New Radionuclides D. Douglas
Miller,
John
B. Gill, Charles
Alan
for Cardiac Imaging
J. Fischman,
A. Boucher.
and
Massachusetts General Hospital, Boston. Supported in part by USPHS Cardiovascular Nuclear Medicine Training Grant HLO7416, and USPHS Fatty Acid Analogs for Myocardial Imaging HL29636. Dr Miller is a Fellow of the Canadian Heart Foundation. Address reprint requests to H. William Strauss, MD, Division of Nuclear Medicine, Massachusetts General Hospital. Boston, Massachusetts 02114. @ 1986 by Grune & Stratton, Inc. 0033-0620/86/2806-0002$05.00/0
The nuclide generator is a convenient method isotopes available at long Vol XXVIII,
No 6 (May/June),
R. Elmaleh,
From the Division of Nuclear Medicine, Department of Radiology and the Cardiac Unit, Department of Medicine,
of making short-lived
Diseases,
David
Strauss
Radionuclide generators provide a means of separating two genetically related radionuclides from one another.” The generator usually consists of a column of an inorganic powder, usually made of aluminum oxide, zirconium oxide, or charcoal, surrounded by a lead shield (Fig 1). The longer lived parent radionuclide is poured (absorbed) on the column, where it continually decays to produce its radioactive daughter. The separation of the daughter from the column is achieved by passing a solution (eluate) through the column. Differences in the adsorption characteristics of the two nuclides for the column at the pH, osmolality, etc, of the eluate causes the daughter to enter the solution while the parent remains on the column. This chromatographic procedure rarely provides a perfect separation of the daughter from the parent. Selection of the column material and elution solutions for the generator are predicated on their stability in high radiation fields. Radiation intensity in the generator typically reaches thousands of Gray, which results in the formation of superoxides in the column. This problem is compounded by aqueous eluates, since most generators are left wet (eluate in contact with the column between elutions). In addition to the potential formation of oxides, the eluate may contain undesirable radionuclide or chemical contaminants. These substances may arise when the parent is prepared in the reactor or cyclotron, or during the chemical separation of the nuclide
GENERATORS
in Cardiovascular
J. Callahan,
distances from the source of production. It serves as a continuous source of a short-lived isotope.-P. Richards, 1966l
WO RADIONUCLIDES, thallium-201 and technetium-99m, have assumed preeminence in cardiovascular nuclear medicine because their photon energies, kinetics, and dosimetry are well-suited to make three major physiologic measurements: perfusion, function, and viability. The photon energies of these nuclides are well matched to the characteristics of the Anger camera, which has optimum efficiency and resolution for energies between 100 and 200 keV. The spatial resolution of the “system” for the average cardiovascular nuclear medicine study (radiopharmaceutical, collimator, camera, and computer) at the depth of the heart is approximately 1 cm full width half maximum (FWHM). Against this background, new radiopharmaceuticals suggested for the evaluation of the heart (Table 1) must offer an improvement in dosimetry and resolution, or provide data on a previously unmeasurable parameter. This review will concentrate on the new radiopharmaceuticals that have met two criteria: (1) experience with the radiopharmaceutical in human subjects, and (2) some likelihood of commercial production of the agent for widespread clinical use. Although equilibrium studies provide high quality data for evaluation of regional and global cardiac function, a high photon flux first pass approach, which could evaluate ventricular function during breathholding (to eliminate respiratory motion), would improve resolution. The ideal first pass radionuclide should have a short physical halflife, have no particulate emissions, produce photons of 100 to 200 keV, and decay to a stable daughter. Such an agent would permit multiple measurements to be performed in each view and would allow repetitive determinations of ventricular function during the action of drugs, exercise, or physiologic maneuvers (Valsalva, etc). The following agents have some of these properties and may supplant Tc-99m as the radionuclide for first pass studies.
T
Progress
Ronald H. William
1986:
pp 419-434
419
420
MILLER
Table
1.
Uses
of Radionuelides Myocardial
Ventricular Radiiuclide
First-Pass
Ultrashort-Lived Krypton-8 Iridium-19 Gold-
Function
in Cardiac
Imaging
Perfusion WocVte
lntracoronary
Equilibrium
IV
Left Hewt
Viability
+4.6
1m 1m
+ 12.
+
26
+
25-Y +
126-131
+ Agents
N- 13 ammonia 0- 15 water
4s-a + ,143 +
C-l
fU
1 butanol
C-l 1 deoxyglucose F- 18 deoxyglucose
+ and
modified fatty acids Fatty Acids
Straight-chain
+
69-M)
(alkyl.
aryl) Branched (CH, substit) Technetium-99m Labeled (LDL)
+Ss,s7-7’ + M*s’32
+80 +sm
+ 72-78 + 6’~s’~82
Agents + (7)
Antimyosin Fab Hex-t-butyl-isonitrile
+ 106 +
+
112.113
Macroaggreg
atheroma
detection’w‘
8%902
+
Albumin Indium-1 11 Labeled Antimyosin
61-63.44
+“.s4.ss
1 palmitate
Lipoprotein
Miscellaneous
+=
13-W + + I*-2,
195m
Indium-113m Positron Emitting
lodinated
Metabolism
Agents
Rubidium-82 Xenon- 133
C-l
ET AL
Agents
Fab
Platelets Leukocytes Colloid
from the target material. To determine if a generator eluate is safe for use, it should be tested for the presence of these chemical contaminants. Since these tests may take hours to days, procedures have been devised to characterize specific generator/elution combinations. In these procedures, the quantity of parent and daughter radionuclide and chemical contaminants are carefully measured in several test generators as a function of elution volume. With repeated elutions, the location of the parent on the column gradually migrates from the top of the column toward the bottom. As a result, every generator will eventually reach a point where the parent can be eluted completely from the column. To avoid inadvertant administration of the parent material, every elution should be tested for the quantity of daughter and parent radionuclide in the eluate. This process can be readily accomplished with daughter radionuclides that have half-lives greater than
+ *s.s*.ss +114-118.11s-122 +
+ thromb”s”“l’s.l~s
,,S,lZ,
+ lymphoscintigraphy’w
several minutes by measuring the relative abundance of photons resulting from the decay of the daughter and the parent (as is commonly done with technetium-99m eluates). The ultrashortlived radionuclides, however, present special problems in this area, since the time required to perform the assay may require several half-lives of the daughter, making the eluate unusable for administration. Typically, quality control of ultrashort-lived generator systems has been accomplished by characterization of the eluate before administration, and knowledge of the generator system (eg plot of parent elution v eluate volume). To test for breakthrough, the eluate is immediately placed in a dose calibrator (ionization chamber calibrated to reflect the change in charge/unit time as a photon flux) to determine the total photon flux. The sample is measured a second time 20 to 30 half-lives later, when any remaining activity is the result of breakthrough. Most generators can be eluted to some total
NEW
CARDIAC
A /
--
421
RADIONUCLIDES
‘-\\
TUREE
YAV
POROUS LEID
sTOPCOcr
POL*ETtlYLLYE
DISK
StIlELD
BOUNDED
OSYIUY
RESIN
.D I x2
ANION EXC,‘ANEE RESIN POROUS l OLlElWYLENE
‘G I x4 DISK ANION EXCUANQE RESIN LG I x4 Op YEYIMNE FILTER POROUS
-
INFUSlON
POLYETWILENE
DISK
SET
Fig 1. (A) A photograph of the external appearance and internal components of the OS-191~lr-191m generator currently used in our laboratory. This generator system, orginally developed by Yeno and Anger in 1968 based on a method described by Campbell and Nelson, separates the short-lived daughter lr-191m (T1/2 = 4.9 seconds) from its parent radionuclide OS-191 fT112 = 15 days). (Courtesy of Dr F. F. Knapp, Oak Ridge National Laboratories.) IB) A diagram illustrating the basic generator components of the OS-~ 91 -b-l 91 m generator. The parent radionuclide. OS-1 91, is adsorbed as OsCl,in the strongly basic AGl anion exchange resin column. Saline eluate is passed through the column. with elution in less than 2 seconds of Ir-191 m for infusion. Osmium breakthrough and iridium extraction decrease with increasing cross-linking of OsCl,to the resin column. (Reprinted with permission of the American Heart Association.“‘)
volume before parent breakthrough increases to undesirable levels. As a result, it is usually possible to predict the breakthough in a given elution. Based on this information, ultrashort-lived generators have been employed for human studies based on characterization of the dose preceding the dose actually administered. The combination of low radiation burden to the subject and high photon flux make the ultra short-lived generators very attractive for use in cardiovascular nuclear medicine. The following discussion describes unique features of these generators. ULTRASHORT-LIVED
RADIONUCLIDES
Krypton-81 m In 1968 Yano and Anger3 proposed the use of the Rubidium-8 1/Krypton-8 1m generator sys-
tem to image the blood pool. The 4.7 hour half-life cyclotron produced Rb-81 (alpha particle bombardment of a Br-79 target [alpha, 2n]), is absorbed to a column, and the 13 second daughter inert gas Kr-81m produced. If the column is filled with dextrose, the resulting solution of dextrose/Kr-81m can be injected intravenously (IV) to determine right ventricular function4,’ and pulmonary perfusion, or intraarterially to determine myocardial perfusioP or regional cerebral perfusion.’ If the generator is opened to the air, the resulting gas can be inhaled to define regional ventilation. The 190 keV energy of the Kr-81m is well-suited for imaging with low or medium energy collimators available on most scintillation cameras. Kr-8 1m is particularly useful for the repetitive evaluation of right ventricular function due to its short effective half-life (ie, T1/2 effective = [(T1/2 biological x
422
T1/2 physical)/(T1/2 biological + T1/2 physi-Cal)]). The short effective half-life comes from the combination of short physical half-life and short biological half-life due to the evolution of the radionuclide from the blood into the alveolus during its passage through the lung. As a result, no significant activity enters the left heart. The short effective half-life results in a low radiation burden/MBq, which permits a large dose to be administered by injection. The resulting photon flux permits high count density data to be recorded during the initial passage of radionuelide through the right heart. Since right ventricular function varies with the respiratory cycle, it may be preferable to measure right ventricular ejection fraction (RVEF) during several respiratory cycles, rather than during a single inspiration or expiration, as is currently done during first pass studies. This can be accomplished by recording a gated collection during a continuous IV infusion over a 30 to 60 second interval instead of using the bolus injection technique. The calculated RVEF with this approach is typically higher than that calculated from equilibrium blood pool studies. Kr-8 1m right heart studies require high dose of Rb-81 on the infusion generator.4*5 The costs of producing the parent radionuclide, coupled with its short physical half-life make this an expensive nuclide. To market the generator, primarily intended for use with inhalation imaging, at a reasonable price, the manufacturer elected to make the generator with 5 mCi of rubidium on the column. As a result, the photon flux available from the typical commercial generators is low compared to that which is theoretically achievable. The detected photon flux of about 5,000 counts available from infusions of Kr-8 1m from this generator are less than 25% of that from Tc-99m during an equilibrium study. These low photon fluxes generate noisy images, which preclude the determination of regional wall motion of the right ventricle. If larger generators become available, Kr-8 1m will be useful for the determination of right heart function. The ultra short physical half-life of Kr-8 lm led to the development of a new approach to measure regional myocardial perfusion.3v@ Since the radionuclide decays in a shorter interval than the transit through the myocardial bed, images recorded during continuous infusion of KR-8 1m are dominated by its input function-myocardial
MILLER
ET AL
perfusion. The biologic half-life of the agent in the myocardium is approximately 30 seconds, while its physical half-life is 13 seconds, giving an effective half-life of 9 seconds. As a result, the usual inert gas clearance approach to measurement of regional myocardial perfusion with this nuclide is dominated by the physical decay of the nuclide, rather than the biologic clearance due to perfusion.” However, a static image recorded during continuous infusion of the agent at the root of the aorta depicts the regional distribution of myocardial perfusion,” as suggested by Kaplan et al.” The Kr-8 lm infusion approach can be used to evaluate the pattern of onset of ischemia with interventions such as pacing. As with the right ventricular (RV) function studies, however, these measurements require a minimum of a 2 mCi equilibrium infusion concentration in the aorta. Since the distribution of perfusion will be determined by the equilibrium activity concentration in the myocardium, the infusion catheter must be positioned to infuse Kr-81m into each coronary distribution in proportion to perfusion. This may be difficult to accomplish due to streaming at the aortic root. To avoid this problem, one coronary vessel may be perfused at a time. This requires a lower dose of activity and can be accomplished at lower infusion rates. An additional advantage of selective infusion of Kr81m is the delineation of the perfusion through collateral vessels. Iridium-I 91m Ir-191m is a generator-produced 4.7 second half-life radionuclide with gamma photons of 129 keV and x-rays of 65 keV.” The parent, reactor-produced OS-191, has a half-life of 15 days. The short half-life of the iridium product makes it difficult to characterize the chemical form of the Group VIII element. Although this generator was originally described in 1968 by Yano and Anger’ for the determination of pulmonary perfusion, it was not until the recent work of Trevesi3-I5 that a generator practical for human use was developed. The radionuclide is associated with a radiation burden of 3-5 mR/ mCi while providing a high photon flux (the majority of the radiation burden stems from the breakthrough of the parent OS-191 into the Ir19 1m eluate. Improvements in the column material recently suggested by Knapp et al indicate
NEW
CARDIAC
423
RADIONUCLIDES
that the radiation burden may be reduced by ten to 100 fold). The combination of high photon flux and exceptionally low radiation burden are well-suited to the pediatric population, to evaluate shunts and ventricular function. Although the agent can be used in adults, the intrathoracic transit time of 8 to 10 seconds is relatively long compared to the 4.7 second halflife. As a result, right heart data is recorded with a photon flux two to four fold greater than that of the left heart. To visualize the left heart well, the count rate from the right heart must be very high. This high photon flux may actually present a problem for Anger type scintillation cameras, since count rates in excess of 100,000 counts/s result in increased dead time of the camera, and a nonlinear relationship between activity in the field of view and counts recorded. The multicrystal gamma camera, or the multi-wire propordescribed by Lacy et al are tional chambe?’ able to take advantage of the very high count rates offered by Ir- 19 1m, since these instruments can process maximum count rates of 500 to 800,000 counts/s. Gold-l 95m Gold-195m is a 30.5 second half-life daughter of the 40.5 hour, cyclotron-produced Hg-195.‘*-” Au-195m has a 262 keV gamma photon which is 68% abundant. The chemical form of the gold eluted from the column is not well-characterized, but it is likely that this Group IB nuclide is ionic. The half-life of Au-195m is long with reference to the central circulation time and permits high quality studies of the left and right heart to be recorded. The combination of short half-life and high photon energy led Mena et al*l to suggest that Au-195m could be coinjected with Tl-201 at the time of bicycle exercise studies to permit an evaluation of global and regional function in conjunction with assessment of myocardial perfusion. The procedure described by Mena consisted of (1) recording a Au-195m first pass ventricular function study; (2) repeaking the camera for Tl-201; and (3) five minutes later recording myocardial perfusion data. As with other short half-life generator-produced radionuclides, the radiation burden to the patient is primarily the result of breakthrough of the parent Hg-195. Since mercury compounds localize in the kidneys, the radiation burden from breakthrough increases the renal dose. Although
improvements in the generator column and eluate have resulted in a marked decrease in the breakthrough problem, a limit of 300 mCi total dose is usually employed to minimize the radiation burden to the kidneys. An additional problem, unique to the Au195m generator system, is the decay of Au- 195m to a long-lived daughter, Au-195 (physical halflife, 190 days). This decay process is continuously underway on the generator, resulting in a high concentration of Au- 195 in the initial eluate from the generator. Biodistribution studies in animals suggest Au-195 localizes in the kidneys, adding to the potential radiation burden from breakthrough of the parent Hg- 195. To minimize the buildup of Au-195, the column should be preeluted within ten minutes of use. Other Single Photon Ultrashort-Lived Generator Systems Two other generator systems, the Cd-109 (half-life, 1.26 years)/Ag-109m (half-life, 39.6 seconds) and the Cs-137 (half-life, 30.3 years)/ Ba-137m (half-life, 2.55 minutes) have been described, but are unlikely to find widespread use in nuclear cardiology.** In the case of the Cd/Ag system, the primary 88 keV gamma of Ag-109m is only 5% abundant, while the energy of Ba137m is too high for use with conventional Anger cameras. An additional problem in both cases is the potential for a large radiation burden to be delivered to the patient by unexpected breakthrough of the parent. Rubidium-82 Rubidium-82 is a 75 second half-life positron emitting daughter of cyclotron produced Sr-82 (Rb-85 (p,4n) - T1/2 physical = 25 days). The production of the parent Sr-82 requires a high energy cyclotron and is accompanied by the production of small quantities of Sr-85 as a radiocontaminant. Since strontium radionuclides localize in bone and have a long biologic half-life, the generator system has been refined to minimize the breakthrough of the parent in the eluate. The generator is tested for breakthrough by the prior elution method described earlier (Fig 2). A maximum of 0.001 &!i Sr-82/mCi Rb-82 results in a radiation burden of 0.019 rads/mCi to the kidney and 0.001 rads/mCi to the total body.23 Rubidium-82, a member of Group IA, is
424
Fig 2. The general (A) and detailed (B) external presently used in our laboratory. Saline is delivered mL/minl. The top of the “pig” is removed to reveal through e system of two filters before reaching the allowed to decay for one hour. Generally, less than reelutad, at full potency. once every tan minutes.
MILLER
ET AL
appearance of the Strontium-%?-Rubidium-82 generator infusion system by a syringe pump at a constant infusion rata of 50 mL/min hnaximum 100 the entry and exit points of the saline aluata, which subsequently passes patient. To detect radionuclide impurities in the aluata, W-82 should be 0.001 mCi of Sr-82 is detected per mCi Rb-B2. The generator may be
NEW
CARDIAC
RADIONUCLIDES
eluted from the generator as a monovalent cation. The agent behaves as a Saperstein tracer (eg, the regional distribution of the radionuclide is proportional to perfusion in organs with high extraction.24) The radionuclide is concentrated in tissues by the Na-K ATPase pump and has a myocardial extraction between 65% and 75%. As with other generator-produced ultrashort-lived nuclides, quality control is by preelution calibration and direct infusion of the dose to the patient. Myocardial imaging with this radionuclide requires fast acquisition of data. Images recorded during the first one to two minutes after IV administration depict the blood pool distribution of the radionuclide (if images are recorded with gating, ejection fraction and regional wall motion can be determined), while images recorded after two minutes depict regional perfusion.25 Reasonable quality images can be recorded for four to six half-lives after infusion, one to two half-lives consumed with blood clearance, the remainder for myocardial perfusion. Although images of this positron emitting nuclide can be recorded with a single photon camera26*27 (see below), the highest quality images are recorded with a multi-slice positron tomograph.28-34 Recent studies by Gould and Mullaniz5”’ demonstrated the ability to measure absolute as well as relative myocardial perfusion from Rb-82 PET images with a time of flight positron camera. A limitation of this approach to calculating absolute flow is the problem of diffusion limitation at myocardial blood flows greater than two times baseline (flow rates commonly observed with dipyridamole infusions). At these perfusion levels, the deposition of Rb-82 in tissue will underestimate regional perfusion.3s However, since coronary disease is associated with a marked decrease in perfusion, the nonlinearity of the measurement in the higher ranges is not of great importance clinically. Selwyn and his colleagues have made several unique observations with the Rb-82 PET imaging technique: (1) In patients with coronary artery disease, marked changes in regional myocardial perfusion were observed during the performance of mental arithmetic. These changes were of similar severity to those induced by exercise.29 (2) Following restoration of perfusion to zones of ischemia,
prolonged abnormalities in cation uptake were observed, presumably due to disturbances in cation transport and trapping.28 If a PET camera is unavailable, images can be recorded with an Anger scintillation camera with a specially constructed high energy tungsten collimator.27 The sensitivity of this single photon approach, however, is about 0.1% that of the positron technique. Even with this low sensitivity, the quality of the images is similar to that of Tl-201. CYCLOTRON-PRODUCED POSITRON COMPOUNDS
EMITTING
Three types of cyclotron-produced positronlabeled radiopharmaceuticals have been described: blood pool agents, myocardial perfusion agents, and metabolic markers (see the article by Geltman et al for more details on the application of specific agents).3”39 The blood pool agents are similar in principle to those found with single photon emitting nuclides-eg, they label either the red cells (eg, carbon- 11 [half-life, 20 minutes] labeled carbon monoxide, which binds with high affinity to hemoglobin), or plasma proteins (eg, Ga-68 [half-life, 68 minutes], which binds to transferrin).40 The cyclotron-produced myocardial perfusion agents are N-l 3-labeled ammonia (half-life, 9.9 minutes), which may enter the cell by an active pump mechanism, O-l 5-labeled water (half-life, 2.2 minutes),4’A3 or C- 1 l-labeled alcohols.44 N- 13 ammonia does not provide a quantitative determination of perfusion in absolute terms,45 since the extraction of ammonia may be altered by tissue oxygenation, pH, and flow rate. Within the flow range of clinical interest, however, the regional distribution of ammonia reflects regional perfusion. To determine myocardial perfusion reserve, N- 13 ammonia has been used with dipyridamole.46p47 This technique has proven sufficiently sensitive to detect a 47% coronary stenosis!8 While the N-13 approach works well, it cannot be readily used to make rapid repetitive determinations of regional perfusion, as can Rb82 or 0-15labeled water, due to the relatively long effective half-life of N-13 in the myocardium.39 Following injection, oxygen-15-labeled water reflects regional perfusion because of its high
426
MILLER
diffusivity at the capillary level (extraction = 96%).4’42 Once out of the capillary, the water is diluted in a large intracellular pool. As a result, the regional concentration of oxygen- 15 immediately after administration of labeled water reflects regional perfusion. The water method has been correlated against microspheres with a correlation of r = 0.94. One difficulty with the water method is the relatively large water space of red cells. When water is used to determine perfusion, the blood volume (red cell space) of the organ provides an unwanted, confounding signal, which must be corrected to obtain the correct flow values. This is a particularly vexing problem in the myocardium, where both the red cell volume of the myocardium and that in the chambers contribute to the signal. (Myocardial blood volume is extremely small in comparison to flow). Butanol labeled with C-l 1 has been suggested for the determination of regional perfusion. The agent has an extraction approaching one, and a longer half-life than oxygen-l 5 thereby easing the constraints on recording the data. Although its manufacture is more complex than that of oxygen-15-labeled water, the precision of the flow measurements available with butanol may be greater than that from oxygen-15labeled water.44 Metabolic
Substrates
The synthesis of positron-labeled metabolic substrates permits the determination of regional myocardial metabolism. When natural substrates have one atom replaced with a radioactive form, the compound is intrinsically labeled, and behaves in an identical fashion to the unlabeled agent. However, the speed of catabolic processes in the myocardium places severe constraints on the time spent making measurements of the regional distribution of metabolism. Fatty acids labeled with carbon- 11, for example, are catabolized to produce CO2 within 30 seconds of entry into the myocardium.50 To permit measurements to be made over longer intervals of time, chemical analogs of the metabolic substrates have been developed, The analogs enter metabolic pathways and proceed through at least one committed step parallel with unmodified substrates. The chemically modified agents reach a specific step in the catabolic cycle where they are recognized
ET AL
as different from the native substance, and usually remain in the cell for a prolonged interval of time. Glucose analogs can be labeled either with C-11 (1X11-2 deoxyglucose)51-53 or with F-18 (2-Fluoro-deoxyglucose),54*s5 while the fatty acid analogs are labeled with either C-l 1 (1-C-l 1-3 methyl heptadecanoic acid) or with iodine.s6 The myocardial extraction of glucose is usually less than 20%, but can vary markedly depending on insulin levels in the blood. Fatty acids have extractions between 50% and 60% under basal fasting circumstances, which may vary depending on the free fatty acid and insulin levels of the recipient. If serial arterial blood samples are obtained at the time of positron imaging with these metabolic agents, the regional myocardial metabolic rates of these agents may be calculated.‘7-5g Although the absolute metabolic data may be important for research, the importance of these values for patient care remains to be defined. Preliminary data suggest that the regional distribution of the metabolic radiopharmaceuticals in the myocardium may be sufficient to identify conditions of clinical importance.6’M6 Whether the quantitative data will add significantly to the understanding of the disease is uncertain. Glucose and fatty acid analogs may play a major role in nuclear cardiology in the near future as a result of their ability to identify underperfused but viable myocardium. Both agents appear to have a relative increase in extraction in the zone of ischemia. IODINATED
FATI-Y ACIDS
Several analogs of fatty acids have been synthesized with iodine labels.67-7L These agents can be readily imaged with a conventional gamma camera, either as planar or single photon emission computer tomography (SPECT) images.‘6*72 To increase the residence time of the fatty acids in the myocardium, analogs were synthesized with a phenyl ring at the omega position of the molecule.73-80 The substitution served both to stabilize the iodine on the molecule and to prevent terminal beta oxidation. The residence halftime of the radiolabel was increased from approximately ten minutes with straight chain iodinated fatty acids, to approximately 20 minutes with the addition of the phenyl group. The
NEW
CARDIAC
427
RADIONUCLIDES
addition of a methyl group at the 3 position (the same branched chain concept employed for the C-l l-labeled analog) in conjunction with a phenyl group at the omega position (to permit a stable attachment of the iodide) provided an increase in the residence half-time to over five hoUrs.WW From a metabolic perspective, the only way the branched chain, phenyl substituted fatty acid can clear from the myocardium is via simple back diffusion, or alpha oxidation. When labeled with the cyclotron-produced 13 hour half-life I-l 23 (159 keV), this radiopharmaceutical provides high quality images with a conventional gamma camera.83 In both animals1*82 and human studies,64 regional differences in the myocardial concentration of branched chain fatty acid analogs have been observed in the pressure overloaded and ischemically stunned myocardium. DETECTION OF ACUTE MYOCARDIAL NECROSIS
Radiopharmaceuticals suggested for the detection of acute myocardial necrosis include radioiodine, chlormerodrin, fluorescien, tetracycline,84 glucoheptonate,85 and pyrophosphate.8”92 An alternative aproach to the detection of acute necrosis is the use of a radiolabeled antibody directed against the heavy chain of human cardiac myosin, antimyosin.93-‘0’ This antibody localizes only in those cells whose membranes have been sufficiently damaged to permit the development of large holes clearly visible on electron micrographs. When cells reach this phase of damage, cell death is inevitable. Since exposure of the antigen can only occur when the membrane is disrupted, localization of antimyosin in the cell is associated only with that tissue that has undergone irreversible necrosis. To maximize the rate of blood clearance, a fragment of the antibody, Antimyosin-Fab, has been used for studies in human subjects.95-97 Antimyosin-Fab has been labeled with TC-99m and In-l 11. Coupling of the radionuclide to the antibody was achieved via a “bifunctional” chelate. The chelate is bifunctional in the sense that one of its functional groups is coupled to a lysine on the protein, while the remaining sites are available to couple to the radiolabel. Preliminary experience with this imaging approach in 24 patients with acute infarction has defined a strong relationship
between the extent of uptake observed on planar or SPECT images and prognosis.“’ Tc-99m
LOW DENSITY
LIPOPROTEINS
Atheromatous lesions are metabolically active, undergoing a repetitive cycle of endothelial injury and repair. During the repair phase, the endothelium recovering the area of damage has an increased permeability to low density proteins and the cholesterol carried by these proteins, resulting in the buildup of the atheromatous lesion. To determine if this could be detected by radionuclide imaging, Roberts et allo3 performed autoradiographic studies in rabbits with catheter-induced injury of the aorta. The autoradiographs demonstrated a marked increase in permeability to radioiodinated low-density lipoproteins (LDL) at the sites of reendothelialization. Subsequent studies by Lees et a1’04*‘05demonstrated that these lesions can be detected by radionuclide imaging in both the intact animal and man. Studies in eight human subjects with Tc-99m-labeled LDL have demonstrated localization in carotid, femoral, or coronary atheromatous lesions in 7/8.1°5 The radiopharmaceutical is prepared by dithionite reduction of TcO, in the presence of autologous LDL. This labeling approach has two disadvantages: (1) the six-hour half-life precludes imaging beyond 24 hours, at times when blood clearance would permit detection of zones of minimal concentration; and (2) the dithionite reduction results in the unavoidable production of some colloid-like material, which increases the liver concentration of the radiopharmaceutical. Despite these shortcomings, examination of surgical specimens obtained at carotid endarterectomy in two patients confirmed the concentration Tc-99m LDL in the most severely narrowed areas. Further studies are underway to couple In-l 11 or Ga-67 to the lipoprotein, to permit imaging at 48 to 72 hours after administration. Tc-99m-LABELED
AGENTS FOR MYOCARDIAL PERFUSION
While Tl-201 is currently the agent of choice for myocardial imaging, it has a number of limitations as a radiopharmaceutical. Thallium has a low energy photopeak (70 to 80 keV mercury x-rays), which results in significant soft tissue attenuation. Its long half-life of 72 hours
42%
and high concentration in the kidney limits the administered dose to about 3 mCi/S rads to the kidneys. Thus, prolonged imaging times are required. Finally, thallium is cyclotron-produced and is expensive. In recent years, there has been much interest in developing a Tc-99m-labeled agent for myocardial perfusion imaging to overcome the limitations of thallium. Deutsch et al have shown that some Tc-99m-labeled cationic complexes accumulate in the myocardium.‘06~‘07 These included Tc-99m DiArs, a diarsenical compound and DMPE-dimethlyphosphinoethane, an organophophosphate ligand.‘08*112 Tc99m DMPE showed promising results in rats and dogs and had the advantage of being soluble in aqueous solution. 108-11’Compared with Tl-201, Tc-99m DMPE showed similar blood clearance, equally good correlation over a wide range of regional blood flows, a higher heart to lung ratio, but higher liver uptake which could potentially interfere with interpretation of the inferior wall of the heart. Unfortunately, patient studies revealed poor uptake by the heart.“’ Liver uptake is prominent. The decrease in heart activity is slower than that of the liver but any improvement in contrast is lost by gradually increasing lung activity. This decreased uptake of Tc-99m DMPE by the human heart points out the importance of different species’ behavior. Another cationic Tc-99m complex, hexakis (t-butylisonitrile)technetium(I) (TBI) has marked cardiac uptake in a number of animal species. After IV injection, there is prompt myocardial uptake with a relatively constant concentration maintained for several hours. There is significant initial lung activity, which clears substantially after one hour. This initial pulmonary activity precludes early visualization of the myocardium. After intracoronary injection there is no myocardial washout for one hour. Initial experience in humans reported by Holman is encouraging. ‘I3 Planar and tomographic images of excellent quality were obtained. By one hour, the heart to lung ratio is 1.5 to 1, permitting satisfactory images. If, as in the animal studies, there is minimal washout of Tc-99m TBI for several hours, ischemia should be readily detected with this agent. In one patient who had both a fixed and transient defect on Tl-201 study, both perfusion defects were demonstrated by To99m TBI one and four hours following
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exercise. Thus, two injections may be necessary to distinguish ischemia from scar. The possibility of some redistribution from clearing lung activity into the myocardium must also be considered. Whole body images of Tc-99m TBI five hours after injection showed primarily heart, liver, spleen, and skeletal muscle uptake. Liver uptake rises steadily after injection. Primary clearance appears to be through the hepatobiliary system into the small bowel. Imaging in the LAO 70“ view is complicated by the superimposition of this liver activity onto the inferior segment of the myocardium. With exercise, the amount of activity in the myocardium remains the same; however, there is less liver uptake and intense uptake by the leg muscles. Although TBI looks promising, more patient experience as well as further research into the cellular mechanisms of uptake and retention by the myocardial cell are needed. Further understanding of these mechanisms may allow modification of the molecule to produce other complexes with more desirable biologic properties such as more rapid lung and liver clearance. INDIUM-111
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RADIONUCLIDES
Indium-1 11, a 2.7 day half-life cyclotronproduced Group IIIA radionuclide, has been used to label leukocytes, platelets, and antibodies. The nuclide decays via electron capture and gamma emission to Co-l 11 with major photons at 247 and 173 keV. The electron capture mode of decay results in the production of Auger electrons, which are associated with a high radiation burden to the intracellular structures in the immediate vicinity of the nuclide. Concerns about this microdosimetry limit the administered dose of this nuclide to c2 mCi for most human applications (200 to 500 &i are typically employed for studies with labeled cells). Platelets “4-‘18~‘19-‘22and white blood cells’23~‘2’ are the major blood components labeled with this nuclide. Platelet imaging has been advocated for the detection of thrombi in left ventricular aneurysms, “4*1’8~1’9 while labeled leukocytes have been advocated for evaluation of the clearance of zones of myocardial necrosis following infarction.‘23*‘21 In-l 11-labeled leukocytes provide an indication of the inflammatory response to infarction. The biologic half-life of autologous In- 11 l-labeled platelets is approximately 45
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hours. The slow clearance of blood pool activity, however, requires images to be recorded at 24 to 72 hours for the detection of thrombi. The potential role of both of these imaging techniques remains to be defined. Xenon-l 33
Xenon-133, an 80 keV, 5.3 day half-life fission product, is an inert noble gas that has been used for the determination of right heart function’ and regional myocardial perfusion.‘2”30 Since the agent is produced as a byproduct of uranium fission, it is available in curie quantities at modest cost. When administered IV in doses of 50 to 80 mCi, the 35% incidence of gamma photons provides a suitable photon flux for the determination of RV function.*31 In patients with normal lung parenchyma, >85% of the dose will be cleared in the first pass.” While the 0.5 rad/ injection radiation burden from these studies is higher than that with Kr-Slm, multiple injections can be administered without exceeding the accepted guidelines of t5 rad/examination. The determination of regional myocardial perfusion, either with direct intracoronary12”‘26 injection or administration via the left ventricular catheter12’ can be recorded with either the single’25,‘26 or multi-crystal’24 camera. The mathematics necessary to convert the observed clearance of the gas into perfusion/g of tissue were described by Kety,13’ and have been well validated by a number of other investigators.” This technique has been found to be particularly useful in conjunction with the coronary arteriogram to define the dynamic significance of a specific antomic abnormality.‘28*‘29 We have used a left heart bolus of Xe-133, administered via the left heart catheter, to determine left ventricular ejection fraction and regional wall motion (from data recorded in the first 10 seconds after injection) and regional myocardial perfusion (from the late myocardial clearance phase).12’ The data recorded with this technique have a good correlation (r = 0.9) with Tc-99m gated blood pool data for the determination of ventricular function. Zones of diminished myocardial perfusion were well-defined, but areas of hyperemia were underestimated due to the loss of the early portion of the clearance curve. Higher energy noble gases, such as cyclotron-
produced Xe- 127 (physical half-life, 36 days) with gamma photons of 172, 203, and 375 keV, may improve spatial resolution over that with Xe-133.13’ The radiation burden from this nuclide is less than that from Xe-133, despite its threefold increase in imageable photons, due to the lack of particulate emissions in the course of its decay. Unfortunately, the high cost of this nuclide has limited its clinical use. Should the cost of this nuclide come down, the combination of a long shelf life and its reasonable gamma energy would make this agent attractive for the performance of myocardial perfusion studies. FUTURE APPLICATIONS
Specific antibodies can be raised to bind to receptor sites. These antiidiotypic antibodies can be used both as tracers of the agonist-receptor distribution and as pharmaceuticals by competing with agonists to occupy receptor sites.‘33-‘40 In addition to antiidiotypic antibodies, receptors can be imaged with labeled antagonists such as hydroxybenzylpindolol. One can envisage imaging the up- and down-reguiation of cardiac alpha and beta receptors in diseases such as congestive heart failure,141 cardiac transplantation,‘42 coronary spasm, 143and sudden death,‘44 or after the chronic administration of adrenergic drugs.‘45 With the use of highly purified cardiac membrane preparations to raise monoclonal antibodies, the degree of nonspecific binding to low affinity sites should diminish. Binding sites for the biologically active peptide atria1 natriuretic factor (ANF) and opiate receptors modulating systemic and coronary vascular tone146,‘47 may soon be imaged in the cardiovascular and central nervous systems of patients with hypertension and coronary vasospasm. Aside from their potential for characterizing hormone- and drug-receptor interactions at the molecular level in vivo, these radioligands may provide valuable insights into the complex neurohumoral relationship between the heart and brain. Meta- [ 12311 iodobenzylguanidine (M- 1231IBG), an analog of the adrenergic neuron blocking agent guanethidine, is taken up by adrenergic neurons via a mechanism similar to norepinephrine. This agent has been employed to image the heart, presumably binding to cardiac adrenergic receptors, in normal human volunteers’48 and patients with suspected pheochromocytoma.‘49
430
Although the myocardium was well-visualized in normal subjects,14* M- 13 1I-IBG uptake was significantly reduced in pheochromocytoma patients, presumeably due to down-regulation of cardiac adrenergic receptors from high circulating levels of norepinephrine.‘49
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The diagnostic promise of metabolic imaging and tomography can only be realized if these and other radiopharmaceuticals are developed to keep pace with rapidly expanding imaging technology.
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