68 research outputs found

    The cyclic stability of rubber-like behaviour in stress-induced martensite aged Ni49Fe18Ga27Co6 (at.%) single crystals

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    In present work, the cyclic stability of the rubber-like behaviour (RLB) was investigated in Ni49Fe18Ga27Co6 (at. %) single crystals. Crystals were aged in the martensite phase at 423 K for 1 h under a compressive stress of 450 MPa, applied along the [110]B2[100]L10-direction. The RLB was induced by a preliminary chemical stabilization of the oriented L10-martensite during stress-induced martensite aging (SIM-aging) and following the reversible reorientation of martensitic variants under a compressive stress applied along the [001]B2[001]L10-direction. The high cyclic stability of the RLB was obtained in 200 loading/unloading cycles, due to the low reorientation stresses of the L10-martensite variants (no higher than 140 MPa) and the high strength properties of the L10-martensite (~1.6 GPa). The irreversible strain after 200 cycles did not exceed 0.6%. An increase in the number of cycles did not lead to the effect of destabilization of the L10-martensite

    Orientation dependence of superelasticity in quenched high-nickel Ti51.8Ni single crystals

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    The orientation dependence of the functional and mechanical properties of quenched Ti-51.8at.%Ni single crystals, undergoing a strain-glass transition upon cooling/heating was investigated. It was found that a compressive stress above 800 MPa leads to the B2-B190 martensitic transformation (MT), regardless of orientation. In the high-strength [0 0 1]-orientation, superelasticity (SE) was observed at 203–248 K, with a reversible strain of 2.3%. Degradation of SE at deforming stresses r > 1000 MPa was associated with the formation of {1 1 3}B2 twins during the reverse MT. In the low-strength 1 1 1-orientation, the formation of stress-induced B190 -martensite occurred simultaneously with the plastic deformation of the B2-phase (due to the formation of reorientation bands and dislocation slip) and a reversible strain was not observed

    Complex Study of Magnetization Reversal Mechanisms of FeNi/FeMn Bilayers Depending on Growth Conditions

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    Magnetization reversal processes in the NiFe/FeMn exchange biased structures with various antiferromagnetic layer thicknesses (0–50 nm) and glass substrate temperatures (17–600β—¦C) during deposition were investigated in detail. Magnetic measurements were performed in the temperature range from 80 K up to 300 K. Hysteresis loop asymmetry was found at temperatures lower than 150 K for the samples with an antiferromagnetic layer thickness of more than 10 nm. The average grain size of FeMn was found to increase with the AFM layer increase, and to decrease with the substrate temperature increase. Hysteresis loop asymmetry was explained in terms of the exchange spring model in the antiferromagnetic layer. Β© 2022 by the authors. Licensee MDPI, Basel, Switzerland.Ministry of Education and Science of the Russian Federation,Β Minobrnauka: FEUZ-2020-0051;Β AgentΓΊra na Podporu VΓ½skumu a VΓ½voja,Β APVV: APVV-20-0324Funding: This work has been supported by the grant of the Slovak Research and Development Agency under the contract No APVV-20-0324. This work was in part financially supported by the Ministry of Science and Higher Education of the Russian Federation, Subject of the state task No. FEUZ-2020-0051. The electron microscopy investigations were carried out on the equipment of Krasnoyarsk Regional Center of Research Equipment of Federal Research Center Β«Krasnoyarsk Science Center SB RASΒ»

    Π‘ΠΈΠ½Ρ‚Π΅Π·, микроструктура ΠΈ ΠΌΠ°Π³Π½ΠΈΡ‚Π½Ρ‹Π΅ свойства магнитомягких ΠΏΠ»Π΅Π½ΠΎΠΊ Π‘ΠΎΠ 

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    Soft magnetic thin CoP films were obtained by means of chemical metallization from aqueous cobalt salt solution in the presence of sodium hydroxide, citric acid and sodium hypophosphite as the reducing agent. The optimal values of the magnetic film parameters (saturation magnetization and width of ferromagnetic resonance line) were obtained by variation of composition of work solutions. It allows to reduce losses in their application in microwave devices. Microphotographs of magnetic film indicate a grain structure with a grain size of about 50 nm and presence of inclusions with the size of 3-5 nm. To determine the magnetic parameters of the investigated films the method of ferromagnetic resonance (FMR) absorption curves processing is used. The values of FMR line width and an effective magnetization of film material saturation were obtained.ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ исслСдования свойств магнитомягких Ρ‚ΠΎΠ½ΠΊΠΈΡ… ΠΏΠ»Π΅Π½ΠΎΠΊ Π‘ΠΎΠ , ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ химичСской ΠΌΠ΅Ρ‚Π°Π»Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ ΠΈΠ· Π²ΠΎΠ΄Π½ΠΎΠ³ΠΎ раствора Π½Π° основС Ρ†ΠΈΡ‚Ρ€Π°Ρ‚Π½Ρ‹Ρ… комплСксов с ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ Π² качСствС Ρ‰Π΅Π»ΠΎΡ‡Π½ΠΎΠ³ΠΎ Ρ€Π΅Π°Π³Π΅Π½Ρ‚Π° NaOH. Π‘ ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ Π²Π°Ρ€ΠΈΠ°Ρ†ΠΈΠΈ составов Ρ€Π°Π±ΠΎΡ‡ΠΈΡ… растворов ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Π΅ значСния ΠΌΠ°Π³Π½ΠΈΡ‚Π½Ρ‹Ρ… ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² ΠΏΠ»Π΅Π½ΠΎΠΊ: намагничСнности насыщСния ΠΈ ΡˆΠΈΡ€ΠΈΠ½Ρ‹ Π»ΠΈΠ½ΠΈΠΈ Ρ„Π΅Ρ€Ρ€ΠΎΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎΠ³ΠΎ рСзонанса

    The Clusters Self-Assembled Crystal and Magnetic Structure During the Martensite Transition in Fe86mn13c Alloy

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    In bulk and thin film state Fe86Mn13C alloy observed experimentally self-assembly of the crystal and magnetic structures on multiscale levels. Offered self-assembly cluster model of atomic structure based on the concept of a liquid-like state of the material in localized areas, formed in the waves of plastic deformation

    Phase with Spinel Structure Type in Plastically Deformed Niti

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    Π˜ΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ‹ ΠΎΠ±Ρ€Π°Π·Ρ†Ρ‹ сплава Ni51Ti49, ΠΏΠΎΠ΄Π²Π΅Ρ€Π³Π½ΡƒΡ‚Ρ‹Π΅ пластичСской Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ. ΠœΠΈΠΊΡ€ΠΎΡΡ‚Ρ€ΡƒΠΊΡ‚ΡƒΡ€Π° исслСдовалась ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ΠΏΡ€ΠΎΡΠ²Π΅Ρ‡ΠΈΠ²Π°ΡŽΡ‰Π΅ΠΉ элСктронной микроскопии ΠΈ ΠΌΠΈΠΊΡ€ΠΎΠ΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ Π½Π° микроскопС Hitachi 7700. Для исслСдования ΠΎΠ±Ρ€Π°Π·Ρ†ΠΎΠ² ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ ΠΏΡ€ΠΎΡΠ²Π΅Ρ‡ΠΈΠ²Π°ΡŽΡ‰Π΅ΠΉ элСктронной микроскопии (ПЭМ) с Π·ΠΎΠ½Ρ‹ Ρ€Π°Π·Ρ€Ρ‹Π²Π° растянутых ΠΎΠ±Ρ€Π°Π·Ρ†ΠΎΠ² Π²Ρ‹Ρ€Π΅Π·Π°Π»ΠΈ диски Π΄ΠΈΠ°ΠΌΠ΅Ρ‚Ρ€ΠΎΠΌ 3 ΠΌΠΌ, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ мСханичСски утоняли, Π·Π°Ρ‚Π΅ΠΌ элСктрохимичСским способом Ρ‚Ρ€Π°Π²ΠΈΠ»ΠΈ Π΄ΠΎ появлСния отвСрстия Π² Ρ†Π΅Π½Ρ‚Ρ€Π΅ диска. Π€ΠΈΠ½Π°Π»ΡŒΠ½Ρ‹ΠΌ этапом ΠΏΠΎΠ΄Π³ΠΎΡ‚ΠΎΠ²ΠΊΠΈ являлось ΠΈΠΎΠ½Π½ΠΎΠ΅ Ρ‚Ρ€Π°Π²Π»Π΅Π½ΠΈΠ΅ Π½Π° установкС PIPS (Gatan). Π£Ρ‚ΠΎΠ½Π΅Π½Π½Ρ‹Π΅ для ΠΏΡ€ΠΎΡΠ²Π΅Ρ‡ΠΈΠ²Π°ΡŽΡ‰Π΅ΠΉ элСктронной микроскопии ΠΎΠ±Ρ€Π°Π·Ρ†Ρ‹ Π±Ρ‹Π»ΠΈ ΠΏΠΎΠ΄Π²Π΅Ρ€Π³Π½ΡƒΡ‚Ρ‹ криомСханичСской ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠ΅ ΠΏΡƒΡ‚Π΅ΠΌ цикличСского охлаТдСния Π² ΠΆΠΈΠ΄ΠΊΠΎΠΌ Π°Π·ΠΎΡ‚Π΅. Π€Π°Π·ΠΎΠ²Ρ‹ΠΉ состав ΠΎΠ±Ρ€Π°Π·Ρ†ΠΎΠ² опрСдСляли ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ рСнтгСновских Π»ΡƒΡ‡Π΅ΠΉ Π² Π΄ΠΈΡ„Ρ€Π°ΠΊΡ‚ΠΎΠΌΠ΅Ρ‚Ρ€Π΅ Β«BrukerΒ» с использованиСм излучСния ΠΌΠ΅Π΄ΠΈ. Π’ Π·ΠΎΠ½Π°Ρ… Π»ΠΎΠΊΠ°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ ΠΎΠ±Π½Π°Ρ€ΡƒΠΆΠ΅Π½Ρ‹ Π»ΠΈΠ½Π·ΠΎΠ²ΠΈΠ΄Π½Ρ‹Π΅ кристаллы Ρ„Π°Π·Ρ‹ Ni2Ti3, содСрТащиС ΠΈΠ·Π³ΠΈΠ±Π½Ρ‹Π΅ экстинкционныС ΠΊΠΎΠ½Ρ‚ΡƒΡ€Ρ‹, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΡΠ²ΠΈΠ΄Π΅Ρ‚Π΅Π»ΡŒΡΡ‚Π²ΡƒΡŽΡ‚ ΠΎ Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ ΠΊΡ€ΠΈΠ²ΠΈΠ·Π½Π΅ кристалличСской Ρ€Π΅ΡˆΠ΅Ρ‚ΠΊΠΈ, ΠΏΠΎΡΠ²Π»ΡΡŽΡ‰Π΅ΠΉΡΡ Π² Π·ΠΎΠ½Π°Ρ… Π»ΠΎΠΊΠ°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ пластичСской Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ. Показано, Ρ‡Ρ‚ΠΎ кристалличСская структура Π»ΠΈΠ½Π·ΠΎΠ²ΠΈΠ΄Π½Ρ‹Ρ… кристаллов прСдставляСт собой Ρ„Π°Π·Ρƒ, ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‰ΡƒΡŽ структурным Ρ‚ΠΈΠΏΠΎΠΌ шпинСли с ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠΌ кристалличСской Ρ€Π΅ΡˆΠ΅Ρ‚ΠΊΠΈ 11,53Β±0,03 Γ…. Для формирования Π»ΠΈΠ½Π·ΠΎΠ²ΠΈΠ΄Π½Ρ‹Ρ… кристаллов нСравновСсной Ρ„Π°Π·Ρ‹ Ni2Ti3 Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎ пСрСраспрСдСлСниС ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚ΠΎΠ² исходного Ρ‚Π²Π΅Ρ€Π΄ΠΎΠ³ΠΎ раствора ΠΈΠ»ΠΈ ΠΈΠ½Ρ‚Π΅Ρ€ΠΌΠ΅Ρ‚Π°Π»Π»ΠΈΠ΄Π½Ρ‹Ρ… Ρ„Π°Π·. Π’ условиях локальной ΠΊΡ€ΠΈΠ²ΠΈΠ·Π½Ρ‹ кристалличСской Ρ€Π΅ΡˆΠ΅Ρ‚ΠΊΠΈ Π² Π·ΠΎΠ½Π°Ρ… ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½Π½Ρ‹Ρ… ΠΌΠ΅ΠΆΠ°Ρ‚ΠΎΠΌΠ½Ρ‹Ρ… расстояний Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡŽΡ‚ особыС структурныС состояния, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΏΠΎΠ²Ρ‹ΡˆΠ°ΡŽΡ‚ число стСпСнСй свободы Π² Π΄Π΅Ρ„ΠΎΡ€ΠΌΠΈΡ€ΡƒΠ΅ΠΌΠΎΠΌ Ρ‚Π²Π΅Ρ€Π΄ΠΎΠΌ Ρ‚Π΅Π»Π΅ ΠΈ Ρ‚Π°ΠΊΠΈΠΌ ΠΎΠ±Ρ€Π°Π·ΠΎΠΌ ΡΠΏΠΎΡΠΎΠ±ΡΡ‚Π²ΡƒΡŽΡ‚ появлСнию Π½ΠΎΠ²Ρ‹Ρ… Ρ„Π°Π·The alloy samples Ni51Ti49, subjected to plastic deformation were investigated. The microstructure and the microdiffraction were investigated by transmission electron microscopy Hitachi 7700. Discs with a diameter of 3 mm for investigation by transmission electron microscopy (TEM) was cut from the fracture zone of the stretched sample. They were mechanically thinned, then electrochemically etched until the hole in the center. The final step was to prepare ion etching in install PIPS (Gatan). TEM specimens were subjected cryomechanical processing. This was done by in liquid nitrogen cooling cyclically. The phase composition of the samples was determined by X-ray diffraction diffractometer "Bruker" using copper radiation. The lens-form crystals Ni2Ti3, containing bending contours, indicating significant internal stresses in the zones of stress localization were detected. The lens-form crystals can be represented as a non-equilibrium phase Ni2Ti3 with spinel structure type with lattice parameter 11,53 Β± 0,03 Γ…. For the formation of lenticular crystals of nonequilibrium phase Ni2Ti3 it is necessary redistribution of the original solid solution components. In local curvature of the crystalline lattice areas, the increased interatomic distances created the special structural states. These states increase the number of degrees of freedom in a deformable solid and thus contribute to the emergence of new phase

    Tunable magnetic properties of Ni-doped CoFe2O4 nanoparticles prepared by the sol\u2013gel citrate self-combustion method

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    The nanostructured spinel ferrites with complex stoichiometry are an important family of the materials in a number of applications, especially in electronics through their good electrical and magnetic properties. In the framework of this study, a set of mixed cobalt and nickel ferrites was prepared with the sol\u2013gel self-combustion route. The structural and morphological features of particles were studied with X-ray diffraction (XRD), Scanning Transmission Electron Microscopy (STEM) and Energy Dispersive X-ray analysis (EDX) techniques. The prepared particles show a crystalline nature with a monotonic distribution of the elements and particles size distribution in the range of 17\u201329 nm. The obtained particles demonstrate good magnetic properties with tunable saturation magnetization and magnetic anisotropy, i.e., coercivity depending on chemical composition

    ΠšΠ»Π°ΡΡ‚Π΅Ρ€Π½Π°Ρ самоорганизация кристалличСской ΠΈ ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎΠΉ структур Π² процСссС мартСнситного прСвращСния Π² сплавС Fe86Mn13C

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    In bulk and thin film state Fe86Mn13C alloy observed experimentally self-assembly of the crystal and magnetic structures on multiscale levels. Offered self-assembly cluster model of atomic structure based on the concept of a liquid-like state of the material in localized areas, formed in the waves of plastic deformationΠ’ массивных ΠΈ Ρ‚ΠΎΠ½ΠΊΠΎΠΏΠ»Π΅Π½ΠΎΡ‡Π½Ρ‹Ρ… ΠΎΠ±Ρ€Π°Π·Ρ†Π°Ρ… сплава Fe86Mn13C ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎ Π½Π°Π±Π»ΡŽΠ΄Π°Π΅Ρ‚ΡΡ самоорганизация кристалличСской ΠΈ ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎΠΉ структур Π½Π° Ρ€Π°Π·Π½ΠΎΠΌΠ°ΡΡˆΡ‚Π°Π±Π½Ρ‹Ρ… уровнях. ΠŸΡ€Π΅Π΄Π»Π°Π³Π°Π΅Ρ‚ΡΡ кластСрная модСль Π°Ρ‚ΠΎΠΌΠ½ΠΎΠΉ самоорганизации, основанная Π½Π° ΠΊΠΎΠ½Ρ†Π΅ΠΏΡ†ΠΈΠΈ ΠΆΠΈΠ΄ΠΊΠΎΠΏΠΎΠ΄ΠΎΠ±Π½ΠΎΠ³ΠΎ состояния ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° Π² Π»ΠΎΠΊΠ°Π»ΡŒΠ½Ρ‹Ρ… участках, ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½Π½Ρ‹Ρ… Π²ΠΎΠ»Π½Π°ΠΌΠΈ пластичСской Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈ
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