13 research outputs found

    Friction and Wear Characteristics of C/Si Bi-layer Coatings Deposited on Silicon Substrate by DC Magnetron Sputtering

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    The tribological behavior of carbon/silicon bi-layer coatings deposited on a silicon substrate by DC magnetron sputtering was assessed and compared to that of amorphous carbon and silicon coatings. The motivation was to develop a wear resistant coating for silicon using thin layers of amorphous carbon and silicon. Wear tests were conducted by sliding a stainless steel ball against the coating specimens under applied normal loads in the range of 20 * 50 mN. Results showed that the wear rate of the bi-layer coating was strongly dependent on the ratio of thickness between the carbon and silicon layers. The wear rate of the bi-layer coating with 25 nm thick carbon and 102 nm thick silicon layers was about 48 and 20 times lower than that of the single-layer amorphous carbon and amorphous silicon coating, respectively. In addition, the steady-state friction coefficient of the bi-layer coating could be decreased to 0.09 by optimizing the thickness of the layer. Finally, a model for the wear reduction mechanism of the carbon/silicon bi-layer coating was proposed

    Fabrication and characterization of a new high density Sc/Si multilayer sliced grating

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    State of the art soft x-ray spectroscopy techniques like Resonant Inelastic X-ray Scattering (RIXS) require diffraction gratings which can provide extremely high spectral resolution of 105-106. This problem may be addressed with a sliced multilayer grating with an ultra-high groove density (up to 50,000 mm-1) proposed in the recent publication [Voronov, D. L., Cambie, R., Feshchenko, R. M., Gullikson, E., Padmore, H. A., Vinogradov, A. V., Yashchuk, V. V., Proc. SPIE 6705, 67050E (2007)]. It has been suggested to fabricate such a grating by deposition of a soft x-ray multilayer on a substrate which is a blazed saw-tooth grating (echellette) with low groove density. Subsequent polishing applied to the coated grating removes part of the coating and forms an oblique-cut multiline structure that is a sliced multilayer grating. The resulting grating has a short-scale periodicity of lines (bilayers), which is defined by the multilayer period and the oblique-cut angle. We fabricated and tested a Sc/Si multilayer sliced grating suitable for EUV applications, which is a first prototype based on the suggested technique. In order to fabricate an echellette substrate, we used anisotropic KOH etching of a Si wafer. The etching regime was optimized to obtain smooth and flat echellette facets. A Sc/Si multilayer was deposited by dc-magnetron sputtering, and after that it was mechanically polished using a number of diamond pastes. The resulting sliced grating prototype with ~;;270 nm line period has demonstrated a dispersive ability in the 41-49 nm photon wavelength range with a diffraction efficiency of ~;;7percent for the optimized 38th order assigned to the echellette grating of 10 mu m period

    Effect of working gas pressure on interlayer mixing in magnetron-deposited Mo/Si multilayers

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    By methods of cross-sectional transmission electron microscopy and small-angle x-ray scattering (Ξ» = 0.154 nm) the influence of Ar gas pressure (1 to 4 mTorr) on the growth of amorphous interfaces in Mo/Si multilayers (MLs) deposited by DC magnetron sputtering is studied. The significant reduction in the ML period, which is evident as a volumetric contraction, is observed in MLs deposited at Ar pressure where the mean-free path for the sputtered atoms is comparable with the magnetronsubstrate distance. Some reduction in the thickness of the amorphous interlayers with Ar pressure increase is found, where the composition of the interlayers is enriched with molybdenum. The interface modification resulted in an increase in EUV reflectance of the Mo/Si ML

    БВРУКВУРА И Π€ΠΠ—ΠžΠ’Π«Π™ Π‘ΠžΠ‘Π’ΠΠ’ ΠœΠΠžΠ“ΠžΠ‘Π›ΠžΠ™ΠΠ«Π₯ Π Π•ΠΠ’Π“Π•ΠΠžΠ’Π‘ΠšΠ˜Π₯ Π—Π•Π ΠšΠΠ› W-Si

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    ΠœΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ рСнтгСновской Π΄ΠΈΡ„Ρ€Π°ΠΊΡ‚ΠΎΠΌΠ΅Ρ‚Ρ€ΠΈΠΈ Π² ТСсткой области (l~0,154 Π½ΠΌ) исслСдована фазовая структура, состав ΠΈ строСниС многослойных рСнтгСновских Π·Π΅Ρ€ΠΊΠ°Π» (ΠœΠ Π—) W/Si с Ρ‚ΠΎΠ»Ρ‰ΠΈΠ½ΠΎΠΉ слоСв Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠ° tW2,7 Π½ΠΌ слои Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠ° ΠΈΠΌΠ΅ΡŽΡ‚ ΠΏΠΎΠ»ΠΈΠΊΡ€ΠΈΡΡ‚Π°Π»Π»ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ (ОЦК) структуру, Π° ΠΏΡ€ΠΈ tW<1,9 Π½ΠΌ ΠΎΠ½ΠΈ Π°ΠΌΠΎΡ€Ρ„Π½Ρ‹. ΠŸΡ€ΠΈ ΠΏΠΎΠΌΠΎΡ‰ΠΈ sin2Y-ΠΌΠ΅Ρ‚ΠΎΠ΄Π° установлСно, Ρ‡Ρ‚ΠΎ Π² Ρ‚ΠΎΠ½ΠΊΠΈΡ… кристалличСских слоях Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠ° (tW<10 Π½ΠΌ) ΠΌΠΎΠΆΠ΅Ρ‚ ΡΠΎΠ΄Π΅Ρ€ΠΆΠ°Ρ‚ΡŒΡΡ Π±ΠΎΠ»Π΅Π΅ 3 Π°Ρ‚.% Si. Π Π°ΡΡ‚ΡΠ³ΠΈΠ²Π°ΡŽΡ‰ΠΈΠ΅ напряТСния Π² слоях кристалличСского Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠ° Π½Π΅ ΠΏΡ€Π΅Π²Ρ‹ΡˆΠ°ΡŽΡ‚ 1,1 Π“ΠŸΠ°. ΠŸΠΎΡΡ‚Ρ€ΠΎΠ΅Π½ΠΈΠ΅ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΉ Ρ€Π°Π΄ΠΈΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ распрСдСлСния Π°Ρ‚ΠΎΠΌΠΎΠ² ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΎ ΡƒΡΡ‚Π°Π½ΠΎΠ²ΠΈΡ‚ΡŒ, Ρ‡Ρ‚ΠΎ Π°ΠΌΠΎΡ€Ρ„Π½Ρ‹Π΅ слои Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠ° ΠΈΠΌΠ΅ΡŽΡ‚ располоТСниС Π°Ρ‚ΠΎΠΌΠΎΠ², Π±Π»ΠΈΠ·ΠΊΠΎΠ΅ ΠΊ b-W. Π’ΠΎ всСх ΠΎΠ±Ρ€Π°Π·Ρ†Π°Ρ… Π·Π° счСт взаимодСйствия Π½Π° ΠΌΠ΅ΠΆΡ„Π°Π·Π½Ρ‹Ρ… Π³Ρ€Π°Π½ΠΈΡ†Π°Ρ… Π½Π°Π±Π»ΡŽΠ΄Π°Π΅Ρ‚ΡΡ Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ силицидных прослоСк, Π² Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π΅ Ρ‡Π΅Π³ΠΎ Ρ€Π΅Π°Π»ΡŒΠ½Π°Ρ Ρ‚ΠΎΠ»Ρ‰ΠΈΠ½Π° слоСв Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠ° мСньшС номинальной. АморфныС силицидныС прослойки, ΠΎΠ±ΡΠ·Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎ Ρ„ΠΎΡ€ΠΌΠΈΡ€ΡƒΡŽΡ‰ΠΈΠ΅ΡΡ Π½Π° стадии изготовлСния ΠœΠ Π—, содСрТат дисилицид Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠ°. Π’ зависимости ΠΎΡ‚ скорости осаТдСния дисилицид ΠΌΠΎΠΆΠ΅Ρ‚ ΠΈΠΌΠ΅Ρ‚ΡŒ располоТСниС Π°Ρ‚ΠΎΠΌΠΎΠ², Π±Π»ΠΈΠ·ΠΊΠΎΠ΅ Π»ΠΈΠ±ΠΎ ΠΊ Ρ‚Π΅Ρ‚Ρ€Π°Π³ΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠΉ Ρ„Π°Π·Π΅, t-WSi2 (~0,6 Π½ΠΌ/с.), Π»ΠΈΠ±ΠΎ ΠΊ гСксагональной Ρ„Π°Π·Π΅, h-WSi2 (~0,15 Π½ΠΌ/с.). ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Π° уточнСнная модСль строСния Π°ΠΌΠΎΡ€Ρ„Π½Ρ‹Ρ… ΠœΠ Π— W/Si. ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Ρ‹ ΠΌΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌΡ‹ формирования силицидных прослоСк, согласно ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΌ Π½ΠΈΠΆΠ½ΠΈΠ΅ силицидныС прослойки (W-Π½Π°-Si) Ρ„ΠΎΡ€ΠΌΠΈΡ€ΡƒΡŽΡ‚ΡΡ прСимущСствСнно Π·Π° счСт баллистичСского ΠΏΠ΅Ρ€Π΅ΠΌΠ΅ΡˆΠΈΠ²Π°Π½ΠΈΡ Π°Ρ‚ΠΎΠΌΠΎΠ² Π²ΠΎΠ»ΡŒΡ„Ρ€Π°ΠΌΠ° ΠΈ крСмния, Π° Π²Π΅Ρ€Ρ…Π½ΠΈΠ΅ – вслСдствиС Π΄ΠΈΡ„Ρ„ΡƒΠ·ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΠ΅Ρ€Π΅ΠΌΠ΅ΡˆΠΈΠ²Π°Π½ΠΈΡ. Π‘Π΄Π΅Π»Π°Π½Π° ΠΎΡ†Π΅Π½ΠΊΠ° коэффициСнтов Π²Π·Π°ΠΈΠΌΠ½ΠΎΠΉ Π΄ΠΈΡ„Ρ„ΡƒΠ·ΠΈΠΈ, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΈ ΡƒΡΡ‚Π°Π½ΠΎΠ²ΠΈΡ‚ΡŒ, Ρ‡Ρ‚ΠΎ осаТдаСмая ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½ΠΎΡΡ‚ΡŒ слоСв ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ Ρ€Π°Π·ΠΎΠ³Ρ€Π΅Ρ‚Π°, ΠΏΠΎ мСньшСй ΠΌΠ΅Ρ€Π΅, Π½Π° 250Β° Π²Ρ‹ΡˆΠ΅ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠΈ. ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Ρ‹ ΠΏΡƒΡ‚ΠΈ сниТСния ΠΌΠ΅ΠΆΡ„Π°Π·Π½ΠΎΠ³ΠΎ взаимодСйствия

    Problems of protection of urban ambient air pollution from industrial dust emissions

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    The development of large cities accompanied by the development of the industry hashistorically led to the fact that now residential areas are located side by side with the industrial production. For instance, exactly this situation has developed in the city of Volgograd, as well as in other Russian cities, where sometimes the distance from large enterprises to a living area is 100 m or less. In addition, small-scale entrepreneurs usually place their production directly in their past places of residence. As a result, the content of harmful substances in the air of city blocks is much higher than the standards of hygiene require. It is obvious that the current situation can be improved through the use of modern, more advanced technologies. However, increasing the efficiency of air systems to protect the city from pollution and industrial emissions is an urgent task. The authors propose a version of the system layout, designed to reduce dust emissions in urban air

    Problems of protection of urban ambient air pollution from industrial dust emissions

    No full text
    The development of large cities accompanied by the development of the industry hashistorically led to the fact that now residential areas are located side by side with the industrial production. For instance, exactly this situation has developed in the city of Volgograd, as well as in other Russian cities, where sometimes the distance from large enterprises to a living area is 100 m or less. In addition, small-scale entrepreneurs usually place their production directly in their past places of residence. As a result, the content of harmful substances in the air of city blocks is much higher than the standards of hygiene require. It is obvious that the current situation can be improved through the use of modern, more advanced technologies. However, increasing the efficiency of air systems to protect the city from pollution and industrial emissions is an urgent task. The authors propose a version of the system layout, designed to reduce dust emissions in urban air
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