Abstract:
A magnetic head measuring apparatus executes measurement with respect to at least one measurement point on a recording head. The apparatus includes a probe having a magnetic substance, a vibrator which vibrates the probe above the at least one measurement point, a first signal generator which supplies a drive signal to the vibrator, a second signal generator which supplies a current containing a direct current and an alternate current to the recording head to generate a magnetic field from the recording head, a detector configured to detect a signal corresponding to a force interaction that acts on the probe due to the magnetic field generated from the recording head in accordance with the current supplied by the second signal generator, and a measurement unit which measures current dependence of the magnetic field of the recording head from the signal detected by the detector.

Description:
CROSS-REFERENCE TO RELATED APPLICATIONS  
         [0001]    This application is based upon and claims the benefit of priority from the prior Japanese Patent Application No. 2001-028551, filed Feb. 5, 2001, the entire contents of which are incorporated herein by reference.  
         BACKGROUND OF THE INVENTION  
         [0002]    1. Field of the Invention  
           [0003]    The present invention relates to a magnetic head measuring apparatus for measuring magnetic field characteristics of a magnetic head and a measuring method applied to the magnetic head measuring apparatus.  
           [0004]    2. Description of the Related Art  
           [0005]    Conventionally, in the process of manufacturing a magnetic head used for, e.g., a hard disk drive, a process of measuring magnetic field characteristics such as field distribution or field saturation phenomenon of a recording head (write head) included in the magnetic head is indispensable. A recording head is formed from, e.g., an inductive thin-film head and has a magnetic gap for generating a recording field corresponding to a signal current applied to the coil.  
           [0006]    As the measurement schemes in the measuring process, (1) a scheme using a measuring apparatus called a spin stand dedicated to a head/disk, (2) a scheme using a dedicated magnetic head measuring apparatus using a magnetic force microscope (MFM), and (3) a scheme using computer simulation are known.  
           [0007]    In the measuring scheme using a spin stand, a signal for measurement is recorded on a disk recording medium while changing a write current value for a recording head to be measured, and the recorded signal is reproduced by a reproduction head (read head). With the spin stand, magnetic field characteristics of the recording head is measured using the recorded signal output from the reproduction head.  
           [0008]    In the measuring scheme using an MFM, a DC (Direct Current) is applied to the recording head, and a DC magnetic field (recorded magnetic field) generated from the recording head is measured by the MFM.  
           [0009]    In the scheme using computer simulation, a DC magnetic field (recorded magnetic field) generated from the recording head when a DC (Direct Current) is applied to the recording head is obtained by simulation on a computer.  
           [0010]    The various kinds of conventional measuring schemes described above have the following problems.  
           [0011]    In the measuring scheme using a spin stand, since a recorded signal is measured through a disk recording medium and reproduction head (MR head), a measurement result including the characteristics of these components is obtained. For this reason, the saturation magnetic field of the recording head cannot be directly observed. In addition, a saturation phenomenon is assumed to occur from a corner (edge) of a magnetic pole of a recording head. However, with this measuring scheme, this phenomenon cannot be locally detected.  
           [0012]    In the measuring scheme using an MFM, since a saturation field is measured by supplying only a DC, an improvement of resolving power cannot be expected. When a current value of DC is increased, a very large magnetic field is generated from a recording head. For this reason, an interaction between a probe used in the MFM and a recording field from the recording head ranges not only to the distal end portion of the probe but also to the rear surface portion of the probe. Additionally, since the interaction at the rear surface portion of the probe includes a magnetic field from the neighborhood of the probe, the interactive effect at the rear surface portion of the probe becomes very large. Hence, contribution from the distal end portion of the probe relatively decreases, resulting in a decrease in resolving power.  
           [0013]    Furthermore, in the computer simulation, the actual field distribution of a recording head cannot be measured.  
         BRIEF SUMMARY OF THE INVENTION  
         [0014]    The present invention provides a magnetic head measuring apparatus capable of realizing direct observation of a saturation field as magnetic field characteristics of a recording head at a high resolving power and consequently improving recording head measurement performance, and a measuring method applied to the magnetic head measuring apparatus.  
           [0015]    According to one aspect of the present invention, there is provided a magnetic head measuring apparatus for executing measurement with respect to at least one measurement point on a recording head, comprising: a probe having a magnetic substance; a vibrator configured to vibrate the probe above the at least one measurement point; a first signal generator configured to supply a drive signal to the vibrator; a second signal generator configured to supply a current containing a direct current (DC) and an alternate current (AC) to the recording head to generate a magnetic field from the recording head; a detector configured to detect a signal corresponding to a force interaction that acts on the probe due to the magnetic field generated from the recording head in accordance with the current supplied by the second signal generator; and a measurement unit configured to measure current dependence of the magnetic field of the recording head from the signal detected by the detector.  
           [0016]    According to another aspect of the present invention, there is provided a measuring method applied to a magnetic head measuring apparatus for executing measurement with respect to at least one measurement point on a recording head, the method comprising: supplying a current containing a direct current (DC) and a alternate current (AC) to the recording head to generate a magnetic field from the recording head; bringing a probe having a magnetic substance close to the recording head while vibrating the probe; detecting a signal corresponding to a force interaction that acts on the probe due to the magnetic field generated from the recording head; and measuring current dependence of the magnetic field of the recording head from the detected signal.  
           [0017]    Additional objects and advantages of the invention will be set forth in the description which follows, and in part will be obvious from the description, or may be learned by practice of the invention. The objects and advantages of the invention may be realized and obtained by means of the instrumentalities and combinations particularly pointed out hereinafter. 
       
    
    
     BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWING  
       [0018]    The accompanying drawings, which are incorporated in and constitute a part of the specification, illustrate embodiments of the invention, and together with the general description given above and the detailed description of the embodiments given below, serve to explain the principles of the invention.  
         [0019]    [0019]FIG. 1 is a block diagram showing main part of a magnetic head measuring apparatus according to an embodiment of the present invention;  
         [0020]    [0020]FIG. 2 is a flow chart for explaining the measurement procedure in the embodiment;  
         [0021]    [0021]FIGS. 3A and 3B are views for explaining derivative of the magnetic field in terms of a DC current obtained in the embodiment;  
         [0022]    [0022]FIGS. 4A and 4B are views showing image data obtained in the embodiment; and  
         [0023]    [0023]FIG. 5 is a view for explaining a modification of the measuring method of the embodiment; and  
         [0024]    [0024]FIG. 6 is a block diagram showing a modification of the magnetic head measuring apparatus shown in FIG. 1. 
     
    
     DETAILED DESCRIPTION OF THE INVENTION  
       [0025]    An embodiment of the present invention will be described below with reference to the accompanying drawing.  
         [0026]    Arrangement of Magnetic Head Measuring Apparatus  
         [0027]    A measuring apparatus of this embodiment is roughly divided into a measuring apparatus main body  1  and computer  20 , as shown in FIG. 1. The measuring apparatus main body  1  is an apparatus dedicated to measure magnetic field characteristics of a recording head (to be sometimes referred to as a sample)  3  using a magnetic force microscope (MFM). The MFM is a kind of scanning probe microscope. The MFM normally brings a probe mounted on a cantilever (leaf spring member) close to a sample to be measured and detects a magnetic field generated from the sample in a non-contact state using a magnetic force interaction (force or force gradient).  
         [0028]    The measuring apparatus main body  1  has a cantilever  2  that supports a probe  10  formed from (or coated with) a magnetic substance, and an actuating piezoelectric element  5  which applies a vibration having a constant vibration amplitude to the cantilever  2 . The actuating piezoelectric element  5  vibrates the cantilever  2  at the mechanical resonance frequency (ωr) of the cantilever  2  or a frequency near the mechanical resonance frequency in accordance with a drive signal from a signal generator  6 .  
         [0029]    On the other hand, a sample, i.e., the recording head  3  to be measured is held by a scanning piezoelectric element  4  which is three-dimensionally driven and controlled along the X-, Y-, and Z-axes. The scanning piezoelectric element  4  has a function of changing the three-dimensional relative position and relative distance between the sample  3  and the probe  10  in accordance with a control signal from a feedback circuit  12  (to be described later).  
         [0030]    The measuring apparatus main body  1  also has a deflection detector  7  for detecting deflection of the cantilever  2  that supports the probe  10 , a phase sensitive detector  8 , a synchronous detector  9 , and an amplitude/DC voltage converter  11 . The phase sensitive detector  8  detects the phase shift between the output signals from the deflection detector  7  and signal generator  6 . The synchronous detector  9  measures an AC (Alternate Current) component from the signal output from the phase sensitive detector  8  (outputs a measurement signal  100 ). That is, the synchronous detector  9  extracts an amplitude component (corresponding to an image of derivative of the magnetic field in terms of a DC current) synchronous with an AC frequency corresponding to the magnetic field of the recording head  3 , which is detected by the force interaction of the probe  10 .  
         [0031]    The amplitude/DC voltage converter  11  converts the amplitude value of the AC signal from the output signal of the deflection detector  7  into a DC (Direct Current) signal  102  and outputs the DC signal  102  to the feedback circuit  12 . The feedback circuit  12  outputs a signal for maintaining the amplitude of the output signal  102  from the amplitude/DC voltage converter  11  constant as a drive control signal  103  for the scanning piezoelectric element  4  and also to the computer  20  as a detection signal  101  of the surface shape (topographical image) of the sample  3 .  
         [0032]    A signal generator  13  corresponds to a circuit having a current source for supplying a signal current  104  for measurement to the coil of the recording head, i.e., sample  3 . The signal current  104  contains DC and AC components. The signal current  104  contains an AC having a very small amplitude (with angular oscillation frequency (ωm)  
         [0033]    The computer  20  controls the entire measuring apparatus main body  1 . The computer  20  also has a function of processing each of the measurement signal  100  corresponding to an image of derivative of the magnetic field in terms of a DC current, which is measured by the measuring apparatus main body  1 , and the measurement signal  101  corresponding to the surface shape (topographical image) of the sample so as to evaluate the measurements. The computer  20  also sets all measurement conditions for the apparatus main body  1  or acquires the operation state. More specifically, the computer  20  sets the time constant of the feedback circuit  12  and the scanning range of the scanning piezoelectric element  4 . The computer  20  also sets operation conditions such as a frequency, amplitude, and offset to generate signal currents from the signal generators  6  and  13 .  
         [0034]    The scanning piezoelectric element  4  is assumed to have a structure fixed with respect to the recording head  3 . However, any other structure capable of changing the relative positions of the probe  10  and recording head  3  can be used.  
         [0035]    Measurement Procedure  
         [0036]    The measurement procedure of this embodiment will be described below with reference to the flow chart shown in FIG. 2 and also FIGS. 3A to  4 B.  
         [0037]    First, the signal current  104  is supplied from the signal generator  13  to the coil of the recording head, i.e., sample  3  (step S 1 ). The signal current  104  contains DC and AC components. The AC has a very small amplitude (with angular oscillation frequency ωm).  
         [0038]    As the amplitude of the AC signal becomes smaller, a signal corresponding to derivative of the magnetic field in terms of a DC current can be more precisely obtained. However, when the detection sensitivity of the MFM is taken into consideration, a certain amplitude is necessary. Since the maximum value of the amplitude of an actual recording head is 30 to 40 mA, the amplitude of the AC is ideally about 3 mA or less.  
         [0039]    However, if the current is too small, an AC component F AC  of measured interaction becomes smaller than noise in the measurement system to make it difficult to execute predetermined measurement. Hence, a current value with which a signal more than the noise level can be obtained must be set. Normally, when noise in circuits of the measurement system is reduced, thermal noise of the cantilever  2  becomes dominant. This noise is defined by statistical thermodynamics and therefore cannot be removed. Hence, measurement must be done while satisfying a condition given by  
         F   AC     &gt;       1   A              4        K   B        TQB       k                   ω   r                                   
 
         [0040]    where A is the vibration amplitude, Q is the Q value, k is the spring constant, and ωr is the and resonance frequency of the cantilever. K B  and T are a Boltzman constant and temperature. B indicates the band width of the measurement system. In the measurement of this embodiment, the band width of the low-pass filter of the synchronous detector  9  is the band B. The actual magnitude of F AC  changes depending on the shape of the probe, or the material, sputtering conditions, and film thickness of the magnetic substance.  
         [0041]    On the other hand, the frequency (ωm) of the AC contained in the signal current  104  must be {fraction (1/10)} the resonance frequency (ωr) of the cantilever  2  or less. The frequency (ωm) is the modulation frequency of the amplitude modulation frequency. The frequency (ωm) is converted into a modulation frequency with phase modulation by the interaction between the probe  10  and the magnetic field, which has a carrier frequency corresponding to the resonance frequency of the cantilever  2 . Hence, it has been confirmed by experiments that the maximum value of the frequency (ωm) depends on the resonance frequency (corresponding to the vibration frequency of the probe  10 ) of the cantilever  2  and cut-off frequency of the low-pass filter which is included in the phase sensitive detector, and sensitive measurement cannot be performed if the frequency (ωm) is not {fraction (1/10)} the resonance frequency (ωr) or less.  
         [0042]    In accordance with supply of the signal current  104 , a magnetic field (recording field) is generated from the gap of the recording head  3 . In this state, when the probe  10  is brought close to the recording head  3 , a force interaction by the magnetic field acts on the probe  10  (step S 2 ).  
         [0043]    On the other hand, to measure the surface shape (topographical image) of the sample  3 , the computer  20  switches measurement operation to receive the measurement signal  101  output from the feedback circuit  12 . That is, the scanning piezoelectric element  4  is controlled to change the three-dimensional relative position and relative distance between the sample  3  and the probe  10  in accordance with a control signal from the feedback circuit  12 .  
         [0044]    The signal generator  6  is caused to supply a signal having the mechanical resonance frequency (ωr) of the cantilever  2  or a frequency near the mechanical resonance frequency to the actuating piezoelectric element  5 . The actuating piezoelectric element  5  vibrates the probe  10  through the cantilever  2 . The probe  10  scans the recording head  3  while making the distal end portion lightly contact (tap) the surface of the recording head  3 .  
         [0045]    The feedback circuit  12  drives and controls the scanning piezoelectric element  4  such that the output signal  102  from the amplitude/DC voltage converter  11  obtains a constant amplitude (such that the distance between the probe and the sample becomes constant). At this time, the feedback circuit  12  outputs the drive control signal to the computer  20  as the detection signal  101  of the surface shape (topographical image) of the recording head  3  (step S 3 ).  
         [0046]    The force interaction acting on the probe  10  is detected by the phase sensitive detector  8  as a phase shift between the vibration of the cantilever  2  measured by the deflection detector  7  and the signal generated by the signal generator  6 .  
         [0047]    The synchronous detector  9  outputs a signal synchronous with the AC (Alternate Current) component of the force interaction (i.e., the magnetic field of the recording head) as the measurement signal  100 . The measurement signal  100  is an amplitude component synchronous with the AC frequency (ωm). The measurement signal  100  corresponds to derivative of the magnetic field in terms of a DC current (dH/dI) obtained by differentiating a magnetic field H generated from the recording head by a current I.  
         [0048]    The computer  20  causes the probe  10  to scan the gap range of the recording head  3 , thereby receiving the measurement signal  100  to measure an image of derivative of the magnetic field in terms of a DC current (step S 4 ).  
         [0049]    It is determined whether a DC current is to be changed (step S 5 ). If yes, the DC current is changed (step S 6 ) and steps S 3  and S 4  are repeated. If no, the processing is terminated.  
         [0050]    In this way, an image of derivative of the magnetic field in terms of a DC current (measurement signal  100 ) as magnetic field characteristics of the recording head  3  and the surface shape (topographical image) of the recording head  3  are measured by the measuring apparatus main body  1  and computer  20 .  
         [0051]    [0051]FIGS. 3A and 3B are views for explaining derivative of the magnetic field in terms of a DC current, obtained in this embodiment.  
         [0052]    The derivative of the magnetic field in terms of a DC current (dH/dI) obtained in this embodiment changes depending on the position (portion) of the recording head (the value has site dependence).  
         [0053]    As shown in FIG. 3A, for magnetic poles P 1  and P 2  of the recording head, for example, measurement of three portions on the magnetic pole P 2  side (gap edge center portion (◯), corner portion (□), and trailing portion (Δ) of the magnetic pole P 2  in FIG. 3A) will be examined. FIG. 3B shows the current dependence of a force gradient by dH/dI (to be referred to as a dH/dI force gradient hereinafter) at the three portions.  
         [0054]    As shown in FIG. 3B, at the gap edge center, since the value dH/dI is becoming constant to about 10 mA, saturation starts at about 10 mA. At the corner portion, since the dH/dI force gradient is uniformly attenuated from a small current, saturation has already started even at a small current value. At the trailing portion of the magnetic pole P 2 , since the dH/dI force gradient is smaller than the remaining two portions, the field strength gradient with respect to the current is small. In addition, since the dH/dI force gradient is flat to about 15 mA, the value dH/dI monotonically increases until 15 mA and then saturation starts. In the measurement according to this embodiment, the saturation phenomenon of the recording head changes depending on the position.  
         [0055]    The computer  20  executes predetermined signal processing for the measurement signal  100  obtained from the measuring apparatus main body  1  to convert an image of derivative of the magnetic field in terms of a DC current, i.e., the measurement result into image data by black contrast, as shown in FIGS. 4A and 4B. When the image data is output and displayed on the screen of a display, the magnetic field characteristics (saturation phenomenon) of the recording head  3  can be directly visually observed.  
         [0056]    [0056]FIG. 4A shows an image of derivative of the magnetic field in terms of a DC current when current value I of the DC of the signal current supplied to the recording head  3  is 3 mA. FIG. 4B shows an image of derivative of the magnetic field in terms of a DC current when current value I of the DC is 20 mA.  
         [0057]    Referring to FIG. 4A, a magnetic field (derivative) distribution (black contrast) can be confirmed along the edge corner of the magnetic poles P 1  and P 2  of the gap of the recording head  3 . Referring to FIG. 4B, it can be confirmed that black contrast around the edge of the magnetic poles P 1  and P 2  disappears, and the magnetic field (derivative) is almost zero, i.e., field saturation occurs at the magnetic pole edge. The computer  20  can calculate a curve of derivative of the magnetic field in terms of a DC current and further calculate a curve of the magnetic field in terms of the DC current from a measurement result obtained by changing the current value of the DC of the signal current  104 , and output the curves onto the display.  
         [0058]    As described above, in this embodiment, an image of derivative of the magnetic field in terms of a DC current and surface shape (topographical image) of the recording head  3  can be measured. Hence, when an image is generated by the computer  20  from the derivative of the magnetic field in terms of a DC current as a measurement result, the magnetic field characteristics (field saturation phenomenon) of the recording head  3  can be visually observed. In addition, when a curve of derivative of the magnetic field in terms of a DC current and then a curve of the magnetic field in terms of the DC current are calculated from a measurement result obtained by changing a current value of the DC, measurement evaluation can be done at a high resolving power.  
         [0059]    &lt;First Modification&gt; 
         [0060]    [0060]FIG. 5 is a view for explaining a modification of the measuring method of this embodiment. FIG. 5 conceptually shows a scanning range  400  of the probe  10  with respect to the recording head  3 , scanning lines  401  (dashed lines), and measurement positions  402  indicated by solid dots.  
         [0061]    In this modification, in the scanning range  400 , the probe  10  is scanned (scanning line  401 ) near the magnetic poles P 1  and P 2  of the recording head  3  (gap  30 ). The scanning is temporarily stopped at the preset measurement position  402 . The computer  20  stores a measurement result (derivative of the magnetic field in terms of a DC current) obtained from the synchronous detector  9  by changing a current value of the DC of the signal current  104  supplied to the recording head  3 , while keeping scanning stopped. The computer  20  analyzes a plurality of measurement results (derivatives of the magnetic field in terms of a CD current) obtained by changing the current value of the DC to calculate a curve of the derivatives of the magnetic field in terms of the DC current. Then the computer  20  calculates a curve of the magnetic field in terms of the DC current from the curve of the derivatives of the magnetic field in terms of the DC current at each predetermined measurement position  402  of the probe  10 .  
         [0062]    According to this modification, since scanning by the probe  10  can be executed simultaneously with changing the current value of the DC, a curve of the magnetic field in terms of a DC current and a curve of the magnetic field in terms of a DC current can be calculated in a short time.  
         [0063]    &lt;Second Modification&gt; 
         [0064]    [0064]FIG. 6 is a block diagram showing a modification of the magnetic head measuring apparatus shown in FIG. 1.  
         [0065]    In the above-described magnetic head measuring apparatus shown in FIG. 1, the phase shift between the signal from the deflection detector  7  and the signal generated by the signal generator  6  is detected using the phase sensitive detector  8 . In the magnetic head measuring apparatus shown in FIG. 6, a frequency demodulator  21  is used to detect the frequency of the signal from the deflection detector  7 , instead of the phase sensitive detector  8 .  
         [0066]    Additionally, the above-described magnetic head measuring apparatus shown in FIG. 1 has the amplitude/DC voltage converter  11 . Instead, a phase shifter  22  and AGC (Automatic Gain Control) circuit  23  are arranged to form a phase control mechanism for frequency detection. In this case, the phase shifter  22  outputs a signal having a phase shift of a predetermined angle with respect to the signal output from the deflection detector  7 . The AGC circuit  23  automatically controls the gain of its output to make the signal output of the deflection detector or the signal to the piezoelectric elements constant. With the constitution, it is possible to appropriately actuate the cantilever  2  with maintaining the phase to be constant. That is, the deflection detector  7 , phase shifter  22 , AGC circuit  23 , actuating piezoelectric element  5 , cantilever  2 , and probe  10  form a positive feedback control system (oscillation system) for phase control.  
         [0067]    In the above arrangement, the synchronous detector  9  measures an AC (Alternate Current) component from the signal output from the frequency demodulator  21  (outputs the measurement signal  100 ). That is, the synchronous detector  9  extracts an amplitude component (corresponding to an image of the magnetic field in terms of a DC current) synchronous with the AC corresponding to the magnetic field of the recording head  3 , which is detected by the force interaction of the probe  10 .  
         [0068]    The output signal from the frequency demodulator  21  is sent not only to the synchronous detector  9  but also to the feedback circuit  12 . Hence, the feedback circuit  12  can generate the signal  103  for driving and controlling the scanning piezoelectric element  4  and the detection signal  101  of the surface shape (topographical image) of the sample  3  by using the output signal from the frequency demodulator  21 , as in the magnetic head measuring apparatus shown in FIG. 1.  
         [0069]    Even in this modification, the same effect as that of the magnetic head measuring apparatus shown in FIG. 1 can be obtained.  
         [0070]    As has been described above in detail, according to the present invention, in a magnetic head measuring apparatus for measuring magnetic field characteristics of a recording head included in a magnetic head using a magnetic force microscope (MFM), when a measured image of the magnetic field in terms of a DC current is converted into an image by predetermined signal processing, a saturation phenomenon of a magnetic field from a magnetic pole edge of the recording head can be visually observed. In addition, by changing the current value to be supplied to the recording head, current dependence of the magnetic field (corresponding to a curve of the magnetic field in terms of a DC current) of the recording head can also be obtained. That is, a saturation field as magnetic field characteristics of a recording head can be directly observed at a high resolving power, and consequently, the recording head measurement performance can be improved.  
         [0071]    Additional advantages and modifications will readily occur to those skilled in the art. Therefore, the invention in its broader aspects is not limited to the specific details and representative embodiments shown and described herein. Accordingly, various modifications may be made without departing from the spirit or scope of the general inventive concept as defined by the appended claims and their equivalents.