| Literature DB >> 22937232 |
Martine M Mirrione1, Stella E Tsirka.
Abstract
Small animal neuroimaging has become increasingly available to researchers, expanding the breadth of questions studied with these methods. Applying these noninvasive techniques to the open questions underlying epileptogenesis is no exception. A major advantage of small animal neuroimaging is its translational appeal. Studies can be well controlled and manipulated, examining the living brain in the animal before, during, and after the disease onset or disease treatment. The results can also be compared to data collected on human patients. Over the past decade, we and others have explored metabolic patterns in animal models of epilepsy to gain insight into the circuitry underlying development of the disease. In this paper, we provide technical details on how metabolic imaging that uses 2-deoxy-2[(18)F]fluoro-D-glucose ((18)FDG) and positron emission tomography (PET) is performed and explain the strengths and limitations of these studies. We will also highlight recent advances toward understanding epileptogenesis through small animal imaging.Entities:
Year: 2011 PMID: 22937232 PMCID: PMC3420690 DOI: 10.1155/2011/369295
Source DB: PubMed Journal: Epilepsy Res Treat ISSN: 2090-1348
Figure 1Schematic of 18FDG-PET imaging principles. (a) 18FDG production step 1: 18O enriched water (95%) is bombarded with protons in a cyclotron creating 18-flouride (18F) which is purified on a resin column and rinsed with potassium carbonate. Step 2: 18F is added with Kryptofix2.2.2 to the precursor glucose starting material and through a nucleophilic substitution, subsequent purification and removal of protecting groups, 18FDG is synthesized. (b) The radiotracer accumulates in tissue where it is transported into metabolically active cells, metabolized by hexokinase, and trapped as FDG-6-phosphate, as it is not a good substrate for further metabolism by glucose phosphate isomerase (GPI). (c) Representation of a mouse in the field of view of a small animal PET camera. When the 18F on a molecule of 18FDG undergoes beta decay, a proton turns into a neutron expelling a positron and neutrino from the atomic nucleus. The positron travels up to a few millimeters before it collides with an electron (inset). The energy of this annihilation expels 2 511 keV gamma rays (γ) approximately 180° apart from each other. These γ rays are detected simultaneously by a ring of LSO crystals that make up the PET camera.