59 research outputs found

    ВлияниС ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ высокоинтСнсивным ΠΏΠΎΡ‚ΠΎΠΊΠΎΠΌ ΠΈΠΎΠ½ΠΎΠ² Zr Π½Π° структуру ΠΈ мСханичСскиС свойства высокопрочной стали 30Π₯ГБН2А

    Get PDF
    ИсслСдованиС структуры ΠΌΠΎΠ΄ΠΈΡ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ повСрхностного слоя высокопрочной стали30Π₯ГБН2А ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ оптичСской ΠΏΡ€ΠΎΡΠ²Π΅Ρ‡ΠΈΠ²Π°ΡŽΡ‰Π΅ΠΉ элСктронной микроскопии, Π° Ρ‚Π°ΠΊ ΠΆΠ΅ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² рСнтгСновской Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ. Π˜ΡΠΏΡ‹Ρ‚Π°Π½ΠΈΡ Π½Π° статичСскоС ΠΈ цикличСскоС растяТСниС проводилидля ΡΡ‚Π°Π»ΡŒΠ½Ρ‹Ρ… ΠΎΠ±Ρ€Π°Π·Ρ†ΠΎΠ² Π² состоянии поставки, Π° Ρ‚Π°ΠΊ ΠΆΠ΅ послС ΠΌΠΎΠ΄ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΠΈ повСрхностного слояпотоком ΠΈΠΎΠ½ΠΎΠ² Zr

    Influence of ion-beam treatment on structure and defor-mation resistance of 12Cr1MoV steel under static, cyclic and dynamic loading

    Get PDF
    Features of modification of structure and properties of 12Cr1MoV steel subjected to ion-beam irradiation by zirconium ion beam have been investigated with the use of optical and electron microscopy, and microhardness measurement. It was shown that after the treat-ment the modification occurs across the entire cross-section of specimens with the thickness of 1 mm. Changes in mechanical properties of these specimens under static, cyclic and impact loading were interpreted in terms of identified structure modifications

    Structural levels of deformation and failure of heat-resistant 12Cr1MoV steel modified by vacuum arc treatment by Zr{+} ion beam

    Get PDF
    Study of structural changes occurring in the surface layer modified by ion-beam irradiation was carried out by means of optical, scanning and transmission electron microscopy. It was shown that irradiation induces the structure modification not only in the surface layer, but along the entire cross section of 1 mm thick specimens. It was elucidated that the complex pattern of structural changes is responsible for the pronounced variation of mechanical properties taking place under static tension and cyclic alternating bending

    Sputtered NbN Films for Ultrahigh Performance Superconducting Nanowire Single-Photon Detectors

    Full text link
    Nowadays ultrahigh performance superconducting nanowire single-photon detectors are the key elements in a variety of devices from biological research to quantum communications and computing. Accurate tuning of superconducting material properties is a powerful resource for fabricating single-photon detectors with a desired properties. Here, we report on the major theoretical relations between ultrathin niobium nitride (NbN) films properties and superconducting nanowire single-photon detectors characteristics, as well as ultrathin NbN films properties dependence on reactive magnetron sputtering recipes. Based on this study we formulate the exact requirements to ultrathin NbN films for ultrahigh performance superconducting nanowire single-photon detectors. Then, we experimentally study ultrathin NbN films properties (morphology, crystalline structure, critical temperature, sheet resistance) on silicon, sapphire, silicon dioxide and silicon nitride substrates sputtered with various recipes. We demonstrate ultrathin NbN films (obtained with more than 100 films deposition) with a wide range of critical temperature from 2.5 to 12.1 K and sheet resistance from 285 to 2000 ~Ξ©\Omega/sq, as well as investigate a sheet resistance evolution over for more than 40\% within two years. Finally, we found out that one should use ultrathin NbN films with specific critical temperature near 9 K and sheet resistance of 400 ~Ξ©\Omega/sq for ultrahigh performance SNSPD.Comment: The following article has been submitted to APL Materials. After it is published, it will be found at https://pubs.aip.org/aip/apm. Copyright 2023 Author(s). This article is distributed under a Creative Commons Attribution (CC BY) Licens

    Origin of exchange bias in [Co/Pt]ML/Fe multilayer with orthogonal magnetic anisotropies

    Full text link
    Magnetization reversal of soft ferromagnetic Fe layer, coupled to [Co/Pt]ML multilayer [ML] with perpendicular magnetic anisotropy (PMA), has been studied in-situ with an aim to understand the origin of exchange bias (EB) in orthogonal magnetic anisotropic systems. The interface remanant state of the ML is modified by magnetic field annealing, and the effect of the same on the soft Fe layer is monitored using the in-situ magneto-optical Kerr effect (MOKE). A considerable shift in the Fe layer hysteresis loop from the centre and an unusual increase in the coercivity, similar to exchange bias phenomena, is attributed to the exchange coupling at the [Co/Pt]ML and Fe interface. The effect of the coupling on spin orientation at the interface is further explored precisely by performing an isotope selective grazing incident nuclear resonance scattering (GINRS) technique. Here, the interface selectivity is achieved by introducing a 2 nm thick Fe57 marker between [Co/Pt]ML and Fe layers. Interface sensitivity is further enhanced by performing measurements under the x-ray standing wave conditions. The combined MOKE and GINRS analysis revealed the unidirectional pinning of the Fe layer due to the net in-plane magnetic spin at the interface caused by magnetic field annealing. Unidirectional exchange coupling or pinning at the interface, which may be due to the formation of asymmetrical closure domains, is found responsible for the origin of EB with an unusual increase in coercivity.Comment: 9 figures, 1 tabl

    Rocking curve measurements revisited

    Get PDF
    The study of materials by diffraction methods started about 100 years ago with the pioneering experiment of Laue, Friedrich and Knipping, when the first X-ray diffraction patterns of single crystals were obtained (Friedrich et al., 1912). This was the beginning of a rapid development fostering many diffraction-based methods and techniques, which is still continuing. The measurement of rocking curves and the associated derived quantitative parameters, such as the β€˜full width at half-maximum’ (FWHM) of the curves, has been performed since at least 1921 (Davis & Stempel, 1921) by exploiting the X-ray diffraction (XRD) properties of crystals. Since then, this has become one of the most powerful methods for the diffraction-based characterization of crystalline materials. The experimentally closely related method of X-ray diffraction imaging or X-ray diffraction topography has been used since about 1931 (Berg, 1931). Soon after World War II, the requirements of the electronics industry for the nondestructive analysis of defects in semiconductor materials like silicon and germanium (and others) boosted the improvement of these methods to their modern high-resolution variants like high-resolution X-ray diffraction and in particular high-resolution and high strain sensitivity X-ray topography (Bond & Andrus, 1952; Lang, 1957). This evolution was additionally accelerated in the late 1970s by the use of synchrotrons as dedicated X-ray sources and later on, starting in the 1990s, by the use of third-generation synchrotron sources...

    Magnetic Dirac semimetal state of (Mn,Ge)Bi2_2Te4_4

    Full text link
    For quantum electronics, the possibility to finely tune the properties of magnetic topological insulators (TIs) is a key issue. We studied solid solutions between two isostructural Z2_2 TIs, magnetic MnBi2_2Te4_4 and nonmagnetic GeBi2_2Te4_4, with Z2_2 invariants of 1;000 and 1;001, respectively. For high-quality, large mixed crystals of Gex_xMn1βˆ’x_{1-x}Bi2_2Te4_4, we observed linear x-dependent magnetic properties, composition-independent pairwise exchange interactions along with an easy magnetization axis. The bulk band gap gradually decreases to zero for xx from 0 to 0.4, before reopening for x>0.6x>0.6, evidencing topological phase transitions (TPTs) between topologically nontrivial phases and the semimetal state. The TPTs are driven purely by the variation of orbital contributions. By tracing the x-dependent 6p6p contribution to the states near the fundamental gap, the effective spin-orbit coupling variation is extracted. As xx varies, the maximum of this contribution switches from the valence to the conduction band, thereby driving two TPTs. The gapless state observed at x=0.42x=0.42 closely resembles a Dirac semimetal above the Neel temperature and shows a magnetic gap below, which is clearly visible in raw photoemission data. The observed behavior of the Gex_xMn1βˆ’x_{1-x}Bi2_2Te4_4 system thereby demonstrates an ability to precisely control topological and magnetic properties of TIs

    Π˜ΡΡ‚ΠΎΡ€ΠΈΡ‡Π΅ΡΠΊΠΈΠ΅ аспСкты матСматичСского Π°Π½Π°Π»ΠΈΠ·Π° Π΄ΠΈΠ°Π³Ρ€Π°ΠΌΠΌ Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ мСталличСских ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ²

    Get PDF
    .
    • …
    corecore