248 research outputs found
Polarizable molecular interactions in condensed phase and their equivalent nonpolarizable models
Earlier, using phenomenological approach, we showed that in some cases
polarizable models of condensed phase systems can be reduced to nonpolarizable
equivalent models with scaled charges. Examples of such systems include ionic
liquids, TIPnP-type models of water, protein force fields, and others, where
interactions and dynamics of inherently polarizable species can be accurately
described by nonpolarizable models. To describe electrostatic interactions, the
effective charges of simple ionic liquids are obtained by scaling the actual
charges of ions by a factor of 1/sqrt(eps_el), which is due to electronic
polarization screening effect; the scaling factor of neutral species is more
complicated. Here, using several theoretical models, we examine how exactly the
scaling factors appear in theory, and how, and under what conditions,
polarizable Hamiltonians are reduced to nonpolarizable ones. These models allow
one to trace the origin of the scaling factors, determine their values, and
obtain important insights on the nature of polarizable interactions in
condensed matter systems.Comment: 43 pages, 3 figure
Metal Phase Formation in Bubbling Reduction of Nickel and Iron from Oxide Melt
Bubbling reduction of nickel and iron from oxide melt is considered. Oxidized nickel ores melts interaction with gases (hydrogen, carbon monoxide, converted natural gas) is accompanied by the ferroalloy formation with high nickel content. This process is associated with the mass transfer, chemical reaction running and metal phase formation in the multi-component oxide melts, regardless of the reducing agent used. Those processes are of great importance for understanding of the ferronickel pyrometallurgical production processes. To describe the process, we used equations that allow one to estimate the size of gas bubble and metal drop moving in an oxide melt without fragmentation, its joint movement direction, flotation rate, sedimentation and separation conditions. The physicochemical characteristics affecting mass transfer (the densities and surface tensions of oxide and metal melts, as well as their interfacial characteristics) have been determined.
Keywords: nickel, iron, reduction, bubbling, metal, oxide, melts, ores, ferroalloy, flotation, sedimentation, reducing ga
Structural, electronic and optical properties of heterointerfaces based on antiferromagnet LaMnO3 and ferroelectrics isostructural to BaTiO3
The reported study was funded by Russian Scientific Foundation according to the research project No. 18-12-00260
Quasi-two-dimensional electron system at the interface between antiferromagnet LaMnO3 and ferroelectric Ba0.8Sr0.2TiO3
The reported study was funded by Russian Scientific Foundation according to the research project No. 18-12-00260
Ultrafast spectroscopy of CdS/CdSe quantum dots
Β© 2017, Allerton Press, Inc. Results from the nonresonance spectroscopy of CdS/CdSe quantum dots (composites of CdSeβCdS nanoparticles (coreβshell)) are presented. The nonlinear optical properties of CdS/CdSe QDs in PMMA are studied with fs pulses at 1053 nm using the transient lens technique. QDs generate rapidly oscillating signals with amplitude rise times of around 200 fs and decay times of around 500 fs, while pure PMMA polymer only generates an oscillating signal whose envelope coincides with its autocorrelation function
Electron dynamics at GaAs-AlGaAs heterojunction studied by ultrafast spectroscopy
In this letter the electron and spin dynamics at GaAs/AlGaAs heterojunction was studied by ultrafast spectroscopy techniques (photon echo and transient grating studies). Relaxation times and diffusion coefficients of photoexcited electrons and spins were obtained using pure optical setup. The estimated spin diffusion coefficient value of 160 cm2/s is relatively high and comparable to the electron diffusion coefficient of 200 cm2/s. This feature makes GaAs/AlGaAs heterosructure a promising material for practical application in semiconductor spintronics. Β© Published under licence by IOP Publishing Ltd
ΠΠΎΠ²Π°Ρ ΠΏΠ°ΡΠ°Π΄ΠΈΠ³ΠΌΠ° ΡΠ΅ΡΠ΅Π½ΠΈΡ Π·Π°Π΄Π°ΡΠΈ ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΎΠ±Π½Π°ΡΡΠΆΠ΅Π½ΠΈΡ ΠΏΠ»Π΅Π½ΠΎΠΊ Π½Π΅ΡΡΠΈ ΠΏΡΠΈ ΡΠΊΠΎΠ»ΡΠ·ΡΡΠΈΡ ΡΠ³Π»Π°Ρ ΠΎΠ±Π»ΡΡΠ΅Π½ΠΈΡ ΠΏΠΎΠ²Π΅ΡΡ Π½ΠΎΡΡΠΈ ΠΌΠΎΡΡ
Low efficiency of using of commercially available marine navigation radars to detect the oil slicks on the sea surface is showed. A new approach to the problem of oil films detection on the sea sur-face by radar at low grazing angles of irradiation is discussed. It's proposed to develop specialized radar, a list of tasks necessary for the creation such radar is formulated.ΠΠΎΠΊΠ°Π·Π°Π½Π° Π½ΠΈΠ·ΠΊΠ°Ρ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ΅ΡΠΈΠΉΠ½ΠΎ Π²ΡΠΏΡΡΠΊΠ°Π΅ΠΌΡΡ
ΡΡΠ΄ΠΎΠ²ΡΡ
Π½Π°Π²ΠΈΠ³Π°ΡΠΈΠΎΠ½Π½ΡΡ
ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΈΠΎΠ½Π½ΡΡ
ΡΡΠ°Π½ΡΠΈΠΉ (Π ΠΠ‘) Π΄Π»Ρ ΠΎΠ±Π½Π°ΡΡΠΆΠ΅Π½ΠΈΡ ΠΏΠ»Π΅Π½ΠΎΠΊ Π½Π΅ΡΡΠΈ Π½Π° ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΌΠΎΡΡ. ΠΠ±ΡΡΠΆΠ΄Π΅Π½ Π½ΠΎΠ²ΡΠΉ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄ ΠΊ ΠΏΠΎΡΡΠ°Π½ΠΎΠ²ΠΊΠ΅ ΠΏΡΠΎΠ±Π»Π΅ΠΌΡ ΠΎΠ±Π½Π°ΡΡΠΆΠ΅Π½ΠΈΡ ΠΏΠ»Π΅Π½ΠΎΠΊ Π½Π΅ΡΡΠΈ Π½Π° ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΌΠΎΡΡ Ρ ΠΏΠΎΠΌΠΎΡΡΡ Π ΠΠ‘ ΠΏΡΠΈ ΡΠΊΠΎΠ»ΡΠ·ΡΡΠΈΡ
ΡΠ³Π»Π°Ρ
ΠΎΠ±Π»ΡΡΠ΅Π½ΠΈΡ. ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ΠΎ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°ΡΡ ΡΠΏΠ΅ΡΠΈΠ°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΡΠ΅ Π ΠΠ‘; ΡΡΠΎΡΠΌΡΠ»ΠΈΡΠΎΠ²Π°Π½ ΠΏΠ΅ΡΠ΅ΡΠ΅Π½Ρ Π·Π°Π΄Π°Ρ, ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ ΠΊΠΎΡΠΎΡΡΡ
Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎ Π΄Π»Ρ ΡΠΎΠ·Π΄Π°Π½ΠΈΡ ΡΠ°ΠΊΠΈΡ
Π ΠΠ‘
ΠΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ ΠΏΠΎΡΡΡΠΎΠ΅Π½ΠΈΡ Π½Π΅ΠΉΡΠΎΠ½Π½ΠΎΠΉ ΡΠ΅ΡΠΈ Π² ΡΠΎΠ±Π°ΡΡΠ½ΠΎΠΉ ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΠ΅ ΠΊΠ»Π°ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈΠΌΠΎΠ½ΠΎΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΡΡ ΠΏΠ»Π΅Π½ΠΎΠΊ Π½Π΅ΡΡΠΈ Π½Π° ΠΏΠΎΠ²Π΅ΡΡ Π½ΠΎΡΡΠΈ ΠΌΠΎΡΡ ΠΏΡΠΈ Π³ΠΎΡΠΈΠ·ΠΎΠ½ΡΠ°Π»ΡΠ½ΠΎΠΉ ΠΏΠΎΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ
Neural network that allows to make a decision about the presence or absence of monomolecular films of medium or heavy oil on the sea surface in the radar with horizontal polarization, integrated into a single system with passive reflectors located either on the perimeter of the port basin, or on special buoys at sea is proposed.ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π° Π½Π΅ΠΉΡΠΎΠ½Π½Π°Ρ ΡΠ΅ΡΡ, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡΠ°Ρ ΠΏΡΠΈΠ½ΡΡΡ ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ ΠΎ Π½Π°Π»ΠΈΡΠΈΠΈ ΠΈΠ»ΠΈ ΠΎΠ± ΠΎΡΡΡΡΡΡΠ²ΠΈΠΈ ΠΌΠΎΠ½ΠΎΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΡΡ
ΠΏΠ»Π΅Π½ΠΎΠΊ ΡΡΠ΅Π΄Π½Π΅ΠΉ ΠΈΠ»ΠΈ ΡΡΠΆΠ΅Π»ΠΎΠΉ Π½Π΅ΡΡΠΈ Π½Π° ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΌΠΎΡΡ. Π Π΅ΡΠ΅Π½ΠΈΠ΅ ΠΏΡΠΈΠ½ΠΈΠΌΠ°Π΅ΡΡΡ Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ ΡΠΈΠ³Π½Π°Π»Π° ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΡΠ°Π½ΡΠΈΠΈ Ρ Π³ΠΎΡΠΈΠ·ΠΎΠ½ΡΠ°Π»ΡΠ½ΠΎΠΉ ΠΏΠΎΠ»ΡΡΠΈΠ·Π°ΡΠΈΠ΅ΠΉ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠΉ Π²ΠΎΠ»Π½Ρ, ΠΎΠ±ΡΠ΅Π΄ΠΈΠ½Π΅Π½Π½ΠΎΠΉ Π² Π΅Π΄ΠΈΠ½ΡΠΉ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡ Ρ ΠΏΠ°ΡΡΠΈΠ²Π½ΡΠΌΠΈ ΠΎΡΡΠ°ΠΆΠ°ΡΠ΅Π»ΡΠΌΠΈ, ΡΠ°ΡΠΏΠΎΠ»ΠΎΠΆΠ΅Π½Π½ΡΠΌΠΈ ΠΏΠΎ ΠΏΠ΅ΡΠΈΠΌΠ΅ΡΡΡ Π°ΠΊΠ²Π°ΡΠΎΡΠΈΠΈ ΠΏΠΎΡΡΠ°, Π° ΡΠ°ΠΊΠΆΠ΅ Π½Π° ΡΠΏΠ΅ΡΠΈΠ°Π»ΡΠ½ΡΡ
Π±ΡΡΡ
Π² ΠΌΠΎΡΠ΅
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