11 research outputs found

    Modeling of gamma-pulse propagation in the "optical" thick medium with inverted population of the nuclear levels of 178Hf isotope

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    The nuclear superfluorescence in the "optical" medium with 178Hf in propagation channel has been modeled. The general equations system describing the nuclear superfluorescence in the "optical" medium has obtained. The numerical simulation in the propagation channel in the "optical" thick medium with Hf has been made

    Modeling of gamma-avalanche formation in the "optical" thick medium with 178Hf through the nuclear diffraction channel

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    The formation of Ξ³-avalanche in the medium with 178Hf isotope has modeled through the nuclear diffraction channel. The equation system describing the process under two-wave Bragg diffraction conditions has obtained. The numerical simulation for the "optical" thick medium has been made

    Modeling of gamma-avalanche formation in the "optical" thick medium with 178Hf through the nuclear diffraction channel

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    The formation of Ξ³-avalanche in the medium with 178Hf isotope has modeled through the nuclear diffraction channel. The equation system describing the process under two-wave Bragg diffraction conditions has obtained. The numerical simulation for the "optical" thick medium has been made

    Modeling of gamma-pulse propagation in the "optical" thick medium with inverted population of the nuclear levels of 178Hf isotope

    No full text
    The nuclear superfluorescence in the "optical" medium with 178Hf in propagation channel has been modeled. The general equations system describing the nuclear superfluorescence in the "optical" medium has obtained. The numerical simulation in the propagation channel in the "optical" thick medium with Hf has been made

    Modeling of gamma-avalanche formation in the "optical" thick medium with 178Hf through the nuclear diffraction channel

    No full text
    The formation of Ξ³-avalanche in the medium with 178Hf isotope has modeled through the nuclear diffraction channel. The equation system describing the process under two-wave Bragg diffraction conditions has obtained. The numerical simulation for the "optical" thick medium has been made

    Modeling of gamma-avalanche formation in the "optical" thick medium with 178Hf through the nuclear diffraction channel

    No full text
    The formation of Ξ³-avalanche in the medium with 178Hf isotope has modeled through the nuclear diffraction channel. The equation system describing the process under two-wave Bragg diffraction conditions has obtained. The numerical simulation for the "optical" thick medium has been made

    Modeling of gamma-pulse propagation in the "optical" thick medium with inverted population of the nuclear levels of 178Hf isotope

    Get PDF
    The nuclear superfluorescence in the "optical" medium with 178Hf in propagation channel has been modeled. The general equations system describing the nuclear superfluorescence in the "optical" medium has obtained. The numerical simulation in the propagation channel in the "optical" thick medium with Hf has been made

    Modeling of gamma-pulse propagation in the "optical" thick medium with inverted population of the nuclear levels of 178Hf isotope

    No full text
    The nuclear superfluorescence in the "optical" medium with 178Hf in propagation channel has been modeled. The general equations system describing the nuclear superfluorescence in the "optical" medium has obtained. The numerical simulation in the propagation channel in the "optical" thick medium with Hf has been made

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    ThΠ΅ expression of the vascular endothelial growth factor and neoangiogenesis in experimental cerebral ischemia in conditions of combined use of erythropoietin and laser radiation

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    The work was performed on 120 white non-linear rats. The cerebral cortex ischemia (CΠ‘I) was induced by diathermocoagulation of the pial vessels in the sensomotor zone of the cerebral cortex. Erythropoietin (EPO) was used intraperitoneally at a total dose of 15,000 IU/ kg, laser radiation (LR) - once to the area of the ischemic focus (970 nm, 2 min). The number of small blood vessels was counted and an expression of the vascular endothelial growth factor (VEGF) was determined in the ischemic focus. In case of CCI the expression of VEGF increases and the number of small blood vessels decreases in the ischemic focus on days 3, 7, 14, and 30. The use of EPO in CCI increases the number of small blood vessels, LR increases an expression of VEGF and the number of small blood vessels on the 3, 7, 14, 30 days of the experiment; the quantity of blood vessels is higher after exposure of LR as compared with the use of EPO. The maximal expression of VEGF and the number of small blood vessels in CCI are revealed after the combined use of EPO and LR.Π Π°Π±ΠΎΡ‚Π° Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Π° Π½Π° 120 Π±Π΅Π»Ρ‹Ρ… Π½Π΅Π»ΠΈΠ½Π΅ΠΉΠ½Ρ‹Ρ… крысах. ИшСмию ΠΊΠΎΡ€Ρ‹ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π° (Π˜ΠšΠ“Πœ) создавали ΠΏΡƒΡ‚Π΅ΠΌ диатСрмокоагуляции ΠΏΠΈΠ°Π»ΡŒΠ½Ρ‹Ρ… сосудов Π² сСнсомоторной Π·ΠΎΠ½Π΅. Эритропоэтин (ЭПО) примСняли Π²Π½ΡƒΡ‚Ρ€ΠΈΠ±Ρ€ΡŽΡˆΠΈΠ½Π½ΠΎ Π² суммарной Π΄ΠΎΠ·Π΅ 15000 МС/ΠΊΠ³, Π»Π°Π·Π΅Ρ€Π½ΠΎΠ΅ ΠΈΠ·Π»ΡƒΡ‡Π΅Π½ΠΈΠ΅ (Π›Π˜) - ΠΎΠ΄Π½ΠΎΠΊΡ€Π°Ρ‚Π½ΠΎ Π½Π° ΠΎΠ±Π»Π°ΡΡ‚ΡŒ ΠΈΡˆΠ΅ΠΌΠΈΡ‡Π΅ΡΠΊΠΎΠ³ΠΎ ΠΎΡ‡Π°Π³Π° (970 Π½ΠΌ, 2 ΠΌΠΈΠ½). Π’ ΠΎΡ‡Π°Π³Π΅ ишСмии подсчитывали количСство ΠΌΠ΅Π»ΠΊΠΈΡ… кровСносных сосудов, опрСдСляли ΡΠΊΡΠΏΡ€Π΅ΡΡΠΈΡŽ Ρ„Π°ΠΊΡ‚ΠΎΡ€Π° роста эндотСлия сосудов (VEGF). ΠŸΡ€ΠΈ Π˜ΠšΠ“Πœ Π² ΠΎΡ‡Π°Π³Π΅ ишСмии ΠΏΠΎΠ²Ρ‹ΡˆΠ°Π΅Ρ‚ΡΡ экспрСссия VEGF ΠΈ сниТаСтся количСство ΠΌΠ΅Π»ΠΊΠΈΡ… кровСносных сосудов Π½Π° 3, 7, 14, 30 сутки. ΠŸΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΏΡ€ΠΈ Π˜ΠšΠ“Πœ ЭПО ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΡŽ количСства ΠΌΠ΅Π»ΠΊΠΈΡ… кровСносных сосудов, воздСйствиС Π›Π˜ - ΠΊ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΡŽ экспрСссии VEGF ΠΈ количСства ΠΌΠ΅Π»ΠΊΠΈΡ… кровСносных сосудов Π½Π° 3, 7, 14, 30 сутки экспСримСнта; ΠΏΡ€Π΅Π΄ΡΡ‚Π°Π²ΠΈΡ‚Π΅Π»ΡŒΡΡ‚Π²ΠΎ кровСносных сосудов Π²Ρ‹ΡˆΠ΅ послС воздСйствия Π›Π˜ ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ЭПО. Максимальная экспрСссия VEGF ΠΈ количСство ΠΌΠ΅Π»ΠΊΠΈΡ… кровСносных сосудов ΠΏΡ€ΠΈ Π˜ΠšΠ“Πœ выявлСны послС ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ примСнСния ЭПО ΠΈ Π›Π˜
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