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Treatment of lung tumor colonies with 90Y targeted to blood vessels: comparison with the alpha-particle emitter 213Bi.

An in vivo lung tumor model system for radioimmunotherapy of lung metastases was used to test the relative effectiveness of the vascular- targeted beta-particle emitter 90Y, and alpha-particle emitter, 213Bi. Yttrium-90 was shown to be stably bound by CHXa" DTPA-MAb 201B conjugates and delivered efficiently to lung tumor blood vessels. Dosimetry calculations indicated that the lung received 16.2 Gy/MBq from treatment with 90Y MAb 201B, which was a sevenfold greater absorbed dose than any other organ examined. Therapy was optimal for 90Y with 3 MBq injected. Bismuth-213 MAb 201B also delivered a similar absorbed dose (15Gy/MBq) to the lung. Yttrium-90 was found to be slightly more effective against larger tumors than 213Bi, consistent with the larger range of 2 MeV beta particles from 90Y than the 8 MeV alpha particles from 213Bi. Treatment of EMT-6 tumors growing in immunodeficient SCID mice with 90Y or 213Bi MAb 201 resulted in significant destruction of tumor colonies; however, 90Y MAb 201B was toxic for the SCID mice, inflicting acute lung damage. In another tumor model, IC-12 rat tracheal carcinoma growing in SCID mouse lungs, 90Y therapy was more effective than 213Bi at destroying lung tumors. However, 90Y MAb 201B toxicity for the lung limited any therapeutic effect. We conclude that, although vascular-targeted 90Y MAb can be an effective therapeutic agent, particularly for larger tumors, in this model system, acute damage to the lung may limit its application.

Animals↗

Measurement of radiation absorbed dose in endovascular Ho-166 brachytherapy using a balloon angio-catheter.

The purpose of this study was to estimate the absorbed dose distribution of Ho-166 endovascular beta irradiation using an angio-catheter. The liquid form of Ho-166 was produced at the Korea Atomic Energy Research Institute (KAERI) by an (n,gamma) reaction. Ho-166 has a half-life of 26.8 h and emits a high-energy beta particle with a maximum energy of 1.85 MeV. GafChromic film was used for the estimation of the absorbed dose of beta particles. A Co-60 teletherapy source and a 6 MV photon beam from a linear accelerator were used to generate dose-optical density calibration curves. The exposed films were read using a videodensitometer. With a modified micrometer, the film was positioned accurately on the surface of the balloon in water. The balloon was filled with Ho-166 solution to a pressure of 4 atm. Several film exposures were made with varying irradiation times and activities. The radiation absorbed dose rates were 1.02, 0.51 and 0.35 Gy x min(-1) x GBq(-1) x ml(-1) at the balloon surface, 0.5 and 1 mm from the balloon surface, respectively. The absorbed dose distribution revealed that Ho-166 is a good source for endovascular irradiation as the beta range is very short, avoiding unnecessary irradiation of normal tissue. A clinically applicable irradiation and duration of exposure were achievable utilizing our system.

Angioplasty, Balloon, Coronary↗

Radium and uranium concentrations in Georgia community water systems.

The first cycle of statewide radionuclide concentration measurements of public drinking water supplies was completed in accord with the Federal and Georgia Safe Drinking Water Acts. The recommended pattern of analysis is initial screening for gross alpha-particle activity, followed by measuring 226Ra if the gross alpha-particle activity is above 5 pCi/l. and then measuring 228Ra if the 226Ra concentration is above 3 pCi/l; and uranium analysis if the gross alpha-particle activity exceeds 15 pCi/l. Surface water supplies for more than 100,000 persons are analyzed for 3H and 90Sr and screened for gross beta-particle activity, with additional analytical requirements if the latter is above 50 pCi/l. Specified supplies downstream for nuclear facilities are analyzed for 3H, 90Sr and 131I, and further analyses are required if the gross beta-particle activity is above 15 pCi/l. More thorough screening was applied for 1400 public water supplies in Georgia, of which about 90% use groundwater. Radium concentrations exceeded the maximum contaminant level (MCL) of 5 pCi/l. in 24 groundwater supplies, mostly due to elevated 226Ra. The gross alpha-particle activity minus uranium concentrations exceeded the 15 pCi/l. MCL in 3 additional samples. No MCL was exceeded in surface water. The S.D.s of analytical results estimated from replicate analyses were approximately twice those based on counting statistics, suggesting that screening levels should be lowered to assure detection of 226Ra at MCL values.

Georgia↗

Real-time analysis of endosomal lipid transport by live cell scintillation proximity assay.

A scintillation proximity assay has been developed to study the endosomal trafficking of radiolabeled cholesterol in living cells. Mouse macrophages were cultured in the presence of tritiated cholesterol and scintillant microspheres. Microspheres were taken up by phagocytosis and stored in phagolysosomes. Absorption of tritium beta particles by the scintillant produces light signals that can be measured in standard scintillation counters. Because of the short range of tritium beta particles and for geometric reasons, scintillant microspheres detect only that fraction of tritiated cholesterol localized inside phagolysosomes or within a distance of approximately 600 nm. By incubating cultures in a temperature-controlled microplate reader, the kinetics of phagocytosis and cholesterol transport could be analyzed in near-real time. Scintillation signals were significantly increased in response to inhibitors of lysosomal cholesterol export. This method should prove a useful new tool for the study of endosomal trafficking of lipids and other molecules.

Animals↗

Antibody therapy in acute myeloid leukemia: current status and future directions.

Monoclonal antibodies have become an important modality for cancer therapy. The genetically engineered, humanized anti-CD33 antibody HuM195 has demonstrated modest activity against overt relapsed acute myeloid leukemia (AML) and more substantial activity against minimal residual disease in acute promyelocytic leukemia. Radioimmunotherpay with beta-particle-emitting isotopes has eliminated large leukemic burdens while minimizing radiation exposure to normal tissues in both nonmyeloablative and myeloablative regimens. Targeted beta-particle immunotherapy with agents such as bismuth 213-labeled HuM195 offers the possibility of a more selective tumor cell kill with less damage to surrounding normal cells. Directed chemotherapy using the anti-CD33-calicheamicin conjugate gemtuzumab ozogamicin (Mylotarg) has produced remissions in patients with relapsed AML.

Antibodies, Monoclonal↗

Estimates of dose to intraperitoneal micrometastases from alpha and beta emitters in radioimmunotherapy.

Intraperitoneal metastases from ovarian and other gynecologic tumors are a significant source of treatment failure. In recent years, investigators have used radiolabeled monoclonal antibodies to treat this disease with encouraging results. We have developed a dose calculational technique which generates isodose distributions from intraperitoneally administered alpha and beta particle emitters. In this study we apply the calculations to tissue biopsy samples to determine the adequacy of dose to ovarian micrometastases. Tissue samples from staging biopsies at the time of surgical debulking are scanned to identify small metastases. The patient population studied comprised those with ovarian disease who based on clinical criteria would be considered good candidates for intraperitoneal radioimmunotherapy. The regions of interest (which include the tumor and surface of the peritoneum) are digitized and tumor volumes are contoured. Dose calculations based on the modeling of intraperitoneally administered antibodies radiolabeled with various isotopes is performed and the minimum dose to tumor and normal tissue is assessed. For example, with tumor uptake of 0.1% injected dose per gram of tissue, the surface tumor dose from alpha emitters is up to 45,000 rads. The dose falls to 6000 rads at approximately 40 microns from the peritoneal surface. The surface dose from 20 mCi 90Y administered in 1500 ml saline is up to 10,000 rads, and at a 2-mm depth, approximately 2000 rads. From our calculation dose distribution from radioimmunotherapy varies as a function of physical characteristics of the isotope, absorption of activity, and amount of disease being treated.

Alpha Particles↗

A new treatment planning formalism for catheter-based beta sources used in intravascular brachytherapy.

Intravascular brachytherapy (IVBT) is an emerging modality for the treatment of atherosclerotic lesions in the artery. As part of the refinement in this rapidly evolving modality of treatment, the current simplistic dosimetry approach based on a fixed-point prescription must be challenged by future rigorous dosimetry method employing image-based three-dimensional (3D) treatment planning. The goals of 3D IVBT treatment planning calculations include (1) achieving high accuracy in a slim cylindrical region of interest, (2) accounting for the edge effect around the source ends, and (3) supporting multiple dwell positions. The formalism recommended by Task Group 60 (TG-60) of the American Association of Physicists in Medicine (AAPM) is applicable for gamma sources, as well as short beta sources with lengths less than twice the beta particle range. However, for the elongated beta sources and/or seed trains with lengths greater than twice the beta range, a new formalism is required to handle their distinctly different dose characteristics. Specifically, these characteristics consist of (a) flat isodose curves in the central region, (b) steep dose gradient at the source ends, and (c) exponential dose fall-off in the radial direction. In this paper, we present a novel formalism that evolved from TG-60 in maintaining the dose rate as a product of four key quantities. We propose to employ cylindrical coordinates (R, Z, phi), which are more natural and suitable to the slim cylindrical shape of the volume of interest, as opposed to the spherical coordinate system (r, theta, phi) used in the TG-60 formalism. The four quantities used in this formalism include (1) the distribution factor, H(R, Z), (2) the modulation function, M(R, Z), (3) the transverse dose function, h(R), and (4) the reference dose rate at 2 mm along the perpendicular bisector, D(R0=2 mm, Z0=0). The first three are counterparts of the geometry factor, the anisotropy function and the radial dose function in the TG-60 formalism, respectively. The reference dose rate is identical to that recommended by TG-60. The distribution factor is intended to resemble the dose profile due to the spatial distribution of activity in the elongated beta source, and it is a modified Fermi-Dirac function in mathematical form. The utility of this formalism also includes the slow-varying nature of the modulation function, allowing for more accurate treatment planning calculations based on interpolation. The transverse dose function describes the exponential fall-off of the dose in the radial direction, and an exponential or a polynomial can fit it. Simultaneously, the decoupling nature of these dose-related quantities facilitates image-based 3D treatment planning calculations for long beta sources used in IVBT. The new formalism also supports the dosimetry involving multiple dwell positions required for lesions longer than the source length. An example of the utilization of this formalism is illustrated for a 90Y coil source in a carbon dioxide-filled balloon. The pertinent dosimetric parameters were generated and tabulated for future use.

Beta Particles↗

[Low level alpha activity measurements with pulse shape discrimination--application to the determination of alpha-nuclides in environmental samples].

Liquid scintillation counting of alpha rays with pulse shape discrimination was applied to the analysis of 226Ra and 239+240Pu in environmental samples and of alpha-emitters in/on a filter paper. The instrument used in this study was either a specially designed detector or a commercial liquid scintillation counter with an automatic sample changer, both of which were connected to the pulse shape discrimination circuit. The background counting rate in alpha energy region of 5-7 MeV was 0.01 or 0.04 cpm/MeV, respectively. The figure of merit indicating the resolving power for alpha- and beta-particles in time spectrum was found to be 5.7 for the commercial liquid scintillation counter.

Alpha Particles↗

Kinetics of positron emitters in vivo characterized with a beta probe.

To facilitate characterization of regional myocardial kinetics of positron-emitting tracers in vivo without distortion by activity outside the region of interest, a probe was developed and evaluated for monitoring radioactivity by detection of positrons themselves. These particles (beta particles) have a maximal range in tissue of only few millimeters rather than the larger range of gamma photons emitted as a result of positron annihiliation. Regional myocardial time-activity curves were determined in open-chest dogs after intracoronary injection of 0.5-1.5 mCi [15O]H2O, a tracer used for measurement of myocardial blood flow, or 6.0-8.0 mCi [11C]palmitate, a tracer used for noninvasive assessment of myocardial metabolism. Time-activity curves after [11C]palmitate injection clearly delineated specific components of myocardial tracer clearance previously identified in vitro in isolated perfused hearts. Myocardial washout of [15O]H2O was monoexponential for more than 2 min without distortion induced by recirculating tracer in ventricular blood. Reproducibility of measured tracer clearance rates during monoexponential clearance was high based on duplicate determinations for both tracers. The beta-detector probe developed overcomes several intrinsic limitations of gamma-probe systems or well counting of serial myocardial biopsies for studies of positron-emitting tracers in vivo and should facilitate assessment of factors of influencing tracer kinetics in vivo relevant to positron-emission tomography.

Animals↗

[Effect of the structure of the cell nucleus chromatin on absorption of low-energy beta-radiation emitted from an incorporated source].

To study the energy absorption in cell nuclei the analysis was made of the level of registration of beta-particles, emitted by the incorporated tritium, using a liquid scintillation counter. It was shown that the treatment, modifying the chromatin structure, changed the number of beta-particles registered. The pattern of the spectral changes indicated that the effect observed was not the result of the quenching processes. The effect was absent when the source of a higher energy (14C) was used. The authors submit the conceptions concerning the mechanisms of the phenomenon observed which are confirmed by the theoretical studies.

Animals↗

DNA strand breakage in Chinese hamster V79 cells caused by low levels of incorporated [3H] and [14C]thymidine.

A sensitive alkali-unwinding assay was used to measure DNA strand breakage in Chinese hamster V79 cells caused by low-level incorporation of methyl-labelled [3H] and [14C] thymidine, and to estimate the effective dose per disintegration relative to low doses of gamma-irradiation. Damage equivalent to 0.0035 +/- 0.0006 and 0.0014 +/- 0.0005 Gy was observed for each 3H and 14C disintegration respectively. These values agree well with those expected from the estimated nuclear radiation dose delivered by the beta particles if a relative biological effect (r.b.e.) of 1.0 is assumed, and suggest that strand-breakage produced by these isotopes is determined by the nuclear radiation dose delivered by the beta particles.

Animals↗

Further electron-microscope studies on the human hepatic sinusoidal wall with special reference to the fat-storing cell.

In biopsy specimens from two normal human livers, fat-storing cells and Kupffer cells were observed by electron microscopy with the following results: 1) In the human Ito cells numerous micropinocytotic caveolae and vesicles occurred either scattered beneath the plasma membrane or fused into short tubules. In the cytoplasm abutting on these structures, minute clusters of glycogen beta-particles were revealed which presumably had been synthesized in the local cytoplasm from carbohydrate (glucose) ingested by pinocytosis. 2) Lipid droplets (vacuoles) were formed within the accumulations of the glycogen beta-particles. These findings support the view that the glycogen synthesized in the Ito cells may represent a transitional compound in the process of lipid synthesis from carbohydrate. 3) Among lipid vacuoles, electron-dense droplets equally large were found, often containing electron-lucent areas in their center. On the surface of these dense droplets, compact clusters of glycogen particles adhered as if they might have permeated into the droplets. These droplets may possibly be immature lipid droplets retaining chemical properties of the glycogen in their superficial part; they remained insoluble during the preparation procedures for ultrathin sections. 4) The occurrence of the worm-like structure has for the first time been revealed in the human Kupffer cells. Besides its short tubular profiles, a more complex structure was demonstrated.

Female↗

Quantitative measurement of local cerebral metabolic rate for glucose utilizing tritiated 2-deoxyglucose.

The [14C]2-deoxyglucose (2-DG) technique has been widely utilized for quantitative measurement of local cerebral metabolic for glucose (1CMRG) in animals. The technique as presently used is limited by the energy of 14C beta-particles, which can travel relatively great distances in tissue. This results in limited audioradiographic resolution and in computed 14C concentrations which are a function of tissue section thickness. [3H]2-DG has less energetic beta-particles; hence, autoradiographs have better resolution and optical densities are independent of tissue thickness for sections greater than 5 micrometer. We have developed a method for quantitation of 1CMRG in rats using [3H]2-DG and a newly developed ultrasensitive X-ray film. Autoradiographic tissue standards were prepared by injecting rats with [3H]2-DG and assaying micro-samples of brain for 3H concentration. Ten rats were used in this study. Five rats received [3H]2-DG (300 muCi/100 g) and 5 rats received [14C]2-DG (7.5 muCi/100 g). The mean 1CMRG values for selected areas of the central nervous system demonstrated no significant difference (P greater than 0.05) between the [14C]2-DG and the [3H]2-DG groups. Values for 1CMRG from the [3H]2-DG group showed no variation attributable to inadequate microtome precision. The improved resolution obtained by utilizing [3H]2-DG is especially evident where gray matter (high 1CMRG) is immediately adjacent to white matter (low 1CMRG).

Animals↗

Pulmonary carcinogenicity of repeated inhalation exposure of rats to aerosols of 239PuO2.

To study the long-term biological effects of repeated inhalation exposure to 239PuO2, 84-day-old rats were exposed to aerosols of 239PuO2 to re-establish desired 239Pu lung burdens of 26, 80 or 250 Bq every other month for 1 year (seven exposures). Other rats were exposed once at 84 or 450 days of age to achieve desired initial lung burdens of 30, 90, 280 or 850 Bq. The incidences of lung tumors were not significantly different (Fisher's exact test; P > 0.05) in groups of rats with similar lifetime mean alpha-particle doses to the lungs of 0.90 +/- 0.39 to 4.4 +/- 1.8 (+/- SD) Gy, whether exposed once or repeatedly. Among rats with mean alpha-particle doses of 12 +/- 2.4 to 10 +/- 2.1 Gy to the lungs after single or repeated exposures, respectively, the crude incidence of lung tumors was significantly less (Fisher's exact test; P < 0.05) in the rats exposed repeatedly. Times to death of rats with lung tumors were compared among groups with similar alpha-particle doses to the lungs after single or repeated exposure to 239PuO2. Those that died with lung tumors after repeated exposures died at times similar to (Mantel-Cox statistic; P > 0.05) or later than (Mantel-Cox statistic; P < 0.05) those for 84-day-old rats exposed once. The risk of lung tumors in rats per unit dose to the lungs was less in the rats exposed repeatedly than in those exposed once. It was concluded that alpha-particle doses to the lung of rats exposed repeatedly to aerosols of 239PuO2 were not more carcinogenic and possibly were less carcinogenic than the dose after a single inhalation exposure when rats with similar lifetime alpha-particle doses to the lungs were compared. The relative biological effectiveness in rats of the alpha-particle dose to the lungs from inhaled 239PuO2 relative to beta-particle doses to the lungs from inhaled 144CeO2 was 21 +/- 3.

Administration, Inhalation↗

Ordered synthesis and mobilization of glycogen in the perfused heart.

The molecular order of synthesis and mobilization of glycogen in the perfused heart was studied by 13C NMR. By varying the glucose isotopomer ([1-13C]glucose or [2-13C]glucose) supplied to the heart, glycogen synthesized at different times during the perfusion was labeled at different carbon sites. Subsequently, the in situ mobilization of glycogen during ischemia was observed by detection of labeled lactate derived from glycolysis of the glucosyl monomers. When [1-13C]glucose was given initially in the perfusion and [2-13C]glucose was given second, [2-13C]lactate was detected first during ischemia and [3-13C]lactate second. This result, and the equivalent result when the glucose labels were given in the reverse order, demonstrates that glycogen synthesis and mobilization are ordered in the heart, where glycogen is found morphologically only as beta particles. Previous studies of glycogen synthesis and mobilization in liver and adipocytes [Devos, P., & Hers, H.-G. (1979) Eur. J. Biochem. 99, 161-167; Devos, P., & Hers, H.-G. (1980) Biochem. Biophys. Res. Commun. 95, 1031-1036] have suggested that the organization of beta particles into alpha particles was partially responsible for ordered synthesis and mobilization. The observations reported here for cardiac glycogen suggest that another mechanism is responsible. In addition to examining the ordered synthesis and mobilization of cardiac glycogen, we have selectively monitored the NMR properties of 13C-labeled glycogen synthesized early in the perfusion during further glycogen synthesis from a second, differently labeled substrate. During synthesis from the second labeled glucose monomer, the glycogen resonance from the first label decreased in integrated intensity and increased in line width.(ABSTRACT TRUNCATED AT 250 WORDS)

Animals↗

Basic characterization of 64Cu-ATSM as a radiotherapy agent.

64Cu-diacetyl-bis(N4-methylthiosemicarbazone) (64Cu-ATSM) is a promising radiotherapy agent for the treatment of hypoxic tumors. In an attempt to elucidate the radiobiological basis of 64Cu-ATSM radiotherapy, we have investigated the cellular response patterns in vitro cell line models. Cells were incubated with 64Cu-ATSM, and the dose-response curves were obtained by performing a clonogenic survival assay. Radiation-induced damage in DNA was evaluated using the alkali comet assay and apoptotic cells were detected using Annexin V-FITC and propidium iodide staining methods. Washout rate and subcellular distribution of 64Cu in cells were investigated to further assess the effectiveness of 64Cu-ATSM therapy on a molecular basis. A direct comparison of subcellular localization of Cu-ATSM was made with the flow tracer analog Cu-pyruvladehyde-bis(N4-methylthiosemicarbazone). In this study, 64Cu-ATSM was shown to reduce the clonogenic survival rate of tumor cells in a dose-dependent manner. Under hypoxic conditions, cells took up 64Cu-ATSM and radioactive 64Cu was highly accumulated in the cells. In the 64Cu-ATSM-treated cells, DNA damage by the radiation emitted from 64Cu was detected, and inhibition of cell proliferation and induction of apoptosis was observed at 24 and 36 h after the treatment. The typical features of postmitotic apoptosis induced by radiation were observed following 64Cu-ATSM treatment. The majority of the 64Cu taken up into the cells remained in the postmitochondrial supernatant (the cellular residue after removal of the nuclei and mitochondria), which indicates that the beta- particle emitted from 64Cu may be as effective as the Auger electrons in 64Cu-ATSM therapy. These data allow us to postulate that 64Cu-ATSM will be able to attack the hypoxic tumor cells directly, as well as potentially affecting the peripheral nonhypoxic regions indirectly by the beta- particle decay of 64Cu.

Animals↗

Background radiation: natural and man-made.

A brief overview and comparison is given of dose rates arising from natural background radiation and the fallout from atmospheric testing of nuclear weapons. Although there are considerable spatial variations in exposure to natural background radiation, it is useful to give estimates of worldwide average overall exposures from the various components of that background. Cosmic-ray secondaries of low linear energy transfer (LET), mainly muons and photons, deliver about 280 microSv a(-1). Cosmic-ray neutrons deliver about another 100 microSv a(-1). These low- and high-LET exposures are relatively uniform to the whole body. The effective dose rate from cosmogenic radionuclides is dominated by the contribution of 12 microSv a(-1) from 14C. This is due to relatively uniform irradiation of all organs and tissues from low-energy beta particles. Primordial radionuclides and their progeny (principally the 238U and 232Th series, and 40K) contribute about 480 microSv a(-1) of effective dose by external irradiation. This is relatively uniform photon irradiation of the whole body. Internally incorporated 40K contributes a further 165 microSv a(-1) of effective dose in adults, mainly from beta particles, but with a significant gamma component. Equivalent doses from 40K are somewhat higher in muscle than other soft tissues, but the distinction is less than a factor of three. Uranium and thorium series radionuclides give rise to an average effective dose rate of around 120 microSv a(-1). This includes a major alpha particle component, and exposures of radiosensitive tissues in lung, liver, kidney and the skeleton are recognised as important contributors to effective dose. Overall, these various sources give a worldwide average effective dose rate of about 1160 microSv a(-1). Exposure to 222Rn, 220Rn and their short-lived progeny has to be considered separately. This is very variable both within and between countries. For 222Rn and its progeny, a worldwide average effective dose rate is about 1105 microSv a(-1). For 220Rn and its progeny, the corresponding value is 91 microSv a(-1). In both cases, the effective dose is mainly due to a particle irradiation of the bronchial tissues of the lungs. Overall, the worldwide average effective dose rate from natural background is about 2400 microSv a(-1) or 2.4 mSv a(-1). For comparison, worldwide average effective dose rates from weapons fallout peaked at 113 microSv a(-1) (about 5% of natural background) in 1963 and have since fallen to about 5.5 microSv a(-1) (about 0.2% of natural background). These values perhaps serve to emphasise that even gross insults to the natural environment from anthropogenic releases of radioactive materials are likely to be of limited significance when set in the context of the ambient radioactive environment within which all organisms, including humans, have developed.

Animals↗

A quantitative study of radionuclide characteristics for radioimmunotherapy from 3D reconstructions using serial autoradiography.

PURPOSE: Using 131I-labeled monoclonal antibody (MoAb) data, assess the dosimetrical impact of labeling the same MoAb with 186Re or 90Y, under the assumption that the biodistribution of the radiolabeled MoAb in tumor relative to blood is independent of the radionuclide. METHODS AND MATERIALS: Radial radioactivity and dose-rate distributions at 1, 4, and 7 days postinjection were derived from three dimensional (3D) reconstructions of serial autoradiographs of LS174T human colon cancer xenografts in athymic nude mice treated with a single intraperitoneal administration of 300 microCi 131I-labeled MoAb 17-1A. Bone marrow dose was calculated taking into account energy deposited external to the bone marrow cavity due to the range of the beta particles. RESULTS: For 1 cm diameter tumors, uptake was mostly at the tumor surface for earlier postinjection times, but exhibited comparable activity levels from the surface to the core of the 7-day sample. The computed dose-rate distributions for 186Re and 90Y were more uniform than for 131I, but smaller fractions of the dose were deposited within the tumor volume due to the larger mean energies of 90Y and 186Re beta particles relative to those for 131I. However, when the tumor doses were normalized to the production of equivalent bone marrow doses, in the case of athymic nude mice, the tumor doses were calculated to be 15.3 Gy (131I), 14.1 Gy (186Re), and 12.0 Gy (90Y). For comparison, these calculations were extended to the case of human therapy, yielding tumor doses of 16.7 Gy (131I), 18.2 Gy (186Re), and 13.4 Gy (90Y). CONCLUSION: In the case of colon cancer xenografts where the MoAb uptake is initially concentrated at the tumor surface, we find a decreasing tumor dose per constant bone marrow dose for radionuclides of increasing mean beta energies and decreasing half-lives. However, a radionuclide with larger mean beta energy such as 90Y generates a significantly more uniform dose deposition within the tumor, especially concerning the core of the tumor, compared to 131I. For human therapy, a gamma component adds little to the tumor dose but increases dose to the marrow.

Animals↗