30 research outputs found

    Self-Organization of a 2D Lattice on a Surface of Ge Single Crystal after Irradiation with Yag: ND Laser

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    Experimentally observed self-organization of a 2D lattice on the surface of Ge single crystal after irradiation by pulsed YAG: Nd laser is repoted. The calculation of time depended distribution of temperature in bulk of the Ge sample show that overheating of the crystal lattice occurs at laser radiation intensities exceeding 30MW/cm2.The two temperature gradients are exists.Comment: Submitted on behalf of TIMA Editions (http://irevues.inist.fr/tima-editions

    MODIFICATION OF BAND-GAP IN SURFACE LAYER OF CDZNTE BY YAG:Nd+3 LASER RADIATION

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    According to the effect, the interstitial atoms of Cd (Cdi) in Cd1-xZnxTe move along the temperature gradient while the Cd vacancies (VCd) and Zn atoms - in the opposite direction, into the bulk of the semiconductor where temperature is lower. Photoluminescence spectra studied at 5 K show that concentration of Cd atoms increases, but concentration of Zn atoms decreases at the surface due to redistribution atoms in temperature gradient of field. Formation of a graded band gap in Cd1- xZnxTe crystal at irradiation by the second harmonic of Nd:YAG laser is found

    Properties of nanocones formed on a surface of semiconductors by laser radiation: quantum confinement effect of electrons, phonons, and excitons

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    On the basis of the analysis of experimental results, a two-stage mechanism of nanocones formation on the irradiated surface of semiconductors by Nd:YAG laser is proposed for elementary semiconductors and solid solutions, such as Si, Ge, SiGe, and CdZnTe. Properties observed are explained in the frame of quantum confinement effect. The first stage of the mechanism is characterized by the formation of a thin strained top layer, due to redistribution of point defects in temperature-gradient field induced by laser radiation. The second stage is characterized by mechanical plastic deformation of the stained top layer leading to arising of nanocones, due to selective laser absorption of the top layer. The nanocones formed on the irradiated surface of semiconductors by Nd:YAG laser possessing the properties of 1D graded bandgap have been found for Si, Ge, and SiGe as well, however QD structure in CdTe was observed. The model is confirmed by "blue shift" of bands in photoluminescence spectrum, "red shift" of longitudinal optical line in Raman back scattering spectrum of Ge crystal, appearance of Ge phase in SiGe solid solution after irradiation by the laser at intensity 20 MW/cm2, and non-monotonous dependence of Si crystal micro-hardness as function of the laser intensity

    Π‘Π˜ΠΠ’Π•Π— И БВРУКВУРА Π“ΠΠ—ΠžΠ§Π£Π’Π‘Π’Π’Π˜Π’Π•Π›Π¬ΠΠ«Π₯ ΠšΠžΠœΠŸΠžΠ—Π˜Π’ΠΠ«Π₯ ΠœΠΠ’Π•Π Π˜ΠΠ›ΠžΠ’ TIO2–MoO3

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    Introduction of molybdenum trioxide to gas sensing materials based on titanium dioxide results in a considerable increase of the output signal in the hydrogen-air environment. It is established that the value of the output signal reaches the maximum at the 1 mol. % MoO3 content in the composite material. Improved gas sensing characteristics of TiO2:MoO3 composite correlate with the structural and phase peculiarities of this system – the inhibition of TiO2 crystallization in the TiO2:MoO3 system, the shift of anatase-rutile phase transition to the higher temperature area in comparison with the temperature of this transition in unloaded TiO2, and with the presence of different types of tetrahonal distortions in MoO6 octahedrons, which ensures the MoO3 lattice high activity in the processes of hydrogen catalytic oxidation, and also with the crystallization of highly dispersed molybdenum oxide with a particle size of 10 nm.Π’Π²Π΅Π΄Π΅Π½ΠΈΠ΅ Π»Π΅Π³ΠΈΡ€ΡƒΡŽΡ‰ΠΈΡ… Π΄ΠΎΠ±Π°Π²ΠΎΠΊ оксида ΠΌΠΎΠ»ΠΈΠ±Π΄Π΅Π½Π° Π² состав Π³Π°Π·ΠΎΡ‡ΡƒΠ²ΡΡ‚Π²ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² Π½Π° основС диоксида Ρ‚ΠΈΡ‚Π°Π½Π° ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΌΡƒ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΡŽ Π²Ρ‹Ρ…ΠΎΠ΄Π½ΠΎΠ³ΠΎ сигнала Π² Π²ΠΎΠ΄ΠΎΡ€ΠΎΠ΄ΠΎ-Π²ΠΎΠ·Π΄ΡƒΡˆΠ½ΠΎΠΉ срСдС. УстановлСно, Ρ‡Ρ‚ΠΎ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Π° Π²Ρ‹Ρ…ΠΎΠ΄Π½ΠΎΠ³ΠΎ сигнала максимальна ΠΏΡ€ΠΈ содСрТании 1 ΠΌΠΎΠ». % МоО3 Π² ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚Π½ΠΎΠΌ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π΅. Π£Π»ΡƒΡ‡ΡˆΠ΅Π½Π½Ρ‹Π΅ Π³Π°Π·ΠΎΡ‡ΡƒΠ²ΡΡ‚Π²ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ характСристики ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚Π° TiO2–MoO3 с 1 ΠΌΠΎΠ». % МоО3 ΠΊΠΎΡ€Ρ€Π΅Π»ΠΈΡ€ΡƒΡŽΡ‚ со структурно-Ρ„Π°Π·ΠΎΠ²Ρ‹ΠΌΠΈ особСнностями Π΄Π°Π½Π½ΠΎΠΉ систСмы – ΠΏΠΎΠ΄Π°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ кристаллизации диоксида Ρ‚ΠΈΡ‚Π°Π½Π° Π² систСмС TiO2–MoO3, смСщСниСм Ρ„Π°Π·ΠΎΠ²ΠΎΠ³ΠΎ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π° анатаз–рутил Π² ΠΎΠ±Π»Π°ΡΡ‚ΡŒ Π±ΠΎΠ»ΡŒΡˆΠΈΡ… Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€ ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€ΠΎΠΉ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π° для Π½Π΅Π»Π΅Π³ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ диоксида Ρ‚ΠΈΡ‚Π°Π½Π°, Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ΠΌ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… Ρ‚ΠΈΠΏΠΎΠ² Ρ‚Π΅Ρ‚Ρ€Π°Π³ΠΎΠ½Π°Π»ΡŒΠ½Ρ‹Ρ… искаТСний Π² октаэдрах МоО6 ΠΏΠΎ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹ΠΌ направлСниям, ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°ΡŽΡ‰ΠΈΡ… Π²Ρ‹ΡΠΎΠΊΡƒΡŽ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ кислорода Ρ€Π΅ΡˆΠ΅Ρ‚ΠΊΠΈ МоО3 Π² процСссах каталитичСского окислСния адсорбированных ΠΌΠΎΠ»Π΅ΠΊΡƒΠ» Π²ΠΎΠ΄ΠΎΡ€ΠΎΠ΄Π°, Π° Ρ‚Π°ΠΊΠΆΠ΅ кристаллизациСй высокодиспСрсного оксида ΠΌΠΎΠ»ΠΈΠ±Π΄Π΅Π½Π° с Ρ€Π°Π·ΠΌΠ΅Ρ€ΠΎΠΌ частиц порядка 10 Π½ΠΌ

    ИсслСдованиС ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Π°Ρ‚ΠΎΠΌΠ½ΠΎ-силовой микроскопии влияния наночастиц Π½Π° структурныС ΠΈ мСханичСскиС свойства ΠΊΠ»Π΅Ρ‚ΠΎΠΊ ΠΏΠΎΡ‡ΠΊΠΈ Π±Ρ‹ΠΊΠ° Π»ΠΈΠ½ΠΈΠΈ MDBK

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    The effect of copper and silver nanoparticles Cu+Ag, silver nitrite AgNO3 and zinc oxide ZnO on morphology and mechanical properties of immunocompetent cells bovine kidney line MDBK is investigated by atomic force microscopy. The results of calculation of the local elastic modulus, strength, surface cell adhesion, adhesion work, and the three-dimensional image analysis of cells in control and after incubation with the nanoparticles bioelements for 20 min are presented.ΠœΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Π°Ρ‚ΠΎΠΌΠ½ΠΎ-силовой микроскопии (АБМ) исслСдовано влияниС наночастиц ΠΌΠ΅Π΄ΠΈ ΠΈ сСрСбра Cu+Ag, Π½ΠΈΡ‚Ρ€ΠΈΡ‚Π° сСрСбра AgNO3 ΠΈ оксида Ρ†ΠΈΠ½ΠΊΠ° ZnO Π½Π° ΠΌΠΎΡ€Ρ„ΠΎΠ»ΠΎΠ³ΠΈΡŽ ΠΈ мСханичСскиС свойства ΠΈΠΌΠΌΡƒΠ½ΠΎΠΊΠΎΠΌΠΏΠ΅Ρ‚Π΅Π½Ρ‚Π½Ρ‹Ρ… ΠΊΠ»Π΅Ρ‚ΠΎΠΊ ΠΏΠΎΡ‡ΠΊΠΈ Π±Ρ‹ΠΊΠ° Π»ΠΈΠ½ΠΈΠΈ MDBK. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Ρ‹ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ расчСтов локального модуля упругости, силы повСрхностной Π°Π΄Π³Π΅Π·ΠΈΠΈ ΠΊΠ»Π΅Ρ‚ΠΎΠΊ, Ρ€Π°Π±ΠΎΡ‚Ρ‹ Π°Π΄Π³Π΅Π·ΠΈΠΈ, Π° Ρ‚Π°ΠΊΠΆΠ΅ Π°Π½Π°Π»ΠΈΠ·Π° Ρ‚Ρ€Π΅Ρ…ΠΌΠ΅Ρ€Π½Ρ‹Ρ… ΠΈΠ·ΠΎΠ±Ρ€Π°ΠΆΠ΅Π½ΠΈΠΉ ΠΊΠ»Π΅Ρ‚ΠΎΠΊ Π² ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»Π΅ ΠΈ послС ΠΈΠ½ΠΊΡƒΠ±Π°Ρ†ΠΈΠΈ с наночастицами биоэлСмСнтов Π² Ρ‚Π΅Ρ‡Π΅Π½ΠΈΠ΅ 20 ΠΌΠΈΠ½
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