172 research outputs found

    Non-resonant wave front reversal of spin waves used for microwave signal processing

    Full text link
    It is demonstrated that non-resonant wave front reversal (WFR) of spin-wave pulses caused by pulsed parametric pumping can be effectively used for microwave signal processing. When the frequency band of signal amplification by pumping is narrower than the spectral width of the signal, the non-resonant WFR can be used for the analysis of the signal spectrum. In the opposite case the non-resonant WFR can be used for active (with amplification) filtering of the input signal.Comment: 4 pages, 3 figure

    Field-induced transition from parallel to perpendicular parametric pumping for a microstrip transducer

    Full text link
    Microstrip transducers used for the excitation of spin waves in magnetic films possess two characteristic properties: high spatial localization of the microwave magnetic field and the presence of field components parallel and perpendicular to the bias field. Here, the effects of these features on the process of parametric pumping are presented. By microwave measurements of the spin-wave instability threshold a transition from parallel pumping to perpendicular pumping at the critical field HcH_{\rm c} with the minimal threshold is observed. This transition is accompanied by a sharp threshold increase above the critical field due to the spatial confinement of the pump region.Comment: 4 pages, 2 figure

    Dispersion Characteristics of Spin-Electromagnetic Waves in Planar Multiferroic Structures with Coplanar Transmission Line

    Get PDF
    Introduction. The distinctive feature of a coplanar transmission line with thin ferrite and ferroelectric films is the absence of undesirable irregularities in dispersion for relatively low frequencies when the wavelength approaches the thickness of ferroelectric layer, in contrast to the open ferrite-ferroelectric wave-guiding structure without metallization.Aim. The purpose of this paper is twofold: (i) to develop a theory of the wave spectra in the multiferroic structures based on the coplanar lines; (ii) using this theory to find ways to enhance the electric tuning range.Materials and methods. The dispersion relation for spin-electromagnetic waves was derived through analytical solution of the full set of the Maxwell's equations utilizing a method of approximate boundary conditions.Results. A theory of spin-electromagnetic wave spectrum has been developed for the thin-film ferrite-ferroelectric structure based on a coplanar transmission line. According to this theory, dispersion characteristics of the spin-electromagnetic waves were described and analyzed for different parameters of the structure. The obtained results show that the investigated structure demonstrates a dual electric and magnetic field tunability of wave spectra. Its efficiency increases with an increase in the thicknesses of the ferrite and ferroelectric films and with a decrease in the width of the central metal strip.Conclusion. The distinctive features of the proposed coplanar waveguides are the thin-film planar topology and dual tunability of the wave spectra. All these advantages make the proposed structures perspective for development of new microwave devices.Introduction. The distinctive feature of a coplanar transmission line with thin ferrite and ferroelectric films is the absence of undesirable irregularities in dispersion for relatively low frequencies when the wavelength approaches the thickness of ferroelectric layer, in contrast to the open ferrite-ferroelectric wave-guiding structure without metallization.Aim. The purpose of this paper is twofold: (i) to develop a theory of the wave spectra in the multiferroic structures based on the coplanar lines; (ii) using this theory to find ways to enhance the electric tuning range.Materials and methods. The dispersion relation for spin-electromagnetic waves was derived through analytical solution of the full set of the Maxwell's equations utilizing a method of approximate boundary conditions.Results. A theory of spin-electromagnetic wave spectrum has been developed for the thin-film ferrite-ferroelectric structure based on a coplanar transmission line. According to this theory, dispersion characteristics of the spin-electromagnetic waves were described and analyzed for different parameters of the structure. The obtained results show that the investigated structure demonstrates a dual electric and magnetic field tunability of wave spectra. Its efficiency increases with an increase in the thicknesses of the ferrite and ferroelectric films and with a decrease in the width of the central metal strip.Conclusion. The distinctive features of the proposed coplanar waveguides are the thin-film planar topology and dual tunability of the wave spectra. All these advantages make the proposed structures perspective for development of new microwave devices

    Theory for a dissipative droplet soliton excited by a spin torque nanocontact

    Full text link
    A novel type of solitary wave is predicted to form in spin torque oscillators when the free layer has a sufficiently large perpendicular anisotropy. In this structure, which is a dissipative version of the conservative droplet soliton originally studied in 1977 by Ivanov and Kosevich, spin torque counteracts the damping that would otherwise destroy the mode. Asymptotic methods are used to derive conditions on perpendicular anisotropy strength and applied current under which a dissipative droplet can be nucleated and sustained. Numerical methods are used to confirm the stability of the droplet against various perturbations that are likely in experiments, including tilting of the applied field, non-zero spin torque asymmetry, and non-trivial Oersted fields. Under certain conditions, the droplet experiences a drift instability in which it propagates away from the nanocontact and is then destroyed by damping.Comment: 15 pages, 12 figure

    Generation of spin-wave dark solitons with phase engineering

    Full text link
    We generate experimentally spin-wave envelope dark solitons from rectangular high-frequency dark input pulses with externally introduced phase shifts in yttrium-iron garnet magnetic fims. We observe the generation of both odd and even numbers of magnetic dark solitons when the external phase shift varies. The experimental results are in a good qualitative agreement with the theory of the dark-soliton generation in magnetic films developed earlier [Phys. Rev. Lett. 82, 2583 (1999)].Comment: 6 pages, including 7 figures, submitted to Phys. Rev.

    Formation of Random Dark Envelope Solitons from Incoherent Waves

    Full text link
    This letter reports experimental results on a new type of soliton: the random temporal dark soliton. One excites an incoherent large-amplitude propagating spin-wave packet in a ferromagnetic film strip with a repulsive, instantaneous nonlinearity. One then observes the random formation of dark solitons from this wave packet. The solitons appear randomly in time and in position relative to the entire wave packet. They can be gray or black. For wide and/or very strong spin-wave packets, one also observes multiple dark solitons. In spite of the randomness of the initial wave packets and the random formation processes, the solitons show signatures that are found for conventional coherent dark solitons.Comment: 10 pages, 4 figures, double-spaced preprint forma

    АналитичСская тСория диспСрсии оптичСских Π²ΠΎΠ»Π½ рСгулярных ΠΌΠΈΠΊΡ€ΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄ΠΎΠ²

    Get PDF
    A method for analysis of dispersion characteristics of guided optical modes propagating in the optical waveguides with small cross-sections is proposed. The method is based on introduction of a correction factor for a longitudinal wavenumber of propagating modes. The correction factor arises when a cross-section of the basic rectangular waveguide is subjected to perturbation. The electromagnetic field distributions along with the mode longitudinal wavenumber are found by means of variable separation method. The longitudinal wavenumber correction factor is analytically calculated in terms of coupled mode theory. The combined use of the complete set of equations of electrodynamics together with the concept of effective sources gives rise to the correction factor in the form of an intermodal coupling coefficient. It is pointed out that the coupling coefficient consists of two components, namely bulk and surface, owing to accurate account of the electrodynamics boundary conditions. Using the method proposed, the dispersion characteristics of the fundamental modes propagating in the practically employed optical waveguides having a trapezoidal cross-section are calculated. An impact of the waveguide cross-section shape to cladding dielectric constant ratio on the mode dispersion characteristics is analyzed. The necessity to take into consideration an imperfection of the waveguide cross-section in a wide range of operating wavelengths is demonstrated.Π Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½ ΠΌΠ΅Ρ‚ΠΎΠ΄ Π°Π½Π°Π»ΠΈΠ·Π° диспСрсионных характСристик направляСмых ΠΌΠΎΠ΄ Π² рСгулярных оптичСских ΠΌΠΈΠΊΡ€ΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π°Ρ… ΠΌΠ°Π»ΠΎΠ³ΠΎ ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎΠ³ΠΎ сСчСния. ΠœΠ΅Ρ‚ΠΎΠ΄ основан Π½Π° Π²Π²Π΅Π΄Π΅Π½ΠΈΠΈ ΠΏΠΎΠΏΡ€Π°Π²ΠΎΠΊ ΠΊ ΠΏΡ€ΠΎΠ΄ΠΎΠ»ΡŒΠ½ΠΎΠΌΡƒ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΌΡƒ числу ΠΌΠΎΠ΄ ΠΏΡ€ΡΠΌΠΎΡƒΠ³ΠΎΠ»ΡŒΠ½ΠΎΠ³ΠΎ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π°, Π²Ρ‹Π±Ρ€Π°Π½Π½ΠΎΠ³ΠΎ Π² качСствС Π±Π°Π·ΠΎΠ²ΠΎΠ³ΠΎ, ΠΏΡ€ΠΈ искаТСнии Ρ„ΠΎΡ€ΠΌΡ‹ Π΅Π³ΠΎ ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎΠ³ΠΎ сСчСния. РаспрСдСлСния элСктромагнитного поля ΠΈ ΠΏΡ€ΠΎΠ΄ΠΎΠ»ΡŒΠ½ΠΎΠ³ΠΎ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ³ΠΎ числа Π±Π°Π·ΠΎΠ²ΠΎΠ³ΠΎ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π° Ρ€Π°ΡΡΡ‡ΠΈΡ‚Ρ‹Π²Π°ΡŽΡ‚ΡΡ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ раздСлСния ΠΏΠ΅Ρ€Π΅ΠΌΠ΅Π½Π½Ρ‹Ρ…. ΠŸΠΎΠΏΡ€Π°Π²ΠΊΠ° ΠΊ ΠΏΡ€ΠΎΠ΄ΠΎΠ»ΡŒΠ½ΠΎΠΌΡƒ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΌΡƒ числу рассчитываСтся аналитичСски Π² Ρ‚Π΅Ρ€ΠΌΠΈΠ½Π°Ρ… Ρ‚Π΅ΠΎΡ€ΠΈΠΈ связанных ΠΌΠΎΠ΄. Указанная ΠΏΠΎΠΏΡ€Π°Π²ΠΊΠ° Π² Π²ΠΈΠ΄Π΅ коэффициСнта ΠΌΠ΅ΠΆΠΌΠΎΠ΄ΠΎΠ²ΠΎΠΉ связи Π²ΠΎΠ·Π½ΠΈΠΊΠ°Π΅Ρ‚ Π½Π° основании совмСстного использования ΠΏΠΎΠ»Π½ΠΎΠΉ систСмы ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ МаксвСлла ΠΏΡ€ΠΈ Π²Π²Π΅Π΄Π΅Π½ΠΈΠΈ понятия ΠΎΠ± эффСктивных источниках. Показано, Ρ‡Ρ‚ΠΎ ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹ΠΉ ΡƒΡ‡Π΅Ρ‚ Π³Ρ€Π°Π½ΠΈΡ‡Π½Ρ‹Ρ… условий элСктродинамики ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ Ρ„ΠΎΡ€ΠΌΠ΅ коэффициСнта связи, Π²ΠΊΠ»ΡŽΡ‡Π°ΡŽΡ‰Π΅ΠΉ ΠΎΠ±ΡŠΠ΅ΠΌΠ½ΡƒΡŽ ΠΈ ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½ΠΎΡΡ‚Π½ΡƒΡŽ ΡΠΎΡΡ‚Π°Π²Π»ΡΡŽΡ‰ΠΈΠ΅. Π Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½Π½Ρ‹ΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄ ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ для расчСта диспСрсионных характСристик Π½ΠΈΠ·ΡˆΠΈΡ… Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π½Ρ‹Ρ… ΠΌΠΎΠ΄, Ρ€Π°ΡΠΏΡ€ΠΎΡΡ‚Ρ€Π°Π½ΡΡŽΡ‰ΠΈΡ…ΡΡ Π² ΠΌΠΈΠΊΡ€ΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π°Ρ… Ρ‚Ρ€Π°ΠΏΠ΅Ρ†ΠΈΠ΅Π²ΠΈΠ΄Π½ΠΎΠ³ΠΎ сСчСния, примСняСмых Π½Π° ΠΏΡ€Π°ΠΊΡ‚ΠΈΠΊΠ΅. ΠŸΡ€ΠΎΠ΄Π΅ΠΌΠΎΠ½ΡΡ‚Ρ€ΠΈΡ€ΠΎΠ²Π°Π½ΠΎ влияниС ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎΠ³ΠΎ сСчСния ΠΌΠΈΠΊΡ€ΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π° Π½Π° диспСрсионныС характСристики ΠΌΠΎΠ΄ Π² зависимости ΠΎΡ‚ ΡΠΎΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΡ сторон, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΎΡ‚ ΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΡ Π·Π½Π°Ρ‡Π΅Π½ΠΈΠΉ диэлСктричСских проницаСмостСй сСрдцСвины ΠΌΠΈΠΊΡ€ΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π° ΠΈ Π΅Π³ΠΎ ΠΎΠ±ΠΎΠ»ΠΎΡ‡ΠΊΠΈ. Показана Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒ ΡƒΡ‡Π΅Ρ‚Π° влияния Ρ„ΠΎΡ€ΠΌΡ‹ ΠΌΠΈΠΊΡ€ΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π° Π½Π° диспСрсионныС характСристики ΠΌΠΎΠ΄ Π² ΡˆΠΈΡ€ΠΎΠΊΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ Π·Π½Π°Ρ‡Π΅Π½ΠΈΠΉ Ρ€Π°Π±ΠΎΡ‡ΠΈΡ… Π΄Π»ΠΈΠ½ Π²ΠΎΠ»Π½ ΠΈ ΠΏΡ€ΠΈ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… распрСдСлСниях диэлСктричСской проницаСмости Π²ΠΎΠ»Π½ΠΎΠ²Π΅Π΄ΡƒΡ‰Π΅ΠΉ структуры
    • …
    corecore