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Analyzer-free, intensity-based, wide-field magneto-optical microscopy
In conventional Kerr and Faraday microscopy, the sample is illuminated with plane-polarized light, and a magnetic domain contrast is generated by an analyzer making use of the Kerr or Faraday rotation. Here, we demonstrate possibilities of analyzer-free magneto-optical microscopy based on magnetization-dependent intensity modulations of the light. (i) The transverse Kerr effect can be applied for in-plane magnetized material, as demonstrated for an FeSi sheet. (ii) Illuminating that sample with circularly polarized light leads to a domain contrast with a different symmetry from the conventional Kerr contrast. (iii) Circular polarization can also be used for perpendicularly magnetized material, as demonstrated for garnet and ultrathin CoFeB films. (iv) Plane-polarized light at a specific angle can be employed for both in-plane and perpendicular media. (v) Perpendicular light incidence leads to a domain contrast on in-plane materials that is quadratic in the magnetization and to a domain boundary contrast. (vi) Domain contrast can even be obtained without a polarizer. In cases (ii) and (iii), the contrast is generated by magnetic circular dichroism (i.e., differential absorption of left- and right-circularly polarized light induced by magnetization components along the direction of light propagation), while magnetic linear dichroism (differential absorption of linearly polarized light induced by magnetization components transverse to propagation) is responsible for the contrast in case (v). The domain-boundary contrast is due to the magneto-optical gradient effect. A domain-boundary contrast can also arise by interference of phase-shifted magneto-optical amplitudes. An explanation of these contrast phenomena is provided in terms of Maxwell-Fresnel theory. Β© 2021 Author(s)
Π Π΅ΠΊΡΡΡΠ΅Π½ΡΠ½ΡΠ΅ Π°Π»Π³ΠΎΡΠΈΡΠΌΡ Π²ΡΡΠΈΡΠ»Π΅Π½ΠΈΡ ΠΊΠΎΡΠ½Ρ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ»ΡΠ½ΠΎΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ Π² ΠΊΠΎΠ»ΡΡΠ΅ Π²ΡΡΠ΅ΡΠΎΠ²
Π£ Π΄Π°Π½ΡΠΉ ΡΠΎΠ±ΠΎΡΡ ΠΎΡΡΠΈΠΌΠ°Π½ΠΎ ΠΊΡΠΈΡΠ΅ΡΡΠΉ ΡΡΠ΅ΠΏΠ΅Π½Π΅Π²ΠΎΡΡΡ Π΅Π»Π΅ΠΌΠ΅Π½ΡΠ° ΡΠΊΡΠ½ΡΠ΅Π½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ ΡΠ° Π½Π°Π²Π΅Π΄Π΅Π½ΠΎ ΠΏΡΠΎΡΡΡ Π°Π»Π³ΠΎΡΠΈΡΠΌΠΈ ΠΎΠ±ΡΠΈΡΠ»Π΅Π½Π½Ρ ΠΊΡΠ±ΡΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΡΠ΅Π½Ρ ΡΠ° ΡΠ΅ΠΊΡΡΠ΅Π½ΡΠ½Ρ Π°Π»Π³ΠΎΡΠΈΡΠΌΠΈ ΠΎΠ±ΡΠΈΡΠ»Π΅Π½Π½Ρ ΠΊΠΎΡΠ΅Π½ΡΠ² Π±ΡΠ»ΡΡ Π²ΠΈΡΠΎΠΊΠΎΠ³ΠΎ ΡΡΠ΅ΠΏΠ΅Π½Ρ Π· Π΅Π»Π΅ΠΌΠ΅Π½ΡΡ ΠΏΠΎΠ»Ρ, ΡΠΊΠΈΠΉ Ρ Π²ΡΠ΄ΠΏΠΎΠ²ΡΠ΄Π½ΠΈΠΌ ΡΡΠ΅ΠΏΠ΅Π½Π΅Π²ΠΈΠΌ Π»ΠΈΡΠΊΠΎΠΌ. ΠΠ»Π³ΠΎΡΠΈΡΠΌΠΈ ΡΠΎΠ·ΠΏΡΠ·Π½Π°Π²Π°Π½Π½Ρ ΡΡΠ΅ΠΏΠ΅Π½Π΅Π²ΠΎΡΡΡ ΡΠ° Π΄ΠΎΠ±ΡΠ²Π°Π½Π½Ρ ΠΊΠΎΡΠ΅Π½Ρ Π·Π° ΡΠΊΠ»Π°Π΄Π΅Π½ΠΈΠΌ ΠΌΠΎΠ΄ΡΠ»Π΅ΠΌ (Π½Π°ΠΏΡΠΈΠΊΠ»Π°Π΄, Π·Π° ΠΌΠΎΠ΄ΡΠ»Π΅ΠΌ n=pq) ΠΏΠΎΠ²Π½ΡΡΡΡ Π²ΠΈΠ·Π½Π°ΡΠ°ΡΡΡΡΡ Π²ΡΠ΄ΠΏΠΎΠ²ΡΠ΄Π½ΠΈΠΌΠΈ Π°Π»Π³ΠΎΡΠΈΡΠΌΠ°ΠΌΠΈ Π·Π° ΠΏΡΠΎΡΡΠΈΠΌ ΠΌΠΎΠ΄ΡΠ»Π΅ΠΌ, Π·Π° ΡΠΌΠΎΠ²ΠΈ, ΡΠΎ Π²ΡΠ΄ΠΎΠΌΠΈΠΉ ΡΠΎΠ·ΠΊΠ»Π°Π΄ ΡΠΈΡΠ»Π° ΠΏ Π½Π° ΠΏΡΠΎΡΡΡ ΠΌΠ½ΠΎΠΆΠ½ΠΈΠΊΠΈ. Π¦ΡΠΊΠ°Π²ΠΎ ΡΠ°ΠΊΠΎΠΆ Π·Π°Π·Π½Π°ΡΠΈΡΠΈ, ΡΠΎ Π·Π°Π΄Π°ΡΠ° ΡΠΎΠ·ΠΊΠ»Π°Π΄Ρ Π½Π° ΠΏΡΠΎΡΡΡ ΠΌΠ½ΠΎΠΆΠ½ΠΈΠΊΠΈ ΡΠ° Π·Π°Π΄Π°ΡΠ° Π΄ΠΎΠ±ΡΠ²Π°Π½Π½Ρ ΠΊΠΎΡΠ΅Π½Ρ Ρ ΠΏΠΎΠ»ΡΠ½ΠΎΠΌΡΠ°Π»ΡΠ½ΠΎ Π΅ΠΊΠ²ΡΠ²Π°Π»Π΅Π½ΡΠ½ΠΈΠΌΠΈ Π²ΡΠ΄Π½ΠΎΡΠ½ΠΎ ΡΠΌΠΎΠ²ΡΡΠ½ΡΡΠ½ΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡΠΈΡΠΌΡ. ΠΠ°Π½Ρ Π°Π»Π³ΠΎΡΠΈΡΠΌΠΈ Ρ, ΠΏΠ΅ΡΡ Π·Π° Π²ΡΠ΅, ΡΡΠΊΠ°Π²ΠΈΠΌΠΈ Π· ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ½ΠΎΡ ΡΠΎΡΠΊΠΈ Π·ΠΎΡΡ, Π° ΡΡ
ΠΏΠΎΠΎΠ΄ΠΈΠ½ΠΎΠΊΠΈΠΉ Π²ΠΈΠΏΠ°Π΄ΠΎΠΊ β Π°Π»Π³ΠΎΡΠΈΡΠΌΠΈ Π΄ΠΎΠ±ΡΠ²Π°Π½Π½Ρ ΠΊΡΠ±ΡΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΡΠ΅Π½Ρ β ΠΌΠΎΠΆΡΡΡ Π±ΡΡΠΈ Π²ΠΈΠΊΠΎΡΠΈΡΡΠ°Π½Ρ ΡΠΊ Π΄ΠΎΠΏΠΎΠΌΡΠΆΠ½Ρ ΠΏΡΠΈ ΠΎΠ±ΡΠΈΡΠ»Π΅Π½Π½Ρ Π±Π°Π·ΠΎΠ²ΠΎΡ ΡΠΎΡΠΊΠΈ ΠΊΡΠΈΠ²ΠΎΡ ΡΠ° ΠΏΡΠΈ "Π²ΠΊΠ»Π°Π΄Π°Π½Π½Ρ" Π²ΡΠ΄ΠΊΡΠΈΡΠΎΠ³ΠΎ ΡΠ΅ΠΊΡΡΡ Ρ ΡΠΎΡΠΊΡ ΠΊΡΠΈΠ²ΠΎΡ, Ρ ΡΠΎΠΌΡ ΡΠΈΡΠ»Ρ Ρ ΡΠΊΡΠΎ ΠΊΡΠΈΠ²Π° Π·Π°Π΄Π°Π½Π° Π½Π°Π΄ ΠΊΡΠ»ΡΡΠ΅ΠΌ Π»ΠΈΡΠΊΡΠ², Π° Π½Π΅ Π½Π°Π΄ ΠΏΠΎΠ»Π΅ΠΌ.In this paper, the criterion of power element of finite field is obtained and simple algorithms for calculating the cubic root and recursive algorithms for calculating the roots of higher powers are constructed. Power recognition algorithm and rooting for composite module (particularly for modulo n=pq) are completely determined by the corresponding algorithms for a simple modules, provided that factorization is known. It is also interesting to note that for n=pq the factorization problem and rooting problem are polynomial equivalent relatively probabilistic algorithm. These algorithms are primarily interesting from a mathematical point of view, and their particular case β the cubic root extraction algorithm β can be used as aids in calculating the base point of the elliptic curve and for "imbedding" of plaintext into curve point, also if curve is defined over the residue rings instead of the field.Π Π΄Π°Π½Π½ΠΎΠΉ ΡΠ°Π±ΠΎΡΠ΅ ΠΏΠΎΠ»ΡΡΠ΅Π½ ΠΊΡΠΈΡΠ΅ΡΠΈΠΉ ΡΡΠ΅ΠΏΠ΅Π½Π½ΠΎΡΡΠΈ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ° ΠΊΠΎΠ½Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ ΠΈ ΠΏΡΠΈΠ²Π΅Π΄Π΅Π½Ρ ΠΏΡΠΎΡΡΡΠ΅ Π°Π»Π³ΠΎΡΠΈΡΠΌΡ Π²ΡΡΠΈΡΠ»Π΅Π½ΠΈΡ ΠΊΡΠ±ΠΈΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΠ½Ρ ΠΈ ΡΠ΅ΠΊΡΡΡΠ΅Π½ΡΠ½ΡΠ΅ Π°Π»Π³ΠΎΡΠΈΡΠΌΡ Π²ΡΡΠΈΡΠ»Π΅Π½ΠΈΡ ΠΊΠΎΡΠ½Π΅ΠΉ Π±ΠΎΠ»Π΅Π΅ Π²ΡΡΠΎΠΊΠΈΡ
ΡΡΠ΅ΠΏΠ΅Π½Π΅ΠΉ ΠΈΠ· ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ° ΠΏΠΎΠ»Ρ, ΠΊΠΎΡΠΎΡΡΠΉ ΡΠ²Π»ΡΠ΅ΡΡΡ ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΠΌ ΡΡΠ΅ΠΏΠ΅Π½Π½ΡΠΌ Π²ΡΡΠ΅ΡΠΎΠΌ. ΠΠ»Π³ΠΎΡΠΈΡΠΌΡ ΡΠ°ΡΠΏΠΎΠ·Π½Π°Π²Π°Π½ΠΈΡ ΡΡΠ΅ΠΏΠ΅Π½Π½ΠΎΡΡΠΈ ΠΈ Π²ΡΡΠΈΡΠ»Π΅Π½ΠΈΡ ΠΊΠΎΡΠ½Ρ ΠΏΠΎ ΡΠΎΡΡΠ°Π²Π½ΠΎΠΌΡ ΠΌΠΎΠ΄ΡΠ»Ρ (Π½Π°ΠΏΡΠΈΠΌΠ΅Ρ, ΠΏΠΎ ΠΌΠΎΠ΄ΡΠ»Ρ n=pq) ΠΏΠΎΠ»Π½ΠΎΡΡΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΡΡΡΡ ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΠΌΠΈ Π°Π»Π³ΠΎΡΠΈΡΠΌΠ°ΠΌΠΈ Π΄Π»Ρ ΠΏΡΠΎΡΡΠΎΠ³ΠΎ ΠΌΠΎΠ΄ΡΠ»Ρ, ΠΏΡΠΈ ΡΡΠ»ΠΎΠ²ΠΈΠΈ, ΡΡΠΎ ΠΈΠ·Π²Π΅ΡΡΠ½ΠΎ ΡΠ°Π·Π»ΠΎΠΆΠ΅Π½ΠΈΠ΅ ΠΌΠΎΠ΄ΡΠ»Ρ Π½Π° ΠΏΡΠΎΡΡΡΠ΅ ΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»ΠΈ. ΠΠ½ΡΠ΅ΡΠ΅ΡΠ½ΠΎ ΡΠ°ΠΊΠΆΠ΅ Π·Π°ΠΌΠ΅ΡΠΈΡΡ, ΡΡΠΎ Π·Π°Π΄Π°ΡΠ° ΡΠ°Π·Π»ΠΎΠΆΠ΅Π½ΠΈΡ Π½Π° ΠΏΡΠΎΡΡΡΠ΅ ΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»ΠΈ ΠΈ Π·Π°Π΄Π°ΡΠ° Π²ΡΡΠΈΡΠ»Π΅Π½ΠΈΡ ΠΊΠΎΡΠ½Ρ ΡΠ²Π»ΡΡΡΡΡ ΠΏΠΎΠ»ΠΈΠ½ΠΎΠΌΠΈΠ°Π»ΡΠ½ΠΎ ΡΠΊΠ²ΠΈΠ²Π°Π»Π΅Π½ΡΠ½ΡΠΌΠΈ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π²Π΅ΡΠΎΡΡΠ½ΠΎΡΡΠ½ΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡΠΈΡΠΌΠ°. ΠΠ°Π½Π½ΡΠ΅ Π°Π»Π³ΠΎΡΠΈΡΠΌΡ ΡΠ²Π»ΡΡΡΡΡ, ΠΏΡΠ΅ΠΆΠ΄Π΅ Π²ΡΠ΅Π³ΠΎ, ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠ½ΡΠΌΠΈ Ρ ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΎΡΠΊΠΈ Π·ΡΠ΅Π½ΠΈΡ, Π° ΠΈΡ
ΡΠ°ΡΡΠ½ΡΠΉ ΡΠ»ΡΡΠ°ΠΉ β Π°Π»Π³ΠΎΡΠΈΡΠΌΡ Π²ΡΡΠΈΡΠ»Π΅Π½ΠΈΡ ΠΊΡΠ±ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΊΠΎΡΠ½Ρ β ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Ρ ΠΊΠ°ΠΊ Π²ΡΠΏΠΎΠΌΠΎΠ³Π°ΡΠ΅Π»ΡΠ½ΡΠ΅ ΠΏΡΠΈ Π²ΡΡΠΈΡΠ»Π΅Π½ΠΈΠΈ Π±Π°Π·ΠΎΠ²ΠΎΠΉ ΡΠΎΡΠΊΠΈ ΠΊΡΠΈΠ²ΠΎΠΉ ΠΈ ΠΏΡΠΈ "Π²Π»ΠΎΠΆΠ΅Π½ΠΈΠΈ" ΠΎΡΠΊΡΡΡΠΎΠ³ΠΎ ΡΠ΅ΠΊΡΡΠ° Π² ΡΠΎΡΠΊΡ ΠΊΡΠΈΠ²ΠΎΠΉ, Π² ΡΠΎΠΌ ΡΠΈΡΠ»Π΅ ΠΈ Π΅ΡΠ»ΠΈ ΠΊΡΠΈΠ²Π°Ρ Π·Π°Π΄Π°Π½Π° Π½Π°Π΄ ΠΊΠΎΠ»ΡΡΠΎΠΌ Π²ΡΡΠ΅ΡΠΎΠ², Π° Π½Π΅ Π½Π°Π΄ ΠΏΠΎΠ»Π΅ΠΌ
Photovoltage spectroscopy of dipolar spin waves in Dy micromagnets
We report on a sensitive spectroscopic technique for probing the spin excitations of individual submicron magnets. This technique uses a high mobility two dimensional electron gas (2DEG) confined in a GaAs/AlGaAs heterojunction to pick up the oscillating dipolar magnetic field emanating from the individual spin wave modes of micromagnets fabricated at its surface. We review a range of dynamic phenomena that demonstrate the formation of magnetostatic waves in finger gate arrays, dipolar edge spin waves in bar magnets, vortex hysteresis in magnetic dots and the photovoltage dependence on microwave polarization.</jats:p
Field-free spin-orbit torque switching enabled by interlayer Dzyaloshinskii-Moriya interaction
Perpendicularly magnetized structures that are switchable using a spin
current under field-free conditions can potentially be applied in spin-orbit
torque magnetic random-access memory(SOT-MRAM).Several structures have been
developed;however,new structures with a simple stack structure and MRAM
compatibility are urgently needed.Herein,a typical structure in a perpendicular
spin-transfer torque MRAM,the Pt/Co multilayer and its synthetic
antiferromagnetic counterpart with perpendicular magnetic anisotropy, was
observed to possess an intrinsic interlayer chiral interaction between
neighboring magnetic layers,namely the interlayer Dzyaloshinskii-Moriya
interaction (DMI) effect. Furthermore, using a current parallel to the
eigenvector of the interlayer DMI, we switched the perpendicular magnetization
of both structures without a magnetic field, owing to the additional
symmetry-breaking introduced by the interlayer DMI. This SOT switching scheme
realized in the Pt/Co multilayer and its synthetic antiferromagnet structure
may open a new avenue toward practical perpendicular SOT-MRAM and other SOT
devices
Fabrication of high-resolution nanostructures of complex geometry by the single-spot nanolithography method
The paper presents a method for the high-resolution production of polymer nanopatterns with controllable geometrical parameters by means of a single-spot electron-beam lithography technique. The essence of the method entails the overexposure of a positive-tone resist, spin-coated onto a substrate where nanoscale spots are exposed to an electron beam with a dose greater than 0.1 pC per dot. A single-spot enables the fabrication of a nanoring, while a chain of spots placed at distance of 5β30 nm from each other allows the production of a polymer pattern of complex geometry of sub-10 nm resolution. We demonstrate that in addition to the naturally oxidized silicon substrates, gold-coated substrates can also successfully be used for the single-spot nanopattering technique. An explanation of the results related to the resist overexposure was demonstrated using Monte Carlo simulations. Our nanofabrication method significantly accelerates (up to 10 times) the fabrication rate as compared to conventional lithography on positive-tone resist. This technique can be potentially employed in the electronics industry for the production of nanoprinted lithography molds, etching masks, nanoelectronics, nanophotonics, NEMS and MEMS devices
Analyzer-free, intensity-based, wide-field magneto-optical microscopy
In conventional Kerr and Faraday microscopy, the sample is illuminated with plane-polarized light, and a magnetic domain contrast is generated by an analyzer making use of the Kerr or Faraday rotation. Here, we demonstrate possibilities of analyzer-free magneto-optical microscopy based on magnetization-dependent intensity modulations of the light. (i) The transverse Kerr effect can be applied for in-plane magnetized material, as demonstrated for an FeSi sheet. (ii) Illuminating that sample with circularly polarized light leads to a domain contrast with a different symmetry from the conventional Kerr contrast. (iii) Circular polarization can also be used for perpendicularly magnetized material, as demonstrated for garnet and ultrathin CoFeB films. (iv) Plane-polarized light at a specific angle can be employed for both in-plane and perpendicular media. (v) Perpendicular light incidence leads to a domain contrast on in-plane materials that is quadratic in the magnetization and to a domain boundary contrast. (vi) Domain contrast can even be obtained without a polarizer. In cases (ii) and (iii), the contrast is generated by magnetic circular dichroism (i.e., differential absorption of left- and right-circularly polarized light induced by magnetization components along the direction of light propagation), while magnetic linear dichroism (differential absorption of linearly polarized light induced by magnetization components transverse to propagation) is responsible for the contrast in case (v). The domain-boundary contrast is due to the magneto-optical gradient effect. A domain-boundary contrast can also arise by interference of phase-shifted magneto-optical amplitudes. An explanation of these contrast phenomena is provided in terms of Maxwell-Fresnel theory
Manipulation of magnetic vortex parameters in disk-on-disk nanostructures with various geometry
Magnetic nanostructures in the form of a sandwich consisting of two permalloy (Py) disks with diameters of 600 and 200 nm separated by a nonmagnetic interlayer are studied. Magnetization reversal of the disk-on-disk nanostructures depends on the distance between centers of the small and big disks and on orientation of an external magnetic field applied during measurements. It is found that manipulation of the magnetic vortex chirality and the trajectory of the vortex core in the big disk is only possible in asymmetric nanostructures. Experimentally studied peculiarities of a motion path of the vortex core and vortex parameters by the magneto-optical Kerr effect (MOKE) magnetometer are supported by the magnetic force microscopy imaging and micromagnetic simulations