Magneto-Optic Recording Medium Having a Metal Oxide Recording Layer

1. Field of the Invention

The present invention relates to a novel metal oxide magnetic substance, a magnetic film consisting thereof, and their uses as magneto optical recording medium and perpendicular magnetic recording medium.

2. Prior Art

In recent years, magneto optical recording mediums designed to carry out magnetic recording by the use of semi-conductor laser beam have been studied and developed so as to be used for high density recording purposes. Usually, the magnetic substances used in magneto optical recording mediums were mostly occupied by those consisting of amorphous alloys made of rare earth metals and transition metals. The preparation of magneto optical recording mediums using such amorphous alloy magnetic substances was carried out generally in the manner of adhering said magnetic substance, for instance Tb-Fe alloy, on a substrate such as glass plate by vacuum vapordeposition, sputtering or the like in the degree of about 0.1-1 .mu.m in thickness to form a magnetic film. The thus obtained magneto optical recording medium is recorded and regenerated as mentioned below. That is, recording is carried out in the manner of radiating the laser beam modulated with a divalent signal, making use of the rapid variation characteristic of a coercive force corresponding to the temperature variation in the neighborhood of the Curie temperature or compensation temperature of the magnetic film, on the magnetic film and heating same, thus inverting the direction of magnetization. Regeneration is carried out by reading out making use of the difference in magneto optical effects of the thus inversion-recorded magnetic film. The photomagnetic recording material using aforesaid amorphous alloy magnetic substance is advantageous in that it can be recorded at high speed (frequency=1 MHz) by means of a semiconductor laser beam because it is of a high recording sensitivity, but is heavily disadvantageous in that the magneto optical characteristic of the magnetic film deteriorates with a lapse of time because the amorphous alloy magnetic substance, in particular the rare earth metal component, is subject to oxidizing corrosion. In order to prevent this, it is known to provide a protective layer consisting of an oxide such as SiO, SiO.sub.2 or a nitride such as TiN, Si.sub.3 N.sub.4 on an amorphous magnetic film by means of vacuum vapordeposition, sputtering or the like as in the preparation of the magnetic film, but this is inadvantageous in that at the time of preparing the magnetic film or the protective layer, the magnetic film is oxidized and corroded by O.sub.2 remaining in the vacuum, O.sub.2, H.sub.2 O or the like adsorbed to the surface of the substrate, and O.sub.2, H.sub.2 O or the like contained in the target consisting of the alloy magnetic substance with a lapse of time and pin holes are occurred, and further the oxidizing corrosion is enhanced by the light and heat at the time of recording. Further, the amorphous magnetic substance is disadvantageous in that it is liable to be crystalized by heat and therefore its magnetic characteristic is liable to be deteriorated. Still further, the reflection type Faraday system which comprises thickening the magnetic film as much as possible, providing a reflective film of Cu, Al, Pt, Au or the like thereon, radiating the laser beam on the magnetic film and permeating it therethrough, thereafter reflecting said beam from the magnetic film at the reflective film, and detecting this reflected beam has been proposed as the regeneration system for enhancing the regeneration output. The Faraday system is surely profitable in that a high S/N signal can be obtained, but the conventional amorphous magnetic film could not be used in this system because said magnetic film is inferior in transmittancy.

A primary object of the present invention is to provide a novel metal oxide magnetic substance which has high recording sensitivity, is superior in oxidizing corrosion resistance and is especially suitable as a material for preparing a magneto optical recording medium; a magnetic film consisting of this metal oxide magnetic substance; and a magneto optical recording medium having said magnetic film on a substrate.

A secondary object of the present invention is to provide a perpendicular magnetic recording medium which comprises providing a magnetic film consisting of said magnetic metal oxide magnetic substance on a substrate.

The metal oxide magnetic substance according to the present invention is the one represented by the general formula I:

(wherein, Me is at least one member of Ba, Sr and Pb, M.sup.I is at least one member of Zn, Sc, In, Cr, Ir, Ru, Rh, Ti, Ta, Sn and Ge, 5.ltoreq.n.ltoreq.6, 0<X.ltoreq.0.8, 0<Y.ltoreq.0.8, and m is an ionic valency of M.sup.I) and the one represented by the general formula II:

(wherein, Me is at least one member of Ba, Sr and Pb, M.sup.II is at least one member of Ga and Al, 5.ltoreq.n.ltoreq.6, and 0<T.ltoreq.1.0); the magnetic film according to the present invention comprises the metal oxide magnetic substances represented by said general formula I or II, and the magneto optical recording medium and the perpendicular magnetic recording medium according to the present invention are each the one having said magnetic film on a substrate.

In this connection, it is to be noted that these metal oxide magnetic substances represented by the general formulas I and II may be added with metals such as Ni, Cu, Sb, Bi, Co, Mo, Nb, Pd, Mn, Yb, V, Te, Zr, Tc, Pt, Os, Re, W and the like in order to improve magneto optical effect or to regulate coercive force or ionic valency (regarding to the regulation of ionic valency, when a divalent metal or a tetravalent metal is used as M.sup.I, a tetravalent metal or a divalent metal is preferably added respectively).

The magnetic substance or magnetic film used in the magneto optical recording medium is required to have the magneto optical characteristics (proper Curie temperature, coercive force and the like) which permit the recording and regeneration using a semi-conductor laser beam, and must have a low Curie temperature Tc in order to obtain a high recording sensitivity and a properly high coercive Hc in order to maintain a recorded memory stably. Generally speaking, the proper range of Tc is considered to be 100.degree.-400.degree. C., and the proper range of Hc is considered to be 200-6000 oersted. The reason is that when Tc is less than 100.degree. C., the recorded memory becomes unstable due to the laser beam at the time of regeneration which leads to the reason for deteriorating the regeneration characteristic and when Tc is more than 400.degree. C., the recording using the laser beam becomes difficult, whilst when Hc is less than 200 oersted, it is possible that the memory becomes unstable and dissipates and when Hc is more than 6000 oersted, the laser output and the outside magnetic field required for magnetic inversion at the time of recording become undesirably large.

On the other hand, hexagonal and spinel metal oxide magnetic substances have hitherto been studied as the magnetic bubble materials. As the hexagonal metal oxide magnetic substance there is known the M type ferrite represented by for instance the general formula III:

(wherein, Me and n are the same as defined in the general formula I or II).

We paid attention to the fact that since the magnetic substance of this sort is itself oxide, there is no peril of being deteriorated by oxidation and that even when the film thickness is increased to 10 .mu., said substance still holds permeability. However, said magnetic substance is disadvantageous in that since the Curie temperature Tc is high (450.degree. C. or more), it makes the recording using the semi-conductor laser beam as described previously still more difficult, and so it itself can not be applied as the material for magneto optical recording medium. In view of this, we have carried out various investigations to find that when part of the Fe atoms in the general formula III is substituted by Ga, Al or said M.sup.I metal, Tc is lowered in each case of substitution by Ga, Al or said M.sup.I metal. At the same time, we found that in the case of Ga substitution and Al substitution coercive force increases and in the case of M.sup.I metal substitution coercive force decreases. Taking the case of the general formula III, the cases of

(1) Ga or In-substituted compound where Me=Ba:BaFe.sub.12-(l/3)z M.sub.z 'O.sub.19 (M' stands for Ga or In, Z stands for the substitution number of Ga or In and l stands for ionic valency of Ga or In.),

(2) Ga or Zn-substituted compound where Me=Ba:BaFe.sub.12-(l/3)z M.sub.z 'O.sub.19 (M' stands for Ga or Zn, Z stands for the substitution number of Ga or Zn and l stands for ionic valency of Ga or Zn.),

(3) Ga or Sc-substituted compound where Me=Ba:BaFe.sub.12-(l/3)z M.sub.z 'O.sub.19 (M' stands for Ga or Sc, Z stands for the substitution number of Ga or Sc and l stands for ionic valency of Ga or Sc.),

(4) Ga or Ti-substituted compound where Me=Ba:BaFe.sub.12-(l/3)z M.sub.z 'O.sub.19 (M' stands for Ga or Ti, Z stands for the substitution number of Ga or Ti and l stands for ionic valency of Ga or Ti.),

(5) Ga or Sn-substituted compound where Me=Ba:BaFe.sub.12-(l/3)z M.sub.z 'O.sub.19 (M' stands for Ga or Sn, Z stands for the substitution number of Ga or Sn and l stands for ionic valency of Ga or Sn.),

(6) Ga, Sc, Ti, Sn or Zn-substituted compound where Me=Ba and Sr:Ba.sub.0.75 Sr.sub.0.25 Fe.sub.12-(l/3)z M.sub.z 'O.sub.19 (M' stands for Ga, Sc, Ti, Sn or Zn, Z stands for the substitution number of Ga, Sc, Ti, Sn or Zn and l stands for ionic valency of Ga, Sc, Ti, Sn or Zn.),

(7) Ga, In, Sc, Ti, Sn or Zn-substituted compound where Me=Pb:PbFe.sub.12-l/3)z M.sub.z 'O.sub.19 (M' stands for Ga, In, Sc, Ti, Sn or Zn, Z stands for the substitution number of Ga, In, Sc, Ti, Sn or Zn and l stands for ionic valency of Ga, In, Sc, Ti, Sn or Zn.), and

(8) Ga, In, Sc, Ti, Sn, Zn, Ta or Ge-substituted compound where Me=Sr and Pb:Sr.sub.0.25 Pb.sub.0.75 Fe.sub.12-(l/3)z M.sub.z 'O.sub.19 (M' stands for Ga, In, Sc, Ti, Sn, Zn, Ta or Ge, Z stands for the substitution number of Ga, In, Sc, Ti, Sn, Zn, Ta or Ge and l stands for ionic valency of Ga, In, Sc, Ti, Sn, Zn, Ta or Ge.), denoted the tendency as shown in FIG. 1, FIG. 2, FIG. 3, FIG. 4, FIG. 5, FIG. 6-1.about.4, FIG. 7-1.about.5 and FIG. 8-1.about.7 with reference to Tc, and denoted the tendency as shown in FIG. 9, FIG. 10, FIG. 11, FIG. 12, FIG. 13, FIG. 14-1.about.4, FIG. 15-1.about.5 and FIG. 16-1.about.7 with reference to Hc respectively. When Al was used as M' in the aforesaid formulas (1)-(8), the same result as in the case of M'=Ga was obtained in each formula. Therefore, while paying attention to the substitution effects of Ga, Al and M' metal and further taking account of the aforesaid proper ranges of Tc and Hc, we have substituted part of Fe in the metal oxide represented by the general formula III by using two kinds of metals consisting of Ga and at least one member of said M' or using at least one member of said M.sup.II in various percentages to find the fact that the metal oxide magnetic substances represented by the general formulas I and II achieve superior characteristics as the magneto optical recording mediums. Based on this finding, the present invention was accomplished.

As is evident from the aforegoing, the present invention has made the metal oxide of the general formula III applicable as the material for magneto optical recording medium by substituting part of Fe atoms in the metal oxide of the general formula III, which was not regarded as the material for use in magneto optical recording medium due to its high Curie temperature, by Ga and M.sup.I metal or by M.sup.II metal atoms so that the Curie temperature may be lowered while maintaining coercive force at a suitably high degree required for the memory and thus the metal oxide of the general formula III may be recorded and regenerated by the semi-conductor laser beam.

In other words, the metal oxide magnetic substance according to the present invention satisfies the proper Curie temperature range and the proper coervice force range required for the magneto optical recording medium material.

For instance, in the case of

(9) BaGa.sub.X' In.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, X' stands for the substitution number of Ga and Y' stands for the substitution number of In)

corresponding to the preceding formula (1), Tc is 220.degree. C. when the substitution number X' of Ga is 1.7 and the substitution number Y' of In is 1.0 as shown in FIG. 17, and Hc is about 600 oersted when the substitution number X' of Ga is 1.7 and the substitution number Y' of In is 1.0 as shown in FIG. 18. In the case of

(10) BaGa.sub.X' Zn.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, X' stands for the substitution number of Ga and Y' stands for the substitution number of Zn)

corresponding to the preceding formula (2), Tc is 230.degree. C. when the substitution number X' of Ga is 2.24 and the substitution number Y' of Zn is 1.75 as shown in FIG. 19, and Hc is about 480 oersted when the substitution number X' of Ga is 2.24 and the substitution number Y' of Zn is 1.75 as shown in FIG. 20. In the case of

(11) BaGa.sub.X' Sc.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, X' stands for the substitution number of Ga and Y' stands for the substitution number of Sc)

corresponding to the preceding formula (3), Tc is 225.degree. C. when the substitution number X' of Ga is 2.24 and the substitution number Y' of Sc is 1.2 as shown in FIG. 21 and Hc is 420 oersted when the substitution number X' of Ga is 2.24 and the substitution number Y' of Sc is 1.2 as shown in FIG. 22. In the case of

(12) BaGa.sub.X' Ti.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, X' stand for the substitution number of Ga and Y' stands for the substitution number of Ti)

corresponding to the preceding formula (4), Tc is 225.degree. C. when the substitution number X' of Ga is 1.68 and the substitution number Y' of Ti is 1.5 as shown in FIG. 23 and Hc is about 1.2K oersted when the substitution number X' of Ga is 1.68 and the substitution number Y' of Ti is 1.5 as shown in FIG. 24. In the case of

(13) BaGa.sub.X' Sn.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, X' stands for the substitution number of Ga and Y' stands for the substitution number of Sn)

corresponding to the preceding formula (5), Tc is 250.degree. C. when the substitution number X' of Ga is 2.24 and the substitution number Y' of Sn is 1.7 as shown in FIG. 25, and Hc is about 250 oersted when the substitution number X' of Ga is 2.24 and the substitution number Y' of Sn is 1.7 as shown in FIG. 26. In the case of

(14) Ba.sub.0.75 Sr.sub.0.25 Ga.sub.X' M'.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, M' stands for Sc, Ti, Sn or Zn, X' stands for the substitution number of Ga, Y' stands for the substitution number of Sc, Ti, Sn or Zn and l is as defined previously)

corresponding to the preceding formula (6), Tc is 225.degree. C. when the substitution number X' of Ga is 2.24 and the substitution number Y' of Sc is 1.2 as shown in FIG. 27-1, and the same tendency can be observed when M'=Ti, Sn and Zn (which see FIG. 27-2, FIG. 27-3 and FIG. 27-4 respectively). Referring to Hc where M'=Sc, it is 420 oersted when the substituion number X' of Ga is 2.24 and the substitution number Y' of Sc is 1.2 as shown in FIG. 28-1, and the same tendency can be observed when M'=Ti, Sn and Zn (which see FIG. 28-2, FIG. 28-3 and FIG. 28-4 respectively) In the case of

(15) PbGa.sub.X' M'.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, M' stands for In, Sc, Ti, Sn or Zn, X' stands for the substitution number of Ga, and Y' stands for the substitution number of In, Sc, Ti, Sn or Zn)

corresponding to the preceding formula (7), where M'=In, Tc is 230.degree. C. when the substitution number X' of Ga is 2.24 and the substitution number Y' of In is 1.2 as shown in FIG. 29-1, and the same tendency can be observed when M'=Sc, Ti, Sn or Zn (which see FIG. 29-2, FIG. 29-3, FIG. 29-4 and FIG. 29-5 respectively). Referring to Hc where M'=In, it is 700 oersted when the substitution number X' of Ga is 2.24 and the substitution number Y' is 1.2 as shown in FIG. 30-1, and the same tendency can be observed when M'=Sc, Ti, Sn or Zn (which see FIG. 30-2, FIG. 30-3, FIG. 30-4 and FIG. 30-5 respectively). In the case of

(16) Sr.sub.0.25 Pb.sub.0.75 Ga.sub.X' M'.sub.Y' Fe.sub.12-X'-(l/3)Y 'O.sub.19 (wherein, M' stands for In, Sc, Ti, Sn, Zn, Ta or Ge, X' stands for the substitution number of Ga, and Y' stands for the substitution number of In, Sc, Ti, Sn, Zn, Ta or Ge)

corresponding to the preceding formula (8), Tc where M'=In is 230.degree. C. when the substitution number X' of Ga is 2.24 and the substitution number Y' of In is 1.2 as shown in FIG. 31-1, and the same tendency can also be found when M'=Sc, Ti, Sn, Zn, Ta and Ge (which see FIG. 31-2, FIG. 31-3, FIG. 31-4, FIG. 31-5, FIG. 31-6 and FIG. 31-7). Referring to Hc where M'=In, it is 700 oersted when the substitution number X' of Ga is 2.24 and the substitution number Y' of In is 1.2 as shown in FIG. 32-1, and the same tendency can also be found when M'=Sc, Ti, Sn, Zn, Ta and Ge (which see FIG. 32-2, FIG. 32-3, FIG. 32-4, FIG. 32-5, FIG. 32-6 and FIG. 32-7). Even when Al was used in place of Ga in the preceding formulas (8).about.(16), the substantially same results as in these formulas were obtained.

The metal oxide magnetic substance according to the present invention can be prepared, in the case of the general formula I, through the steps of mixing and pulverizing at least one member of BaCO.sub.3, SrCO.sub.3 and PbCO.sub.3 with Fe.sub.2 O.sub.3, Ga.sub.2 O.sub.3 and at least one member of said M.sup.I metal oxides and if necessary at least one member of said additional metals, each being in a predetermined quantity, calcinating same at a temperature of 1000.degree..about.1100.degree. C.; thereafter pulverizing same again; placing the thus pulverized one in a propershaped mold for press-molding; and thereafter calcinating it at a temperature of 1200.degree..about.1400.degree. C. In the case of the metal oxide magnetic substance according to the general formula II, it can be prepared through the steps of mixing and pulverizing at least one member of BaCO.sub.3, SrCO.sub.3 and PbCO.sub.3 with at least one member of Fe.sub.2 O.sub.3, Ga.sub.2 O.sub.3 and Al.sub.2 O.sub.3, each being in a predetermined quantity; and thereafter subjecting it to the same procedure as employed in the manufacturing method according to the general formula I.

Concrete examples of the metal oxide magnetic substances obtained as mentioned above will be given as follows.

Metal oxide magnetic substance according to the formula I:

BaO.6[Ga.sub.0.27 In.sub.0.13 Fe.sub.1.6 O.sub.3 ]

BaO.5.9[Ga.sub.0.33 In.sub.0.17 Fe.sub.1.5 O.sub.3 ]

BaO.6[Ga.sub.0.4 In.sub.0.17 Fe.sub.1.43 O.sub.3 ]

BaO.5.5[Ga.sub.0.13 In.sub.0.15 Fe.sub.1.92 O.sub.3 ]

SrO.6[Ga.sub.0.25 In.sub.0.3 Fe.sub.1.45 O.sub.3 ]

SrO.5.5[Ga.sub.0.18 In.sub.0.05 Fe.sub.0.77 O.sub.3 ]

SrO.5.6[Ga.sub.0.09 In.sub.0.09 Fe.sub.1.82 O.sub.3 ]

BaO.6[Ga.sub.0.67 In.sub.0.08 Fe.sub.1.25 O.sub.3 ]

BaO.5.8[Ga.sub.0.52 In.sub.0.07 Fe.sub.1.41 O.sub.3 ]

SrO.5.7[Ga.sub.0.53 In.sub.0.12 Fe.sub.1.35 O.sub.3 ]

BaO.5[Ga.sub.0.2 Zn.sub.0.15 Fe.sub.1.7 O.sub.3 ]

BaO.5.6[Ga.sub.0.3 Zn.sub.0.15 Ti.sub.0.075 Fe.sub.1.5 O.sub.3 ]

BaO.5.6[Ga.sub.0.3 Zn.sub.0.3 Fe.sub.1.6 O.sub.3 ]

BaO.6[Ga.sub.0.2 Zn.sub.0.15 Ta.sub.0.075 Fe.sub.1.6 O.sub.3 ]

BaO.6[Ga.sub.0.4 Zn.sub.0.3 Fe.sub.1.4 O.sub.3 ]

SrO.5[Ga.sub.0.2 Zn.sub.0.15 Ge.sub.0.075 Fe.sub.1.6 O.sub.3 ]

SrO.5.6[Ga.sub.0.3 Zn.sub.0.15 Sn.sub.0.075 Fe.sub.1.5 O.sub.3 ]

SrO.5.6[Ga.sub.0.2 Zn.sub.0.3 Fe.sub.1.6 O.sub.3 ]

SrO.6[Ga.sub.0.2 Zn.sub.0.15 Ir0.075Fe.sub.1.6 O.sub.3 ]

SrO.6[Ga.sub.0.3 Zn.sub.0.3 Fe.sub.1.5 O.sub.3 ]

BaO.5.6[Ga.sub.0.2 Sc.sub.0.07 Fe.sub.1.73 O.sub.3 ]

BaO.6.0[Ga.sub.0.2 Sc.sub.0.08 Fe.sub.1.72 O.sub.3 ]

SrO.5.6[Ga.sub.0.2 Sc.sub.0.07 Fe.sub.1.73 O.sub.3 ]

SrO.6.0[Ga.sub.0.2 Sc.sub.0.08 Fe.sub.1.72 O.sub.3 ]

BaO.5.6[Ga.sub.0.36 Sc.sub.0.07 Fe.sub.1.57 O.sub.3 ]

BaO.6.0[Ga.sub.0.33 Sc.sub.0.08 Fe.sub.1.59 O.sub.3 ]

SrO.5.6[Ga.sub.0.38 Sc.sub.0.07 Fe.sub.1.57 O.sub.3 ]

SrO.6.0[Ga.sub.0.33 Sc.sub.0.08 Fe.sub.1.59 O.sub.3 ]

BaO.5.6[Ga.sub.0.3 Ti.sub.0.21 Fe.sub.1.42 O.sub.3 ]

BaO.6[Ga.sub.0.3 Ti.sub.0.21 Fe.sub.1.42 O.sub.3 ]

BaO.6[Ga.sub.0.2 Ru.sub.0.2 Fe.sub.1.6 O.sub.3 ]

BaO.6[Ga.sub.0.3 Ti.sub.0.3 Fe.sub.1.3 O.sub.3 ]

SrO.5.6[Ga.sub.0.3 Ti.sub.0.3 Fe.sub.1.3 O.sub.3 ]

SrO.6[Ga.sub.0.3 Ti.sub.0.3 Fe.sub.1.3 O.sub.3 ]

BaO.6[Ga.sub.0.35 Sn.sub.0.075 Zn.sub.0.15 Fe.sub.1.45 O.sub.3 ]

BaO.6[Ga.sub.0.2 Sn.sub.0.09 Fe.sub.1.68 O.sub.3 ]

BaO.6[Ga.sub.0.65 Sn.sub.0.12 Fe.sub.1.29 O.sub.3 ]

SrO.5.8[Ga.sub.0.4 Sn.sub.0.21 Fe.sub.1.32 O.sub.3 ]

SrO.6[Ga.sub.0.3 Sn.sub.0.09 Fe.sub.1.58 O.sub.3 ]

BaO.5.6[Ga.sub.0.4 Sn.sub.1.12 Fe.sub.1.44 O.sub.3 ]

Ba.sub.0.75 Sr.sub.0.25 O.6[Ga.sub.0.37 Sc.sub.0.13 Fe.sub.1.5 O.sub.3 ]

Ba.sub.0.75 Sr.sub.0.25 O.6[Ga.sub.0.37 Zn.sub.0.15 Ti.sub.0.075 Fe.sub.1.43 O.sub.3 ]

Ba.sub.0.75 Sr.sub.0.25 O.6[Ga.sub.0.3 Ti.sub.0.21 Fe.sub.1.42 O.sub.3 ]

Ba.sub.0.5 Sr.sub.0.5 O.6[Ga.sub.0.45 Sn.sub.0.075 Zn.sub.0.15 Fe.sub.1.3 O.sub.3 ]

PbO.6[Ga.sub.0.4 Cr.sub.0.15 Fe.sub.1.45 O.sub.3 ]

PbO.6[Ga.sub.0.4 Sc.sub.0.15 Fe.sub.1.45 O.sub.3 ]

PbO.6[Ga.sub.0.4 Zn.sub.0.15 Ta.sub.0.075 Fe.sub.1.40 O.sub.3 ]

PbO.6[Ga.sub.0.3 Ti.sub.0.21 Fe.sub.1.42 O.sub.3 ]

PbO.6[Ga.sub.0.4 Sn.sub.0.075 Zn.sub.0.15 Fe.sub.1.4 O.sub.3 ]

PbO.5.6[Ga.sub.0.5 In.sub.0.15 Fe.sub.1.35 O.sub.3 ]

PbO.5.6[Ga.sub.0.5 Rh.sub.0.15 Fe.sub.1.35 O.sub.3 ]

PbO.5.6[Ga.sub.0.3 Zn.sub.0.15 Ir.sub.0.075 Fe.sub.1.8 O.sub.3 ]

SrO.6[Ga.sub.0.2 Zn.sub.0.15 Ge.sub.0.075 Fe.sub.1.6 O.sub.3 ]

SrO.6[Ga.sub.0.3 Zn.sub.0.12 Fe.sub.1.62 O.sub.3 ]

SrO.6[Ga.sub.0.4 Zn.sub.0.15 Ta.sub.0.075 Fe.sub.1.4 O.sub.3 ]

SrO.6[Ga.sub.0.5 Zn.sub.0.3 Fe.sub.1.30 O.sub.3 ]

SrO.6[Ga.sub.0.35 Zn.sub.0.15 Fe.sub.1.55 O.sub.3 ]

SrO.5.5[Ga.sub.0.4 Zn.sub.0.15 Rh.sub.0.075 Fe.sub.1.4 O.sub.3 ]

SrO.5.8[Ga.sub.0.2 Zn.sub.0.21 Fe.sub.1.66 O.sub.3 ]

Pb.sub.0.5 Ba.sub.0.5 O.6[Ga.sub.0.35 In.sub.0.15 Fe.sub.1.5 O.sub.3 ]

Pb.sub.0.5 Ba.sub.0.5 O.6[Ga.sub.0.2 In.sub.0.1 Fe.sub.1.7 O.sub.3 ]

Pb.sub.0.5 Ba.sub.0.5 O.6[Ga.sub.0.35 Sc.sub.0.21 Fe.sub.1.44 O.sub.3 ]

Pb.sub.0.5 Ba.sub.0.5 O.6[Ga.sub.0.35 Sn.sub.0.21 Fe.sub.1.47 O.sub.3 ]

Pb.sub.0.5 Sr.sub.0.5 O.6[Ga.sub.0.35 In.sub.0.15 Fe.sub.1.5 O.sub.3 ]

Pb.sub.0.5 Sr.sub.0.5 O.6[Ga.sub.0.35 Zn.sub.0.15 Ti.sub.0.075 Fe.sub.1.45 O.sub.3 ]

Pb.sub.0.5 Ba.sub.0.5 O.6[Ga.sub.0.35 Ta.sub.0.21 Fe.sub.1.47 O.sub.3 ]

Pb.sub.0.5 Ba.sub.0.5 O.6[Ga.sub.0.35 Ge.sub.0.21 Fe.sub.1.47 O.sub.3 ]

Pb.sub.0.5 Sr.sub.0.5 O.6[Ga.sub.0.35 In.sub.0.15 Fe.sub.1.5 O.sub.3 ]

Pb.sub.0.5 Sr.sub.0.5 O.6[Ga.sub.0.35 Sc.sub.0.21 Fe.sub.1.44 O.sub.3 ]

PbO.6[Ga.sub.0.2 Zn.sub.0.12 Ti.sub.0.06 Fe.sub.1.64 O.sub.3 ]

SrO.6 [Ga.sub.0.08 Zn.sub.0.12 Ti.sub.0.06 Fe.sub.1.76 O.sub.3 ]

BaO.6[Ga.sub.0.2 Ir.sub.0.1 Fe.sub.1.67 O.sub.3 ]

Metal oxide magnetic substance according to the formula II:

BaO.5.6[Ga.sub.0.7 Fe.sub.1.3 O.sub.3 ]

SrO.5.6[Ga.sub.0.5 Al.sub.0.5 Fe.sub.1.0 O.sub.3 ]

BaO.5.9[Ga.sub.0.8 Fe.sub.1.2 O.sub.3 ]

BaO.5.7[Ga.sub.0.6 Fe.sub.1.6 O.sub.3 ]

BaO.5.2[Ga.sub.1.0 Fe.sub.1.0 O.sub.3 ]

BaO.5.8[Ga.sub.0.6 Fe.sub.1.4 O.sub.3 ]

SrO.5.7[Ga.sub.0.6 Fe.sub.1.4 O.sub.3 ]

SrO.5.6[Ga.sub.0.7 Fe.sub.1.3 O.sub.3 ]

SrO.5.9[Ga.sub.0.8 Fe.sub.1.2 O.sub.3 ]

PbO.5.6[Ga.sub.0.7 Fe.sub.1.3 O.sub.3 ]

PbO.5.8[Ga.sub.0.5 Fe.sub.1.5 O.sub.3 ]

BaO.5.8[Ga.sub.0.4 Al.sub.0.3 Fe.sub.1.3 O.sub.3 ]

BaO.5.7[Ga.sub.0.3 Al.sub.0.6 Fehd 1.1O.sub.3 ]

BaO.5.9[Ga.sub.0.4 Al.sub.0.2 Fe.sub.1.4 O.sub.3 ]

SrO.5.6[Ga.sub.0.4 Al.sub.0.3 Fe.sub.1.3 O.sub.3 ]

SrO.5.7[Ga.sub.0.5 Al.sub.0.3 Fe.sub.1.2 O.sub.3 ]

BaO.6Ga.sub.0.3 Fe.sub.1.7 O.sub.3 ]

Metal oxide magnetic substance according to the formula I or II, containing said additional metal:

BaO.5[Ga.sub.0.2 Ti.sub.0.075 Co.sub.0.15 Fe.sub.1.6 O.sub.3 ]

BaO.5.6[Ga.sub.0.3 Ti.sub.0.075 Cu.sub.0.15 Fe.sub.1.5 O.sub.3 ]

SrO.5[Ga.sub.0.2 Ti.sub.0.075 Ni.sub.0.15 Fe.sub.1.6 O.sub.3 ]

SrO.5.6[Ga.sub.0.3 Ti.sub.0.075 Co.sub.0.15 Fe.sub.1.5 O.sub.3 ]

SrO.6[Ga.sub.0.3 Ti.sub.0.075 Ni.sub.0.15 Fe.sub.1.5 O.sub.3 ]

BaO.5.6[Ga.sub.0.3 Sn.sub.0.075 Ni.sub.0.15 Fe.sub.1.5 O.sub.3 ]

SrO.6[Ga.sub.0.5 Sn.sub.0.075 Co.sub.0.15 Fe.sub.1.3 O.sub.3 ]

SrO 6[Ga.sub.0.4 Zn.sub.0.15 Sr.sub.0.075 Fe.sub.1.4 O.sub.3 ]

Pb.sub.0.5 Ba.sub.0.5 O.6[Ga.sub.0.35 Zn.sub.0.075 Co.sub.0.15 Fe.sub.1.45 O.sub.3 ]

Pb.sub.0.5 Ba.sub.0.5 O.6[Ga.sub.0.3 Ti.sub.0.045 Co.sub.0.9 Fe.sub.1.48 O.sub.3 ]

BaO.6[Ga.sub.0.2 Co.sub.0.12 Ti.sub.0.06 Fe.sub.1.64 O.sub.3 ]

SrO.5.7[Ga.sub.0.1 Rh.sub.0.075 Co.sub.0.15 Fe.sub.1.7 O.sub.3 ]

BaO.6[Ga.sub.0.2 Ru.sub.0.06 Co.sub.0.12 Fe.sub.1.64 O.sub.3 ]

BaO.6[Ga.sub.0.3 Ti.sub.0.06 Ni.sub.0.12 Fe.sub.1.54 O.sub.3 ]

BaO.6[Ga.sub.0.3 Ta.sub.0.075 Co.sub.0.15 Fe.sub.1.5 O.sub.3 ]

BaO.6[Ga.sub.0.05 Ti.sub.0.03 Co.sub.0.06 Fe.sub.1087 O.sub.3 ]

BaO.6[Ga.sub.0.6 Co.sub.0.1 Fe.sub.1.33 O.sub.3 ]

SrO.6[Ga.sub.0.4 Ni.sub.0.1 Fe.sub.1.53 O.sub.3 ]

PbO.6[Ga.sub.0.3 Sb.sub.0.1 Fe.sub.1.6 O.sub.3 ]

BaO.6[Al.sub.0.2 Bi.sub.0.1 Fe.sub.1.7 O.sub.3 ]

BaO.6[Al.sub.0.4 Sb.sub.0.3 Fe.sub.1.3 O.sub.3 ]

BaO.5.8[Al.sub.0.3 Co.sub.0.12 W.sub.0.06 Fe.sub.1.54 O.sub.3 ]

SrO.6[Al.sub.0.4 Sb.sub.0.3 Fe.sub.1.3 O.sub.3 ]

When intending to prepare the magnetic film using our metal oxide magnetic substance, although depending on the kind of the substrate, it is generally be prepared by adhering this magnetic substance onto the substrate so that the film thickness may be in the range of about 0.1.about.10 .mu.m, with a substrate temperature of 400.degree..about.800.degree. C. as a target and by means of vacuum vapor-deposition, sputtering, ion-plating or the like. Thus, there can be obtained a magneto optical recording medium having a vertical magnetic anisotropy-magnetic film 2 on a substrate 1. In this instance, the magnetic film may be formed at a substrate temperature of not more than 400.degree. C. as occasion demands. In this instance, however, there is the necessity of heat-treating the thus formed magnetic film at a temperature of 400.degree..about.800.degree. C., while impressing the magnetic field as the case may be, for vertical magnetization. The substrate materials used herein generally include heat-resisting metals such as aluminum and the like; quartz glass; gallium - garnet - gadolinium; saphire; lithium tantalate; crystallized transparent glass; Pyrex glass; Vycor glass; aluminosilicate glass; surface oxidationtreated or untreated single crystal silicon; transparent ceramic materials such as Al.sub.2 O.sub.3, Al.sub.2 O.sub.3.MgO, MgO.LiF, Y.sub.2 O.sub.3.LiF, BeO, ZrO.sub.2.Y.sub.2 O.sub.3, ThO.sub.2.CaO and the like; inorganic materials such as inorganic silicon materials (Goods on the market, for instance such as "Tosguard" produced by Toshiba Silicone Co. and "Sumiceram P" produced by Sumitomo Kagaku Co.) and the like; opaque ceramic materials such as Al.sub.2 O.sub.3, ZrO.sub.2 AlN; metals such as Al, steel, stainless steel; and heatresisting organic resin materials such as polyamide resin, polyimide resin, polyether sulfone and the like.

The magnetic film according to the present invention is applicable to not only the monolayer type magneto optical recording medium as shown in FIG. 33 but also all well known multilayer type magneto optical recording mediums. As these multilayer type ones, there can be enumerated those constructed as shown in FIGS. 34-37. In the drawing, reference numeral 1' denotes a substrate equipped with a guide track, 3 denotes a reflective film, 4 denotes a transparent dielectric layer, 5 denotes a guide track layer, 6 denotes a protective film, 7 denotes a transparent adhesive layer and 8 denotes a heat-resisting layer. The substrate equipped with a guide track 1' may be prepared by processing the above mentioned organic material by virtue of injection molding, extrusion molding, photoetching process or the like. The guide track of the substrate acts to guide the laser beam at the time of recording and regeneration. The reflective film 3 can be formed by adhering Cu, Al, Ag, Au, Cr, Rh, Ni, Pt, TeOx, TeC, SeAs, TeAs, TiN, TaN, CrN, cyanine dye, phthalocyanine dye, methine dye or the like on a target surface by means of vacuum vapordeposition, sputtering, ion-plating or the like so that the film thickness may be about 500-10,000 .ANG.. This reflective film is provided for the purpose of increasing Faraday effect caused by reflecting the laser beam having permeated through the magnetic film and permeating said laser beam through the magnetic film again. The transparent dielectric layer 4 is formed by adhering SiO.sub.2, SiO, TiO.sub.2 TiO, CeO, HfO.sub.2, BeO, ThO.sub.2, SiN, Si.sub.3 N.sub.4, TiN or the like on a target surface by means of the above mentioned process so that the film thickness may be about 0.05-0.5 .mu.m. This transparent dielectric layer is provided for the purpose of increasing Faraday's angle of rotation and enhancing regenerative output. The guide track layer 5 is formed by applying a ultraviolet ray-curing resin onto a target surface, thereafter radiating the ultraviolet ray thereto while press-attaching a guide grooved mold, and curing said resin. The protective layer 6 is formed by adhering acrylic resin, polyurethane resin, polycarbonate resin, polyether sulfone resin, polyamide resin, epoxy resin, TiN, SiN, Si.sub.3 N.sub.4, TaN, CrN, AlN, SiO.sub.2, SiO, TiO.sub.2 or the like on a target surface so that the resulting film thickness may be about 0.1-100 .mu.m, by means of a coating process in the case of the resin and by means of vacuum vapordeposition, sputtering, ion-plating or the like in the other case. This protective layer is provided for the purpose of protecting the surface layer, i.e. the reflective film 3 in this case. The transparent adhesive layer 7 is formed by adhering the reflective film of the substrate 1' with a guide track provided with the reflective film 3 and the magnetic film of the heat-resisting layer 8 provided with the magnetic film 2 (said heat-resisting layer 8 comprises said inorganic material, and therefore "the heat-resisting layer provided with the magnetic film "corresponds to aforesaid monolayer type magneto optical recording medium.) using epoxy resin, polyurethane resin, polyamide resin or the like so as to have a thickness of about 0.1-10 .mu.m. Accordingly, this transparent adhesive may be said to be a mere layer for connecting the reflective film 3 on the substrate 1' with the magnetic film 2 consisting of the monolayer type magneto optical recording medium. In this connection, it is to be noted that the heatresisting layer 8, which is consisted of the aforesaid inorganic material, corresponds to the substrate 1, but is provided herein for the purpose of enhancing the heat-resisting property of the magnetic film 2. The suitable thickness thereof is about 0.1-2 mm.

The protective film 6 may be provided not only for the surface of the recording medium as shown in FIG. 36 but also on the surface of the recording medium shown in FIGS. 33-35 and 37. In order to improve the vertical magnetic anisotropic property of the magnetic film, furthermore, there may be used the substrates treated with ZnO, .alpha.-Fe.sub.2 O.sub.3, .alpha.-Al.sub.2 O.sub.3, AlN, SiO.sub.2, MgO, MnZn-ferrite or the like.

The above mentioned magneto optical recording medium using magnetic film according to the present invention is subjected to recording and regeneration in the manner of radiating a modulated or deflected laser beam from the side of the magnetic film or substrate as usually done.

The metal oxide magnetic substance or magnetic film according to the present invention has proper Tc and Hc required for the magneto optical recording medium material and is of a high recording sensitivity. In spite of this, it has the oxidizing corrosion resistance and transparency which could not be observed in the usual one, and therefore is free from deterioration in the magneto optical characteristics with a lapse of time and can use a transmitted light on regeneration. Thus, regeneration can be effected in the manner of making use of Faraday's angle of rotation which is high in regenerative output. Still further, the metal oxide magnetic substance or magnetic film according to the present invention can be used also in the perpendicular magnetic recording medium (which structure is basically identical with that of said monolayer type magneto optical recording medium). In this instance, however, as the preferable metal oxide magnetic substances there are enumerated those being low in the metal substitution numbers X and Y, and T, in particular those satisfying 0<X.ltoreq.0.2 and 0<Y.ltoreq.0.2 in the formula I, and 0<T.ltoreq.0.4 in the formula II.

FIG. 1, FIG. 2, FIG. 3, FIG. 4, FIG. 5, FIGS. 6-1.about.4, FIGS. 7-1.about.5 and FIG. 8-1.about.7 are each a relational diagram between the substitution number Z of M' and the Curie temperature Tc in each of the following metal oxide magnetic substances:

(1) BaFe.sub.12-(l/3)z M'.sub.z O.sub.19 (wherein, M' stands for Ga or In, Z stands for the substitution number of M', and l stands for the ionic valency of M'),

(2) BaFe.sub.12-(l/3)z M'.sub.z O.sub.19 (wherein, M' stands for Ga or Zn, Z stands for the substitution number of M', and l stands for the ionic valency of M'),

(3) BaFe.sub.12-(l/3)z M'.sub.z O.sub.19 (wherein, M' stands for Ga or Sc, Z stands for the substitution number of M', and l stands for the ionic valency of M'),

(4) BaFe.sub.12-(l/3)z M'.sub.z O.sub.19 (wherein, M' stands for Ga or Ti, Z stands for the substitution number of M', and l stands for the ionic valency of M'),

(5) BaFe.sub.12-(l/3)z M'.sub.z O.sub.19 (wherein, M' stands for Ga or Sn, Z stands for the substitution number of M', and l stands for the ionic valency of M'),

(6) Ba.sub.0.75 Sr.sub.0.25 Fe.sub.12-(l/3)z M'.sub.z O.sub.19 (wherein, M' stands for Ga, Sc, Ti, Sn or Zn, Z stands for the substitution number of M', and l stands for the ionic valency of M'),

(7) PbFe.sub.12-(l/3)z M'.sub.z O.sub.19 (wherein, M' stands for Ga In, Sc, Ti, Sn or Zn, Z stands for the substitution number of M', and l stands for the ionic valency of M'), and

(8) Sr.sub.0.25 Pb.sub.0.75 Fe.sub.12-(l/3)z M'.sub.z O.sub.19 (wherein M' stands for Ga, In, Sc, Ti, Sn, Zn, Ta or Ge, Z stands for the substitution number of M' and l stands for the ionic valency of M');

FIG. 9, FIG. 10, FIG. 11, FIG. 12, FIG. 13, FIGS. 14-1.about.4, FIGS. 15-1.about.5, and FIGS. 16-1.about.7 are each a relational diagram between the substitution number of M' and the coercive force Hc of M' in each of said metal oxide magnetic substances: (1).about.(8);

FIG. 17, FIG. 19, FIG. 21, FIG. 23, FIG. 25, FIGS. 27-1.about.4, FIGS. 29-1.about.5 and FIGS. 31-1.about.7 are each a relational diagram between the following Y' and the Curie temperature Tc in each of the following metal oxide magnetic materials:

(9) BaGa.sub.X' In.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, X' stands for the substitution number of Ga, and Y' stands for the substitution number of In),

(10) BaGa.sub.X' Zn.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, X' stands for the substitution number of Ga and Y' stands for the substitution number of Zn),

(11) BaGa.sub.X' Sc.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, X' stands for the substitution number of Ga and Y' stands for the substitution number of Sc),

(12) BaGa.sub.X' Ti.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, X' stands for the substitution number of Ga and Y' stands for the substitution number of Ti),

(13) BaGa.sub.X' Sn.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, X' stands for the substitution number of Ga and Y' stands for the substitution number of Sn),

(14) Ba.sub.0.75 Sr.sub.0.25 Ga.sub.X' M'.sub.Y' Fe.sub.12-X40 -(l/3)Y' O.sub.19 (wherein, M' stands for Sc, Ti, Sn or Zn, X' stands for the substitution number of Ga and Y' stands for the substitution number of M'),

(15) PbGa.sub.X' M'.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, M' stands for In, Sc, Ti, Sn or Zn, X' stands for the substitution number of Ga and Y' stands for the substitution number of M') and

(16) Sr.sub.0.25 Pb.sub.0.75 Ga.sub.X' M'.sub.Y' Fe.sub.12-X'-(l/3)Y' O.sub.19 (wherein, M' stands for In, Sc, Ti, Sn, Zn, Ta or Ge, X' stands for the substitution number of Ga and Y' stands for the substitution number of M');

FIG. 18, FIG. 20, FIG. 22, FIG. 24, FIG. 26, FIGS. 28-1.about.4, FIGS. 30-1.about.5 and FIG. 32-1.about.7 are each a relational diagram between said Y' and the coercive force Hc in each of said metal oxide magnetic substances(9)-(16); and

FIG. 33 to FIG. 37 are each a block diagram illustrating one example of the magneto optical recording medium using the magnetic substance or magnetic film according to the present invention.

1 . . . substrate

1'. . . substrate equipped with a guide track

2 . . . magnetic film

3 . . . reflective film

4 . . . transparent dielectric layer

5 . . . guide track layer

6 . . . protective layer

7 . . . transparent adhesive layer

8 . . . heat-resisting layer

Examples of the present invention will be given as follows.

A quartz substrate, whose surface had been abrasion-treated optically, was subjected to 2 hours' sputtering the respective targets consisting of metal oxide magnetic substances shown in the following table under the conditions of Ar partial pressure: 2.0 mm Torr, O.sub.2 partial pressure: 0.3 mm Torr, discharge electric power: 0.35 KW and substrate temperature: 620.degree. C. to thereby form 0.5 .mu.m-thick magnetic films thereon. The results obtained by measuring there magnetic films with reference to Curie temperature Tc and coercive force Hc will be shown in the following table.

Next, each of the thus obtained magneto optical recording mediums was magnetized in one direction by applying a magnetic field of 10K oersted perpendicular to the surface of each recording medium. In succession, recording was carried out by radiating a semi-conductor laser beam having an output of 20 mW from the substrate side under the contition of luminous intensity on the recording medium surface: 10 mW and at a pulse of frequency: 1 mHz, while impressing a magnetic field of 0.5K oersted opposite to said magnetized direction, for magnetic inversion. On every recoriing medium, there was formed a recorded bit having a diameter of about 1.5 .mu.m.

A GGG substrate was subjected to 2 hours' sputtering using SiO.sub.2 under the conditions of Ar partial pressure: 2.times.10.sup.-2 Torr, O.sub.2 partial pressure: 2.times.10.sup.-2 Torr, discharge electric power: 0.4 KW, and substrate temperature: 300.degree. C. to thereby provide a 1000.ANG.-thick undercoat thereon, thereafter same was subjected to 3 hours' sputtering using BaO.6[Ga.sub.0.2 CO.sub.0.12 Ti.sub.0.06 Fe.sub.1.64 O.sub.3 ]under the conditions of Ar partial pressure: 2.times.10.sup.-3 Torr, O.sub.2 partial pressure: 2.times.10.sup.-4 Torr, discharge electric power: 0.4 KW, and substrate temperature: 550.degree. C. to thereby provide a 1.mu.m-thick magnetic film on said undercoat, and further same was subjected to 0.5 hour's vapordeposition using Al under the condition of substrate temperature: 300.degree. C., to thereby provide a 1000.ANG.-thick reflective film thereon. The magnetic characteristics of the thus obtained magneto optical recording medium were superior, i.e. Tc= 300.degree. C. and Hc=1800 Oe.

Next, this recording medium was magnetized in a fixed direction according to the same procedure as in Example 1, and thereafter recording medium was carried out by radiating a semi-conductor laser beam having an output of 20 mW from the substrate side under the condition of luminous intensity on the recording medium surface: 10 mW and at a pulse of frequency: 0.1 MHz, while impressing a magnetic field, to thereby form a recorded bit having a diameter of about 1.5.mu.m on the recording medium.

This recording medium was left standing for 7 days in the atmosphere of 100.degree. C. in order to measure its preservability. However, no substantial change was observed in the magnetic characteristics.

On the other hand, for comparison's sake there was prepared a magneto optical recording medium according to the exactly same procedure as this Example except that a 0.5.mu.m-thick magnetic film consisting of an amorphous alloy magnetic substance was formed using Tb.sub.0.24 F.sub.0.76 as the magnetic target. Next, this control recording medium was subjected to 7 days' preservability test at 100.degree. C. likewise to find that during the test, oxidation and crystallization took place and consequently the magnetic characteristics deteriorated markedly.

The results obtained from the preservability tests of both magneto optical recording medium are as shown below.

The above data were obtained from the substrate side portion of each magnetic film.

A magneto optical recording medium was prepared according to the exactly same procedure as in Example 104 except that BaO.6[Ga.sub.0.3 Fe.sub.1.7 O.sub.3 ] was used as the magnetic target. The magnetic characteristics of this recording medium were superior, i.e. Tc=330.degree. C. and Hc=3500 Oe .

This magneto optical recording medium was subjected to 7 days' preservability test at 100.degree. C. likewise in Example 104 to obtain the results concerning Faraday's angle of rotation: 2.theta..sub.F as initial value=0.43 degree and 2.theta..sub.F after acceleration test under 90.degree. C. and 80%RH=0.41 degree.

A magneto optical recording medium was formed on a monocrystal Si wafer substrate using SrO.5.7[Ga.sub.0.1 Rh.sub.0.075 Co.sub.0.15 Fe.sub.1.7 O.sub.3 ] as the magnetic target and according to the same procedure as in Example 104. The magnetic characteristics of this recording medium were superior, i.e. Tc=350.degree. C. and Hc=3000 Oe.

This magneto optical recording medium was subjected to one month's preservability test under the same condition (acceleration test under 90.degree. C. and 80%RH) as in Example 104 to thereby obtain the result concerning Faraday's angle of rotation that 2.theta..sub.F after acceleration preserving was 1.55 degree, while 2.theta..sub.F as initial value was 1.60 degree.

A magneto optical recording medium was prepared according to the exactly same procedure as in Example 104 except that PbO.6[Ga.sub.0.2 Zn.sub.0.12 Ti.sub.0.06 Fe.sub.1.64 O.sub.3 ] was used as the magnetic target. The magnetic characteristics of this recording medium were superior, i.e. Tc=310.degree. C. and Hc=1500 Oe.

This magneto optical recording medium was subjected to the same acceleration preservability test as in Example 104 to find that 2.theta..sub.F as the initial value of Faraday's angle of rotation was 0.38 degree and 2.theta..sub.F after acceleration was 0.35 degree

A 1000.ANG.-thick SiO.sub.2 undercort was provided on a substrate consisting of a crystalliyed glass (Trade name: Microlan produced by Nihon Gaishi K.K.) under the same conditions as in Example 104, and same was subjected to 2 hours' sputtering using ZnO under the conditions of discharge electlic power: 80 W, Gas pressure: 4.times.10.sup.-2 Torr, P.sub.Ar /P.sub.02 =1/1 (P.sub.Ar : Ar partial pressure, P.sub.02 : O.sub.2 partial pressure) and substrate temperature: 300.degree. C. to thereby form a 3000.ANG.- thick undercoat further on said SiO.sub.2 undercoat. Thereafter, a 1.mu.m -thick magnetic film was formed on this undercoat by sputtering a magnetic target consisting of BaO.6[Ga.sub.0.2 Ru.sub.0.06 Co.sub.0.12 Fe.sub.1.64 O.sub.3 ] under the conditions of Ar partial pressure: 2.times.10.sup.-3 Torr, O.sub.2 partial pressure: 2.times.10.sup.-4 Torr, discharge electric power: 0.4 KW and substrate temperature: 570.degree. C., and a 500.ANG. - thick reflective film was formed on said magnetic film by vapor-depositing Au for 1 hour under the conditions of atmospheric gas pressure: 1.times.10.sup.-5 Torr and substrate temperature: 400.degree. C. The thus obtained magneto optical recording medium was superior in magnetic characteristics, i.e. Tc=320.degree. C. and Hc=2000 Oe.

Further, this magneto optical recording medium was subjected to acceleration preservability test under the same concitions as in Example 104 to find that its initial value of Faraday's angle of rotation (2.theta..sub.F) was 1.5 degree and 2.theta..sub.F after the lapse of one month was 1.4 degree.

A magneto optical recording medium was prepared according to the exactly same procedure as in Example 104 except that BaO.6[Ga.sub.0.3 Ti.sub.0.06 Ni.sub.0.12 Fe.sub.1.54 O.sub.3 ] was used as the magnetic target. The magnetic characteristics of this recording medium were superior, i.e. Tc=280.degree. C. and Hc=1800 Oe.

This magneto optical recording medium was further subjected to preservability test under the same conditions as in Example 104 to find that its initial value of Faraday's angle of rotation (2.theta..sub.F) was 0.46 degree and 2.theta..sub.F after the lapse of one month was 0.42 degree.

A magneto optical recording medium was prepared according to the exactly same procedure as in Example 104 except that the SiO.sub.2 used for the formation of the first undercoat was replaced by AlN and BaO.6[Ga.sub.0.3 Ta.sub.0.075 Co.sub.0.15 Fe.sub.1.5 O.sub.3 ] was used as the magnetic target. The magnetic characteristics of this recording medium were superior, i.e. Tc=280.degree. C. and Hc=2500 Oe.

This magneto optical recording medium was subjected to preservability test under the same conditions as in Example 104 to find that the initial value of Faraday's angle of rotation (2.theta..sub.F) was 1.6 degree and 2.theta..sub.F after the lapse of one month was 1.5 degree.

A 2000.ANG.- thick ZnO film was formed on a monocrystal Si wafer substrate through 1 hour's sputtering using ZnO under the conditions of atmospheric oxygen pressure: 2.times.10.sup.-3 Torr and substrate temperature: 400.degree. C., and same was subjected to 2 hours' sputtering using MnO.sub.0.6 ZnO.sub.0.4 Fe.sub.2 O.sub.3 under the conditions of atmospheric gas pressure: 2.times.10.sup.-3 Torr (P.sub.Ar /P.sub.02 =1.8/0.2.times.10.sup.-3 torr) and substrate temperature 450.degree. C., to thereby form thereon a 5000.ANG.- thick MnO.sub.0.6 ZnO.sub.0.4 Fe.sub.2 O.sub.3 film. The same was subjected to 2 hours' sputtering using a magnetic target BaO.6[Ga.sub.0.05 Ti.sub.0.03 Co.sub.0.06 Fe.sub.1.87 O.sub.3 ] under the conditions of atmospheric gas pressure: 2.times.10.sup.-3 Torr (O.sub.2 /Ar ratio=1/6) and substrate temperature: 570.degree. C. to thereby adhere a 5000.ANG.- thick magnetic film. Thus, there was obtained a parpendicular magnetic recording medium. Recording was carried out using a ferrite ring head (the winding number N=50T) having a gap width 0.4 .mu.m under the condition of relative spped between the medium and the head=1.51 m/s. The thus obtained recording density D.sub.50 was 87.6 KFRPI.

A parpendicular magnetic recording medium was prepared according to the exactly same procedure as in Example 111 except that alumina was used as the substrate material and SrO.6[Ga.sub.0.08 Zn.sub.0.12 Ti.sub.0.06 Fe.sub.1.76 O.sub.3 ] was used as the magnetic target. This recording medium was found to have a recording density: D.sub.50 =60.0 KFRPI.