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Basic Science Investigations |
1 Division of Radiological Sciences, Mallinckrodt Institute of Radiology, Washington University School of Medicine, St. Louis, Missouri
2 Biomedical Imaging Research Center, Fukui Medical University, Matsuoka, Fukui, Japan
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ABSTRACT |
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 TOP ABSTRACT INTRODUCTIONMATERIALS AND METHODSRESULTSDISCUSSIONCONCLUSIONREFERENCES |
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3 h after occlusion, retention of *Cu-ATSM within 20 min was greater in ischemic regions (myocardial blood flow, 0.28 ± 0.26 mL·min-1·g-1) than in normal tissue (myocardial blood flow, 0.52 ± 0.19 mL·min-1·g-1) (1/kmono, 40.72 ± 39.0 min vs. 26.69 ± 22.29 min [P < 0.05]; 1/k4, 6.85 ± 4.90 min vs. 3.51 ± 1.97 min [P < 0.05]). In selected dogs, tracer retention decreased at 24 h, suggesting the development of necrosis with no subsequent retention of *Cu-ATSM. In protocol III, dobutamine infusion after stenosis placement resulted in increased tracer retention consistent with hypoxia in the damaged regions. Conclusion: *Cu-ATSM PET has shown quantitative selective uptake in hypoxic myocardium within 20 min of tracer administration in 3 canine models of hypoxia.
Key Words: copper(II)-diacetyl-bis(N4-methylthiosemicarbazone) • imaging • ischemia • hypoxia
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INTRODUCTION |
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TOPABSTRACTINTRODUCTIONMATERIALS AND METHODSRESULTSDISCUSSIONCONCLUSIONREFERENCES |
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The importance of developing imaging agents capable of delineating hypoxia in tissue is well established (1,2). Misonidazole analogs and 2-nitroimidazole functionalities have been labeled with iodine radionuclides (e.g., 123I-iodoazomycin arabinoside (3,4)) and with 99mTc for SPECT and 18F for PET imaging of hypoxia. The 99mTc-compounds 99mTc-HL91 (5), BMS-181321 (6), and BMS-194796 (7) have demonstrated increased uptake in hypoxic and low-flow ischemic myocardium. The PET agent 18F-fluoromisonidazole (FMISO) is retained in hypoxic tissue in the myocardium, and clinical studies show differences that can be imaged between normal and hypoxic tissues (8–11). Nitroimidazole-based agents suffer from 2 disadvantages, low cellular uptake and slow normal-tissue clearance, requiring long periods between injection and imaging (2,8,9).
Copper(II)-diacetyl-bis(N4-methylthiosemicarbazone) (copper-ATSM) is in a class of copper bis(thiosemicarbazones) that have been evaluated in vitro and display uptake that either is not hypoxia selective (e.g., copper[II]-pyruvaldehyde-bis[N4-methylthiosemicarbazone], copper-PTSM (12,13)) or is hypoxia selective (14–16). In vivo, 64Cu-ATSM is rapidly retained in hypoxic tumors and myocardium but diffuses in normoxic tissue (14,17–19). In experimental tumor models, the selective uptake of 64Cu-ATSM depended on the partial pressure of oxygen (pO2), and a direct correlation between tissue uptake of 64Cu-ATSM and tissue pO2 was observed, with significantly greater retention in hypoxic tissue (14,18). Studies using an acute myocardial infarction rat heart model, in which oxygen concentration can be controlled, showed that specific retention of 64Cu-ATSM is due to oxygen depletion (16). The results of preliminary studies in Japan have demonstrated the potential of 62Cu-ATSM for hypoxia imaging in acute ischemia syndromes (19). Because of the increasing availability of positron-emitting isotopes of copper (60Cu [half-life (t1/2) = 0.40 h, ß+ = 93%, electron capture (EC) = 7%], 61Cu [t1/2 = 3.32 h, ß+ = 62%, EC = 40%], 62Cu [t1/2 = 0.16 h, ß+ = 98%, EC = 2%], and 64Cu [t1/2 = 12.7 h, ß+ = 17.4%, EC = 43%]) (20–22), we have continued to investigate *Cu-ATSM (where *Cu is defined as either 60Cu, 61Cu, or 64Cu) as a noninvasive selective marker for myocardial hypoxia in canine models of ischemia before human evaluation.
Previous studies using rodent hypoxia models have established the hypoxia selectivity of *Cu-ATSM in vivo (14,17,18), and the current study was undertaken to determine the selectivity of *Cu-ATSM for myocardial models of hypoxia in canines before human trials. Protocol I was undertaken to determine the relationship between *Cu-ATSM retention/washout and myocardial blood flow (MBF). Protocol II was undertaken to elucidate the usefulness of *Cu-ATSM PET for acute ischemic syndromes such as myocardial infarction when flow is limited. This model was also used to demonstrate the kinetics of *Cu-ATSM in necrotic tissue. Protocol III was undertaken to show the imaging characteristics of *Cu-ATSM when ischemia is induced without a severe flow limitation (as is observed in an abnormal rest/stress echocardiogram), which is the most common clinical scenario in which myocardial hypoxia is documented. Hypoxia and ischemia are 2 different physiologic states, and this study was performed to examine the oxygen-deprived myocardial states of both hypoxia and ischemia.
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MATERIALS AND METHODS |
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TOPABSTRACTINTRODUCTIONMATERIALS AND METHODSRESULTSDISCUSSIONCONCLUSIONREFERENCES |
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resistivity). Radioactive samples were counted on a 
-counter (model 8000; Beckman, Irvine, CA).
Radioisotope Production and Characteristics
64Cu-, 61Cu-, and 60Cu-ATSM were prepared as previously described (20,21). At our institution, we can make these 3 copper radioisotopes on demand, and the choice of which isotope to use for a particular study was based on radioactive half-life to allow for repeated imaging sessions when required. To ensure a similar resolution between each isotope, the phantom of Derenzo et al. (23) for 64Cu and 60Cu was imaged on our ECAT 962 HR+ scanner (Siemens, Knoxville, TN). The phantom consists of 10-cm cylindric holes drilled into a clear plastic cylinder (23). The rods are arranged in a pielike pattern and have diameters of 2.5, 3, 3.5, 4, 5, and 6.25 mm. The phantom was filled with water containing a dilute amount of 60Cu or 64Cu with a concentration of 296 kBq/mL. The total volume of the phantom is 220 mL. Imaging was performed by acquiring static emission data for 1 h. Images were then reconstructed with filtered backprojection using a ramp filter at Nyquist frequency and a zoom of 2. A calculated attenuation correction was applied. The resulting pixel size was 0.24 cm. The entire volume of data for 1 bed position was reconstructed and contained 63 slices of 128 x 128 pixels. Data were corrected for scatter using the manufacturer-provided method. The random coincidences were removed using the delayed window technique.
Animal Protocol
Male mongrel dogs (20–25 kg) were purchased from Butler Farms USA, Inc. (Clyde, NY). All animal experiments were conducted in compliance with the Guidelines for the Care and Use of Research Animals established by the Animal Studies Committee at our institution. Dogs were premedicated with 1–1.5 mg/kg of morphine sulfate injection (King Pharmaceuticals, Bristol, TN). Anesthesia was induced by 12.5 mg/kg of 5% sodium thiopental solution and maintained by titrating the recommended doses of 
-chloralose as needed. Each dog was hemodynamically monitored throughout the experiment. Percutaneous sheaths were placed in bilateral femoral arteries and veins for direct arterial blood pressure measurement; anesthesia maintenance; and fluid, drug, or radiopharmaceutical administration. The sheaths were kept in situ until euthanasia.
Protocol I: Induction of Myocardial Hypoxia by Generation of Global Hypoxia (n = 3).
The dogs were administered a fractional concentration of oxygen in inspired gas of 100%, and 15O-H2O PET and 60Cu-ATSM PET were performed as described in Imaging Protocols and Data Collection. After the first 60Cu-ATSM PET scan was complete, global hypoxia was induced by ventilating the dog on 90% N2:10% O2 (24), a mixture for which, at these pO2 levels, hypoxemia leads to hypoxia. The measurement of blood oxygen levels throughout the study demonstrated arterial blood hypoxemia, suggesting global tissue hypoxia, and with the evident increase in blood flow and the external signs of cyanosis, the presence of hypoxic myocardium was expected. After the arterial pO2 levels decreased to 35%–45% that of baseline (approximately 50 min), 15O-H2O and 60Cu-ATSM PET imaging was repeated.
Protocol II: Induction of Acute Myocardial Ischemia (n = 9).
Acute coronary occlusion was created in the mid left anterior descending (LAD) coronary artery by placement of a 3- to 5-mm copper coil under fluoroscopic guidance in a closed-chest preparation as previously described (25). Fluoroscopic imaging was performed on a cardiovascular mobile digital C-arm (OEC series 9800; General Electric Medical Systems, Milwaukee, WI). Complete coronary occlusion was documented with coronary catheterization and was confirmed by typical electrocardiographic signs of ischemia, including ST elevation and ventricular arrhythmia. 15O-H2O and 61Cu-ATSM (or 60Cu-ATSM) were administered within 3 h of coil placement, and PET scanning proceeded as described in Imaging Protocols and Data Collection.
After the 3-h scan, 4 dogs were maintained over 24 h to determine the selectivity of *Cu-ATSM between ischemic and necrotic myocardium. 15O-H2O and 64Cu-ATSM were administered for a second time 22–24 h after coil placement, and PET scanning proceeded as described in Imaging Protocols and Data Collection. After euthanasia, infarct size (percentage of the total left ventricle) was determined semiquantitatively using 1% 2,3,5-triphenyltetrazolium chloride (TTC) staining based on previous methods (26,27). The same heart slices were examined on an electronic autoradiography system (InstantImager; Packard Instrument Co., Meriden, CT). Heart slices were mounted and placed in the InstantImager to show the distribution of 64Cu-ATSM.
Protocol III: Induction of Demand Ischemia (n = 4).
Coronary artery stenosis was induced by the insertion of a Teflon (Dupont, Wilmington, DE) stenosis into the mid LAD coronary artery under fluoroscopic guidance as described previously (28). Fluoroscopic imaging confirmed placement of the Teflon stenosis, with the formation of between 65% and 80% stenosis as determined by the standard software package supplied with the cardiovascular mobile digital C-arm. In protocol III, because of the nature of the experiment and the titration of dobutamine (DOB), the use of 15O-H2O would have extended the length of intervention (to allow for 15O decay) and would have caused a delay between MBF determination and 60Cu-ATSM PET. Therefore, in protocol III, myocardial perfusion was measured with radioactive microspheres by following previously reported methods (29). The first 60Cu-ATSM scan (and concurrent microsphere administration) was performed within 1 h of stenosis placement under resting conditions as described in Imaging Protocols and Data Collection. On completion of the first scan, the animals were titrated with DOB from 0 to 40 µg/kg/min for 30 min. Because of the difficulty in measuring regional pO2, echocardiography was used as a surrogate marker for the presence of ischemia. Wall motion decreases and diminished systolic function in the LAD region (LADR), consistent with ischemia, were seen on the echocardiograms. In this protocol, once the stress echocardiogram confirmed the presence of ischemia, a second dose of 60Cu-ATSM (or of 61Cu- or 64Cu-ATSM) (and microspheres) was administered and a second *Cu-ATSM PET study was performed.
Imaging Protocols and Data Collection
PET studies were conducted on the ECAT 962 HR+ scanner. After a transmission scan, myocardial perfusion for protocols I and II was determined by administering 666–925 MBq of 15O-H2O as an intravenous bolus and acquiring dynamic PET data for 5 min (5-s frames). In protocol III, myocardial perfusion was measured with 85Sr (rest) and 46Sc (with DOB) microspheres (15 µm in 0.01% Tween; NEN Life Science Products, Inc. Boston, MA). In all protocols, *Cu-ATSM (labeled with 60Cu [44.4–388.5 MBq], 61Cu [222.0–240.5 MBq], or 64Cu [214.6–569.8 MBq]) was administered as a bolus injection, followed by the immediate collection of dynamic data until 45 min.
Image Analysis
Myocardial 15O-H2O and *Cu-ATSM dynamic images were reoriented to generate standard short-axis and horizontal and vertical long-axis views. To generate myocardial time-activity curves from the global hypoxia studies (protocol I), for which no differences in regional flow or hypoxia were expected, regions of interest encompassing the anterolateral wall (3–5 cm3) were placed on 2 or 3 standard short-axis slices of a composite *Cu-ATSM image. Myocardial time-activity curves for the ischemic studies (protocols II and III), for which regional flow and hypoxia heterogeneity were expected, were generated from normally perfused and ischemic myocardium by placing 3 or 4 regions of interest on the normal myocardium and 2 or 3 LADRs. 15O-H2O myocardial and blood time-activity curves were used in conjunction with a validated kinetic model (30) to estimate MBF (mL·min-1·g-1). In protocols II and III, regions were defined as hypoperfused or normal on the basis of both the 15O-H2O PET images and the *Cu-ATSM PET images. Anteroapical regions with activity less than 50% of peak radioactive counts were defined as hypoperfused. Regions representing myocardium remote from the LAD and with activity at 80%–100% of peak radioactive counts were defined as normally perfused. The same regions were then placed on the 15O-H2O and *Cu-ATSM dynamic images to measure MBF (protocol II) and myocardial ischemia (protocols II and III), respectively.
Monoexponential Analysis.
For each myocardial region generated from the *Cu-ATSM PET images, the washout phase (from the peak radioactive counts to the end of data collection) of the myocardial *Cu-ATSM curves was fitted to a simple monoexponential, and the estimated rate of clearance (kmono [min-1]) was assumed to be inversely proportional to *Cu-ATSM myocardial retention and, therefore, an index of myocardial hypoxia. The assumption that the washout phase is proportional to hypoxia is supported by results from experimental rodent tumor and ischemic myocardium models (17,18). Myocardial retention was then expressed as the inverse of kmono (retention = 1/kmono [min]). The kmono values were obtained from the individual regions of interest and were averaged for the normally perfused regions (NLRs) and LADRs. Paired t tests were performed to determine statistical significance among grouped data. Correlations were calculated by linear regression.
Kinetic Modeling.
A 2-compartment model (Fig. 1) was used to describe the myocardial kinetics of *Cu-ATSM. This was a feasibility kinetic model, and full validation is required before routine use. Compartment 1 represents vascular *Cu-ATSM that exchanges with the extravascular and interstitial spaces, and compartment 2 represents *Cu-ATSM that enters the myocyte. Vascular *Cu-ATSM (Ca[t]) enters compartment 1 at a rate of K1 (mL·min-1·g-1). Once the tracer is in this compartment, either it can diffuse back into the vasculature at a rate of k2 (min-1) or it can enter the myocyte (compartment 2) at a rate of k3 (min-1). Under normoxic conditions, *Cu-ATSM washes out of the cell at a rate of k4 (min-1), whereas under hypoxic conditions, copper-ATSM is selectively retained by the myocyte (i.e., decreased k4). After correction of blood time-activity curves for *Cu-ATSM metabolites (to obtain the true input function), myocardial curves were used in conjunction with the input function to estimate model transfer rates K1–k4 and the blood-to-tissue spillover fraction. The rate k4 should, at that point, represent washout of tracer from the myocyte (and not from the entire myocardium, as kmono does). For dogs in which perfusion was measured with 15O-H2O, the tissue recovery coefficient obtained from 15O-H2O analysis was used to correct *Cu-ATSM counts (partial volume). For dogs in which radioactive microspheres were used instead of 15O-H2O PET, an average tissue recovery fraction obtained from the other studies was used. Myocyte tracer retention was then expressed as the inverse k4 (retention k4 = 1/k4 [min]). The k4 values were obtained from the individual regions of interest and were averaged for the NLRs and LADRs. Paired t tests were performed to determine statistical significance among grouped data. Correlations were calculated by linear regression.
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-counter. Analysis by radio-TLC confirmed that extractable radioactivity was in the form of 64Cu-ATSM. At each time point, the value of the fraction of octanol-extractable 64Cu-ATSM in blood was obtained. The resulting curve represented the fraction of *Cu-ATSM present in the blood over time. A multiexponential function was fitted to this fraction so that it could be defined at any given time and used to correct the total blood activity of radiocopper obtained from the PET images. This function (with averaged parameter values) was used for all animals studied. |
RESULTS |
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TOPABSTRACTINTRODUCTIONMATERIALS AND METHODSRESULTSDISCUSSIONCONCLUSIONREFERENCES |
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Protocol III: *Cu-ATSM Retention After Induction of Demand Ischemia
This protocol closely examined retention of *Cu-ATSM after induced ischemia without severe flow limitation, which is the most common diagnostic situation in which myocardial hypoxia is documented. In protocol III, MBF was higher in the NLR than in the LADR, indicating reduced perfusion to the LADR (Table 3). Under resting conditions, the transmural MBF between the NLR and LADR and the endocardium-to-epicardium ratios are not significantly different, showing that ischemia was not likely to have been induced with the stenosis. Because we could not confirm this, we assumed that the tissue was under normal levels of oxygenation. During DOB infusion, the transmural MBF increased equivalently in both the NLR and the LADR, while the endocardium-to-epicardium ratio was significantly lower, consistent with the greater flow limitations of the endocardium.
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DISCUSSION |
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TOPABSTRACTINTRODUCTIONMATERIALS AND METHODSRESULTSDISCUSSIONCONCLUSIONREFERENCES |
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Tissue hypoxia plays a central role in the pathogenesis of myocardial ischemia. The other manifestations of myocardial ischemia, including perturbations in metabolism, mechanical dysfunction, and electric instability, are secondary to hypoxia. Currently, methods of diagnosing myocardial ischemia include those such as coronary angiography, which detect abnormalities in MBF; those such as stress electrocardiography and echocardiography, which detect the secondary manifestations of ischemia; and those such as the multiple imaging methods that measure myocardial perfusion. Unfortunately, a direct correlation does not always exist between the readouts from these imaging techniques and the presence of myocardial ischemia. For example, the presence of coronary artery stenosis does not always imply abnormalities in myocardial perfusion. Moreover, the presence of reversible perfusion abnormalities on rest/stress myocardial perfusion imaging may signify impairment in myocardial vasodilatory reserve but not necessarily inadequate oxygen supply to meet demand and, thus, myocardial ischemia. Conversely, in the presence of resting electrocardiographic abnormalities or systolic dysfunction, it frequently is difficult to definitively couple the presence of these abnormalities with the induction of myocardial ischemia. Consequently, accurate detection of myocardial hypoxia would have numerous applications both in cardiovascular research and in the management of patients with cardiovascular disease. The detection of hypoxia in these patients could potentially further our understanding of these cardiac disease processes as well as provide an important marker to monitor the efficacy of novel strategies to treat them. Given the importance of the presence of myocardial ischemia and, thus, hypoxia as a marker of increased cardiac risk in patients with coronary artery disease, hypoxic imaging may prove useful in assigning prognosis in patients with this disease. The results of the current study suggest that PET with *Cu-ATSM may potentially be useful in the detection of hypoxia both after acute coronary occlusion and during the demand-induced ischemia that occurs with stress testing. Certain characteristics are desirable in an imaging agent for myocardial hypoxia. First, retention of the agent should be directly proportional to the decline in tissue oxygenation. Second, the myocardial kinetics of the agent should permit rapid imaging and relatively simply image interpretation. Finally, the imaging approach should be available for clinical use. To a large extent, PET imaging with *Cu-ATSM fulfills these requirements. In isolated perfused hearts, retention of *Cu-ATSM is directly proportional to tissue oxygenation (16,17). Imaging can be completed within 20–45 min after tracer administration, and measurement of the myocardial retention rate of copper-ATSM is straightforward. The kinetics of *Cu-ATSM are such that administration of DOB and *Cu-ATSM could occur out of the PET scanner and then images such as that shown in Figure 5B (right) can be obtained after the patient is subsequently positioned in the scanner. The continued wide dissemination of PET, primarily because of its oncologic applications, and the ability to radiolabel ATSM with positron-emitting radionuclides of copper increase the potential availability of this imaging method.
The positron-emitting isotopes of copper—60Cu, 61Cu, and 64Cu—can be produced at high specific activity on all biomedical cyclotrons using identical target systems and chemistry (20,21). The technology for the production of 64Cu, 61Cu, and 60Cu (Newton Scientific, Inc., Cambridge, MA) has been obtained by institutions in the United States, Europe, Japan, and Canada. As shown in the current study, the resolution qualities of these copper radioisotopes (taking the 2 extremes, 64Cu and 60Cu) are similar in good-quality PET cameras. The distance traveled by the positron before annihilation, or the positron range, will cause additional blurring that prevents the discrimination of small structures. An understanding of the positron range spectra for each isotope comes from a detailed analysis of their respective decay schemes. In ß+ decay, the positron will be emitted with a spectra that can be defined by a Fermi function, with the endpoint determined by the Q-value of the decay. 64Cu decays by positron emission, with a branching ratio of 17.4% and a maximum ß+ energy of 653 keV. This endpoint energy is thus similar to that of 18F decay (634 keV) (31), and the maximum range of the positron will therefore be similar to that of 18F, with an average value of 0.4 mm in water. Although the Q-value of the ß+ decay of 60Cu is high (5.105 MeV), the decay will proceed to excited states in 60Ni. The most probable levels are 1.3325 MeV (5%), 2.159 MeV (15%), 3.124 MeV (49%), and 3.194 MeV (11.6%) (31). The maximum energy of the ß+ will therefore be strongly reduced. The maximum positron range of such high-energy positrons is close to 16 mm in water. However, these are relatively rare events, and on average, the positron range will be approximately only 3 mm in water. The imaging performance of 60Cu was therefore only slightly impaired relative to 64Cu, and in particular, the long-range component of the 60Cu ß+ spectra reduced the contrast only around small structures, as is apparent on the 60Cu phantom of Derenzo et al. (23), in which the smallest rods (2.5 mm) could not be identified. The complex decay scheme of 60Cu will also result in the emission of numerous -rays with energy mostly greater than 0.826 MeV. These -rays detected in coincidence with annihilation photons will contribute to reducing camera performance. These events will increase camera dead time and create a uniform distribution of counts in the images. Given the relatively weak activity in the field of view, the number of prompt -rays associated with the decay of 60Cu did not reduce image quality in comparison with image quality from the 64Cu phantom.
The easy and economic production of a sterile and radiochemically pure preparation of 60Cu-ATSM at Washington University School of Medicine takes approximately 50 min. Between February 1998 and April 2002, 92 patients with a variety of tumors, including those of the head and neck, lung, and cervix, were imaged with 60Cu-ATSM in ongoing clinical trials (21,32,33). 61Cu, with its 3.32-h half-life, can feasibly be produced and supplied by national distribution centers, just as are 18F-radiopharmaceuticals (21). The longer-lived 64Cu is currently produced and supplied through a National Institutes of Health/National Cancer Institute-funded research resource grant to more than 15 institutions throughout the United States (34). Preparation of 62Cu through a 62Zn/62Cu generator has been reported by several groups (13,22,35,36), and one such system has been commercialized (22). The wide dissemination of the copper radionuclides, and the availability of shorter-lived isotopes that allow for repeated imaging, makes the use of copper radiopharmaceuticals particularly attractive.
One aim of this study was to investigate whether mathematic modeling of the kinetics of *Cu-ATSM, compared with simple clearance analysis of myocardial *Cu-ATSM curves, results in more accurate and reliable detection of hypoxia. Myocardial clearance analysis is simple and requires only the washout phase of the myocardial curves. In contrast, defining the entire myocardial kinetic of *Cu-ATSM using kinetic modeling requires *Cu-ATSM myocardial as well as blood activity over the entire study period. To ensure that blood activity is not contaminated by labeled metabolites, it must be corrected for these metabolites, and such correction requires blood sampling and analysis. It is hoped that a single multiexponential function will be clinically applicable after validation in humans, including validation during different interventions and a full analysis of metabolites.
Global myocardial hypoxia without ischemia (protocol I) was detected as well by monoexponential clearance analysis as by kinetic modeling; both methods demonstrated a 4-fold increase in retention. Furthermore, regional variations of 1/kmono and 1/k4 values were also comparable (23% ± 26% vs. 30% ± 11%, P = not statistically significant). Both methods are also similar in their ability to assess myocardial hypoxia in the presence of ischemia (protocol II, 3 h, and protocol III). Regional variations of 1/kmono retention tended to be lower than those of 1/k4 retention (13% ± 12% vs. 22% ± 13%, P = 0.09). However, in the 4 animals studied 24 h after LAD occlusion (protocol III), and in which hypoxia as well as necrosis was present, retention values derived from monoexponential clearance were different from those derived from kinetic modeling (Fig. 6C vs. Fig. 6D). Monoexponential clearance analysis showed a consistent and significant increase in retention in all 4 animals, suggesting the presence of hypoxia but not of necrosis. These results were inconsistent with the postmortem TTC staining results. In contrast, kinetic modeling analysis demonstrated similar or a lowering of retention in the LADR, compared with the NLRs, in the 3 animals that had sustained severe ischemia and an MBF of less than 50% of normal. However, an increase in retention was shown in the ischemic regions of the only animal in which perfusion to the LADRs was within 80% of normal. Thus, differences in retention between hypoxic and necrotic tissue were detected with kinetic modeling but not with monoexponential analysis. This discrepancy is understandable when one considers that kinetic modeling takes into account spillover effects and partial-volume corrections and uses the true input function. Further, kinetic modeling decouples perfusion kinetics from retention and washout of the tracer; the insensitive nature of the monoexponential analysis is inadequate for this particular analysis. These results strongly suggest that kinetic modeling will better detect hypoxia in ischemic myocardium. Although this model is superior to monoexponential analysis, the 2-compartment model in the current study was used for feasibility purposes and requires further validation before full implementation.
123I and 99mTc-misonidazole analogs have been investigated as hypoxia-avid agents for use with SPECT (2). The 99mTc-compounds, 99mTc-HL91, BMS-181321, and BMS-194796, have demonstrated increased uptake in hypoxic and low-flow ischemic myocardium (5–7,37). BMS-181321 displayed high liver uptake, which excluded this tracer from routine clinical use, but the analog BMS-194796 may provide a realistic alternative, with reduced hepatic uptake and increased tracer uptake in ischemic tissue (38). 99mTc-HL91 is one of the most promising 99mTc-agents for both the imaging of tumor hypoxia (39) and the imaging of ischemic myocardium (5); however, acutely injured nonviable myocardium has shown 99mTc-HL91 uptake and retention similar to those of normal myocardium (40). In PET imaging with 18F-FMISO after 3 h of coronary occlusion in dogs, Shelton et al. showed that the residual fraction of activity averaged 23% ± 18% in ischemic myocardium, compared with 2% ± 1% in normal tissue (10). A similar study found that the binding ratio of 18F-FMISO at 4 h was 1.8–2.4 times higher in ischemic regions than in normal regions (11). In the present study, *Cu-ATSM was taken up rapidly and selectively in hypoxic and ischemic tissue within 20 min after administration, showing that differences between hypoxic and normal tissue can be imaged. Our data, by showing that *Cu-ATSM was not retained in necrotic tissue (protocol II, 24 h), confirmed that *Cu-ATSM is an efficient tracer for the delineation of myocardial hypoxia.
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CONCLUSION |
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ACKNOWLEDGMENTS |
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FOOTNOTES |
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For correspondence or reprints contact: Michael J. Welch, PhD, Mallinckrodt Institute of Radiology, Washington University School of Medicine, Campus Box 8225, 510 S. Kingshighway Blvd., St. Louis, MO 63110.
E-mail: welchm{at}mir.wustl.edu
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| JOURNAL OF NUCLEAR MEDICINE TECHNOLOGY | THE JOURNAL OF NUCLEAR MEDICINE |
) and apical region (
) show similar kinetics. Although data collection continued until 45 min, figure shows only first 12 min, for clarity. (B) In myocardial time-activity curves obtained after injection of 64Cu-ATSM in dog 13 after DOB infusion (protocol III), normal septal/lateral region (