BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a diagram illustrating the operational principle of a perpendicular recording technology;
FIG. 2 is a diagram showing an embodiment of the invention;
FIG. 3 is a functional block diagram of a hard disk device;
FIG. 4 is a schematic diagram of configuration of a magnetic head;
FIG. 5 is a schematic diagram of tip of a main magnetic pole;
FIG. 6 is a diagram of the main magnetic pole as viewed from a magnetic disk;
FIG. 7 is a graph showing the relationship between the number of layers forming the main magnetic pole and the saturation magnetic flux density Bs and coercive force Hc of the main magnetic pole as a whole; and
FIG. 8 is a graph showing the saturation magnetic flux densities and coercive forces of various magnetic materials conventionally widely used as materials for the main magnetic pole.
DETAILED DESCRIPTION OF THE INVENTION
The exemplary embodiments of the invention will be described with reference to the drawings.
FIG. 2 is a diagram showing an embodiment of the invention.
A hard disk device 100 shown in FIG. 2 corresponds to an embodiment of an information storage device in accordance with the invention. An embodiment of a magnetic head in accordance with the invention is applied to the hard disk device 100. The hard disk device 100 is connected to or incorporated into a host apparatus represented by a personal computer or the like.
As shown in FIG. 2, a housing 101 of the hard disk device 100 accommodates a magnetic disk 1 on which information is recorded, a spindle motor 102 which rotates the magnetic disk 1 in the direction of arrow R, a floating head slider 104 located in proximity to and opposite a surface of the magnetic disk 1, an arm shaft 105, a carriage arm 106 having the floating head slider 104 secured to its tip and moving around the arm shaft 105 over and along the surface of the magnetic disk 1, a voice coil motor 107 that drives the carriage arm 106, and a control circuit 108 that controls the operation of the hard disk device 100. A combination of the spindle motor 102 and voice coil motor 107 corresponds to an example of a moving mechanism in accordance with the invention.
A magnetic head 109 is provided at a tip of the floating head slider 104 to apply a magnetic field to the magnetic disk 1. The hard disk device 100 uses this magnetic field to record information on the magnetic disk 1 and read information recorded on the magnetic disk 1. The hard disk device 100 inherently includes multiple magnetic disks 1 for each of which the magnetic head 109 is provided. However, for simplification, the description of the present embodiment focuses on one magnetic disk 1 and one magnetic head 109 provided for the magnetic disk 1.
FIG. 3 is a functional block diagram of the hard disk device 100. FIG. 4 is a schematic diagram showing the configuration of the magnetic head 109.
As shown in FIG. 3, the hard disk device 100 includes the spindle motor 102, voice coil motor 107, control circuit 108, and magnetic head 109, which are also shown in FIG. 2. The control circuit 108 is composed of a hard disk control section 111 that controls the whole hard disk device 100, a servo control section 112 that controls the spindle motor 102 and voice coil motor 107, a voice coil motor driving section 113 that drives the voice coil motor 107, a spindle motor driving section 114 that drives the spindle motor 102, a formatter 115 that formats the magnetic disk 1, a read/write channel 116 that generates a write current carrying write information to be written to the magnetic disk 1 and that converts a reproduction signal obtained by reading information recorded on the magnetic disk 1 by the magnetic head 109, into digital data, a buffer 117 used as a cache for the hard disk control section 111, a RAM 118 used as a work area for the hard disk control section 111, and the like.
FIG. 4 shows the sectional structure of a part of the magnetic head 109. Rotation of the magnetic disk 1 in the direction of arrow R causes the magnetic head 109, positioned over the magnetic disk 1, to appear as if it moves in the direction of arrow R′ that is opposite to the rotating direction of the magnetic disk 1.
The magnetic head 109 has a main magnetic pole 210 that generates a magnetic flux, a coil 250 that generates a magnetic field, an auxiliary magnetic pole 230 that picks up the magnetic flux generated by the main magnetic pole 210 to feed it back to the main magnetic pole 210, and a reproduction head 240 that reads information recorded on the magnetic disk 1; these components are arranged in this order from the backward of the moving direction R′. The magnetic head 109 also includes a yoke 220 that couples the main magnetic pole 210 and the auxiliary magnetic pole 230 together. The main magnetic pole 210 corresponds to an example of a magnetic pole in accordance with the invention. The coil 250 corresponds to an example of a coil in accordance with the invention.
The magnetic disk 1 has a recording layer 1A and a soft magnetic layer 1B stacked on a substrate 1C; information is recorded in the recording layer 1A and the soft magnetic layer 1B is composed of a soft magnetic substance. The magnetic disk 1 corresponds to an example of a recording medium in accordance with the invention.
A method for accessing the magnetic disk 1 will be described with reference to FIGS. 3 and 4.
To write information to the magnetic disk 1, a host apparatus 200 shown in FIG. 3 sends the hard disk device 100 write information to be recorded on the magnetic disk 1 and a logical address for a write position. The hard disk control section 111 converts the logical address into a physical address and transmits the latter to the servo control section 112.
The servo control section 112 instructs the spindle motor driving section 114 to rotate the spindle motor 102. The servo control section 112 also instructs the voice coil motor driving section 113 to move the carriage arm 106 (see FIG. 2). The spindle motor driving section 114 drives the spindle motor 102 to rotate the magnetic disk 1. The voice coil motor driving section 113 drives the voice coil motor 107 to move the carriage arm 106. This allows the magnetic head 109 to be positioned over the magnetic disk 1.
Positioning of the magnetic head 109 causes the hard disk control section 111 to transmit a write signal to the read/write channel 116. The read/write channel 116 then applies a write current carrying write information to the magnetic head 109.
The write signal is input to a coil 250 in the magnetic head 109 which is shown in FIG. 4. The coil 250 generates a magnetic field in a direction corresponding to the write signal. The main magnetic pole 210 emits a magnetic flux corresponding to the magnetic field generated by the coil 250 to the magnetic disk 1. This forms magnetization acting in a direction corresponding to the information, in the recording layer 1A in the magnetic disk 1. The information is thus recorded on the magnetic disk 1. The magnetic flux having formed the magnetization in the recording layer 1A is returned to the auxiliary magnetic pole 230 through the soft magnetic layer 1B. The magnetic flux is then fed back to the main magnetic pole 210 via the yoke 220.
To read information recorded on the magnetic disk 1, the host apparatus 200, shown in FIG. 3, sends the hard disk device 100 a logical address for a recording position at which information is recorded. Then, as is the case with the information writing operation, the hard disk control section 111 converts the logical address into a physical address. The spindle motor 102 is rotationally driven to rotate the magnetic disk 1. The voice coil motor 107 is driven to move the carriage arm 106. This allows the magnetic head 109 to be positioned over the magnetic disk 1.
The magnetic head 109, shown in FIG. 4, has a reproduction element 240a incorporated therein to offer a resistance value corresponding to a magnetic field resulting from magnetization. Passing a current through the reproduction element 240a generates a reproduction signal corresponding to a magnetization state. The embodiment does not particularly limit the specific type of the reproduction element 240a. The reproduction element 240a may be, for example, a GMR (Giant MagnetoResistive) element or a TMR (Tunnel MagnetoResistive) element.
The reproduction signal is converted into digital data by the read/write channel 116, shown in FIG. 3. The digital data is then sent to the host apparatus 200 via the hard disk control section 111.
Basically, information accesses are made to the magnetic disk 1 as described above.
The magnetic head 109 will be described below in further detail.
FIG. 5 is a schematic diagram of tip of the main magnetic pole 210. FIG. 6 is a diagram of the main magnetic pole 210 as viewed from the magnetic disk 1.
As shown in FIG. 5, the main magnetic pole 210 has a facing surface 211 located opposite the magnetic disk 1 and shaped to be narrower toward the front of the moving direction R′ of the magnetic disk 1 and wider toward the back of the moving direction R′. The main magnetic pole 210 tapered from back to front of the moving direction R′ makes it possible to control the side erase caused by an angle of yaw.
Further, as shown in FIG. 6, the main magnetic pole 210 has two layers of a first materials 211A and two layers of a second material 211B alternately stacked on one another along the moving direction R′ of the magnetic disk 1; the first material 211A is, for example, FeNi and has a saturation magnetic flux density Bs of 2.1 [T] and a low coercive force Hc of at most 200 [A/m], and the second material 211B is, for example, FeCo and has a high saturation magnetic flux density Bs of at least 2.3 [T]. The first material 211A corresponds to a first magnetic material in accordance with the invention. The second material 211B corresponds to a second magnetic material in accordance with the invention. In the embodiment, the layers of the first material 211A, which effectively inhibits the pole erase, and the layers of the second material 211B, to which information can be written at a high recording density, are alternately stacked on one another so that the first material 211A is located in the front of the moving direction R′, where the side erase is likely to occur, whereas the second magnetic material, to which information can be written at a high saturation magnetic flux density, is located in the back of the moving direction R′. This reduces the coercive force of the main magnetic pole as a whole below that of the second magnetic material to inhibit the pole erase. It is also possible to achieve both the inhibition of the side erase and an increased recording density. Furthermore, FeNi and FeCo are stacked films having different alloy compositions which belong to a high saturation magnetic flux density composition area and which have body-centered cubit lattice structures. However, advantageously, owing to their similar crystal structures, FeNi and FeCo can be grown in an almost uniform crystal state, with almost no damage layer formed between these layers. During the manufacture of the main magnetic pole 210, FeNi and FeCo can be stacked on one another by using a plating method superior in mass productivity and production cost.
As described above, the embodiment can suppress an increase in manufacturing costs and achieve both the inhibition of the pole erase and side erase and an increased recording density.
In the above example, the main magnetic pole has the two layers of the first material and the two layers of the second material alternately attacked on one another. However, the magnetic pole in accordance with the invention may have a total of four or more layers of the first magnetic material and second magnetic material. A third material different from the first and second magnetic materials may be additionally stacked. The third material may be nonmagnetic provided that it is conductive. If the third material is magnetic, it preferably offers as low a coercive force as possible in order to inhibit the pole erase and side erase.
When the first magnetic material and the second magnetic material are stacked, the saturation magnetic flux density Bs is the sum of saturation magnetic flux densities of all the layers. However, the coercive force Hc of the magnetic head as a whole depends on, for example, the crystallinity of the material constituting each layer. Consequently, the coercive force Hc of the magnetic head as a whole cannot be simply determined from the coercive force of each layer. It is thus preferable to make the layer of the second magnetic material, having a high saturation magnetic flux density, as thick as possible to increase the saturation magnetic flux density of the magnetic head as a whole and then to adjust the thickness of layer of the first magnetic material, offering a low coercive force, to reduce the coercive force of the magnetic head as a whole.
The second magnetic material in accordance with the invention may be FeCO (60<Fe<80 ar %), FeCoNi (55<Fe<80 at %, 20<Co<45 at %, 0<Ni<20 at %), or the like. The first magnetic material in accordance with the invention is preferably a FeNi alloy (Fe>75 at %), a FeCo alloy (Fe>75 at %), or the like. If a third material is stacked between the first magnetic material and the second magnetic material, it may be a permalloy, a 50% nickel permalloy, NiP, NiFeMo, NiMo, Ru, Pd, Pt, Rh, Cu, or the like.
EXAMPLE
An example of the invention will be described.
FIG. 8 is a graph showing the saturation magnetic flux densities and coercive forces of various magnetic materials conventionally widely used for the main magnetic pole.
In FIG. 8, the axis of abscissa is associated with the saturation magnetic flux density Bs [T]. The axis of ordinate is associated with the coercive force Hc [A/m]. CoNiFe-containing magnetic materials are plotted with circles. NiFe-containing materials are plotted with squares. FeCo-containing materials are plotted with rhombuses.
Normally, to inhibit the pole erase, the main magnetic pole needs to offer a coercive force Hc of at most 500 [A/m]. Further, to increase the recording density, the main magnetic pole needs to offer a saturation magnetic flux density Bs of at least 2.1 [T].
Disadvantageously, as shown in FIG. 8, the NiFe-containing materials (plotted with squares) offer coercive forces Hc of at most 500 [A/m] but too low saturation magnetic flux densities Bs. The CoNiFe-containing materials (plotted with circles) offer too large coercive forces Hc or too low saturation magnetic flux densities Bs, and none of them meets both conditions. Only one of the FeCo-containing materials (plotted with rhombuses) meets both conditions, whereas the others offer too high coercive forces Hc. Thus, very few materials formed into single layers can reliably achieve both an increased recording density and the inhibition of the pole erase.
Thus, the present example uses the main magnetic pole 210 that has a first material 211A having a low coercive force Hc and a second material 211B having a high saturation magnetic flux density Bs which are alternately stacked on each other as shown in FIG. 6. The first material 211A is FeNi, which has a saturation magnetic flux density Bs of more than 2 [T] and less than 2.1 [T] and a coercive force Hc of less than 300 [A/m]. The second material 211B is FeCo, which has a saturation magnetic flux density Bs of more than 2.3 [T] and a coercive force Hc of about 800 [A/m]. Layers of the first and second materials having the same film thickness are alternately stacked on one another by using a plating method so that the main magnetic pole is narrower toward the first material 211A side. Thus, the following are prepared: a main magnetic pole composed of a single second layer 211B and main magnetic poles composed of alternately stacked two, four, six, eight, or ten layers of the first material 211A and second material 211B. These main magnetic poles are used to measure the saturation magnetic flux density Bs and coercive force Hc of each main magnetic pole as a whole.
FIG. 7 shows the relationship between the number of layers forming the main magnetic pole and the saturation magnetic flux density Bs and coercive force Hc of the main magnetic pole as a whole.
In FIG. 7, the axis of abscissa is associated with the number of layers forming the main magnetic pole. The axis of ordinate is associated with the saturation magnetic flux density Bs [T] and coercive force Hc [A/m] of the main magnetic pole as a whole. The saturation magnetic flux density is plotted with squares. The coercive force in the hard axis of magnetization is plotted with black rhombuses. The coercive force in the easy axis of magnetization is plotted with white rhombuses.
As shown in FIG. 8, the main magnetic pole composed only of the second material 211B offers a coercive force Hc of more than 500 [A/m], which may cause the pole erase.
However, stacking the first material 211A and second material 211B on each other reduces the saturation magnetic flux density Bs and coercive force Hc of the main magnetic pole as a whole. Stacking four or more layers reduces the saturation magnetic flux density Bs down to about 2.2 [T] and the coercive force Hc down to about 300 [A/m]. This state satisfies both the coercive force Hc required to inhibit the pole erase (at most 500 [A/m]) and the saturation magnetic flux density Bs required to achieve an increased recording density (at least 2.1 [T]). This demonstrates the usefulness of the invention.
Patent Application
20080055775
