WO1999050833A1 - Procede et appareil d'enregistrement magnetique - Google Patents
Procede et appareil d'enregistrement magnetique Download PDFInfo
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- WO1999050833A1 WO1999050833A1 PCT/JP1999/000546 JP9900546W WO9950833A1 WO 1999050833 A1 WO1999050833 A1 WO 1999050833A1 JP 9900546 W JP9900546 W JP 9900546W WO 9950833 A1 WO9950833 A1 WO 9950833A1
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- Prior art keywords
- magnetic
- thin film
- signal
- recording
- magnetic recording
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Classifications
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y10/00—Nanotechnology for information processing, storage or transmission, e.g. quantum computing or single electron logic
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- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
- G11B11/10502—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing characterised by the transducing operation to be executed
- G11B11/10504—Recording
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- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
- G11B11/10502—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing characterised by the transducing operation to be executed
- G11B11/10528—Shaping of magnetic domains, e.g. form, dimensions
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- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
- G11B11/10582—Record carriers characterised by the selection of the material or by the structure or form
- G11B11/10584—Record carriers characterised by the selection of the material or by the structure or form characterised by the form, e.g. comprising mechanical protection elements
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- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/02—Recording, reproducing, or erasing methods; Read, write or erase circuits therefor
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- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/127—Structure or manufacture of heads, e.g. inductive
- G11B5/1278—Structure or manufacture of heads, e.g. inductive specially adapted for magnetisations perpendicular to the surface of the record carrier
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- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/74—Record carriers characterised by the form, e.g. sheet shaped to wrap around a drum
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- G11B5/84—Processes or apparatus specially adapted for manufacturing record carriers
- G11B5/855—Coating only part of a support with a magnetic layer
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- G—PHYSICS
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- G11C—STATIC STORES
- G11C11/00—Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor
- G11C11/02—Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using magnetic elements
- G11C11/14—Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using magnetic elements using thin-film elements
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11C—STATIC STORES
- G11C11/00—Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor
- G11C11/02—Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using magnetic elements
- G11C11/16—Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using magnetic elements using elements in which the storage effect is based on magnetic spin effect
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- G—PHYSICS
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- G11C11/00—Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor
- G11C11/02—Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using magnetic elements
- G11C11/16—Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using magnetic elements using elements in which the storage effect is based on magnetic spin effect
- G11C11/165—Auxiliary circuits
- G11C11/1675—Writing or programming circuits or methods
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- G11C19/02—Digital stores in which the information is moved stepwise, e.g. shift registers using magnetic elements
- G11C19/08—Digital stores in which the information is moved stepwise, e.g. shift registers using magnetic elements using thin films in plane structure
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
- G11B11/10502—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing characterised by the transducing operation to be executed
- G11B11/10517—Overwriting or erasing
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- G—PHYSICS
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- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B9/00—Recording or reproducing using a method not covered by one of the main groups G11B3/00 - G11B7/00; Record carriers therefor
- G11B9/12—Recording or reproducing using a method not covered by one of the main groups G11B3/00 - G11B7/00; Record carriers therefor using near-field interactions; Record carriers therefor
- G11B9/14—Recording or reproducing using a method not covered by one of the main groups G11B3/00 - G11B7/00; Record carriers therefor using near-field interactions; Record carriers therefor using microscopic probe means, i.e. recording or reproducing by means directly associated with the tip of a microscopic electrical probe as used in Scanning Tunneling Microscopy [STM] or Atomic Force Microscopy [AFM] for inducing physical or electrical perturbations in a recording medium; Record carriers or media specially adapted for such transducing of information
- G11B9/1409—Heads
Definitions
- the present invention relates to a high-density magnetic recording method and a magnetic recording device thereof.
- a device for recording and reproducing a signal on a magnetic recording medium using a magnetic head For example, there is a magnetic disk drive.
- a magneto-optical recording device that records a signal with a magnetic head while irradiating a laser beam, and reproduces a recorded signal by a Kerr rotation of the laser beam.
- An optical disc device that records and reproduces a signal by detecting a change in the state of the recording medium by the laser beam and detecting the change in the state corresponds to the change.
- This type of recording method and apparatus has a recording density of 1 GbZcm 2 and will be about 10 Gb / cm 2 in the future. However, if you need a large amount of information, recording density in the 1 G b Bruno cm 2 ⁇ 1 0 G bcm 2 described above, hardly recording density is insufficient, can not you to record large amounts of information, Not satisfactory.
- the present invention theoretically elucidated the conditions for forming spin vortices in a magnetic thin film and the structure thereof, and clarified the relationship between the magnetic properties of the thin film for the first time. Based on the results, that is, for the first time, the conditions for writing, reading, or rewriting signals when using spin vortices as a recording unit were clarified. In particular, despite the extremely small recording unit of about 10 nm, for the first time, it was shown that spin vortices are magnetically or thermally stable and can be used for magnetic recording.
- the present invention proposes a novel magnetic recording method using a spin vortex as a recording unit and a magnetic recording apparatus therefor. Further, the conditions of a magnetic thin film as a magnetic recording medium peculiar to spin vortex recording, and a magnetic head It is about conditions.
- an object of the present invention is to provide a magnetic recording method and a magnetic recording apparatus capable of performing high-density recording by using a spin vortex as a recording unit. Disclosure of the invention
- a recording signal is recorded by forming a spin vortex consisting of magnetization surrounding the center perpendicular magnetization in a ring by a signal magnetic field in a small area of the magnetic thin film, and the recording signal is recorded, and the magnetization of the spin vortex is detected and recorded. The signal is reproduced.
- any one of the recording, rewriting, and reproduction of a signal or a combination thereof is performed using a cylindrical magnetic needle.
- the perpendicular magnetization at the center is generated by a signal magnetic field in a minute area.
- the magnetic thin film is an ultrathin film whose thickness is about the thickness of the domain wall or smaller than the thickness of the domain wall.
- the magnetic thin film is a magnetic thin film having small in-plane magnetic anisotropy.
- the magnetic thin film has an easy magnetization axis perpendicular to a plane.
- the magnetic thin film is an array of disk-shaped thin films.
- the magnetic thin film is formed on a lattice of soft magnetic thin wires.
- the magnetic thin film is a thin film formed on an array of disks of a high magnetic flux density material smaller than the diameter of a spin vortex.
- the magnetic thin film is formed on an array of magnets or antiferromagnetic disks smaller than the diameter of the spin vortex, whereby the magnetic thin film is locally perpendicular to the position of the disks. It is a thin film having anisotropy.
- the magnetic recording method and the magnetic recording apparatus of the present invention basically use a magnetic recording method of force and spin vortices for magnetic recording to construct a new recording unit in principle. It is possible to realize a high-density recording 100 times as large as that of the above method.
- FIG. 1 is a diagram showing the magnetic structure of positive and negative spin vortices recorded on a recording medium (magnetic ultrathin film) according to the present invention.
- FIG. 2 is a conceptual diagram of magnetic recording using a spin vortex as a recording unit according to the present invention.
- FIG. 3 is a schematic diagram showing a configuration example of a recording medium for spin vortex recording according to the present invention.
- FIG. 4 is a schematic diagram showing an example of a magnetic recording operation using a spin vortex according to the present invention.
- the present invention utilizes a magnetic structure formed in a minute region of a magnetic thin film as a recording unit.
- the minute magnetic structure has a structure in which the magnetization is perpendicular to the thin film surface at the center and the magnetization surrounds the ring in a circle.
- the size of this magnetic structure depends on the thin-film magnetic material, but its radius from the center is about 10 nm.
- a micromagnetic structure used as a recording unit of the present invention is called a spin vortex.
- the magnetic thin film be magnetically isotropic in the film plane and have uniaxial magnetic anisotropy perpendicular to the plane, and the anisotropy constant be K.
- K shall have a negative value if the vertical direction is the easy axis.
- the stiffness constant of the exchange interaction of a magnetic thin film is A
- the spin vortex according to the present invention is a structure in which the magnetic structure does not basically change in the thickness direction of the magnetic thin film, and the case where the thickness of the magnetic thin film is t schemeor less.
- the radius of the spin vortex is D1 ⁇ 22.5 (A / (K + 2 TTMS 2 )) 1/2 Since D is negative, K Also, the saturation magnetization decreases as the M S force increases, and decreases as the magnetic material of A, that is, the lower the Curie temperature, decreases (if K has a positive easy surface, the smaller the anisotropy constant, the smaller).
- the magnetic material that is, the value of D of the ultra-thin film having the (100) plane of Fe, the (001) plane of Co, and the (111) plane of Ni is Indicated.
- the radius of the above-mentioned spin vortex is 5 [2 A / (M s H s )] 1/2 , so the smaller the spin vortex, the larger the switching field.
- a magnetic field is applied ultra thin film of more than H s of demagnetized state, to form a spin vortex in the direction of applied magnetic field.
- the spread of H s is about 2D.
- Table 1 shows the characteristics of a single spin vortex as a magnetic recording unit for typical ultrathin magnetic materials.
- the magnetic recording by the spin vortex according to the present invention has a magnetic structure in which the spin vortex is inherently stable, when used for high-density recording, the recording unit is as small as about 10 nm when compared with the conventional magnetic recording technology. Nevertheless, it is extremely stable. This is because, when the recording unit is about 100 nm in the conventional magnetic recording technology, instability such as attenuation or extinction of the magnetization of the recording unit due to a leakage magnetic field or thermal disturbance is a major problem. Is one of the important features.
- This stability of the spin vortex is a force that requires a large magnetic field for recording and rewriting.
- the magnetic field required for recording and rewriting can be reduced by locally heating the magnetic thin film.
- the magnetic field of the thin film is reduced by heating, and the reversal magnetic field is reduced, so that recording or rewriting can be performed with a small magnetic field.
- the recorded signal can be erased by performing thermal demagnetization.
- Laser light can be used for local heating.
- the magnetic material for a thin film suitable for the present invention is essentially a soft magnetic material, whereas a conventional magnetic recording medium is a hard magnetic material.
- a material having zero magnetic anisotropy a Ni-Fe alloy having a crystal magnetic anisotropy ⁇ magnetostriction constant of zero is known as a so-called permalloy alloy.
- the magnetic thin film according to the present invention is used in the form of an ultrathin film having a thickness of 20 nm or less, a normal soft magnetic material may be used.
- an ultra-thin film of Fe, Ni or CQ with a thickness of 10 nm is grown on an appropriate underlayer, and the thin film described in Table 1 is formed.
- the thin film has magnetic anisotropy perpendicular to the plane and is isotropic in the plane. Since a K ⁇ 0, H s is 4 vr M s less than (Table 1).
- an amorphous material such as glass or plastic or a crystal material plate such as A1 or Si is used depending on the purpose.
- the magnetic thin film according to the present invention When the magnetic thin film according to the present invention is used as a magnetic recording medium for recording with a spin vortex, it is desirable that a spin vortex is easily formed at a predetermined position of the thin film.
- One method for this is to construct a magnetic recording medium with an array of thin-film disks having a diameter equal to or smaller than the diameter of the spin vortex, and to record a signal by forming a spin vortex on each thin-film disk in response to a signal. Since the spin vortex formed in the disk has a unique magnetization determined by the diameter of the disk, if the diameter of the disk is changed as necessary, the magnitude of the magnetization of the positive and negative spin vortices can be changed, resulting in a multilevel signal. Magnetic recording can be performed, and it becomes a more advanced information processing recording medium.
- Another method is to add a high magnetic flux density magnetic material or a magnet or antiferromagnetic disk with a diameter smaller than the spin vortex at a predetermined position on the thin film.
- the magnitude of M s and K of the thin film is locally large, so the H s of the thin film is small and the spin vortex is stable at this position.
- Another method is to make a lattice with two sets of straight lines that intersect each other with a width of soft magnetic material narrower than the size of the spin vortex, and then form a magnetic thin film on top of it. Because be further ⁇ thickness of the soft magnetic wire at the intersection of two straight lines, H s is more small Kunar.
- the intersection of the two straight lines is the most stable position of the spin vortex.
- a stable position of the spin vortex and a path for the spin vortex to move can be created in the magnetic thin film, so that not only magnetic recording and storage, but also a device with more various signal processing functions can be made. Since the spin vortex according to the present invention actually moves when a magnetic field having a gradient is applied, a logic operation element utilizing the spin vortex can be configured.
- a columnar magnetic needle for the so-called write head used for writing and rewriting the spin vortex of the present invention. This is because a circularly symmetric magnetic field is generated around the tip of the cylindrical magnetic needle. The strength of the highest magnetic field is needed is a H s.
- head field may be a weaker magnetic field than H s. If a magnetic needle is made of a magnet material and the distance to the magnetic thin film is adjusted according to the signal, it becomes a writing head. In particular, if the exchange force between the magnetic materials is used, writing and rewriting using an effectively large magnetic field can be performed.
- a high-sensitivity magnetic sensor is required, and a technique of a probe scanning microscope, a technique of a tunnel current, a magnetic force or an exchange force microscope can be used. Detection by the magnetoresistive effect or the magneto-optical effect can also be used for signal reading. In particular, the use of a scanning spin microscope that can detect individual spins is effective for detecting minute magnetization.
- FIG. 1 is a schematic diagram showing the magnetic structure of positive and negative spin vortices recorded on a recording medium (magnetic ultrathin film) according to the present invention
- FIG. 1 (a) is a medium showing the magnetization of those spin vortices
- Figure 1 (b) shows the distribution of the component of the magnetization of the spin vortex perpendicular to the medium surface (in the case of positive spin).
- the magnetization distribution of the spin vortex recorded on the recording medium is determined by the following equation, where ⁇ is the tilt angle of the magnetization from the medium surface normal, and p is the distance from the center of the spin vortex.
- FIG. 2 is a conceptual diagram of magnetic recording using a spin vortex as a recording unit according to the present invention.
- FIG. 2 (a) shows an arrangement of spin vortices recorded on a recording medium, and FIG. The magnetization state of the cut surface along the recording track indicated by the chain line A--A in FIG. 2 (a) is shown.
- 1 is a magnetic ultrathin film as a recording medium
- 2 is a recorded positive and negative spin vortex
- 3 is a recording track.
- the direction of the center magnetization of each recording spin vortex is indicated by an arrow.
- 2D is the diameter of the spin vortex
- t is the thickness of the recording medium.
- the recording medium 1 is made of a magnetic ultra-thin film, in which recorded positive and negative spin vortices 2 are arranged.
- FIG. 3 is a schematic view showing an example of the configuration of a recording medium for spin vortex recording according to the present invention, and the arrow indicates the recording surface.
- FIG. 3 (a) is a view showing a soft magnetic ultrathin film medium having essentially no in-plane magnetic anisotropy on a support, where 10 is the support and 11 is no in-plane magnetic anisotropy. It is a soft magnetic ultra-thin film medium.
- FIG. 3 (b) is a diagram showing a recording medium composed of an array of disks of a soft magnetic ultra-thin film on a support, wherein 10 is a support, and 13 is a disk of a soft magnetic ultra-thin film.
- Fig. 3 (c) is a diagram showing a recording medium (support is omitted) consisting of a soft magnetic ultra-thin film formed on a lattice of two sets of soft magnetic ultra-thin thin wires. 23 is a lattice of soft magnetic wires.
- Fig. 3 (d) is a diagram showing a soft magnetic ultra-thin film medium to which an array of magnetic disks having a diameter smaller than the size of the spin vortex to be recorded is added, and the magnetic disk 24 of the recording medium 21 has a high magnetic flux density. It consists of a soft magnetic material, a magnet magnetized perpendicular to the disk surface, or an antiferromagnetic material having an easy axis perpendicular to the disk surface (the support is omitted).
- FIG. 4 is a schematic diagram showing an example of a magnetic recording operation using a spin vortex according to the present invention.
- Fig. 4 (a) writing and rewriting of signals using an electromagnet type head (high magnetic flux density soft magnetic cylinder type magnetic core) 34, leakage of the end of the electromagnet type head due to signal current
- an electromagnet type head high magnetic flux density soft magnetic cylinder type magnetic core
- the distance h between the recording medium 31 and the electromagnetic head 3 4 is kept constant.
- the electromagnet type head 34 can scan by changing the relative position with respect to the recording medium 31 with necessary precision.
- Reference numeral 32 denotes a center line of the electromagnet type head 34
- reference numeral 35 denotes a coil through which a signal current i flows.
- FIG. 4 (b) shows an example of thermomagnetic recording, in which the distance h between the cylindrical magnet needle 36 and the recording medium 31 is made variable according to a signal.
- the distance h is made smaller (closer) and local heating is performed by irradiation with a heating laser pulse 37, a spin vortex 33 is formed.
- the spin vortex is thermally demagnetized.
- the cylindrical magnet needle 36 can scan on the recording medium.
- Fig. 4 (c) is an example of detection of spin vortex magnetization (reproduction of recorded signal).
- Detection based on the tunnel current method is possible. That is, by scanning the recording medium 31 with the conductive cylindrical needle as the detection head 38 and measuring the electrical resistance between the detection head 38 and the recording medium 31 with the current measuring device 39, The direction and magnitude of the magnetization of the spin vortex 33 are detected as a change in the tunnel current due to the magnetoresistance effect, and the recorded signal can be reproduced.
- the distance h between the detection head 38 and the recording medium 31 is kept constant.
- a suitable underlayer having a thickness of 1 nm is grown on a predetermined crystal surface of the support in an ultra-high vacuum, and each of Fe, C0, and Ni is grown thereon.
- These thin films are aggregates of microcrystalline particles having a fibrous structure in which specific crystal axes are aligned perpendicular to the thin film surface. Since they are polycrystalline, their in-plane magnetic anisotropy is small.
- a magnetic needle having a ⁇ 100 ⁇ axis of the single crystal of Fe as a central axis is prepared, and a tip is formed by electropolishing, ion milling and evaporation in a strong electric field to form a tip having a (100) face. Then, an electromagnet having this as a magnetic core was formed and used as a writing head, and a signal was written to the magnetic thin film by changing the direction of magnetization at the tip in accordance with a signal current by vertically approaching the magnetic thin film.
- the size of the recorded spin vortex measured by electron microscopy is about 15 nm, 20 nm, and 35 nm in the above order.
- the magnetization of the recorded spin vortex measured by a scanning spin microscope was 550 G, 450 G, and 150 G in the above order, and both the magnitude and the magnetization intensity almost coincide with the theoretical values shown in Table 1.
- An alloy having an atomic percentage of 80% and a composition of 1 ⁇ 120% of 1 ? E was vapor-deposited on a glass support to form a disk of a polycrystalline film having a thickness of 10 nm.
- the in-plane magnetic anisotropy is small.
- the diameter of the disk was two types, 40 nm and 20 nm.
- a magnetic needle is made of Ni, and an electromagnet having this as a magnetic core is used as a writing head.
- the head is brought close to the recording medium from the vertical direction, and pulsed laser light is irradiated simultaneously with the signal current. A spin vortex in the same direction as the head magnetization was formed on the recording medium disk, and the signal was recorded.
- the magnitudes of magnetization of the two types of disks were 200 G and 50 G in the above order.
- the recording operation was performed by changing the magnitude of the signal current, It was confirmed that writing was possible even when the maximum magnetic field of the portion was smaller than the reversal magnetic field of the medium.
- Example 3
- An array of disks of the same alloy having a diameter of 20 nm and a thickness of 10 nm was formed on a 10 nm-thick alloy vapor-deposited film having the same composition as in Example 2, and this was used as a recording medium.
- the needle of the PtCo magnet is used as a magnetic head, and the recording medium is irradiated with a laser pulse at the same time as the disk is brought close to the disk on the recording medium.
- a spin vortex is formed on the disk near the head. Without laser irradiation, no spin vortex is formed.
- the signal can be recorded in the form of a spin vortex if the laser is driven to 0 n-0 f f in response to the signal. If only the laser is irradiated without bringing the head close, the spin vortex disappears and the signal can be erased.
- the Co film disk will have the [0 0 1] axis of the easy magnetization perpendicular to the thin film surface, and the C 0 disk will be added.
- the vertical anisotropy is locally applied at the position of the thin film surface, and the reversal magnetic field of the thin film at this position is reduced, and it is confirmed that the spin vortex recorded by the same writing operation as above becomes a stable position.
- Example 3 instead of the arrangement of the disks, a grid consisting of two sets of vertical and horizontal straight lines having a width of 20 nm and a thickness of 10 nm is formed.
- a spin vortex is formed at the intersection of the closest lattice, and the signal can be written.
- the recorded signal can also be erased.
- the present invention can use a spin vortex as a recording unit, and is useful as a recording method capable of high-density storage and a magnetic recording apparatus thereof.
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- Engineering & Computer Science (AREA)
- Computer Hardware Design (AREA)
- Chemical & Material Sciences (AREA)
- Nanotechnology (AREA)
- Physics & Mathematics (AREA)
- Mathematical Physics (AREA)
- Theoretical Computer Science (AREA)
- Crystallography & Structural Chemistry (AREA)
- Manufacturing & Machinery (AREA)
- Magnetic Record Carriers (AREA)
- Recording Or Reproducing By Magnetic Means (AREA)
- Manufacturing Of Magnetic Record Carriers (AREA)
Description
Claims
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP99902860A EP0996113A4 (en) | 1998-03-30 | 1999-02-09 | MAGNETIC RECORDING PROCESS AND DEVICE |
US09/424,370 US6504665B1 (en) | 1998-03-30 | 1999-02-09 | Method and apparatus for magnetic recording |
KR10-1999-7011140A KR100375360B1 (ko) | 1998-03-30 | 1999-02-09 | 자기기록방법 및 그 자기기록장치 |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10/83994 | 1998-03-30 | ||
JP8399498 | 1998-03-30 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO1999050833A1 true WO1999050833A1 (fr) | 1999-10-07 |
Family
ID=13818097
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/JP1999/000546 WO1999050833A1 (fr) | 1998-03-30 | 1999-02-09 | Procede et appareil d'enregistrement magnetique |
Country Status (6)
Country | Link |
---|---|
US (1) | US6504665B1 (ja) |
EP (1) | EP0996113A4 (ja) |
JP (1) | JP3153252B2 (ja) |
KR (1) | KR100375360B1 (ja) |
CN (1) | CN1109329C (ja) |
WO (1) | WO1999050833A1 (ja) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2005123617A (ja) * | 2003-10-14 | 2005-05-12 | Internatl Business Mach Corp <Ibm> | パターン化しない連続磁性層にデータを記憶するシステムおよび方法 |
JP2014078560A (ja) * | 2012-10-09 | 2014-05-01 | Institute Of Physical & Chemical Research | 絶縁材料およびその製造方法 |
JPWO2016158230A1 (ja) * | 2015-03-31 | 2017-09-07 | 国立研究開発法人科学技術振興機構 | スキルミオン生成装置、スキルミオン生成方法、および磁気記憶装置 |
Families Citing this family (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6787798B1 (en) * | 2001-01-17 | 2004-09-07 | The Texas A&M University System | Method and system for storing information using nano-pinned dipole magnetic vortices in superconducting materials |
JP3482469B2 (ja) * | 2001-05-21 | 2003-12-22 | 北海道大学長 | 磁気記憶素子、磁気メモリ、磁気記録方法、磁気記憶素子の製造方法、及び磁気メモリの製造方法 |
US6759138B2 (en) * | 2001-07-03 | 2004-07-06 | Hoya Corporation | Antiferromagnetically coupled magnetic recording medium with dual-layered upper magnetic layer |
US6816470B2 (en) | 2001-09-18 | 2004-11-09 | Interdigital Technology Corporation | Method and apparatus for interference signal code power and noise variance estimation |
DE60236878D1 (de) | 2001-09-18 | 2010-08-12 | Interdigital Tech Corp | Verfahren und vorrichtung zur störsignalcodeleistungs- und rauschvarianz schätzung |
KR20050048667A (ko) * | 2002-10-03 | 2005-05-24 | 코닌클리케 필립스 일렉트로닉스 엔.브이. | 판독전용 자기 메모리장치 엠알오엠 |
US7038878B2 (en) * | 2003-10-28 | 2006-05-02 | Hewlett-Packard Development Company, L.P. | Micromover configured to move a magnetic storage medium in perpendicular directions in a plane |
WO2009051442A2 (en) * | 2007-10-19 | 2009-04-23 | Snu R & Db Foundation | Method for read-out of information in magnetic recording element and method for read-out of information in magnetic random access memory |
KR100931582B1 (ko) * | 2008-08-04 | 2009-12-14 | 재단법인서울대학교산학협력재단 | 자기소용돌이를 이용한 자기기록매체의 자기헤드 |
Family Cites Families (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE1921700C3 (de) * | 1969-04-28 | 1974-07-04 | Messerschmitt-Boelkow-Blohm Gmbh, 8000 Muenchen | Einrichtung zur elektronischen Speicherung großer Datenmengen |
CH624516A5 (ja) * | 1977-11-14 | 1981-07-31 | Ibm | |
US4412264A (en) * | 1979-10-22 | 1983-10-25 | Kokusai Denshin Denwa Co., Ltd. | Magneto-optic recording medium |
CA1280207C (en) * | 1986-01-23 | 1991-02-12 | Masatoshi Hayakawa | Device for producing a high frequency modulation magnetic field usedin magneto-optical recording |
JPS6457438A (en) * | 1987-08-28 | 1989-03-03 | Mitsubishi Electric Corp | Recording medium |
KR930009225B1 (ko) * | 1989-09-05 | 1993-09-24 | 미쯔비시덴기 가부시끼가이샤 | 광자기 기록 매체, 광자기 기록 장치 및 광자기 기록 매체의 제조방법 |
US5079219A (en) * | 1989-12-22 | 1992-01-07 | University Of Colorado Foundation, Inc. | Storing information-bearing signals in a superconductive environment using vortices as digital storage elements |
US5331491A (en) * | 1991-03-07 | 1994-07-19 | Sony Corporation | High-density magnetic recording and reproducing head |
JPH05342503A (ja) * | 1992-06-12 | 1993-12-24 | Hitachi Ltd | 記憶装置 |
US5287302A (en) * | 1992-06-22 | 1994-02-15 | The United States Of America As Represented By The Secretary Of The Air Force | Superconducting optically reconfigurable magnetic device |
US5629922A (en) * | 1995-02-22 | 1997-05-13 | Massachusetts Institute Of Technology | Electron tunneling device using ferromagnetic thin films |
-
1999
- 1999-02-09 EP EP99902860A patent/EP0996113A4/en not_active Withdrawn
- 1999-02-09 JP JP54915299A patent/JP3153252B2/ja not_active Expired - Fee Related
- 1999-02-09 US US09/424,370 patent/US6504665B1/en not_active Expired - Fee Related
- 1999-02-09 CN CN99800421A patent/CN1109329C/zh not_active Expired - Fee Related
- 1999-02-09 KR KR10-1999-7011140A patent/KR100375360B1/ko not_active IP Right Cessation
- 1999-02-09 WO PCT/JP1999/000546 patent/WO1999050833A1/ja active IP Right Grant
Non-Patent Citations (6)
Title |
---|
CAIRNS J ET AL.: "The use of high temperature superconducting films for the magnetic storage of information", September 1992, INSTITUTION OF ELECTRICAL ENGINEERS |
FREDKIN D R, KOCHLER T R: "NUMERICAL MICROMAGNETICS: RECTANGULAR PARALLELOPIPEDS", IEEE TRANSACTIONS ON MAGNETICS., IEEE SERVICE CENTER, NEW YORK, NY, US, vol. 26, no. 05, 1 January 1990 (1990-01-01), NEW YORK, NY, US, pages 1518 - 1520, XP002921213, ISSN: 0018-9464, DOI: 10.1109/20.104431 * |
ISHII Y, NAKAZAWA Y: "MAGNETIZATION CURLING IN A DISK WITH A UNIAXIAL ANISOTROPY", JOURNAL OF APPLIED PHYSICS, AMERICAN INSTITUTE OF PHYSICS, US, vol. 81, no. 04, 1 January 1997 (1997-01-01), US, pages 1847 - 1850, XP002921214, ISSN: 0021-8979, DOI: 10.1063/1.364067 * |
RUNGE K., ET AL.: "HIGH-RESOLUTION OBSERVATION OF MAGNETIZATION PROCESSES IN 2 MUM X 2MUM X 0.04 MUM PERMALLOY PARTICLES.", JOURNAL OF APPLIED PHYSICS, AMERICAN INSTITUTE OF PHYSICS, US, vol. 79., no. 08, PART 02A., 15 April 1996 (1996-04-15), US, pages 5075 - 5077., XP000695698, ISSN: 0021-8979, DOI: 10.1063/1.361921 * |
See also references of EP0996113A4 |
TONOMURA A, MATSUDA T, ENDO J: "DIRECT OBSERVATION OF FINE STRUCTURE OF MAGNETIC DOMAIN WALLS BY ELECTRON HOLOGRAPHY", PHYSICAL REVIEW LETTERS., AMERICAN PHYSICAL SOCIETY. NEW YORK., US, vol. 44, no. 21, 1 January 1980 (1980-01-01), US, pages 1430 - 1433, XP002921212, DOI: 10.1103/PhysRevLett.44.1430 * |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
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JP2005123617A (ja) * | 2003-10-14 | 2005-05-12 | Internatl Business Mach Corp <Ibm> | パターン化しない連続磁性層にデータを記憶するシステムおよび方法 |
JP4516817B2 (ja) * | 2003-10-14 | 2010-08-04 | インターナショナル・ビジネス・マシーンズ・コーポレーション | パターン化しない連続磁性層にデータを記憶するシステムおよび方法 |
JP2014078560A (ja) * | 2012-10-09 | 2014-05-01 | Institute Of Physical & Chemical Research | 絶縁材料およびその製造方法 |
JPWO2016158230A1 (ja) * | 2015-03-31 | 2017-09-07 | 国立研究開発法人科学技術振興機構 | スキルミオン生成装置、スキルミオン生成方法、および磁気記憶装置 |
US10134460B2 (en) | 2015-03-31 | 2018-11-20 | Japan Science And Technology Agency | Skyrmion generation device, skyrmion generation method, and magnetic memory device |
Also Published As
Publication number | Publication date |
---|---|
US6504665B1 (en) | 2003-01-07 |
CN1109329C (zh) | 2003-05-21 |
KR20010013157A (ko) | 2001-02-26 |
JP3153252B2 (ja) | 2001-04-03 |
CN1262763A (zh) | 2000-08-09 |
EP0996113A4 (en) | 2006-02-22 |
EP0996113A1 (en) | 2000-04-26 |
KR100375360B1 (ko) | 2003-03-08 |
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