CN109166599A - A kind of complete optomagnetic inverting method of rotation direction dependence based on single order rotation direction polarization vortex light - Google Patents

A kind of complete optomagnetic inverting method of rotation direction dependence based on single order rotation direction polarization vortex light Download PDF

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Publication number
CN109166599A
CN109166599A CN201811154711.9A CN201811154711A CN109166599A CN 109166599 A CN109166599 A CN 109166599A CN 201811154711 A CN201811154711 A CN 201811154711A CN 109166599 A CN109166599 A CN 109166599A
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rotation direction
optomagnetic
complete
single order
light
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王思聪
魏琛
李向平
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Jinan University
University of Jinan
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Jinan University
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    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11CSTATIC STORES
    • G11C13/00Digital stores characterised by the use of storage elements not covered by groups G11C11/00, G11C23/00, or G11C25/00
    • G11C13/04Digital stores characterised by the use of storage elements not covered by groups G11C11/00, G11C23/00, or G11C25/00 using optical elements ; using other beam accessed elements, e.g. electron or ion beam
    • G11C13/06Digital stores characterised by the use of storage elements not covered by groups G11C11/00, G11C23/00, or G11C25/00 using optical elements ; using other beam accessed elements, e.g. electron or ion beam using magneto-optical elements

Abstract

The invention discloses a kind of rotation directions based on single order rotation direction polarization vortex light to rely on complete optomagnetic inverting method, since polarization singular point and phase singularity are focusing the interaction in space, the single order rotation direction that topological charge is+1 and -1 polarizes vortex light will generate Left-hand circular polarization field and right-hand circular polarization field respectively in focusing space, under the conditions of high-NA, single order rotation direction polarizes vortex light and generates the circular polarization focousing field that lateral dimension is less than traditional circularly polarized light focal beam spot lateral dimension.The rotation direction realized using the method for the present invention relies on complete optomagnetic inversion region area will be smaller by 30% than inversion region area caused by traditional circularly polarized light, provide effective solution for ultra high density, ultrafast magnetic storage.

Description

A kind of complete optomagnetic inverting method of rotation direction dependence based on single order rotation direction polarization vortex light
Technical field
The invention belongs to optomagnetic technical field of memory, and in particular to a kind of rotation direction based on single order rotation direction polarization vortex beam Rely on complete optomagnetic inverting method technology.
Background technique
Magnetic storage plays highly important role in field of data storage.For example, the hard disk being widely used now (Hard Disk Drive, HDD) just carries out mass memory and quickly processing to huge information data using magnetic storage technology. With the progress of science, magnetic storage technology is constantly developed and reformed to people.Over the last couple of decades, with logical bits " 0 " " 1 " is widely used in high density magnetic storage as the perpendicular recording digital storage technique of storage unit.In this technology In, people hang down to magnetic material magnetization unit to realize using applying vertical magnetic field (i.e. magnetic direction is perpendicular to magnetic material surface) Straight reversion control.In order to steadily keep records of information for more time, big coercitive magnetic material is often used as storage Medium.For this purpose, additional high-intensity magnetic field becomes the necessary condition to realize high-density perpendicular magnetic recording.However, current commercial product Magnetic head can only generate less than the limited magnetic field of 2.4T, bring huge difficulty to high-density perpendicular magnetic recording.To solve this One problem, there has been proposed heat-assisted magnetic recording method (the Heat assisted magnetic for combining laser pulse radiation recording,HAMR).Laser pulse can fast lifting magnetic material temperature, be reduced rapidly the coercivity of magnetic material, and then subtract Small required externally-applied magnetic field.Nevertheless, the electron spin of magnetic material is come in the form of precession under the action of external magnetic field Reversion process is completed, the characteristic time is several nanoseconds, this just greatly limits the rate of magnetic inversion.As it can be seen that how to realize super Fast magnetic inversion becomes the important issue of magnetic fields.
2007, complete optomagnetic reversion (All-optical magnetic switching, AOS) was put forward for the first time by people (C.D.Stanciu,et al.,Phys.Rev.Lett.99,047601(2007)).Studies have shown that without any externally-applied magnetic field Under conditions of, merely with the circularly polarized laser pulse that pulsewidth is 40fs as excitaton source, ferrimagnetic material GdFeCo can be realized The complete optomagnetic reversion (All-optical helicity-dependent switching, AO-HDS) that rotation direction relies on.Due to this One magnetic inversion process is to realize (I.Radu, et al., Nature by the strong exchange-coupling interaction of Gd and Fe subgrain compartment 472,205 (2011)), reversing time can foreshorten within 100ps (K.Vahaplar, et al., Phys.Rev.Lett.103,117201(2009)).This provides effective way for ultrafast magnetic recording.However, current people are only Using circularly polarized incident light in ferrimagnetic material (GdFeCo, TbCo, TbFe etc.) or ferromagnetic material under the conditions of low numerical aperture Full magneto-optical recorder is carried out on (Co/Pt multilayer material, FePtAgC membrana granulosa etc.), spatially transverse reversion size rests on micron Scale is unfavorable for high density data storage.Therefore, the small spatial scale focal beam spot with circular polarization state how is obtained to superelevation Density, ultrafast magnetic storage are most important.
The polarization state that single order rotation direction polarizes vortex light is rotation direction polarization state (Azimuthal polarization), phase With topological charge be ± 1, i.e. 0~2 π, Spiral distribution.Under the conditions of high NA focus, such light beam focal beam spot is horizontal It is much smaller than traditional circularly polarized light focal beam spot to size, and there is purely lateral circular polarization state.
Summary of the invention
The purpose of the present invention is to overcome the shortcomings of the existing technology and deficiency, provides a kind of polarize using single order rotation direction and is vortexed Light realizes that rotation direction relies on the completely new technical solution of complete optomagnetic reversion.
To achieve the purpose of the present invention, used scheme are as follows: it is a kind of based on single order rotation direction polarization vortex light rotation direction according to The optomagnetic inverting method of Lai Quan is the incident light of rotation direction polarization state including polarization state, and it is ± 1 spiral shell that the incident light, which has topological charge, Revolve phase distribution;
The incident light that topological charge is+1 or -1 is radiated in magnetic storage media, makes magnetic storage media that rotation direction occur and relies on entirely Optomagnetic reversion;
The magnetic storage media is the ferrimagnetic material or ferromagnetic material that can be realized rotation direction and rely on complete optomagnetic reversion.
Preferably, the incident light generates by the following method, using pulse laser by rotation direction polarization conversion device with The helical phase modulator that topological charge is ± 1 polarizes incident light, produced by phase-modulation.
More preferably, rotation direction polarization conversion device be using birefringent or dichroism to incident linear polarization or circularly polarized light into Row polarization state modulates and generates rotation direction polarised light.Common rotation direction polarization conversion device includes liquid crystal polarized converter, half-wave plate Combination, sub-wave length grating etc..In addition, can also generate rotation direction polarization by laser cavity external interference or the selection of laser intracavity modal Light.Common helical phase modulator includes spiral phase plate, spatial light modulator etc..
Preferably, ferrimagnetic material GdFeCo, TbFeCo, TbFe, TbCo, DyCo or HoFeCo, or, ferromagnetic material is Co/Pt multilayer material or FePtAgC membrana granulosa.
Preferably, the incident light is focused in the magnetic storage media using condenser lens, focal beam spot has pure Lateral circular polarization state.
Preferably, when the magnetic storage media is GdFeCo, the mean energy density of the incident light is not less than 4.83mJ/cm2
Preferably, by incident light by single laser pulse excitation in a manner of be radiated in magnetic storage media, or, by incident light with The mode of more laser pulse scanning excitations is radiated in magnetic storage media.
Preferably, the magnetic storage media can also be rare earth-transition metal multi-layer film structure or heterojunction structure.
Preferably, the magnetic storage media is obtained by Grown by Magnetron Sputtering mode.
Preferably, the incident light is focused in the magnetic storage media using condenser lens, and, the number of condenser lens Value aperture is NA=0.95, annular factor-beta=0.95 of incident light.
Preferably, focal beam spot polarizes field component that annular is not longitudinal, and remains solid purely lateral polarization field The lateral dimension of focal beam spot is reduced under the premise of keeping lateral circular polarization state, and then can obtain there is smaller lateral dimension Complete optomagnetic inversion region.
The present invention realizes that small spatial scale rotation direction relies on the principle of complete optomagnetic reversion using single order rotation direction polarization vortex beam It is as follows:
The center of single order rotation direction polarization vortex beam has polarization singular point and phase singularity, in focusing, due to inclined The interaction of vibration singular point and phase singularity can generate solid focal beam spot in focusing space, and the polarization state of focal spot is pure Lateral circular polarization or elliptical polarization.When the numerical aperture of condenser lens is larger, traditional circularly polarized light focal beam spot can be generated The extremely strong longitudinal polarization field of annular, and single order rotation direction polarization vortex beam focal beam spot remains purely lateral polarization field, into And the lateral dimension of focal beam spot is reduced under the premise of keeping circular polarization state.Circular polarization focal beam spot exposes to complete optomagnetic anti- Turn after material (by taking ferrimagnetic material GdFeCo as an example), material is brought rapidly up to more than Curie temperature, Gd sublattice and Fe subgrain Lattice can generate extremely strong exchange interaction, cause the rapid reversion of sublattice.Entire spin-flip process (including reversion Relaxation process) occur within 100ps.Since the complete optomagnetic reversion material has apparent magnetocircular dichroism, to not It is different with rotation direction circularly polarized light absorption efficiency, and then produce the energy window that rotation direction relies on complete optomagnetic reversion.It is i.e. final to realize Ultrafast, small spatial scale rotation direction relies on complete optomagnetic reversion.
The present invention has the following advantages and effects with respect to the prior art:
(1) when the numerical aperture of condenser lens is larger, it is vertical that traditional circularly polarized light focal beam spot can generate extremely strong annular To polarization field, and single order rotation direction polarization vortex light focal beam spot remains solid purely lateral polarization field, can keep horizontal To the lateral dimension for reducing focal beam spot under the premise of circular polarization state.Experiment shows that the rotation direction realized using the method is relied on Complete optomagnetic inversion region area will be smaller by 30% than inversion region area caused by traditional circularly polarized light.
(2) under the conditions of high-NA, longitudinal direction polarization field produced by traditional circularly polarized light focal beam spot reduces focal spot The polarization purity of lateral circular polarization field greatly affected the energy window that rotation direction relies on complete optomagnetic reversion.And single order rotation direction is inclined The purely lateral circular polarization focal beam spot of vibration vortex light can get optimal energy window.
Detailed description of the invention
Fig. 1 is the polarization state for the single order rotation direction polarization vortex beam that topological charge is ± 1 and phase distribution and its corresponding focuses The schematic diagram of normalization field strength and the polarization state distribution of field;
Fig. 2 is that traditional circularly polarized light (CP beam) focal beam spot and single order rotation direction polarize vortex light (FAPV beam) and focus The surface chart that hot spot transverse direction full width at half maximum (FWHM) changes with the annular factor (β) of NA and incident ring light;
Fig. 3 is the variation in Fig. 2 with NA and β, and compared with traditional circularly polarized light, single order rotation direction polarizes vortex light and focuses light The diminution percentage schematic diagram of spot lateral dimension;
Fig. 4 is to polarize vortex light using single order rotation direction to realize that rotation direction relies on complete optomagnetic reversion on ferrimagnetic material GdFeCo Schematic diagram;
Fig. 5 is the initial magnetization field distribution schematic diagram of GdFeCo material in the embodiment of the present invention;
Fig. 6 is to polarize GdFeCo material under vortex light excites in the single order rotation direction that topological charge is+1 in the embodiment of the present invention Reversion schematic diagram;
Fig. 7 is to polarize GdFeCo material under vortex light excites in the single order rotation direction that topological charge is -1 in the embodiment of the present invention Reversion schematic diagram;
Fig. 8 be the embodiment of the present invention in laser mean energy density to GdFeCo material entirely optomagnetic reversion influence variation show It is intended to.
Specific embodiment
Specific embodiments of the present invention will be further explained with reference to the accompanying drawing:
Fig. 1 show the polarization state and phase distribution and its corresponding for the single order rotation direction polarization vortex beam that topological charge is ± 1 The numerical simulation result of normalization field strength and the polarization state distribution of focal plane focousing field.The a length of 400nm of incident light wave, condenser lens Numerical aperture (NA) is 0.005.Topological charge be+1 and -1 incident light focousing field polarization state be respectively Left-hand circular polarization state and Right-hand circular polarization state passes through the rotation direction of the positive and negative i.e. controllable focal beam spot circular polarization state of control incident light topological charge.
Fig. 2 show traditional circularly polarized light (CP beam) focal beam spot and single order rotation direction polarization vortex light (FAPV beam) The surface chart that focal beam spot transverse direction full width at half maximum (FWHM) changes with NA and β.Wherein, in order to reduce the transverse direction of focal spot as much as possible Size, the NA in addition to increasing condenser lens usually also introduce ring-incidence light beam, and the ratio of internal diameter and outer diameter is β.
Fig. 3 show the variation with NA and β, and compared with traditional circularly polarized light, single order rotation direction polarizes vortex light and focuses light The diminution percentage of spot lateral dimension.From in figure it can be found that under optimal condition, i.e. when NA=0.95, β=0.95, two The lateral dimension of kind light beam focal beam spot is respectively 228nm and 160nm, i.e. focal spot lateral dimension reduces 30%.
Fig. 4 is shown in the present embodiment, and rotation is realized on ferrimagnetic material GdFeCo using single order rotation direction polarization vortex light To the schematic diagram for relying on complete optomagnetic reversion.In the present embodiment, incident pulse optical maser wavelength is 400nm, pulsewidth 40fs.Utilize arteries and veins Rush the repetitive rate that selector accurately controls pulse laser.Use in conjunction polarization conversion device and phase-modulator, can will be incident Linearly polarized light is converted to single order rotation direction polarization vortex light.Ferrimagnetic material GdFeCo alloy is as obtained by the method for magnetron sputtering It arrives, for example, one of specific component can choose Gd27Fe63.87Co9.13, specific film layer structure is Glass/AlTi (10nm)/SiN(5nm)/GdFeCo(20nm)/SiN(60nm).Detection light is wavelength 800nm, pulsewidth 40fs, repetitive rate 1kHz Linear polarization pulse laser.According to Faraday effect, the magnetizing field of different orientation can generate identical Polarization Detection light different Rotation effect.Under the action of analyzer, the magnetization field areas of different orientation can be presented on charge-coupled device (CCD) contrasts Spend different pictures.The present embodiment is to carry out at room temperature in air.
Further:
Vortex light focusing light field, which is polarized, for verifying single order rotation direction realizes that rotation direction relies on complete optomagnetic reversion in GdFeCo material Feasibility, we choose condenser lens NA=0.005, and corresponding focal beam spot lateral dimension is about 42 μm.Exciting light is averaged Energy density is 5.08mJ/cm2 (mean energy density is equal to single pulse energy divided by the horizontal area of focal beam spot).
Fig. 5 show the initial magnetization field of GdFeCo material, and black region (left side) indicates that magnetizing field initial orientation is downward, White area (right side) indicates that magnetizing field initial orientation is upward.
Fig. 6 show the reversion result of the GdFeCo material in the case where the single order rotation direction that topological charge is+1 polarizes the excitation of vortex light. Wherein, the dotted inversion region of black that right area generates is to be excited to generate by single laser pulse, and black ribbon inversion region is It is generated by the multiple-pulse scanning excitation that repetitive rate is 100Hz, laser scanning speed is about 29.8 μm/s.It can be found that when excitation When the topological charge of light is+1, complete optomagnetic reversion is had occurred in white area, and black region keeps original state.
Fig. 7 show the reversion result of the GdFeCo material in the case where the single order rotation direction that topological charge is -1 polarizes the excitation of vortex light. It can be found that complete optomagnetic reversion has occurred in black region, and white area keeps initial when the topological charge of exciting light is -1 State.The above results, which clearly demonstrate single order rotation direction polarization vortex light focusing light field, can be realized rotation direction in GdFeCo material Rely on the effect of complete optomagnetic reversion.
Fig. 8 show influence of the laser mean energy density to the optomagnetic reversion entirely of GdFeCo material.Incident light is topological charge Vortex light is polarized for+1 single order rotation direction.As can be seen that complete optomagnetic inversion region lateral dimension is with laser mean energy density Reduction and reduce.When laser mean energy density is decreased to 4.83mJ/cm2When, complete optomagnetic inversion region diameter is about 1.1 μ m.When laser mean energy density is less than 4.83mJ/cm2When, complete optomagnetic reversal development will not occur for GdFeCo material.This is Since GdFeCo has soft magnetic characteristic, the smallest domain size is about 1-3 μm.Therefore, even if increasing the numerical value of condenser lens Aperture reduces the lateral dimension of focal beam spot, and single order rotation direction polarization vortex light can not be also verified in GdFeCo material to be produced The complete optomagnetic inversion region of raw smaller lateral dimension.
Nevertheless, complete optomagnetic inverting method proposed by the invention but can be applied to other ferrimagnetic materials (such as TbFe, TbCo, TbFeCo) or ferromagnetic material (Co/Pt multilayer material, FePtAgC membrana granulosa etc.).These complete optomagnetic reversion materials There are lesser domain size (about tens nanometers), under the irradiation of single order rotation direction polarization vortex light, these materials be can be realized Rotation direction relies on complete optomagnetic reversion.Therefore, compared to traditional circularly polarized light, single order rotation direction polarization vortex light in these materials can The rotation direction for generating smaller lateral dimension relies on complete optomagnetic inversion region, and then realizes ultrafast, the full magneto-optical recorder of ultra high density.
Above-described embodiment is one of embodiments of the present invention, but embodiments of the present invention are not by above-described embodiment Limitation, such as the production method of single order rotation direction polarization vortex beam, complete optomagnetic reversion material component or film layer structure in the present invention Change.Other any changes, modifications, substitutions, combinations, simplifications made without departing from the spirit and principles of the present invention, It should be equivalent substitute mode, be included within the scope of the present invention.

Claims (9)

1. a kind of rotation direction based on single order rotation direction polarization vortex light relies on complete optomagnetic inverting method, it is characterised in that: including polarization State is the incident light of rotation direction polarization state, and there is the incident light helical phase that topological charge is ± 1 to be distributed;
The incident light that topological charge is+1 or -1 is radiated in magnetic storage media, makes magnetic storage media that rotation direction dependence occur complete optomagnetic Reversion;
The magnetic storage media is the ferrimagnetic material or ferromagnetic material that can be realized rotation direction and rely on complete optomagnetic reversion.
2. the rotation direction according to claim 1 based on single order rotation direction polarization vortex light relies on complete optomagnetic inverting method, special Sign is: the incident light generates by the following method,
Incident light is carried out by the helical phase modulator that rotation direction polarization conversion device and topological charge are ± 1 using pulse laser Produced by polarization, phase-modulation.
3. the rotation direction according to claim 1 based on single order rotation direction polarization vortex light relies on complete optomagnetic inverting method, special Sign is: ferrimagnetic material GdFeCo, TbFeCo, TbFe, TbCo, DyCo or HoFeCo, or,
Ferromagnetic material is Co/Pt multilayer material or FePtAgC membrana granulosa.
4. the rotation direction according to claim 1 based on single order rotation direction polarization vortex light relies on complete optomagnetic inverting method, special Sign is: being focused on the incident light in the magnetic storage media using condenser lens, focal beam spot has purely lateral circle inclined Polarization state.
5. the rotation direction according to claim 4 based on single order rotation direction polarization vortex light relies on complete optomagnetic inverting method, special Sign is: when the magnetic storage media is GdFeCo, the mean energy density of the incident light is not less than 4.83mJ/cm2
6. the rotation direction according to claim 1 based on single order rotation direction polarization vortex light relies on complete optomagnetic inverting method, special Sign is: incident light is radiated in magnetic storage media in a manner of the excitation of single laser pulse, or,
Incident light is radiated in magnetic storage media in a manner of the scanning excitation of more laser pulses.
7. the rotation direction according to claim 1 based on single order rotation direction polarization vortex light relies on complete optomagnetic inverting method, special Sign is: the magnetic storage media can also be rare earth-transition metal multi-layer film structure or heterojunction structure.
8. the rotation direction according to claim 1 based on single order rotation direction polarization vortex light relies on complete optomagnetic inverting method, special Sign is: the magnetic storage media is obtained by Grown by Magnetron Sputtering mode.
9. the rotation direction according to claim 1 based on single order rotation direction polarization vortex light relies on complete optomagnetic inverting method, special Sign is: the incident light focused in the magnetic storage media using condenser lens, and, the numerical aperture of condenser lens is NA=0.95, annular factor-beta=0.95 of incident light.
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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111257407A (en) * 2020-03-08 2020-06-09 北京工业大学 First-order reversal magnetization response matrix characterization method for ferromagnetic material performance
CN112562744A (en) * 2020-07-03 2021-03-26 暨南大学 Double-pulse excitation method for ultrafast and super-resolution full photomagnetic recording

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20160077167A1 (en) * 2014-02-19 2016-03-17 Infinitum Solutions, Inc. Integrated optical nanoscale probe
CN105811953A (en) * 2016-04-21 2016-07-27 山东师范大学 Application of plumbum iodide (PbI2) film in sub-picosecond all-optical magnetic switch

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20160077167A1 (en) * 2014-02-19 2016-03-17 Infinitum Solutions, Inc. Integrated optical nanoscale probe
CN105811953A (en) * 2016-04-21 2016-07-27 山东师范大学 Application of plumbum iodide (PbI2) film in sub-picosecond all-optical magnetic switch

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
C. D. STANCIU等: "All-Optical Magnetic Recording with Circularly Polarized Light", 《PHYSICAL REVIEW LETTERS》 *
SICONG WANG等: "Ultralong pure longitudinal magnetization needle induced by annular vortex binary optics", 《OPTICS LETTERS》 *
XIANGPING LI等: "Super-resolved pure-transverse focal fields with an enhanced energy density through focus of an azimuthally polarized first-order vortex beam", 《OPTICS LETTERS》 *

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111257407A (en) * 2020-03-08 2020-06-09 北京工业大学 First-order reversal magnetization response matrix characterization method for ferromagnetic material performance
CN111257407B (en) * 2020-03-08 2023-04-14 北京工业大学 Method for representing first-order reversal magnetization response matrix of ferromagnetic material performance
CN112562744A (en) * 2020-07-03 2021-03-26 暨南大学 Double-pulse excitation method for ultrafast and super-resolution full photomagnetic recording
CN112562744B (en) * 2020-07-03 2021-09-03 暨南大学 Double-pulse excitation method for ultrafast and super-resolution full photomagnetic recording
WO2022000937A1 (en) * 2020-07-03 2022-01-06 暨南大学 Dual-pulse excitation method for ultrafast and super-resolution all-optical magnetic recording

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Application publication date: 20190108