19 research outputs found

    ИсслСдованиС ΠΊΠ°Π½Π°Π»ΡŒΠ½Ρ‹Ρ… Π±Π»ΠΎΠΊΠ°Ρ‚ΠΎΡ€ΠΎΠ² NMDA Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€Π° Π² ряду ΠΊΠΎΠ½ΡŠΡŽΠ³Π°Ρ‚ΠΎΠ² ΠΌΠ΅Ρ‚ΠΈΠ»Π΅Π½ΠΎΠ²ΠΎΠ³ΠΎ синСго с использованиСм QSAR ΠΈ молСкулярного модСлирования

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    29 conjugates of methylene blue and four chemical structures, including derivatives of carbazole, tetrahydrocarbazole, substituted indoles and Ξ³-carboline, combined with a 1-oxopropylene spacer have been studied as channel blockers of the NMDA receptor (binding site of MK-801) by using four QSAR methods (multiple linear regression, random forest, support vector machine, Gaussian process) and molecular docking. QSAR models have satisfactory characteristics. The analysis of regression models at the statistical level revealed an important role of the hydrogen bond in the complex formation. This was also confirmed by the study of modeled by docking complexes. It was found that the increase in the inhibitory activity of the part of compounds could be attributed to appearance of additional H bonds between the ligands and the receptor.Π‘ использованиСм 4-Ρ… ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² QSAR (мноТСствСнная линСйная рСгрСссия, случайный лСс, ΠΌΠ΅Ρ‚ΠΎΠ΄ ΠΎΠΏΠΎΡ€Π½Ρ‹Ρ… Π²Π΅ΠΊΡ‚ΠΎΡ€ΠΎΠ², гауссовский процСсс) ΠΈ молСкулярного Π΄ΠΎΠΊΠΈΠ½Π³Π° исслСдованы Π² качСствС Π±Π»ΠΎΠΊΠ°Ρ‚ΠΎΡ€ΠΎΠ² NMDA Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€Π° (сайт связывания МК-801) 29 ΠΊΠΎΠ½ΡŠΡŽΠ³Π°Ρ‚ΠΎΠ² ΠΌΠ΅Ρ‚ΠΈΠ»Π΅Π½ΠΎΠ²ΠΎΠ³ΠΎ синСго ΠΈ Ρ‡Π΅Ρ‚Ρ‹Ρ€Π΅Ρ… Ρ‚ΠΈΠΏΠΎΠ² соСдинСний, Π²ΠΊΠ»ΡŽΡ‡Π°Ρ ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Π΅ ΠΊΠ°Ρ€Π±Π°Π·ΠΎΠ»Π°, Ρ‚Π΅Ρ‚Ρ€Π°Π³ΠΈΠ΄Ρ€ΠΎΠΊΠ°Ρ€Π±Π°Π·ΠΎΠ»Π°, Π·Π°ΠΌΠ΅Ρ‰Π΅Π½Π½Ρ‹Ρ… ΠΈΠ½Π΄ΠΎΠ»ΠΎΠ² ΠΈ Ξ³-ΠΊΠ°Ρ€Π±ΠΎΠ»ΠΈΠ½Π°, ΠΎΠ±ΡŠΠ΅Π΄ΠΈΠ½Π΅Π½Π½Ρ‹Ρ… 1-оксопропилСновым спСйсСром. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ QSAR ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈΠΌΠ΅ΡŽΡ‚ ΡƒΠ΄ΠΎΠ²Π»Π΅Ρ‚Π²ΠΎΡ€ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ характСристики. На основС Π°Π½Π°Π»ΠΈΠ·Π° рСгрСссионных ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ Π½Π° статистичСском ΡƒΡ€ΠΎΠ²Π½Π΅ выявлСна ваТная Ρ€ΠΎΠ»ΡŒ Π²ΠΎΠ΄ΠΎΡ€ΠΎΠ΄Π½ΠΎΠΉ связи ΠΏΡ€ΠΈ Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠΈ комплСкса. Π­Ρ‚ΠΎ нашло ΠΏΠΎΠ΄Ρ‚Π²Π΅Ρ€ΠΆΠ΄Π΅Π½ΠΈΠ΅ ΠΏΡ€ΠΈ исслСдовании ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ комплСксов, ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… молСкулярным Π΄ΠΎΠΊΠΈΠ½Π³ΠΎΠΌ. УстановлСно, Ρ‡Ρ‚ΠΎ ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΠ΅ ΠΈΠ½Π³ΠΈΠ±ΠΈΡ€ΡƒΡŽΡ‰Π΅ΠΉ способности части исслСдуСмых соСдинСний обусловлСно появлСниСм Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… Н-связСй ΠΌΠ΅ΠΆΠ΄Ρƒ Π»ΠΈΠ³Π°Π½Π΄Π°ΠΌΠΈ ΠΈ Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€ΠΎΠΌ

    Investigation of the prompt neutron emission mechanism in low energy fission of

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    A series of experiments has been performed to measure prompt neutron angular and energy distributions from thermal neutron-induced fission of 235,233U in correlation with the fission fragments. These distributions have been analyzed with the assumption of neutron isotropic emission from accelerated fission fragments. The performed analysis demonstrates that all obtained results can be described within 5% accuracy using this assumption. This discrepancy is approximately constant and doesn’t depend on fragment mass and the total kinetic energy (TKE). Some minor peculiarities of angular distribution may be interpreted as a result of anisotropy of the fission neutron angular distribution in the fragment center-of-mass system

    Investigation of the prompt neutron emission mechanism in low energy fission of 235,233U(nth, f) and 252Cf(sf)

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    A series of experiments has been performed to measure prompt neutron angular and energy distributions from thermal neutron-induced fission of 235,233U in correlation with the fission fragments. These distributions have been analyzed with the assumption of neutron isotropic emission from accelerated fission fragments. The performed analysis demonstrates that all obtained results can be described within 5% accuracy using this assumption. This discrepancy is approximately constant and doesn’t depend on fragment mass and the total kinetic energy (TKE). Some minor peculiarities of angular distribution may be interpreted as a result of anisotropy of the fission neutron angular distribution in the fragment center-of-mass system

    Angular distributions and anisotropy of fission fragments from neutron-induced fission of 239Pu, 237Np, and natPb in energy range 1–200 MeV

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    This work summarizes some results of a series of experiments aimed at the investigation of energy dependence of anisotropy of fission fragments (FFs) in (n, f) reactions for neutron energies from low to intermediate. Angular distributions of FFs from the neutron-induced fission of 239Pu, 237Np, and natPb have been measured in the energy range 1–200 MeV at the neutron TOF spectrometer GNEIS based on the spallation neutron source at 1 GeV proton synchrocyclotron of the Petersburg Nuclear Physics Institute (Gatchina, Russia). The anisotropies of FFs deduced from the measured angular distributions are presented. In the neutron energy range above 20 MeV the results have been obtained for the first time in our works. The experimental data for FF anisotropy in 237Np(n, f) are compared with calculations based on "adapted" TALYS software

    Angular distributions and anisotropy of fission fragments from neutron-induced fission of

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    This work summarizes some results of a series of experiments aimed at the investigation of energy dependence of anisotropy of fission fragments (FFs) in (n, f) reactions for neutron energies from low to intermediate. Angular distributions of FFs from the neutron-induced fission of 239Pu, 237Np, and natPb have been measured in the energy range 1–200 MeV at the neutron TOF spectrometer GNEIS based on the spallation neutron source at 1 GeV proton synchrocyclotron of the Petersburg Nuclear Physics Institute (Gatchina, Russia). The anisotropies of FFs deduced from the measured angular distributions are presented. In the neutron energy range above 20 MeV the results have been obtained for the first time in our works. The experimental data for FF anisotropy in 237Np(n, f) are compared with calculations based on "adapted" TALYS software

    Mass, Kinetic Energy and Neutron Emission of Fragments in Spontaneous Fission 252Cf, 244Cm, 248Cm.

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    Abstract not availableJRC.D-Institute for Reference Materials and Measurements (Geel
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