JP5748639B2 - Magnetron sputtering target and method for manufacturing the same - Google Patents

Description

  The present invention relates to a magnetron sputtering target having a ferromagnetic metal element and a method for producing the same.

  In magnetron sputtering, a magnet is arranged on the back surface of a target, and plasma is concentrated at high density by leakage magnetic flux leaking to the front surface side of the target. Thereby, stable high-speed sputtering is enabled.

  For this reason, a target used for magnetron sputtering is required to increase the amount of leakage magnetic flux leaking to the surface side of the target.

  For example, Patent Document 1 discloses a magnetron sputtering target having Co, which has a magnetic phase containing Co, a nonmagnetic phase containing Co, and an oxide phase, and the magnetic phase and the nonmagnetic phase. And the oxide phase are dispersed in each other, the magnetic phase contains Co and Cr as main components, and the Co content in the magnetic phase is from 76 at% to 80 at% A sputtering target or a magnetron sputtering target having Co, comprising a magnetic phase containing Co and a nonmagnetic phase containing Co, wherein the magnetic phase and the nonmagnetic phase are dispersed with each other, The nonmagnetic phase is a Pt—Co alloy phase containing Pt as a main component, and the Co content in the Pt—Co alloy phase is greater than 0 at% and less than or equal to 13 at%. It describes a magnetron sputtering target, wherein the door.

  These magnetron sputtering targets can increase the amount of leakage magnetic flux from the target surface during magnetron sputtering without reducing the content of Co, which is a ferromagnetic metal element contained in the target. It can be done well.

Japanese Patent No. 4422203

  However, there is a need to further increase the amount of leakage magnetic flux during magnetron sputtering without reducing the content of the ferromagnetic metal element contained in the target.

  The present invention has been made in view of the above points, and it is possible to increase the amount of magnetic flux leakage during magnetron sputtering more than before without reducing the content of the ferromagnetic metal element contained in the target. It is an object to provide a sputtering target and a manufacturing method thereof.

The present invention relates to a magnetron sputtering target having a ferromagnetic metal element, the magnetic phase containing the ferromagnetic metal element, and a plurality of non-components containing the ferromagnetic metal element and having different constituent elements or their content ratios. and magnetic phase, a magnetron sputtering target for chromatic and oxide phase, when the shape of Fai152.4Mm × thickness 7.0 mm, the average leakage magnetic flux rate based on ASTM F2086-01 is 50% or more The above-described problems are solved by a magnetron sputtering target.

  The “magnetic phase” is a phase having magnetism (excluding a phase having a sufficiently small magnetism compared to a normal magnetic material), and the “non-magnetic phase” is zero in magnetism. It is a concept that includes not only phases but also phases that are sufficiently smaller in magnetism than ordinary magnetic materials.

  According to the present invention, by providing a plurality of nonmagnetic phases containing a ferromagnetic metal element and having different constituent elements or their content ratios, the amount of the ferromagnetic metal element in the entire target is kept constant. The volume fraction of the magnetic phase containing the ferromagnetic metal element with respect to the entire target can be reduced, and the magnetism of the entire target can be reduced. Thereby, without decreasing the content of the ferromagnetic metal element contained in the target, the amount of leakage magnetic flux from the target surface can be increased during magnetron sputtering, and magnetron sputtering can be performed satisfactorily.

  The plurality of nonmagnetic phases can be, for example, two types of nonmagnetic phases.

  The ferromagnetic metal element is, for example, Co. In this case, when magnetron sputtering is performed using the target, it is easy to obtain a magnetic recording medium having excellent magnetic recording characteristics.

  The magnetic phase can be, for example, a Co—Cr alloy phase containing Co and Cr as main components. In this case, the volume fraction of the nonmagnetic phase with respect to the entire target is increased and the volume fraction of the magnetic phase is decreased. In view of increasing the amount of leakage magnetic flux from the target surface, the Co content in the magnetic phase is preferably 85 at% or more. Furthermore, in the above point, it is more preferable that the magnetic phase is a phase composed of simple Co.

  At least one of the nonmagnetic phases is a Co—Cr alloy phase in which the Co content is greater than 0 at% and less than or equal to 75 at% or the Co content ratio is greater than 0 at% and less than 73 at%. The Pt alloy phase is preferable, and at least one of the nonmagnetic phases is preferably a Co—Pt alloy phase having a Co content of 12 at% or less.

The oxide phase is, for _{example, SiO 2, TiO 2, Ti} 2 O 3, Ta 2 O 5, Cr 2 O 3, CoO, Co 3 O 4, B 2 O 5, Fe 2 O 3, CuO, Y 2 At least one of O ₃ , MgO, Al ₂ O ₃ , ZrO ₂ , Nb ₂ O ₅ , MoO ₃ , CeO ₂ , Sm ₂ O ₃ , Gd ₂ O ₃ , WO ₂ , WO ₃ , HfO ₂ , NiO ₂ It can include seeds.

  Some of the targets can be suitably used for forming a magnetic recording layer.

The target includes, for example, a magnetron using a magnetic metal powder containing a ferromagnetic metal element, a plurality of nonmagnetic metal powders containing the ferromagnetic metal element and having different constituent elements or different content ratios, and an oxide powder. This is a method for producing a sputtering target, and when the shape of the obtained magnetron sputtering target is φ152.4 mm × thickness 7.0 mm, the average leakage magnetic flux rate based on ASTM F2086-01 of the obtained magnetron sputtering target is The magnetron sputtering target can be manufactured by the method for manufacturing a magnetron sputtering target, which is 50% or more .

  Here, the magnetic metal powder is a powder having magnetism (except for a powder having a sufficiently small magnetism compared with a normal magnetic material), and the non-magnetic metal powder is a powder having zero magnetism. In addition, it is a concept that includes a powder that is sufficiently smaller in magnetism than a normal magnetic material.

  The plurality of nonmagnetic metal powders can be, for example, two types of nonmagnetic metal powders.

  The ferromagnetic metal element is, for example, Co. In this case, when magnetron sputtering is performed using the target manufactured by the manufacturing method, a magnetic recording medium having excellent magnetic recording characteristics can be easily obtained.

  It is preferable that the magnetic metal powder contains Co and Cr as main components and the Co content in the magnetic metal powder is 85 at% or more in terms of improving the leakage magnetic flux rate of the target to be manufactured. The powder is more preferably composed of simple Co.

  At least one of the plurality of non-magnetic metal powders is a Co—Cr alloy having a Co content ratio of greater than 0 at% and 75 at% or less, or a Co—Cr alloy having a Co content ratio of greater than 0 at% and less than 73 at%. -Pt alloy is preferable, and at least one of the plurality of nonmagnetic metal powders is preferably made of a Co-Pt alloy having a Co content of 12 at% or less.

  According to the present invention, it is possible to increase the amount of magnetic flux leakage from the target surface during magnetron sputtering without reducing the content of the ferromagnetic metal element contained in the target, and to improve magnetron sputtering. It can be carried out.

Example metal micrograph showing the microstructure of a target according to this embodiment A graph showing the relationship between the Co content and magnetism in a Co-Cr alloy The graph which shows the relationship between the content rate of Co, and magnetism in a Co-Pt alloy Metal micrograph of the cross section of a sintered compact obtained by pressure sintering magnetic mixed powder Metal micrograph of a cross section of a sintered body obtained by pressure sintering the first magnetic mixed powder Metal micrograph of cross section of sintered body obtained by pressure sintering second magnetic mixed powder Metal micrograph of cross section of sintered body obtained by pressure sintering second magnetic mixed powder Metallic micrograph (low magnification) of the cross section in the thickness direction of the test piece of Example 1 Metal micrograph (high magnification) of thickness direction cross section of test piece of Example 1 SEM photograph of cross section in thickness direction of test piece of Example 1 (low magnification) SEM photograph of cross section in thickness direction of test piece of Example 1 (high magnification) Metal micrograph (low magnification) of thickness direction cross section of test piece of Example 2 Metal micrograph (high magnification) of thickness direction cross section of test piece of Example 2 SEM photograph of cross section in thickness direction of test piece of Example 2 (low magnification) SEM photograph of cross section in thickness direction of test piece of Example 2 (high magnification) Metallic micrograph (low magnification) of the cross section in the thickness direction of the test piece of Comparative Example 1 Metallic micrograph (high magnification) of the cross section in the thickness direction of the test piece of Comparative Example 1 SEM photograph of cross section in thickness direction of test piece of Comparative Example 1 (low magnification) SEM photograph of cross section in thickness direction of test piece of Comparative Example 1 (high magnification) Metal micrograph of the cross section in the thickness direction of the test piece of Comparative Example 2 (low magnification) Metallic micrograph (high magnification) of the cross section in the thickness direction of the test piece of Comparative Example 2 SEM photograph of cross section in thickness direction of test piece of Comparative Example 2 (low magnification) SEM photograph of cross section in thickness direction of test piece of Comparative Example 2 (high magnification) Metallic micrograph (low magnification) of the cross section in the thickness direction of the test piece of Comparative Example 3 Metallic micrograph (high magnification) of the cross section in the thickness direction of the test piece of Comparative Example 3 Metal micrograph (low magnification) of cross section in thickness direction of test piece of Comparative Example 5 Metal micrograph of the cross section in the thickness direction of the test piece of Comparative Example 5 (high magnification)

  The magnetron sputtering target according to the present invention is a magnetron sputtering target having a ferromagnetic metal element, and includes a magnetic phase containing the ferromagnetic metal element, the ferromagnetic metal element, and a constituent element or its inclusion It has a plurality of nonmagnetic phases and oxide phases having different ratios.

  In the present invention, by providing a plurality of nonmagnetic phases containing a ferromagnetic metal element and having different constituent elements or their content ratios, the content ratio of each constituent element including the ferromagnetic metal elements in the entire target is kept constant. In addition, the volume fraction of the nonmagnetic phase with respect to the entire target can be increased, and the volume fraction of the magnetic phase with respect to the entire target can be decreased. Thereby, the magnetism of the whole target can be weakened, the amount of leakage magnetic flux from the target surface can be increased during magnetron sputtering, and magnetron sputtering can be performed satisfactorily.

  For example, as described later, in a Co—Cr alloy, the magnetism is almost zero when the Co content is 75 at% or less, and in the Co—Pt alloy, the magnetism is almost zero when the Co content is 12 at% or less. become. Therefore, when the metal elements contained in the target are three elements of Co, Cr, and Pt, the nonmagnetic phase is one phase of a Co—Cr alloy phase in which the Co content is 75 at% or less or the Co content is 12 at% or less. The non-magnetic phase is composed of two phases: a Co—Cr alloy phase having a Co content of 75 at% or less and a Co—Pt alloy phase having a Co content of 12 at% or less. In this case, the volume fraction of the nonmagnetic phase relative to the entire target can be increased while the composition of the entire target is kept constant, and the volume fraction of the magnetic phase relative to the entire target can be decreased.

  In this way, the nonmagnetic phase containing the ferromagnetic metal element is changed to a plurality of nonmagnetic phases having different constituent elements or their content ratios, so that the composition of the entire target is constant compared to the case where the number of nonmagnetic phases is one. The volume fraction of the non-magnetic phase with respect to the entire target can be increased while the volume of the target is maintained, and the volume fraction of the magnetic phase with respect to the entire target can be decreased, thereby reducing the magnetism of the entire target.

  If the volume fraction of the nonmagnetic phase with respect to the entire target is increased while keeping the composition of the entire target constant, the volume fraction of the magnetic phase decreases and the content of the ferromagnetic metal element in the magnetic phase increases. However, as will be described later, for example, in a Co—Cr alloy, when the Co content is 85 at% or more, the magnetism is about the same as that of Co alone, and even if the Co content is further increased, the magnetism is about the same. Keep. Therefore, if the content of the ferromagnetic metal element in the magnetic phase exceeds a certain value, even if the content of the ferromagnetic metal element in the magnetic phase is further increased, the magnetism of the magnetic phase will not increase significantly. . For this reason, even if the content ratio of the ferromagnetic metal element in the magnetic phase is increased, the volume fraction of the non-magnetic phase with respect to the entire target is increased, and the volume fraction of the magnetic phase with respect to the entire target is decreased, thereby reducing the target volume. The magnetism as a whole can be weakened.

  Further, the magnetron sputtering target according to the present invention has a ferromagnetic metal element, and therefore can be used for the production of a magnetic recording medium. The ferromagnetic metal element applicable to the present invention is not particularly limited, and for example, Co, Fe, and Ni can be used. When Co is used as the ferromagnetic metal element, a recording layer (magnetic layer) having a large coercive force can be formed, which can be a suitable target for manufacturing a hard disk.

  Further, in the magnetron sputtering target according to the present invention, the metal elements other than the ferromagnetic metal elements contained in the magnetic phase and the nonmagnetic phase are not particularly limited. For example, Cr, Pt, Au, Ag, Ru, Rh, Pd , Ir, W, Ta, Cu, B, Mo, and other metal elements can be included in the magnetic phase and / or the nonmagnetic phase.

In the following, Co—Cr—Pt—SiO ₂ that can be suitably used for the production of a magnetic recording layer.
A —TiO ₂ —Cr ₂ O ₃ target is taken up as an embodiment of the present invention and will be described in detail. In this embodiment, the metal phase has a three-phase structure composed of one magnetic phase and two nonmagnetic phases, but the metal phase has four or more phases composed of one magnetic phase and three or more nonmagnetic phases. A multiphase structure can also be used.

1. Component of target The component of the target according to the present embodiment is Co—Cr—Pt—SiO ₂ —TiO ₂ —Cr ₂ O ₃ . Co, Cr, and Pt become magnetic particles (fine magnets) in the granular structure of the magnetic recording layer formed by sputtering. Oxides (SiO ₂ , TiO ₂ , Cr ₂ O ₃ ) form a nonmagnetic matrix that partitions magnetic particles (fine magnets) in a granular structure.

The content ratio of metal (Co, Cr, Pt) and the content ratio of oxide (SiO ₂ , TiO ₂ , Cr ₂ O ₃ ) with respect to the entire target is determined by the component composition of the target magnetic recording layer, and the metal with respect to the entire target. (Co, Cr, Pt) content is 88～94Mol% of content ratio of the oxide to the total target _{(SiO 2, TiO 2, Cr} 2 O 3) is 6~12mol%.

  Co is a ferromagnetic metal element, and plays a central role in the formation of granular magnetic particles (fine magnets) in the magnetic recording layer. The content ratio of Co is 60 to 80 at% with respect to the entire metal (Co, Cr, Pt).

  Cr has a function of reducing the magnetic moment of Co by alloying with Co in a predetermined composition range, and has a role of adjusting the magnetic strength of the magnetic particles. The content ratio of Cr is 4 to 24 at% with respect to the entire metal (Co, Cr, Pt).

  Pt has a function of increasing the magnetic moment of Co by alloying with Co in a predetermined composition range, and has a role of adjusting the magnetic strength of the magnetic particles. The content ratio of Pt is 1 to 22 at% with respect to the entire metal (Co, Cr, Pt).

In this embodiment, SiO ₂ , TiO ₂ , and Cr ₂ O ₃ are used as oxides. However, oxides to be used are not limited to SiO ₂ , TiO ₂ , and Cr ₂ O _3. For example, SiO ₂ , TiO _{2 are used.} Ti ₂ O ₃ , Ta ₂ O ₅ , Cr ₂ O ₃ , CoO, Co ₃ O ₄ , B ₂ O ₅ , Fe ₂ O ₃ , CuO, Y ₂ O ₃ , MgO, Al ₂ O ₃ , ZrO ₂ , An oxide containing at least one of Nb ₂ O ₅ , MoO ₃ , CeO ₂ , Sm ₂ O ₃ , Gd ₂ O ₃ , WO ₂ , WO ₃ , HfO ₂ , and NiO ₂ can also be used.

2. Microstructure of target The microstructure of the target according to the present embodiment is a magnetic phase (Co content is 85 at% or more as shown in FIG. 1 (SEM photograph of the cross section in the thickness direction of the target of Example 1)). Co—Cr alloy phase), a first nonmagnetic phase (Co—Cr—Pt alloy phase having a Co content of greater than 0 at% and not more than 73 at%), and a second nonmagnetic phase (Co content of 0 at The Co—Pt alloy phase of greater than 12% and 12 at% or less) is dispersed in each other and is partitioned by the oxide phase and is not in contact with each other. In this embodiment, the magnetic phase (Co—Cr alloy phase having a Co content of 85 at% or more) may be a Co single phase having a Co content of 100 at%, and the Co content is 85 at% or more. The Co—Cr alloy phase includes a single Co phase having a Co content of 100 at%.

In FIG. 1, reference numeral 10 denotes a target according to the present embodiment, a phase indicated by reference numeral 12 (gray gray and relatively large phase) is a magnetic phase (Co phase), and a phase indicated by reference numeral 14 (magnetic phase 12 and second non-phase). The intermediate gray phase of the magnetic phase 16 is the first nonmagnetic phase (69Co-22Cr-9Pt alloy phase), and the phase indicated by the reference numeral 16 (the most whitish phase) is the second nonmagnetic phase (5Co -95Pt alloy phase), portion indicated by reference numeral 18 (dark gray, sites and partitions between the metal phase) is oxide phase _{(SiO 2 -TiO 2 -Cr 2 O} 3 phase).

  The metal phase is not a single phase of the Co—Cr—Pt alloy phase, but one magnetic phase (Co—Cr alloy phase with a Co content of 85 at% or more) and two nonmagnetic phases (Co content of 0 at%). A three-phase structure composed of a Co—Cr—Pt alloy phase of greater than 73 at% and a Co—Pt alloy phase of Co content greater than 0 at% and less than 12 at%. It is possible to reduce the volume fraction of the magnetic phase with respect to the entire target while keeping the content ratio of each constituent element including the element constant. This makes it possible to weaken the magnetism of the entire target while keeping the content ratio of each constituent element in the entire target constant, and to increase the amount of leakage magnetic flux from the target surface during magnetron sputtering. Sputtering can be performed satisfactorily.

  In the present embodiment, the reason why the Co content ratio is set to 85 at% or more in the Co—Cr alloy phase that is the magnetic phase will be described.

  Table 1 below shows the experimental results of tensile stress on a magnetic evaluation scale measured by changing the Co content ratio in a Co—Cr alloy (magnetism increases as the value of tensile stress increases, as will be described later). FIG. 2 is a graph of the following Table 1, and is a graph showing the relationship between the Co content and magnetism in a Co—Cr alloy, with the horizontal axis representing the Co content and the vertical axis representing the Co content. This is the tensile stress of the magnetic evaluation scale.

  As shown in Table 1 and FIG. 2, in the Co—Cr alloy, when the Co content is 75 at% or less, the Co—Cr alloy has almost zero magnetism, and when the Co content exceeds 75 at%, Begins to increase rapidly, and when the Co content is 83 at% or more, the increase in magnetism becomes moderate and becomes a substantially constant value. Therefore, in a Co—Cr alloy that is a magnetic phase, even if the Co content is increased from 83 at%, the magnetism is hardly increased as compared to when the Co content is 83 at% or more.

  Therefore, in the present embodiment, the Co content in the Co—Cr alloy phase is set to 85 at% or more, and the Co— which is the magnetic phase is hardly increased compared with the case where the Co content is 83 at%. The content ratio of Co in the Cr alloy phase is increased. The larger the Co content in the Co—Cr alloy phase, the smaller the volume fraction of the Co—Cr alloy phase, which is the magnetic phase, while keeping the amount of Co in the entire target constant, and the nonmagnetic phase (the Co content is less The volume fraction of the Co—Cr—Pt alloy phase of greater than 0 at% and less than 73 at%, and the Co—Pt alloy phase of Co content greater than 0 at% and less than or equal to 12 at% can be increased. Can be reduced.

  Next, the reason why the Co content in the Co—Cr—Pt alloy phase is greater than 0 at% and not greater than 73 at% will be described.

  As shown in Table 1 and FIG. 2, in the Co—Cr alloy, by setting the Co content ratio to 75 at% or less with respect to the total of Co and Cr, the magnetism of the Co—Cr alloy is kept at a substantially zero level. Co can be contained in the alloy. A Co-Cr-Pt alloy in which Pt is added to a Co-Cr alloy is considered to show the same tendency. Therefore, if the Co content to the total of Co, Cr, and Pt is 75 at% or less, the Co-Cr It can also be considered that Co can be contained in the alloy while the magnetism of the alloy is kept at a substantially zero level. However, as described above, since Pt has a function of increasing the magnetic moment of Co by alloying with Co in a predetermined composition range, in this embodiment, the content ratio of Co to the total of Co, Cr, and Pt is set to 73 at. % Or less. Actually, in the example described later, the first nonmagnetic phase is a 69Co-22Cr-9Pt alloy phase (the Co content is 69 at%, and is 73 at% or less), thereby providing a large leakage magnetic flux rate. Has been obtained. However, when the Co content ratio is zero, Co is not contained in the Co—Cr—Pt alloy phase, which is a nonmagnetic phase, and the content ratio of constituent elements including Co in the entire target 10 is kept constant. It does not contribute to reducing the volume fraction of the Co—Cr alloy phase (magnetic phase). Therefore, in the present embodiment, the Co content in the Co—Cr—Pt alloy phase is set to be greater than 0 at% and equal to or less than 73 at%, and the content ratio of the constituent elements including Co in the entire target 10 is kept constant. -The volume fraction of the Cr alloy phase (magnetic phase) is decreased, the magnetism of the entire target is decreased, and good magnetron sputtering can be performed.

  Next, the reason why the Co content in the Co—Pt alloy phase is greater than 0 at% and not greater than 12 at% will be described.

  Table 2 below shows the experimental results on the tensile stress of the magnetic evaluation scale measured by changing the Co content ratio in the Co-Pt alloy (the magnet becomes stronger as the value of the tensile stress increases as will be described later). FIG. 3 is a graph of the following Table 2. In the Co—Pt alloy, the graph shows the relationship between the Co content ratio and magnetism, the horizontal axis is the Co content ratio, and the vertical axis is This is the tensile stress of the magnetic evaluation scale.

  As shown in Table 2 and FIG. 3, in the Co—Pt alloy, by setting the Co content ratio to 12 at% or less with respect to the total of Co and Pt, the magnetism of the Co—Pt alloy is kept at a substantially zero level. Co can be contained in the alloy. However, when the Co content ratio is zero, the volume fraction of the Co—Cr alloy phase (magnetic phase) is decreased while the content ratio of the constituent elements including Co in the entire target 10 is kept constant, and the magnetic properties of the entire target 10 are reduced. Does not contribute to reducing Therefore, in the present embodiment, the Co content in the Co—Pt alloy phase is set to be greater than 0 at% and equal to or less than 12 at%, and the content ratio of the constituent elements including Co in the entire target 10 is kept constant. The volume fraction of the alloy phase (magnetic phase) is reduced, the magnetism of the entire target is reduced, and good magnetron sputtering can be performed.

In addition, the data of Table 1, Table 2, FIG. 2, and FIG. 3 are the data obtained by this inventor, and specifically measured as follows. In the case of the data in Table 1 and FIG. 2, Co and Cr are distributed so as to have a volume of 1 cm ³ , arc-melted, and a disk-shaped sample having a bottom area of 0.785 cm ² is produced by changing the composition ratio. did. Then, after attaching the bottom surface of the disk-shaped sample to a magnet (material ferrite) having a residual magnetic flux density of 500 gauss, the sample was pulled in a direction perpendicular to the bottom surface, and the force when it was separated from the magnet was measured. Since the tensile stress obtained by dividing this force by the base area of 0.785 cm ² has a positive correlation with the magnetism of the sample, this was used as an evaluation scale for magnetism, and the values in Table 1 and the vertical axis in FIG. In the case of the data in Table 2 and FIG. 3, data was obtained in the same manner as in the case of the data in Table 1 and FIG. 2, except that Pt and Co were distributed so as to have a volume of 1 cm ³ .

  As described above, in the target 10 according to the present embodiment, the Co—Cr—Pt alloy phase (the Co content is greater than 0 at% and less than 73 at%) and the Co—Pt alloy phase, which are nonmagnetic phases containing Co. (Co content ratio is larger than 0 at% and not more than 12 at%), the Co—Cr alloy phase, which is a magnetic phase, is maintained while keeping the content ratio of each constituent element including Co in the entire target 10 constant. The volume fraction can be reduced, and the magnetism of the entire target 10 can be reduced. Further, in the Co—Cr alloy phase that is the magnetic phase, the Co content is 85 at% or more, so that the magnetism is hardly increased compared to when the Co content is 83 at%, and the Co is the magnetic phase. The content ratio of Co in the -Cr alloy phase can be increased, and the volume fraction of the Co-Cr alloy phase that is a magnetic phase can be reduced while keeping the amount of Co in the entire target constant. Magnetism can be reduced.

  Therefore, in this embodiment, the leakage magnetic flux from the target surface is not reduced during magnetron sputtering without reducing the content of the ferromagnetic metal element contained in the target (without changing the content of each constituent element contained in the target). The amount can be increased, and magnetron sputtering can be performed satisfactorily.

3. Target Manufacturing Method The target 10 according to the present embodiment can be manufactured as follows.

(1) Preparation of magnetic mixed powder Co and Cr are weighed so as to have a predetermined composition (Co content is 85 at% or more), a molten alloy is prepared, gas atomization is performed, and a predetermined composition (Co content is included). Co-Cr alloy atomized magnetic powder having a ratio of 85 at% or more is prepared. Here, the atomized magnetic powder of Co alone may be used without containing Cr, and in this embodiment, the Co—Cr alloy atomized magnetic powder having a predetermined composition (Co content of 85 at% or more) The atomized magnetic powder is also included.

The produced Co—Cr atomized magnetic powder and oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder) are mixed and dispersed to produce a magnetic mixed powder. In oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder), fine primary particles are aggregated to form secondary particles, but the degree of mixing and dispersion is Co-Cr atomized magnetism. The process is performed until the periphery of the particles is densely covered with oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder).

FIG. 4 is a metallographic micrograph of a cross section of a sintered body obtained by pressure-sintering magnetic mixed powder (Co powder coated with oxide powder) at a temperature of 1160 ° C., a pressure of 24.5 MPa, and a time of 1 h. The whitish phase indicated by reference numeral 20 is a magnetic phase (Co phase), and the dark gray portion indicated by reference numeral 22 is an oxide phase (SiO ₂ —TiO ₂ —Cr ₂ O ₃ phase). As can be seen from FIG. 4, the periphery of the magnetic phase (Co phase) 20 is partitioned by an oxide phase (SiO ₂ —TiO ₂ —Cr ₂ O ₃ phase) 22, and Co—Cr alloy atomized magnetic powder and oxide The magnetic mixed powder prepared by mixing and dispersing powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder) is an oxide powder (SiO ₂ powder, TiO ₂ powder) around the Co—Cr alloy atomized magnetic powder. , Cr ₂ O ₃ powder).

(2) Production of first non-magnetic mixed powder Co, Cr, and Pt are weighed so as to have a predetermined composition (Co content ratio is greater than 0 at% and not greater than 73 at%), and a molten alloy is produced. Then, a Co—Cr—Pt alloy atomized nonmagnetic powder having a predetermined composition (Co content ratio is larger than 0 at% and not larger than 73 at%) is produced.

The produced Co—Cr—Pt alloy atomized nonmagnetic powder and oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder) are mixed and dispersed to produce a first nonmagnetic mixed powder. In the oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder), fine primary particles are aggregated to form secondary particles, but the degree of mixing and dispersion is Co—Cr—Pt. The process is performed until the periphery of the alloy atomized non-magnetic particles is covered with oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder).

FIG. 5 shows pressure sintering of the first non-magnetic mixed powder (Co—Cr—Pt alloy powder having a predetermined composition coated with oxide powder (Co content is greater than 0 at% and less than 73 at%)) Is a metallographic micrograph of the cross section of the sintered body obtained, wherein the whitish phase indicated by reference numeral 24 is a non-magnetic phase (69Co-22Cr-9Pt alloy phase), and the dark gray portion indicated by reference numeral 26 is an oxide phase. (SiO ₂ —TiO ₂ —Cr ₂ O ₃ phase). As can be seen from FIG. 5, the oxide phase (SiO ₂ —TiO ₂ —Cr ₂ O ₃ phase) covers the periphery of the nonmagnetic phase (69Co-22Cr-9Pt alloy phase) containing Co, and Co—Cr -Pt alloy atomized first nonmagnetic mixed powder prepared by mixing and dispersing nonmagnetic powder and oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder) is Co-Cr-Pt alloy atomized It is considered that the periphery of the nonmagnetic powder is covered with oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder).

(3) Preparation of second non-magnetic mixed powder Co and Pt are weighed so as to have a predetermined composition (Co content ratio is greater than 0 at% and not more than 12 at%), a molten alloy is prepared, and gas atomization is performed. A Co—Pt alloy atomized nonmagnetic powder having a predetermined composition (Co content ratio of greater than 0 at% and 12 at% or less) is produced.

The produced Co—Pt alloy atomized nonmagnetic powder and oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder) are mixed and dispersed to produce a second nonmagnetic mixed powder. In oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder), fine primary particles are aggregated to form secondary particles. The degree of mixing and dispersion is determined by Co-Pt alloy atomization. The process is performed until the periphery of the nonmagnetic particles is covered with oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder).

6 and 7 show pressure sintering of the second non-magnetic mixed powder (Co-Pt powder having a predetermined composition coated with oxide powder (Co content is greater than 0 at% and not more than 12 at%)). FIG. 6 is a case where the nonmagnetic phase is a 5Co-95Pt alloy phase, and FIG. 7 is a case where the nonmagnetic phase is a 10Co-90Pt alloy phase. In FIG. 6, reference numeral 28 is a nonmagnetic phase (5Co-95Pt alloy phase), and the dark gray portion indicated by reference numeral 30 is an oxide phase (SiO ₂ —TiO ₂ —Cr ₂ O ₃ phase). In FIG. 7, reference numeral 32 is a nonmagnetic phase (10Co-90Pt alloy phase), and the dark gray portion indicated by reference numeral 34 is an oxide phase (SiO ₂ —TiO ₂ —Cr ₂ O ₃ phase). 6 and 7, the non-magnetic phase is covered with an oxide phase (SiO ₂ —TiO ₂ —Cr ₂ O ₃ phase). Therefore, the second nonmagnetic mixed powder prepared by mixing and dispersing the Co—Pt alloy atomized nonmagnetic powder and the oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder) is Co— It is considered that the Pt alloy atomized nonmagnetic powder is covered with oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder).

(4) Preparation of mixed powder for pressure sintering The produced magnetic mixed powder (Co-Cr alloy powder coated with oxide powder), first non-magnetic mixed powder (Co-Cr coated with oxide powder) -Pt alloy powder) and second non-magnetic mixed powder (Co-Pt alloy powder coated with oxide powder) are mixed and dispersed until they are substantially uniform to produce a pressure-sintered mixed powder. When preparing this mixed powder for pressure sintering, an oxide powder is added to the magnetic mixed powder, the first nonmagnetic mixed powder, and the second nonmagnetic mixed powder, if necessary, and mixed and dispersed. Also good. In addition, the mixing and dispersion in this step is stopped to such an extent that each particle diameter does not become small. When mixing and dispersing are performed as each particle size becomes smaller, the oxide powder layer covering the atomized metal powder is destroyed, and three types of atomized metal powders (Co-Cr alloy powder, Co-Cr-Pt alloy powder, Co -Pt alloy powders) come into contact with each other and metal atoms diffuse due to mixing and dispersion, and the composition of each atomized metal powder may deviate from a predetermined composition.

(5) Molding The produced mixed powder for pressure sintering is shaped by pressure sintering, for example, by a vacuum hot press method to produce a target.

(6) Features of Manufacturing Method A feature of the manufacturing method according to the present embodiment is that each metal powder (Co—Cr alloy powder, Co—Cr—Pt alloy powder, Co—Pt alloy powder) is converted into an oxide powder (SiO _2). Powder, TiO ₂ powder, Cr ₂ O ₃ powder) and mixed powder in which metal particles are covered with oxide powder (mixing at the first stage), and then mixed and dispersed with each other. Thus, a mixed powder for pressure sintering is obtained (mixing at the second stage), and the mixed powder for pressure sintering is produced through two stages of mixing.

In the first stage mixing, each metal particle (Co—Cr alloy particle, Co—Cr—Pt alloy particle, Co—Pt alloy particle) is surrounded by oxide powder (SiO ₂ powder, TiO ₂ powder, Cr _2). In contrast to mixing (the particle size of the oxide powder is reduced by this mixing) until it is densely covered with (O ₃ powder), in the second stage of mixing, mixing and dispersion are performed for each particle size. Is stopped to the extent that does not become small.

In the first stage of mixing, each metal particle (Co-Cr alloy particle, Co-Cr-Pt alloy particle, Co-Pt alloy particle) is surrounded by oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder) ), Until the oxide powder is sufficiently finely coated, the metal particles are densely coated, and the metal particles are effectively prevented from coming into contact with each other. Can do.

  On the other hand, the mixing in the second stage stops mixing and dispersion to such an extent that each particle size does not become small. Therefore, the oxide powder layer covering the atomized metal powder is not destroyed, and three types of atomized metal powders (Co -Cr alloy powder, Co-Cr-Pt alloy powder, Co-Pt alloy powder) are suppressed from contacting each other, and the composition of each atomized metal powder deviates from a predetermined composition due to diffusion of metal atoms during mixing and dispersion. Is suppressed.

  In addition, since the surface of each atomized metal powder is covered with oxide powder, diffusion of metal atoms between atomized metal powders hardly occurs even when vacuum hot pressing is performed, and each metal during pressure sintering It can also be prevented that the content ratio of the constituent elements in the phases (Co—Cr alloy phase, Co—Cr—Pt alloy phase, Co—Pt alloy phase) fluctuates. As a result, in the target obtained, it is possible to prevent the phase designed to become a nonmagnetic phase from becoming magnetized, and the volume fraction of the nonmagnetic phase in the entire target is increased as designed. The amount of leakage magnetic flux from the target surface can be reliably increased during magnetron sputtering.

Example 1
The composition of the whole target produced as Example 1 was 91 (73Co-11Cr-16Pt) -4SiO ₂ -2TiO ₂ -3Cr ₂ O ₃ , and was produced and evaluated as follows. In addition, the content ratio of Co to the metal (Co, Cr, Pt) of the entire target is 73 at%, the content ratio of Cr is 11 at%, and the content ratio of Pt is 16 at%.

  Co simple substance was heated to 1700 ° C. to make a molten metal of Co simple substance, and gas atomization was performed to produce Co powder (magnetic metal powder).

  Further, each metal was weighed so that the alloy composition would be Co: 69 at%, Cr: 22 at%, Pt: 9 at%, heated to 1700 ° C. to obtain a 69Co-22Cr-9Pt alloy melt, and gas atomization was performed to obtain 69Co— 22Cr-9Pt alloy powder (first nonmagnetic metal powder) was produced.

  Further, each metal is weighed so that the alloy composition becomes Co: 5 at% and Pt: 95 at%, heated to 2000 ° C. to form a 5Co-95Pt alloy melt, gas atomized, and 5Co-95Pt alloy powder (second Nonmagnetic metal powder) was prepared.

  The prepared three types of atomized metal powders (Co powder, 69Co-22Cr-9Pt alloy powder, 5Co-95Pt alloy powder) are each classified by a 150-mesh sieve, and three types of atomized metal powders having a particle size of φ106 μm or less ( Co powder, 69Co-22Cr-9Pt alloy powder, 5Co-95Pt alloy powder).

After the classification, 1470.00 g of Co powder was mixed with 65.80 g of SiO ₂ powder, 43.81 g of TiO ₂ powder, and 124.95 g of Cr ₂ O ₃ powder, and mixed and dispersed to obtain a magnetic mixed powder (coated with oxide powder). Co powder) was obtained. The SiO ₂ powder, TiO ₂ powder, and Cr ₂ O ₃ powder used had aggregated primary particles with a center diameter of 0.6 μm to form secondary particles with a particle diameter of about 100 μm. Mixing and dispersing with a ball mill until the periphery is densely covered with oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder), magnetic mixed powder (Co powder coated with oxide powder) )

Further, 43.60 g of SiO ₂ powder, 28.98 g of TiO ₂ powder, and 82.76 g of Cr ₂ O ₃ powder were added to 1150.00 g of the 69Co-22Cr-9Pt alloy powder after classification, and mixed and dispersed. A nonmagnetic mixed powder (69Co-22Cr-9Pt alloy powder coated with oxide powder) was obtained. In the used SiO ₂ powder, TiO ₂ powder, and Cr ₂ O ₃ powder, primary particles with a center diameter of 0.6 μm aggregated to form secondary particles with a particle diameter of about φ100 μm, but 69Co-22Cr -9Pt alloy particles were mixed and dispersed with a ball mill until the surroundings were densely covered with oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder), and the first non-magnetic mixed powder ( 69Co-22Cr-9Pt alloy powder coated with oxide powder).

Further, 208.22 g of SiO ₂ powder, 13.83 g of TiO ₂ powder, and 39.32 g of Cr ₂ O ₃ powder were added to 1480.00 g of the 5Co-95Pt alloy powder after classification, and mixed and dispersed. A magnetic mixed powder (5Co-95Pt alloy powder coated with oxide powder) was obtained. In the SiO ₂ powder, TiO ₂ powder, and Cr ₂ O ₃ powder used, primary particles with a center diameter of 0.6 μm aggregated to form secondary particles with a particle diameter of about φ100 μm, but 5Co-95Pt The alloy particles are mixed and dispersed by a ball mill until the surroundings of the alloy particles are densely covered with oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder), and the second non-magnetic mixed powder (oxide) 5Co-95Pt alloy powder coated with powder).

  Next, 805.67 g of magnetic mixed powder (Co powder coated with oxide powder), 1229.89 g of first nonmagnetic mixed powder (69Co-22Cr-9Pt alloy powder coated with oxide powder), second 744.44 g of the nonmagnetic mixed powder (5Co-95Pt alloy powder coated with oxide powder) was mixed and dispersed to obtain a mixed powder for pressure sintering. Specifically, within a range where the particle size of each powder (magnetic mixed powder, first nonmagnetic mixed powder, second nonmagnetic mixed powder) does not become small, mixing and dispersing are performed so that each powder is dispersed almost uniformly. To obtain a mixed powder for pressure sintering.

30 g of the prepared mixed powder for pressure sintering was hot pressed under the conditions of sintering temperature: 1100 ° C., pressure: 31 MPa, time: 60 min, atmosphere: 5 × 10 ⁻² Pa or less, and a test piece (φ30 mm) was obtained. Produced. The thickness of the obtained test piece was about 4.5 mm. It was 9.041 (g / cm < ³ >) when the density of the produced test piece was measured. Since the theoretical density was 9.24 (g / cm ³ ), the relative density was 97.85%.

  8 and 9 are metallographic micrographs of the cross section in the thickness direction of the obtained test piece, FIG. 8 is a low-magnification photograph, and FIG. 9 is a high-magnification photograph. 10 and 11 are SEM photographs of the cross section in the thickness direction of the obtained test piece, FIG. 10 is a photograph with a low magnification, and FIG. 11 is a photograph with a high magnification.

As a result of elemental analysis by EPMA, in the SEM photograph of FIG. 11, the relatively large gray portion of the phase is the Co phase, the whitish portion is the 5Co-95Pt alloy phase, and the Co phase and 5Co-95Pt The middle gray portion of the alloy phase is the 69Co-22Cr-9Pt alloy phase, and the gray portion separating the metal phases is the oxide phase (SiO ₂ —TiO ₂ —Cr _2). an O ₃ phase), it was found that the metal phase to each other are partitioned by the oxide phase _{(SiO 2 -TiO 2 -Cr 2 O} 3 phase).

Next, hot pressing is performed using the prepared powder mixture for pressure sintering under conditions of sintering temperature: 1070 ° C., pressure: 31 MPa, time: 60 min, atmosphere: 5 × 10 ⁻² Pa or less, φ152. Two targets of 4 mm × 7.0 mm thickness were produced. It was 9.009 and 9.009 (g / cm < ³ >) when the density of the produced two targets was measured. Since the theoretical density was 9.24 (g / cm ³ ), the relative densities were 97.50% and 97.50%.

  About the produced two targets, based on ASTM F2086-01, evaluation about the leakage magnetic flux was performed. A horseshoe magnet (material: alnico) was used as a magnet for generating magnetic flux. The magnet was attached to a leakage magnetic flux measuring device, and a Gauss meter was connected to the Hall probe. The hall probe was arranged so as to be located right above the center between the magnetic poles of the horseshoe magnet.

  First, without placing a target on the table of the measuring apparatus, the magnetic flux density in the horizontal direction on the surface of the table was measured, and the Source Field defined by ASTM was measured to be 900 (G) and 900 (G).

  Next, the tip of the Hall probe is raised to the position at the time of measuring the leakage magnetic flux of the target (the thickness of the target + the height of 2 mm from the table surface), and is placed on the table surface without placing the target on the table surface. The leakage magnetic flux density in the direction was measured, and the Reference field defined by ASTM was measured to be 563 (G) and 572 (G).

  Next, the target was placed on the table surface so that the distance between the center of the target surface and a point immediately below the hole probe on the target surface was 43.7 mm. Then, the target is rotated 5 times counterclockwise without moving the center position, and then the target is rotated 0 degrees, 30 degrees, 60 degrees, 90 degrees, 120 degrees without moving the center position. Then, the leakage magnetic flux density in the direction horizontal to the table surface was measured. The five magnetic flux density values obtained were divided by the value of the reference field and multiplied by 100 to obtain the leakage magnetic flux rate (%). The average of five points of leakage magnetic flux rate (%) was taken, and the average value was taken as the average leakage magnetic flux rate (%) of the target. As shown in Tables 3 and 4 below, the average leakage magnetic flux rate of the two produced targets is 51.0% and 50.7%, and the average of the two average leakage magnetic flux rates is 50.9%. there were.

(Example 2)
The composition of the entire target produced as Example 2 is 91 (73Co-11Cr-16Pt) -4SiO ₂ -2TiO ₂ -3Cr ₂ O _3, which is the same as that of Example 1, but is the second produced by atomization. The difference is that the nonmagnetic metal powder is a 10Co-90Pt alloy powder.

  The target of Example 2 was produced and evaluated as follows.

  Atomization and classification were performed in the same manner as in Example 1 except that only the alloy composition was changed to obtain 10Co-90Pt alloy powder. In addition, the heating temperature and the injection temperature during atomization to obtain 10Co-90Pt alloy powder were 2000 ° C.

Mixing and dispersing were carried out in the same manner as in Example 1 except that 21.77 g of SiO ₂ powder, 14.52 g of TiO ₂ powder, and 41.50 g of Cr ₂ O ₃ powder were added to 1500.00 g of the obtained 10Co-90Pt alloy powder. A second nonmagnetic mixed powder (10Co-90Pt alloy powder coated with oxide powder) was obtained.

Further, the same procedure as in Example 1 was performed except that 64.91 g of SiO ₂ powder, 43.22 g of TiO ₂ powder, and 123.26 g of Cr ₂ O ₃ powder were added to 1450.00 g of Co powder obtained by atomization in Example 1. Thus, magnetic dispersion powder (Co powder coated with oxide powder) was obtained.

Also, except for adding SiO ₂ powder 43.60g, TiO ₂ powder 28.98G, the Cr ₂ O ₃ powder 82.76g a 69Co-22Cr-9Pt alloy powder 1150.00g obtained by atomization in Example 1 carried out Mixing and dispersing were carried out in the same manner as in Example 1 to obtain a first nonmagnetic mixed powder (69Co-22Cr-9Pt alloy powder coated with oxide powder).

  Next, 791.37 g of magnetic mixed powder (Co powder coated with oxide powder), 1229.89 g of first nonmagnetic mixed powder (69Co-22Cr-9Pt alloy powder coated with oxide powder), second 758.74 g of a nonmagnetic mixed powder (10Co-90Pt alloy powder coated with oxide powder) was mixed and dispersed in the same manner as in Example 1 to obtain a mixed powder for pressure sintering.

30 g of the prepared mixed powder for pressure sintering was hot pressed under the conditions of sintering temperature: 1100 ° C., pressure: 31 MPa, time: 60 min, atmosphere: 5 × 10 ⁻² Pa or less, and a test piece (φ30 mm) was obtained. Produced. The thickness of the obtained test piece was about 4.5 mm. It was 9.052 (g / cm < ³ >) when the density of the produced test piece was measured. Since the theoretical density was 9.24 (g / cm ³ ), the relative density was 97.96%.

  12 and 13 are metallographic micrographs of the cross section in the thickness direction of the obtained test piece, FIG. 12 is a low-magnification photograph, and FIG. 13 is a high-magnification photograph. 14 and 15 are SEM photographs of the cross section in the thickness direction of the obtained test piece, FIG. 14 is a low-magnification photograph, and FIG. 15 is a high-magnification photograph.

As a result of elemental analysis by EPMA, in the SEM photograph of FIG. 15, the relatively large gray portion is the Co phase, the whitest portion is the 10Co-90Pt phase, the Co phase and the 10Co-90Pt phase. The middle gray portion of the layer is the 69Co-22Cr-9Pt phase, and the gray portion separating the metal phases is the oxide phase (SiO ₂ —TiO ₂ —Cr ₂ O ₃ phase). It was found that the metal phases were partitioned by an oxide phase (SiO ₂ —TiO ₂ —Cr ₂ O ₃ phase).

Next, hot pressing is performed using the prepared powder mixture for pressure sintering under conditions of sintering temperature: 1080 ° C., pressure: 31 MPa, time: 60 min, atmosphere: 5 × 10 ⁻² Pa or less, φ152. Two targets of 4 mm × 7.0 mm thickness were produced. The density of the two produced targets was measured and found to be 9.023 and 9.014 (g / cm ³ ). Since the theoretical density was 9.24 (g / cm ³ ), the relative densities were 97.65% and 97.55%.

  About the produced two targets, it carried out similarly to Example 1, and evaluated about the leakage magnetic flux. As shown in Tables 5 and 6 below, the average leakage magnetic flux rates were 50.6% and 50.7%, and the average of the two average leakage magnetic flux rates was 50.7%.

(Comparative Example 1)
The composition of the entire target produced as Comparative Example 1 is 91 (73Co-11Cr-16Pt) -4SiO ₂ -2TiO ₂ -3Cr ₂ O _3, which is the same as Examples 1 and 2, but Examples 1 and 2 Instead of the second non-magnetic metal powder (5Co-95Pt alloy powder, 10Co-90Pt alloy powder), a target is prepared using 50Co-50Pt alloy powder, which is magnetic metal powder, and the nonmagnetic phase is 1 (The two magnetic phases are the Co phase and the 50Co-50Pt alloy phase).

  The target of Comparative Example 1 was prepared and evaluated as follows.

  Atomization and classification were performed in the same manner as in Example 1 except that only the alloy composition was changed to obtain 50Co-50Pt alloy powder. In addition, the heating temperature and the injection temperature at the time of atomization which obtains 50Co-50Pt alloy powder were 1800 degreeC.

Mixing and dispersing were carried out in the same manner as in Example 1 except that 38.55 g of SiO ₂ powder, 25.63 g of TiO ₂ powder and 72.93 g of Cr ₂ O ₃ powder were added to 1850.00 g of the obtained 50Co-50Pt alloy powder. A second magnetic mixed powder (50Co-50Pt alloy powder coated with oxide powder) was obtained.

Further, the same procedure as in Example 1 was performed except that 48.34 g of SiO ₂ powder, 32.19 g of TiO ₂ powder, and 91.81 g of Cr ₂ O ₃ powder were added to 1080.00 g of Co powder obtained by atomization in Example 1. The first magnetic mixed powder (Co powder coated with oxide powder) was obtained by mixing and dispersing.

Further, Example 1 except that 430.000 g of SiO ₂ powder, 28.98 g of TiO ₂ powder, and 82.76 g of Cr ₂ O ₃ powder were added to 1150.00 g of 69Co-22Cr-9Pt alloy powder obtained in Example 1. The mixture was dispersed in the same manner as above to obtain a first nonmagnetic mixed powder (69Co-22Cr-9Pt powder coated with oxide powder).

  Next, 574.04 g of magnetic mixed powder (Co powder coated with oxide powder), 1229.89 g of the first nonmagnetic mixed powder (69Co-22Cr-9Pt alloy powder coated with oxide powder), second 976.07 g of the above magnetic mixed powder (50Co-50Pt alloy powder coated with oxide powder) was mixed and dispersed in the same manner as in Example 1 to obtain a mixed powder for pressure sintering.

30 g of the prepared mixed powder for pressure sintering was hot pressed under the conditions of sintering temperature: 1100 ° C., pressure: 31 MPa, time: 60 min, atmosphere: 5 × 10 ⁻² Pa or less, and a test piece (φ30 mm) was obtained. Produced. The thickness of the obtained test piece was about 4.5 mm. It was 9.023 (g / cm < ³ >) when the density of the produced test piece was measured. Since the theoretical density was 9.24 (g / cm ³ ), the relative density was 97.65%.

  16 and 17 are metallographic micrographs of the cross section in the thickness direction of the obtained test piece, FIG. 16 is a low-magnification photograph, and FIG. 17 is a high-magnification photograph. 18 and 19 are SEM photographs of the cross section in the thickness direction of the obtained test piece, FIG. 18 is a photograph with a low magnification, and FIG. 19 is a photograph with a high magnification.

As a result of elemental analysis by EPMA, in the SEM photograph of FIG. 19, the relatively large gray portion of the phase is the Co phase, the whitest portion is the 50Co-50Pt phase, the Co phase and the 50Co-50Pt phase. The middle gray portion of the layer is the 69Co-22Cr-9Pt phase, and the gray portion separating the metal phases is the oxide phase (SiO ₂ —TiO ₂ —Cr ₂ O ₃ phase). It was found that the metal phases were partitioned by an oxide phase (SiO ₂ —TiO ₂ —Cr ₂ O ₃ phase).

Next, hot pressing is performed using the prepared powder mixture for pressure sintering under conditions of sintering temperature: 1090 ° C., pressure: 31 MPa, time: 60 min, atmosphere: 5 × 10 ⁻² Pa or less, φ152. Two targets of 4 mm × 7.0 mm thickness were produced. It was 9.071 and 9.065 (g / cm < ³ >) when the density of the produced two targets was measured. Since the theoretical density was 9.24 (g / cm ³ ), the relative densities were 98.17% and 98.11%.

  About the produced two targets, it carried out similarly to Example 1, and evaluated about the leakage magnetic flux. As shown in Tables 7 and 8 below, the average leakage magnetic flux rates were 44.8% and 44.9%, and the average of the two average leakage magnetic flux rates was 44.9%.

(Comparative Example 2)
The composition of the entire target produced as Comparative Example 2 is 91 (73Co-11Cr-16Pt) -4SiO ₂ -2TiO ₂ -3Cr ₂ O _3, which is the same as in Examples 1 and 2 and Comparative Example 1. The magnetic metal powder used for the production of the target is Co powder, the first nonmagnetic metal powder is 69Co-22Cr-9Pt alloy powder, the second magnetic metal powder is 50Co-50Pt alloy powder, and the target The composition of the three types of metal powder used in the production of is the same as in Comparative Example 1.

However, in this comparative example 2, the above-mentioned three kinds of metal powder and oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder) are mixed and dispersed simultaneously (in one step) and then pressure sintered. 3 types of metal powders were mixed and dispersed with oxide powders (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder), respectively. This is different from Examples 1 and 2 and Comparative Example 1 in which the mixed powder is further mixed (after mixing in two stages) to obtain a mixed powder for pressure sintering.

  The target of Comparative Example 2 was prepared and evaluated as follows.

254.74 g of Co powder obtained by atomization in Example 1, 557.61 g of 69Co-22Cr-9Pt alloy powder obtained by atomization in Example 1, and 50Co-50Pt alloy powder 467 obtained by atomization in Comparative Example 1 .65 g, SiO ₂ powder 42.35 g, TiO ₂ powder 28.18 g, Cr ₂ O ₃ powder 80.26 g were mixed and dispersed at the same time to obtain a mixed powder for pressure sintering by one-stage mixing. . Specifically, mixing and dispersion were performed with a ball mill at the same time and strength as in Example 1, and a mixed powder for pressure sintering was produced by one-stage mixing.

30 g of the produced powder mixture for pressure sintering was hot pressed under the conditions of sintering temperature: 1100 ° C., pressure: 24.5 MPa, time: 60 min, atmosphere: 5 × 10 ⁻² Pa or less, and a test piece (φ30 mm ) Was produced. The thickness of the obtained test piece was about 4.5 mm. It was 9.027 (g / cm < ³ >) when the density of the produced test piece was measured. Since the theoretical density was 9.24 (g / cm ³ ), the relative density was 97.69%.

  20 and 21 are metallographic micrographs of the cross section in the thickness direction of the obtained test piece, FIG. 20 is a low-magnification photograph, and FIG. 21 is a high-magnification photograph. 22 and 23 are SEM photographs of the cross section in the thickness direction of the obtained test piece, FIG. 22 is a photograph with a low magnification, and FIG. 23 is a photograph with a high magnification.

  As a result of elemental analysis by EPMA, in the SEM photograph of FIG. 23, most of the portion that can be observed as the metal phase is the Co phase, and the relatively large portion that can be observed as the 50Co-50Pt alloy phase is the portion shown in FIG. The other part is a phase in which a metal and an oxide are mixed, and it is considered that the metal phases are not partitioned by the oxide phase.

Next, using the prepared mixed powder for pressure sintering, hot pressing is performed under the conditions of sintering temperature: 1100 ° C., pressure: 24.5 MPa, time: 60 min, atmosphere: 5 × 10 ⁻² Pa or less, One target of φ152.4 mm × 7.0 mm thickness was produced.

  Further, another target having a diameter of 152.4 mm and a thickness of 7.0 mm was manufactured by the same process as the manufacturing process described above.

It was 9.07 and 9.06 (g / cm < ³ >) when the density of the produced two targets was measured. Since the theoretical density was 9.24 (g / cm ³ ), the relative density was 98.2% and 98.1%.

  About the produced two targets, it carried out similarly to Example 1, and evaluated about the leakage magnetic flux. As shown in Tables 9 and 10 below, the average leakage magnetic flux rates were 31.9% and 31.5%, and the average of the two average leakage magnetic flux rates was 31.7%.

(Comparative Example 3)
The composition of the entire target produced as Comparative Example 3 is 91 (71Co-11Cr-18Pt) -3SiO ₂ -2TiO ₂ -4Cr ₂ O ₃ . In addition, the content ratio of Co to the metal (Co, Cr, Pt) of the entire target is 71 at%, the content ratio of Cr is 11 at%, and the content ratio of Pt is 18 at%.

  The magnetic metal powder used for the preparation of the target in Comparative Example 3 is Co powder, the first nonmagnetic metal powder is 69Co-22Cr-9Pt alloy powder, and the second nonmagnetic metal powder is Pt powder. In the present comparative example 3, of the two nonmagnetic metal powders, the first nonmagnetic metal powder (69Co-22Cr-9Pt alloy powder) contains Co, which is a ferromagnetic metal element. The nonmagnetic metal powder (Pt powder) does not contain a ferromagnetic metal element.

  The target of Comparative Example 3 was prepared and evaluated as follows.

  Co simple substance was heated to 1700 ° C. to make a molten metal of Co simple substance, and gas atomization was performed to produce Co powder (magnetic metal powder).

  Further, each metal was weighed so that the alloy composition would be Co: 69 at%, Cr: 22 at%, Pt: 9 at%, heated to 1700 ° C. to obtain a 69Co-22Cr-9Pt alloy melt, and gas atomization was performed to obtain 69Co— 22Cr-9Pt alloy powder (first nonmagnetic metal powder) was produced.

  Moreover, Pt simple substance was heated to 2000 degreeC, it was set as the molten metal of Pt simple substance, and gas atomization was performed, and Pt powder (nonmagnetic metal powder) was produced.

  Then, the obtained metal powder was classified in the same manner as in Example 1 to obtain Co powder, 69Co-22Cr-9Pt alloy powder, and Pt powder.

Mixing and dispersing in the same manner as in Example 1 except that 23.56 g of SiO ₂ powder, 20.84 g of TiO ₂ powder and 79.32 g of Cr ₂ O ₃ powder were added to 700.00 g of the classified Co powder, and magnetic mixing was performed. A powder (Co powder coated with oxide powder) was obtained.

Further, the same procedure as in Example 1 was performed except that 29.81 g of SiO ₂ powder, 26.43 g of TiO ₂ powder, and 100.67 g of Cr ₂ O ₃ powder were added to 1050.00 g of the 69Co-22Cr-9Pt alloy powder after classification. Mixing and dispersing were performed to obtain a first nonmagnetic mixed powder (69Co-22Cr-9Pt alloy powder coated with oxide powder).

Further, mixing and dispersion were carried out in the same manner as in Example 1 except that 8.49 g of SiO ₂ powder, 7.52 g of TiO ₂ powder, and 28.76 g of Cr ₂ O ₃ powder were added to 840.00 g of classified Pt powder, A second nonmagnetic mixed powder (Pt powder coated with oxide powder) was obtained.

  Next, 738.62 g of magnetic mixed powder (Co powder coated with oxide powder), 1107.63 g of first non-magnetic mixed powder (69Co-22Cr-9Pt alloy powder coated with oxide powder), second A non-magnetic mixed powder (Pt powder coated with an oxide powder) of 653.75 g was mixed and dispersed in the same manner as in Example 1 to prepare a mixed powder for pressure sintering.

30 g of the prepared mixed powder for pressure sintering was hot pressed under the conditions of sintering temperature: 1070 ° C., pressure: 31 MPa, time: 60 min, atmosphere: 5 × 10 ⁻² Pa or less, and a test piece (φ30 mm) was obtained. Produced. The thickness of the obtained test piece was about 4.5 mm. It was 9.375 (g / cm < ³ >) when the density of the produced test piece was measured. Since the theoretical density was 9.56 (g / cm ³ ), the relative density was 98.06%.

  24 and 25 are metallographic micrographs of the cross section in the thickness direction of the obtained test piece, FIG. 24 is a low-magnification photograph, and FIG. 25 is a high-magnification photograph.

In FIGS. 24 and 25, the whitish portion is a metal phase (Co phase, 69Co-22Cr-9Pt alloy phase, Pt phase), and the dark gray portion partitioning between these metal phases is an oxide phase (SiO 2). _2— TiO ₂ —Cr ₂ O ₃ phase), and the metal phases are partitioned by an oxide phase (SiO ₂ —TiO ₂ —Cr ₂ O ₃ phase).

Next, hot pressing is performed using the prepared powder mixture for pressure sintering under conditions of sintering temperature: 1030 ° C., pressure: 31 MPa, time: 60 min, atmosphere: 5 × 10 ⁻² Pa or less, φ152. A target of 4 mm × thickness 6.0 mm was produced. It was 9.388 (g / cm < ³ >) when the density of the produced target was measured. Since the theoretical density was 9.56 (g / cm ³ ), the relative density was 98.20%.

  About the produced target, it carried out similarly to Example 1, and evaluated about the leakage magnetic flux. As shown in Table 11 below, the average leakage magnetic flux rate was 50.3%.

(Comparative Example 4)
In the same manner as in Comparative Example 3, except that the sintering temperature at the time of producing a target of φ152.4 mm × thickness 6.0 mm was 1000 ° C. and the sintering temperature of Comparative Example 3 was lower than 1030 ° C., φ152. A target of 4 mm × thickness 6.0 mm was produced.

  About the produced target, it carried out similarly to Example 1, and evaluated about the leakage magnetic flux. As shown in Table 12 below, the average leakage magnetic flux rate was 51.0%.

(Comparative Example 5)
In Examples 1 and 2 and Comparative Examples 1 to 4, there were three types of atomized metal powders used for target preparation, but the atomized metal powder used for target preparation in Comparative Example 5 was 71Co-11Cr-. One type of 18Pt alloy powder.

The composition of the whole produced target is 91 (71Co-11Cr-18Pt) -3SiO ₂ -2TiO ₂ -4Cr ₂ O _3, which is the same as Comparative Examples 3 and 4.

  The target of Comparative Example 5 was prepared and evaluated as follows.

  Each metal was weighed so that the alloy composition would be Co: 71 at%, Cr: 11 at%, Pt: 18 at%, heated to 1700 ° C. to make a 71Co-11Cr-18Pt alloy melt, and gas atomized to 71Co-11Cr— 18Pt alloy powder was produced. And it classified like Example 1, and obtained 71Co-11Cr-18Pt alloy powder.

270.004g of SiO ₂ powder, 24.26g of TiO ₂ powder, 92.17g of Cr ₂ O ₃ powder were added to 1140.00g of 71Co-11Cr-18Pt alloy powder after classification and mixed and dispersed for pressure sintering A mixed powder (71Co-11Cr-18Pt alloy powder coated with oxide powder) was obtained. In the used SiO ₂ powder, TiO ₂ powder, and Cr ₂ O ₃ powder, primary particles having a central diameter of 0.6 μm aggregated to form secondary particles having a particle diameter of about φ100 μm, but 71Co-11Cr -18Pt alloy particles were mixed and dispersed with a ball mill until the periphery of the particles was densely covered with oxide powder (SiO ₂ powder, TiO ₂ powder, Cr ₂ O ₃ powder). 71Co-11Cr-18Pt alloy powder coated with oxide powder).

30 g of the prepared mixed powder for pressure sintering was hot pressed under the conditions of sintering temperature: 1160 ° C., pressure: 24.5 MPa, time: 60 min, atmosphere: 5 × 10 ⁻² Pa or less, and a test piece (φ30 mm ) Was produced. The thickness of the obtained test piece was about 4.5 mm. It was 9.402 (g / cm < ³ >) when the density of the produced test piece was measured. Since the theoretical density was 9.56 (g / cm ³ ), the relative density was 98.35%.

  26 and 27 are metallographic micrographs of the cross section in the thickness direction of the obtained test piece, FIG. 26 is a low-magnification photograph, and FIG. 27 is a high-magnification photograph.

  In FIGS. 26 and 27, the whitish portion is the metal phase (71Co-11Cr-18Pt phase). Compared with FIGS. 24 and 25 of Comparative Example 3, the size of the metal phase (whiter portion) is smaller and the area of the dark gray portion is wider. Therefore, in this comparative example 5, it is considered that the metal phase itself is made finer than the comparative examples 3 and 4, and the region where the metal phase and the oxide phase are finely dispersed is increased. .

Next, using the prepared powder for pressure sintering, hot pressing is performed under conditions of sintering temperature: 1160 ° C., pressure: 24.5 MPa, time: 60 min, atmosphere: 5 × 10 ⁻² Pa or less, A target of φ152.4 mm × thickness 6.0 mm was produced. It was 9.397 (g / cm < ³ >) when the density of the produced target was measured. Since the theoretical density was 9.56 (g / cm ³ ), the relative density was 98.30%.

  About the produced target, it carried out similarly to Example 1, and evaluated about the leakage magnetic flux. As shown in Table 13 below, the average leakage magnetic flux rate was 40.0%.

(Discussion)
The measurement results for Examples 1 and 2 and Comparative Examples 1 to 5 in which the average leakage magnetic flux rate was measured are summarized in Table 14 below. However, the thickness of the target whose average leakage magnetic flux rate was measured in Examples 1 and 2 and Comparative Examples 1 and 2 was 7 mm, whereas the thickness of the target whose average leakage magnetic flux rate was measured in Comparative Examples 3 to 5 Is 6 mm, and due to the difference in thickness, it is necessary to note that the average leakage magnetic flux ratio of Comparative Examples 3 to 5 is larger than those of Examples 1 and 2 and Comparative Examples 1 and 2 and can be easily measured. . Further, the composition of the entire targets of Examples 1 and 2 and Comparative Examples 1 and 2 was 91 (73Co-11Cr-16Pt) -4SiO ₂ -2TiO ₂ -3Cr ₂ O ₃ , whereas those of Comparative Examples 3 to 5 The composition of the entire target is 91 (71Co-11Cr-18Pt) -3SiO ₂ -2TiO ₂ -4Cr ₂ O ₃ , and the Co content in the targets of Examples 1 and 2 and Comparative Examples 1 and 2 is 66.43 mol%. In contrast, the Co content in the targets of Comparative Examples 3 to 5 is 64.61 mol%, and the target of Comparative Examples 3 to 5 has a smaller content of Co, which is a ferromagnetic metal element. In terms of the content ratio of Co, which is a ferromagnetic metal element, Comparative Examples 3 to 5 have a larger average leakage magnetic flux rate than Examples 1 and 2 and Comparative Examples 1 and 2 and are easily measured. It is necessary to keep in mind There is a point.

  In Examples 1 and 2, a magnetic layer containing Co (ferromagnetic metal element) and a plurality of nonmagnetic phases (first non-magnetic phase) containing Co (ferromagnetic metal element) and having different constituent elements or their content ratios. A magnetic phase and a second non-magnetic phase) and are within the scope of the present invention. In Examples 1 and 2, both the first nonmagnetic phase and the second nonmagnetic phase contain Co, and the volume fraction of the magnetic phase (Co phase) is maintained while keeping the amount of Co in the entire target constant. Can be reduced, and the average leakage magnetic flux rate of the target can be increased.

  In Comparative Example 1, the Co content in the Co—Pt alloy phase is as large as 50 at%, the Co—Pt alloy phase is a magnetic phase, and the nonmagnetic phase is only the 69Co-22Cr-9Pt alloy phase. For this reason, the volume fraction of the magnetic phase with respect to the whole target is larger than that of Examples 1 and 2, and the average leakage magnetic flux rate is about 12% smaller than that of Examples 1 and 2. Therefore, providing a plurality of nonmagnetic phases containing a ferromagnetic metal element is considered important for improving the average leakage magnetic flux rate of the target.

  In Comparative Example 2, the Co content of the Co—Pt alloy phase is as large as 50 at%, the Co—Pt alloy phase is a magnetic phase, and the nonmagnetic phase is only the 69Co-22Cr-9Pt alloy phase. Moreover, the mixed powder for pressure sintering is produced by one-step mixing, and metal powders with different compositions are connected during mixing, and metal atoms move (diffusion) during mixing and pressure sintering. It seems to have been. For this reason, even in the phase formed from the 69Co-22Cr-9Pt alloy powder, a part of the phase may be a magnetic phase. Actually, the average leakage magnetic flux rate of the target of Comparative Example 2 is 31.7%, which is about 38% smaller than Examples 1 and 2, and about 29% smaller than that of Comparative Example 1. Part of the phase formed from the 69Co-22Cr-9Pt alloy powder is considered to be a magnetic phase. Therefore, producing the mixed powder for pressure sintering by mixing in two stages as in Examples 1 and 2 is considered important for improving the average leakage magnetic flux rate of the target.

  Comparative Examples 3 and 4 have two nonmagnetic phases as in Examples 1 and 2, but the second nonmagnetic phase is a single Pt phase and does not contain Co, which is a ferromagnetic metal element. For this reason, it is considered that the volume fraction of the magnetic phase in the entire target is not sufficiently small, and the average leakage magnetic flux rate is not sufficiently improved. Although the average leakage magnetic flux rate of Comparative Examples 3 and 4 is approximately the same as the average leakage magnetic flux rate of Examples 1 and 2, as described above, the target thickness of Comparative Examples 3 and 4 is the same as that of Examples 1 and 2. Since the content ratio of Co contained in the targets of Comparative Examples 3 and 4 is smaller than that of Examples 1 and 2, which is smaller than the thickness of the target, when these are aligned with Examples 1 and 2, Comparative Example The average leakage magnetic flux rates of 3 and 4 are considered to be considerably smaller than the average leakage magnetic flux rates of Examples 1 and 2.

  When the average leakage magnetic flux rates of Comparative Examples 3 and 4 are compared, Comparative Example 4 with a sintering temperature of 1000 ° C. has a smaller average leakage magnetic flux rate than Comparative Example 3 with a sintering temperature of 1030 ° C. Is getting bigger. This is probably because the lower the sintering temperature, the more difficult the atom diffusion occurs. Therefore, in order to produce a target with an improved amount of magnetic flux leakage during magnetron sputtering, a lower sintering temperature is preferable.

  In Comparative Example 5, the metal phase is only the 71Co-11Cr-18Pt alloy phase. This metal phase is a magnetic phase, and it is considered that the nonmagnetic metal phase does not exist in the target of Comparative Example 5, and the volume fraction of the magnetic phase is considered to be high. For this reason, it is considered that the average leakage magnetic flux rate of the target of Comparative Example 5 was smaller than the average leakage magnetic flux rate of the targets of Comparative Examples 3 and 4. In addition, although the average leakage magnetic flux rate of the target of Comparative Example 5 is 40.0%, when the thickness of the target and the content ratio of Co are matched with Examples 1 and 2 and Comparative Examples 1 and 2, the average leakage magnetic flux The rate value appears to be significantly less than 40.0%.

DESCRIPTION OF SYMBOLS 10 ... Target 12 ... Magnetic phase 14 ... 1st nonmagnetic phase 16 ... 2nd nonmagnetic phase 18, 22, 26, 30, 34 ... Oxide phase 20 ... Co phase 24 ... 69 Co-22Cr-9Pt alloy phase 28 ... 5Co-95Pt alloy phase 32 ... 10Co-90Pt alloy phase

Claims (17)

A magnetron sputtering target having a ferromagnetic metal element,
Wherein the ferromagnetic magnetic phase comprising a metallic element, comprising the ferromagnetic metal element and the constituent elements or different non-magnetic phase of its content, a magnetron sputtering target for chromatic and oxide phase,
A magnetron sputtering target characterized by having an average leakage magnetic flux rate of 50% or more based on ASTM F2086-01 when φ152.4 mm × 7.0 mm in thickness . In claim 1,
The magnetron sputtering target, wherein the plurality of nonmagnetic phases are two types of nonmagnetic phases. In claim 1 or 2,
The magnetron sputtering target, wherein the ferromagnetic metal element is Co. In claim 3,
The magnetron sputtering target, wherein the magnetic phase is made of a Co—Cr alloy phase having a Co content of 85 at% or more. In claim 3,
The magnetron sputtering target, wherein the magnetic phase is a simple substance of Co. In any one of Claims 3-5,
At least one of the nonmagnetic phases is a Co—Cr alloy phase in which the Co content is greater than 0 at% and less than or equal to 75 at% or the Co content ratio is greater than 0 at% and less than 73 at%. A magnetron sputtering target comprising a Pt alloy phase. In any one of Claims 3-6,
At least one of the nonmagnetic phases comprises a Co—Pt alloy phase having a Co content of 12 at% or less. In any one of Claims 1-7,
The oxide _{phase, SiO 2, TiO 2, Ti} 2 O 3, Ta 2 O 5, Cr 2 O 3, CoO, Co 3 O 4, B 2 O 5, Fe 2 O 3, CuO, Y 2 O 3 MgO, Al ₂ O ₃ , ZrO ₂ , Nb ₂ O ₅ , MoO ₃ , CeO ₂ , Sm ₂ O ₃ , Gd ₂ O ₃ , WO ₂ , WO ₃ , HfO ₂ , NiO ₂ A magnetron sputtering target comprising: In any one of Claims 1-8,
The target for magnetron sputtering, wherein the target is used for forming a magnetic recording layer. Magnetron sputtering target manufacturing method using magnetic metal powder containing a ferromagnetic metal element, a plurality of nonmagnetic metal powders containing the ferromagnetic metal element and having different constituent elements or different content ratios, and oxide powder And
When the shape of the obtained magnetron sputtering target is φ152.4 mm × thickness 7.0 mm, the average leakage magnetic flux rate based on ASTM F2086-01 of the obtained magnetron sputtering target is 50% or more. A method for manufacturing a target for magnetron sputtering. In claim 10,
The method of manufacturing a target for magnetron sputtering, wherein the plurality of nonmagnetic metal powders are two types of nonmagnetic metal powders. In claim 10 or 11,
The method of manufacturing a magnetron sputtering target, wherein the ferromagnetic metal element is Co. In claim 12,
The method of manufacturing a target for magnetron sputtering, wherein the magnetic metal powder contains Co and Cr as main components, and the content ratio of Co in the magnetic metal powder is 85 at% or more. In claim 12,
The method of manufacturing a target for magnetron sputtering, wherein the magnetic metal powder is made of simple Co. In any one of Claims 10-14,
At least one of the plurality of non-magnetic metal powders is a Co—Cr alloy having a Co content ratio of greater than 0 at% and 75 at% or less, or a Co—Cr alloy having a Co content ratio of greater than 0 at% and less than 73 at%. A method for producing a target for magnetron sputtering, comprising a Pt alloy. In any one of Claims 10-15,
At least one of the plurality of nonmagnetic metal powders is made of a Co—Pt alloy having a Co content of 12 at% or less.   A magnetron sputtering target obtained by the production method according to claim 10.