MAGNETO-OPTICAL INFORMATION REPRODUCING APPARATUS

Abstract: In a magneto-optical information reproducing apparatus in which polarised light is projected from a source (21) onto a magneto-optical recording medium (26) and the reflected light is transmitted via a polarisation analyser (27) to a detector (29), the principal axis of the analyser is set at an angle other than 45 degrees to the initial polarisation direction and in particular is set at an angle to maximise the signal to noise ratio of the detector output.

Description: BACKGROUND OF THE INVENTION Field of the Invention The present invention relates to a magneto-optical information reproducing apparatus for reproducing information magnetically recorded on a recording medium by the utilization of the magneto-optical effect. Description of the Related Art In recent years, optical memories for effecting recording and reproduction by a laser beam have been actively studied and developed for practical use as high-density recording memories. Of these, magneto-optical disks capable of erasing and re-writing have been regarded as promissing with optical disks exclusively for reproduction typified by compact disks and direct read after write (DRAW) type optical disks. Magneto-optical disks are such that information is magnetically recorded by the utilization of the localized temperature rise of a magnetic thin film caused by the application of a laser spot thereto and the information is reproduced by the magneto-optical effect (particularly the Kerr effect). The Kerr effect refers to the phenomenon that the plane of polarization is rotated when light is reflected by a magnetic recording medium. The basic construction of a magneto-optical disk apparatus according to the prior art is shown in Figure 1 of the accompanying drawings. In Figure 1, the reference numeral 1 designates a semiconductor laser, the reference numeral 2 denotes a collimator lens, the reference numeral 11 designates a half-mirror, the reference numeral 4 denotes an objective lens, the reference numeral 6 designates a magneto-optical recording medium, the reference numeral 7 denotes an analyzer, the reference numeral 8 designates a condensing lens, and the reference numeral 9 denotes a photodetector. The direction of P-polarization is parallel to the plane of the drawing sheet, and the direction of S-polarization is perpendicular to the plane of the drawing sheet. Description will now be made of a case where magneto-optical information is reproduced in such apparatus. A light beam emitted from the semiconductor laser 1 as a rectilinearly polarized light in the direction of P-polarization is collimated by the collimator lens 2 and passes through the half-mirror 11. If the P-polarized component amplitude transmittance is tp and the S-polarized component amplitude transmittance is ts, |tp|²=|ts|²=0.5 in the half mirror 11. The light beam is imaged as a minute spot on the magneto-optical recording medium 6 by the objective lens 4. Where a magnetic section (pit) is pre-formed on the medium 6, as shown in Figure 2 of the accompanying drawings, the reflected light from the medium 6 is subjected to the rotation of the plane of polarization of ±ϑk by the Kerr effect in conformity with whether the direction of magnetization of the spot-applied area is upward or downward. Here, if the P-polarized component of the amplitude reflectance of the recording medium 6 is R and the S-polarized component is K, the following equation is established: The magneto-optically modulated reflected light is again collimated by the objective lens 4 and reflected by the half-mirror 11, whereafter it is converted to a light beam intensity-modulated by the analyzer 7. That is, in Figure 2, the reflected light is analyzed as a regular projection of the amplitude thereof onto the optic axis of the analyzer and therefore, if the intensity of the incident light onto the magneto-optical medium is I O and the angle of the optic axis of the analyzer with respect to the direction of P-polarization is ϑA, the intensities I + ϑk and I - ϑk of the light beams transmitted through the analyzer in conformity with the Kerr rotation angles ±ϑk can be expressed as follows: Since ϑk ∼ 1°, |R|² » |K|² is established and thus, equation (2) can be expressed as follows: In expression (3), the second term in the parentheses is the magneto-optical modulated component and the first term in the parentheses is the non-modulated component, and the intensities thereof are defined as I K and I R , respectively. Such a detection light beam is detected as a magneto-optical signal by the photodetector 9 via the condensing lens 8. Considering that the rotation angle ϑk of the plane of polarization by the Kerr effect is generally of the order of 1° and that the magneto-optical modulated component obtained through the analyzer 7 is of a very minute amount, it is necessary that the azimuth angle ϑA of the optic axis of the analyzer be set to such an optimum position that the C/N (the ratio between the carrier wave and the noise) of the detection signal becomes maximum. For example, in U.S. Patent No. 4,569,035 issued on February 4, 1986, there is shown an example of an apparatus using as a photodetector an avalanche photodiode (APD) or the like having a multiplying action wherein the azimuth of the transmission axis (the optic axis) of the analyzer is optimized. On the other hand, in an apparatus using as a photo-detector a PIN photodiode or the like having no multiplying action, the azimuth angle ϑA of the optical axis of the analyzer has been set to 45° with respect to the direction of polarization of the incident light beam in order to maximize the magneto-optical modulated component intensity expressed by expression (4). However, when the noise superposed on the detection signal is taken into consideration, maximum C/N cannot always be obtained by providing ϑA = 45°. On the other hand, a magneto-optical information reproducing apparatus using a polarizing beam splitter instead of the half-mirror 11 shown in Figure 1 to improve the C/N of the above-mentioned reproducing signal is proposed in U.S. Patent No. 4,561,032 issued on December 24, 1985. Further, an example in which the polarizing characteristic of this polarizing beam splitter is set so that C/N is maximum is disclosed in U.S. Patent No. 4,558,440 issued on December 10, 1985. However, in these examples as well, the azimuth angle of the optic axis of the analyzer is defined as 45°, and no mention is made of optimizing this azimuth angle and a specific method therefor. SUMMARY OF THE INVENTION It is the object of the present invention to further improve the above-described prior art and to provide a magneto-optical information reproducing apparatus which is simple in construction and capable of reproducing magneto-optical signals good in C/N enabling the use of an inexpensive photodetector such as a PIN photo-diode having no amplifying action. The above object of the present invention is achieved by constructing a magneto-optical information reproducing apparatus according to the appended claims. BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 schematically shows an example of a magneto-optical information reproducing apparatus according to the prior art. Figure 2 illustrates the principle of the general magneto-optical signal detection. Figure 3 schematically shows an optical system according to an embodiment of the present invention. Figure 4 schematically shows a signal processing system in the embodiment shown in Figure 3. Figure 5 shows the polarized state of the reflected light from a magneto-optical recording medium. Figures 6 and 7 are graphs showing the relation between the azimuth angle of the optic axis of an analyzer in the embodiment shown in Figure 3 and C/N. Figures 8A - 11 schematically show further embodiments of the present invention. Figures 12 and 13 are graphs showing the relation between the azimuth of the optic axis of an analyzer in an embodiment using a polarizing beam splitter and C/N and the relation between the polarizing characteristic of the polarizing beam splitter and C/N, respectively. Figures 14A and 14B schematically show still another embodiment of the present invention. DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will hereinafter be described in detail with reference to the drawings. Figures 3 and 4 show a first embodiment of a magneto-optical information reproducing apparatus according to the present invention, and more particularly, Figure 3 schematically shows the construction of an optical system and Figure 4 schematically shows the construction of a signal processing circuit. In Figure 3, the reference numeral 21 designates a semiconductor laser, the reference numeral 22 denotes a collimator lens, the reference numeral 23 designates a half-mirror, the reference numeral 24 denotes an objective lens, the reference numeral 26 designates a magneto-optical recording medium, the reference numeral 27 denotes an analyzer, the reference numeral 28 designates a condensing lens, and the reference numeral 29 denotes a photodetector. The direction of P-polarization is parallel to the plane of the drawing sheet, and the direction of S-polarization is perpendicular to the plane of the drawing sheet. The reference numeral 13 designates a light beam transmitted through the analyzer 27. This detection light beam 13 is photoelectrically converted by the photodetector 29 as shown in Figure 4, is voltage-amplified by an amplifier 15 including a load resistor 16 and is output as a reproduction signal from a terminal 14. The half-mirror 23 has the beam shaping function, whereby the light beam of the semiconductor laser 21 having an elliptical far field image can be efficiently imaged as a circular spot on the recording medium 26. A surface a is inclined by a predetermined angle so that no stray light enters the photodetector 29. On the recording medium 26, tracking grooves (not shown) are formed in a direction perpendicular to the plane of the drawing sheet, and the light condensed on the recording medium 26 by the objective lens 24 is diffracted by these grooves. The reference numeral 25 designates a photodetector for detecting the unbalance of ±1st-order diffracted lights caused by track deviation. The photodetector 25 is fixed to the marginal edge of an opening in the objective lens 24. Therefore, there is an advantage that no offset is caused in the tracking error signal even if the objective lens 24 is moved in a direction perpendicular to the track grooves. The photodetector 29 is a photodetector having no amplifying action, such as an Si-PIN photodiode, and effects the detection of a magneto-optical signal and a focus error signal. A conventional method is used for the detection of the focus error, but it has no direct relation with the present invention and therefore need not be described in detail. In the above-described apparatus, the semi-conductor laser 21 emits a P-polarized light beam. This emitted light beam is collimated by the collimator lens 22, is transmitted through the half-mirror 23 and is applied as a light spot of intensity I O onto the recording medium 26 by the objective lens 24. The light beam reflected by the recording medium 26 is modulated into a polarized state in conformity with the information magnetically recorded on the recording medium 26, again passes through the objective lens 24, is reflected by the half-mirror 23 and is directed to the analyzer 27. The detection light 13 passed through the analyzer 27 is intensity-modulated and is received by the photo-detector 29 through the condensing lens 28. The light beam 13 passed through the analyzer 27 and intensity-modulated is converted into a photo-current by the photodetector 29 shown in Figure 4. The photoelectric conversion efficiency κ is given by the following equation: κ = eρ hν , (6) where e is the amount of charge, h is Plancks constant, ρ is the quantum efficiency of the photodetector and ν is the number of vibration of the light beam. In this regard, the following four kinds of noises are considered to be noise sources in signal reading-out: 1) the noise attributable to the square mean intensity fluctuation ΔI²R of a non-modulated component light IR; 2) the noise attributable to the square mean intensity fluctuation ΔI²K of a modulated component light IK; 3) the shot noise of the photodetector; and 4) the thermal noise by the amplifier. The noise by ΔI²R mentioned under item 1) above and the noise by ΔI²K mentioned under item 2) above are caused by the surface roughness and heterogeneity of the recording medium and the intensity fluctuation of the semiconductor laser, and if the constants determined by the noise sources such as the meidum and the semiconductor laser are ξ and ζ, respectively, and the averages of the actual effective values of the non-modulated component and the modulated component are I R and I K, respectively, then the following equations are established: where ΔB is the band width of the detection signal. If the noise attributable to ΔI²R, the noise attributable to ΔI²K, the shot noise and the thermal noise are FR, FK, S and T, respectively, they can be expressed as follows: where k is the Boltzmann constant, Te is the equivalent noise temperature and Rf is the resistance value of the load resistor 16. By equations (4) and (5), with respect to the azimuth angle ϑA of the optic axis of the analyzer, the magneto-optical modulated component intensity IK has the dependency of sin²ϑA and the non-modulated component intensity IR has the dependency of cos²ϑA and therefore, the ϑA-dependencies of the respective noises can be expressed as follows: By the use of these, C/N can be expressed in decibel indication as follows: The C/N of equation (17) is a function of the azimuth angle ϑA of the optic axis of the analyzer and therefore, equation (17) is differentiated by ϑA to find the extremal value. The extremal value found with respect to ϑA is as follows: If the azimuth angle of the optic axis of the analyzer which will satisfy expressions (18) - (21) is set, C/N can be made a maximum value. In the foregoing description, the reduction in the signal level has been described as being not caused by the recording medium and the optical system, but it must be taken into account in exactly foreseeing the C/N in the actual optical system. As the causes of the reduction in-the signal level, the following two points are conceivable: (I) Loss of the quantity of light (the reduction in amplitude by absorption and eclipse); and (II) The phase difference between P-polarized light and S-polarized light. (I) and (II) contribute to the reduction in the magneto-optical modulated component intensity, and (I) alone contributes to the reduction in the non-modulated component intensity. To evaluate the reduction in the magneto-optical non-modulated component intensity (loss of the quantity of light), the light utilization efficiency εR is defined. It should be noted that in the present invention, as the light utilization efficiency, attention is paid to the ratio between the quantity of light on the recording medium and the quantity of light reaching the photodetector. In the present embodiment, when finding εR, the following points have been taken into consideration: (A) The rate at which the diffracted light from the tracking grooves (pitch 1.6 µm, depth λ/8, λ = 835 nm) enters the entrance pupil of the objective lens is regarded as the light utilization efficiency; and (B) With the product along the optical path of the square of the P-polarization direction amplitude transmittances (or reflectances) of n optical elements except the analyzer present in the optical path leading from the recording medium to the photodetector being taken into consideration, the light utilization efficiency is defined as ε₁. If the amplitude transmittance and reflectance of the i th optical element are tpi and rpi, respectively, ε₁ can be expressed as follows: In an equation (22), where the light beam is reflected by the i th optical element, |rpi|² may be substituted instead of |tpi|². The transmittance of the analyzer is handled as an amount of variation during the calculation of C/N and is therefore excepted from ε₁. From (A) and (B), the light utilization efficiency εR of the magneto-optical non-modulated component can be expressed as follows: ε R = ε ₀ ε ₁ (23) The reduction in the intensity of the magneto-optical modulated component is now considered. For this purpose, the phase difference between the P-polarized light and the S-polarized light must be taken into account in addition to the loss of quantity of light. For example, it is known that as shown in Figure 5, the reflected light from the recording medium is generally not a rectilinearly polarized light as shown in Figure 2 but an elliptically polarized light whose major axis is inclined by the Kerr rotation angle ϑk due to the phase difference created between the P-polarized component and the S-polarized component. That is, the P- and S-polarized components R and K of the amplitude reflectance of the recording medium can be expressed as follows: where αo and βo are the phase components of respective amplitude reflectances. In this case, the Kerr rotation angle ϑk can be expressed as follows: If Δo = nπ (n = integer), the reflected light from the recording medium becomes a rectilinearly polarized light, but in the other cases, it decreases ϑk, and this is not preferable. This also holds true of the optical elements, and in the present embodiment, the light utilization efficiency εk is defined to evaluate the reduction in the intensity of the magneto-optical modulated component, and when finding εk, the following point has been taken into consideration. For the magneto-optical modulated component, the light utilization efficiency is defined as ε₂ with the product along the optical path of the P and S polarization direction amplitude transmittances (or reflectances) of n optical elements except the analyzer present in the optical path leading from the recording medium to the photodetector being taken into consideration. If the P and S polarization direction amplitude transmittances of the i th optical element are tpi and tsi (in the case of the reflectances, rpi and rsi), the following equations are established: By the use of (26), ε₂ is expressed as follows: In (27), where the light beam is reflected by the i th optical element, |rpi| |rsi| may be substituted instead of |tpi|·|tsi|. The transmittance of the analyzer is handled as an amount of variation during the calculation of C/N and is therefore excepted from ε₂. Thus, the light utilization efficiency εk of the magneto-optical modulated component is expressed as follows: ε K = ε ₀ ε ₂ (28) More accurate evaluation is also made of the analyzer. If the amplitude transmittance and the extinction ratio of the analyzer are tA and ηA, respectively, consideration may be given with cosϑA substituted for by |tA|·(cosϑA + √ ηA sinϑA and sinϑA substituted for by |tA|·(sinϑA + √ ηA cosϑA in equation (2). As 0R|² » |K|², the product of εk and the transmittance ε₃ of the analyzer given by the following equation may be taken for the magneto-optical modulated component intensity: The amplitude transmittance of the analyzer has been equal between the P-polarized component direction and the S-polarized component direction and has provided no phase difference between the P-polarized light and the S-polarized light. For the magneto-optical non-modulated component, the product of εR and the transmittance ε₄ of the analyzer given by the following equation may be taken: Thus, if the intensities of the magneto-optical modulated component and non-modulated component are IK and IR, respectively, they are expressed as follows: By substituting expressions (31) and (32) into equation (17), the angle ϑA of the optic axis of the analyzer with respect to the direction of polarization of the incident light beam which maximizes C/N can be found as follows: Conditions for calculation will be shown below. The semiconductor laser 21 has a wavelength of λ = 835 nm and the output thereof is adjusted irrespective of the transmittance |tp|² of the half-mirror 23 so that the quantity of incident light on the recording medium 26 is I O = 2 x 10⁻³W. GdTbFeCo non-crystalline magnetic alloy is used as the recording layer of the recording medium 26, |R|²= 0.12, ϑk = 0.74° and the phase difference Δo between the phase components αo and βo of P- and S-polarization direction amplitude reflectances is Δo = 20°. The light utilization efficiency εo is εo = 0.6 when the diffracted light from the tracking grooves (pitch 1.6 µm and depth λ/8) is received by an objective lens of N.A. = 0.5. The light utilization efficiency ε₁ is ε₁ = 0.39 with the product of the transmittances (in the case of the half-mirror, the reflectances) of the optical elements except the analyzer present in the optical path leading from the recording medium to the photodetector being taken into consideration. As regards the light utilization efficiency ε₂, the product of the P and S amplitude transmittances (in the case of the half-mirror, the reflectances) of the optical elements except the analyzer present in the optical path leading from the recording medium to the photodetector may be taken into consideration. The half-mirror 23 used in the present embodiment is adapted to create a phase difference of ΔHM = 160° between the P-polarized light and the S-polarized light. Accordingly, between ΔHM and the phase difference Δo created by the recording medium, there is a relation that Δo + ΔHM = π (37) and thereby, any reduction in the magneto-optical modulated component intensity is prevented. In the present embodiment, there is no optical element which provides a phase difference between the P-polarized light and the S-polarized light during transmission and therefore, The photodetector 25 is an Si - PIN photodiode of photoelectric conversion factor K = 0.54. The constants ξ and ζ determined by the noise sources such as the recording medium and the semiconductor laser are given as follows: ξ = 2 × 10⁻¹³ (R.I.N) ζ = 1 × 10⁻¹¹ (R.I.N) Also, the thermal noise T is given as T = 5 x 10⁻²¹ with the Boltzmann constant k being k = 1.38 x 10⁻²³, the equivalent noise temperature Te being Te = 300[K], the load resistance Rf being Rf = 1 x 10⁻⁵[Ω] and the band width ΔB of the signal detection being ΔB = 3 x 10⁴ [1/Hz]. In some cases, the thermal noise T cannot be described in such a simple form as shown in equation (12) depending on the capacity or the like of the photodetector and therefore, in such cases, T need not conform to such form. The analyzer has an amplitude transmittance tp of |tp|² = 0.84 and an extinction ratio ηA = 1 x 10⁻³. Figure 6 is a graph showing the relation between the angle ϑA of the optic axis of the analyzer in the direction of polarization of the incident light beam and C/N. It is seen that the C/N of the present embodiment becomes maximum at optimum ϑA = 79.4° given by expressions (33) - (36). In the present embodiment, as compared with the conventional apparatus in which ϑA = 45°, C/N is improved over 8dB. If ϑA = 70° - 85°, sufficiently good C/N will be obtained. Figure 7 is a graph showing the relation between ϑA and C/N when the value of the constant ξ which determines the square mean fluctuation of the magneto-optical non-modulated component intensity is changed to ξ = 1 x 10⁻¹¹, 10⁻¹², 10⁻¹³, 10⁻¹⁴. This graph shows that where due to expression (33), the noise FR attributable to ΔI²R and the shot noise S are great relative to the thermal noise T, the optimum value of ϑA approaches 90°. Also comparing the C/N at the optimum value of ϑA with the C/N at ϑA = 45°, it is seen that C/N is improved when FR and S becomes great relative to T. For example, where ξ = 1 x 10⁻¹¹, C/N is improved over 18dB, and this means that the present invention is very effective. Figures 8A and 8B schematically show a second embodiment of the present invention, Figure 8B being a view in which Figure A is seen in the direction of arrow A. In Figures 8A and 8B, members similar to those in Figure 3 are given similar reference numerals and need not be described in detail. Again in the present embodiment, the signal processing system subsequent to the photodetector 29 is constructed as shown in Figure 4. The present embodiment employs a half-mirror 10 in place of the half-mirror 23 in the first embodiment, and is designed to detect the light transmitted through this half-mirror 10. The surface b of the half-mirror 10 is inclined by a predetermined angle so that stray light may not enter the photodetector 29. In the present embodiment, consideration may be given with the P- and S-polarization directions used in the description of Figure 3 being replaced with each other. Figure 9 schematically shows the construction of a third embodiment of the present invention. In Figure 9, members similar to those in Figure 3 are given similar reference numerals and need not be described in detail. Again in the present embodiment, the signal processing system subsequent to the photo-detector 29 is constructed as shown in Figure 4. The present embodiment employs a polarizing beam splitter 12 instead of the half-mirror 23 shown in Figure 3. When the amplitude transmittances of the polarizing beam splitter 12 for P-polarized light and S-polarized light are tp and ts, respectively, and the amplitude reflectances thereof are rp and rs, respectively, and the amplitude transmittance of the analyzer 27 is t A (equal between the direction of P-polarization and the direction of S-polarization) and the extinction ratio is ηA and the intensity of the incident light on the medium is I O , the intensity of the detection light 13 can be expressed as follows: With the fact that [R|²»[K[² being taken into consideration, equation (38) is expressed as follows: In expresssion (39), the second term in the parentheses is the magneto-optical modulated component and the first term in the parentheses is the nonmodulated component, and the intensities thereof are I K and I R , respectively. It is to be understood that the output of the semiconductor laser is adjusted irrespective of the amplitude transmittances tp and ts of the polarizing beam splitter so that the incident light I O may be of a predetermined quantity of light. Considering the ϑA-dependencies of the respective noises in the process similar to the aforementioned expression (6) - (12), the magneto-optical modulated component intensity I K has a dependency of (1 - ηA)sin2ϑA and the non-modulated component intensity I R has a dependency of cos²ϑA + ηAsin²ϑA and therefore, the ϑA-dependencies of the respective noises can be expressed as follows: If by the use of these, C/N is to be expressed in decibel indication, it can be expressed by the following equation (17') as in the embodiment of Figure 3. However, unlike the case of Figure 3, I K , I R , etc. conform to expressions (38) - (41). The C/N of equation (17') is a function of the amplitude reflectances rp and rs of the polarizing beam splitter and the inclination ϑA of the optic axis of the analyzer with respect to the direction of P-polarization and therefore, equation (17') may be differentiated by |rp|, |rs| and ϑA to find a maximum value. C/N can be made a maximum value by the following conditions: Figure 10 schematically shows the construction of an optical system according to a fourth embodiment of the present invention. The present embodiment is a modification of the third embodiment in which the light beam transmitted through the polarizing beam splitter 12 is detected. In Figure 10, members similar to those in Figuer 9 are given similar reference numerals and need not be described in detail. Also, the signal processing circuit may be similar to that shown in Figure 4. In the case of the present embodiment, consideration may be given with the direction of polarization of the semiconductor laser 21 being regarded as the direction of S-polarization perpendicular to the plane of the drawing sheet and with the directions of P-polarization and S-polarization used in the description of Figure 9 being replaced with each other. However, in expressions (38) - (41), rp and rs need be replaced with ts and tp, respectively. That is, The C/N of equation (17') is a function of the amplitude transmittances ts and tp of the polarizing beam splitter and the inclination ϑA of the optic axis of the analyzer with respect to the direction of P-polarization and therefore, equation (17') may be differentiated by |ts|, |tp| and ϑA to find a maximum value. Accordingly, C/N can be made a maximum value by the following conditons: Figure 11 schematically shows fifth embodiment of the present invention. In Figure 11, members similar to those in Figure 3 are given similar reference numerals and need not be described in detail. Again in the present embodiment, the signal processing system subsequent to the photodetector 29 is constructed as shown in Figure 4. In the present embodiment, a polarizing beam splitter 30 having the beam shaping function is employed instead of the half-mirror 23 in the first embodiment. The surface C of the polarizing beam splitter 30 is inclined by a predetermined angle so that stray light may not enter the photodetector 29. Even where a polarizing beam splitter is employed as in the third to fifth embodiments, the reduction in the signal level by the recording medium and the optical system must be taken into consideration. The influences of the other elements than the polarizing beam splitter are entirely similar to those described previously in connection with expressions (22) - (28). As regards the polarizing beam splitter, if the amplitude reflectances in the directions of P-polarization and S-polarization are rp and rs, respectively. where r and δ are the phase components of the respective amplitude reflectances. Thus, if the intensities of the magneto-optical modulated component and now-modulated component are I K and I R , respectively, they may be expressed as follows: By substituting expressions (57) and (58) into equation (17'), the polarizing characteristic of the polarizing beam splitter which maximizes C/N and the angle ϑA of the optic axis of the analyzer with respect to the direction of P-polarization can be found as follows: Conditions for calculation will be shown below. The semiconductor laser 21 has an S wavelength of λ = 835 nm, and the output thereof is adjusted irrespective of the transmittance |tp|² of the polarizing beam splitter so that the quantity of incident light I O on the recording medium 26 is I O = 2 x 10⁻³W. GdTbFeCo non-crystalline magnetic alloy is used as the recording layer of the recording medium 26, and |R|² = 0.12, ϑK = 0.74°, and the phase difference Δ0 between the phase components α0 and β0 of the amplitude reflectances in the directions of P-polarization and S-polarization is Δ0 = 20°. The light utilization efficiency ε0 = 0.6 when the diffracted light from the tracking grooves (pitch 1.6 µm and depth λ/8) is received by an objective lens of N.A. = 0.5. The light utilization efficiency ε1 is ε1 = 0.79 with the product of the transmittances of the optical elements except the polarizing beam splitter and analyzer present in the optical path leading from the recording medium to the photodetector being taken into consideration. As regards the light utilization efficiency ε2, the product of the P and S amplitude transmittances of the optical elements except the polarizing beam splitter the analyzer present in the optical path leading from the recording medium to the photodetector may be considered. In the present embodiment, there is no optical element which provides a phase difference between the P-polarized light and the S-polarized light during the transmittance and therefore, The photodetector 25 is an Si - PIN photodiode of photoelectric conversion efficiency K = 0.54. The constants ξ and ζ determined by the noise sources such as the recording medium and the semiconductor laser are given as follows: ξ = 2 x 10⁻¹³ (R.I.N.) ζ = 1 x 10⁻¹¹ (R.I.N.) Also, the thermal noise T is given as T = 5 x 10⁻²¹ with the Boltzmann constant K being K = 1.38 x 10⁻²³, the equivalent noise temperature Te being Te = 300[K], the load resistance Rf being Rf = 1 x 10⁵ [Ω] and the band width ΔB of the signal detection being ΔB = 3 x 10⁴ [1/Hz]. In some cases, the thermal noise T cannot be described in the simple form as shown in equation (12) due to the capacity or the like of the photodetector and therefore, in such cases, it need not conform to such form. The transmittance of the analyzer is |tA|² = 0.84 and the extinction ratio thereof is ηA = 1 x 10⁻³. Figure 12 shows the C/N of the present embodiment (indicated by solid line) using a polarizing beam splitter having the polarizing characteristics |rp|² = 0.18 and |rs|² = 1 given by expressions (59), (60) and (61) and the C/N of the apparatus (indicated by dot-and-dash line) using a half-mirror. In Figure 12, the ordinate represents C/N and the abscissa represents the angle ϑA of the optic axis of the analyzer with respect to the direction of P-polarization. In the present embodiment, for ϑA = 79.9°, C/N becomes maximum. Also, if ϑA is 75° - 85°, sufficiently good C/N can be obtained. Figure 13 is a graph showing the relation between the polarizing characteristic |rp|² of the polarizing beam splitter and C/N. In Figure 13, the ordinate represents C/N and the abscissa represents |rp|², and in any of these |rs|² = 1 and ϑA = 79.9°. From this, sufficiently good C/N could be obtained if |rp|² is 0.08 - 0.4. In the present embodiment, the phase difference ΔPBS between the directions of P-polarization and S-polarization created by the polarizing beam splitter is ΔPBS = 160° in any case, and has the relation that ΔO + ΔPBS = π (63) with respect to the phase difference ΔO created by the recording medium. Thereby, any reduction in the magneto-optical modulated component intensity is prevented. It is easy to make a polarizing beam splitter of such polarizing characteristic. Figures 14A and 14B schematically show a sixth embodiment of the present invention, Figure 14B being a view in which Figure 14A is seen in the direction of arrow A. In Figures 14A and 14B, members similar to those in Figure 11 are given similar reference numerals and need not be described in detail. Again in the present embodiment, the signal processing system subsequent to the photodetector 29 is constructed as shown in Figure 4. The present embodiment uses a polarizing beam splitter 31 instead of the polarizing beam splitter 30 in the fifth embodiment, and is designed to detect the light transmitted through this polarizing beam splitter 31. The surface d of the polarizing beam splitter 31 is inclined by a predetermined angle so that stray light may not enter the photodetector 29. In the present embodiment, consideration may be given with the directions of P-polarization and S-polarization used in the description of Figure 11 being replaced with each other. However, in expressions (57) and (58), rp and rs need be replaced with ts and tp, respectively. That is, if the intensities of the magneto-optical modulated component and non-modulated component are I K and I R , respectively, they can be expressed as follows: By substituting expressions (64) and (65) into equation (17′), the polarizing characteristic of the polarizing beam splitter with maximizes C/N and the angle of the optic axis of the analyzer with respect to the direction of P-polarization can be derived from the following expressions: If the conditions for calculation are selected in the same manner, there will be obtained a result similar to the result shown in Figures 12 and 13. However, the abscissa represents |ts|². It is easy to make such a polarizing beam splitter having a polarizing characteristic which will compensate for the phase difference between the directions of P-polarization and S-polarization created by the recording medium. Besides the above-described embodiments, the present invention permits various applications. For example, in the embodiments illustrated, the reflected light from the magneto-optical recording medium has been detected, whereas design may be made such that the light beam transmitted through the magneto-optical recording medium and modulated by the Faraday effect is detected.

Claims: A magneto-optical information reproducing apparatus comprising means (21,22,24) for applying a light beam polarized in a predetermined direction onto a recording medium (26) on which information is magnetically recorded, analyzer means (27) for analyzing the reflected or transmitted light beam from said recording medium (26) modulated into a polarized state in conformity with said information by the magneto-optical effect, a half-mirror (10,23) for separating the reflected light from said medium (26) from the light beam applied to said medium (26) and directing it to said analyzer means (27), a photodetector (29) photoelectrically detecting the light beam transmitted through said analyzer means (27), and amplifying means (15,16) for amplifying the detection signal of said photodetector and reproducing said information, characterized in that the angle ϑ A formed between the optical axis of said analyzer means and said predetermined direction of said polarized light beam satisfies the following conditions: where the average of the intensities of polarized components entering said photodetector (29) and not modulated by the magneto-optical effect is I R ; the square mean of the intensity fluctuation in a magneto-optical signal observation frequency is ΔI² R ; ξ = ΔI 2 / R/ I 2 / R; the quantity of light of the incident light beam on said recording medium (26) is I O ; the amplitude reflectance of said recording medium (26) is R; the light utilization efficiency of the optical system from the recording medium (26) to the photodetector (29) except said analyzer means (27) is ε; the photoelectric conversion efficiency of said photodetector (29) is κ ; the amount of charge is e; the thermal noise of said amplifying means (15,16) in the magneto-optical signal observation frequency is T; the band width of the detection signal is ΔB; the amplitude transmittance of said analyzer means (27) is t A ; and the extinction ratio of said analyzer means (27) is η A . A magneto-optical information reproducing apparatus comprising means (21,22,24) for applying a light beam polarized in a predetermined direction onto a recording medium (26) on which information is magnetically recorded, a polarizing beam splitter (12,30) for reflecting and transmitting therethrough the reflected or transmitted light beam from said recording medium (26), said light beam being modulated into a polarized state in conformity with said information by the magneto-optical effect, at a predetermined rate corresponding to the polarized component thereof, analyzer means (27) for analyzing the light beam reflected by said polarizing beam splitter (12,30), a photodetector (29) photoelectrically detecting the light beam transmitted through said analyzer means (27), and amplifying means (15,16) for amplifying the detection signal of said photodetector (29) and reproducing said information, characterized in that the amplitude reflectance rp of said polarizing beam splitter (12,30) for the polarized component in said predetermined direction, the amplitude reflectance rs of said polarizing beam splitter (12,30) for the polarized component in a direction perpendicular to said predetermined direction and the angle ϑ A formed between the optical axis of said analyzer means (27) and said predetermined direction of said polarized light beam satisfy the following conditions: where the symbols have the same meanings as in claim 1. A magneto-optical information reproducing apparatus comprising means (21,22,24) for applying a light beam polarized in a predetermined direction onto a recording medium (26) on which information is magnetically recorded, a polarizing beam splitter (12,31) for reflecting and transmitting therethrough the reflected or transmitted light beam from said recording medium (26), modulated into a polarized state in conformity with said information by the magneto-optical effect, at a predetermined rate corresponding to the polarized component thereof, analyzer means (27) for analyzing the light beam transmitted through said polarizing beam splitter (12,31), a photodetector (29) photoelectrically detecting the light beam transmitted through said analyzer means, and amplifying means (15,16) for amplifying the detection signal of said photodetector (29) and reproducing said information, characterized in that the amplitude transmittance tp of said polarizing beam splitter (12,31) for the polarized component in said predetermined direction, the amplitude transmittance ts of said polarizing beam splitter (12,31) for the polarized component in a direction perpendicular to said predetermined direction and the angle ϑ A formed between the optical axis of said analyzer means (27) and said predetermined direction of said polarized light beam satisfy the following conditions: where the symbols have the same meanings as in claim 1. A magneto-optical information reproducing apparatus according to any preceding claim, wherein said means for applying a light beam comprises a semiconductor laser (21), and an optical system (22,24) for condensing the light beam emitted from said semiconductor laser (21) on said medium (26). A magneto-optical information recording apparatus according to any preceding claim, wherein said photodetector (29) has no amplifying action. A magneto-optical information reproducing apparatus according to claim 6, wherein said photodetector is a PIN photodiode (29).

Inventors: KOYAMA, OSAMU
Applicants: CANON KABUSHIKI KAISHA
Application year: 1987
Main classification: G11B11
IPC codes: G11B11