MAGNETORESISTANCE EFFECT TYPE MAGNETIC HEAD APPARATUS

Abstract: A magnetoresistance effect type magnetic head appa­ ratus has a magnetoresistance effect sensing element (5), means (3) for applying a bias magnetic field to the sensing element (5), a detecting circuit (81) for obtaining a detecting signal, a low pass filter (32) for deriving an unwanted signal component from the detecting signal, and means for ap­ plying a cancelling magnetic field to the sensing element (5) so as to eliminate the unwanted signal component. An additional sensing element (25) may also be provided to detect an external magnetic field (H N ), and a corresponding signal is generated which is applied to a first sensing element (5) so as to cancel the effects of the external magnetic field (H N ).

Description: The present invention relates to a magnetoresistance effect type magnetic head apparatus. A magnetoresistance effect type (hereinafter referred to as "MR") magnetic head apparatus has a magnetic head element h as shown in Figure 12. On a magnetic substrate 1 of Ni-Zn ferrite or MN-Zn ferrite, or through an insulating layer 2 of SiO₂ or the like on the substrate 1 if it is conductive, a bias conductor 3 is applied which provides a bias magnetic field generated by current passing therethrough to supply a bias magnetic field to a sensing element 5 having the magnetoresistance effect (hereinafter referred to as "MR sensing element") as described below. The bias conductor 3 may be formed by a band-shaped conductive film extending in one direction. An MR sensing element 5 comprising a MR magnetic thin film of Ni-Fe alloys or NI-Co alloys is arranged over the bias conductor 3 on an insulation layer 4. A pair of magnetic layers 7 and 8 of Mo permalloy or the like as a magnetic core of a magnetic circuit are formed so that the magnetic layers 7 and 8 are positioned at each end over the MR sensing element 5 on a thin insulation layer 6, and extend across the bias conductor 3 and the MR sensing element 5. A protective substrate 10 is provided on the substrate 1 through a non-magnetic insulation protective layer 9. A front magnetic gap g is formed between one magnetic layer 7 and the front end of the substrate 1 through a non-magnetic gap spacer layer 11 comprising, for example, the insulation layer 6 having a required thickness. A front surface of the substrate 1, the gap spacer layer 11, the magnetic layer 7, the protective layer 9, and the protective substrate 10 are polished such that a surface 12 including the free end of the magnetic gap g faces a magnetic recording medium (not shown). The rear end of the magnetic layer 7 which forms the magnetic gap g, and the front end of the other magnetic layer 8, are formed to ride on the MR sensing element 5 through the insulation layer 6, and both ends are spaced from each other by a discontinuous portion 13. The rear end of the magnetic layer 7 and the front end of the magnetic layer 8 are electrically insulated by interposition of the insulation layer 6 at both ends of the MR sensing element 5, but are magnetically connected. The discontinuity portion 13 between both magnetic layers 7 and 8 is magnetically connected by the MR sensing element 5, so that a magnetic circuit is formed in a closed magnetic path which, starting from the substrate 1, includes the magnetic gap g - the magnetic layer 7 - the MR sensing element 5 - the magnetic layer 8 - ending again with the substrate 1. In such a MR type magnetic head apparatus, a signal magnetic flux by a signal recorded on the magnetic recording medium flows from the magnetic gap g opposite the magnetic recording medium into the magnetic circuit. Thus a resistance value of the MR sensing element 5 in the magnetic circuit varies in response to the external magnetic field by the signal magnetic flux. Variation of the resistance value is detected as a voltage variation across the MR sensing element 5 and a sensing current i MR flows through the MR sensing element 5. Thus a reproduction of the recording signal on the magnetic recording medium is effected. Figure 13 shows a magnetoresistance characteristic curve of the MR sensing element. It is clear that the magnetoresistance characteristic curve of the MR sensing element 5 becomes a parabolic curve in a certain range of the magnetic field. Consequently, the sensitivity characteristics show a maximum value at two values of the magnetic field as shown in Figure 14. A point of maximum sensitivity becomes also a point of good linearity. Consequently, in such a magnetic head, the bias magnetic field H B is applied with a nearly equal value to that supplying the maximum sensitivity to the MR sensing element 5. The bias magnetic field H B is supplied mainly by the external bias magnetic field H BO by a magnetic field induced by current flowing through the bias conductor 3. In actual practice, however, in addition to the magnetic field H BO , the bias magnetic field H B is supplied also by the magnetic field H MR generated by sensing current i MR flowing internally through the MR sensing element 5. In such an MR type magnetic head apparatus as clearly seen in the schematic diagram of Figure 15, the MR sensing element 5 is supplied with the magnetic field generated while a prescribed d.c. current i BO flows through the bias conductor 3, and at the same time prescribed sensing current i MR flows through the MR sensing element 5. In such a state, the MR sensing element 5 is supplied with the bias magnetic field H B formed of the magnetic field H BO generated by energizing the bias conductor 3 and the magnetic field H MR generated by the sensing current i MR flowing through the MR sensing element 5, the signal magnetic field H S being applied from the magnetic recording medium. A voltage across the MR sensing element 5 on the basis of resistance variation by the signal magnetic field H S , i.e. a variation of potential at point A, is amplified by an amplifier 14 and detected at an output terminal 15. Numeral 16 designates a coupling capacitor. In the MR type magnetic head apparatus as above described, a required bias magnetic field H B is applied to the MR sensing element such that the working point is set to a position with good sensitivity and linearity on the characteristic curve of Fig. 13. However, if the magnetic head element in the MR type magnetic head apparatus is supplied with an undesirable external noise magnetic field H N other than the output magnetic field from the magnetic recording medium, for example a magnetic field generated from a motor or the like (hereinafter referred to as "external magnetic field"), the setting state of the magnetic field for the MR sensing element varies. Thus there is a variation of the sensitivity and linearity which causes generation of distortion and noise in the reproduction signal. In the MR magnetic head element having characteristics as described in Figure 13 and Figure 14, if the external magnetic field H N of H N = 0 (0e), H N = +10 (0e), H N = -10 (0e) is applied to the band-shaped MR sensing element in the width direction, the sensitivity characteristic curves are as shown in Figure 16. In Figure 16, the sensitivity characteristic curve of H N = 0 (0e) does not pass through the origin, because, in addition to the magnetic field generated by current flowing through the bias conductor, i.e. the bias current i BO , the magnetic field H MR by the sensing current i MR flowing through the MR sensing element affects it. In order to diminish the influence, it is known from document US-A-3 969 769 to detect an external magnetic field independently of the data field by using a second magneto resistance element placed away from the data track so as to prevent reading of the data. Compensation of the external magnetic field effects is achieved by subtracting the signal produced by the external field as detected by the second magneto resistance element from the signal generated by the data field reading element. It is also known from document GB-A-2 023 326 to use the signal obtained from the second magneto resistance element as a feed back current to a bias conductor element for the data field reading magneto resistance element. However, the idea of compensating the influence of the external fields as realized according to the said prior art documents does not provide for a sufficiently fast and complete counter-balancing of the undesired external field effects. Accordingly, it is an object of the present invention to provide an MR type magnetic head apparatus in which a shift of the working point of the MR sensing element caused by an external magnetic field influence can be completely avoided even under varying temperature conditions, for example due to changing frictional conditions between the magnetic recording medium and the magnetic head device. According to the invention, a magneto resistance effect type magnetic head device comprised a magnetic head element including a main magneto resistance effect sensing element and a bias conductor supplied with a bias current for applying a bias magnetic field to said main sensing element for reproducing a recording signal on a magnetic recording medium adjacent the magnetic head element and detecting means with an additional magnetic head element having a further magneto resistance effect sensing element for detecting an external magnetic field which effects said magnetic head element, and the invention is characterized by additional bias conductor means for applying a bias magnetic field to said sensing element of the additional magnetic head element and for producing a signal corresponding to said external magnetic field effecting the magnectic head element but substantially not responsive to a signal magnetic field caused by the recording signal on the magnetic recording medium, and negative feed back loop means for applying said sensing element bias conductor means with a superimposed correcting current so as to substantially eliminate the external magnetic field effects on said magnetic head element. Advantageous details and improvements of the invention as defined above are the subject of dependent claims and will be explained below with reference to the accompanying drawings of which Figure 1 is a diagram illustrating an MR type magnetic head apparatus in a first embodiment of the invention; Figure 2 is a block diagram illustrating means for applying a bias magnetic field and an example of an output circuit; Figure 3 is a diagram of an MR characteristic curve illustrating operation of the MR type magnetic head apparatus of the invention; Figure 4 is a waveform chart illustrating operation of the MR type magnetic head apparatus of the invention; Figure 5 is a block diagram illustrating means for applying a bias magnetic field and an output circuit as employed in a second embodiment of the invention further described in Figure 7; Figure 6 is a diagram of an MR characteristic curve illustrating the operation of the magnetic head apparatus in Figure 5; Figure 7 is a diagram illustrating an MR type magnetic head apparatus in a second embodiment of the invention; Figure 8 is a diagram illustrating an MR type magnetic head apparatus in a third embodiment of the invention; Figure 9 is a diagram illustrating an MR type magnetic head apparatus in a fourth embodiment of the invention; Figure 10 is a schematic enlarged sectional view of a magnetic head element for detecting an external field; Figure 11 is a diagram illustrating an MR type magnetic head apparatus in a fifth embodiment of the invention; Figure 12 is a schematic enlarged sectional view of an example of an MR magnetic head element; Figure 13 is a diagram of a working characteristic curve of the magnetic head element in Figure 12; Figure 14 is a diagram of a sensitivity characteristic curve of the magnetic head element in Figure 12; Figure 15 is a block diagram illustrating a magnetic head apparatus of the prior art; and Figure 16 is a diagram of a sensitivity characteristic curve of the magnetic head apparatus in Figure 15. DESCRIPTION OF THE PREFERRED EMBODIMENTS An MR type magnetic head apparatus, in a first embodiment of the invention, will now be described by referring to Figure 1. In the embodiment, a magnetic recording medium has a plurality of data tracks thereon, and a multi-track magnetic head element unit 18 for reproducing data tracks is installed and formed of an arrangement of a plurality of MR magnetic head elements h to reproduce a signal magnetic field, i.e. a recording signal corresponding to the plurality of data tracks on the magnetic recording medium. Each magnetic head element h may be formed as already described with reference to Figure 12, but with common substrates 1 and 10. A bias conductor 3 for each element h of the magnetic head element unit 18 for reproducing data tracks formed by a band-shaped conductive film extending and crossing all MR sensing elements 5 of all head elements h is provided on the substrate 1. In Figure 1, reference numeral 17 designates drive sources in general already described in Figure 15, including a current source to obtain sensing current i MR for an MR sensing element 5 also referred as the "main sensing element", a circuit for taking the reproduction output from the sensing element, i.e. a capacitor 16 accompanying each magnetic head element h, and an amplifier 14. Particularly in the invention, an external magnetic field detecting means 20 is installed at a position which is near the reproduction magnetic head element unit 18 having MR magnetic head elements h adjacent the magnetic recording medium. The external magnetic field detecting means 20 may be formed of a pair of additional MR magnetic head elements h S1 and h S2 for detecting an external magnetic field. They are similar in construction and characteristics to the main magnetic head elements h of the reproduction magnetic head element unit 18. These additional magnetic head elements h S1 and h S2 may be formed as a magnetic head element unit H and interposed between the magnetic substrate 1 and the protective substrate 10, as already described in connection with Figure 12. The detecting means 20 is installed as close as possible to the reproduction magnetic head element unit 18 so as to obtain the same external magnetic field H N but at a position which is not adjacent to the magnetic recording medium facing the magnetic head element unit 18 as above described. Numeral 25 designates an MR sensing element for each of the additional elements h S1 and h S2 corresponding to the MR sensing element 5 for the magnetic head element h. Numeral 23 designates schematically a bias conductor which is formed along an entire lower side of the sensing elements 25 for applying the bias magnetic field to the sensing elements 25 in common fashion, and corresponds to the bias conductor 3 formed in common fashion in the magnetic head unit 18. Each of the additional sensing MR magnetic head elements h S1 and h S2 is grounded at one end and connected at the other end to one input each of a differential amplifier 21. Both inputs of the differential amplifier 21 are connected to a common power source V S and the MR sensing elements 25 of the head elements h S1 and h S2 are supplied with sensing currents i S1 , i S2 in reverse directions to each other with respect to the common external magnetic field to be detected. An output of the differential amplifier 21 is connected to a current driver 22, and a required current i E obtained from the current driver 22 is superimposed on the bias current i BO leading to the bias conductor 3 of the reproduction magnetic head element 18. Thus this superposition current is supplied to the bias conductor 3. A part of the output of the differential amplifier 21 is supplied to a current driver 24, and the output current from the current driver 24 is supplied to the bias conductor 23. In this construction, when the external magnetic field H N is not applied, but each MR sensing element 5 of the magnetic head element unit 18 for reproducing data tracks is supplied with a required sensing current i MR , the bias current i BO to apply the d.c. bias magnetic field from the bias conductor 3 to each sensing element 5 is set so that the optimum sensitivity and linearity can be obtained. When an external magnetic field does not influence the detecting means 20, the MR sensing elements 25 of the head elements h S1 and h S2 are supplied with the prescribed detecting currents i S1 and i S2 , respectively by the power source V S , and the bias magnetic field is set so that a high sensitivity is obtained in each sensing element 25 itself by the magnetic field generated by flowing of the detecting current. Also in this construction, when an external magnetic field H N does not exist, the output from the differential amplifier 21 is set to zero so that an output current is not obtained from the differential amplifier 21, and only the prescribed bias current i BO as above described is supplied to the bias conductor 3 of the reproduction magnetic head element unit 18. The prescribed sensitivity is thus obtained. If a common external magnetic field H N is applied to the reproduction magnetic head element unit 18 and the detecting means 20 in this state, an output from the differential amplifier 21 is obtained by an output signal from each of the head elements h S1 and h S2 of the detecting means 20. The output from the differential amplifier 21 is supplied to the current driver 22, and a cancellation current i E for cancelling the influence of the external magnetic field H N is obtained from the current driver 22. More specifically, the cancellation current i E is superimposed on the bias current i BO as above described, and is supplied to the bias conductor 3 of the magnetic head element unit 18 for reproducing data tracks. Thus, a variation of the magnetic field applied to each MR sensing element 5 of each magnetic head element h caused by the external magnetic field H N can be cancelled. A part of the output from the differential amplifier 21 is introduced to the current driver 24, and a current obtained from the current driver 24 is supplied to the bias conductor 23 of the detecting means 20. Thus, an influence of the external magnetic field H N with respect to each sensing element 25 of the detecting means can be cancelled. Although a d.c. bias magnetic field is applied to each of the MR magnetic head elements h, h S1 , h S2 in the embodiment shown in Figure 1, an a.c. bias magnetic field may be superimposed on the d.c. bias magnetic field as applied to the MR magnetic head element, or an a.c. bias magnetic field may be applied to the head element. When a a.c. bias magnetic field or an a.c. bias magnetic field superimposed on the d.c. field is applied to the MR sensing element, a reduction of temperature dependence of the MR magnetic head element, an improvement of the linearity, and a decrease of the distortion results. This feature will be described in detail first. A design wherein the a.c. bias magnetic field or an a.c. field is superimposed on the d.c. field, and wherein these fields are applied to the MR sensing element, has been already proposed in the not prepublished document EP-A-0 154 307. The influence on the working characteristics of the MR sensing element 5 will be considered again with reference to Figure 13. The prescribed bias magnetic field H B is applied to the MR sensing element as above described, and the signal magnetic field shown by numeral 26 in Figure 13 is applied from the magnetic recording medium. Corresponding to the signal magnetic field, an output according to a variation of the resistance value as shown by numeral 27 in Figure 13 is obtained. In this case, however, an increasing signal magnetic field results in an increase of the second harmonic distortion. In the MR type magnetic head apparatus, a potential at point A of Figure 15 is determined by a combination of a fixed component and a variable component of the resistance in the MR sensing elements 5, 25. Since the fixed component in this case is about 98% and is largely dependent on temperature, the temperature drift of the potential at point A becomes large. The resistance value R in the MR sensing element is represented by the following formula. R = R₀ (1 + α cos² ϑ) (1) wherein R₀ stands for the fixed component of resistance, α represents the maximum resistance variation factor, and ϑ indicates the angle between the current direction and the magnetizing direction in the MR sensing element. For example, if the MR sensing element is an MR magnetic thin film of 81 Ni - 19 Fe alloy (permalloy) with a thickness of 25 nm, the measured value of α becomes about α = 0.017. The value of α in this case is dependent more or less on the thickness or the material of the MR magnetic thin film of the MR sensing element, and becomes about α = 0.05 at most. On the other hand, R₀ is represented by the following formula: R₀ = Ri (1 + a Δ t ) , (2) wherein Ri stands for the initial value of resistance, a stands for the termperature coefficient, and Δ t stands for the temperature variable component. The measured value of the temperature coefficient a in the above example of the MR sensing element is about a = 0.0027/deg. This may produce a large noise while detecting the d.c. magnetic field. Moreover, in such an MR type magnetic head element, since the temperature coefficient is large as described above, for example when heat generated by energizing the MR sensing element or by the bias current flowing through the bias conductors 3, 23 is radiated, or if the MR sensing element is transferred in an unstable condition such as by friction between the head element and the magnetic recording medium, the head temperature varies, and a large noise, a so-called rubbing noise, may be produced. If the amplifier 14 in Fig. 15 has a low-impedance input, assuming that the cut-off frequency by the capacitor 16 is fo, the required capacitance C for the capacitor 16 becomes wherein ω o = 2 πfo. If the MR sensing element is made of permalloy with a thickness of 25 nm and a length of 50 µm, the resistance value R becomes about 120 Ω. If fo as 1kHz, the value of C must be as large as C - 1.3 µF. This becomes a problem particularly for a multi-track magnetic head. The permeability in the magnetic circuit, particularly that in the magnetic layers 7 and 8 having a relatively small thickness and sectional area, is preferably as large as possible. Since the permeability becomes a maximum when the external magnetic field is zero, the application of the above-mentioned bias magnetic field lowers the permeability. The above-mentioned disadvantages can be eliminated or improved by the system as hereinafter described. As shown in Figure 2, a small a.c. bias current i A of high frequency fc superimposed on the d.c. bias current i BO flows through a bias conductor 3, 23 of a head element h. Thus, a high frequency magnetic field is applied to an MR sensing element 5, 25. In this case, the waveform of the a.c. bias current i A and hence the waveform of the a.c. magnetic field may be sinusoidal or rectangular. Thus, the MR sensing element is supplied with a a.c. bias magnetic field superimposed on a d.c. bias magnetic field. Accordingly, an a.c. signal of the frequency fc is obtained across the MR sensing element, i.e. at point A in Figure 2. Figure 3A shows the operation when the d.c. bias magnetic field H B is a summation of the external d.c. bias magnetic field H BO applied to the MR sensing element from outside by the d.c. bias current i BO flowing through the bias conductor, and the self bias magnetic field H MR generated by the sensing current to the MR sensing element. The signal magnetic field H S and the a.c. bias magnetic field H A of the a.c. current i A are superimposed. If a variation Δ H of the a.c. bias magnetic field H A is small, the amount of resistance variation ΔR to the variation of the a.c. bias magnetic field at a given point in time is obtained as an absolute value of the differential of a curve in Figure 3A. Since this is the differential of a parabolic curve, the resistance variation in response to the amount of the total d.c. bias magnetic field H B and the signal magnetic fields H S becomes linear in principle as shown in Figure 3B. Consequently, the amount of the a.c. signal obtained at the point A in Figure 2 becomes an output which varies in correspondence with a sum of the total d.c. bias magnetic field H B and the signal magnetic field from the magnetic recording medium. As shown in Figure 2, the output at the point A passes through a high pass filter 30 to select the above-mentioned frequency component fc, and is rectified by a rectifier 31 and then passes through a low pass filter 32. Thus, an output is received corresponding to the signal magnetic field from the magnetic recording medium. If the final output obtained at an output terminal 15 must have the frequency band 0 -100 kHz, the frequency fc of the a.c. current i A may be made much higher than the frequency band, for example fc = 1 MHz In this case, the low cutoff frequency of the high pass filter 30 is selected higher than 100 kHz and lower than fc = 1 MHz, for example at 500 kHz. An output from the high pass filter 30 is rectified by the rectifier 31 and then passes through the low pass filter 32 with the cutoff frequency of 100 kHz as already described. Thus a signal of the frequency band 0 - 100 kHz is obtained. In the magnetic head apparatus of such a construction, if the magnetic field (signal magnetic field H S + total d.c. bias magnetic field H B ) shown in Figure 4A is applied to the MR sensing element, the output shown in Figure 4B, wherein the carrier of frequency fc is amplitude-modulated by the signal, is obtained at point B in Figure 2. An output corresponding to the signal magnetic field H S as shown in Figure 4C is obtained at the output terminal 15. In the magnetic head apparatus of the invention, since linear operation characteristics of the MR sensing element corresponding to the differential of the original operation characteristic curve are employed, a distortionless reproduction signal can be obtained. Even if the fixed component of resistance of the MR sensing element is largely dependent on temperature, the operation according to the differential of the operating characteristic curve of the MR sensing element in this construction can eliminate the influence of the temperature dependence of the fixed component and reduce the temperature drift significantly. Since the temperature dependence of the fixed component of resistance of the MR sensing element is eliminated as above described, noise influences caused by rubbing with the magnetic recording medium can be improved. Furthermore, since only the frequency fc has to pass the capacitor 16, if fc is 500 kHz for example, the capacitance C of the capacitor 16 may be C = 1600 pF. If fc is further increased, the capacitance C may be further reduced. Figure 5 is a construction diagram of an MR type magnetic head apparatus a.c. bias, as a second embodiment of the invention. Parts in Figure 5 corresponding to Figure 2 are designated by the same reference numerals and the repeated description shall be omitted. In this case, a bias conductor 3, 23 is not supplied with a d.c. bias current, but rather with an a.c. bias current i A only. Figure 6 shows the operation schematically. In Figure 6, the real R-H operation characteristic curve is shown by a solid line 61, an extrapolation of a parabolic curve portion of the characteristics is shown by broken lines, and the magnetic field indicating the minimum resistance value Rmin in the extrapolation becomes +Ho and -Ho. As shown in Figure 6, an a.c. bias magnetic field H A is superimposed on the signal magnetic field H S . A resistance variation of an MR sensing element in response to the a.c. bias magnetic field is obtained, corresponding to the polarity and the intensity of the signal magnetic field. In this case, the MR operation characteristic curve is a parabolic curve, and the resistance value R MR of the MR sensing element is represented as follows: where ΔRmax = Rmax - Rmin. The magnetic field H applied to the MR sensing element is represented by the sum of the bias magnetic field H A (t) and the signal magnetic field H S (t) as follows: H(t) = H A (t) + H S (t) (5) where H A (t) is generated by the bias conductor 3, 23 and set to H(t) = H A · sin(ω C · t) , and (6) where ω C = 2 πfc . (7) If the MR detecting current is represented by i MR , the output V(t) of the MR sensing element becomes V(t) = i MR R MR . (8) From the above formulas (4), (5), and (6), it follows that Next, the V(t) and a signal having the same phase and frequency as that of the a.c. bias magnetic field H A , e.g. sin (ω t), are multiplied by a multiplier 52. The multiplication output Vz(t) becomes Then the output Vz passes through a low pass filter 32, and the terms having an ω component in formula (10) are eliminated. It follows therefore that Consequently, the output voltage Vo(t) obtained at a terminal 15 becomes Thus, a voltage proportional to the signal magnetic field H S (t) is obtained. Even if a signal magnetic field component H S (t) is contained in the input to the multiplier 52, it does not appear in the output in this case. Consequently, the high pass filter 30 is not necessarily required. According to the above construction, an output corresponding to the polarity of the external magnetic field can be obtained. In addition to the advantages similar to those in the embodiment of Figure 2, the circuit arrangement of Fig. 5 is advantageous since the dynamic range becomes large. Furthermore, in this case if the magnetic bias is an a.c. component only, a decrease of permeability of the magnetic circuit caused by the d.c. bias can be avoided. Figure 7 shows an embodiment of the invention wherein the a.c. bias system described with reference to Figure 5 is adopted as an external magnetic field detecting means 20. In this case, the differential connection of a pair of MR magnetic head elements as shown in Figure 1 is not adopted as the MR magnetic head element for detecting the external magnetic field. Rather, only one MR magnetic head element hs is employed. Parts in Figure 7 corresponding to that in Figure 1 and Figure 2 are designated by the same reference numerals, and a redundant description shall be omitted. In Figure 7, a differential amplifier 70 is installed at the output side of the external magnetic field detecting means 20, and is set so that a required bias current i BO is supplied to bias conductors 3 and 23 for MR magnetic head elements h and hs in a magnetic head element unit 18 for data tracks and the external magnetic head detecting means 20, when an external magnetic field H N is not applied, by adjusting an offset means 71. Numeral 72 designates an adder, and a part of the output current from the differential amplifier 70 is added to the a.c. bias current from an a.c. bias source 73 at the adder 72, and is then supplied to the bias conductor 23. Numerals 74 and 75 designate resistors installed on current supply passages for the bias conductors 3 and 23, and the output from the differential amplifier 70 is set to the prescribed ratio by these resistors. When an external magnetic field H N is effective, the output corresponding to the external magnetic field is taken from the magnetic head element hs of the detecting means 20, and an output current corresponding to the variation of the external magnetic field H N is obtained from the differential amplifier 70. This output current is supplied to the bias conductor 3 of the reproduction magnetic head element unit 18 for data tracks, and at the same time it is supplied, i.e. fed back, to the bias conductor 23 of the magnetic head element hs of the detecting means 20. Thus, a variation of the substantial bias magnetic field to the bias conductors 3 and 23 of the magnetic head elements h and hs caused by the external magnetic head element H N can be cancelled. In the embodiment of Figure 7, an output from the differential amplifier 70 is fed back to the magnetic head element hs for detecting the external magnetic field. However, if the differential amplifier 70 is provided in itself with a gain adjusting means 76 based on its own output as shown in Figure 8, the feedback path for the head element hs may be omitted. Parts in Figure 8 corresponding to that in Figure 7 are designated by the same reference numerals. Figure 9 shows still another embodiment of the invention. Parts in Figure 9 corresponding to that in Figure 7 are designated by the same reference numerals. In this case the magnetic head element hs for detecting the external magnetic field of an external magnetic field detecting means 20, in addition to a bias conductor 23a for applying an a.c. bias magnetic field to an MR sensing element 25, a bias conductor 23b extending from a bias conductor 3 in a magnetic head element h for reproducing data tracks is provided. Thus, the bias variation to the MR sensing element 25 caused by the external field H N can be cancelled. Accordingly, the feedback circuit for the magnetic head element hs may be omitted in a manner similar to Figure 8. In the magnetic head element hs for detecting the external magnetic field, in this case, the bias conductors 23a and 23b are arranged across the MR sensing element 25 and the magnetic layer 8 to construct the magnetic circuit for the head element hs as shown in Figure 10. Parts in Figure 10 corresponding to that in Figure 12 are designated by the same reference numerals. Figure 11 is a diagram illustrating the construction of another embodiment of the invention. In this embodiment, an a.c. bias magnetic field is applied also to an MR magnetic head element h of each track of a magnetic head element unit 18 for reproducing data tracks. Parts in Figure 11 corresponding to that in Figure 7 are designated by the same reference numerals. In Figure 11, numeral 77 designates an output circuit corresponding to each of the MR magnetic head elements h and hs. A bias conductor 23 of the magnetic head element hs for detecting the external field extends from a bias conductor 3 of the magnetic head element unit 18 for reproducing data tracks, and both are connected electrically in common. The reproduction signal may be an audio/video/data signal in an analog/digital system. According to the present invention as above described, the external magnetic field detecting means 20 is installed near the magnetic head element 18 for reproducing data tracks at substantially the same condition as that of the magnetic head element 18 so as to receive the unrequired external magnetic field H N . Since the amount of current to the bias conductor 3 of the magnetic head element 18 for reproducing data tracks is controlled, and a variation of a bias state of each magnetic field caused by the unneeded magnetic field H N is eliminated, the magnetic head apparatus can be always operated at a stable state with the best sensitivity and linearity.

Claims: A magnetoresistance effect type magnetic head device comprising: a magnetic head element (h) including a main magnetoresistance effect sensing element (5) and a bias conductor (3) supplied with a bias current for applying a bias magnetic field to said main sensing element (5) for reproducing a recording signal on a magnetic recording medium adjacent the magnetic head element (h); and detecting means (20) with an additional magnetic head element (h S ) having a further magnetoresistance effect sensing element (25) for detecting an external magnetic field (H N ) which effects said magnetic head element (h), characterized by additional bias conductor means (23; 23a) for applying a bias magnetic field to said sensing element (25) of the additional magnetic head element (h S ) and for producing a signal corresponding to said external magnetic field (H N ) effecting the magnetic head element (h) but substantially not responsive to a signal magnetic field caused by the recording signal on the magnetic recording medium; and negative feed back loop means for supplying said sensing element bias conductor means (3) with a superimposed correcting current (i E ) so as to substantially eliminate the external magnetic field effects on said magnetic head element (h). The magnetic head device according to claim 1, characterized in that means are provided for connecting an output of the detecting means (20) so as to control the current in said bias conductor means (3) and thus control the bias magnetic field, and said additional bias conductor means (23; 23a) of said further detecting element (h S ) is supplied by said negative feed back loop means with an adapted corresponding compensating current for eliminating the external magnetic field effects on said magnetic head element (h). The magnetic head device according to claim 2, characterized in that said negative feed back loop means comprises means for extracting a relatively low frequency current signal component corresponding to said external magnetic field (H N ) and generating the correction signal current (i E ) therefrom which is superimposed on the current (i Bo ) flowing in said bias conductor means (3) and also flowing correspondingly adapted in said additional bias conductor means (23). The magnetic head device according to claim 3, characterized in that said additional magnetic head element (h S ) comprises first and second magnetoresistance effect sensing elements (25). The magnetic head device according to claim 4, characterized in that a diffential amplifier (21) having first and second inputs, respectively is connected to the respective first and second sensing elements (25), and in that an output of said differential amplifier (21) connects through an amplifier (24) to supply said compensating bias current to said additional bias conductor means (23) common to said additional first and second magnetic head elements (hs1, hs2) and also connects through a further amplifier (22) to supply said correcting bias current (i E ) superimposed on said bias current (i Bo ) feeding the bias conductor means (30) of said magnetic head element (h). The magnetic head device according to claim 2, characterized in that the additional sensing element (25) of said detecting means (20) is positioned to detect the external magnetic field (H N ) at a distance sufficient to prevent substantial influencing by a signal magnetic field created by said recording signal. The magnetic head device according to claim 1, characterized by an AC bias source (73) connected to the bias conductor means (23) of the additional magnetic head element (h S ); a multiplier (52) having a first input connected to an additional head element AC bias source (73) and a second input connected to the additional magnetic head sensing element (25); an output of the multiplier (52) connecting to a low pass filter (32) for deriving a current signal (i E ) corresponding to said external magnetic field (H N ); and means for combining the external magnetic field current signal (i E ) with said bias current (i Bo ) and providing an output bias to said bias conductor means (3) of said magnetic head element (h). The magnetic head device according to claim 7, characterized by an adder means (72) having an output connected to the bias source means (23) for the additional magnetic head element (hs), a first input of which is connected to the AC bias source (73) and a second input of which is connected to an output of a differential amplifier (70), the differential amplifier (70) having its first input connected to said low pass filter (32) and a second input connected to an adjustable voltage source (71). The magnetic head device according to claim 7, characterized in that the input of said means for combining the external magnetic field current (i E ) with said bias current (i Bo ) is connected to the output of said differential amplifier (70). The magnetic head device according to claim 2, characterized in that said bias conductor means (3, 23b) is common to and running adjacent both the main sensing element (5) and the further sensing element (25); said additional bias conductor means (23a) is also running adjacent the further sensing element (25); an output of the further sensing element (25) is connected to a first input of a multiplier (52), a second input of the multiplier (52) being connected to an AC bias source (73) which also connects to the additional bias conductor means (23a); an output of the amplifier (52) is connected through a low pass filter (32) for deriving an output signal indicative of the external field (H N ); and in that means (70) are provided for connecting an output of the low pass filter (32) together with a DC bias source (71) to the common bias conductor means (3, 23b). The magnetic head device according to claim 2, characterized in that said bias conductor means (3, 23) is common to and for applying a bias magnetic field to both the main and the further sensing elements (5, 25); a first output circuit (77) is connected with its input to the first sensing element (5) and a second output circuit (77) is connected with its input to the second sensing element (25); an output of the second output circuit (77) is connected through a combining means (70) for combining the output thereof with a DC bias offset (71), an output of the combining means (70) is coupled to a first input of an adder (72), a second input of the adder (72) being connected to an AC bias source (73); and in that an output of the adder (72) is connected to the common bias conductor means (3, 23).

Inventors: FUKUYAMA, MUNEKATSU, IMAKOSHI, SHIGEYOSHI, SOUDA, YUTAKA, SUYAMA, HIDEO
Applicants: SONY CORPORATION
Application year: 1985
Main classification: G11B5
IPC codes: G11B5