determination of Oxygen Concentration using a Single Acquisition In this example the imaged object was a rubber bag of volume 0.5 liters. An application of 3 He bolus 0.1 1, flushed by 0.4 1 of air (0 2 concentration 21%) was performed. The imaging was performed on (Siemens Vision Scanner with B=l .5 T equipped with transmit/receive coil resonant to 3 He at 48.44 MHz) using a 2D Flash sequence, partition thickness 12 cm, covering entire volume of bag. Parameter variation was realized with one single imaging sequence, permitting quantification of flip angle and oxygen concentration. 7 images were taken with U HF =5 V, interscan time 2.6s. Thereafter, 6 images were taken with U HF =20 V, interscan time Is. Flip angle was determined from a fit of intensities of a ROI of the last 6 images, "guessing" an initial oxygen concentration. Obtained result was used to compute [0 2 ] (t) from a fit of intensities of a ROI of the first 7 images. Accuracy was improved by iterating this process 2 times. Results: flip angle a was determined to be 4.40(7)° for 20 V excitation. Oxygen concentration was determined to 0.186(7) amagat, consistent with 0 2 concentration in room air. Since a phantom was imaged, no decrease of oxygen - 26 - was observed, see Fig. 10. Example 7 A First Oxygen Determination Routine using Variation of Low Flip Angle Hyperpolarized 3 Helium ( 3 He) is described as non- radioactive inhalational contrast agent for magnetic resonance (MR) tomography of ventilated lung spaces. In 3 He-MRI, signal intensity is destroyed irrecoverably by (1) the presence of paramagnetic oxygen in the respiratory gas and (2) MR image acquisition itself. Regional intrapulmonary [0 2 ] as a sum of inspiratory oxygen concentration (FjOg) , distribution of ventilation, and oxygen uptake is determined in clinical practice globally over the whole lung. The aim was to use the effect of oxygen upon 3 He to visualise regional intrapulmonary [0 2 ] in MR for the first time on a regional basis. Animal and Methods: Eight anesthetized healthy pigs (28+2 kg) were normoventilated in a 1.5 T MRI unit fitted with a Helmholtz transmit-receive coil tuned to 48.4 MHz. Hemodynamic parameters and end-tidal [0 2 ] were measured continuously. Interventions included variation of 3 He bolus sizes, of RF amplitudes for MR-image acquisition (10V and 20V) , of end-tidal [0 2 ] (0.16, 0.25, 0.35 and 0.45), and comparison of intrapulmonary [0 2 ] before and after induction of cardiac arrest. Using a dedicated application unit specifically designed by our group, see PCT/EP98/07516 (copy filed herewith) , boli of 3 He (up to 45% polarized) were administered at the beginning of inspiratory tidal volumes. During subsequent inspiratory apnea, serial 3 He images of airways and lungs were acquired using a two- dimensional FLASH sequence (image acquisition time = 1 - 27 - s; TR = 11 ms/TE = 4.2 ms; 1.5 s inter-image delay) . The decay of MR signal intensities in various regions of interest within pulmonary cross-sections was analysed with respect to the different interventions. RF excitation effects upon signal intensity decay were separated from oxygen effects by comparison of image series acquired with two different flip angles <7°. Results: Single-breath, single-bolus 3 He administration allowed reproducible visualization of airways and lungs. Bolus volumina between 20 mL and 100 mL could be administered reproducibly (40 mL : 39 ± 4 mL; 100 mL : 100 + 4 mL; n=25) . Images containing regions with a signal-to-noise ratio > 3 were required for analysis of the signal decay function; this could be achieved in up to 10 subsequent images following a single 3 He bolus. T : of hyperpolarized 3 He demonstrated a similar relationship to ambient [0 2 ] as had been found in vi tro . Signal analysis within two consecutive images, which were acquired at a known F et 0 2 , allowed determination of polarization loss due to MR acquisition (for 10V or 20V, respectively) . Taking this effect into account, the analysis of independently acquired image series yielded estimates for regional [0 2 ] . Analysis of MR signal decay in defined ROIs of two-dimensional 3 He images yielded values for regional intrapulmonary [0 2 ] which correlated closely with end-expiratory [0 2 ] (r = 0.94; p<0.001, Figure 4) before induction of cardiac arrest, and with inspiratory oxygen concentration during absence of perfusion. Conclusions: This study demonstrates a) reproducible visualization of small quantities of 3 He in the lungs, b) in vivo confirmation of the oxygen-T relationship described by Saam et al . in Phys.Rev. A52, 862 (1995) , c) feasibility of non-invasive MR-based analysis of regional intrapulmonary [0 2 ] in a range of oxygen concentrations which is used in ventilator- dependent patients, and d) , significant correlation of - 28 - 3 He-MR-determined with measured end-expiratory oxygen concentrations. As hyperpolarized 3 He can be distributed in special glass cells (half-time of hyperpolarization > 80 h) , and technical requirements are limited to a spectroscopy option for the used MR scanner and a dedicated 3 He-coil, early propagation of this method is expected. The new technique may provide insight into regional 0 2 exchange in the lungs . Further human and animal studies are necessary to demonstrate the spatial and temporal resolution in the analysis of 0 2 distribution and exchange under pathological conditions by this non-invasive new technique. Figure 5 shows the analysis of the time course of oxygen concentration in the lung of a male volunteer, analysed with the double acquisition method with variation of flip angle as described in the present example above. Initial oxygen concentration at the beginning of the breathhold (0.189) and calculated oxygen decrease during apnea (0.01/s) can be followed. Example 8 3 He gas was hyperpolarized to approximately 40-50% by optical pumping. 12 volunteers and 10 pneurologic patients inhaled such gas from glass cylinders of 300 mL volume and 3 bar pressure. 3 He-MRI was performed during breathhold using a 3D gradient-recalled-echo imaging sequence on a Siemens 1.5T clinical scanner, adjusted to have a transmitter frequency of 48.4 MHz and using a Helmholtz transmit/receive RF coil. A flip angle less than 5° was used. In quantitative studies, faster, repeated 3D images (TR=5ms, TE=2ms) were acquired at intervals of 0.8, 16, 42 and 55 seconds in normal volunteers. From these 5 images, extraction of both regional flip angle and regional T l was possible defining the effects of repeated RF pulsing and longitudinal relaxation in terms of decay - 29 - rate constants, r RF and r RELAX respectively. For a pulse train of duration T, consisting of N pulses of flip angle φ, r RF is given by: r RF T = [cos(φ)] N (15) On the other hand, the contribution of longitudinal relaxation depends on absolute time, not on the duration of the RF pulsing. Thus by using a non-linear image timing sequence, the two effects can be resolved and both flip angle and T x determined regionally. A final study, using an ultrafast 2D sequence, generated images every 1 second during inspiration, breathhold and expiration. Results: All volunteers and 8/10 patients were able to perform the necessary inhalation. One patient was claustrophobic and 1 patient could not maintain a 25-second breathhold. The central airways were consistently visualized. Volunteers demonstrated homogeneous signal intensity; patients with obstructive lung disease and/or pneumonia demonstrated characteristically inhomogeneous signal intensities, specific for the disorder. Flip angle calibration confirmed an estimated flip angle of 1-2°. T : was derived to be 32±3 seconds in normal lung. In phantoms, longitudinal relaxation was negligible compared with RF pulsing over a time period of 1 minute (this is consistent with predicted T x values of tens of hours) . Using the rapid 2D sequence, the inspiratory process could be seen to have a timecourse of less than Is in normal lung (providing ' instantaneous ' uniform signal) . Expiration gave rise to slower signal change. The signal reducing effect of expiration could be clearly discriminated from the continuing destruction of polarization by RF pulsing, allowing estimation of hung residual volume. - 30 - Conclusion: 3 He-MRI with inspiration of hyperpolarized 3 He provides a means of imaging lung ventilation. Lung filling and ventilatory obstruction can be examined with dynamic MRI. Quantitation, particularly of regional 3 He T 2 , provides a means of assessing local physiologic parameters, such as p0 2 . The simple quantitative approaches described in this Example slow 3 He-MRI of the lung provides a modality capable of providing regional functional and physiological information. Example 9 Ultrafast Ventilation Scan Material and methods: Coronal images of the lung were acquired at 48.44 MHz using ultrafast gradient-echo pulse sequence with TR/TE/a=2. Oms/0.7ms/l .5° . A series of 160 projection images was obtained with 128ms temporal resolution. Imaging was performed before, during and after application of a single bolus of approximately 300ml 3 He in five healthy volunteers (spontaneous breathing) . The signal intensities were corrected for depolarisation by RF excitation on the basis of equation (5) of this invention. Images from a healthy volunteer at time 0s, 0.13s, 0.26s, 0.65s, 1.17s, 1.95s, 3.77s and 6.37s after inspiration of a single bolus (285 mL) hyperpolarized Helium-3 are shown in Figure 11. Figure 12, meanwhile, shows signal-time- curves in trachea and in parenchyma on the right side of the lung in the patient of Figure 11. Shaded areas denote intervals of expiration (determined from the diaphragm position) , interrupted by intervals of inspiration (not shaded) . During the first phase of inspiration, 3He signal appears in the trachea. It reappears during the expiratory cycles. After a delayed signal increase in alveolar space, 3He signal decreases - 31 - there due to T x relaxation, depolarisation by RF pulses, and due to expiration and inspiration with air. Results: In these gradient recalled images no susceptibility artifacts are observed. Distribution of the 3 He boli was observed in the trachea, in mainstem and distal bronchi down to fourth order, and in alveolar space. The temporal resolution was 130 ms, spatial resolution was 2.5mm x 4.4mm. The signal of a single bolus of 3 He was detected in the lung for up to 20s. The peak signal-to-noise ratio in the lung was 11.7±7.7. While the time-to-peak of the bolus signal in the trachea was 260ms, it was significantly longer in lung parenchyma (910ms) . Conclusion: Individual phases of inspiration, distribution of 3 He within the alveolar space and expiration can be visualized by ultrafast imaging of a single bolus of hyperpolarized He gas. This method may allow for regional analysis of lung function with temporal and spatial resolution superior to conventional methods.

Claims: - 32 - Claims 1. A method of detecting regional variations in oxygen uptake from the lungs of an air-breathing animal subject, said method comprising administering into the lungs of said subject a diagnostically effective amount of a gaseous hyperpolarized magnetic resonance imaging agent, detecting the magnetic resonance signal from said agent in said lungs, determining the temporal variation in relaxation rate for said signal for at least one region of interest within said lungs, and from said variation generating a qualitative or quantitative value or image indicative of the oxygen concentration in at least one region of interest, and if desired the time dependency of such concentration. 2. A method as claimed in claim 1 wherein said hyperpolarized agent comprises 3 He . 3. A method as claimed in claim 1 wherein detection of said magnetic resonance signal is effected during a period of at least 1 second during which there is substantially no gas flow into or out of the lungs. 4. A method as claimed in claim 1 wherein said regions of interest comprise regions of alveolar space. 5. A method as claimed in claim 1 wherein a temporal and/or spatial mr image of at least part of the lungs comprising said regions of interest is also generated. 6. A method as claimed in claim 5 wherein said temporal and/or spatial image is constructed from magnetic resonance signals from said hyperpolarized agent. 7. A method as claimed in claim 5 wherein said - 33 - temporal and/or spatial image is constructed from magnetic resonance signals from magnetic resonance active nuclei in a further magnetic resonance imaging agent administered into the vasculature or lungs of said subject. 8. A method as claimed in claim 7 wherein said further agent comprises a 19 F fluorocarbon. 9. A method as claimed in claim 1 wherein said magnetic resonance signals are detected in at least two different types of magnetic resonance imaging sequence. 10. A method as claimed in claim 9 wherein said types of sequence differ in the intensity of the magnetic resonance signal stimulating radiation. 11. A method as claimed in claim 9 wherein said types of sequence differ in the sequence timing. 12. A method as claimed in claim 9 wherein said types of sequence are interleaved. 13. A method as claimed in claim 1 wherein magnetic resonance signal detection is effected in an imaging sequence with an image acquisition time of less than 2 seconds . 14. A method as claimed in claim 1 wherein magnetic resonance signal detection is effected in an imaging sequence involving imposition of a flip angle of less than 7°. 15. A method as claimed in claim 1 wherein said hyperpolarized agent is administered as a bolus. 16. A method as claimed in claim 1 wherein said - 34 - hyperpolarized agent is administered as a bolus of volume 1 to 1000 ml. 17. A method as claimed in claim 1 wherein a mr imager with a primary field strength in the range of 0.05 to 8T, preferably 0.05 to 3.5T, is used to detect said magnetic resonance signal. 18. A method as claimed in claim 1 wherein said hyperpolarized agent comprises 129 Xe. 19. A method as claimed in any one of the preceding claims wherein the acquisition time of said image is in the subsecond range . 20. A method as claimed in any one of the preceding claims wherein said image is produced by any method selected from the group of gradient-recalled-echo imaging, echo-planar imaging, turbo-spin-echo imaging and imaging based on projection techniques. 21. A method as claimed in any one of the preceding claims allowing determination of functional residual capacity, dead space and regional ventilation.

Inventors: DENINGER ANSELM, EBERLE BALTHASAR, EBERT MICHAEL, GROSSMAN TINO, HEIL WERNER, KAUCZOR HANS-ULRICH, LAUER LARS, MARKSTALLER KLAUS, ROBERTS TIMOTHY, SCHREIBER WOLFGANG, SURKAU REINHARD, WEILER NORBERT, DENINGER, ANSELM, EBERLE, BALTHASAR, EBERT, MICHAEL, GROSSMAN, TINO, HEIL, WERNER, KAUCZOR, HANS-ULRICH, LAUER, LARS, MARKSTALLER, KLAUS, ROBERTS, TIMOTHY, SCHREIBER, WOLFGANG, SURKAU, REINHARD, WEILER, NORBERT
Applicants: DENINGER ANSELM, EBERLE BALTHASAR, EBERT MICHAEL, GROSSMAN TINO, HEIL WERNER, KAUCZOR HANS ULRICH, LAUER LARS, MARKSTALLER KLAUS, ROBERTS TIMOTHY, SCHREIBER WOLFGANG, SURKAU REINHARD, WEILER NORBERT, DENINGER, ANSELM, EBERLE, BALTHASAR, EBERT, MICHAEL, GROSSMAN, TINO, HEIL, WERNER, KAUCZOR, HANS-ULRICH, LAUER, LARS, MARKSTALLER, KLAUS, ROBERTS, TIMOTHY, SCHREIBER, WOLFGANG, SURKAU, REINHARD, WEILER, NORBERT
Application year: 1999
Main classification: G01R33
IPC codes: G01R33