Biodistribution and kinetics of 67Ga- β-neurotoxin using SPECT molecular imaging
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چکیده
At least venomous snake bites 2000 persons each year in US. The severity of envenomation depends of the snake specie, its size, location of the bite and quantity of venom injected; but also depends of the health of the victim, age, size, and the time it takes to receive medical care. The envenomation is a medical emergency that requires fast attention to avoiding fatalities; in this sense, knowledge about distribution and kinetics of venom is valuable information that significantly helps to clinicians for treating it. The main reported method for detecting and quantify venom or isolated toxins, in experimental envenomation, is the immunoassay ELISA. However, it has some limitations; for example, it needs significant volume of blood for quantitation, requires to sacrifice the animal to obtain organs and tissues, and sometimes the quantification is not possible due to the integrity of the antigen was lost during procedures of extraction from tissues. Biodistribution study of toxins and venoms by radiolabeling molecular imaging presents several advantages such as: 1) allows the tracking of toxins in blood for long in the same alive animal, reducing the number of animals used in each experiment; 2) permits to measure the accumulation in organs at different times without sacrifice the animal; 3) the distribution by lymphatic system, which is a common route for distribution of snake toxins, can easily distinguished. Radiolabeling molecular imaging techniques are powerful tools for studying physiological processes on a cellular level as well as biodistribution and kinetics of radiolabeled biomarkers proposed for diagnostic and therapy. Imaging modalities can be distinguished based on whether they are structural (CT and MRI) or functional imaging techniques (SPECT and PET) [1]. Single Photon Emission Computed Tomography (SPECT) uses radioactive tracers and a radiation detector scanner with specific performance to localize (radio)activity distribution within the body that a computer constructs into twoor three-dimensional images; this information is used to detect a physiological abnormality or to track the kinetics of radiolabeled molecules in vivo and in real time. Principal radionuclides routinely employed for SPECT imaging include the gamma emitters 99mTc, 111In, 67Ga and 131I. In the field of toxinology, significant efforts have been done to study the pharmacokinetics (PK) and the envenoming development caused by snake venoms. In order to determine the PK of venoms or isolated toxins some researchers have took advantage of radiolabeling techniques, especially by radioiodination. In 1997 Riviere et al., performed an elegant experiment in order to improve the antivenom therapy. They analyze the PK of the Vipera aspis venom radiolabeled with 125I and its modification in presence of the antivenom; their results made a great contribution in the field of toxinology providing invaluable information to design and improve the antivenom therapy. Unfortunately, incomplete knowledge still exists with regarding to absorption, biodistribution and elimination of most of venoms or isolated toxins. Several works have reported the radiolabeling of isolated toxins or complete venoms using 99mTc, which is the most common radionuclide employed in molecular imaging; for instance, the tityustoxin from the scorpion Tityus serrulatus, a bee venom and the Crotalus durissus terrificus snake venom; all of them with successful results [2-4]. By considering that antivenoms are essentially antibodies or their fragments, they also could be radiolabeled on the same way that some therapeutic antibodies used in radioimmunotherapy of cancer and used to evaluate its behavior in the presence of the venom. We recently reported the use of 67Ga to radiolabeling a β-neurotoxin (β-NTx) from venom of the eastern coral snake Micrurus fulvius and its biodistribution by SPECT molecular imaging [5]. The 67Ga is an excellent radionuclide for long-time tracking of β-NTx, since it has a large half-life time (3.2 days) and emits three main gamma energies (93.3, 184.6 and 300.2 keV) that are suitable for SPECT imaging; its cost and availability, as compared with 111In, a radionuclide with 2.8 days halfIrene Vergara-Bahena1 & Luis Alberto Medina*1,2
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