40 research outputs found

    ΠžΡ†Π΅Π½ΠΊΠ° стСпСни кристаллографичСского упорядочСния ΠΌΠ°Π³Π½ΠΈΡ‚ΠΎΠ°ΠΊΡ‚ΠΈΠ²Π½Ρ‹Ρ… ΠΈΠΎΠ½ΠΎΠ² Π² Sr2FeMoO6-Ξ΄ с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ интСнсивности рСнтгСновского ΠΏΠΈΠΊΠ° (101)

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    Strontium ferromolybdate (Sr2FeMoO6-Ξ΄, SFMO) having a double Perovskite structure shows good promise as a basic material for spintronics. However SFMO has not yet found wide application due to the low reproducibility of its magnetic properties which partially originates from their strong dependence on the ordering degree of Fe and Mo ions in the BΒ΄ and BΒ² sublattices of double perovskite A2BΒ΄BΒ²O6. We have considered a rapid method of determining strontium ferromolybdate disorder degree. Sublattice population with Fe and Mo ions has been estimated for stoichiometric and nonstoichiometric Sr2FeMoO6-Ξ΄ with a 5% Fe and Mo excess, respectively. We have calculated the intensity ratio between the superstructural ordering (101) peak and the most intense (112 + 200) peak. The calculated curves have been fitted to the analytical expression for similar cases known from literature. The calculation results obtained using this method are in agreement with the results of experimental data processing using the Rietveld method accurate to within Β±25 %. Thus this method can be used instead of the Rietveld method if the exposure time set in an X-ray diffraction experiment is insufficient. We have discussed the dependence of the I(101)/I(112 + 200) peak intensity ratio on various factors including diffraction peak instrumental broadening, peak twinning due to grain size reduction, thin film lattice parameter variation due to substrate lattice mismatch and lattice parameter variation due to oxygen vacancies. The method is useful as it allows evaluating the superlattice ordering degree in Sr2FeMoO6-d without large time consumption for X-ray diffraction pattern recording and processing with the Rietveld method which may be essential when dealing with large amounts of experimental dataΠ€Π΅Ρ€Ρ€ΠΎΠΌΠΎΠ»ΠΈΠ±Π΄Π°Ρ‚ стронция (Sr2FeMoO6-d, SFMO), ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‰ΠΈΠΉ структурой Π΄Π²ΠΎΠΉΠ½ΠΎΠ³ΠΎ пСровскита, являСтся ΠΌΠ½ΠΎΠ³ΠΎΠΎΠ±Π΅Ρ‰Π°ΡŽΡ‰ΠΈΠΌ ΠΊΠ°Π½Π΄ΠΈΠ΄Π°Ρ‚ΠΎΠΌ для использования Π² качСствС основного ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° Π² спинтроникС. Однако Π½Π° Π΄Π°Π½Π½Ρ‹ΠΉ ΠΌΠΎΠΌΠ΅Π½Ρ‚ SFMO Π½Π΅ нашСл ΡˆΠΈΡ€ΠΎΠΊΠΎΠ³ΠΎ примСнСния ΠΈΠ·-Π·Π° Π½ΠΈΠ·ΠΊΠΎΠΉ воспроизводимости Π΅Π³ΠΎ ΠΌΠ°Π³Π½ΠΈΡ‚Π½Ρ‹Ρ… свойств, Π²Ρ‹Π·Π²Π°Π½Π½ΠΎΠΉ, Π² Ρ‚ΠΎΠΌ числС, ΠΈΡ… сильной Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ‚ΡŒΡŽ ΠΎΡ‚ стСпСни упорядочСния ΠΊΠ°Ρ‚ΠΈΠΎΠ½ΠΎΠ² Fe ΠΈ Mo Π² ΠΏΠΎΠ΄Ρ€Π΅ΡˆΠ΅Ρ‚ΠΊΠ°Ρ… BΒ΄ ΠΈ BΒ² Π΄Π²ΠΎΠΉΠ½ΠΎΠ³ΠΎ пСровскита A2BΒ΄BΒ²O6. РассмотрСн экспрСсс-ΠΌΠ΅Ρ‚ΠΎΠ΄ опрСдСлСния стСпСни разупорядочСния Ρ„Π΅Ρ€Ρ€ΠΎΠΌΠΎΠ»ΠΈΠ±Π΄Π°Ρ‚Π° стронция. Π‘Ρ‚Π΅ΠΏΠ΅Π½ΡŒ засСлСния ΠΏΠΎΠ΄Ρ€Π΅ΡˆΠ΅Ρ‚ΠΎΠΊ ΠΊΠ°Ρ‚ΠΈΠΎΠ½Π°ΠΌΠΈ Fe ΠΈ Mo ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Π° ΠΊΠ°ΠΊ для стСхиомСтричСского, Ρ‚Π°ΠΊ ΠΈ для нСстСхиомСтричСского Sr2FeMoO6-Ξ΄ с 5%-Π½Ρ‹ΠΌ ΠΈΠ·Π±Ρ‹Ρ‚ΠΊΠΎΠΌ Fe ΠΈ Mo соотвСтствСнно. Рассчитано ΡΠΎΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΠ΅ интСнсивности ΠΏΠΈΠΊa свСрхструктурного упорядочСния (101) ΠΊ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ интСнсивному ΠΏΠΈΠΊΡƒ (112 + 200). ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π° ΠΏΠΎΠ΄Π³ΠΎΠ½ΠΊΠ° расчСтных ΠΊΡ€ΠΈΠ²Ρ‹Ρ… ΠΏΠΎΠ΄ извСстноС для Π°Π½Π°Π»ΠΎΠ³ΠΈΡ‡Π½Ρ‹Ρ… случаСв аналитичСскоС Π²Ρ‹Ρ€Π°ΠΆΠ΅Π½ΠΈΠ΅. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ расчСтов ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π½Ρ‹ΠΌ Π°Π²Ρ‚ΠΎΡ€Π°ΠΌΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ΡΠΎΠ²ΠΏΠ°Π΄Π°ΡŽΡ‚ с Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°ΠΌΠΈ ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Ρ… Π΄Π°Π½Π½Ρ‹Ρ… ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Π ΠΈΡ‚Π²Π΅Π»ΡŒΠ΄Π° Π² ΠΏΡ€Π΅Π΄Π΅Π»Π°Ρ… Β±25 %, Ρ‡Ρ‚ΠΎ позволяСт ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΠΎΠ²Π°Ρ‚ΡŒ этот ΠΌΠ΅Ρ‚ΠΎΠ΄ Π² качСствС Π°Π»ΡŒΡ‚Π΅Ρ€Π½Π°Ρ‚ΠΈΠ²Ρ‹ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρƒ Π ΠΈΡ‚Π²Π΅Π»ΡŒΠ΄Π° Π² Ρ‚ΠΎΠΌ случаС, ΠΊΠΎΠ³Π΄Π° врСмя Π²Ρ‹Π΄Π΅Ρ€ΠΆΠΊΠΈ для рСнтгСноструктурного Π°Π½Π°Π»ΠΈΠ·Π° установлСно нСдостаточно большим. ΠžΠ±ΡΡƒΠΆΠ΄Π΅Π½ΠΎ влияниС Ρ‚Π°ΠΊΠΈΡ… Ρ„Π°ΠΊΡ‚ΠΎΡ€ΠΎΠ², ΠΊΠ°ΠΊ ΠΏΡ€ΠΈΠ±ΠΎΡ€Π½ΠΎΠ΅ ΡƒΡˆΠΈΡ€Π΅Π½ΠΈΠ΅ Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΎΠ½Π½Ρ‹Ρ… ΠΏΠΈΠΊΠΎΠ², ΡƒΡˆΠΈΡ€Π΅Π½ΠΈΠ΅ ΠΏΠΈΠΊΠΎΠ² вслСдствиС ΡƒΠΌΠ΅Π½ΡŒΡˆΠ΅Π½ΠΈΡ Ρ€Π°Π·ΠΌΠ΅Ρ€Π° кристаллитов, ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² Ρ€Π΅ΡˆΠ΅Ρ‚ΠΊΠΈ Ρ‚ΠΎΠ½ΠΊΠΈΡ… ΠΏΠ»Π΅Π½ΠΎΠΊ Π·Π° счСт ΠΈΡ… нСсоотвСтствия с ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠΎΠΉ ΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² Ρ€Π΅ΡˆΠ΅Ρ‚ΠΊΠΈ Π·Π° счСт появлСния кислородных вакансий Π½Π° ΡΠΎΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΠ΅ интСнсивности ΠΏΠΈΠΊΠΎΠ² I(101)/I(112 + 200). ΠΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° состоит Π² Ρ‚ΠΎΠΌ, Ρ‡Ρ‚ΠΎ ΠΎΠ½ позволяСт ΠΎΡ†Π΅Π½ΠΈΡ‚ΡŒ ΡΡ‚Π΅ΠΏΠ΅Π½ΡŒ свСрхструктурного упорядочСния Sr2FeMoO6-d Π½Π΅ трСбуя Π±ΠΎΠ»ΡŒΡˆΠΈΡ… Π·Π°Ρ‚Ρ€Π°Ρ‚ Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ съСмки ΠΈ ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ Π΄Π°Π½Π½Ρ‹Ρ… Π΄ΠΈΡ„Ρ€Π°ΠΊΡ‚ΠΎΠ³Ρ€Π°ΠΌΠΌ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Π ΠΈΡ‚Π²Π΅Π»ΡŒΠ΄Π°, Ρ‡Ρ‚ΠΎ ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ ΠΏΠΎΠ»Π΅Π·Π½ΠΎ Π² случаС, ΠΊΠΎΠ³Π΄Π° прСдстоит ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚Π°Ρ‚ΡŒ большоС количСство Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² ΠΈΠ·ΠΌΠ΅Ρ€Π΅Π½ΠΈΠΉ

    ΠœΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ²Π΅Π΄Ρ‡Π΅ΡΠΊΠΈΠ΅ вопросы тСрмодинамичСского модСлирования Ρ‚ΠΎΠ½ΠΊΠΎΠΏΠ»Π΅Π½ΠΎΡ‡Π½Ρ‹Ρ… Ρ‚Π²Π΅Ρ€Π΄ΠΎΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… элСктрокалоричСских ΠΎΡ…Π»Π°Π΄ΠΈΡ‚Π΅Π»Π΅ΠΉ

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    Materials properties affecting EC device operation are discussed based on an analytically tractable model of a layered EC refrigerator. Special attention was paid to thermal and interface thermal resistances. Estimates of the average cooling power of a stacked MEMS-based EC refrigerator were made.ЭлСктрокалоричСскоС ΠΎΡ…Π»Π°ΠΆΠ΄Π΅Π½ΠΈΠ΅ являСтся экологичСски бСзопасной Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠ΅ΠΉ прСобразования энСргии. ЭлСктричСскоС ΠΏΠΎΠ»Π΅, Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎΠ΅ для возбуТдСния Ρ†ΠΈΠΊΠ»Π° элСктрокалоричСского охлаТдСния, ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ создано Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ ΠΏΡ€ΠΎΡ‰Π΅ ΠΈ с Π³ΠΎΡ€Π°Π·Π΄ΠΎ мСньшими Π·Π°Ρ‚Ρ€Π°Ρ‚Π°ΠΌΠΈ ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с ΠΌΠ°Π³Π½ΠΈΡ‚Π½Ρ‹ΠΌΠΈ полями, ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅ΠΌΡ‹ΠΌΠΈ для магнСтокалоричСского охлаТдСния. ΠšΡ€ΠΎΠΌΠ΅ Ρ‚ΠΎΠ³ΠΎ, элСктричСская ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒ, нСобходимая для элСктрокалоричСского охлаТдСния, ΠΌΠΎΠΆΠ΅Ρ‚ ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°Ρ‚ΡŒΡΡ стационарными ΠΈΠ»ΠΈ ΠΌΠΎΠ±ΠΈΠ»ΡŒΠ½Ρ‹ΠΌΠΈ солнСчными батарСями, Π° Ρ‚Π°ΠΊΠΆΠ΅ аккумуляторами элСктромобиля. Π­Ρ‚ΠΎ ΠΎΡ‚ΠΊΡ€Ρ‹Π²Π°Π΅Ρ‚ ΡΠΎΠ²Π΅Ρ€ΡˆΠ΅Π½Π½ΠΎ Π½ΠΎΠ²Ρ‹Π΅ возмоТности для экологичСски бСзопасного ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½ΠΎΠ³ΠΎ прогрСсса Π² Ρ€Π°Π·Π²ΠΈΠ²Π°ΡŽΡ‰ΠΈΡ…ΡΡ странах. На основС аналитичСски Ρ€Π΅ΡˆΠ°Π΅ΠΌΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ многослойного элСктрокалоричСского охладитСля обсуТдСны свойства ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ², Π²Π»ΠΈΡΡŽΡ‰ΠΈΠ΅ Π½Π° эксплуатационныС характСристики элСктрокалоричСских ΠΏΡ€ΠΈΠ±ΠΎΡ€ΠΎΠ². ОсобоС Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ ΡƒΠ΄Π΅Π»Π΅Π½ΠΎ ΠΎΠ±ΡŠΠ΅ΠΌΠ½ΠΎΠΌΡƒ тСрмичСскому ΡΠΎΠΏΡ€ΠΎΡ‚ΠΈΠ²Π»Π΅Π½ΠΈΡŽ ΠΈ тСрмичСскому ΡΠΎΠΏΡ€ΠΎΡ‚ΠΈΠ²Π»Π΅Π½ΠΈΡŽ интСрфСйсов. Π”Π°Π½Ρ‹ ΠΎΡ†Π΅Π½ΠΊΠΈ срСднСй ΠΎΡ…Π»Π°ΠΆΠ΄Π°ΡŽΡ‰Π΅ΠΉ мощности стСка микроэлСктромСханичСского элСктрокалоричСского охладитСля

    Formation of the Microcrystalline Structure in LiNbO3 Thin Films by Pulsed Light Annealing

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    LiNbO3 thin films with a thickness of 200 nm were deposited onto Al2O3 substrate by RF-magnetron sputtering technique without intentional substrate heating. The results demonstrate that post-growth infrared pulsed light annealing of the amorphous LiNbO3 films leads to the formation of two phases, LiNbO3 and LiNb3O8. After annealing at temperatures of 700 to 800 Β°C, the percentage of the nonferroelectric phase LiNb3O8 was minimal. The surface composition of the films annealed at different temperatures was examined by X-ray photoelectron spectroscopy. Piezoresponse force microscopy was used to study both the vertical and the lateral polarization and to visualize the piezoelectric inactivity of LiNb3O8 grains. A comparison of the results of PFM and XPS measurements revealed that there is a correlation between the fraction of the piezoelectric phase and the film composition: At an annealing temperature higher than 850 Β°C, the atomic ratio of lithium to niobium decreases compared to the initial value along with a decrease of the fraction of the piezoelectric phase

    Giant phonon anomalies and central peak due to charge density wave formation in YBa2_2Cu3_3O6.6_{6.6}

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    The electron-phonon interaction is a major factor influencing the competition between collective instabilities in correlated-electron materials, but its role in driving high-temperature superconductivity in the cuprates remains poorly understood. We have used high-resolution inelastic x-ray scattering to monitor low-energy phonons in YBa2_2Cu3_3O6.6_{6.6} (superconducting Tc=61\bf T_c = 61 K), which is close to a charge density wave (CDW) instability. Phonons in a narrow range of momentum space around the CDW ordering vector exhibit extremely large superconductivity-induced lineshape renormalizations. These results imply that the electron-phonon interaction has sufficient strength to generate various anomalies in electronic spectra, but does not contribute significantly to Cooper pairing. In addition, a quasi-elastic "central peak" due to CDW nanodomains is observed in a wide temperature range above and below Tc\bf T_c, suggesting that the gradual onset of a spatially inhomogeneous CDW domain state with decreasing temperature is a generic feature of the underdoped cuprates

    Progress in Neutron Scattering Studies of Spin Excitations in High-Tc Cuprates

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    Neutron scattering experiments continue to improve our knowledge of spin fluctuations in layered cuprates, excitations that are symptomatic of the electronic correlations underlying high-temperature superconductivity. Time-of-flight spectrometers, together with new and varied single crystal samples, have provided a more complete characterization of the magnetic energy spectrum and its variation with carrier concentration. While the spin excitations appear anomalous in comparison with simple model systems, there is clear consistency among a variety of cuprate families. Focusing initially on hole-doped systems, we review the nature of the magnetic spectrum, and variations in magnetic spectral weight with doping. We consider connections with the phenomena of charge and spin stripe order, and the potential generality of such correlations as suggested by studies of magnetic-field and impurity induced order. We contrast the behavior of the hole-doped systems with the trends found in the electron-doped superconductors. Returning to hole-doped cuprates, studies of translation-symmetry-preserving magnetic order are discussed, along with efforts to explore new systems. We conclude with a discussion of future challenges.Comment: revised version, to be published in JPSJ, 20 pages, 21 figure

    Electrocaloric Cooling - A New Application of Relaxor Ferroelectrics

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    Until now, relaxor ferroelectrics are considered as a class of disordered materials possessing peculiar structures and properties which are not yet generalized into a universal model explaining the significant amount of experimental data available. In this work, we demonstrate that one feature of relaxor ferroelectrics - the extraordinary dielectric response - is well-suited for application in electrocaloric refrigerators. We consider the electrocaloric effect with special attention to relaxor ferroelectrics, the dielectric response in the temperature region of interest, the efficiency and the figure of merit of relaxor ferroelectrics for electrocaloric application

    Electrocaloric Cooling - A New Application of Relaxor Ferroelectrics

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    Until now, relaxor ferroelectrics are considered as a class of disordered materials possessing peculiar structures and properties which are not yet generalized into a universal model explaining the significant amount of experimental data available. In this work, we demonstrate that one feature of relaxor ferroelectrics - the extraordinary dielectric response - is well-suited for application in electrocaloric refrigerators. We consider the electrocaloric effect with special attention to relaxor ferroelectrics, the dielectric response in the temperature region of interest, the efficiency and the figure of merit of relaxor ferroelectrics for electrocaloric application

    Characterisation of the polarisation state of embedded piezoelectric transducers by thermal waves and thermal pulses

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    In this work, we apply the thermal wave method and the thermal pulse method for non-destructive characterisation of the polarisation state of embedded piezoelectric transducers. Heating the sample with a square-wave modulated laser beam or a single laser pulse leads to a pyroelectric current recorded in the frequency or time domain, respectively. It carries information about the polarisation state. Analytical and numerical finite element models describe the pyroelectric response of the piezoceramic. Modelling and experimental results are compared for a simple lead–zirconate–titanate (PZT) plate, a low-temperature co-fired ceramics (LTCC)/PZT sensor and actuator, and a macro-fibre composite (MFC) actuator
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