| Literature DB >> 12721514 |
Georges Vassaux, Thomas Groot-Wassink.
Abstract
Gene therapy is reaching a stage where some clinical benefits have been demonstrated on patients involved in phase I/II clinical trials. However, in many cases, the clinical benefit is hardly measurable and progress in the improvement of gene therapy formulations is hampered by the lack of objective clinical endpoints to measure transgene delivery and to quantitate transgene expression. However, these endpoints rely almost exclusively on the analysis of biopsies by molecular and histopathological methods. These methods provide only a limited picture of the situation. Therefore, there is a need for a technology that would allow precise, spacio-temporal measurement of gene expression on a whole body scale upon administration of the gene delivery vector. In the field of gene therapy, a considerable effort is being invested in the development of noninvasive imaging of gene expression and this review presents the various strategies currently being developed.Entities:
Year: 2003 PMID: 12721514 PMCID: PMC323954 DOI: 10.1155/S1110724303209050
Source DB: PubMed Journal: J Biomed Biotechnol ISSN: 1110-7243
Figure 1General principles of biological imaging. (a) Enzymes as reporter genes; upon expression of the reporter gene, the imaging marker (M) that can freely cross the plasmic membrane is metabolised within the cell (the most commonly used enzymatic reaction is a phosphorylation). As a result, the phosphorylated marker becomes incapable of recrossing the plasmic membrane and is trapped within the cell. (b) Receptors as reporter genes; upon expression of the reporter gene, the imaging ligand (L) binds to its receptor, resulting in the accumulation of the detectable ligand in the transduced tissue. This signal can be amplified when the receptor gets internalised. (c) Transporter as reporter genes; upon expression of the transporter, the imaging compound (C) is selectively transported into the cell where it concentrates. Depending on its nature, the imaging tracer is either trapped into the cell, or released when the extracellular concentration decreases (question mark), leading to a transient signal.
Reporter genes and corresponding probes for in vivo imaging.
| Reporter genes | Mechanism | Imaging agents | Imaging | References |
| Cytosine deaminase | Deamination | 5-[19F]fluorocytosine | MRS | [ |
| HSV1- | Phosphorylation | [131I]FIAU, [131I]FIAU | SPECT, gamma camera | [ |
| [124I]FIAU | PET | [ | ||
| [123/125I]FIAU | Gamma camera | [ | ||
| [14C]GCV, [3H]GCV | Autoradiography | [ | ||
| [18F]GCV | PET | [ | ||
| [18F]PCV | PET | [ | ||
| [18F]FHPG | PET | [ | ||
| [18F]FHBG | PET | [ | ||
| HSV1-sr39 | Phosphorylation | [18F]PCV, [18F]FHBG | PET | [ |
| D2R | Receptor-ligand | [18F]FESP | PET | [ |
| Mutant D2R | Receptor-ligand | [18F]FESP | PET | [ |
| Somatostatin receptor | Affinity binding | [111In]DTPA-D-Phe1-octreotide | Gamma camera | [ |
| [64Cu]-TETA-octreotide | Tissue dose counting | [ | ||
| [188Re]-somatostatin analogue, 99mTc somatostatin analogue | Gamma camera | [ | ||
| Na/I symporter | Active transport | [131I], [123I] | Gamma camera | [ |
| PET | [ | |||
| Luciferase | Luciferin reaction | Bioluminescence | CCD camera | [ |
| Cathepsin D | Quenched fluorochromes | Fluorescence activation | CCD camera | [ |
| Metalloproteinase | Quenched fluorochromes | Fluorescence activation | CCD camera | [ |
| Hydrolysis of | EgadMe | MRI | [ | |
| Mutated transferrin receptor | Receptor-ligand | Tf-MION | MRI | [ |
| Creatine kinase | Dephosphorylation | Phosphocreatine | MRS | [ |
| Arginine kinase | Dephosphorylation | Phosphoarginine | MRS | [ |
Figure 2Imaging of hNIS expression by PET. Individual coronal slices from PET images of two nude mice intravenously treated with 5 × 107 GFU adenovirus in which a CMV promoter drives hNIS expression (left) and a PBS-treated control (right) followed, 72 hours later, by injection of [124I] iodide as a tracer. In both pictures, the chosen slice lies at the level of the thyroid region (T). Tracer is seen in the stomach (S) and in the bladder (B) of the control animal. Tracer uptake in the treated animal is in the upper abdomen consistent with adenoviral homing to the liver (for detailed experimental conditions, see [69]).
Comparison between SPECT and PET.
| Method | Advantages | Disadvantages | In vivo animal use | Clinical use | |
| SPECT | - resolution limited by technology only (submillimeter) | - 2D (planar images) and reconstructed 3D | - converted clinical cameras (pinhole collimator) | - readily available and in widespread use | |
| - low sensitivities | - semiquantitative data only | - dedicated cameras evolving | - wide range of clinically tested traces | ||
| - can differentiate between isotopes with different radiation energies | |||||
| PET | - high sensitivity | - short-lived isotopes | currently evolving: | - [18F]FDG becoming routine in oncology | |
| - 3D acquisition | - isotopes produced in cyclotrons | - microPET | - special applications in neurology and cardiology | ||
| - good resolution, but with a physical limit | - expensive tracer production | ||||
| - quantification possible | - expensive equipment | ||||
| - higher tissue doses, but balanced by higher sensitivity | |||||
Figure 3(a) A positron and a neutrino are released when a proton becomes a neutron. (b) Two annihilation photons travel away from each other at 180± 0.25°. (c) The scanner records simultaneous events within a 10–80 ns time window. These are from true coincidences, scattered coincidences, and random coincidences from independent annihilation events. Single events are not processed further (see [77]).
Energy and half-life characteristics of selected positron-emitting isotopes.
| Isotope | Half-life | Maximum positron | Maximum range | Spatial resolution | Radiation dose with |
| 18F | 109 min | 0.63 MeV | 2.6 mm | 0.22 mm | 0.049 mSv/MBq |
| 11C | 20 min | 0.96 MeV | 4.2 mm | 0.28 mm | 0.024 mSv/MBq |
| 13N | 9.9 min | 1.2 MeV | 5.4 mm | 0.35 mm | n/a |
| 15O | 122 s | 1.74 MeV | 8.4 mm | 1.22 mm | n/a |
| 82Rb | 1.3 min | 3.15 MeV | 17.1 mm | 2.6 mm | n/a |
| 124I | 4.2 d | 2.14 MeV | ∼ 1.5 mm | 13 mSv/MBq | |
| 64Cu | 12.7 h | 3.3 MeV | 0.12 mSv/MBq | ||
| 120I | 81 min | 5.6 MeV | n/a | ||