11 research outputs found
Modeling of gamma-pulse propagation in the "optical" thick medium with inverted population of the nuclear levels of 178Hf isotope
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
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
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
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
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
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
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
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
ThΠ΅ expression of the vascular endothelial growth factor and neoangiogenesis in experimental cerebral ischemia in conditions of combined use of erythropoietin and laser radiation
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±ΠΎΡΠ° Π²ΡΠΏΠΎΠ»Π½Π΅Π½Π° Π½Π° 120 Π±Π΅Π»ΡΡ
Π½Π΅Π»ΠΈΠ½Π΅ΠΉΠ½ΡΡ
ΠΊΡΡΡΠ°Ρ
. ΠΡΠ΅ΠΌΠΈΡ ΠΊΠΎΡΡ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π° (ΠΠΠΠ) ΡΠΎΠ·Π΄Π°Π²Π°Π»ΠΈ ΠΏΡΡΠ΅ΠΌ Π΄ΠΈΠ°ΡΠ΅ΡΠΌΠΎΠΊΠΎΠ°Π³ΡΠ»ΡΡΠΈΠΈ ΠΏΠΈΠ°Π»ΡΠ½ΡΡ
ΡΠΎΡΡΠ΄ΠΎΠ² Π² ΡΠ΅Π½ΡΠΎΠΌΠΎΡΠΎΡΠ½ΠΎΠΉ Π·ΠΎΠ½Π΅. ΠΡΠΈΡΡΠΎΠΏΠΎΡΡΠΈΠ½ (ΠΠΠ) ΠΏΡΠΈΠΌΠ΅Π½ΡΠ»ΠΈ Π²Π½ΡΡΡΠΈΠ±ΡΡΡΠΈΠ½Π½ΠΎ Π² ΡΡΠΌΠΌΠ°ΡΠ½ΠΎΠΉ Π΄ΠΎΠ·Π΅ 15000 ΠΠ΅/ΠΊΠ³, Π»Π°Π·Π΅ΡΠ½ΠΎΠ΅ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΠ΅ (ΠΠ) - ΠΎΠ΄Π½ΠΎΠΊΡΠ°ΡΠ½ΠΎ Π½Π° ΠΎΠ±Π»Π°ΡΡΡ ΠΈΡΠ΅ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΎΡΠ°Π³Π° (970 Π½ΠΌ, 2 ΠΌΠΈΠ½). Π ΠΎΡΠ°Π³Π΅ ΠΈΡΠ΅ΠΌΠΈΠΈ ΠΏΠΎΠ΄ΡΡΠΈΡΡΠ²Π°Π»ΠΈ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ ΠΌΠ΅Π»ΠΊΠΈΡ
ΠΊΡΠΎΠ²Π΅Π½ΠΎΡΠ½ΡΡ
ΡΠΎΡΡΠ΄ΠΎΠ², ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ»ΠΈ ΡΠΊΡΠΏΡΠ΅ΡΡΠΈΡ ΡΠ°ΠΊΡΠΎΡΠ° ΡΠΎΡΡΠ° ΡΠ½Π΄ΠΎΡΠ΅Π»ΠΈΡ ΡΠΎΡΡΠ΄ΠΎΠ² (VEGF). ΠΡΠΈ ΠΠΠΠ Π² ΠΎΡΠ°Π³Π΅ ΠΈΡΠ΅ΠΌΠΈΠΈ ΠΏΠΎΠ²ΡΡΠ°Π΅ΡΡΡ ΡΠΊΡΠΏΡΠ΅ΡΡΠΈΡ VEGF ΠΈ ΡΠ½ΠΈΠΆΠ°Π΅ΡΡΡ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ ΠΌΠ΅Π»ΠΊΠΈΡ
ΠΊΡΠΎΠ²Π΅Π½ΠΎΡΠ½ΡΡ
ΡΠΎΡΡΠ΄ΠΎΠ² Π½Π° 3, 7, 14, 30 ΡΡΡΠΊΠΈ. ΠΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΏΡΠΈ ΠΠΠΠ ΠΠΠ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΡ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π° ΠΌΠ΅Π»ΠΊΠΈΡ
ΠΊΡΠΎΠ²Π΅Π½ΠΎΡΠ½ΡΡ
ΡΠΎΡΡΠ΄ΠΎΠ², Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΠΠ - ΠΊ ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΡ ΡΠΊΡΠΏΡΠ΅ΡΡΠΈΠΈ VEGF ΠΈ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π° ΠΌΠ΅Π»ΠΊΠΈΡ
ΠΊΡΠΎΠ²Π΅Π½ΠΎΡΠ½ΡΡ
ΡΠΎΡΡΠ΄ΠΎΠ² Π½Π° 3, 7, 14, 30 ΡΡΡΠΊΠΈ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°; ΠΏΡΠ΅Π΄ΡΡΠ°Π²ΠΈΡΠ΅Π»ΡΡΡΠ²ΠΎ ΠΊΡΠΎΠ²Π΅Π½ΠΎΡΠ½ΡΡ
ΡΠΎΡΡΠ΄ΠΎΠ² Π²ΡΡΠ΅ ΠΏΠΎΡΠ»Π΅ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡ ΠΠ ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΠΠΠ. ΠΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½Π°Ρ ΡΠΊΡΠΏΡΠ΅ΡΡΠΈΡ VEGF ΠΈ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ ΠΌΠ΅Π»ΠΊΠΈΡ
ΠΊΡΠΎΠ²Π΅Π½ΠΎΡΠ½ΡΡ
ΡΠΎΡΡΠ΄ΠΎΠ² ΠΏΡΠΈ ΠΠΠΠ Π²ΡΡΠ²Π»Π΅Π½Ρ ΠΏΠΎΡΠ»Π΅ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΠΠ ΠΈ ΠΠ