86 research outputs found
Macrophage and tumor cell responses to repetitive pulsed X-ray radiation
To study a response of tumor cells and macrophages to the repetitive pulsed low-dose X-ray radiation. Methods. Tumor growth and lung metastasis of mice with an injected Lewis lung carcinoma were analysed, using C57Bl6. Monocytes were isolated from a human blood, using CD14+ magnetic beads. IL6, IL1-betta, and TNF-alpha were determined by ELISA. For macrophage phenotyping, a confocal microscopy was applied. "Sinus-150" was used for the generation of pulsed X-ray radiation (the absorbed dose was below 0.1 Gy, the pulse repetition frequency was 10 pulse/sec). The irradiation of mice by 0.1 Gy pulsed X-rays significantly inhibited the growth of primary tumor and reduced the number of metastatic colonies in the lung. Furthermore, the changes in macrophage phenotype and cytokine secretion were observed after repetitive pulsed X-ray radiation. Conclusion. Macrophages and tumor cells had a different response to a low-dose pulsed X-ray radiation. An activation of the immune system through changes of a macrophage phenotype can result in a significant antitumor effect of the low-dose repetitive pulsed X-ray radiation
Generation of electromagnetic fields of extremely high intensity by coherent summation of Cherenkov superradiance pulses
We demonstrate both theoretically and experimentally the possibility of correlating the phase of a Cherenkov superradiance (SR) pulse to the sharp edge of a current pulse, when spontaneous emission of the electron bunch edge serves as the seed for SR processes. By division of the driving voltage pulse across several parallel channels equipped with independent cathodes we can synchronize several SR sources to arrange a two-dimensional array. In the experiments carried out, coherent summation of radiation from four independent 8-mm wavelength band SR generators with peak power 600 MW results in the interference maximum of the directional diagram with an intensity that is equivalent to radiation from a single source with a power of 10 GW
Coherent summation of emission from relativistic Cherenkov sources as a way of production of extremely high-intensity microwave pulses
For relativistic Cherenkov devices, we investigate the process of high-power microwave pulse generation with its phase correlating to the sharp edge of an e-beam current pulse. Our theoretical consideration is referred to quasi-stationary and superradiative (SR) generation regimes when spontaneous emission of the e-beam edge serves as the seed for the development of further coherent oscillations. Phase correlation of the excited microwave pulses with the characteristics of the current pulse front and/or an initial external electromagnetic pulse has been additionally confirmed by particle-in-cell simulations. Pulse-to-pulse stability of the radiation phase within several percents of the oscillation period makes it possible to arrange multichannel schemes producing mutually coherent microwave pulses. In the experiments that have been carried out, the cathodes of independent generators were powered by identical accelerating pulses from strictly synchronized voltage modulators, or by splitting the pulse from a single powerful modulator. For the 2-ns regime with the power of each Ka-band backward-wave oscillator about 100 MW, we demonstrate quadratic growth of the power density in the interference maximum of the directional diagram. In a short pulse SR regime, with the peak power of 600 MW in a single channel, for a four-channel 2-D array, we attained a 16-fold radiation intensity gain
ΠΠ»ΠΈΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ΅ΡΠΌΠΈΡΠ΅ΡΠΊΠΈΡ ΡΡΠ»ΠΎΠ²ΠΈΠΉ ΠΠ°ΡΡΠΊΠΎΠ³ΠΎ ΠΌΠΎΡΡ Π·Π° ΠΏΠΎΡΠ»Π΅Π΄Π½ΠΈΠ΅ 40 Π»Π΅Ρ
The paper discusses air (Ta) and sea surface temperature (SST) year-to-year variability due to warming of the Kara Sea, using the data from regular observations at the meteorological stations Roshydromet (GMS) in 1978β2017, NOAA optimum interpolation and reanalysis data. We use the methods of cluster, correlation analysis and Empirical Orthogonal Functions (EOF). We investigate possible cause and effect relationships of these changes with the variations of the wind field components, climatic indices and the sea ice concentration field. The cluster analysis of the three main EOF components has allowed us to identify four areas on the basis of the nature of changes of the water temperature anomalies field. The climatic changes in these areas, in the coastal and island zones of the Kara Sea have manifested themselves in the steady increase of the annual air temperature at GMS from 0,47β0,77 Β°C/10 years on the southwest coast to 1,33β1,49 Β°C/10 years in the north of the sea. This is equivalent to warming from 1,9 to 6,0 Β°C in the last 40 years. For the open sea the value of the Ta trend is about 1,22 Β°C/10 years, which corresponds to an increase in the average Ta by 4,9 Β°C in the last 40 years. This value is approximately 3 times greater than that for all the Northern hemisphere for the same period.Annualy, the maximal trend was observed in November and April mainly and exceeded 2β3 Β°C/10 years at some of the stations. We identify anomalously warm (2016 and 2012) and anomalously cold (1978, 1979, 1992 and 1998) years: the warmest year was 2012, the coldest β 1979. Positive SST trends were observed over all the sea area during the warm period of year (to 1 Β°C/10 years). SST increased to 2,4 Β°C, which is approximately 1,5 times greater than the corresponding SST values for the Northern hemisphere. The maximum SST trend (0,4 Β°C/10 years) was observed in the northwest and southwest parts of the sea. From June to August the trends of SST exceed the annual ones 1,5β2 times. Interannual SST and Ta variations are characterized by close correlation links. Until approximately 1998β2004 the warming was rather insignificant, and after that the growth rate of Ta and SST increased many fold. Apparently it indicates changes in the mode and the large-scale atmospheric circulation in the early 2000s. We also observed a trend of strengthening of the southern wind during the cold period of the year and the northern one β in the warm period (0,5β0,6 m/s in 40 years). It is shown that there is a close correlation between the Ta increase and the changes in the meridional component of the wind speed during the cold period of the year for all the sea areas. For the warm period it is statistically insignificant both for Ta and SST. For the cold season we observed a contribution of the large-scale mode of atmospheric circulation into the variability of V component of the wind speed. The conribution was expressed through the indeces NAO, SCAND, Pol/EUR, AZOR, ISL and the differences of ISLSIB. For the warm season this contribution is expressed through the NAO, SCAND and AO only. For the warm period we showed statistically significant correlation between the increase in SST, Ta and the processes parametrized by the AMO, EA/WR and AZOR indeces. For the cold period the indeces are AMO, Pol/Eur, SIB and ISL SIB. The interannual variations of the sea ice concentration field are characterized by close correlation with Ta changes both in the annual cycle and during the periods of ice cover formation and evolution (RΒ = β0,7... β0,9). For these periods we showed statistically significant relationships between the first EOF mode fluctuations and two climatic indeces β AMO (RΒ = 0,5) and Pol/Eur (RΒ = 0,4). The relationships between the temporary variability of the sea ice concentration and the wind field characteristics are weaker and statistically significant only for the meridional component of the wind speed (RΒ = β0,4).ΠΠΎ Π΄Π°Π½Π½ΡΠΌ ΡΡΠΎΡΠ½ΡΡ
Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΠΉ Π½Π° Π³ΠΈΠ΄ΡΠΎΠΌΠ΅ΡΠ΅ΠΎΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΠ°Π½ΡΠΈΡΡ
Π ΠΎΡΠ³ΠΈΠ΄ΡΠΎΠΌΠ΅ΡΠ° Π·Π° 1978β2017 Π³Π³., Π΄Π°Π½Π½ΡΡ
ΠΎΠΏΡΠΈΠΌΠ°Π»ΡΠ½ΠΎΠΉ ΠΈΠ½ΡΠ΅ΡΠΏΠΎΠ»ΡΡΠΈΠΈ ΠΈ ΡΠ΅Π°Π½Π°Π»ΠΈΠ·Π° NOAA Π²ΡΠΏΠΎΠ»Π½Π΅Π½ Π°Π½Π°Π»ΠΈΠ· ΠΌΠ΅ΠΆΠ³ΠΎΠ΄ΠΎΠ²ΠΎΠΉ ΠΈΠ·ΠΌΠ΅Π½ΡΠΈΠ²ΠΎΡΡΠΈ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠ½ΠΎΠΉ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ Π²ΠΎΠ΄Ρ ΠΈ Π²ΠΎΠ·Π΄ΡΡ
Π° Π² ΠΠ°ΡΡΠΊΠΎΠΌ ΠΌΠΎΡΠ΅ Π½Π° ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠΌ ΡΡΠ°ΠΏΠ΅ ΠΏΠΎΡΠ΅ΠΏΠ»Π΅Π½ΠΈΡ ΠΊΠ»ΠΈΠΌΠ°ΡΠ°. ΠΠ΅ΡΠΎΠ΄Ρ ΠΊΠ»Π°ΡΡΠ΅ΡΠ½ΠΎΠ³ΠΎ, ΠΊΠΎΡΡΠ΅Π»ΡΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΠΈ Π°ΠΏΠΏΠ°ΡΠ°ΡΠ° ΡΠΌΠΏΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΡΡΠΎΠ³ΠΎΠ½Π°Π»ΡΠ½ΡΡ
ΡΡΠ½ΠΊΡΠΈΠΉ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Ρ Π΄Π»Ρ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΠΏΡΠΎΡΡΡΠ°Π½ΡΡΠ²Π΅Π½Π½ΠΎ-Π²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠΉ ΡΡΡΡΠΊΡΡΡΡ ΠΏΠΎΠ»Ρ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΈ ΡΠ°ΠΉΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π°ΠΊΠ²Π°ΡΠΎΡΠΈΠΈ ΠΏΠΎ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΡΠΌ ΠΊΠ»ΠΈΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΡΠ΅ ΠΏΡΠΈΡΠΈΠ½Π½ΠΎ-ΡΠ»Π΅Π΄ΡΡΠ²Π΅Π½Π½ΡΠ΅ ΡΠ²ΡΠ·ΠΈ ΡΡΠΈΡ
ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ Ρ Π²Π°ΡΠΈΠ°ΡΠΈΡΠΌΠΈ ΡΠΎΡΡΠ°Π²Π»ΡΡΡΠΈΡ
ΠΏΠΎΠ»Ρ Π²Π΅ΡΡΠ°, ΠΊΠ»ΠΈΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΈΠ½Π΄Π΅ΠΊΡΠ°ΠΌΠΈ ΠΈ ΡΠΏΠ»ΠΎΡΠ΅Π½Π½ΠΎΡΡΡΡ Π»ΡΠ΄Π°. Π ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΡΠ΄Π°Π»ΠΎΡΡ ΡΡΠΎΡΠ½ΠΈΡΡ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ ΠΎΡΠ΅Π½ΠΊΡ ΡΠ΅Π½Π΄Π΅Π½ΡΠΈΠΉ ΠΈ Π²ΡΡΠ²ΠΈΡΡ ΡΠ΅Π³ΠΈΠΎΠ½Π°Π»ΡΠ½ΡΠ΅ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠ΅ΠΉ ΠΌΠ΅ΠΆΠ³ΠΎΠ΄ΠΎΠ²ΠΎΠΉ ΠΈΠ·ΠΌΠ΅Π½ΡΠΈΠ²ΠΎΡΡΠΈ ΡΠ΅ΡΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΠ»ΠΎΠ²ΠΈΠΉ ΠΠ°ΡΡΠΊΠΎΠ³ΠΎ ΠΌΠΎΡΡ
ΠΡΠ΅Π½ΠΊΠ° Π²Π»ΠΈΡΠ½ΠΈΡ Π½Π°Π½ΠΎΡΠ΅ΠΊΡΠ½Π΄Π½ΡΡ ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ²ΡΠΊΠΈΡ ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ² Π½Π° ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΌΠΈΡΠΎΡ ΠΎΠ½Π΄ΡΠΈΠΉ ΠΏΠ΅ΡΠ΅Π½ΠΈ ΠΌΡΡΠ΅ΠΉ
The effect of nanosecond pulses of X-ray (pulse repetition rate of 8β22 pulses per second, dose 0,3β1,8 mR per pulse) on the functional activity of isolated mitochondria of mice liver. The effects of changing the rate of oxygen consumption by mitochondria in different metabolic states of Chance and the degree of coupling of oxidation and phosphorylation were investigated. That effect depends on the parameters of exposure.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΎ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ²ΡΠΊΠΈΡ
ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ² Π½Π°Π½ΠΎΡΠ΅ΠΊΡΠ½Π΄Π½ΠΎΠΉ Π΄Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ (ΡΠ°ΡΡΠΎΡΠ° ΠΏΠΎΠ²ΡΠΎΡΠ΅Π½ΠΈΡ 8β22 ΠΈΠΌΠΏΡΠ»ΡΡΠ° Π² ΡΠ΅ΠΊΡΠ½Π΄Ρ, Π΄ΠΎΠ·Π° Π² ΠΈΠΌΠΏΡΠ»ΡΡΠ΅ 0,3β1,8 ΠΌΠ ) Π½Π° ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΈΠ·ΠΎΠ»ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΌΠΈΡΠΎΡ
ΠΎΠ½Π΄ΡΠΈΠΉ ΠΏΠ΅ΡΠ΅Π½ΠΈ ΠΌΡΡΠ΅ΠΉ. ΠΡΡΠ»Π΅Π΄ΡΠ΅ΠΌΠΎΠ΅ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΠΈΠ·ΠΌΠ΅Π½ΡΠ΅Ρ ΡΠΊΠΎΡΠΎΡΡΡ ΠΏΠΎΡΡΠ΅Π±Π»Π΅Π½ΠΈΡ ΠΊΠΈΡΠ»ΠΎΡΠΎΠ΄Π° ΠΌΠΈΡΠΎΡ
ΠΎΠ½Π΄ΡΠΈΡΠΌΠΈ Π² ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΠΌΠ΅ΡΠ°Π±ΠΎΠ»ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΎΡΡΠΎΡΠ½ΠΈΡΡ
ΠΏΠΎ Π§Π°Π½ΡΡ ΠΈ ΡΡΠ΅ΠΏΠ΅Π½Ρ ΡΠΎΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ² ΠΎΠΊΠΈΡΠ»Π΅Π½ΠΈΡ ΠΈ ΡΠΎΡΡΠΎΡΠΈΠ»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ. ΠΠ°Π½Π½ΡΠΉ ΡΡΡΠ΅ΠΊΡ Π·Π°Π²ΠΈΡΠΈΡ ΠΎΡ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡ
Π Π°Π·Π»ΠΈΡΠΈΡ ΡΡΠ΅ΠΊΡΠΎΠ² ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΠΎ-ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ²ΡΠΊΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π² ΠΎΠΏΡΡ ΠΎΠ»Π΅Π²ΡΡ ΠΊΠ»Π΅ΡΠΊΠ°Ρ Π»ΠΈΠ½ΠΈΠΈ MOLT-4 ΠΈ Π»ΠΈΠΌΡΠΎΡΠΈΡΠ°Ρ ΠΏΠ΅ΡΠΈΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΊΡΠΎΠ²ΠΈ ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ°
Effects of ionizing radiation registered in cells after low dose irradiation are still poorly understood. Thus, the aim of this study was to analyze effects of pulsed X-rays on level of radiation-induced DNA double-strand breaks and their repair kinetics in cancer and normalhuman cells in vitro. Analysis of radiation-induced Ξ³H2AX and 53BP1 repair foci in MOLT-4 cells with lymphoblastic origin was used for assessment of DNA double-strand breaks (DSB) in these cells. Number of residual radiation-induced Ξ³H2AX and 53BP1 foci at 18 hafter irradiation depended on frequency of X-ray pulses: at 8 pulses per second effect was highest in MOLT-4 cells and lowest in peripheral blood lymphocytes. It suggests that pulsed X-rays with various frequencies could be used for target influence on cancer cells being lessdeleterious for normal human cells.Π Π°Π·ΡΠ°Π±ΠΎΡΠ°Π½Ρ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠΈ, ΡΠΏΠΎΡΠΎΠ±Π½ΡΠ΅ Π³Π΅Π½Π΅ΡΠΈΡΠΎΠ²Π°ΡΡ ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΠΎ-ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ²ΡΠΊΠΎΠ΅ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΠ΅ (ΠΠΠ Π) Π² Π½Π°Π½ΠΎΡΠ΅ΠΊΡΠ½Π΄Π½ΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ Ρ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ°ΡΡΠΎΡΡ ΠΏΠΎΠ²ΡΠΎΡΠ΅Π½ΠΈΡ ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ² ΠΈ Π΄ΠΎΠ·Ρ Π·Π° ΠΈΠΌΠΏΡΠ»ΡΡ. Π¦Π΅Π»ΡΡ Π½Π°ΡΡΠΎΡΡΠ΅Π³ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΡΠ°Π» Π°Π½Π°Π»ΠΈΠ· Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡ ΠΠΠ Π Π½Π° ΡΡΠΎΠ²Π΅Π½Ρ Π΄Π²ΡΠ½ΠΈΡΠ΅Π²ΡΡ
ΡΠ°Π·ΡΡΠ²ΠΎΠ² ΠΠΠ Π² ΠΎΠΏΡΡ
ΠΎΠ»Π΅Π²ΡΡ
ΠΈ Π½ΠΎΡΠΌΠ°Π»ΡΠ½ΡΡ
ΠΊΠ»Π΅ΡΠΊΠ°Ρ
ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ° Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
in vitro. ΠΠ»Ρ ΠΎΡΠ΅Π½ΠΊΠΈ ΡΡΠΎΠ²Π½Ρ Π΄Π²ΡΠ½ΠΈΡΠ΅Π²ΡΡ
ΡΠ°Π·ΡΡΠ²ΠΎΠ² ΠΠΠ ΠΈ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΈΡ
ΡΠ΅ΠΏΠ°ΡΠ°ΡΠΈΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π»ΡΡ ΠΌΠ΅ΡΠΎΠ΄ Π°Π½Π°Π»ΠΈΠ·Π° ΡΠ»ΡΠΎΡΠ΅ΡΡΠ΅Π½ΡΠ½ΡΡ
ΡΠΎΠΊΡΡΠΎΠ² Π±Π΅Π»ΠΊΠΎΠ² ΡΠ΅ΠΏΠ°ΡΠ°ΡΠΈΠΈ ΠΠΠ Ξ³H2AX ΠΈ 53BP1 Π² ΠΊΠ»Π΅ΡΠΊΠ°Ρ
ΠΎΠΏΡΡ
ΠΎΠ»Π΅Π²ΠΎΠΉ Π»ΠΈΠ½ΠΈΠΈ MOLT-4, ΠΈΠΌΠ΅ΡΡΠ΅ΠΉ Π»ΠΈΠΌΡΠΎΠ±Π»Π°ΡΡΠ½ΠΎΠ΅ ΠΏΡΠΎΠΈΡΡ
ΠΎΠΆΠ΄Π΅Π½ΠΈΠ΅, ΠΏΠΎΡΠ»Π΅ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡ ΠΠΠ Π Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
in vitro. ΠΠ°ΠΈΠ±ΠΎΠ»ΡΡΠΈΠΉ ΡΡΠΎΠ²Π΅Π½Ρ ΡΠΎΠΊΡΡΠΎΠ² Ξ³H2AX ΠΈ 53BP1 ΡΠ΅ΡΠ΅Π· 18 Ρ ΠΏΠΎΡΠ»Π΅ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡ, ΡΠ²Π»ΡΡΡΠΈΠΉΡΡ ΠΌΠ°ΡΠΊΠ΅ΡΠΎΠΌ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΡΠ΅ΠΏΠ°ΡΠ°ΡΠΈΠΈ ΠΠΠ, Π² ΠΊΠ»Π΅ΡΠΊΠ°Ρ
Π»ΠΈΠ½ΠΈΠΈ MOLT-4 ΠΎΡΠΌΠ΅ΡΠ°Π»ΡΡ ΠΏΡΠΈ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠΈ ΠΠΠ Π Ρ ΡΠ°ΡΡΠΎΡΠΎΠΉ ΠΏΠΎΠ²ΡΠΎΡΠ΅Π½ΠΈΡ ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ² 8 ΠΈΠΌΠΏ./Ρ, ΠΏΡΠΈ ΠΊΠΎΡΠΎΡΠΎΠΉ ΡΠ°Π½Π΅Π΅ Π² Π»ΠΈΠΌΡΠΎΡΠΈΡΠ°Ρ
Π½Π°Π±Π»ΡΠ΄Π°Π»ΠΎΡΡ Π½Π°ΠΈΠΌΠ΅Π½ΡΡΠ΅Π΅ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ Π΄Π²ΡΠ½ΠΈΡΠ΅Π²ΡΡ
ΡΠ°Π·ΡΡΠ²ΠΎΠ² ΠΠΠ. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΡΠΊΠ°Π·ΡΠ²Π°ΡΡ, ΡΡΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΠΠ Π Ρ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠΌΠΈ ΡΠ°ΡΡΠΎΡΠ°ΠΌΠΈ ΠΏΠΎΠ²ΡΠΎΡΠ΅Π½ΠΈΡ ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ² ΠΌΠΎΠΆΠ΅Ρ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΡΡΠ΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΎΠ²Π°ΡΡ Π½Π° ΠΎΠΏΡΡ
ΠΎΠ»Π΅Π²ΡΠ΅ ΠΊΠ»Π΅ΡΠΊΠΈ, Π½Π΅Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π°Ρ ΠΏΡΠΈ ΡΡΠΎΠΌ Π½ΠΎΡΠΌΠ°Π»ΡΠ½ΡΠ΅ ΠΊΠ»Π΅ΡΠΊΠΈ ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ°
ΠΠΠΠ―ΠΠΠ ΠΠΠΠ£ΠΠ¬Π‘ΠΠ-ΠΠΠ ΠΠΠΠΠ§ΠΠ‘ΠΠΠΠ Π ΠΠΠ’ΠΠΠΠΠΠ‘ΠΠΠΠ ΠΠΠΠ£Π§ΠΠΠΠ― ΠΠ ΠΠΠΠ’ΠΠ ΠΠΠ£Π₯ΠΠΠ Π ΠΠΠ‘Π’ΠΠΠΠ ΠΠΠΠΠ ΠΠ«Π¨ΠΠ
The results of the effect of pulse-periodic X-ray exposure (PPXE) generated by Sinus-150 accelerator on tumor and normal cells of mice have been presented. Chromosomal aberrations (metaphase analysis) of bone marrow cells were studied. Using the cultured Lewis lung carcinoma cell lines, the level of apoptotic cells and cells with high concentration of active oxygen forms (AOF) was assessed by the flow cytofluorometry analysis (FACSCantoII, BD). In vivo X-ray radiation in the pulse-periodic mode lead to the moderate increase in chromosomal aberrations of bone marrow cells of mice. PPXE induced apoptotic death in Lewis lung carcinoma cells in vitro due to AOF production. Dose-effect relation was not observed at the irradiation doses 0.2β1.0 Gy. The data obtained show that further studies are necessary to justify the use of PPXE in tumor therapy.ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΠ·ΡΡΠ΅Π½ΠΈΡ Π²Π»ΠΈΡΠ½ΠΈΡ ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΠΎ-ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ²ΡΠΊΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ (ΠΠΠ Π), Π³Π΅Π½Π΅ΡΠΈΡΡΠ΅ΠΌΠΎΠ³ΠΎ ΡΠ½ΠΈΠΊΠ°Π»ΡΠ½ΡΠΌ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠΎΠΌ Β«Π‘ΠΈΠ½ΡΡ-150Β» (ΠΠ½ΡΡΠΈΡΡΡ ΡΠΈΠ»ΡΠ½ΠΎΡΠΎΡΠ½ΠΎΠΉ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΈΠΊΠΈ Π‘Π Π ΠΠ, Π³. Π’ΠΎΠΌΡΠΊ), Π½Π° ΠΎΠΏΡΡ
ΠΎΠ»Π΅Π²ΡΠ΅ ΠΈ Π½ΠΎΡΠΌΠ°Π»ΡΠ½ΡΠ΅ ΠΊΠ»Π΅ΡΠΊΠΈ. ΠΠ·ΡΡΠ°Π»ΠΈ Ρ
ΡΠΎΠΌΠΎΡΠΎΠΌΠ½ΡΠ΅ Π°Π±Π΅ΡΡΠ°ΡΠΈΠΈ (ΠΌΠ΅ΡΠ°ΡΠ°Π·Π½ΡΠΉ Π°Π½Π°Π»ΠΈΠ·) ΠΊΠ»Π΅ΡΠΎΠΊ ΠΊΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π° ΠΌΡΡΠ΅ΠΉ, ΠΎΠ±Π»ΡΡΠ΅Π½Π½ΡΡ
ΠΠΠ Π Π² ΡΠ΅ΠΆΠΈΠΌΠ°Ρ
, ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°ΡΡΠΈΡ
ΠΏΡΠΎΡΠΈΠ²ΠΎΠΎΠΏΡΡ
ΠΎΠ»Π΅Π²ΡΠΉ ΡΡΡΠ΅ΠΊΡ. ΠΠ° ΠΊΡΠ»ΡΡΡΡΠ°Ρ
ΠΊΠ»Π΅ΡΠΎΠΊ ΠΊΠ°ΡΡΠΈΠ½ΠΎΠΌΡ ΠΡΡΠΈΡ, ΠΎΠ±Π»ΡΡΠ΅Π½Π½ΡΡ
ΠΠΠ Π, ΠΎΡΠ΅Π½ΠΈΠ²Π°Π»ΠΈ ΡΡΠΎΠ²Π΅Π½Ρ Π°ΠΏΠΎΠΏΡΠΎΠ·Π° ΠΊΠ»Π΅ΡΠΎΠΊ ΠΈ ΠΊΠ»Π΅ΡΠΎΠΊ Ρ Π²ΡΡΠΎΠΊΠΈΠΌ ΡΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΈΠ΅ΠΌ Π°ΠΊΡΠΈΠ²Π½ΡΡ
ΡΠΎΡΠΌ ΠΊΠΈΡΠ»ΠΎΡΠΎΠ΄Π° (ΠΠ€Π) ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΠΏΡΠΎΡΠΎΡΠ½ΠΎΠΉ ΡΠΈΡΠΎΡΠ»ΡΠΎΡΠΈΠΌΠ΅ΡΡΠΈΠΈ (FACSCantoII, BD). ΠΡΠΈ Π»ΠΎΠΊΠ°Π»ΡΠ½ΠΎΠΌ ΠΎΠ±Π»ΡΡΠ΅Π½ΠΈΠΈ ΠΠΠ Π in vivo Π² ΡΠ΅ΠΆΠΈΠΌΠ°Ρ
, Π²ΡΠ·ΡΠ²Π°ΡΡΠΈΡ
ΠΏΡΠΎΡΠΈΠ²ΠΎΠΎΠΏΡΡ
ΠΎΠ»Π΅Π²ΡΠΉ ΡΡΡΠ΅ΠΊΡ, Π½Π°Π±Π»ΡΠ΄Π°Π΅ΡΡΡ ΡΠΌΠ΅ΡΠ΅Π½Π½ΠΎΠ΅ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ Π°Π±Π΅ΡΡΠ°ΡΠΈΠΉ Π² Ρ
ΡΠΎΠΌΠΎΡΠΎΠΌΠ°Ρ
ΠΊΠ»Π΅ΡΠΎΠΊ ΠΊΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π° ΠΌΡΡΠ΅ΠΉ. ΠΠΠ Π ΠΈΠ½Π΄ΡΡΠΈΡΡΠ΅Ρ ΠΏΡΠΎΡΠ΅ΡΡ Π°ΠΏΠΎΠΏΡΠΎΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π³ΠΈΠ±Π΅Π»ΠΈ Π² ΠΊΠ»Π΅ΡΠΊΠ°Ρ
ΠΊΠ°ΡΡΠΈΠ½ΠΎΠΌΡ Π»Π΅Π³ΠΊΠΈΡ
ΠΡΡΠΈΡ in vitro Π·Π° ΡΡΠ΅Ρ ΠΏΡΠΎΠ΄ΡΠΊΡΠΈΠΈ ΠΠ€Π. ΠΡΠΈ ΡΡΠΎΠΌ Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ 0,2β1,0 ΠΡ Π½Π΅ ΠΎΡΠΌΠ΅ΡΠ°Π΅ΡΡΡ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΡΡΡΠ΅ΠΊΡΠ° ΠΎΡ Π΄ΠΎΠ·Ρ ΠΎΠ±Π»ΡΡΠ΅Π½ΠΈΡ. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ Π΄Π°Π½Π½ΡΠ΅ ΡΠ²ΠΈΠ΄Π΅ΡΠ΅Π»ΡΡΡΠ²ΡΡΡ ΠΎ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠΈΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Π΄Π»Ρ ΠΎΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΠΠΠ Π Π² ΡΠ΅ΡΠ°ΠΏΠΈΠΈ ΠΎΠΏΡΡ
ΠΎΠ»Π΅ΠΉ
ΠΠ΅ΠΉΡΡΠ²ΠΈΠ΅ Π½Π°Π½ΠΎΡΠ΅ΠΊΡΠ½Π΄Π½ΠΎΠ³ΠΎ ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΠΎ-ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΌΠΈΠΊΡΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π½Π° ΠΏΡΠΎΡΠ΅ΡΡΡ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΈ
The effects of pulse periodic microwaves (10 GHz, duration of pulse 100 ns, pulse repetition frequency 4β19 pps, peak power density 40β1 520 W/cm2 ) on the reparative regeneration of full-thickness skin wounds on mice was investigated. This effect depends on the pulse repetition frequency and peak power density.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΎ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΠΎ-ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΌΠΈΠΊΡΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ (10 ΠΠΡ, Π΄Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡ ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ² 100 Π½Ρ, ΡΠ°ΡΡΠΎΡΠ° ΠΏΠΎΠ²ΡΠΎΡΠ΅Π½ΠΈΡ 4β19 ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ² Π² ΡΠ΅ΠΊΡΠ½Π΄Ρ, ΠΏΠΈΠΊΠΎΠ²Π°Ρ ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΡ ΠΏΠΎΡΠΎΠΊΠ° ΠΌΠΎΡΠ½ΠΎΡΡΠΈ 40β1 520 ΠΡ/ΡΠΌ2 ) Π½Π° ΡΠ΅ΠΏΠ°ΡΠ°ΡΠΈΠ²Π½ΡΡ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΡ ΠΏΠΎΠ»Π½ΠΎΡΠ»ΠΎΠΉΠ½ΠΎΠΉ ΠΊΠΎΠΆΠ½ΠΎΠΉ ΡΠ°Π½Ρ Ρ ΠΌΡΡΠ΅ΠΉ. ΠΡΡΠ»Π΅Π΄ΡΠ΅ΠΌΠΎΠ΅ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΠΌΠΎΠΆΠ΅Ρ ΡΡΠΈΠΌΡΠ»ΠΈΡΠΎΠ²Π°ΡΡ Π·Π°ΠΆΠΈΠ²Π»Π΅Π½ΠΈΠ΅ ΡΠ°Π½. ΠΠ°Π½Π½ΡΠΉ ΡΡΡΠ΅ΠΊΡ Π·Π°Π²ΠΈΡΠΈΡ ΠΎΡ ΡΠ°ΡΡΠΎΡΡ ΠΏΠΎΠ²ΡΠΎΡΠ΅Π½ΠΈΡ ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ² ΠΈ Π²Π΅Π»ΠΈΡΠΈΠ½Ρ ΠΏΠΈΠΊΠΎΠ²ΠΎΠΉ ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΠΈ ΠΏΠΎΡΠΎΠΊΠ° ΠΌΠΎΡΠ½ΠΎΡΡΠΈ
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