115 research outputs found

    Cooperative localization-delocalization in the high Tc cuprates

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    The intrinsic metastable crystal structure of the cuprates results in local dynamical lattice instabilities, strongly coupled to the density fluctuations of the charge carriers. They acquire in this way simultaneously both, delocalized and localized features. It is responsible for a partial fractioning of the Fermi surface, i.e., the Fermi surface gets hidden in a region around the anti-nodal points, because of the opening of a pseudogap in the normal state, arising from a partial charge localization. The high energy localized single-particle features are a result of a segregation of the homogeneous crystal structure into checker-board local nano-size structures, which breaks the local translational and rotational symmetry. The pairing in such a system is dynamical rather than static, whereby charge carriers get momentarily trapped into pairs in a deformable dynamically fluctuating ligand environment. We conclude that the intrinsically heterogeneous structure of the cuprates must play an important role in this type of superconductivity.Comment: 14 pages, 8 figures, Proceedings of the "International Conference on Condensed Matter Theories", Quito, 2009 Int. J. Mod. Phys. B 2010 (Accepted

    Superconductivity in charge Kondo systems

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    We present a theory of superconductivity in charge Kondo systems, materials with resonant quantum valence fluctuations, in the regime where the transition temperature is comparable to the charge Kondo resonance. We find superconductivity induced by charge Kondo impurities, study how pairing of a superconducting host is enhanced due to charge Kondo centers and investigate the interplay between Kondo-scattering and inter-impurity Josephson coupling. We discuss the implications of our theory for Tl-doped PbTe, which has recently been identified as a candidate charge Kondo system.Comment: 4 pages, 4 figures; revised version; detailed discussion on the physics of Tl-doped PbTe adde

    Charge Kondo anomalies in PbTe doped with Tl impurities

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    We investigate the properties of PbTe doped with a small concentration xx of Tl impurities acting as acceptors and described by Anderson impurities with negative onsite correlation energy. We use the numerical renormalization group method to show that the resulting charge Kondo effect naturally accounts for the unusual low temperature and doping dependence of normal state properties, including the self-compensation effect in the carrier density and the non-magnetic Kondo anomaly in the resistivity. These are found to be in good qualitative agreement with experiment. Our results for the Tl s-electron spectral function provide a new interpretation of point contact data.Comment: 5 pages, 3 figures; published versio

    Sedimentation of Ultradispersed Diamonds in the Citrate Copper-Plating Electrolyte

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    Abstractβ€”The aggregation and sedimentation of ultradispersed diamonds (UDDs) in a citrate copper-plating electrolyte (CCPE) used to fabricate composite electrochemical coatings are investigated. The sedimentation and aggregation stability is investigated in order to select the UDD concentration in the CCPE. This is necessary to fabricate composite copper coatings with improved operational characteristics (increased hardness, wear resistance, and corrosion resistance), as well as impart them new properties (antifriction and catalytic). The UDD content in the electrolyte varies in limits from 0.2 to 2.0 g/L. The size distribution of the UDD particles in the electrolyte immediately after the suspension preparation and after the 10-day holding is determined using a Malvern Mastersizer 2000 laser diffraction analyzer. The aggregation and sedimentation stability of the UDD suspension in the CCPE is investigated by the gravimetric method with the continuous weighing of a quartz small cap immersed into this suspension. The quartz cap is associated with a Sartorius R200D analytical balance with the help of a quartz wire. The experimentally determined time dependence of the weight of settling UDD particles is Q = f(t). The relative size distribution of the particles is determined from this dependence. It is established that the sedimentation stability is substantially affected by the aggregation of the particles, the intensity of which increases with an increase in the UDD concentration. The results satisfying the requirements on the aggregation and sedimentation stability are found for the UDD suspension in the CCPE with a concentration of 1.0 g/L. In this case, the high content of the dispersed phase is combined with aggregation and sedimentation stability, which makes it possible to fabricate copper composite coatings with improved operational properties. Β© 2019, Allerton Press, Inc

    Optimization of PET ion-track membranes parameters

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    Nowadays polymer ion-track membranes are used for a wide range of practical applications, which include various levels of filtration (micro-, ultra-, nanofiltration and osmosis), the creation of flexible electronic circuits and sensors based on polymer substrate, and using as templates for shape-controlled nanostructures synthesis. New applications demand clear understanding of the processes that occur during track membranes formation. For high-precision control of the end-product parameters, it is necessary to establish the correlation between etching conditions and track membranes characteristics (pores dimensions, porosity and membranes thicknesses). For this purpose, in the paper it is considered the technique of membranes formation with 10 nm - 10 ΞΌm cylindrical pores and correlation between their parameters and processing modes is studied. Β© 2019 Elsevier Ltd

    ВлияниС Ρ†ΠΈΡ‚Ρ€Π°Ρ‚Π½ΠΎΠ³ΠΎ элСктролита мСднСния, Π΅Π³ΠΎ ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚ΠΎΠ² ΠΈ Π΄ΠΎΠ±Π°Π²ΠΎΠΊ ΡƒΠ»ΡŒΡ‚Ρ€Π°Π΄ΠΈΡΠΏΠ΅Ρ€ΡΠ½Ρ‹Ρ… Π°Π»ΠΌΠ°Π·ΠΎΠ² Π½Π° повСрхностныС свойства стали

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    The state of the steel substrate (steel 3) was studied before the application of composite copper coatings from citrate copper-plating electrolyte. The properties of steel base in the investigated copper-plating electrolyte with the addition of ultradispersed diamonds (UDD) have been studied. A component-by-component analysis of the citrate copper-plating electrolyte was carried out, and the effect of each component on the properties of the steel electrode was evaluated. The possibility of using the considered electrolyte for coating directly on steel is shown, which significantly distinguishes it from currently used ethylenediamine, pyrophosphate, acid and other electrolytes. Electrochemical impedance spectroscopy and cathodic polarization were used as research methods. It was found that the lowest resistance of the steel surface (about 15 Ξ©) corresponded to the sample immersed in citrate copper-plating electrolyte with the addition of 1.0 g/l of UDD. Diffusion current density for suspensions with 1.0 g/l UDD in citrate copper-plating electrolyte was 2.6 A/dm2. Ultradispersed diamonds in citrate copper-plating electrolyte shielded the surface of the steel sample, while reducing the total resistance of the passive layer of steel 3. Equivalent electrical circuits of the surface of steel samples immersed in citrate copper-plating electrolyte and its components are also presented. Β ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½Ρ‹ исслСдования состояния ΡΡ‚Π°Π»ΡŒΠ½ΠΎΠΉ ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠΈ (Π‘Ρ‚ 3) ΠΏΠ΅Ρ€Π΅Π΄ нанСсСниСм ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ†ΠΈΠΎΠ½Π½Ρ‹Ρ… ΠΌΠ΅Π΄Π½Ρ‹Ρ… ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ ΠΈΠ· Ρ†ΠΈΡ‚Ρ€Π°Ρ‚Π½ΠΎΠ³ΠΎ элСктролита мСднСния. Π˜Π·ΡƒΡ‡Π΅Π½Ρ‹ свойства ΡΡ‚Π°Π»ΡŒΠ½ΠΎΠΉ основы Π² исслСдуСмом элСктролитС мСднСния с Π΄ΠΎΠ±Π°Π²ΠΊΠΎΠΉ ΡƒΠ»ΡŒΡ‚Ρ€Π°Π΄ΠΈΡΠΏΠ΅Ρ€ΡΠ½Ρ‹Ρ… Π°Π»ΠΌΠ°Π·ΠΎΠ² (УДА). ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ ΠΏΠΎΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½Ρ‹ΠΉ Π°Π½Π°Π»ΠΈΠ· Ρ†ΠΈΡ‚Ρ€Π°Ρ‚Π½ΠΎΠ³ΠΎ элСктролита мСднСния ΠΈ ΠΎΡ†Π΅Π½Π΅Π½ΠΎ влияниС ΠΊΠ°ΠΆΠ΄ΠΎΠ³ΠΎ ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π° Π½Π° свойства ΡΡ‚Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ элСктрода. Показана Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ примСнСния рассматриваСмого элСктролита для нанСсСния ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ нСпосрСдствСнно Π½Π° ΡΡ‚Π°Π»ΡŒ, Ρ‡Ρ‚ΠΎ Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ ΠΎΡ‚Π»ΠΈΡ‡Π°Π΅Ρ‚ Π΅Π³ΠΎ ΠΎΡ‚ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅ΠΌΡ‹Ρ… Π² настоящСС врСмя этилСндиаминовых, пирофосфатных, кислотных ΠΈ Π΄Ρ€ΡƒΠ³ΠΈΡ… элСктролитов. Π’ качСствС ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² исслСдования примСняли ΡΠ»Π΅ΠΊΡ‚Ρ€ΠΎΡ…ΠΈΠΌΠΈΡ‡Π΅ΡΠΊΡƒΡŽ ΠΈΠΌΠΏΠ΅Π΄Π°Π½ΡΠ½ΡƒΡŽ ΡΠΏΠ΅ΠΊΡ‚Ρ€ΠΎΡΠΊΠΎΠΏΠΈΡŽ ΠΈ ΠΊΠ°Ρ‚ΠΎΠ΄Π½ΡƒΡŽ ΠΏΠΎΠ»ΡΡ€ΠΈΠ·Π°Ρ†ΠΈΡŽ. УстановлСно, Ρ‡Ρ‚ΠΎ наимСньшСС сопротивлСниС повСрхности стали (ΠΎΠΊΠΎΠ»ΠΎ 15 Ом) ΠΎΡ‚Π²Π΅Ρ‡Π°Π»ΠΎ ΠΎΠ±Ρ€Π°Π·Ρ†Ρƒ, ΠΏΠΎΠ³Ρ€ΡƒΠΆΠ΅Π½Π½ΠΎΠΌΡƒ Π² Ρ†ΠΈΡ‚Ρ€Π°Ρ‚Π½Ρ‹ΠΉ элСктролит мСднСния с Π΄ΠΎΠ±Π°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ 1,0 Π³/Π» УДА. Диффузионная ΠΏΠ»ΠΎΡ‚Π½ΠΎΡΡ‚ΡŒ Ρ‚ΠΎΠΊΠ° для суспСнзий с 1,0 Π³/Π» УДА Π² Ρ†ΠΈΡ‚Ρ€Π°Ρ‚Π½ΠΎΠΌ элСктролитС мСднСния составила 2,6 А/Π΄ΠΌ2. Π£Π»ΡŒΡ‚Ρ€Π°Π΄ΠΈΡΠΏΠ΅Ρ€ΡΠ½Ρ‹Π΅ Π°Π»ΠΌΠ°Π·Ρ‹ Π² Ρ†ΠΈΡ‚Ρ€Π°Ρ‚Π½ΠΎΠΌ элСктролитС мСднСния экранировали ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½ΠΎΡΡ‚ΡŒ ΡΡ‚Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ ΠΎΠ±Ρ€Π°Π·Ρ†Π°, ΠΏΡ€ΠΈ этом сниТая ΠΎΠ±Ρ‰Π΅Π΅ сопротивлСниС пассивного слоя стали Π‘Ρ‚ 3. Π’Π°ΠΊΠΆΠ΅ прСдставлСны эквивалСнтныС элСктричСскиС схСмы повСрхности ΡΡ‚Π°Π»ΡŒΠ½Ρ‹Ρ… ΠΎΠ±Ρ€Π°Π·Ρ†ΠΎΠ², ΠΏΠΎΠ³Ρ€ΡƒΠΆΠ΅Π½Π½Ρ‹Ρ… Π² Ρ†ΠΈΡ‚Ρ€Π°Ρ‚Π½Ρ‹ΠΉ элСктролит мСднСния ΠΈ ΡΠΎΡΡ‚Π°Π²Π»ΡΡŽΡ‰ΠΈΠ΅ Π΅Π³ΠΎ ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Ρ‹.

    ЭлСктрохимичСскоС осаТдСниС ΠΆΠ΅Π»Ρ‚ΠΎΠΉ Π»Π°Ρ‚ΡƒΠ½ΠΈ Π² условиях ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ½ΠΎΠ³ΠΎ элСктролиза

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    Electrodeposition of copper-zinc alloy of non-cyanide sorbate electrolyte at current densities of 1,0-3,5 A/dm2 allows to produce yellow brass with a copper content of about 63-64 wt.Β°%. Using pulsed current allows to intensify the process of deposition 1,3-1,6 times and to increase the current efficiency of the alloy by 1,2-4,2 %. Coatings obtained by pulsed electrolysis have fine-grained structure, more compact and with good adhesion to the steel substrate. Imposition of pulsed current allows deposition of homogeneous phase coating and eliminates formation of intermetallic compounds.ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ исслСдований бСсцианистого сорбатного элСктролита латунирования ΠΈ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… ΠΈΠ· Π½Π΅Π³ΠΎ ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ. Π˜ΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ‹ кинСтичСскиС особСнности совмСстного осаТдСния ΠΌΠ΅Π΄ΠΈ ΠΈ Ρ†ΠΈΠ½ΠΊΠ°. Π˜Π·ΡƒΡ‡Π΅Π½ΠΎ влияниС ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ½ΠΎΠ³ΠΎ Ρ‚ΠΎΠΊΠ° ΠΈ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² нСстационарности Π½Π° Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½ Ρ€Π°Π±ΠΎΡ‡ΠΈΡ… плотностСй Ρ‚ΠΎΠΊΠ° ΠΈ качСство Π»Π°Ρ‚ΡƒΠ½Π½Ρ‹Ρ… ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ. Π’Ρ‹Π±Ρ€Π°Π½Ρ‹ ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Π΅ Ρ€Π΅ΠΆΠΈΠΌΡ‹ осаТдСния Π»Π°Ρ‚ΡƒΠ½Π½Ρ‹Ρ… ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ Π² условиях ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ½ΠΎΠ³ΠΎ элСктролиза. ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ исслСдования влияния ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ½ΠΎΠ³ΠΎ Ρ‚ΠΎΠΊΠ° Π½Π° Ρ„Π°Π·ΠΎΠ²Ρ‹ΠΉ состав ΠΈ микроструктуру осаТдСнного сплава

    Charge Kondo Effect in Thermoelectric Properties of Lead Telluride doped with Thallium Impurities

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    We investigate the thermoelectric properties of PbTe doped with a small concentration xx of Tl impurities acting as acceptors and described by Anderson impurities with negative on-site (effective) interaction. The resulting charge Kondo effect naturally accounts for a number of the low temperature anomalies in this system, including the unusual doping dependence of the carrier concentration, the Fermi level pinning and the self-compensation effect. The Kondo anomalies in the low temperature resistivity at temperatures T≀10 KT\leq 10\, {\rm K} and the xx-dependence of the residual resistivity are also in good agreement with experiment. Our model also captures the qualitative aspects of the thermopower at higher temperatures T>300 KT>300\, {\rm K} for high dopings (x>0.6x>0.6%) where transport is expected to be largely dominated by carriers in the heavy hole band of PbTe.Comment: chapter contributed to 'New Materials for Thermoelectric Applications: Theory and Experiment' Springer Series: NATO Science for Peace and Security Series - B: Physics and Biophysics, pp. 67-80, ed. Veljko Zlati\'c, and Alex Hewson (Editor). ISBN: 978-94-007-4983-2 (2013

    ΠžΠ‘ΠžΠ‘Π•ΠΠΠžΠ‘Π’Π˜ БВРУКВУРЫ ΠŸΠžΠ’Π•Π Π₯НОБВИ ΠœΠ•Π”ΠΠ«Π₯ ΠŸΠžΠšΠ Π«Π’Π˜Π™ ПРИ Π’Π’Π•Π”Π•ΠΠ˜Π˜ Π’ Π­Π›Π•ΠšΠ’Π ΠžΠ›Π˜Π’ ΠœΠ•Π”ΠΠ•ΠΠ˜Π― Π£Π›Π¬Π’Π ΠΠ”Π˜Π‘ΠŸΠ•Π Π‘ΠΠ«Π₯ ΠΠ›ΠœΠΠ—ΠžΠ’ И ΠΠ›ΠœΠΠ—ΠΠžΠ™ ШИΠ₯Π’Π«

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    The properties of composite copper coatings with inclusions of ultradispersed diamonds (UDD) and diamond soot (DS) in copper citrate electrolyte have been investigated. The concentrations of diamond-containing additives have been varied in the range of 0.2–2 g/l. Sizes of copper microcrystals, UDD and DS particles were determined from the scanning electron microscopy images. By means of the X-ray fluorescent analysis, the interrelation between concentration of diamondbearing additives in electrolyte and their content in the obtained coatings has been established. The minimal microporosity and the maximal microhardness correspond to concentration of 1.0 g/l for both UDD and DS suspensions in citrate copper coating electrolytes. Copper-UDD coating has increased protective properties (porosity 2 time/cm2 ) and uniformity of distribution of diamond-bearing particles on a surface in comparison with a monocoating and copper-DS coating. Using UDD in citrate copper coating electrolyte with a concentration of diamond-bearing additive of 1.0 g/l is more preferable for production of composite electrochemical coatings.Β Π˜ΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ‹ свойства ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ†ΠΈΠΎΠ½Π½Ρ‹Ρ… ΠΌΠ΅Π΄Π½Ρ‹Ρ… ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ с Π²ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΡΠΌΠΈ ΡƒΠ»ΡŒΡ‚Ρ€Π°Π΄ΠΈΡΠΏΠ΅Ρ€ΡΠ½Ρ‹Ρ… Π°Π»ΠΌΠ°Π·ΠΎΠ² (УДА) ΠΈ Π°Π»ΠΌΠ°Π·Π½ΠΎΠΉ ΡˆΠΈΡ…Ρ‚Ρ‹ (АШ) Π² Ρ†ΠΈΡ‚Ρ€Π°Ρ‚Π½ΠΎΠΌ элСктролитС мСднСния. ΠšΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠΈ алмазосодСрТащих Π΄ΠΎΠ±Π°Π²ΠΎΠΊ Π²Π°Ρ€ΡŒΠΈΡ€ΠΎΠ²Π°Π»ΠΈ Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ 0,2–2 Π³/Π». По изобраТСниям, ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹ΠΌ с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ растрового элСктронного микроскопа, ΠΎΠΏΡ€Π΅Π΄Π΅Π»ΠΈΠ»ΠΈ Ρ€Π°Π·ΠΌΠ΅Ρ€Ρ‹ микрокристаллов ΠΌΠ΅Π΄ΠΈ, частиц УДА ΠΈ АШ. Π‘ ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ рСнтгСнофлуорСсцСнтного Π°Π½Π°Π»ΠΈΠ·Π° установили взаимосвязь ΠΌΠ΅ΠΆΠ΄Ρƒ ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠ΅ΠΉ алмазосодСрТащих Π΄ΠΎΠ±Π°Π²ΠΎΠΊ Π² элСктролитС ΠΈ ΠΈΡ… содСрТаниСм Π² ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… покрытиях. Минимальная ΠΌΠΈΠΊΡ€ΠΎΠΏΠΎΡ€ΠΈΡΡ‚ΠΎΡΡ‚ΡŒ ΠΈ максимальная ΠΌΠΈΠΊΡ€ΠΎΡ‚Π²Π΅Ρ€Π΄ΠΎΡΡ‚ΡŒ соотвСтствуСт ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠΈ 1,0 Π³/Π» ΠΊΠ°ΠΊ для суспСнзии с УДА, Ρ‚Π°ΠΊ ΠΈ для суспСнзии с АШ Π² Ρ†ΠΈΡ‚Ρ€Π°Ρ‚Π½Ρ‹Ρ… элСктролитах мСднСния. ΠŸΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΡ мСдь-УДА ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‚ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½Π½Ρ‹ΠΌΠΈ Π·Π°Ρ‰ΠΈΡ‚Π½Ρ‹ΠΌΠΈ свойствами (ΠΏΠΎΡ€ΠΈΡΡ‚ΠΎΡΡ‚ΡŒ 2 ΠΏΠΎΡ€/см2 ) ΠΈ ΠΎΠ΄Π½ΠΎΡ€ΠΎΠ΄Π½ΠΎΡΡ‚ΡŒΡŽ распрСдСлСния алмазосодСрТащих частиц ΠΏΠΎ повСрхности Π² сравнСнии с ΠΌΠΎΠ½ΠΎΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠ΅ΠΌ ΠΈ мСдь-АШ. Для получСния ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ†ΠΈΠΎΠ½Π½Ρ‹Ρ… элСктрохимичСских ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ ΠΏΡ€Π΅Π΄ΠΏΠΎΡ‡Ρ‚ΠΈΡ‚Π΅Π»ΡŒΠ½Π΅Π΅ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΠΎΠ²Π°Ρ‚ΡŒ УДА Π² Ρ†ΠΈΡ‚Ρ€Π°Ρ‚Π½ΠΎΠΌ элСктролитС мСднСния с ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠ΅ΠΉ алмазосодСрТащСй Π΄ΠΎΠ±Π°Π²ΠΊΠΈ 1,0 Π³/Π».
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