Gene/Protein Disease Symptom Drug Enzyme Compound
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Query: UNIPROT:P00492 (hypoxanthine-guanine phosphoribosyltransferase)
 2,385 document(s) hit in 31,850,051 MEDLINE articles (0.00 seconds)

Dense ionization tracks from high linear energy transfer (LET) radiations form multiple damaged sites (MDS), which involve several types of DNA lesions in close vicinity. The primary DNA damage triggers sensor proteins that activate repair processes, cell cycle control or eventually apoptosis in subsequent cellular responses. The question how homologous recombination (HR) and non-homologous end joining (NHEJ) interact in the repair of radiation-induced DNA damage of MDS type has been addressed in different model systems but several questions remain to be answered. We have therefore challenged cells with treatments of ionizing radiation of different qualities to investigate whether primary DNA damages of different complexity are reflected in the processes of repair by HR as well as cell survival. We used the V79 derived SPD8 cell line to determine the induction of HR in the hprt exon 7 and clonogenic assay for survival in response to radiation. SPD8 cells were irradiated with gamma-rays (137Cs 0.5 keV/microm), boron ions (40 and 80 keV/microm) and nitrogen ions (140 keV/microm), with doses up to 5 Gy. Analysis of clonogenic survival showed that B-ions (80 keV/microm) and N-ions were more toxic than gamma-rays, 4.1 and 5.0 times respectively, while B-ions at 40 keV/microm were 2.0 times as toxic as gamma-rays. Homologous recombination in the cells exposed to B-ions (80 keV/microm) increased 2.9 times, a significant response as compared to cells exposed to gamma-rays, while for B-ions (40 keV/microm) and N-ions a nonsignificant increase in HR of 1.2 and 1.4, respectively, was observed. We hypothesize that the high-LET generated formation of MDS is responsible for the enhanced cytotoxicity as well as for the mobilization of the HR machinery.
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PMID:Induction of homologous recombination in the hprt gene of V79 Chinese hamster cells in response to low- and high-LET irradiation. 1516 43

To investigate bystander mutagenic effects induced by alpha particles during boron neutron capture therapy (BNCT), we mixed cells that were electroporated with borocaptate sodium (BSH), which led to the accumulation of (10)B inside the cells, with cells that did not contain the boron compound. BSH-containing cells were irradiated with alpha particles produced by the (10)B(n,alpha)(7)Li reaction, whereas cells without boron were only affected by the (1)H(n,gamma)(2)H and (14)N(n,rho)(14)C reactions. The frequency of mutations induced in the hypoxanthine-guanine phosphoribosyltransferase (HPRT) locus was examined in Chinese hamster ovary (CHO) cells irradiated with neutrons (Kyoto University Research Reactor: 5 MW). Neutron irradiation of 1:1 mixtures of cells with and without BSH resulted in a survival fraction of 0.1, and the cells that did not contain BSH made up 99.4% of the surviving cell population. Using multiplex polymerase chain reactions (PCRs), molecular structural analysis indicated that most of the mutations induced by the bystander effect were point mutations and that the frequencies of total and partial deletions induced by the bystander effect were lower than those resulting from the alpha particles produced by the (10)B(n,alpha)(7)Li reaction or the neutron beam from the (1)H(n,gamma)(2)H and (14)N(n,rho)(14)C reactions. The types of point mutations induced by the BNCT bystander effect were analyzed by cloning and sequencing methods. These mutations were comprised of 65.5% base substitutions, 27.5% deletions, and 7.0% insertions. Sequence analysis of base substitutions showed that transversions and transitions occurred in 64.7% and 35.3% of cases, respectively. G:C-->T:A transversion induced by 8-oxo-guanine in DNA occurred in 5.9% of base substitution mutants in the BNCT bystander group. The characteristic mutations seen in this group, induced by BNCT alpha particles, differed from those typical of gamma ray radiation.
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PMID:Bystander effect-induced mutagenicity in HPRT locus of CHO cells following BNCT neutron irradiation: characteristics of point mutations by sequence analysis. 1937 34

Based on experiments and numerical simulations, a study is carried out pertaining to the conversion of dose-to-graphite to dose-to-water in a carbon ion beam. This conversion is needed to establish graphite calorimeters as primary standards of absorbed dose in these beams. It is governed by the water-to-graphite mass collision stopping power ratio and fluence correction factors, which depend on the particle fluence distributions in each of the two media. The paper focuses on the experimental and numerical determination of this fluence correction factor for an 80 MeV/A carbon ion beam. Measurements have been performed in the nuclear physics laboratory INFN-LNS in Catania (Sicily, Italy). The numerical simulations have been made with a Geant4 Monte Carlo code through the GATE simulation platform. The experimental data are in good agreement with the simulated results for the fluence correction factors and are found to be close to unity. The experimental values increase with depth reaching 1.010 before the Bragg peak region. They have been determined with an uncertainty of 0.25%. Different numerical results are obtained depending on the level of approximation made in calculating the fluence correction factors. When considering carbon ions only, the difference between measured and calculated values is maximal just before the Bragg peak, but its value is less than 1.005. The numerical value is close to unity at the surface and increases to 1.005 near the Bragg peak. When the fluence of all charged particles is considered, the fluence correction factors are lower than unity at the surface and increase with depth up to 1.025 before the Bragg peak. Besides carbon ions, secondary particles created due to nuclear interactions have to be included in the analysis: boron ions ((10)B and (11)B), beryllium ions ((7)Be), alpha particles and protons. At the conclusion of this work, we have the conversion of dose-to-graphite to dose-to-water to apply to the response of a graphite calorimeter in an 80 MeV/A carbon ion beam. This conversion consists of the product of two contributions: the water-to-graphite electronic mass collision stopping power ratio, which is equal to 1.115, and the fluence correction factor which varies linearly with depth, as k(fl, all) = 0.9995 + 0.0048(zw-eq). The latter has been determined on the basis of experiments and numerical simulations.
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PMID:Conversion from dose-to-graphite to dose-to-water in an 80 MeV/A carbon ion beam. 2387 66