• 专利附录
  • 专利说明
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    • 专利摘要:
    The present invention relates to a magnetic recording apparatus and method, wherein the magnetic recording apparatus comprises a magnetic recording medium having a recording layer formed on a substrate, the recording layer comprising magnetic particles and a nonmagnetic material formed between the magnetic particles, A heating unit configured to heat the recording layer, and a magnetic recording unit configured to apply a magnetic field to the recording layer, wherein the magnetic recording medium, the heating unit, and the magnetic recording unit satisfy the following relationship. Is configured to T / RKu (T) <11200 / (ln (t) + 20.72) Here, Ku (T) is the magnetic anisotropy energy density of the recording layer at temperature T, Ku (Ta) is the magnetic anisotropy energy density of the recording layer at ambient temperature Ta, and R Ku (T) is Ku It represents a (T) / Ku (Ta) ratio, and t represents the time elapsed after the application of the magnetic field is completed.
    公开号:KR20000071441A
    申请号:KR1020000012677
    申请日:2000-03-14
    公开日:2000-11-25
    发明作者:기키츠아키라；이치하라가츠타로
    申请人:니시무로 타이죠；가부시끼가이샤 도시바；
    IPC主号:
    专利说明:

    Magnetic recording device and magnetic recording method {MAGNETIC RECORDING APPARATUS AND METHOD OF MAGNETIC RECORDING}
    This application is an application enjoying the priority benefit of Japanese Patent Application No. 11-068185 for which it applied on March 15, 1999, The whole content of the said application is referred here.
    The present invention relates to a magnetic recording apparatus and a magnetic recording method in which recording and reproduction of information are performed magnetically.
    With recent advances in computer processing speed, magnetic recording devices (e.g., hard disk drives (HDDs)) designed to record and reproduce information require further improvements in recording speed and density. However, there is a physical limit to increasing the recording density.
    In order to perform high density recording as a magnetic recording apparatus, it is necessary to allow small magnetic domains to be recorded in the recording layer. In order to distinguish the small write magnetic domains, the magnetic domain edges need to be gentle. To meet the above requirement, the size of the magnetic particles constituting the recording layer must be reduced. It is also required that the recording layer have a small thickness for high density recording, which in turn reduces the size of the magnetic particles. However, if the magnetic particle size is reduced, the magnetic anisotropic energy of the magnetic particles (ie, the product of the magnetic anisotropic energy density Ku and the magnetic particle volume) will be less than the thermal change energy. If the magnetic anisotropy energy of the magnetic particles is smaller than the heat change energy, the magnetization of the recorded magnetic domains will be reversed again, and thus the retention of the recorded information will no longer be possible. This phenomenon is called the thermal change limit or the superferromagnetic limit. It is conceivable to increase the Ku of the magnetic particles in order to prevent the magnetization reversal due to the thermal change. However, when the Ku of the magnetic particles becomes high, the coercive force of the magnetic particles will increase in proportion to Ku. Therefore, it may be impossible to reverse the magnetization with a magnetic field generated by a normal recording head.
    It is an object of the present invention to provide a magnetic recording apparatus and method to achieve such high density recording while exceeding the thermal change limit.
    1 is a schematic diagram showing an embodiment of a magnetic recording apparatus according to the present invention;
    2 is a graph showing the relationship between Ku, R Ku , T / Ku, T / R Ku , and temperature T;
    3 is a graph showing the relationship between the log ln (t) of elapsed time t and the inverse 1 / T of temperature T in a magnetic recording medium according to the present invention;
    4 is a graph showing the relationship between R Ku / T and ln (t) in the magnetic recording medium according to the present invention;
    5 is a graph showing a relationship between T / R Ku and elapsed time t after recording in a magnetic recording medium according to the present invention;
    6 is a graph showing the relationship between R Ku / T and ln (t) as a magnetic recording medium according to the present invention; And
    7 is a graph showing the relationship between T / R Ku and elapsed time t after recording in the magnetic recording medium according to the present invention.
    * Explanation of symbols for the main parts of the drawings
    10 magnetic recording medium 12 lower layer
    13: recording layer 14: protective layer
    20: slider 30: recording / reading element
    40: waveguide
    According to the present invention, there is provided a magnetic recording medium made on a substrate and having a recording layer made of magnetic particles and a nonmagnetic material formed between the magnetic particles, a heating unit made to heat the recording layer, and a magnetic field to the recording layer. There is provided a magnetic recording device made of a magnetic recording unit made to apply, wherein the magnetic recording medium, the heating unit and the magnetic recording unit are configured to satisfy the following relation:
    T / RKu (T) <11200 / (ln (t) + 20.72)
    Where Ku is the magnetic anisotropy energy density of the recording layer at temperature T, Ku (Ta) is the magnetic anisotropy energy density of the recording layer at ambient temperature, and RKu (T) is the ratio Ku (T) / Ku (Ta). T represents the elapsed time after the application of the magnetic field is completed.
    In the magnetic recording apparatus of the present invention, the recording layer preferably has a coercive force of 4 k0e or more at ambient temperature.
    According to the present invention, for a magnetic recording medium comprising a recording layer formed on a substrate and made of magnetic particles and a nonmagnetic material formed between the magnetic particles, a magnetic recording method and a magnetic field comprising the steps of heating the recording layer It is proposed to perform recording by applying to the recording layer and the steps satisfy the following relation:
    T / RKu (T) <11200 / (ln (t) + 20.72)
    Where Ku is the magnetic anisotropy energy density of the recording layer at temperature T, Ku (Ta) is the magnetic anisotropy energy density of the recording layer at ambient temperature, and RKu (T) is the ratio Ku (T) / Ku (Ta) T represents the elapsed time after the application of the magnetic field is completed.
    In the present invention, for example, a method in which the recording layer is heated such that RKu (Tmax) at the maximum temperature Tmax is 0.01 or less in the heating step may be used, and within 1 to 50 ns after the recording layer reaches the maximum temperature in the recording step. The recording operation is completed.
    In the present invention, another method may be used in which the recording layer is heated such that RKu (T) is zero before the recording layer reaches the maximum temperature in the heating step, and 20 after the recording layer reaches the maximum temperature in the recording step. The write operation is completed within ˜100 ns.
    Additional objects and advantages of the invention will be set forth in part in the description which follows, and in part will be obvious from the description, or will be learned by the practice of the invention. The objects and advantages of the invention will be realized and obtained by various means and in particular by the combinations indicated below.
    The accompanying drawings, which form a part of this specification, illustrate the principles of the invention together with the description of the preferred embodiments and the invention, which will be described below in conjunction with the foregoing description.
    The magnetic recording apparatus according to the present invention is composed of a magnetic recording medium, a heating unit, and a magnetic recording unit. The heating of the recording layer of the magnetic recording medium in the apparatus of the present invention is performed by using a heating unit, and then a magnetic field is applied to the recording layer by using the magnetic recording unit, whereby recording is performed. This method is referred to as heat-assisted recording. When the temperature of the magnetic layer rises, the coercive force is thereby reduced, and the magnetization of the magnetic layer can be reversed by applying a magnetic field, thereby enabling magnetic recording. The magnetic recording apparatus of the present invention can perform magnetic recording even at a magnetic material having a coercive force Hc of 4 kOe or more at ambient temperature.
    The magnetic recording apparatus of the present invention has a structure in which a recording layer made of magnetic particles and a nonmagnetic material formed between the magnetic particles is made on a substrate. The lower layer can be sandwiched between the substrate and the recording layer. In addition, a protective layer can be formed on the recording layer.
    The substrate helps to assist the recording layer and may be formed of metal, glass, ceramic, or the like.
    The recording layer is a so-called granular layer composed of magnetic particles and a nonmagnetic material formed between the magnetic particles. A recording layer having such a structure can be formed as follows. For example, as in the case of forming a recording layer of a conventional hard disk, when magnetic material is deposited on a substrate by sputtering, circular magnetic crystals grow and at the same time a nonmagnetic element is isolated around the magnetic crystals. Thus, a nonmagnetic material (particle boundary) is formed between the magnetic particles.
    Alternatively, a continuous film of amorphous magnetic material may be deposited on the substrate, followed by treatment of the continuous film to form circular magnetic particles. Depositing the nonmagnetic material over the entire surface of the substrate and polishing the resulting surface can result in a structure in which the nonmagnetic material is formed between the magnetic particles. In addition, only coating a lubricant on the entire surface of the substrate can create a structure in which a nonmagnetic material is formed between the magnetic particles.
    As the material for forming the recording layer, a magnetic material showing high saturation magnetization (Is) and high magnetic anisotropy is suitable. As such a magnetic material, it is possible to use at least one kind of magnetic metal material selected from the group consisting of Co, Pt, Sm, Fe, Ni, Cr, Mn, Bi, Al and alloys of these metals. Of these magnetic metal materials, Co-based alloys having high crystalline magnetic anisotropy, in particular CoPt-based alloys, SmCo-based alloys and CoCr-based alloys, are preferred. Specific examples of magnetic metal materials include Co-Cr, Co-Pt, Co-Cr-Ta, Co-Cr-Pt, Co-Cr-Ta-Pt, Co and Fe.
    Atypical rare earths such as Tb-Fe, Tb-Fe-Co, Tb-Co, Gd-Tb-Fe-Co, Gd-Dy-Fe-Co, Nd-Fe-Co and Nd-Tb-Fe-Co as magnetic materials It is possible to use transition metal alloys, sequential alloys such as PtMnSb and FePt, magnetized oxides such as Co ferrite and Ba ferrite, and the like.
    At least one kind of element selected from Fe and Ni may be added to the magnetic material to control magnetization properties such as saturation magnetization and coercivity. Furthermore, Cr, Nb, V, Ta, Ti, W, Hf, Cr, V, In, Si, B or such with at least one element selected from oxygen, nitrogen, carbon, and hydrogen to improve the magnetization properties Compounds of the elements can be added to the magnetic material.
    The recording layer may be a recording layer showing coplanar magnetic anisotropy, such as a recording layer of a hard disk, or a recording layer showing vertical magnetic anisotropy, such as a recording layer of a magnetic optical disc.
    The bottom layer can be composed of magnetic or nonmagnetic materials. The underlying layer made of magnetic material may be magnetically coupled to the magnetic region in the recording layer through exchange coupling interactions or magnetostatic coupling interactions. The magnetic domain can be stabilized when a magnetic underlayer with high saturation coercivity is disposed below the recording layer and exchange-coupled with the magnetic domain in the recording layer. Moreover, when a magnetic underlayer having a high magnetization is disposed below the recording layer and exchange-coupled with the magnetic domain in the recording layer, the output signal can be raised.
    A lower layer made of a nonmagnetic material may be disposed for the purpose of controlling the crystallinity of the recording layer or to prevent impurities from occurring in the substrate and mixing into the recording layer. For example, when a lower layer having a lattice constant close to the crystal lattice of the recording layer is disposed, the crystallinity of the recording layer can be controlled. An example of such an underlayer is a Cr layer. By using an amorphous underlayer, the recording layer can generally be atypical. In order to prevent impurities from occurring in the substrate and mixing into the recording layer, a thin film or a dense thin film having a small lattice constant should be used as the lower layer as much as possible.
    Moreover, the magnetic underlayer may have the above mentioned function of the nonmagnetic underlayer. For example, the magnetic underlayer can help to control the crystallinity of the recording layer. In this case, both the effect of improving the read / write characteristics and the effect of improving the crystallinity can be obtained. An example of such an underlayer is an amorphous CoZrNb underlayer.
    Note that the underlayer may consist of a modified surface layer of the substrate. The modified surface layer can be obtained by methods such as ion plating, doping of gas components, neuron beam irradiation, and the like. In this case, depositing the underlying layer can be omitted.
    As protective layer it is possible to use carbon, SiN, SiO 2 , Au or a stack of these materials.
    The heating unit may be designed to heat the whole or part of the surface of the recording medium. High density magnetic recording media are generally damaged under the influence of heat changes when heated, resulting in worsening data storage characteristics. Therefore, partial heating is preferably such that most of the recording medium is maintained at ambient temperature. However, in the case of the magnetic recording apparatus having the recording medium in which the data storage characteristics hardly deteriorate even during the entire heating, the entire heating may be preferred in terms of cost reduction.
    As an example of a heating unit that enables high speed partial heating, it is conceivable to use heating with a laser, induction heating, or heating with a probe heated with a heating wire, as in an optical disc.
    Heating system for focusing the laser beam through a lens on the surface of the recording medium to perform more partial heating, heating system for induction heating using a precision antenna attached to the end of the probe, or facing the medium It is also possible to use a heating system in which the tip of the probe is as sharp as possible or the heating is done using a heating probe where the tip of the probe is located as close as possible to the medium. Such heating means may be located next to or opposite the recording surface of the recording medium.
    It is possible to use an ordinary magnetic recording head as the magnetic recording unit. The recording head may constitute a magnetic circuit composed of magnetic polarity and induction coil. It is also possible to use a permanent magnet as the magnetic recording unit. When using a permanent magnet, the permanent magnet is arranged in such a way that the distance can be changed so that the recording medium or the permanent magnet can be precisely processed to apply a high-resolution magnetic field at high speed. It is also possible to use an additional magnetic layer laminated on the recording layer as a method of applying the magnetic field. When there is a temperature distribution in the additional magnetic layer by heating or light irradiation, a magnetization distribution is made in the layer so that a magnetic field can be applied to the recording layer. The leakage magnetic field generated in the magnetic layer can be applied to the recording layer as a recording magnetic field.
    An embodiment of a magnetic recording apparatus according to the present invention will be described with reference to FIG. In FIG. 1, the magnetic recording medium 10 has a structure in which the lower layer 12, the recording layer 13, and the protective layer 14 are stacked on the disk substrate 11 in order. This magnetic recording medium 10 rotates in the direction indicated by arrow A in FIG.
    A slider 20 is disposed on the magnetic recording medium 10, and a recording / reading element 30 is mounted on the end surface thereof. The recording element portion of the recording / reading element 30 functions as a magnetic recording unit (means for applying a magnetic field). The slider 20 has a waveguide 40 through which a laser beam is transmitted, so that the laser beam is irradiated onto the medium 10 from the end portion 41 of the waveguide 40. The slider 20 is designed to slide as it slides over the magnetic recording medium 10 when rotated. The waveguide 40 and the recording / reading element 30 are arranged so that a laser beam is first irradiated from the end portion 41 of the waveguide 40 and then a magnetic field is applied to the recording layer 13 by the recording element. Are arranged.
    According to the magnetic recording apparatus of the present invention, the recording operation is performed when the temperature and the magnetic property of the recording layer with respect to the elapsed time t after the application of the magnetic field to the recording layer are completed satisfy the following expression (1).
    Where T is the temperature of the recording layer. Further, Ku (T) is the magnetic anisotropy energy density value of the recording layer at the temperature T, Ku (Ta) is the value at the ambient temperature Ta, and the ratio between the two values at RKu (T), that is, Ku ( Assume that T) / Ku (Ta) is represented. As long as the recording layer satisfies Equation 1, even if the recording layer is made of magnetic particles having a small size and high coercive force, a uniform and distinct magnetic domain in the recording layer is formed. It is possible to form. As a result, it is possible to perform high density magnetic recording that exceeds the thermal change limit.
    The relationship of Equation 1 will be described in more detail.
    Among the physical properties for the magnetization reversal of the recording layer, the magnetic anisotropy energy density Ku varies greatly with temperature. Magnetic anisotropy energy density Ku decreases with increasing temperature T. Since the coercive force Hc changes in approximately proportional to Ku, the coercive force Hc may decrease due to an increase in the temperature T. On the contrary, in Equation 1, the T / RKu (T) value increases with temperature (T). 2 illustrates the property relationship between these functions.
    First, the inventors of this application simulated the temperature response of the recording medium which has a thin film laminated structure as shown in FIG. 1 by irradiating a medium with a laser beam. As a result, it has been found that there is a relationship between the inverse 1 of the temperature T of the recording medium T after completion of the magnetic field application and the log value ln (t) of the elapsed time t. Fig. 3 shows an example of the relationship between the inverse 1 / T of the temperature T of the recording medium after the application of the magnetic field and the log value ln (t) of the elapsed time t. As is apparent from Fig. 3, 1 / T is almost proportional to ln (t) at the initial stage as well as at the later stage of the cooling procedure of the recording medium, so that the relationship between them is approached by a pair of straight lines (dotted line in Fig. 3). It becomes possible. Therefore, the inventors of the present application completely recorded by examining the state recorded for ln (t) through recording / reading attempts under various temperature reactions in the recording layer, even when the magnetization reversal occurs during the cooling process of the recording layer. Expected a state to perform the state.
    The change in the magnetic anisotropy energy density Ku, which is closely related to the magnetization reversal of the recording layer, continues to change with T as described above. However, since both T and Ku change together during the cooling procedure of the recording layer, it is difficult to correlate these variables individually to the recording layer. Thus, the inventors of the present application find that either function Ku / T decreasing with temperature or function RKu / T obtained by normalizing Ku / T according to the Ku value at ambient temperature is useful for correlating with ln (t). I found out.
    The magnetic recording medium 10 shown in FIG. 1 is a lower layer 20 with a 70 nm thick Cr layer, a recording layer 13 with a 20 nm thick CoPtCr alloy layer, and a 2.5 inch thin glass disk substrate 11. The protective layer 14 was laminated with a 10 nm thick carbon layer. The recording layer 13 formed of the CoPtCr alloy layer has a coercive force of 8 × 10 6 erg / cc Ku and 4 kOe at ambient temperature.
    The magnetic recording medium 10 was rotated at 4500 rpm in the direction indicated by the arrow A, and the flying height of the slider 20 was set to 80 nm. A laser beam having a wavelength of 650 nm and a power of 3 mW is continuously irradiated onto the recording medium 10 through the end portion 41 of the light waveguide 40 and a magnetic field is directed to the recording medium 10 by the recording element. Recording was performed at a recording frequency of 200 kfci. The beam spot size on the surface of the recording medium was set to 2 mu m in total width at half the maximum value. The recording state of the recording medium was determined by observing the magnetic domain with a magnetic force microscope (MFM).
    With this apparatus, it is impossible to form a distinct magnetic domain when no laser beam is irradiated onto the recording medium. On the other hand, when the above-mentioned state condition laser beam was irradiated on the recording medium, it was confirmed that a magnetic domain was formed.
    Moreover, in order to study the state in which the magnetic domains are formed, recording experiments were performed not only by heating states by a laser beam but also by various rotational speeds of the recording medium. Then, the recording medium was observed by MFM to see if a uniform and distinct magnetic domain was formed or not.
    In this case, the Ku (T) value of the recording medium was determined through measurement, and RKu (T) was calculated. The temperature of the recording medium was determined based on the simulation.
    The experimental results are expressed in the coordinates of RKu (T) and ln (t). The hollow circles in FIG. 4 indicate where magnetic domains are formed and the black circles indicate where magnetic domains are not formed. It will be appreciated that it is possible to perform recording in the state of the upper partial region of the straight line shown in this figure. This relationship can be expressed as
    In order to make it easier to understand this relationship in which the temperature T is lowered with the elapsed time t, the results of the experiment are shown in FIG. 5 after elapsed time t and T / RKu coordinates. In Fig. 5, the hollow circle also indicates where the magnetic domain is formed and the black circle indicates where the magnetic domain is not formed. Fig. 5 shows that it is possible to perform recording under the condition in the lower area of the curve. The relationship of FIG. 5 is obtained by changing the numerator and denominator of Equation 2, which can be expressed as follows.
    T / RKu (T) <11200 / (ln (t) + 20.72)
    As long as the above Equation 1 is satisfied, the magnetic domain can be formed in the recording layer.
    In the same manner as mentioned above, heating to the recording medium and magnetic recording are carried out under four conditions to track the change of elapsed time RKu / T after recording. These four states are selected near the boundary of FIG. The experimental results are shown in FIG. 6 by RKu / T and ln (t) coordinates. Four marks in FIG. 6 correspond to four states, respectively. The hollow circles in FIG. 6 also indicate where magnetic domains are formed, and the black circles indicate where magnetic domains are not formed. In FIG. 6, the upper region of the straight line is represented by Equation 2 mentioned above. Fig. 6 shows that at any temperature, if Equation 2 is not satisfied after recording, no magnetic domain can be formed in the recording layer under that condition.
    Experimental results are shown in the coordinates of T / RKu and elapsed time (t) in FIG. 7 so that the relationship that the temperature (T) is lowered with the elapsed time (t) can be easily understood. The mark in FIG. 7 has the same meaning as in FIG. 6. In FIG. 7, the lower partial region of the curve is represented by Equation 1 mentioned above. Fig. 7 shows that no magnetic domain can be formed in the recording layer under such a condition even if Equation 1 is not satisfied after recording at any temperature. Therefore, it can be concluded that in the state represented by Equation 1, it is satisfied at any time in the cooling procedure after recording.
    According to the magnetic recording apparatus of the present invention, it is composed of a magnetic recording medium, a heating unit, and a magnetic recording unit, so that the recording operation can be performed so as to satisfy the above expression (1). Next, the components to be considered to satisfy the above equation 1 will be described below.
    The method of changing the temperature of the recording layer can be adjusted as follows. For example, using a recording medium in which a heat sink layer having a high thermal conductivity or a heat-insulating layer made of a dielectric material having a low thermal conductivity is disposed in the vicinity of a recording medium such as is adopted in an optical recording medium. do. When the heat sink layer is used, the rate of change (dT / dt) of the temperature (T) of the recording layer with respect to the time (t) gradually increases, and there may be a sudden temperature change. As a material for the heat sink layer, a conductive material such as Ag can be used. On the other hand, in the case of using the heat-insulating layer, (dT / dt) gradually decreases, and there may be a smooth temperature change. As the heat-insulating material, a dielectric material such as SiO 2 may be used.
    In addition, when both the heat sink layer and the dielectric layer are used, it may be possible to design a desired temperature change in the recording layer. Such a recording medium can be applied to a system using laser heating or induction heating. In a system using laser heating, the dT / dt of the recording medium can be controlled by using a light absorbing layer whose absorption and thickness are appropriately adjusted.
    Therefore, the temperature dependency of Ku of the recording layer, i.e., RKu (t), can be controlled by selecting a material suitable for the recording layer. In the present invention, the coercive force Hc of the recording layer is 4 kOe or its in order to be able to record to the recording layer containing fine magnetic particles through heating and to maintain the recorded data at ambient temperature. The above is appropriate.
    When the recording layer is made of ferromagnetic CoPr, the Curie temperature decreases as Pt increases, so that it is possible to increase dKu / dT near the ambient temperature. The same effect can be obtained even in the CoPtCr recording layer by increasing the Cr content. Generally speaking, increasing the content of the nonmagnetic element in the recording layer can increase dKu / dT near the ambient temperature. In other words, if an element that increases the Curie temperature is added to the recording layer, the opposite effect to that described above can be obtained.
    When the recording layer is made of ferromagnetic TbFeCo used in a magneto-optical recording medium, if the Co content is reduced, the Curie temperature can be lowered and the dKu / dT near the ambient temperature can be increased. Furthermore, if the recording layer is formed using a ferromagnetic material having a Curie temperature higher than the maximum temperature of the recording layer obtained by heating, recording can be performed under the condition that the coercive force (Hc) is lowered while RKu is kept at a constant value. Can be. In this case, since there is a proportional relationship between T / RKu and T, there is an advantage in terms of designing a magnetic recording medium.
    It is also possible to control the RKu of the recording layer by adjusting the size of the magnetic particles constituting the recording layer. As mentioned above, the recording layer composed of CoCrPaTa used in the hard disk is composed of fine magnetic crystalline particles separated from each other so that the binding interaction does not change. When the recording layer is formed by reducing the size of the magnetic crystalline particles, the influence of thermal energy becomes relatively large, and the dKu / dT value can be large. On the other hand, using a material with a high Ku can minimize this effect. The RKu of the recording layer can be controlled by selecting a material with an appropriate Ku value.
    In addition, the Ku value of the recording layer can be increased by randomly arranging the magnetization inversion axis without orientation in the plane of the recording layer without changing the material of the recording layer.
    In order to satisfy the above state of Equation 1, the laser heating can be adjusted in various ways as follows.
    (1) The laser power can be adjusted. As the laser power is increased, the maximum temperature of the recording layer further increases.
    (2) The laser beam irradiation method can be adjusted. For example, continuous irradiation of a laser beam results in a heating flow from an area already passed by the laser beam. As a result, the temperature change of the recording layer becomes smoother.
    (3) The linear velocity of the recording layer relative to the laser can be adjusted. More particularly, the rotational speed of the disc can be adjusted. Increasing the moving speed of the recording layer shortens the irradiation time of the laser beam onto the area in the recording layer, so that the temperature rise of the recording layer can be suppressed, and at the same time its temperature change is sharpened.
    (4) The laser can be operated in a pulsed manner, and at the same time the pulse width can be adjusted. When the pulse width is narrowed, the temperature rise of the recording layer is suppressed, and its temperature change is sharpened.
    (5) In addition to the above (4) method, the laser power can be adjusted at every pulse. For example, short pulses of low power may be irradiated in advance for preheating and then high power pulses to the main heating source. By using this method, it is possible to smooth the temperature rise. In this case, an almost obscure combination of pulse width, modulation, and power of the pulse train may be considered. Therefore, a pulse train with an optimal combination must be determined in a manner that satisfies the state of Equation 1 above for a recording layer exhibiting a given RKu (T) characteristic.
    (6) The shape of the laser beam spot can change. In the case of making the shape of the beam spot elliptical on the main axis lying along the moving direction of the medium, the temperature change of the recording layer can be smooth due to the effect as mentioned in (2) above. In this case, the optical system for a laser may operate as a piezoelectric element or a micromachine to change the shape of the beam spot. Using this method, the shape of the laser beam can be adjusted to the type of recording medium which exhibits various RKu (T) characteristics, the linear velocity of the recording medium, and the radius of rotation.
    (7) The distance between the recording element and the laser for applying the magnetic field can be adjusted. The greater the distance between the recording element and the laser, the smoother the temperature change of the recording layer during recording is in progress. In this case, the position of the tip of the irradiation tip for the laser beam may coincide with the piezoelectric element or the micromachine. By using this method, the distance can be adjusted to the type of recording medium which exhibits various RKu (T) characteristics, the linear velocity of the recording medium, and the radius of rotation.
    The above methods (1) to (7) can be appropriately combined with each other. In the case of using a heating unit other than a laser, the same method as described above can be applied.
    Next, an embodiment in which recording is performed on a magnetic recording medium having a recording layer composed of an amorphous rare earth transition metal alloy will be described. A glass substrate 2.5 inches thick with a 110 nm thick SiN layer as a lower layer 12, a 20 nm thick GdTbFeCo alloy layer as a recording layer 13, and a 40 nm thick SiN and 25 nm thick Au layer as a protective layer 14. A magnetic recording medium 10 constructed by laminating on (11) is used.
    The GdTbFeCo recording layer 13 is used as an optical magnetic medium and is a ferromagnetic material exhibiting perpendicular magnetic anisotropy. Its Ku at ambient temperature is 10 8 erg / cc and its coercivity is as high as 8 kOe. Ku of the recording layer 13 gradually decreases linearly as the temperature T contacts the Curie temperature. By controlling the mixing ratio between GdTb and FeCo, it is possible to significantly lower the coercive force (He) without Ku, which is greatly reduced by the temperature rise. This is an inherent property of ferromagnetic materials.
    The recording layer rotates at a linear speed of 8 m / s. By using the pickup for the optical disk, a laser beam having a wavelength of 650 nm is irradiated from the glass substrate side 11. Focus the laser beam spot size to 0.7 mu m on the surface of the record carrier. The recording operation is performed using the recording / reading element 30 mounted on the slider 10 at a flight height of 100 nm as in FIG. While continuously irradiating a laser beam of 3 mW, magnetic recording proceeds at a recording frequency of 200 kfci. The recording track width is 2 mu m. Regeneration is performed using a regeneration head composed of GMR elements.
    When the recording layer 13 is heated to the maximum temperature, RKu becomes 0.9, but the coercive force He decreases from 8 kOe value to 0.9 kOe at ambient temperature. When the coercive force is around this value, a normal recording head can form a magnetic domain. This was found from the measurement of the time dependence of T / RKu in this experiment where the Equation 1 state is insufficiently satisfied because the RKu value is large.
    However, when the GdTbFeCo recording layer is formed of an amorphous continuous film, domain walls are inevitably formed, which makes it difficult to form precise magnetic domains.
    Thus, after forming a continuous film of GdTbFeCo, the film is adjusted by electron-beam lithography to form a structure arranged in columnar magnetic particles each having a diameter of 10 nm and 10 nm. Next, a recording experiment for the medium was performed in the same manner as described above, and its magnetic domain was observed by MFM. As a result, it was confirmed that each of the recorded magnetic domains composed of single domain particles did not form any domain wall. This means that high density recording in a single-domain size unit can be realized. As described above, it has been found that a magnetic recording medium maintaining a high density can be produced by treating the recording layer.
    Next, an experiment was conducted to study proper timing of applying a magnetic field to the recording layer after irradiating a laser beam. In this experiment, a magnetic recording medium having a CoPtCr recording layer was used.
    (A) The structure of the medium, the laser power and the rotational speed of the disc are adjusted in such a way that the state of RKu ≧ 0.01 can be maintained at the maximum temperature of the magnetic recording medium. The recording experiments were carried out such that the medium had a period from the time when the maximum temperature was reached at the time when the recording was set to 1, 2, 5, 10, 20, 50 and 100 ns, respectively. After the recording operation, the recording layer was observed by MFM to confirm whether a magnetic domain was formed. As a result, it was found that the proper magnetic domain was formed in all states except for the 100 ns cycle. This result is interpreted to be difficult to perform proper recording because the coercive force He increases with the time elapsed after the recording layer reaches the maximum temperature. In addition, in order to keep the medium temperature high enough to allow sufficient recording in a period of about 100 ns, the maximum temperature of the medium must be raised. As a result, the periphery of the magnetic domain becomes unstable, and as a result, the magnetic domain can be reversed.
    (B) The structure of the medium, the laser power and the rotational speed of the disc are adjusted in such a way that the maximum temperature of the recording layer exceeds the Curie temperature. In this case, the recording medium loses magnetization, so that RKu returns to zero before the recording layer reaches the maximum temperature. The recording experiments were performed in such a way that the period was set to 1, 2, 5, 10, 20, 50 and 100 ns from the time the medium reached the maximum warmth to the completion of the recording, respectively. After the recording operation, the recording layer was observed by MFM to observe whether a magnetic domain was formed. As a result, unlike the above (A), it was found that an appropriate magnetic domain was formed only when the period was set to 20 ns or more. This result is interpreted that the recorded magnetic domain is extremely unstable near RKu = 0, so that the magnetic domain may be reversed if recording is performed within a short time after the recording layer reaches the maximum temperature. On the other hand, if a long time is required before recording is completed in this case, it is not preferable in view of improvement of recording density and transfer rate. However, in this case, since it is possible to use a recording medium having a very high coercive force He at the ambient temperature, it is possible to apply the medium to a low speed recording system having excellent recording characteristics.
    Additional advantages and modifications will be apparent to those skilled in the art. Therefore, more broad aspects of the invention are not limited to the specific description or illustrated embodiments and details described herein. Accordingly, various modifications may be made without departing from the spirit and scope of the invention as defined by the appended claims.
    According to the magnetic recording apparatus and method according to the present invention, high density recording can be performed even if the thermal change limit is exceeded.
    权利要求:
    Claims (14)
    [1" claim-type="Currently amended] A magnetic recording medium having a recording layer made of magnetic particles and a nonmagnetic material formed between the magnetic particles on a substrate;
    A heating unit configured to heat the recording layer; And
    A magnetic recording unit configured to apply a magnetic field to the recording layer,
    The magnetic recording medium, the heating unit and the magnetic recording unit are configured to satisfy the following relationship:
    T / RKu (T) <11200 / (ln (t) + 20.72)
    Here, Ku (T) is the magnetic anisotropy energy density of the recording layer at the temperature T, Ku (Ta) is the magnetic anisotropy energy density of the recording layer at the atmospheric temperature Ta, and RKu (T) is A magnetic recording apparatus characterized by indicating a Ku (T) / Ku (Ta) ratio, and t indicating an elapsed time after completion of magnetic field application.
    [2" claim-type="Currently amended] The method of claim 1,
    And the coercive force of the recording layer is 4 kOe or more at ambient temperature.
    [3" claim-type="Currently amended] The method of claim 1,
    And the recording layer is formed of a Co-based alloy.
    [4" claim-type="Currently amended] The method of claim 1,
    And the recording layer is formed of a rare earth transition metal alloy.
    [5" claim-type="Currently amended] The method of claim 1,
    And the heating unit is a laser.
    [6" claim-type="Currently amended] The method of claim 1,
    And the magnetic recording unit is a magnetic recording head.
    [7" claim-type="Currently amended] The method of claim 1,
    And the heating unit and the magnetic recording unit are integrally provided.
    [8" claim-type="Currently amended] A magnetic recording method for a magnetic recording medium comprising a recording layer formed on a substrate and composed of magnetic particles and a nonmagnetic material formed between the magnetic particles, the method comprising:
    Heating the recording layer; And
    Applying a magnetic field to the recording layer to perform recording;
    The above steps satisfy the following relationship:
    T / RKu (T) <11200 / (ln (t) + 20.72)
    Here, Ku (T) is the magnetic anisotropy energy density of the recording layer at the temperature T, Ku (Ta) is the magnetic anisotropy energy density of the recording layer at the atmospheric temperature Ta, and RKu (T) is And wherein k represents the Ku (T) / Ku (Ta) ratio, and t represents the time that has elapsed since the application of the magnetic field was completed.
    [9" claim-type="Currently amended] The method of claim 8,
    The coercive force of the recording layer is 4 kOe or more at ambient temperature.
    [10" claim-type="Currently amended] The method of claim 8,
    The heating step is performed such that the RKu (Tmax) of the recording layer at the highest temperature is 0.01 or less; And
    And the recording step is performed such that the recording operation is completed within 1 ns to 50 ns after the recording layer reaches the highest temperature.
    [11" claim-type="Currently amended] The method of claim 8,
    The heating step is performed such that RKu (T) of the recording layer becomes zero before the recording layer reaches the highest temperature; And
    And the recording step is performed such that the recording operation is completed within 20ns to 100ns after the recording layer reaches the highest temperature.
    [12" claim-type="Currently amended] The method of claim 8,
    And the heating unit is a laser.
    [13" claim-type="Currently amended] The method of claim 12,
    The intensity of the laser beam irradiated onto the recording layer from the laser and the rotational speed of the recording medium are adjusted.
    [14" claim-type="Currently amended] The method of claim 12,
    And a pulsed laser beam of which pulse width is adjusted to the recording layer.
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    同族专利:
    公开号 | 公开日
    EP1037198B1|2006-05-03|
    CN1267054A|2000-09-20|
    EP1037198A3|2002-04-10|
    EP1037198A2|2000-09-20|
    US6493164B1|2002-12-10|
    KR100371453B1|2003-02-06|
    DE60027629D1|2006-06-08|
    DE60027629T2|2006-09-14|
    CN1201317C|2005-05-11|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    法律状态:
    1999-03-15|Priority to JP6818599
    1999-03-15|Priority to JP11-068185
    2000-03-14|Application filed by 니시무로 타이죠, 가부시끼가이샤 도시바
    2000-11-25|Publication of KR20000071441A
    2003-02-06|Application granted
    2003-02-06|Publication of KR100371453B1
    优先权:
    申请号 | 申请日 | 专利标题
    JP6818599|1999-03-15|
    JP11-068185|1999-03-15|
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