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Evidence for non-chromosomal hepatitis B virus surface (HBsAg)- and core antigen (HBcAg)-specific DNA sequences in a hepatoma cell line.

As demonstrated previously, a "beta particle" fraction isolated from the cytoplasm of PLC/PRF/5 cells contains hepatitis B virus (HBV)-specific DNA. Here, further evidence is provided that the specificity of the DNA for HBV is represented at least by sequences coding for the surface and core antigen (HBsAg and HBcAg). This was shown by two different hybridization techniques. One of them, the technique of Southern, distinguished these hybrid molecules formed from those containing HBV DNA integrated into chromosomes. The HBV-specific beta particle DNA forms two distinct bands separate from the high molecular weight cellular DNA.

Base Sequence↗

Electron microscope radioautographic study of glycogen synthesis in the rabbit retina.

Glycogen is present in the rabbit retina in monoparticulate form. Beta particles ( approximately 229 A) are abundant in Müller cell cytoplasm, particularly in its inner portion, decreasing in number outwards along the cell. They are slightly larger ( approximately 250 A) and much scarcer in neurons, though regularly present in the juxtanuclear Golgi region of ganglion cells. When the retina was incubated in a glucose-free medium, it was rapidly depleted of native glycogen. On further incubation in medium containing glucose-(3)H plus unlabeled glucose, glycogen reappeared in the form of beta particles of the same size and distribution as native ones, while radioautography revealed the appearance of amylase-labile radioactivity in the same locations. This newly formed glycogen was not associated with any particular organelle. The rate of synthesis, as judged from the amount of radioactivity, was high in the inner portion of Müller cells and declined uniformly toward the cell outer end, following a logarithmic gradient. The rate of synthesis was low in ganglion cells, at best approaching values in the outer portion of Müller cells. The concentration of glycogen in the inner portion of Müller cells is consistent with the view that it may be the source of glucose for the anaerobic glycolysis prevailing in the inner retina.

Animals↗

Radioisotope stents for the prevention of restenosis: what did we learn from pre-clinical studies?

This article will discuss the lessons learned by using stents implanted with low activities of radioisotopes to prevent in-stent restenosis. A continuous low-dose rate radiation delivered by radioisotope stents has been shown to reduce the proliferative activity of smooth muscle cells and to inhibit neointimal growth. However, the radiation also delays endothelialization of the stents. Both the dose rate and the cumulative dose delivered by radioisotope stents appear to affect outcome. The neointima covering radioactive stents is characterized by a reduced cellularity, increased amounts of fibrin and extracellular matrix proteins. Aneurysm formation or excessive tissue destruction due to the radiation were not observed. Animals studies including up to 1 year follow-up periods suggest that beta-particle-radiation as well as gamma-radiation are effective in reducing neointimal hyperplasia. It is still unknown, however, which range of activities are needed and if a combination of radioisotopes, i.e. with short and long halflives, further reduce neotima formation over the long-term. An appropriate stent design for homogenous dose distribution around the stent may be important, i.e. articulations or large cell sizes may have disadvantages. Augmented neointima formation at the ends of radioactive stents, in particular when using beta-particle emitting stents, has been observed in animal models. Future studies will focus on the effects of increasing activity levels at the stent ends, optimal stent designs, alternative isotopes and different dosing strategies.

Journal Article↗

Regional tidal volume assessed by gated lung imaging.

We have measured regional lung tidal volumes and functional residual capacities by accumulating and framing iso-volumic images while the patient rebreathes 127Xe. As the lung changes shape during ventilation corrections for changes in geometry were obtained by simultaneous collection of 99Tcm counts from the gated perfusion scan. Regions of interest were made to vary throughout the respiratory cycle so that a region had always the same value of 99Tcm counts. From the corrected 127Xe counts regional tidal volumes (TVr) and functional residual capacities (FRCr) were derived. In patients with established chronic bronchitis and emphysema FRCr were greater and the ratio TVr/FRCr decreased compared with patients with relatively normal static and dynamic lung volumes. Preliminary studies suggest that this ratio was a better discriminator between normal and abnormal regional function than estimates of regional xenon washout. Studies with xenon-133 have contributed to our understanding of the physiology of ventilation but have contributed somewhat less to routine clinical practice. This results in part from the unsatisfactory physical properties of xenon-133. Its relatively low gamma ray energy of 80 keV results in significant self-absorption losses and the activity which may be administered is limited by the radiation dose from the associated beta particles so that relatively poor counting statistics are obtained. With inhaled technetium-99m (99Tcm) microspheres imaging conditions are greatly improved but the distribution of these particles may not equate with the distribution of ventilation particularly if wet particles are used. Moreover, simultaneous microsphere perfusion scans with technetium-99m as a label are impossible. Krypton-81m gas has a suitable energy but the short half-life of the rubidium-81m generator (4.7 h) makes supply difficult and the ultrashort half-life of the krypton-81m gas (13 s) leads to problems in calculating the indices of ventilation. Xenon-127 (127Xe) gas has a more favourable dosimetry profile than xenon-133 because it does not have associated beta particles. Further it has an energy (203 keV) suitable for modern gamma cameras and may be used in the presence of injected 99Tcm microspheres to provide simultaneous ventilation/perfusion imaging. Conventional techniques have assumed that a static image of a dynamic process is adequate. As the lungs move during imaging, some account of this respiratory movement should be made.(ABSTRACT TRUNCATED AT 250 WORDS)

Adult↗

Consideration of tissue response in the application of the two-mutation model to radiation carcinogenesis.

The Moolgavkar-Venzon-Knudson (MVK) two-mutation model of carcinogenesis is an analytical model that predicts the variation of cancer yield-rate with time, and with dose of a carcinogen. The model is biologically based, and assumes that a specific mutation in a stem-cell will increase its rate of proliferation compared with that of unmutated cells, so that a clone of pre-malignant cells develops; a second specific mutation in any one of these will make it malignant, and a cancer will start to grow. The model has been used in recent years to analyse a number of sets of epidemiological data on carcinogenesis. The purpose of this paper is to point to a problem in the use of this model for radiation-induced carcinogenesis, namely that ionizing radiation causes reproductive death of stem cells, which leads to regenerative division and hence a change in the number of stem-cells at risk. The possible effects of such changes on the predictions of the model are discussed. At low dose-rates of continuous or chronic irradiation and at low doses of acute irradiation, it is expected that pre-malignant cells will be killed along with the unmutated cells, and that the regenerative division of the surviving pre-malignant cells will restore the numbers of both stem cells and pre-malignant cells to what they would have been in the absence of cell killing; hence, no net effect of the tissue regeneration is expected. At high dose-rates, the initial delay in regenerative division and subsequent faster proliferation are expected to lead to an initial reduction in tumour yield-rate with time (compared with that predicted by the MVK model) followed by a faster increase. For acute irradiation, in the particular case of beta-particle irradiation of the skin, at high doses where there are practically no surviving cells in the irradiated area, repopulation by unirradiated cells from the margin is predicted to lead to a decrease in tumour yield-rate with dose. The predictions have been compared with published data on the induction of osteosarcoma in mouse by repeated injection of 89Sr, the induction of skin tumours in rat by acute and chronic irradiation with electrons, and the induction of skin tumours in mouse by acute irradiation with beta-particles. At low doses and dose-rates the basic MVK model fitted the data well. At higher doses and dose-rates the expected effects of tissue regeneration were observed qualitatively, although there were some discrepancies in detail; these are discussed.

Animals↗

In vitro toxicity of A-431 carcinoma cells with antibodies to epidermal growth factor receptor and epithelial glycoprotein-1 conjugated to radionuclides emitting low-energy electrons.

PURPOSE: The ability of antibodies (Abs) conjugated to radionuclides emitting low-energy electrons to specifically kill nonadherent lymphoma target cells in vitro was demonstrated previously. This study extends this work to adherent carcinoma cells. The fact that these cells are spread out on plastic can potentially make it more difficult to deliver radiation to the nucleus from decays in the cytoplasm or on the cell surface. EXPERIMENTAL DESIGN: The Abs tested were anti-epidermal growth factor receptor and anti-epithelial glycoprotein-1, conjugated to indium-111 or iodine-125, which emit low-energy Auger and conversion electrons. Conjugates of the beta-particle emitter, iodine-131, also were tested, for comparison. Abs were incubated with the cells for 2 days, and then the treated cells were assayed for colony-forming units. The radiation dose delivered to the nucleus was calculated from the cumulative decays per cell. RESULTS: With conjugates of (111)In, very potent killing was obtained with both of the Abs, with 100% kill (approximately 4-5 logs) even at subsaturating Ab concentrations. Lower levels of kill were obtained with (125)I or (131)I conjugates. Conjugates with (131)I, a beta-particle emitter, produced greater nonspecific toxicity. The greater potency of (111)In could be attributed to the higher specific activity that was obtained routinely with this radiolabel, up to 70 mCi/mg. Uptake of radioactivity peaked at approximately 200 cpm per cell. Dosimetry calculations, using subcellular S values, demonstrated that the toxicity observed was consistent with the amount of radiation delivered to the nucleus. CONCLUSIONS: These results are similar to previous results obtained with B lymphoma cells and indicate that this approach is applicable to a wide range of tumor types. Radionuclides emitting low-energy electrons are effective at killing target cells with relatively little nonspecific toxicity, if sufficient activity is delivered to the cell. Most Abs to high-density cell surface antigens would probably be effective.

Carcinoma, Squamous Cell↗

A novel method for large-area sources preparation for the calibration of beta- and alpha-contamination monitors.

A method is proposed for the preparation of large-area reference sources for the calibration of beta- and alpha-contamination monitors. It is based on the incorporation, by the ion-exchange mechanism, of the radionuclide in a thin film of a conducting polymer ion-exchanger preliminarily grown on a metal support. Conducting pyrrole-based polymer functionalized by carboxylic cation-exchange groups is used to prepare 60Co and 90Sr-90Y beta-particle sources. Electrochemical polymerization of the corresponding monomer on different conducting supports is studied and a special electrochemical equipment developed permitting the preparation of large-area polymer films of controlled and reproducible thickness. The ion-exchanger obtained is characterized in terms of chemical affinity for cations Co2+ and Sr2+. Incorporation of the radionuclides in the large-area ion-exchanger films thus obtained is studied and optimized with respect to the uniform distribution of the radionuclide. The performance of the procedure is demonstrated using the example of circular sources 44 mm in diameter prepared on stainless steel supports. The sources obtained are characterized in terms of activity, beta-particle flux, uniformity and source efficiency.

Journal Article↗

Radioimmunotherapy for model B cell malignancies using 90Y-labeled anti-CD19 and anti-CD20 monoclonal antibodies.

In recent years, radioimmunotherapy (RIT) with beta(-) particle emitting radionuclides targeting the CD20 antigen on B cells in the treatment of non-Hodgkin's lymphoma has provided the most compelling human clinical data for the success of RIT. CD19, like CD20, is an antigen expressed on the surface of cells of the B lineage, and CD19 may provide an alternative target for radioimmunotherapy of B cell neoplasms. CD19 has been largely overlooked as a target for conventional 131I RIT, because the antigen rapidly internalizes upon binding of antibody, resulting in catabolism and significant release of 131I. Such modulation may be an advantage to RIT with radiometals such as 90Y, 177Lu, 213Bi and 225Ac. Herein, we have compared beta(-) particle RIT with antibodies targeting either CD19 or CD20. The anti-CD19 and anti-CD20 antibodies, B4 or C2B8, respectively, were appended with the SCN-CHX-A''-DTPA bifunctional chelating agent and labeled with 90Y. In the tumor model used, there were three times as many CD20 target sites on lymphoma cells as compared to CD19 sites (62000 vs 20000 binding sites, respectively). We compared the efficacy of the 90Y-labeled antibodies to reduce lymphoma in a nude mouse xenograft solid tumor model, after measurable lymphoma appeared. Reduction in tumor size began at day 3 in all three 90Y-treated groups, but tumor began to recur in many animals 9 days after the treatments. There was one cure in each specific treatment group. In contrast, the tumor in the two control groups showed no regression. There was a significant prolongation of median survival time from xenograft (P < 0.0001) in all the 90Y-labeled antibody construct-treated groups (32 days for 0.15 mCi 90Y-B4; 26 days for 0.20 mCi 90Y-C2B8, and 23 days for 0.15 mCi 90Y-C2B8) in comparison to the two control groups (11 days for 0.02 mg of C2B8 and 9 days for untreated growth controls). Specificity of the radioimmunotherapy was also shown. In conclusion, 90Y-labeled anti-CD19 antibody has efficacy comparable to 90Y-labeled anti-CD20 antibody in the treatment of mice bearing human lymphoma xenografts. These data suggest that CD19-targeted RIT merits further study.

Animals↗

The role of nuclear medicine in the treatment of non-Hodgkin's lymphoma (NHL).

The emergence of radioimmunotherapy (RIT) provides a new therapeutic approach in which monoclonal antibodies directed against tumor-specific antigens are used to target therapeutic radioisotopes to sites of disseminated disease. The target cell is eliminated and adjacent tumor cells, to which antibody has not bound, are also killed. To date, 90Y-ibritumomab tiuxetan and 131I-tositumomab are the only FDA-approved, and most extensively studied, radioimmunoconjugates for RIT of non-Hodgkin's lymphoma (NHL). Both 90Y-ibritumomab tiuxetan and 131I-tositumomab utilize an anti-CD20 monoclonal antibody to target radioactivity to malignant B-cells. 90Y-ibritumomab tiuxetan emits pure therapeutic beta radiation, permitting outpatient treatment. The high energy of the beta particles emitted by 90Y (2.3 MeV) achieves a wide-ranging crossfire effect. Approximately 90% of the energy is deposited within 5 mm of the radiation source, which kills not only antibody-bound cells but also neighboring malignant cells within a diameter of up to 12 mm. In addition, the half-life of 90Y matches the in vivo biological half-life of the monoclonal antibody (64 h), with negligible excretion of 90Y in urine. With 90Y-ibritumomab tiuxetan, hematological adverse events correlate with the degree of bone marrow involvement and the bone marrow reserve, rather than with dosimetric parameters, and doses to normal organs and red marrow are well below the accepted limits of 20 Gy to normal organs and 3 Gy to red marrow. A dosing schedule based on patient weight and baseline platelet counts has therefore been developed, and dosimetry is not routinely required. 131I, the isotope used in tositumomab RIT, emits both therapeutic beta radiation and highly penetrating gamma emissions. The lower energy of the beta particles emitted by 131I (0.6 MeV) achieves a crossfire effect of up to 2 mm in diameter, which is used to treat tumors. The gamma radiation emitted by 131I allows both dosimetry and biodistribution studies to be performed; such studies are important because the rate of 131I-tositumomab clearance varies among individuals. Therefore, dosimetry must be performed in each patient before the therapeutic dose of 131I-tositumomab is administered. Similarly, because of this variability in 131I clearance, the dosage of 131I-tositumomab is calculated accordingly for each patient. 131I-tositumomab is a substrate for dehalogenases, which decouple the radioisotope from the antibody moiety, resulting in free, circulating 131I, which can accumulate in the thyroid. Patients who receive 131I-tositumomab therapy are usually hospitalized in radioprotection wards, and are treated by specially trained hospital staff. The administration of RIT requires an integrated team approach, involving nuclear medicine (or, in some countries, radiation oncology), hematology-oncology, nursing, radiopharmacy and radiation safety personnel. Effective collaboration between all members of the RIT team is essential to treatment success, and understanding the properties of these novel agents will facilitate their safe and effective administration.

Antibodies, Monoclonal↗

Bystander cell proliferation is modulated by the number of adjacent cells that were exposed to ionizing radiation.

BACKGROUND: Direct cell-to-cell contact appears to be a prerequisite for the proliferative response of bystander WB-F344 cells co-cultured with irradiated cells; however, neither gap junctional intercellular communication nor long-range factors released into the medium appear to be involved (Cytometry 2003;56A:71-80). The present work investigated whether the proliferative bystander response depends on the number of irradiated cells (cells exposed to external gamma-rays or cells exposed to short-range beta-particles emitted by DNA-incorporated (3)H-thymidine) that are adjacent to unirradiated bystander cells. METHODS: Subconfluent monolayers of rat liver epithelial cells (WB-F344) were incubated in the presence of (methyl-(3)H)thymidine at a concentration of 5.8 kBq/ml for 18 h. Radiolabeled cells containing 0.7 x 10(-3) Bq/cell (absorbed dose: 0.14 Gy) were plated together with unlabeled cells in proportions of 6% and 94%, 12% and 88%, 25% and 75%, 50% and 50%, and 75% and 25%, respectively, keeping constant the total number of plated cells. In a parallel experiment, cells acutely exposed to 5 Gy of (137)Cs gamma-rays were plated with unirradiated cells in the same proportions. In both experiments, cells were co-cultured for 24 h followed by a flow cytometric study of their proliferation. The two cell populations in the co-cultures were distinguished by staining one population with carboxyfluorescein diacetate, succinimidyl ester, which metabolizes intracellularly. RESULTS: Increasing the fraction of irradiated cells relative to unirradiated bystander cells led to an increase in proliferation of bystander cells. Specifically, in co-cultures in which irradiated cells were initially mixed with unirradiated cells in proportions of 50% and 50% and of 75% and 25%, respectively, bystander cells showed a statistically significant increase of their proliferation compared with the controls. CONCLUSIONS: The proliferative response of WB-F344 bystander cells is modulated by the number of adjacent cells that are exposed to ionizing radiation from external gamma-rays or intracellularly emitted (3)H beta-particles.

Animals↗

Marrow-sparing effects of 117mSn(4+)diethylenetriaminepentaacetic acid for radionuclide therapy of bone cancer.

UNLABELLED: Several bone-seeking radionuclides (32P, 89Sr, 186Re, and 153Sm) have been used to treat bone pain. The limiting factor in this modality is marrow toxicity. Our hypothesis is that marrow toxicity can be reduced while maintaining therapeutic efficacy using radionuclides that emit short-range beta particles or conversion electrons (CEs). A recent study on 47 patients using the short-range CE emitter 117mSn(4+)diethylenetriaminepentaacetic acid (117mSn(4+)DTPA) supports this hypothesis. The hypothesis is now tested using 117mSn(4+)DTPA in a mouse femur model. METHODS: The survival of granulocyte-macrophage colony-forming cells (GM-CFCs) in femoral marrow is used as a biologic dosimeter for bone marrow. The dosimeter is calibrated by irradiating mice with exponentially decreasing dose rates of 137Cs gamma-rays with a dose-rate decrease half-time, Td, equal to the effective clearance half-time of 117mSn(4+)DTPA from the femur (222 h). When Td = 222 h, the mean absorbed dose required to achieve a survival fraction of 37% is 151 cGy. After calibration, 117mSn(4+)DTPA is administered and GM-CFC survival is determined as a function of injected activity. These data are used to experimentally determine the mean absorbed dose to the femoral marrow per unit injected activity. The kinetics of radioactivity in the marrow, muscle, and femoral bone are also determined. Finally, a theoretic dosimetry model of the mouse femur is used, and the absorbed doses to the femoral marrow and bone are calculated. RESULTS: The experimental mean absorbed dose to the femoral marrow per unit injected activity of 117mSn(4+)DTPA is 0.043 cGy/kBq. The theoretic mean absorbed dose to the femoral bone per unit injected activity is 1.07 cGy/kBq. If these data are compared with those obtained previously for 32P-orthophosphate, the radiochemical 117mSn(4+)DTPA yields up to an 8-fold therapeutic advantage over the energetic beta emitter 32P. CONCLUSION: The CE emitter 117mSn offers a large dosimetric advantage over energetic beta-particle emitters for alleviating bone pain, and possibly for other therapeutic applications, while minimizing marrow toxicity.

Animals↗

Comparative pathology: radiation-induced coronary artery disease in man and animals.

The occurrence of coronary artery disease following mediastinal radiation for malignancies has long been debated. However, the development of coronary pathology in young individuals following radiation who lack risk factors for atherosclerosis is highly suggestive of a cause-and-effect relationship. By far the most convincing pathologic changes are adventitial scarring and medial atrophy with severe intimal atherosclerotic disease consisting of necrotic core, fibrous tissue, and calcification. Initial clinical studies in patients with coronary atherosclerosis treated with intraluminal radiation following stenting hold great promise in the treatment and prevention of restenosis. There are little or no data, however, on long-term effects of intra-coronary radiation therapy in man. Therefore, it may be important to study the chronic effects of radiation in animal models in order to predict what is likely to occur in humans. We evaluated the effects of varying doses (0.15-23.0 microCi of 32P) of beta-particle-emitting radioactive stents in pig coronary arteries at 1 and 6 months. At 1 month, there were dose-dependent changes in the morphology of the intima and media. High activities (>3 microCi) caused medial necrosis with fibrin deposition in the media and intima, with interspersed red cells most marked in regions surrounding the stent struts. Only rare smooth muscle cells (SMCs) and inflammatory cells were seen away from the stent struts. In the intermediate (1 microCi) stent activity group, the neointima was expanded by SMCs and a proteoglycan-rich matrix with focal endothelialization of the luminal surface. Neovascular capillaries and extravascular red cells were present adjacent to stent struts. At low activities (<0.5 microCi), the neointima was significantly smaller than control stents and consisted of SMCs and matrix with complete endothelialization of the luminal surface. The neointimal cell density of the media and intima decreased with increasing doses of radiation. In pigs 6 months after radioactive stenting (activities ranging from 0.5-12 microCi 32P), >3.0 microCi radioactive stents induced marked neointimal thickening, with changes similar to atherosclerosis, consisting of necrotic debris containing cholesterol clefts surrounded by macrophage collections, fibrosis, and focal calcification. There was increased adventitial thickening in the radiated vs non-radiated arteries. The intermediate stent activity (1.0 microCi) also showed greater neointimal thickening (vs control stents) and consisted mostly of SMCs in a proteoglycan-rich matrix. At <1.0 microCi, there were minimal differences seen between radiated and control non-radiated stented arteries. The media was unevenly injured in all stent activities and varied from less than to significantly greater than controls. These data suggest that radiation-induced coronary atherosclerosis seen in man is partially simulated in normal porcine coronary arteries 6 months following high-dose beta-particle-emitting radioactive stent placement. There is greater fibrosis and thickness of the adventitia and focal attenuation of the media in man and severe luminal narrowing in pig coronary arteries treated with high doses of radiation. Only long-term clinical follow up and careful autopsy studies will determine if endoluminal or intra-arterial radiation is a viable means of reducing restenosis in man.

Animals↗

Supramolecular Structure of Precipitated Nanosize beta-Carotene Particles.

A combination of analytical methods and molecular modeling calculations has provided a detailed picture of the supramolecular and microscopic structure of precipitated lipophilic carotenoids. The nanoparticles have a core/shell structure (see schematic representation) in which the particle core (120 nm) consists of a variety of molecular aggregates of different sizes, and the shell (40 nm) consists of an adsorbed gelatin layer.

Journal Article↗

Investigations of electron helicity in optically active molecules using polarized beams of electrons and positrons.

We will discuss one possible correlation between the origin of optical activity in biological molecules and the helicity of beta particles emitted in nuclear beta decay. This correlation is based on the supposition of Hrasko and Garay that electrons in optically active molecules possess helicity. Positronium formation experiments are significantly more sensitive to this particular effect than radiolysis experiments although no experiments of any type to date have obtained the sensitivity that our preliminary calculations indicate is necessary. We discuss a new experiment in which positronium is formed in vacuum with a low energy polarized positron beam. An improvement of up to 10(4) in sensitivity to the effect is possible.

Electrons↗

Incorporation of [3H]2-deoxyglucose into glycogen in nervous tissues.

Mice were injected with [3H]2-deoxyglucose and after 1 h high molecular weight glycogen was extracted from brain, liver and muscle tissues. 1-2% of the total radioactivity in each tissue was recovered in the glycogen fraction. Isolated buccal ganglia of the pond snail, Planorbis, and isolated abdominal ganglia of the horse leech Haemopis, were exposed in vitro to [3H]2-deoxyglucose for 1 h. 1-10% of the total radioactivity in these tissues was located in the high molecular weight glycogen fraction. Treatment of the extracted labelled glycogen fractions with amyloglucosidase caused release of the label in a manner consistent with the breakdown of labelled glycogen. Ganglia of snail and leech were exposed to [3H]2-deoxyglucose, fixed in glutaraldehyde and osmium tetroxide solutions, and prepared for autoradiography using aqueous histological processing. Light and electron microscope autoradiography showed that over 90% of the label was positively associated with glycogen particles (alpha- and beta-particles). Certain previously published reports on the incorporation of 2-deoxyglucose into glycogen are discussed in relation to these findings. It is concluded that [3H]2-deoxyglucose is partially incorporated into glycogen in nervous tissue; the labelled 2-deoxyglycogen withstands aqueous histological processing and can be visualized directly by autoradiography.

Animals↗