78 research outputs found

    Electrical Resistivity Peculiarities of the Nanograined Bi2Te3 Material

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    The hot quasiisostaic pressure method was applied to sinter the nanograined Bi2Te3 material. The samples with various mean grain size of 64, 61, 56 and 51 nm were prepared by changing the pressure of sintering. It was found that the specific electrical resistivity of the material under study increases when the mean grain size decreases. The Hall effect was measured to extract the concentration and mobility values of the charge carries. It was found that the electron concentration decreases as the mean grain size decreases while the electron mobility has extreme dependence on the grain size

    Characterization of Bulk Nanostructural Bi2Te3-based Material Prepared by Microwave-solvothermal Synthesis and Hot Isostatic Pressure

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    The bulk nanostructural Bi2Te3-based material was prepared by microwave assisted solvothermal method and hot isostatic pressure. Optimal synthesis conditions of the Bi2Te3 nanopowder were found. It was established that hot isostatic pressing of the nanopowders at the temperature of 400 Π‘ and the pres-sures of 2, 4, 6 and 8 GPa allowed us to prepare the homogeneous and dense Bi2Te3-based material with the mean grain size of~50 nm. It is found that an electrical resistivity increases as the mean grain size of the material under study decreases. When you are citing the document, use the following link http://essuir.sumdu.edu.ua/handle/123456789/3638

    Linear Positive Magnetoresistivity of the Bi1.9Lu0.1Te3 Alloy with Inhomogeneous Micrograined Structure

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    Positive nonsaturating transverse magnetoresistivity (MR) has been observed below room temperature in the Bi1.9Lu0.1Te3 alloy with inhomogeneous micrograined structure. A crossover from parabolic MR ~ B2 dependence in low magnetic fields to linear MR ~ B dependence in high fields was found in the magnetoresistivity curves. The crossover field is shifted to lower magnetic fields as temperature decreases. Within the temperature range of β€œmetal” type of conductivity, the temperature dependences of the specific electrical resistivity and MR magnitude are determined by the temperature dependence of the carrier mobility due to acoustic phonon scattering. Linear MR can be associated with microstructural inhomogeneity leading to strong electrical disorder of the Bi1.9Lu0.1Te3

    Electrical Resistivity Peculiarities of the Nanograined Bi2Te3 Material

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    The hot quasiisostaic pressure method was applied to sinter the nanograined Bi2Te3 material. The samples with various mean grain size of 64, 61, 56 and 51 nm were prepared by changing the pressure of sintering. It was found that the specific electrical resistivity of the material under study increases when the mean grain size decreases. The Hall effect was measured to extract the concentration and mobility values of the charge carries. It was found that the electron concentration decreases as the mean grain size decreases while the electron mobility has extreme dependence on the grain size

    Hopping Conductivity and Negative Magnetoresistance of the Bulk Nanograined Bi2Te3 Material

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    The bulk nanograined Bi2Te3 material was prepared by the microwave assisted solvothermal method and cold isostatic pressure method. It was found that above T* β‰ˆ 190 K the temperature dependence of the specific electrical resistivity of material is of metallic type, while below this temperature a semiconductor conductivity takes place. Within the temperature Ξ”T β‰ˆ 90 K-35 K interval the electrical conductivity of material can be described by the variable-range hopping conductivity mechanism. Negative magnetoresistance was observed at the same temperature interval

    Plasma focus installation as a tool for the study of the interaction of high power plasma streams with condensed matter

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    In this work the possibilities of the use of the high-current discharges of Plasma Focus type for the investigation of the effect of plasma on the materials are discussed. From this point of view the properties of plasma streams and ion beams arising in the PF discharges are studied. Here, as an example of an application of the Plasma Focus device (PF), we studied the influence on Vanadium (perspective material in nuclear power engineering) a cumulative streams producing in the P

    Unconventional ferromagnetism and transport properties of (In,Mn)Sb dilute magnetic semiconductor

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    Narrow-gap higher mobility semiconducting alloys In_{1-x}Mn_{x}Sb were synthesized in polycrystalline form and their magnetic and transport properties have been investigated. Ferromagnetic response in In_{0.98}Mn_{0.02}Sb was detected by the observation of clear hysteresis loops up to room temperature in direct magnetization measurements. An unconventional (reentrant) magnetization versus temperature behavior has been found. We explained the observed peculiarities within the frameworks of recent models which suggest that a strong temperature dependence of the carrier density is a crucial parameter determining carrier-mediated ferromagnetism of (III,Mn)V semiconductors. The correlation between magnetic states and transport properties of the sample has been discussed. The contact spectroscopy method is used to investigate a band structure of (InMn)Sb near the Fermi level. Measurements of the degree of charge current spin polarization have been carried out using the point contact Andreev reflection (AR) spectroscopy. The AR data are analyzed by introducing a quasiparticle spectrum broadening, which is likely to be related to magnetic scattering in the contact. The AR spectroscopy data argued that at low temperature the sample is decomposed on metallic ferromagnetic clusters with relatively high spin polarization of charge carriers (up to 65% at 4.2K) within a cluster.Comment: 19 pages, 9 figures, 1 tabl

    A multi-country test of brief reappraisal interventions on emotions during the COVID-19 pandemic

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    The COVID-19 pandemic has increased negative emotions and decreased positive emotions globally. Left unchecked, these emotional changes might have a wide array of adverse impacts. To reduce negative emotions and increase positive emotions, we tested the effectiveness of reappraisal, an emotion-regulation strategy that modifies how one thinks about a situation. Participants from 87 countries and regions (n = 21,644) were randomly assigned to one of two brief reappraisal interventions (reconstrual or repurposing) or one of two control conditions (active or passive). Results revealed that both reappraisal interventions (vesus both control conditions) consistently reduced negative emotions and increased positive emotions across different measures. Reconstrual and repurposing interventions had similar effects. Importantly, planned exploratory analyses indicated that reappraisal interventions did not reduce intentions to practice preventive health behaviours. The findings demonstrate the viability of creating scalable, low-cost interventions for use around the world

    Π’ΡƒΠ½Π½Π΅Π»ΡŒΠ½Π°Ρ ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒ свСрхпроводящСго индия Π² пористом стСклС

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    Π•Π»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π½ΠΈΠΉ ΠΎΠΏΡ–Ρ€ Ρ–Π½Π΄Ρ–ΡŽ Ρ–Π½Π΄Ρ–ΡŽ Π² пористому склі Π· Ρ€ΠΎΠ·ΠΌΡ–Ρ€ΠΎΠΌ ΠΏΠΎΡ€ 7 Π½ΠΌ Π±ΡƒΠ»ΠΎ Π²ΠΈΠ²Ρ‡Π΅Π½ΠΎ Π² Ρ–Π½Ρ‚Π΅Ρ€Π²Π°Π»Ρ– Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€ 2,3-300 K. ВиявлСно, Ρ‰ΠΎ дослідТуваний ΠΌΠ°Ρ‚Π΅Ρ€Ρ–Π°Π» Π·Π°Π·Π½Π°Ρ” ΠΏΠ΅Ρ€Π΅Ρ…Ρ–Π΄ Π² Π½Π°Π΄ΠΏΡ€ΠΎΠ²Ρ–Π΄Π½ΠΈΠΉ стан ΠΏΡ€ΠΈ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ– TC = 3,9 K. Π Ρ–Π·ΠΊΠΈΠΉ асимСтричний ΠΏΡ–ΠΊ Π½Π° ΠΊΡ€ΠΈΠ²Ρ–ΠΉ R(T) виявлСний ΠΏΡ€ΠΈ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ– 6,4 K. Π’ΠΏΠ΅Ρ€ΡˆΠ΅ R(T) Π·Π°Π»Π΅ΠΆΠ½Ρ–ΡΡ‚ΡŒ ΠΏΡ€ΠΎΠ°Π½Π°Π»Ρ–Π·ΠΎΠ²Π°Π½Π° для Π½ΠΎΡ€ΠΌΠ°Π»ΡŒΠ½ΠΎΡ— Ρ„Π°Π·ΠΈ. ВстановлСно, Ρ‰ΠΎ Π² Ρ–Π½Ρ‚Π΅Ρ€Π²Π°Π»Ρ– Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€ 15-80 K Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½Π° Π·Π°Π»Π΅ΠΆΠ½Ρ–ΡΡ‚ΡŒ ΠΎΠΏΠΎΡ€Ρƒ ΠΎΠΏΠΈΡΡƒΡ”Ρ‚ΡŒΡΡ ΠΌΠ΅Ρ…Π°Π½Ρ–Π·ΠΌΠΎΠΌ Ρ‚ΡƒΠ½Π΅Π»ΡŽΠ²Π°Π½Π½Ρ носіїв заряду Π² Ρ€Π°ΠΌΠΊΠ°Ρ… ΠΌΠΎΠ΄Π΅Π»Ρ– Π¨Π΅Π½Π³Π°. ДослідТуваний ΠΌΠ°Ρ‚Π΅Ρ€Ρ–Π°Π» ΠΌΠΎΠΆΠ½Π° розглядати як Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π½ΠΎ Π½Π΅ΠΎΠ΄Π½ΠΎΡ€Ρ–Π΄Π½ΠΈΠΉ ΠΌΠ°Ρ‚Π΅Ρ€Ρ–Π°Π», Π² якому ΠΌΠ΅Ρ‚Π°Π»Π΅Π²Ρ– області Π² ΠΏΠΎΡ€Π°Ρ… ΠΊΠΎΠ½Ρ‚Π°ΠΊΡ‚ΡƒΡŽΡ‚ΡŒ ΠΌΡ–ΠΆ собою Π·Π° допомогою Π΄Ρ–Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π½ΠΈΡ… містком ΠΌΠ°Ρ‚Ρ€ΠΈΡ†Ρ– Π·Ρ– скла. ΠŸΠ΅Ρ€Π΅Π½Π΅ΡΠ΅Π½Π½Ρ заряду ΠΌΡ–ΠΆ ΠΌΠ΅Ρ‚Π°Π»Π΅Π²ΠΈΠΌΠΈ областями Π²Ρ–Π΄Π±ΡƒΠ²Π°Ρ”Ρ‚ΡŒΡΡ Π·Π° допомогою Ρ‚ΡƒΠ½Π΅Π»ΡŽΠ²Π°Π½Π½Ρ Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Ρ–Π² Ρ‡Π΅Ρ€Π΅Π· ΠΏΠΎΡ‚Π΅Π½Ρ†Ρ–ΠΉΠ½Ρ– Π±Π°Ρ€'Ρ”Ρ€ΠΈ, Π²Ρ–Π΄ΠΏΠΎΠ²Ρ–Π΄Π½Ρ– Π΄Ρ–Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π½ΠΈΠΌ містках.ЭлСктричСскоС сопротивлСниС индия индия Π² пористом стСклС с Ρ€Π°Π·ΠΌΠ΅Ρ€ΠΎΠΌ ΠΏΠΎΡ€ 7 Π½ΠΌ Π±Ρ‹Π»ΠΎ ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΎ Π² ΠΈΠ½Ρ‚Π΅Ρ€Π²Π°Π»Π΅ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€ 2,3-300 K. ΠžΠ±Π½Π°Ρ€ΡƒΠΆΠ΅Π½ΠΎ, Ρ‡Ρ‚ΠΎ исслСдуСмый ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π» ΠΏΡ€Π΅Ρ‚Π΅Ρ€ΠΏΠ΅Π²Π°Π΅Ρ‚ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄ Π² свСрхпроводящСС состояниС ΠΏΡ€ΠΈ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π΅ TC = 3,9 K. Π Π΅Π·ΠΊΠΈΠΉ ассимСтричный ΠΏΠΈΠΊ Π½Π° ΠΊΡ€ΠΈΠ²ΠΎΠΉ R(T) ΠΎΠ±Π½Π°Ρ€ΡƒΠΆΠ΅Π½ ΠΏΡ€ΠΈ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π΅ 6,4 K. Π’ΠΏΠ΅Ρ€Π²Ρ‹Π΅ R(T) Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ‚ΡŒ ΠΏΡ€ΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡ€ΠΎΠ²Π°Π½Π° для Π½ΠΎΡ€ΠΌΠ°Π»ΡŒΠ½ΠΎΠΉ Ρ„Π°Π·Ρ‹. УстановлСно, Ρ‡Ρ‚ΠΎ Π² ΠΈΠ½Ρ‚Π΅Ρ€Π²Π°Π»Π΅ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€ 15-80 K тСмпСратурная Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ‚ΡŒ сопротивлСния описываСтся ΠΌΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌΠΎΠΌ туннСлирования носитСлСй заряда Π² Ρ€Π°ΠΌΠΊΠ°Ρ… ΠΌΠΎΠ΄Π΅Π»ΠΈ Π¨Π΅Π½Π³Π°. Π˜ΡΡΠ»Π΅Π΄ΡƒΠ΅ΠΌΡ‹ΠΉ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π» ΠΌΠΎΠΆΠ½ΠΎ Ρ€Π°ΡΡΠΌΠ°Ρ‚Ρ€ΠΈΠ²Π°Ρ‚ΡŒ ΠΊΠ°ΠΊ элСктричСски Π½Π΅ΠΎΠ΄Π½ΠΎΡ€ΠΎΠ΄Π½Ρ‹ΠΉ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π», Π² ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΌ мСталличСскиС области Π² ΠΏΠΎΡ€Π°Ρ… ΠΊΠΎΠ½Ρ‚Π°ΠΊΡ‚ΠΈΡ€ΡƒΡŽΡ‚ ΠΌΠ΅ΠΆΠ΄Ρƒ собой посрСдством диэлСктричСских мостиков ΠΌΠ°Ρ‚Ρ€ΠΈΡ†Ρ‹ ΠΈΠ· стСкла. ΠŸΠ΅Ρ€Π΅Π½ΠΎΡ заряда ΠΌΠ΅ΠΆΠ΄Ρƒ мСталличСскими областями происходит посрСдством туннСлирования элСктронов Ρ‡Π΅Ρ€Π΅Π· ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Π΅ Π±Π°Ρ€ΡŒΠ΅Ρ€Ρ‹, ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΠ΅ диэлСктричСским мостикам.Electrical resistance of indium in 7 nm-pore glass has been studied in the temperature 2.3-300 K interval. It was found that material under study undergoes the transition into the superconducting state at TC = 3.9 K. A sharp asymmetric R(T) maximum was found at temperature of 6.4 K. The R(T) dependence has been for the first time analyzed for the normal phase. It was found that the temperature dependence of the resistance in the temperature 15-80 K interval can be described by tunnelling mechanism of the charge carriers in the frames of the Sheng’s model. Material under study can be considered as electrically inhomogeneous material in which metallic domains in pores are contacting each other via dielectric bridges of glass matrix. A charge transfer between the metallic domains can be realized by the electron tunneling through the potential barriers corresponding to the dielectric bridges
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