57 research outputs found

    Analysis of growth kinetics and proliferative heterogeneity of Lewis lung carcinoma cells growing as unfed culture

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    Аim: To analyze the growth kinetics and proliferative heterogeneity of Lewis lung carcinoma (LLC) cells during their growth in monolayer for 5 days without replacement of culture medium (unfed culture). Methods: Cell biology methods, sandwich enzyme-linked immunosorbent assay for vascular endothelial growth factor (VEGF) detection (ELISA), enzymatic glucose-oxidase method for glucose measurements, mathematical modeling. Results: Created mathematical model showed good fit to experimental data; that allowed to determine kinetic (model) parameters of LLC cells and predict the changes in number of proliferating and quiescent cells (proliferative heterogeneity) during their growth. It was shown that growth kinetics of viable LLC cells possesses non-monotonous character β€” during first three days of growth the number of cells raised exponentially, with following decrease after the maximal level was achieved. At the same time the decrease of number of viable cells/increase of number of dead cells has been observed upon complete depletion of culture medium by glucose content. Glucose dependence of cell transition rate from proliferation to resting state predicted by mathematical model possessed a pronounced two-phase character. At a wide range of relatively high glucose concentrations (> 1.0 mg/ml) the transition rate was close to zero. At concentrations lower than 0.7 mg/ml, the rate of transition swiftly increased resulting in sharp change in cellular composition. At an interval from 70 to 90 h, practically all proliferating cells transited to a resting state. The rate of quiescent cell death was relatively low, and this was in part caused by too low level of glucose consumption compared to proliferating cells. It was shown that during LLC cells growth VEGF production rate decreased monotonously in spite of the fact that the level of VEGF in incubation medium increased monotonously. Observed monotonous decrease of VEGF production rate could not be explained by VEGF degradation in incubation medium (our results displayed the stability of VEGF molecule during investigations). Conclusions: Weak dependence of cell transition rate from proliferating to resting state from glucose level (> 0.7 mg/ml) and low rate of cell death provided slow decrease of the pool of quiescent cells in the population, thus significantly increasing their chance to survive upon nutritional deficiency.ЦСль: провСсти Π°Π½Π°Π»ΠΈΠ· ΠΊΠΈΠ½Π΅Ρ‚ΠΈΠΊΠΈ роста ΠΈ ΠΏΡ€ΠΎΠ»ΠΈΡ„Π΅Ρ€Π°Ρ‚ΠΈΠ²Π½ΠΎΠΉ гСтСрогСнности ΠΊΠ»Π΅Ρ‚ΠΎΠΊ ΠΊΠ°Ρ€Ρ†ΠΈΠ½ΠΎΠΌΡ‹ Π»Π΅Π³ΠΊΠΎΠ³ΠΎ Π›ΡŒΡŽΠΈΡ (LLC) ΠΏΡ€ΠΈ ΠΈΡ… ростС Π² монослоС Π½Π° протяТСнии 5 сут Π±Π΅Π· Π·Π°ΠΌΠ΅Π½Ρ‹ ΠΊΡƒΠ»ΡŒΡ‚ΡƒΡ€Π°Π»ΡŒΠ½ΠΎΠΉ срСды (unfed culture). ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹: ΠΈΠΌΠΌΡƒΠ½ΠΎΡ„Π΅Ρ€ΠΌΠ΅Π½Ρ‚Π½Ρ‹ΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄ опрСдСлСния уровня ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ†ΠΈΠΈ VEGF ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅Π²Ρ‹ΠΌΠΈ ΠΊΠ»Π΅Ρ‚ΠΊΠ°ΠΌΠΈ; Π³Π»ΡŽΠΊΠΎΠ·ΠΎΠΎΠΊΡΠΈΠ΄Π°Π·Π½Ρ‹ΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄ опрСдСлСния уровня Π³Π»ΡŽΠΊΠΎΠ·Ρ‹ Π² срСдС ΠΈΠ½ΠΊΡƒΠ±Π°Ρ†ΠΈΠΈ; матСматичСскоС ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹: прСдлоТСнная матСматичСская модСль Ρ…ΠΎΡ€ΠΎΡˆΠΎ описываСт ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Π΅ Π΄Π°Π½Π½Ρ‹Π΅, Ρ‡Ρ‚ΠΎ позволяСт ΠΎΠΏΡ€Π΅Π΄Π΅Π»ΠΈΡ‚ΡŒ кинСтичСскиС ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹ роста ΠΊΠ»Π΅Ρ‚ΠΎΠΊ LLC ΠΈ ΠΏΡ€Π΅Π΄ΡΠΊΠ°Π·Π°Ρ‚ΡŒ измСнСния количСства ΠΏΡ€ΠΎΠ»ΠΈΡ„Π΅Ρ€ΠΈΡ€ΡƒΡŽΡ‰ΠΈΡ… ΠΈ покоящихся ΠΊΠ»Π΅Ρ‚ΠΎΠΊ (пролифСративная Π³Π΅Ρ‚Π΅Ρ€ΠΎΠ³Π΅Π½Π½ΠΎΡΡ‚ΡŒ) Π² процСссС ΠΈΡ… роста. ΠšΠΈΠ½Π΅Ρ‚ΠΈΠΊΠ° роста ΠΊΠ»Π΅Ρ‚ΠΎΠΊ LLC носит Π½Π΅ΠΌΠΎΠ½ΠΎΡ‚ΠΎΠ½Π½Ρ‹ΠΉ Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ β€” Π² Ρ‚Π΅Ρ‡Π΅Π½ΠΈΠ΅ ΠΏΠ΅Ρ€Π²Ρ‹Ρ… 3 сут ΠΈΡ… роста количСство ΠΊΠ»Π΅Ρ‚ΠΎΠΊ ΡΠΊΡΠΏΠΎΠ½Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½ΠΎ увСличиваСтся ΠΈ Π΄Π°Π»Π΅Π΅, ΠΏΠΎ достиТСнии максимальной плотности, сниТаСтся. Π’ Ρ‚ΠΎ ΠΆΠ΅ врСмя ΡƒΠΌΠ΅Π½ΡŒΡˆΠ΅Π½ΠΈΠ΅ количСства ΠΆΠΈΠ²Ρ‹Ρ… ΠΊΠ»Π΅Ρ‚ΠΎΠΊ/ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΠ΅ количСства ΠΌΠ΅Ρ€Ρ‚Π²Ρ‹Ρ… ΠΊΠ»Π΅Ρ‚ΠΎΠΊ тСсно связано с истощСниСм Π³Π»ΡŽΠΊΠΎΠ·Ρ‹ Π² срСдС ΠΈΠ½ΠΊΡƒΠ±Π°Ρ†ΠΈΠΈ. Π—Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ‚ΡŒ скорости ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π° ΠΊΠ»Π΅Ρ‚ΠΎΠΊ ΠΈΠ· состояния ΠΏΡ€ΠΎΠ»ΠΈΡ„Π΅Ρ€Π°Ρ†ΠΈΠΈ Π² состояниС покоя ΠΎΡ‚ содСрТания Π³Π»ΡŽΠΊΠΎΠ·Ρ‹ Π² срСдС ΠΈΠ½ΠΊΡƒΠ±Π°Ρ†ΠΈΠΈ ΠΈΠΌΠ΅Π΅Ρ‚ Π²Ρ‹Ρ€Π°ΠΆΠ΅Π½Π½Ρ‹ΠΉ Π΄Π²ΡƒΡ…Ρ„Π°Π·Π½Ρ‹ΠΉ Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€. Π’ ΡˆΠΈΡ€ΠΎΠΊΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ ΠΎΡ‚Π½ΠΎΡΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ высоких ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠΉ Π³Π»ΡŽΠΊΠΎΠ·Ρ‹ (> 1,0 ΠΌΠ³/ ΠΌΠ») ΡΠΊΠΎΡ€ΠΎΡΡ‚ΡŒ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π° Π±Π»ΠΈΠ·ΠΊΠ° ΠΊ Π½ΡƒΠ»ΡŽ. ΠŸΡ€ΠΈ концСнтрациях < 0,7 ΠΌΠ³/ΠΌΠ» ΡΠΊΠΎΡ€ΠΎΡΡ‚ΡŒ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π° ΡΡ‚Ρ€Π΅ΠΌΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ возрастаСт, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ Ρ€Π΅Π·ΠΊΠΈΠΌ измСнСниям ΠΊΠ»Π΅Ρ‚ΠΎΡ‡Π½ΠΎΠ³ΠΎ состава ΠΊΠ»Π΅Ρ‚ΠΎΡ‡Π½ΠΎΠΉ популяции. Π’ ΠΈΠ½Ρ‚Π΅Ρ€Π²Π°Π»Π΅ ΠΎΡ‚ 70 Π΄ΠΎ 90 Ρ‡ практичСски всС ΠΏΡ€ΠΎΠ»ΠΈΡ„Π΅Ρ€ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠ΅ ΠΊΠ»Π΅Ρ‚ΠΊΠΈ пСрСходят Π² состояниС покоя. Π‘ΠΊΠΎΡ€ΠΎΡΡ‚ΡŒ Π³ΠΈΠ±Π΅Π»ΠΈ покоящихся ΠΊΠ»Π΅Ρ‚ΠΎΠΊ ΠΎΡ‚Π½ΠΎΡΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ низкая, Ρ‡Ρ‚ΠΎ, Π² частности, связано с Π½ΠΈΠ·ΠΊΠΈΠΌ ΡƒΡ€ΠΎΠ²Π½Π΅ΠΌ потрСблСния Π³Π»ΡŽΠΊΠΎΠ·Ρ‹ этими ΠΊΠ»Π΅Ρ‚ΠΊΠ°ΠΌΠΈ ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с Ρ‚Π°ΠΊΠΎΠ²Ρ‹ΠΌ ΠΏΡ€ΠΎΠ»ΠΈΡ„Π΅Ρ€ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠΌΠΈ ΠΊΠ»Π΅Ρ‚ΠΊΠ°ΠΌΠΈ. УстановлСно, Ρ‡Ρ‚ΠΎ Π² процСссС роста ΡΠΊΠΎΡ€ΠΎΡΡ‚ΡŒ ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ†ΠΈΠΈ VEGF ΠΊΠ»Π΅Ρ‚ΠΊΠ°ΠΌΠΈ LLC ΠΌΠΎΠ½ΠΎΡ‚ΠΎΠ½Π½ΠΎ сниТаСтся, нСсмотря Π½Π° Ρ‚ΠΎ, Ρ‡Ρ‚ΠΎ Π² срСдС ΠΈΠ½ΠΊΡƒΠ±Π°Ρ†ΠΈΠΈ Π΅Π³ΠΎ ΡƒΡ€ΠΎΠ²Π΅Π½ΡŒ ΠΌΠΎΠ½ΠΎΡ‚ΠΎΠ½Π½ΠΎ нарастаСт. Π’Ρ‹Π²ΠΎΠ΄Ρ‹: низкая Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ‚ΡŒ скорости ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π° ΠΊΠ»Π΅Ρ‚ΠΎΠΊ LLC ΠΈΠ· состояния ΠΏΡ€ΠΎΠ»ΠΈΡ„Π΅Ρ€Π°Ρ†ΠΈΠΈ Π² состояниС покоя ΠΎΡ‚ уровня Π³Π»ΡŽΠΊΠΎΠ·Ρ‹ (> 0,7 ΠΌΠ³/ΠΌΠ») Π² срСдС ΠΈΠ½ΠΊΡƒΠ±Π°Ρ†ΠΈΠΈ, Π° Ρ‚Π°ΠΊΠΆΠ΅ Π½ΠΈΠ·ΠΊΠΈΠΉ ΡƒΡ€ΠΎΠ²Π΅Π½ΡŒ ΠΈΡ… Π³ΠΈΠ±Π΅Π»ΠΈ обусловливаСт ΠΌΠ΅Π΄Π»Π΅Π½Π½ΠΎΠ΅ сниТСниС ΠΏΡƒΠ»Π° покоящихся ΠΊΠ»Π΅Ρ‚ΠΎΠΊ Π² популяции, Ρ‡Ρ‚ΠΎ Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ ΠΏΠΎΠ²Ρ‹ΡˆΠ°Π΅Ρ‚ ΠΈΡ… ΡˆΠ°Π½ΡΡ‹ Π²Ρ‹ΠΆΠΈΡ‚ΡŒ Π² условиях Π΄Π΅Ρ„ΠΈΡ†ΠΈΡ‚Π° ΠΏΠΈΡ‚Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… субстратов

    Ferroelectric switching in epitaxial GeTe films

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    In this paper, using a resonance-enhanced piezoresponse force microscopy approach supported by density functional theory computer simulations, we have demonstrated the ferroelectric switching in epitaxial GeTe films. It has been shown that in films with thickness on the order of several nanometers reversible reorientation of polarization occurs due to swapping of the shorter and longer Ge-Te bonds in the interior of the material. It is also hinted that for ultra thin films consisting of just several atomic layers weakly bonded to the substrate, ferroelectric switching may proceed through exchange of Ge and Te planes within individual GeTe layers

    Spatial antibunching of photons with parametric down-conversion

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    The theoretical framework behind a recent experiment by Nogueira et. al. [Phys. Rev. Lett. 86}, 4009 (2001)] of spatial antibunching in a two-photon state generated by collinear type II parametric down-conversion and a birefringent double-slit is presented. The fourth-order quantum correlation function is evaluated and shown to violate the classical Schwarz-type inequality, ensuring that the field does not have a classical analog. We expect these results to be useful in the rapidly growing fields of quantum imaging and quantum information.Comment: 5 pages, 3 figures. Minor changes made, accepted for publication in PR

    Non-local model of hollow cathode and glow discharge - theory calculations and experiment comparison

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    General form of the non-local equation for an ionization source in glow discharge and hollow cathode 3D-simulation is formulated. It is a fundamental equation in a hollow cathode theory, which allows to make up a complete set of field equations for a self-consistent problem in a stationary glow discharge and a hollow cathode. It enables to describe adequately the region of negative glow and the hollow cathode effect. Here you can see first attempts to compare calculation results of electrical dependences (pressure - voltage) and experimental data, - under conditions of gradual appearance of the hollow cathode effect.Comment: 4 pages, 2 figure

    Multi-photon, multi-mode polarization entanglement in parametric down-conversion

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    We study the quantum properties of the polarization of the light produced in type II spontaneous parametric down-conversion in the framework of a multi-mode model valid in any gain regime. We show that the the microscopic polarization entanglement of photon pairs survives in the high gain regime (multi-photon regime), in the form of nonclassical correlation of all the Stokes operators describing polarization degrees of freedom

    A toy model of fractal glioma development under RF electric field treatment

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    A toy model for glioma treatment by a radio frequency electric field is suggested. This low-intensity, intermediate-frequency alternating electric field is known as the tumor-treating-field (TTF). In the framework of this model the efficiency of this TTF is estimated, and the interplay between the TTF and the migration-proliferation dichotomy of cancer cells is considered. The model is based on a modification of a comb model for cancer cells, where the migration-proliferation dichotomy becomes naturally apparent. Considering glioma cancer as a fractal dielectric composite of cancer cells and normal tissue cells, a new effective mechanism of glioma treatment is suggested in the form of a giant enhancement of the TTF. This leads to the irreversible electroporation that may be an effective non-invasive method of treating brain cancer.Comment: Submitted for publication in European Physical Journal

    Transition from Townsend to glow discharge: subcritical, mixed or supercritical

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    The full parameter space of the transition from Townsend to glow discharge is investigated numerically in one space dimension in the classical model: with electrons and positive ions drifting in the local electric field, impact ionization by electrons (Ξ±\alpha process), secondary electron emission from the cathode (Ξ³\gamma process) and space charge effects. We also perform a systematic analytical small current expansion about the Townsend limit up to third order in the total current that fits our numerical data very well. Depending on Ξ³\gamma and system size pd, the transition from Townsend to glow discharge can show the textbook subcritical behavior, but for smaller values of pd, we also find supercritical or some intermediate ``mixed'' behavior. The analysis in particular lays the basis for understanding the complex spatio-temporal patterns in planar barrier discharge systems.Comment: 12 pages, 10 figures, submitted to Phys. Rev.

    Π­ΠšΠ‘ΠŸΠ•Π Π˜ΠœΠ•ΠΠ’ΠΠ›Π¬ΠΠΠ― ΠžΠ¦Π•ΠΠšΠ ΠšΠžΠœΠŸΠžΠ—Π˜Π¦Π˜ΠžΠΠΠžΠ“Πž ΠœΠΠ’Π•Π Π˜ΠΠ›Π НА ΠžΠ‘ΠΠžΠ’Π• Π‘Π•Π›ΠšΠžΠ’Πž-ΠœΠ˜ΠΠ•Π ΠΠ›Π¬ΠΠ«Π₯ ΠšΠžΠœΠŸΠžΠΠ•ΠΠ’ΠžΠ’ И Π Π•ΠšΠžΠœΠ‘Π˜ΠΠΠΠ’ΠΠžΠ“Πž ΠšΠžΠ‘Π’ΠΠžΠ“Πž ΠœΠžΠ Π€ΠžΠ“Π•ΠΠ•Π’Π˜Π§Π•Π‘ΠšΠžΠ“Πž Π‘Π•Π›ΠšΠ-2 Π’ ΠšΠΠ§Π•Π‘Π’Π’Π• ПОКРЫВИЯ Π’Π˜Π’ΠΠΠžΠ’Π«Π₯ Π˜ΠœΠŸΠ›ΠΠΠ’ΠΠ’ΠžΠ’

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    The influence of both, the composite material based on the protein-mineral components including the prolonged form of theΒ recombinant human bone morphogenetic protein 2 (rhBMP-2) and the method of the titanium implant’s surface treatment,Β on the reparative osteogenesis and adhesion strength of the bone tissue – implant’s surface contact was evaluated. CoveringΒ of implants with the composite coating promotes significant acceleration of the bone tissue regeneration processes in the siteΒ of implants loading. The composition coating with prolonged form of the rhBMP-2 promoted increasing of the neogenic boneΒ tissue’s adhesion with the implants, as compared with the coating without recombinant human bone morphogenetic protein. TheΒ implants treated with microarc oxidation demonstrated higher values of the breakout force during the separation of the implantsΒ from the bone than the implants treated with sandblasting method.ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π° ΠΎΡ†Π΅Π½ΠΊΠ° влияния ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ†ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° Π½Π° основС Π±Π΅Π»ΠΊΠΎΠ²ΠΎ-ΠΌΠΈΠ½Π΅Ρ€Π°Π»ΡŒΠ½Ρ‹Ρ… ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚ΠΎΠ², ΡΠΎΠ΄Π΅Ρ€ΠΆΠ°Ρ‰Π΅Π³ΠΎΒ ΠΏΡ€ΠΎΠ»ΠΎΠ½Π³ΠΈΡ€ΠΎΠ²Π°Π½Π½ΡƒΡŽ Ρ„ΠΎΡ€ΠΌΡƒ Ρ€Π΅ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Π½Ρ‚Π½ΠΎΠ³ΠΎ костного морфогСнСтичСского Π±Π΅Π»ΠΊΠ°-2 Ρ‡Π΅Π»ΠΎΠ²Π΅ΠΊΠ° (rhΠ’ΠœΠ -2), ΠΈ способа ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ повСрхности Ρ‚ΠΈΡ‚Π°Π½ΠΎΠ²ΠΎΠ³ΠΎ ΠΈΠΌΠΏΠ»Π°Π½Ρ‚Π°Ρ‚Π° Π½Π° Ρ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΈΠ²Π½Ρ‹ΠΉ остСогСнСз ΠΈ Π°Π΄Π³Π΅Π·ΠΈΠΎΠ½Π½ΡƒΡŽ ΠΏΡ€ΠΎΡ‡Π½ΠΎΡΡ‚ΡŒ ΠΊΠΎΠ½Ρ‚Π°ΠΊΡ‚Π° костной ткани с ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½ΠΎΡΡ‚ΡŒΡŽ ΠΈΠΌΠΏΠ»Π°Π½Ρ‚Π°Ρ‚Π°. НанСсСниС Π½Π° ΠΈΠΌΠΏΠ»Π°Π½Ρ‚Π°Ρ‚Ρ‹ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ†ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚Π°/покрытия способствовало Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΌΡƒ ΡƒΡΠΊΠΎΡ€Π΅Π½ΠΈΡŽ процСссов Ρ€Π΅Π³Π΅Π½Π΅Ρ€Π°Ρ†ΠΈΠΈ костной Ρ‚ΠΊΠ°Π½ΠΈ Π² мСстС ввСдСния ΠΈΠΌΠΏΠ»Π°Π½Ρ‚Π°Ρ‚ΠΎΠ². ΠšΠΎΠΌΠΏΠΎΠ·ΠΈΡ†ΠΈΠΎΠ½Π½ΠΎΠ΅ ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠ΅ с ΠΏΡ€ΠΎΠ»ΠΎΠ½Π³ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠΉ Ρ„ΠΎΡ€ΠΌΠΎΠΉ rhBMP-2, способствовало ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΡŽ Π°Π΄Π³Π΅Π·ΠΈΠΎΠ½Π½Ρ‹Ρ… связСй Π½ΠΎΠ²ΠΎΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½Π½ΠΎΠΉ костной Ρ‚ΠΊΠ°Π½ΠΈ с ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½ΠΎΡΡ‚ΡŒΡŽ ΠΎΠ±Ρ€Π°Π·Ρ†ΠΎΠ² ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠ΅ΠΌ, Π½Π΅ содСрТащим Ρ€Π΅ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Π½Ρ‚Π½ΠΎΠ³ΠΎ костного морфогСнСтичСского Π±Π΅Π»ΠΊΠ°.Β Π˜ΠΌΠΏΠ»Π°Π½Ρ‚Π°Ρ‚Ρ‹ с ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½ΠΎΡΡ‚ΡŒΡŽ, ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚Π°Π½Π½ΠΎΠΉ с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ ΠΌΠΈΠΊΡ€ΠΎΠ΄ΡƒΠ³ΠΎΠ²ΠΎΠ³ΠΎ оксидирования, дСмонстрировали Π±ΠΎΠ»Π΅Π΅ высокиС значСния Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Ρ‹ усилия ΠΎΡ‚Ρ€Ρ‹Π²Π° ΠΈΠΌΠΏΠ»Π°Π½Ρ‚Π°Ρ‚Π° ΠΎΡ‚ кости, Ρ‡Π΅ΠΌ ΠΌΠΎΠ΄ΠΈΡ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Π΅ пСскоструйной ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΎΠΉ

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