61 research outputs found

    Ferroelectric Nanotubes

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    We report the independent invention of ferroelectric nanotubes from groups in several countries. Devices have been made with three different materials: lead zirconate-titanate PbZr1-xTixO3 (PZT); barium titanate BaTiO3; and strontium bismuth tantalate SrBi2Ta2O9 (SBT). Several different deposition techniques have been used successfully, including misted CSD (chemical solution deposition) and pore wetting. Ferroelectric hysteresis and high optical nonlinearity have been demonstrated. The structures are analyzed via SEM, TEM, XRD, AFM (piezo-mode), and SHG. Applications to trenching in Si dynamic random access memories, ink-jet printers, and photonic devices are discussed. Ferroelectric filled pores as small as 20 nm in diameter have been studied

    ΠœΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌΡ‹ формирования Π³Π΅Ρ‚Π΅Ρ€ΠΎΡ„Π°Π·Π½Ρ‹Ρ… сСгнСтоэлСктричСских ΠΏΠ»Π΅Π½ΠΎΠΊ Ρ†ΠΈΡ€ΠΊΠΎΠ½Π°Ρ‚Π°-Ρ‚ΠΈΡ‚Π°Π½Π°Ρ‚Π° свинца

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    An experimental and theoretical study of the formation processes of "impurity" phase inclusions in ferroelectric oxides is carried out via example of polycrystalline lead zirconate-titanate (PZT) films. A feature of these compositions is relatively high volatility of lead oxides, which can lead to deficiency of these components in the composition of the ferroelectric film formed during high-temperature crystallization. To avoid lead losses, some excess is added to the solution in the process of synthesis. Experimental samples of PZT films are obtained using sol-gel method with different contents of lead oxide, the crystallization of the ferroelectric phase of the films is carried out in air at 600 Β°C. In the films, the inclusions of lead oxide impurity phase are found, and the size distribution of these inclusions are obtained. Model concepts are presented and a system of equations is proposed describing the dispersed inclusions formation kinetics of new phases of different stoichiometric composition at the interfaces in polycrystalline films of multicomponent ferroelectric oxides due to bulk diffusion and grain-boundary segregation. Comparison of the experimental data with the theoretical model gives qualitative agreement. The approach generality makes it possible to extend the model to other systems of multicomponent ferroelectric polycrystalline materials.ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎΠ΅ ΠΈ тСорСтичСскоС ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΈΠ΅ процСссов образования Π²ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠΉ "примСсных" Ρ„Π°Π· Π² сСгнСтоэлСктричСских оксидах Π½Π° ΠΏΡ€ΠΈΠΌΠ΅Ρ€Π΅ поликристалличСских ΠΏΠ»Π΅Π½ΠΎΠΊ Ρ†ΠΈΡ€ΠΊΠΎΠ½Π°Ρ‚Π°-Ρ‚ΠΈΡ‚Π°Π½Π°Ρ‚Π° свинца (Π¦Π’Π‘). ΠžΡΠΎΠ±Π΅Π½Π½ΠΎΡΡ‚ΡŒΡŽ Π΄Π°Π½Π½Ρ‹Ρ… составов являСтся ΡΡ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ высокая Π»Π΅Ρ‚ΡƒΡ‡Π΅ΡΡ‚ΡŒ оксидов свинца, Ρ‡Ρ‚ΠΎ ΠΌΠΎΠΆΠ΅Ρ‚ ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ΡŒ ΠΊ Π΄Π΅Ρ„ΠΈΡ†ΠΈΡ‚Ρƒ этих ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚ΠΎΠ² Π² составС Ρ„ΠΎΡ€ΠΌΠΈΡ€ΡƒΠ΅ΠΌΠΎΠΉ сСгнСтоэлСктричСской ΠΏΠ»Π΅Π½ΠΊΠΈ Π² Ρ…ΠΎΠ΄Π΅ высокотСмпСратурной кристаллизации. Π§Ρ‚ΠΎΠ±Ρ‹ ΠΈΠ·Π±Π΅ΠΆΠ°Ρ‚ΡŒ ΠΏΠΎΡ‚Π΅Ρ€ΠΈ свинца, Π² процСссС синтСза Π² раствор Π΄ΠΎΠ±Π°Π²Π»ΡΡŽΡ‚ Π΅Π³ΠΎ Π½Π΅ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΉ ΠΈΠ·Π±Ρ‹Ρ‚ΠΎΠΊ. Π­ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Π΅ ΠΎΠ±Ρ€Π°Π·Ρ†Ρ‹ ΠΏΠ»Π΅Π½ΠΎΠΊ Π¦Π’Π‘ Π±Ρ‹Π»ΠΈ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ золь-гСль-ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ с Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹ΠΌ содСрТаниСм оксида свинца, кристаллизация сСгнСтоэлСктричСской Ρ„Π°Π·Ρ‹ ΠΏΠ»Π΅Π½ΠΎΠΊ ΠΎΡΡƒΡ‰Π΅ΡΡ‚Π²Π»ΡΠ»Π°ΡΡŒ Π½Π° Π²ΠΎΠ·Π΄ΡƒΡ…Π΅ ΠΏΡ€ΠΈ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π΅ 600 Β°C. Π’ ΠΏΠ»Π΅Π½ΠΊΠ°Ρ… ΠΎΠ±Π½Π°Ρ€ΡƒΠΆΠ΅Π½Ρ‹ Π²ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΡ примСсной Ρ„Π°Π·Ρ‹ оксида свинца, ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½ΠΎ распрСдСлСниС Π²ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠΉ ΠΏΠΎ Ρ€Π°Π·ΠΌΠ΅Ρ€Π°ΠΌ. Π˜Π·Π»ΠΎΠΆΠ΅Π½Ρ‹ ΠΌΠΎΠ΄Π΅Π»ΡŒΠ½Ρ‹Π΅ прСдставлСния ΠΈ ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π° систСма ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ, ΠΎΠΏΠΈΡΡ‹Π²Π°ΡŽΡ‰ΠΈΠ΅ ΠΊΠΈΠ½Π΅Ρ‚ΠΈΠΊΡƒ образования диспСрсных Π²ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠΉ Π½ΠΎΠ²Ρ‹Ρ… Ρ„Π°Π· Ρ€Π°Π·Π»ΠΈΡ‡Π½ΠΎΠ³ΠΎ стСхиомСтричСского состава Π½Π° Π³Ρ€Π°Π½ΠΈΡ†Π°Ρ… Ρ€Π°Π·Π΄Π΅Π»Π° Π² поликристалличСских ΠΏΠ»Π΅Π½ΠΊΠ°Ρ… ΠΌΠ½ΠΎΠ³ΠΎΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½Ρ‹Ρ… сСгнСтоэлСктричСских оксидов Π·Π° счСт процСссов объСмной Π΄ΠΈΡ„Ρ„ΡƒΠ·ΠΈΠΈ ΠΈ Π·Π΅Ρ€Π½ΠΎΠ³Ρ€Π°Π½ΠΈΡ‡Π½ΠΎΠΉ сСгрСгации. БопоставлСниС ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Ρ… Π΄Π°Π½Π½Ρ‹Ρ… с тСорСтичСской модСлью Π΄Π°Π»ΠΎ согласиС Π½Π° качСствСнном ΡƒΡ€ΠΎΠ²Π½Π΅. ΠžΠ±Ρ‰Π½ΠΎΡΡ‚ΡŒ ΠΏΠΎΠ΄Ρ…ΠΎΠ΄Π° позволяСт Ρ€Π°ΡΠΏΡ€ΠΎΡΡ‚Ρ€Π°Π½ΠΈΡ‚ΡŒ модСль Π½Π° Π΄Ρ€ΡƒΠ³ΠΈΠ΅ систСмы ΠΌΠ½ΠΎΠ³ΠΎΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½Ρ‹Ρ… сСгнСтоэлСктричСских поликристалличСских ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ²

    Nanocomposites: synthesis, structure, properties and new application opportunities

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    Dead layer thickness estimation at the ferroelectric film-metal interface in PZT

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    Yu. Podgorny acknowledges the program of Ministry of Education and Science (3.5726.2017/8.9) and K. Vorotilov and A. Sigov thank the program of Ministry of Education and Science (11.2259.2017).Different models for estimation of the dead layer thickness at the ferroelectric film-metal interface are discussed, including the small-signal capacitance model and two methods based on dielectric hysteresis analysisβ€”one based on slopes of the hysteresis loops at the coercive field and the other method based on comparison of dielectric hysteresis portraits. It is shown that the latter technique yields more reliable data as it excludes the effect of leakage and relaxation loss. Conductivity may have a pronounced effect on the validity of dead-layer thickness data. This work relates peripherally to negative capacitance in ferroelectric films and to lozenge-shaped hysteresis curves.Publisher PDFPeer reviewe
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