Patent Application
20180061545
The present invention relates to a thin film magnet manufactured by a thin-film process and a method for manufacturing a thin film magnet.
Thin film magnets have been used as permanent magnets for use in equipment, such as sensors, actuators, and motors, in recent years. In a thin film magnet, a magnetic layer containing magnetic particles is formed on a substrate. A known magnetic layer contains samarium cobalt (SmCo), which is one of rare-earth element (R)-cobalt (Co) compounds, as a magnetic layer (see, for example, PTL 1).
In another known thin film magnet, layers containing Ta in order to reduce oxidation of a magnetic layer are disposed on both surface of the magnetic material to sandwich the magnetic layer (see, for example, PTL 2).
PTL 1: Japanese Patent Laid-Open Publication No. 2004-134416
PTL 2: Japanese Patent Laid-Open Publication No. 2003-17320
A thin film magnet includes a substrate, an oxidation-inhibiting layer in an amorphous state disposed on an upper surface of the substrate, a first magnetic layer disposed on the oxidation-inhibiting layer, an intermediate layer disposed on the first magnetic layer, a second magnetic layer disposed on the intermediate layer, and a second oxidation-inhibiting layer in an amorphous state disposed above the second magnetic layer. The intermediate layer contains metal particles. The metal particles are diffused in the first magnetic layer and the second magnetic layer. The concentration of the metal particles in a part of the first magnetic layer decreases as a distance from the intermediate layer to the part of the first magnetic layer increases. The concentration of the metal particles in a part of the second magnetic layer decreases as a distance from the intermediate layer to the part of the second magnetic layer increases.
Permanent magnets for use in equipment such as sensors, actuators and motors are required to have high energy products. Recent magnets are used for various purposes and required to have various properties in accordance with purposes. For example, equipment such as sensors and actuators need to generate strong magnetic field in specific directions, and thus, a required thin film magnet has anisotropy in a specific direction such as an in-plane direction or a normal direction, a sufficiently large coercive force, and a high residual flux density (residual magnetization as magnet performance).
As described above, a permanent magnet having a high energy product is required as a permanent magnet for use in equipment such as a sensor, an actuator or and a motor. Environments where such equipment is used have become more and more severe through years, and permanent magnets for use in the equipment are required to have high heat resistance and reliability.
In general, a neodymium magnet is known as a permanent magnet having a high energy product. The neodymium magnet, however, needs to be supplemented with dysprosium (Dy), which is a heavy metal whose reserves are small, in order to have high heat resistance, and therefore, is expensive. In view of this, permanent magnets except the neodymium magnet are also demanded.
For example, a permanent magnet using SmxCoy, which is a rare-earth element (R)-cobalt (Co) material, has a relatively high energy product and a high heat resistance and is excellent in temperature characteristics and corrosion resistance. A permanent magnet having a high energy product can have its volume necessary for obtaining the same energy reduced, and electronic equipment or other devices using such a permanent magnet can also be reduced in size. In view of this, attention has been given on permanent magnets using SmxCoy.
Characteristics of a permanent magnet include a residual flux density and a coercive force of a magnetic flux density (B)-magnetic field (H) characteristic. The residual flux density is related to the intensity of a magnetic force generated as a magnet. The coercive force is related to the difficulty in reversing magnetic poles of a magnet by an external magnetic field. In general, as a permanent magnet, it is preferable that the residual flux density and the coercive force are both high and a squareness of magnetization (J)-magnetic field (H) characteristics is high. A thin film magnet has been also developed from the viewpoint of increasing both the residual flux density and the coercive force.
Permanent magnets are used for various purposes and are required to have characteristic in accordance with the purposes. Permanent magnets for use in sensors or actuators are required to generate strong magnetic fields in specific directions. To meet such a request for magnets, there have been developed magnets not only having increased residual flux density and coercive force as required in techniques to data but also having characteristics in accordance with purposes.
Specifically, developed is a rare-earth element (R)-cobalt (Co) compound thin film magnet having a strong anisotropy in a predetermined crystal orientation of a crystal material constituting a magnet, that is, having a so-called strong magnetocrystalline anisotropy, showing a sufficiently large coercive force and a high residual flux density, and a square J-H curve showing a relationship between magnetization and a magnetic field.
A permanent magnet for use in, for example, a sensor or an actuator is required to have magnetization directions arranged in an arbitrary single direction or a plurality of specific directions, such as an X direction, a Y direction, and/or a Z direction. In view this, in the case of using the rare-earth element (R)-cobalt (Co) compound having high magnetocrystalline anisotropy described above, a so-called magnetizing process of arranging magnetization in arbitrary directions by using polycrystalline in which crystal orientation is isotropic in three dimensions can be employed. In this case, however, since crystal orientations showing strong magnetization are isotropically arranged in three dimensions, magnetization becomes weak in each desired axial direction, resulting in a failure in producing a necessary magnetic field. In view of this, a process of arranging crystal orientation in specific directions is effective, and with this process, material performance can be efficiently obtained. To obtain a thin film magnet showing strong magnetization in a plurality of arbitrary directions, however, it is necessary to form a buffer layer for reducing a lattice constant difference from a substrate material to control crystal orientation. In general, in the case of using the techniques described above, a technique of performing crystallization simultaneously with crystal growth of a thin film is employed, and thus, the crystal growth needs to be performed in a high-temperature atmosphere, resulting in an increase in cost due to an increase in facility cost and a decrease in throughput. In addition, it is difficult to form a thin film having magnetocrystalline anisotropy in different crystal orientation directions on the same substrate, and formation of such a thin film magnet takes a high cost.
Exemplary embodiments will be hereinafter described in detail with reference to the drawings. In the drawings, especially in cross-sectional views, to facilitate understanding of the structure, ratios between actual dimensions of a thin film magnet and dimensions in the drawings are different between the longitudinal direction and the transverse direction.
Each of the following exemplary embodiments is a specific example of the present disclosure. Numerical values, shapes, materials, components, positions in arrangement of the components, connection states, steps, the order of steps, and so forth are examples, and are not intended to limit the present disclosure. Components of the following exemplary embodiments not recited in an independent claim showing a generic concept will be described as optional components.
In the following exemplary embodiments, a crystal having a hexagonal close-packed structure will be simply referred to as a hexagonal crystal. A crystal having a face-centered cubic structure and a crystal having a body-centered cubic structure will be simply referred to a cubic crystal when these crystals do not need to be distinguished.
Substrate 10 is, for example, a Si substrate having a surface at which a thermal oxidation film of SiO2 serving as an insulator is formed. Substrate 10 is not limited to the Si substrate and may be any substrate that can withstand heat treatment performed later. Substrate 10 may be, for example, a single crystalline substrate made of material, such as heat-resistant glass, a sapphire substrate, or a MgO substrate, a ceramic substrate mainly containing Al2O3, ZrO2, or MgO, or a substrate including a ceramic substrate and a heat-resistant glass glaze formed on the ceramic substrate.
Each of oxidation-inhibiting layers 20a and 20b is constituted by, for example, an amorphous layer containing Ta, which is a high-melting-point metal. The metal contained in oxidation-inhibiting layers 20a and 20b is not necessarily Ta, by may be at least one of Ta, Nb, W, and Mo.
Each of magnetic layers 31 and 33 contains a rare-earth element (R). Specifically, the rare-earth element (R) is Sm. For example, magnetic layers 31 and 33 are constituted by SmCo5 having a hexagonal crystal structure. Each of magnetic layers 31 and 33 has a thickness of about 250 nm in stacking direction D1. Magnetic layers 31 and 33 may be constituted by Sm2Co17 having a rhombohedral crystal structure, besides SmCo5. In accordance with the embodiments, in cases where SmCo5 and Sm2Co17 are not distinguished from each other, these materials are simply referred to as SmxCoy with positive numbers x and y.
Intermediate layer 32 contains metal particles 32p having a coercive force lower than that of magnetic layer 31 and exhibiting a residual magnetization larger than that of magnetic layer 31. In stacking direction D1, intermediate layer 32 is sufficiently thinner than any of magnetic layers 31 and 33 and has a thickness ranging, e.g. from about 1 nm to about 10 nm. Intermediate layer 32 is made of a material having a crystallization temperature lower than that of each of magnetic layers 31 and 33 in order to cause magnetic layers 31 and 33 to be in an amorphous state during formation of magnetic layer 33 subsequent to the formation of magnetic layer 31 and intermediate layer 32.
Intermediate layer 32 is constituted by, e.g. a layer containing metal particles 32p made of Co or Cu. Co constituting intermediate layer 32 has a face-centered cubic structure, i.e., a cubic crystal oriented in a (110) direction. Cu constituting intermediate layer 32 has a face-centered cubic structure, i.e., a cubic crystal oriented in a (111) direction.
In a case where intermediate layer 32 contains Co, magnetic layers 31 and 33 has a hexagonal crystal or a rhombohedral crystal oriented in a (11-20) direction of SmxCoy after crystallization. Thus, each of magnetic layers 31 and 33 has a structure in which a plane parallel to upper surface 810 of substrate 10 is oriented in parallel with a (11-20) plane of SmxCoy as a hexagonal crystal or a rhombohedral crystal. Magnetic layers 31 and 33 thus have magnetocrystalline anisotropy in in-plane direction D10a parallel to upper surface 810 of substrate 10. Metal particles 32p of Co are diffused in magnetic layers 31 and 33. The concentration of metal particles 32p of Co diffused in a part of each magnetic layer decreases as the distance from intermediate layer 32 to the part of the magnetic layer increases.
Magnetocrystalline anisotropy of magnetic layers 31 and 32 is affected by the direction of crystal orientation in boundaries in intermediate layer 32 with magnetic layer 31 and magnetic layer 32. Thus, in the case where intermediate layer 32 is constituted by three layers, magnetocrystalline anisotropy of magnetic layer 31 is affected by the direction of crystal orientation of lower layer 32b while magnetocrystalline anisotropy of magnetic layer 32 is affected by the direction of crystal orientation of upper layer 32c.
In the following description of the present disclosure, a case where intermediate layer 32 is a single layer and a case where intermediate layer 32 is constituted by plural layers will not be distinguished. When the description is directed to the composition and crystal orientation of intermediate layer 32, attention is focused on the boundaries between intermediate layer 32 and each of magnetic layers 31 and 32.
Magnetization of thin film magnet 1 will be described below.
As shown in
In a case where metal particles 32p of intermediate layer 32 is made of Cu, magnetic layer 31 and magnetic layer 33 are oriented in a (0001) direction of SmxCoy that is a hexagonal crystal or a rhombohedral crystal after crystallization. Thus, each of magnetic layer 31 and magnetic layer 33 has a structure in which a (0001) plane of SmxCoy as a hexagonal crystal or a rhombohedral crystal is parallel to surface 810 of substrate 10. Magnetic layers 31 and 33 thus have magnetocrystalline anisotropy in normal direction D10b perpendicular to surface 810 of substrate 10. Metal particles 32p made of Cu are dispersed in magnetic layers 31 and 33. The concentration of metal particles 32p made of Cu diffused in a part of magnetic layer 31 decreases as the distance from intermediate layer 32 to the part of magnetic layer 31 increases, and the concentration of metal particles in a part of magnetic layer 33 decreases as the distance from intermediate layer 32 to the part of magnetic layer 33 increases.
In the case that metal particles 32p made of Cu oriented in the (111) direction are dispersed in intermediate layer 32, in thin film magnet 1 after heat treatment, magnetic layers 31 and 33 have magnetocrystalline anisotropy in normal direction D10b and produce strong magnetic fields in normal direction D10b.
A configuration of thin film magnet 100 according to Embodiment 1 will be described below.
Thin film magnet 100 has a structure in which plural magnetic bodies 30 each including magnetic layer 31, intermediate layer 32, and magnetic layer 33 of thin film magnet 1 described above are stacked on one another. More specifically, thin film magnet 100 has a structure in which magnetic body 40 having a structure of magnetic body 30 and oxidation-inhibiting layer 20c are further stacked on oxidation-inhibiting layer 20b of thin film magnet 1 described above.
Specifically, as illustrated in
Oxidation-inhibiting layers 20a, 20b, and 20c are made of materials similar to one another.
Magnetic body 40 has a structure similar to that of magnetic body 30 of thin film magnet 1 described above, and includes magnetic layer 41 disposed on upper surface 820b of oxidation-inhibiting layer 20b, intermediate layer 42 disposed on upper surface 841 of magnetic layer 41, and magnetic layer 43 disposed on upper surface 842 of intermediate layer 42. Upper surface 843 of magnetic layer 43 constitutes upper surface 840 of magnetic body 40. Magnetic body 40 has a structure similar to that of magnetic body 30 of the basic structure of thin film magnet 1 described above. Magnetic layer 41, intermediate layer 42, and magnetic layer 43 correspond to magnetic layer 31, intermediate layer 32, and magnetic layer 33 of magnetic body 30, respectively, in the basic structure of thin film magnet 1 described above.
Oxidation-inhibiting layer 20c is disposed on upper surface 840 of magnetic body 40 (on upper surface 843 of magnetic layer 43).
Intermediate layer 32 contains metal particles 32p made of, e.g. Co. As described above, magnetic layers 31 and 33 are oriented in parallel with a (11-20) plane of SmxCoy as a hexagonal crystal or a rhombohedral crystal with respect to surface 810 of substrate 10. Thus, magnetic layers 31 and 33 have magnetocrystalline anisotropy in in-plane direction D10a parallel to surface 810 of substrate 10.
Intermediate layer 42 contains metal particles 42p made of, e.g. Cu. Magnetic layers 41 and 43 are oriented such that a (0001) plane of SmxCoy of a hexagonal crystal or a rhombohedral crystal is parallel to surface 810 of substrate 10. Thus, magnetic layers 41 and 43 have magnetocrystalline anisotropy in normal direction D10b perpendicular to surface 810 of substrate 10.
In accordance with Embodiment 1, SmxCoy is used as a specific example of a rare-earth element (R)-cobalt (Co) compound. Alternatively, Pr, Nd, Y, La, or Gd may be used as a rare-earth element.
A method for manufacturing thin film magnet 100 according to the embodiment will be described below.
In the manufacturing of thin film magnet 100, first, substrate 10 is prepared. Substrate 10 may be, as described above, a Si substrate having a surface having a thermal oxidation film of SiO2 serving as an insulator formed.
Next, as illustrated in
After that, as illustrated in
The surface temperature of substrate 10 is determined based on a result obtained by previously measuring the temperature of another substrate having the same thermal capacity as substrate 10 with a thermocouple embedded in the substrate. The lower limit of the temperature of substrate 10 is determined in consideration of a reaction rate of sputtering and cooling capacity, and may be a room temperature. In the case of using a device having a cooling ability, the lower limit of the temperature of substrate 10 may be lower than room temperature.
The surface temperature of substrate 10 is thus determined to be lower than a crystallization temperature of SmxCoy, and allows the crystal structure of magnetic layer 31 immediately after deposition of SmxCoy by sputtering to be in an amorphous state.
The deposition of SmxCoy may use an alloy having an adjusted composition. The alloy having an adjusted composition can be obtained by adjusting electric power ratio between a single Sm metal and a single Co metal and performing sputtering at the same time (co-sputtering). Alternatively, the alloy may have a super lattice structure subjected to composition control by adjusting a thickness ratio between a single Sm metal and a single Co metal. In the case of using the super lattice structure, a super lattice layer of a Sm metal layer and a Co metal layer in an amorphous state is formed while the thickness of the super lattice structure may be preferably equal to or smaller than 1 nm.
Subsequently, as illustrated in
After that, as illustrated in
The temperature in the forming of magnetic layer 31, intermediate layer 32, and magnetic layer 33 may be a room temperature, and the surface temperature of substrate 10 at the starting of formation of these layers may range from 16° C. to 25° C.
Then, as illustrated in
After that, as illustrated in
Subsequently, as illustrated in
Then, as illustrated in
The temperature in the forming of magnetic layer 41, intermediate layer 42, and magnetic layer 43 may be a room temperature, and the surface temperature of substrate 10 at the starting of formation of these layers may range from 16° C. to 25° C.
Subsequently, oxidation-inhibiting layer 20c is formed on upper surface 843 of magnetic layer 43 by a thin film formation technique. Similarly to oxidation-inhibiting layer 20b, oxidation-inhibiting layer 20c is formed by depositing Ta by sputtering. At this moment, oxidation-inhibiting layer 20c deposited on magnetic layer 43 is in an amorphous state.
Next, substrate 10 including oxidation-inhibiting layer 20a, magnetic layer 31, intermediate layer 32, magnetic layer 33, oxidation-inhibiting layer 20b, magnetic layer 41, intermediate layer 42, magnetic layer 43, and oxidation-inhibiting layer 20c is crystallized by a heat treatment. The heat treatment is preferably performed in a vacuum atmosphere, a reduction atmosphere, or a non-oxidizing atmosphere. The vacuum atmosphere is preferably an ultrahigh vacuum or extremely high vacuum atmosphere from which residual oxygen and residual water are sufficiently removed. The reduction atmosphere is preferably an atmosphere to which hydrogen is introduced after evacuation to change the back pressure to an extremely high vacuum. The non-oxidizing atmosphere is preferably an atmosphere to which an argon (Ar) gas is introduced after exhausting to an extremely high vacuum.
The temperature at the heat treatment is determined such that the surface temperature of substrate 10 is equal to higher than 500° C. The upper limit of the temperature of the heat treatment on substrate 10 is not specifically limited, and may be in a range in which any magnetic layer 31 and magnetic layer 33 is not oxidized by, e.g. a SO2 carrier gas supplied from the device and diffused into magnetic body 30. The heat treatment temperature is preferably lower than crystallization temperatures of oxidation-inhibiting layer 20a, oxidation-inhibiting layer 20b, and oxidation-inhibiting layer 20c in order to enable oxidation-inhibiting layer 20a, oxidation-inhibiting layer 20b, and oxidation-inhibiting layer 20c to maintain the amorphous state.
Crystallization by heat treatment may be performed in a vacuum while a surface temperature of substrate 10 is equal to or higher than 500° C. and equal to or lower than 700° C. The back pressure of the device before the start of heating may be equal to or lower than 10−4 Pa, and the pressure at the heating may be equal to or lower than 5×10−4 Pa.
The temperature and vacuum conditions of substrate 10 in performing the heat treatment are not limited to these conditions, and may be an atmosphere that can reduce oxidation of magnetic layers 31 and 33 due to diffusion of a SO2 carrier gas into magnetic body 30. For example, the degree of vacuum in the heat treatment may be equal to or lower than 10−3.
The heat treatment causes metal particles 32p of Co in intermediate layer 32 to be diffused to magnetic layers 31 and 33. Magnetic layers 31 and 33 are crystallized. In this crystallization, magnetic layers 31 and 33 are oriented in accordance with orientation of intermediate layer 32. As described above, in the case of using metal particles 32p of Co oriented in the (110) direction for intermediate layer 32, in thin film magnet 100 after the heat treatment, magnetic layers 31 and 33 are oriented such that the (11-20) plane of SmxCoy as a hexagonal crystal or a rhombohedral crystal is parallel to surface 810 of substrate 10. Thus, magnetic layers 31 and 33 have magnetocrystalline anisotropy in in-plane direction D10a. Since oxidation-inhibiting layers 20a and 20b are in an amorphous state in the heat treatment, magnetic layers 31 and 33 are oriented in in-plane direction D10a and crystallized using, as a start point of crystal growth, the interface between intermediate layer 32 and each of magnetic layers 31 and 33.
The heat treatment causes metal particles 42p of Cu in intermediate layer 42 to be diffused into magnetic layers 41 and 43. Magnetic layers 41 and 43 are crystallized. In this crystallization, magnetic layers 41 and 43 are oriented in accordance with orientation of intermediate layer 42. As described above, in the case of using metal particles 42p of Cu oriented in the (111) direction for intermediate layer 42, in thin film magnet 100 after the heat treatment, magnetic layers 41 and 43 are oriented such that the (0001) plane of SmxCoy as a hexagonal crystal or a rhombohedral crystal is parallel to surface 810 of substrate 10. Thus, magnetic layers 41 and 43 have magnetocrystalline anisotropy in normal direction D10b. Since oxidation-inhibiting layers 20c and 20d are in an amorphous state in the heat treatment, magnetic layers 41 and 43 are oriented in normal direction D10b and crystallized using, as a start point of crystal growth, the interface between intermediate layer 42 and each of magnetic layers 41 and 43.
The crystallization of intermediate layers 32 and 42 described above is performed simultaneously by the same heat treatment.
As described above, through the process of performing heat treatment, magnetic layer 31, intermediate layer 32, and magnetic layer 33 constitute magnetic body 30 while magnetic layer 41, intermediate layer 42, and magnetic layer 43 constitute magnetic body 40. Magnetic body 30 has magnetocrystalline anisotropy in in-plane direction D10a parallel to surface 810 of substrate 10 while magnetic body 40 has magnetocrystalline anisotropy in normal direction D10b perpendicular to surface 810 of substrate 10.
After that, magnetic bodies 30 and 40 are magnetized. As a method for magnetization, a magnetic field is applied to magnetic bodies 30 and 40 so that magnetic fluxes penetrate magnetic bodies 30 and 40 in the direction of magnetization.
In general, a magnetic field necessary for magnetic saturation in the direction of an axis of hard magnetization of a magnetic material is sufficiently larger than that in the direction of an axis of easy magnetization. Thus, a magnetic field necessary for magnetic saturation in the hard axis direction (normal direction D10b) of magnetic body 30 having in-plane magnetic anisotropy, for example, is sufficiently larger than a magnetic field necessary for magnetic saturation in the easy axis direction (normal direction D10b) of magnetic body 40 having normal magnetic anisotropy. A magnetic field necessary for magnetic saturation in the hard axis direction (in-plane direction D10a) of magnetic body 40 is sufficiently larger than a magnetic field necessary for magnetic saturation in the easy axis direction (in-plane direction D10a) of magnetic body 30. Thus, coercive forces of magnetic body 30 and magnetic body 40 in the direction of axis of easy magnetization are compared so that magnetization is first performed on one of the magnetic bodies having a larger coercive force and then on the other, in the direction of the easy axis. In a case where a coercive force of magnetic body 30 in the easy axis direction (in-plane direction D10a) is equal to a coercive force of magnetic body 40 in the easy axis direction (normal direction D10b), a magnetic field necessary for saturation is larger in magnetic body 40 under the influence of a demagnetizing field, and thus, magnetization is first performed on magnetic body 40.
The manufacturing method described above allows magnetic body 30 to generate a magnetic field in in-plane direction D10a, and allows magnetic body 40 to generate a magnetic field in normal direction D10b.
The order of strengths of magnetic fields necessary for magnetic saturation is reversed from the order described above between in-plane direction D10a and normal direction D10b depending on various conditions, such as a composition ratio of Sm and Co, crystal orientation, particle size, an additive, and a combination of these conditions. In the case that the order is reversed, the order of performing magnetization may be reversed.
In accordance with the embodiment, the heat treatment and the magnetization are performed separately, but may be performed simultaneously.
As described above, in thin film magnet 100 according to Embodiment 1, SmxCoy having a high energy product is used for magnetic layers 31, 33, 41, and 43. Co and Cu are contained in intermediate layer 32 and intermediate layer 42, respectively. This configuration allows thin film magnet 100 to have magnetocrystalline anisotropy in in-plane direction D10a and normal direction D10b, and have a high energy product, a sufficiently large coercive force, and a high residual flux density. In addition, since magnetic bodies 30 and 40 exhibiting different orientations are stacked, magnetic bodies 30 and 40 having magnetic anisotropy in in-plane direction D10a and normal direction D10b are formed simultaneously in thin film magnet 100.
The c axes of crystalline particles of magnetic body 30, that is, axes in the (0001) direction of SmxCoy, are generally oriented in in-plane direction D10a. However, magnetic body 30 according to Embodiment 1 has a polycrystal structure and includes crystalline dispersion, and thus, it is not intended that the c axes of all the crystalline particles are completely oriented in the same direction in a plane. For example, in the case that Co is used in the intermediate layer, magnetic body 30 has magnetocrystalline anisotropy in in-plane direction D10a. This, however, means that the c axes of crystalline particles of magnetic body 30 are generally oriented in in-plane direction D10a and does not mean that the c axes of all the crystalline particles are completely oriented in in-plane direction D10a. In magnetic body 30 in accordance with Embodiment 1, the c axes are oriented in in-plane direction D10a as a whole. As long as the number of crystalline particles having c axes at angles ranging from 0° to 45° with respect to in-plane direction D10a is larger than the number of crystalline particles having c axes at angles ranging from 45° to 90° with respect to in-plane direction D10a, similar advantages can be obtained although the degree of the advantages is different.
Regarding magnetocrystalline anisotropy in in-plane direction D10a, in accordance with Embodiment 1, magnetocrystalline anisotropy isotropically appears in in-plane direction D10a in magnetic body 30. In this manner, on the same substrate 10, thin film magnets having large coercive forces in arbitrary directions of in-plane direction D10a and normal direction D10b can be formed simultaneously. Magnetization can be caused in an arbitrary direction in in-plane direction D10a.
Since in-plane magnetic anisotropy in in-plane direction D10a is isotropic, magnetization may be performed such that magnetic fields are generated in two different directions from each other by about 90° in in-plane direction D10a. This configuration provides thin film magnet 100 capable of efficiently generating magnetic fields in three directions of, for example, the X direction, the Y direction, and the Z direction at once on the same substrate 10.
In accordance with Embodiment 1, magnetic layers 31, 33, 41, and 43 are made of SmxCoy, but may not be made of SmxCoy. For example, part of Co may be replaced by Cu and Fe to enhance magnetization and a coercive force as a material. To increase the effect of replacement between Co and other elements, Zr or other elements may be mixed as an additive. In magnetic layers 31, 33, 41, and 43, Co of SmxCoy may be replaced by Fe so that Sm2Fe17N3 containing N, which is an interstitial material, is obtained. Sm2Fe17N3 is a rhombohedral crystal. In this case, magnetic layers 31, 33, 41, and 43 may be produced in an atmosphere subjected to nitrogen replacement in crystallization to cause nitrogen to enter. A material containing a nitride material may be used for magnetic layers 31, 33, 41, and 43 and intermediate layer 32.
In this case, since Sm—Fe—N is discomposed at a temperature equal to or higher than 650° C., magnetic layers 31, 33, 41, and 43 are preferably crystallized at a temperature equal to or lower than 600° C.
Specifically, an amorphous SmFeN layer may be formed above substrate 10 by performing a low-temperature sputtering on a SmFeN target in a mixed atmosphere of Ar gas and N2 gas. Alternatively, an amorphous SmFeN may be formed above substrate 10 by performing a low-temperature sputtering on a SmFe target in mixed atmosphere of Ar gas and N2 gas.
After that, the back pressure of the SmFeN layer formed above substrate 10 is evacuated to a vacuum atmosphere or an extremely high vacuum, and then, is subjected to a heat treatment in high-purity nitrogen at a pressure adjusted to be reduced. This configuration crystallizes SmFeN.
In accordance with Embodiment 1 described above, magnetic body 30 has magnetocrystalline anisotropy in in-plane direction D10a while magnetic body 40 has magnetocrystalline anisotropy in normal direction D10b. Alternatively, magnetocrystalline anisotropy of magnetic body 30 may appear in normal direction D10b while magnetocrystalline anisotropy of magnetic body 40 may appear in in-plane direction D10a. More specifically, intermediate layer 32 may be constituted by Cu oriented in the (111) direction while intermediate layer 42 may be constituted by Co oriented in the (110) direction.
Instead of Co, intermediate layer 32 described above may contain Fe that is a cubic crystal having a (110) plane oriented in parallel with surface 810 of substrate 10. Similarly, instead of Co, CoFe that is a cubic crystal having a (110) plane oriented in parallel with surface 810 of substrate 10 may be used. In intermediate layer 42, Cu may be replaced by Ni having a (111) plane with crystalline orientation. In intermediate layer 32, Cu may be replaced by metal particles 32p of a hexagonal crystal having a (0001) plane with crystalline orientation. In metal particles 32p of this hexagonal crystal, Ti, Co, Zr, Mg, or Hf may be used. In particular, Ti is preferable because of a small amount of lattice mismatch. Co as a hexagonal crystal can be obtained by controlling conditions of sputtering. Materials constituting intermediate layers 32 and 42 may be replaced with each other.
Each of oxidation-inhibiting layers 20a, 20b, and 20c may contain Nb, W, or Mo, instead of Ta. Oxidation-inhibiting layers 20a, 20b, and 20c are preferably made of non-magnetic materials and have high melting points. In particular, each of oxidation-inhibiting layers 20a, 20b, and 20c preferably has a melting point equal to or higher than three times as high as the heat treatment temperature at which SmCo5 films of magnetic layers 31, 33, 41, and 43 are crystallized. This configuration can effectively reduce recrystallization of oxidation-inhibiting layers 20a, 20b, 20c in the crystallizing of magnetic layers 31, 33, 41, and 43. Each of oxidation-inhibiting layers 20a, 20b, and 20c contain at least one of Ta, Nb, W, and Mo.
Oxidation-inhibiting layer 20a, oxidation-inhibiting layer 20b, and oxidation-inhibiting layer 20c do not need to be made of the same material, but are made of the same material in this exemplary embodiment from the viewpoint of reduction of materials to be used.
Intermediate layers 32 and 42 may not necessarily be continuous in in-plane direction D10a of substrate 10, and may have partially island shapes or be interrupted. In this cases raise no problems in function. That is, in accordance with Embodiment 1, the “intermediate layer” includes any layer disposed between magnetic layers including not only a case where the intermediate layer is continuous in in-plane direction D10a of substrate 10 but also a case where the intermediate layer has partially an island shape or be interrupted.
The presence of intermediate layers 32 and 42 may be detected by a method of performing observation with a transmission electron microscope. In addition to the observation with a transmission electron microscope, a method of measuring the concentrations of metal particles 32p and 42p constituting intermediate layers 32 and 42 and determining, as intermediate layers 32 and 42, regions where the distribution concentrations of metal particles 32p and 42p are locally high.
It was confirmed that similar advantages can be obtained when the thickness of each of intermediate layers 32 and 42 in stacking direction D1 changes within a range from 1 nm to 30 nm. The observation with a scanning-type transmission electron microscope confirmed a structure in which intermediate layer 32 spreads into magnetic layers 31 and 33 to have partially island shapes in magnetic body 30. Thus, it can be concluded that the same advantages can be obtained when the thicknesses changes, as described above.
A modification of Embodiment 1 will be described below.
As illustrated in
In thin film magnet 100 illustrated in
More specifically, in thin film magnet 200, as illustrated in
In general, in a thin film magnet having magnetocrystalline anisotropy in the normal direction, a demagnetizing field inversely proportional to the thickness of the thin film is generated in the thickness direction, and thus, the intensity of magnetization significantly depends on the thickness of the thin film That is, as the thickness decreases, the intensity of magnetization of the thin film magnet decreases. This may cause degradation of performance, such as a decrease in the density of magnetic fluxes generated from magnetic body 40 to the outside or a flux reversal in a magnetic field opposite to the magnetization direction.
In thin film magnet 200, since the directions of magnetization of regions 40a and 40b of magnetic body 40 in normal direction D10b is opposite to each other, a magnetic flux that has penetrated region 40a in downward direction D910b parallel to normal direction D10b penetrates magnetic body 30 having magnetocrystalline anisotropy in in-plane direction D10a, and further penetrates region 40b in upward direction D810b parallel to normal direction D10b. Thus, the magnetic path length in which magnetic fluxes pass increases and the influence of a demagnetizing field decreases so that magnetization increases. Accordingly, in thin film magnet 200, magnetization in normal direction D10b increases, stabilizing the direction of magnetization in magnetic body 40. In a configuration including a soft magnetic layer instead of magnetic body 30, stability of the direction of magnetization in magnetic body 40 can be obtained, but in heat treatment, degradation of surface properties of the soft magnetic layer, alloying due to inter-diffusion, or degradation of magnetic properties due to particle growth, occurs. On the other hand, thin film magnet 200 described above does not raise such problems.
As an example, in magnetic body 40, the thickness of each of magnetic layers 41 and 43 in stacking direction D1 (normal direction D10b) is about 250 nm while the thickness of intermediate layer 42 in stacking direction D1 (normal direction D10b) ranges from about 5 nm to about 100 nm. The width of each of regions 40a and 40b in in-plane direction D10a is, e.g. about several micrometers.
In thin film magnet 100 according to Embodiment 1 illustrated in
As illustrated in
Thin film magnet 300a includes oxidation-inhibiting layer 320a provided on upper surface 810 of substrate 10, magnetic body 330 provided on upper surface 8320a of oxidation-inhibiting layer 320a, and oxidation-inhibiting layer 320b provided on upper surface 8330 of magnetic body 330. Substrate 10, oxidation-inhibiting layer 320a, magnetic body 330, and oxidation-inhibiting layer 320b are stacked on one another in this order in stacking direction D1. Magnetic body 330 includes magnetic layer 331 provided on upper surface 8320a of oxidation-inhibiting layer 320a, intermediate layer 332 provided on upper surface 8331 of magnetic layer 331, and magnetic layer 333 provided on upper surface 8332 of intermediate layer 332. Magnetic layer 331, intermediate layer 332, and magnetic layer 333 are stacked on one another in this order in stacking direction D1. Upper surface 8333 of magnetic layer 333 constitutes upper surface 8330 of magnetic body 330. Magnetic layer 330 has magnetocrystalline anisotropy in in-plane direction D10a.
Intermediate layer 332 includes metal particles 332p having a coercive force lower than that of magnetic layer 331 and exhibiting residual magnetization higher than that of magnetic layer 331. Metal particles 332p are diffused in magnetic layers 331 and 333. The concentration of diffused metal particles 332p at a part of magnetic layer 331 decreases as the distance from intermediate layer 332 to the part of magnetic layer 331 increases. The concentration of diffused metal particles 332p at a part of magnetic layer 333 decreases as the distance from intermediate layer 332 to the part of magnetic layer 333 increases
Thin film magnet 300b includes oxidation-inhibiting layer 320c provided on upper surface 810 of substrate 10, magnetic body 340 provided on upper surface 8320c of oxidation-inhibiting layer 320c, and oxidation-inhibiting layer 320d provided on upper surface 8340 of magnetic body 340. Substrate 10, oxidation-inhibiting layer 320c, magnetic body 340, and oxidation-inhibiting layer 320d are stacked on one another in this order in stacking direction D1. Magnetic body 340 includes magnetic layer 341 provided on upper surface 8320c of oxidation-inhibiting layer 320c, intermediate layer 342 provided on upper surface 8341 of magnetic layer 341, and magnetic layer 343 provided on upper surface 8342 of intermediate layer 342. Magnetic layer 341, intermediate layer 342, and magnetic layer 343 are stacked on one another in this order in stacking direction D1. Upper surface 8343 of magnetic layer 343 constitutes upper surface 8340 of magnetic body 340. Magnetic layer 340 has magnetocrystalline anisotropy in normal direction D10b.
Intermediate layer 342 includes metal particles 342p having a coercive force lower than that of magnetic layer 341 and showing residual magnetization higher than that of magnetic layer 341. Metal particles 342p are diffused in magnetic layers 341 and 343. The concentration of diffused metal particles 342p at a part of magnetic layer 341 decreases as the distance from intermediate layer 342 to the part of magnetic layer 341 increases. The concentration of diffused metal particles 342p at a part of magnetic layer 343 decreases as the distance from intermediate layer 342 to the part of magnetic layer 343 increases.
In such a configuration, magnetic body 330 and magnetic body 340 exhibiting different orientations are formed in the same plane by a single manufacturing process so that thin film magnet 300 having magnetocrystalline anisotropy in in-plane direction D10a and normal direction D10b can be provided at once.
A method for manufacturing thin film magnet 300 will be described below.
In manufacturing of thin film magnet 300, substrate 10 is first prepared similarly to the manufacturing of thin film magnet 100 according to Embodiment 1. Substrate 10 is a Si substrate, having a surface having a thermal oxidation film of SiO2 serving as an insulator formed at the surface, as described above.
Next, as illustrated in
Oxidation-inhibiting layer 420a is formed by depositing Ta by sputtering. At this moment, oxidation-inhibiting layer 420a deposited on upper surface 810 of substrate 10 is in an amorphous state. The metal contained in each of oxidation-inhibiting layer 320a (420a), oxidation-inhibiting layer 320b, oxidation-inhibiting layer 320c (420a), and oxidation-inhibiting layer 320d is not limited to Ta, and may include at least one of Ta, Nb, W, and Mo.
Subsequently, magnetic layer 431 constituting magnetic layers 331 and 341 is formed on upper surface 8420a of oxidation-inhibiting layer 420a by a thin film formation technique. Magnetic layers 331 and 341 are formed simultaneously at once as magnetic layer 431 with the same material by the same process.
Magnetic layer 431 is formed by depositing SmxCoy by sputtering. In the forming of magnetic layer 431, the surface temperature of substrate 10 is equal to or lower than 400° C. to maintain magnetic layer 431 in an amorphous state.
The deposition of SmxCoy may employ an alloy having an adjusted composition, an alloy having a composition obtained by adjusting electric power ratio between a single Sm metal and a single Co metal and performing sputtering at the same time (co-sputtering), or an alloy having a super lattice structure subjected to composition control by adjusting a thickness ratio between a single Sm metal and a single Co metal. In the case of employing the super lattice structure, a super lattice layer of a Sm metal layer and a Co metal layer in an amorphous state is formed, and has preferably a super lattice structure equal to or less than 1 nm.
Next, as illustrated in
Similarly to the formation of magnetic layer 431, in the forming of intermediate layer 432, the temperature of substrate 10 is equal to or lower than 400° C. This configuration reduces crystallization of magnetic layer 431, and maintain magnetic layer 431 in an amorphous state. Formation at a lower temperature can minimize the influence of decrease in pattern accuracy caused by a shift of the mask due to the difference in thermal expansion between materials constituting metal mask 350 and substrate 10 at a high temperature or a temperature warp of metal mask 350. Co constituting intermediate layer 432 is crystallized and oriented in the (110) direction.
Subsequently, as illustrated in
Similarly to the formation of magnetic layer 431, in the forming of intermediate layer 442, the temperature of substrate 10 is equal to or lower than 400° C. This configuration reduces crystallization of magnetic layer 431, and maintain magnetic layer 431 in an amorphous state. Formation at a lower temperature can minimize the influence of a shift of the mask due to the difference in thermal expansion between metal mask 360 and substrate 10. Cu constituting intermediate layer 442 is crystallized and oriented in the (111) direction.
Next, as illustrated in
Magnetic layer 433 is formed by depositing SmxCoy by sputtering. Similarly to the formation of magnetic layer 431, in the forming of magnetic layer 433, the temperature of substrate 10 is equal to or lower than 400° C. This configuration maintains the crystal structure of magnetic layer 333 in an amorphous state.
As an example, the temperature in the forming of magnetic layer 431, intermediate layer 432, and magnetic layer 433 may be a room temperature, and the surface temperature of substrate 10 in the starting of the formation of these layers may range from 16° C. to 25° C.
After that, as illustrated in
Similarly to oxidation-inhibiting layer 420a, oxidation-inhibiting layer 420b is formed by depositing Ta by sputtering. At this moment, oxidation-inhibiting layer 420b deposited on upper surface 8433 of magnetic layer 433 is in an amorphous state.
Subsequently, as illustrated in
Then, as illustrated in
After that, as illustrated in
After that, substrate 10 having thin film magnets 300a and 300b provided thereon is crystallized by heat treatment. Conditions for the heat treatment are similar to those for thin film magnet 100 according to Embodiment 1, and their detailed description will not be repeated.
In the above description, resist 370 employs a photosensitive organic resist, but may employ an inorganic material obtained by patterning an inorganic material, such as a non-magnetic metal material or an oxide material, by mask evaporation or other techniques as a substitute for the resist. This material can preferably eliminate the process of removing the resist after patterning, and allow thin film formation, patterning, and heat treatment to proceed without breaking a vacuum atmosphere so that oxidation of side surfaces of magnets 330 and 340 exposed to hole 380 is suppressed.
As a metal material as the non-magnetic material, Ta or W, or SiO2 as an oxide of the non-magnetic material may be used. These materials are selected in consideration of selectivity in etching as a subsequent process. The same material as oxidation-inhibiting layers 320b and 320d may be used as a metal material of the non-magnetic material. In this case, however, each of oxidation-inhibiting layers 320b and 320d has a thickness large enough to allow layers 320b and 320d to function as oxidation-inhibiting layers after the etching.
The heat treatment diffuses metal particles of Co constituting intermediate layer 332 into magnetic layers 331 and 333. Magnetic layers 331 and 333 are crystallized. In this crystallization, the magnetic layers 331 and 333 are oriented in accordance with orientation of intermediate layer 332. As described above, in the case of using Co oriented in the (110) direction for intermediate layer 332, in thin film magnet 100 after the heat treatment, magnetic layers 331 and 333 are oriented such that the (11-20) plane of SmxCoy as a hexagonal crystal or a rhombohedral crystal is parallel to the substrate surface of substrate 10. Thus, magnetic layers 331 and 333 have magnetocrystalline anisotropy in in-plane direction.
The heat treatment causes the metal particles of Cu constituting intermediate layer 342 to be diffused into magnetic layers 341 and 343. Magnetic layers 341 and 343 are crystallized. In this crystallization, the magnetic layers 341 and 343 are oriented in accordance with orientation of intermediate layer 342. As described above, in the case of using Cu oriented in the (111) direction for intermediate layer 342, in thin film magnet 100 after the heat treatment, magnetic layers 341 and 343 are oriented such that the (0001) plane of SmxCoy as a hexagonal crystal or a rhombohedral crystal is parallel to the substrate surface of substrate 10. Thus, magnetic layer 341 and magnetic layer 343 have magnetocrystalline anisotropy in the normal direction.
As described above, the heat treatment allows magnetic layer 331 formed below intermediate layer 332, intermediate layer 332, magnetic layer 333 formed above intermediate layer 332 to constitute magnetic body 330, and allows magnetic layer 341 formed below intermediate layer 342, intermediate layer 342, magnetic layer 343 formed above intermediate layer 342 to constitute magnetic body 340. Magnetic body 330 has magnetocrystalline anisotropy in in-plane direction D10a parallel to surface 810 of substrate 10 while magnetic body 340 has magnetocrystalline anisotropy in normal direction D10b perpendicular to surface 810 of substrate 10.
After that, magnetic bodies 330 and 340 are magnetized. As a method for magnetization, a magnetic field is applied to magnetic bodies 330 and 340 so that magnetic fluxes penetrate magnetic bodies 330 and 340 in the direction of magnetization.
In general, a magnetic field necessary for magnetic saturation in an axis direction in which magnetization of a magnetic material is difficult is much larger than that in an axis direction in which magnetization is easy. Thus, a magnetic field necessary for magnetic saturation in the axis direction in which magnetization of magnetic body 330 having in-plane magnetic anisotropy is difficult (normal direction D10b), for example, is much larger than a magnetic field necessary for magnetic saturation in the axis direction in which magnetization of magnetic body 340 having normal magnetic anisotropy is easy (normal direction D10b). A magnetic field necessary for magnetic saturation in the axis direction in which magnetization of magnetic body 40 is difficult (in-plane direction D10a) is much larger than a magnetic field necessary for magnetic saturation in the axis direction in which magnetization of magnetic body 30 is easy (in-plane direction D10a). Thus, coercive forces of magnetic bodies 330 and 340 in the directions of axes of easy magnetization are compared so that magnetization is first performed on one of the magnetic material having a larger coercive force and then on the other, in the axis direction in which magnetization of the magnetic material is easy. In the case where a coercive force in the axis direction in which magnetization of magnetic body 330 is easy (in-plane direction D10a) is equal to a coercive force in the axis direction in which magnetization of magnetic body 340 is easy (normal direction D10b), a magnetic field necessary for saturation in magnetic body 340 under the influence of a demagnetizing field is larger. In view of this, magnetic body 340 is first magnetized.
In the magnetizing of magnetic body 330, this magnetization is preferably performed with magnetic fluxes larger than a magnetic field necessary for magnetic saturation of magnetic body 330 and smaller than a coercive force of magnetic body 340.
The above manufacturing method allows magnetic body 330 to generate a magnetic field in in-plane direction D10a, and allows magnetic body 340 to generate a magnetic field in normal direction D10b.
The order of intensities of magnetic fields necessary for magnetic saturation is reversed from the order described above between in-plane direction D10a and normal direction D10b depending on various conditions such as a composition ratio of Sm and Co, crystal orientation, particle size, an additive, and a combination of these conditions. When the order is reversed, the order of performing magnetization may be reversed.
In accordance with Embodiment 2, the heat treatment and the magnetization are performed separately, but may be performed simultaneously.
As described above, in thin film magnet 300 according to Embodiment 2, magnetic bodies 330 and 340 exhibiting different orientations are formed on single surface 810. Thus, thin film magnet 300 having magnetocrystalline anisotropy in in-plane direction D10a and normal direction D10b can be obtained at once.
Although the foregoing description is directed to the thin film magnets according to exemplary embodiments of the present disclosure, the present disclosure is not limited to these embodiments.
For example, although SmxCoy as a specific example of a rare-earth element (R)-cobalt (Co) compound is used for a material constituting a magnetic layer in accordance with the above embodiments, a material constituting a magnetic layer is not limited to this, and Pr, Nd, Y, La, or Gd may be used as the rare-earth element. A material in which part of Co in SmxCoy is replaced by Cu and Fe may be used, or a material in which Zr or other elements is mixed as an additive may be used. Alternatively, Co may be replaced by Fe, that is, Sm2Fe17N3 may be used.
As described above, the material of the oxidation-inhibiting layer is not limited to a material containing Ta, and may include Nb, W, or Mo, instead of Ta. The same material may be used for all the oxidation-inhibiting layers, or different materials may be used for the oxidation-inhibiting layers.
The substrate is not limited to a Si substrate having a thermal oxidation film of SiO2 formed at a surface thereof, and may be, for example, a single crystalline substrate, such as heat-resistant glass, a sapphire substrate, or a MgO substrate, a ceramic (containing, as main component, Al2O3, ZrO2, or MgO) substrate, or a substrate including a ceramic substrate and a heat-resistant glass glaze on the ceramic substrate.
The oxidation-inhibiting layer and the magnetic layer intermediate layer may be formed by sputtering as described in accordance with the above embodiments or may be formed by other methods. The heat treatment temperature is not limited to the temperatures described above, and may be changed appropriately depending on materials.
In accordance with Embodiments 1 and 2, the configurations and the manufacturing methods are described using thin film magnets, that is, magnetic materials, as an example. However, the configurations and the production methods are also applicable to other materials, such as a piezoelectric material as well as the magnetic material.
The present disclosure is not limited to the exemplary embodiments. Embodiments in which variations conceivable to those skilled in the art are made on the exemplary embodiments and embodiments using combinations of components of different exemplary embodiments may be included within the range of one or more aspects, as long as these embodiments are within the gist of the present disclosure.
As described above, thin film magnet 100 according to Embodiment 1 includes substrate 10, amorphous oxidation-inhibiting layer 20a provided on substrate 10, magnetic body 30 provided on oxidation-inhibiting layer 20a, amorphous oxidation-inhibiting layer 20b provided on magnetic body 30, magnetic body 40 provided on oxidation-inhibiting layer 20b, and amorphous oxidation-inhibiting layer 20c provided on magnetic body 40. Magnetic body 30 includes magnetic layer 31 provided on oxidation-inhibiting layer 20a, intermediate layer 32 provided on magnetic layer 31, and magnetic layer 33 provided on intermediate layer 32. Intermediate layer 32 includes metal particles 32p. Magnetic body 40 includes magnetic layer 41 provided on oxidation-inhibiting layer 20b, intermediate layer 42 provided on magnetic layer 41, and magnetic layer 43 provided on intermediate layer 42. Intermediate layer 42 includes metal particles 42p. One of magnetic bodies 30 and 40 has magnetocrystalline anisotropy in in-plane direction D10a that is parallel to surface 810 of substrate 10. The other of magnetic bodies 30 and 40 has magnetocrystalline anisotropy in normal direction D10b that is perpendicular to surface 810 of substrate 10.
This configuration provides magnetic bodies 30 and 40 exhibiting different orientations stacked by a single manufacturing process, hence providing thin film magnet 100 in which magnetic bodies 30 and 40 having magnetocrystalline anisotropy in in-plane direction D10a and normal direction D10b, respectively, are stacked on single substrate 10. In addition, thin film magnet 100 has a high energy product, a sufficiently large coercive force, and a high residual flux density.
Each of oxidation-inhibiting layers 20a, 20b, and 20c may contain at least one of tantalum (Ta), niobium (Nb), tungsten (W), and molybdenum (Mo).
This configuration provides oxidation-inhibiting layers 20a, 20b, and 20c having high oxidation reduction function.
Thin film magnet 300 according to Embodiment 2 includes substrate 10, amorphous oxidation-inhibiting layer 320a provided on substrate 10, magnetic body 330 provided on oxidation-inhibiting layer 320a, amorphous oxidation-inhibiting layer 321b provided on magnetic body 330, amorphous oxidation-inhibiting layer 320c provided on substrate 10, magnetic body 340 provided on oxidation-inhibiting layer 320c, and amorphous oxidation-inhibiting layer 320d provided on magnetic body 340. Magnetic body 330 includes magnetic layer 331 provided on oxidation-inhibiting layer 320a, intermediate layer 332 provided on magnetic layer 331, and magnetic layer 333 provided on intermediate layer 332. Intermediate layer 332 includes metal particles 332p. Magnetic body 340 includes magnetic layer 341 provided on oxidation-inhibiting layer 320c, intermediate layer 342 provided on magnetic layer 341, and magnetic layer 343 provided on intermediate layer 342. Intermediate layer 342 includes metal particles 342p. One of magnetic bodies 330 and 340 has magnetocrystalline anisotropy in in-plane direction D10a that is parallel to surface 810 of substrate 10. The other of magnetic bodies 330 and 340 has magnetocrystalline anisotropy in normal direction D10b that is perpendicular to surface 810 of substrate 10.
In this configuration, magnetic bodies 330 and 340 exhibiting different orientations are formed in a single plane by a single manufacturing process so that thin film magnet 300 having magnetocrystalline anisotropy in in-plane direction D10a and normal direction D10b can be formed by a single manufacturing process.
Each of oxidation-inhibiting layers 320a, 320b, 320c, and 320d may contain at least one of tantalum (Ta), niobium (Nb), tungsten (W), and molybdenum (Mo).
This configuration provides oxidation-inhibiting layers 320a, 320b, 320c, and 320d having high oxidation suppressing function.
One of intermediate layer 32 (332) and intermediate layer 42 (342) may be constituted by a crystal with a cubic crystal structure oriented in the (110) direction or a crystal with a hexagonal crystal structure oriented in the (11-20) direction. The other of intermediate layer 32 (332) and intermediate layer 42 (342) may be constituted by a crystal with a cubic crystal structure oriented in the (111) direction or a crystal with a hexagonal crystal structure oriented in the (0001) direction.
This configuration allows orientations of magnetic layers 31, 33, 41, and 43 (331, 333, 341, and 343) to be easily controlled in in-plane direction D10a or normal direction D10b in accordance with orientations of intermediate layers 32 and 42 (332 and 342).
The crystal with a cubic crystal structure oriented in the (110) direction or the crystal with a hexagonal crystal structure oriented in the (11-20) direction is a crystal containing at least one of cobalt (Co) and iron (Fe). The crystal with a cubic crystal structure oriented in the (111) direction or the crystal with a hexagonal crystal structure oriented in the (0001) direction may be a crystal containing titanium (Ti) or zirconium (Zr).
With this configuration, Co for intermediate layers 32 and 42 (332 and 342) allows orientations of magnetic layers 31, 33, 41, and 43 (331, 333, 341, and 343) to be easily controlled in in-plane direction D10a. In addition, Cu for intermediate layers 32 and 42 (332 and 342) allows orientations of magnetic layers 31, 33, 41, and 43 (331, 333, 341, and 343) to be easily controlled in normal direction D10b.
Metal particles 32p (332p) are diffused in magnetic layer 31 (331) and magnetic layer 33 (333). The concentration of metal particles 32p (332p) in a part of magnetic layer 31 (331) may decrease as the distance from intermediate layer 32 (332) to the part of magnetic layer 31 (331) increases. The concentration of metal particles 32p (332p) in a part of magnetic layer 33 (333) may decrease as the distance from intermediate layer 32 (332) to the part of magnetic layer 33 (333) increases. In addition, metal particles 42p (342p) are diffused in magnetic layer 41 (341) and magnetic layer 43 (343). The concentration of metal particles 42p (342p) in a part of magnetic layer 41 (341) may decrease as the distance from intermediate layer 42 (342) to the part of magnetic layer 41 (341) increases. The concentration of metal particles 42p (342p) in a part of magnetic layer 43 (343) may decrease as the distance from intermediate layer 42 (342) to the part of magnetic layer 43 (343) increases.
In this configuration, metal particles 32p and 42p (332p and 342p) diffused in intermediate layers 32 and 42 (332 and 342) allows orientations of magnetic layers 31, 33, 41, and 43 (331, 333, 341, and 343) to be easily controlled in in-plane direction D10a or normal direction D10b in accordance with orientations of intermediate layers 32 and 42 (332 and 342).
In one of magnetic body 30 (330) and magnetic body 40 (340), a crystal may be oriented such that magnetocrystalline anisotropy isotropically occurs in in-plane direction D10a.
With this configuration, on the same substrate 10, thin film magnet 100 (300) having coercive forces in arbitrary directions of in-plane direction D10a and normal direction D10b can be formed at once.
Intermediate layer 32 (332) may have a crystallization temperature lower than that of magnetic layer 31 (331). Intermediate layer 42 (342) may have a crystallization temperature lower than that of magnetic layer 41 (341).
With this configuration, even when intermediate layers 32 and 42 (332 and 342) are crystallized, magnetic layers 31 and 41 (331 and 341) can be maintained in an amorphous state.
Each of magnetic layers 31, 33, 41, and 43 (331, 333, 341, and 343) may contain Co and one of Sm, Pr, Nd, Y, La, and Gd.
With this configuration, a material, such as SmxCoy, containing Sm for magnetic layers 31, 33, 41, and 43 (331, 333, 341, and 343) provides a thin film magnet having a high energy product.
Thin film magnet 100 can be manufactured by the following method. First, oxidation-inhibiting layer 20a in an amorphous state is formed on substrate 10. Magnetic layer 31 in an amorphous state is formed on oxidation-inhibiting layer 20a. Intermediate layer 32 including metal particles 32p is formed on magnetic layer 31. Magnetic layer 33 in an amorphous state is formed on intermediate layer 32. Oxidation-inhibiting layer 20b in an amorphous state is formed on magnetic layer 33. Magnetic layer 41 in an amorphous state is formed on oxidation-inhibiting layer 20b. Intermediate layer 42 including metal particles 42p is formed on magnetic layer 41. Magnetic layer 43 in an amorphous state is formed on intermediate layer 42. Oxidation-inhibiting layer 20c in an amorphous state is formed on magnetic layer 43. A heat treatment is performed on oxidation-inhibiting layers 20a, 20b, and 20c, magnetic layers 31, 33, 42, and 43, and intermediate layers 32 and 42. The heat treatment allows magnetic layers 31 and 33 and intermediate layer 32 to constitute magnetic body 30. Magnetic layers 41 and 43 and intermediate layer 42 constitute magnetic body 40. One of magnetic bodies 30 and 40 has magnetocrystalline anisotropy in in-plane direction D10a that is parallel to surface 810 of substrate 10. The other of magnetic bodies 30 and 40 has magnetocrystalline anisotropy in normal direction D10b that is perpendicular to surface 810 of substrate 10.
With this configuration, magnetic bodies 30 and 40 exhibiting different orientations are stacked by a single manufacturing process, thus providing thin film magnet 100 in which magnetic bodies 30 and 40 having magnetocrystalline anisotropy in in-plane direction D10a and normal direction D10b are stacked on single substrate 10. Thin film magnet 100 has a high energy product, a sufficiently large coercive force, and a high residual flux density.
One of intermediate layers 32 and 42 may be constituted by a crystal with a cubic crystal structure oriented in the (110) direction or a crystal with a hexagonal crystal structure oriented in the (11-20) direction. The other of intermediate layers 32 and 42 may be constituted by a crystal with a cubic crystal structure oriented in the (111) direction or a crystal with a hexagonal crystal structure oriented in the (0001) direction.
This configuration allows orientations of magnetic layers 31, 33, 41, and 43 to be easily controlled in in-plane direction D10a or normal direction D10b in accordance with orientations of intermediate layers 32 and 42.
In the process of forming magnetic layers 31, 33, 41, and 43, magnetic layers 31, 33, 41, and 43 may be made of a material containing Co and at least one of Sm, Pr, Nd, Y, La, and Gd.
With this configuration, a material, such as SmxCoy, containing Sm for magnetic layers 31, 33, 41, and 43 provides thin film magnet 100 having a high energy product.
In the process of forming magnetic layers 31, 33, 41, and 43, magnetic layers 31, 33, 41, and 43 may be formed in an amorphous state. In the process of forming intermediate layers 32 and 42, intermediate layers 32 and 42 may be formed by crystallization. Magnetic layers 31, 33, 41, and 43 may be crystallized by the heat treatment.
This configuration allows orientations of magnetic layers 31, 33, 41, and 43 to be easily controlled in accordance with orientations of intermediate layers 32 and 42.
In the process of forming magnetic layers 31, 33, 41, and 43, magnetic layers 31, 33, 41, and 43 may be formed at the surface temperature of substrate 10 equal to or lower than 400° C. In the process of forming intermediate layers 32 and 42, intermediate layers 32 and 42 may be formed at the surface temperature of substrate 10 equal to or lower than 400° C. The heat treatment may be performed on oxidation-inhibiting layers 20a, 20b, and 20c, magnetic layers 31, 33, 41, and 43, and intermediate layers 32 and 42 at the surface temperature of substrate 10 equal to or higher than 500° C.
With this configuration, in the forming of intermediate layer 32, intermediate layer 32 can be crystallized, and magnetic layer 31 can be maintained in an amorphous state. In addition, in the forming of intermediate layer 42, intermediate layer 42 can be crystallized, and magnetic layer 41 can be maintained in an amorphous state. Thus, orientations of magnetic layers 31 and 33 can be easily controlled in accordance with orientation of intermediate layer 32. Orientations of magnetic layers 41 and 43 can be easily controlled in accordance with orientation of intermediate layer 42.
Thin film magnet 300 can be manufactured by the following method. Oxidation-inhibiting layer 420a in an amorphous state is formed on substrate 10. Magnetic layer 431 in an amorphous state is formed on oxidation-inhibiting layer 420a. Intermediate layer 432 including metal particles 332p is formed on magnetic layer 431. Intermediate layer 442 including metal particles 342p is formed on magnetic layer 431. Magnetic layer 433 in an amorphous state is formed on intermediate layers 432 and 442. Oxidation-inhibiting layer 420b in an amorphous state is formed on magnetic layer 433. Hole 380 penetrating oxidation-inhibiting layers 420a and 420b and magnetic layers 431 and 433 is formed. After the formation of hole 380, a heat treatment is performed on oxidation-inhibiting layers 420a and 420b, magnetic layers 431 and 433, and intermediate layers 432 and 442. The heat treatment allows a portion of magnetic layer 431 located below intermediate layer 332 (magnetic layer 331), intermediate layer 332, and a portion of magnetic layer 433 located above intermediate layer 332 (magnetic layer 333) to constitute magnetic body 330. The heat treatment also allows a portion of magnetic layer 431 located below intermediate layer 342 (magnetic layer 341), intermediate layer 342, and a portion of magnetic layer 433 located above intermediate layer 342 (magnetic layer 343) to constitute magnetic body 340. One of magnetic bodies 330 and 340 has magnetocrystalline anisotropy in in-plane direction D10a that is parallel to surface 810 of substrate 10. The other of magnetic bodies 330 and 340 has magnetocrystalline anisotropy in normal direction D10b that is perpendicular to surface 810 of substrate 10.
In this configuration, magnetic bodies 330 and 340 exhibiting different orientations are formed in a single plane by a single manufacturing process, hence providing thin film magnet 300 having magnetic anisotropy in in-plane direction D10a and normal direction D10b by s single manufacturing process.
One of intermediate layers 332 and 342 may be constituted by a crystal with a cubic crystal structure oriented in the (110) direction or a crystal with a hexagonal crystal structure oriented in the (11-20) direction. The other of intermediate layers 332 and 342 may be constituted by a crystal with a cubic crystal structure oriented in the (111) direction or a crystal with a hexagonal crystal structure oriented in the (0001) direction.
This configuration allows orientations of magnetic layers 331, 333, 341, and 343 to be easily controlled in in-plane direction D10a or normal direction D10b in accordance with orientations of intermediate layers 332 and 342.
In the process of forming magnetic layers 431 and 433, each of magnetic layers 431 and 433 may be made of a material containing Co and at least one of Sm, Pr, Nd, Y, La, and Gd.
With this configuration, a material, such as SmxCoy, containing Co and at least one of Sm, Pr, Nd, Y, La, and Gd for magnetic layers 431 and 433 provides thin film magnet 300 with a high energy product.
In the process of forming magnetic layers 432 and 442, magnetic layers 432 and 442 may be formed by crystallization, and magnetic layers 331, 333, 341, and 343 may be crystallized by heat treatment.
This configuration allows orientations of magnetic layers 331, 333, 341, and 343 to be easily controlled in accordance with orientations of intermediate layers 332 and 342.
In the process of forming magnetic layers 431 and 433, magnetic layers 431 and 433 may be formed at the surface temperature of substrate 10 equal to or lower than 400° C. In the process of forming intermediate layers 432 and 442, intermediate layers 432 and 442 may be formed at the surface temperature of substrate 10 equal to or lower than 400° C. In the process of performing the heat treatment, heat treatment may be performed on oxidation-inhibiting layers 320a to 320d, magnetic layers 331, 333, 341, and 343, and intermediate layers 332 and 342 at the surface temperature of substrate 10 equal to or higher than 500° C.
With this configuration, in the forming of intermediate layers 332 and 342, intermediate layer 332 and 342 can be crystallized, and magnetic layer 331 and magnetic layer 333 can be maintained in an amorphous state. Orientations of magnetic layers 331, 333, 341, and 343 can be easily controlled in accordance with orientations of intermediate layers 332 and 342.
Intermediate layer 442 may be disposed adjacent to intermediate layer 432 at boundary portion P300. In this case, hole 380 including boundary portion P300 may penetrate oxidation-inhibiting layers 420a and 420b, magnetic layers 431 and 433, and intermediate layers 432 and 442.
A method for manufacturing thin film magnet 100a according to Embodiment 4 will be described below.
As indicated in
Next, oxidation-inhibiting layer 20a is formed on upper surface 810 of substrate 10 by a thin film formation technique (step S11). Oxidation-inhibiting layer 20a is formed by depositing Ta by sputtering. At this moment, oxidation-inhibiting layer 20a deposited on upper surface 810 of substrate 10 is in an amorphous state. The metal contained in each of oxidation-inhibiting layers 20a and 20b is not limited to Ta, and may include at least one of Ta, Nb, W, and Mo.
Then, magnetic layer 31 is formed on upper surface 820a of oxidation-inhibiting layer 20a by a thin film formation technique (step S12). Magnetic layer 31 is formed by depositing SmxCoy by sputtering. In the forming of magnetic layer 31, the surface temperature of substrate 10 is equal to or lower than 400° C. The surface temperature of substrate 10 equal to or lower than 400° C. allows magnetic layer 31 to be formed at a temperature lower than a crystallization temperature of SmxCoy in order to maintain magnetic layer 31 in an amorphous state.
The surface temperature of substrate 10 is determined based on a result obtained by previously measuring the temperature of another substrate having the same thermal capacity as substrate 10 with a thermocouple embedded in the substrate. The lower limit of the temperature of substrate 10 may be a room temperature in consideration of a reaction rate of sputtering and cooling ability. In the case of using a device having cooling ability, the lower limit of the temperature of substrate 10 may be lower than a room temperature.
The temperature of substrate 10 is thus lower than the crystallization temperature of SmxCoy so that the crystal structure of magnetic layer 31 immediately after deposition of SmxCoy by sputtering is maintained in an amorphous state.
Then, intermediate layer 32 is formed on upper surface 831 of magnetic layer 31 by a thin film formation technique (step S13). Intermediate layer 32 is formed by depositing Co by sputtering. Similarly to the formation of magnetic layer 31, in the forming of intermediate layer 32, the temperature of substrate 10 is equal to or lower than 400° C. This configuration reduces crystallization of magnetic layer 31, and maintains magnetic layer 31 in an amorphous state. Co constituting intermediate layer 32 is crystallized and oriented in the (110) direction. In order to crystallize Co oriented in the (110) direction, formation conditions of sputtering are controlled.
After that, magnetic layer 33 is formed on upper surface 832 of intermediate layer 32 by a thin film formation technique (step S14). Magnetic layer 33 is formed by depositing SmxCoy by sputtering. Similarly to the formation of magnetic layer 31, in the forming of magnetic layer 33, the temperature of substrate 10 is equal to or lower than 400° C. The crystal structure of magnetic layer 33 immediately after deposition of SmxCoy by sputtering is maintained in an amorphous state.
As an example, the temperature in the forming of magnetic layer 31, intermediate layer 32, and magnetic layer 33 may be a room temperature. The surface temperature of substrate 10 at starting formation of these layers may range from 16° C. to 25° C.
Subsequently, oxidation-inhibiting layer 20b is formed on upper surface 833 of magnetic layer 33 by a thin film formation technique (step S15). Similarly to oxidation-inhibiting layer 20a, oxidation-inhibiting layer 20b is formed by depositing Ta by sputtering. At this moment, oxidation-inhibiting layer 20b deposited on upper surface 833 of magnetic layer 33 is in an amorphous state.
Next, substrate 10 having oxidation-inhibiting layer 20a, magnetic layer 31, intermediate layer 32, magnetic layer 33, and oxidation-inhibiting layer 20b formed thereon is crystallized by a heat treatment (step S16). The heat treatment is preferably performed in a vacuum atmosphere, a reduction atmosphere, or a non-oxidizing atmosphere. The vacuum atmosphere is preferably an ultrahigh vacuum or extremely high vacuum atmosphere from which residual oxygen and residual water are sufficiently removed. The reduction atmosphere is preferably a hydrogen atmosphere in which replacement with hydrogen is performed after evacuation to an extremely high vacuum. The non-oxidizing atmosphere is preferably an atmosphere in which replacement with argon (Ar) is performed after evacuation to an extremely high vacuum.
The temperature of the heat treatment is determined such that the surface temperature of substrate 10 is equal to or higher than 500° C. The upper limit of the temperature of heat treatment on substrate 10 is not specifically limited, and may be within a range in which magnetic layers 31 and 33 are not oxidized by, e.g. a SO2 carrier gas supplied from the device for heat treatment and diffused into magnetic body 30. The heat treatment temperature is preferably lower than the crystallization temperatures of oxidation-inhibiting layers 20a and 20b in order to maintain oxidation-inhibiting layers 20a and 20b in an amorphous state.
As an example, crystallization by heat treatment may be performed in a vacuum at a surface temperature of substrate 10 equal to or higher than 500° C. or and equal to or lower than 700° C. The back pressure of the device before the start of heating may be equal to or lower than 10−4 Pa while the pressure in heating may equal to or lower than 5×10−4 Pa.
The temperature and vacuum conditions of substrate 10 in performing the heat treatment are not limited to these conditions, and may be an atmosphere that can suppress oxidation of magnetic layers 31 and 33 due to diffusion of a SO2 carrier gas into magnetic body 30. For example, the degree of vacuum in the heat treatment may be equal to or lower than 10−3 Pa.
The heat treatment allows metal particles 32p of Co constituting intermediate layer 32 to be diffused into magnetic layers 31 and 33. Magnetic layers 31 and 33 are crystallized. In this crystallization, magnetic layers 31 and 33 are oriented in accordance with orientation of intermediate layer 32. As described above, in the case of using Co oriented in the (110) direction for intermediate layer 32, in thin film magnet 100a after the heat treatment, magnetic layers 31 and 33 are oriented such that the (11-20) plane of SmxCoy as a hexagonal crystal or a rhombohedral crystal is parallel to surface 810 of substrate 10. Thus, magnetic layers 31 and 33 have magnetocrystalline anisotropy in in-plane direction D10a.
In the process of forming intermediate layer 32 described above, in a case where intermediate layer 32 is constituted by Cu oriented in the (111) direction instead of Co oriented in the (110) direction, in thin film magnet 100a after the heat treatment, magnetic layers 31 and 33 are oriented such that the (0001) plane of SmxCoy as a hexagonal crystal or a rhombohedral crystal is parallel to surface 810 of substrate 10. Thus, magnetic layers 31 and 33 have magnetocrystalline anisotropy in normal direction D10b.
The crystal structure and magnetic properties of thin film magnet 100a manufactured by the method described above were evaluated in the following manner.
First, the crystal structure of thin film magnet 100a was evaluated.
The crystal structure of thin film magnet 100a in the case of using Co oriented in the (110) direction for intermediate layer 32 will be first described below.
As shown in
Thin film magnet 100a before the heat treatment does not exhibit diffraction indicating crystallization, as shown in
In
Thus, before the heat treatment, neither magnetic layer 31 nor magnetic layer 33 is crystallized, and the crystal structure of intermediate layer 32 is a cubic crystal, and the (110) plane of Co constituting intermediate layer 32 is oriented in parallel with surface 810 of substrate 10. It is also demonstrated that crystallization of magnetic layers 31 and 33 starts from intermediate layer 32 before the heat treatment. It is also demonstrated that, in the crystallization, metal particles 32p of Co included in intermediate layer 32 are diffused into magnetic layers 31 and 33 to form a crystal of SmCo5 or Sm2Co17. It is also confirmed that the (11-20) plane of SmxCoy as a hexagonal crystal or a rhombohedral crystal that is the (110) plane of a crystal of SmCo5 or Sm2Co17 is oriented in parallel with surface 810 of substrate 10. It is observed that oxidation-inhibiting layers 20a and 20b are in an amorphous state.
A comparative example of a thin film magnet was prepared. The comparative example of the thin film magnet had the same configuration as thin film magnet 100a according to Embodiment 4 except for no intermediate layer.
As shown in
As shown in
However, Co diffusion depends on the Ta volume in the oxidation-inhibiting layer and can be limited by reducing the thicknesses of oxidation-inhibiting layers 20a and 20b.
Diffusion of Co of magnetic particles from magnetic layers 31 and 33 to oxidation-inhibiting layers 20a and 20b causes Co of magnetic particles included in oxidation-inhibiting layer 20a and Ta included in magnetic layer 31 to form an alloy near the boundary between oxidation-inhibiting layer 20a and magnetic layer 31. Similarly, Co of magnetic particles included in oxidation-inhibiting layer 20b and Ta included in oxidation-inhibiting layer 20b form an alloy near the boundary between magnetic layer 33 and oxidation-inhibiting layer 20b. It is confirmed that these alloys are also in an amorphous state.
Oxidation-inhibiting layer 20a can suppress oxygen diffusion from SiO2 as a constituent material of substrate 10 into magnetic layer 31. Oxidation-inhibiting layer 20b can suppress entering of oxygen into magnetic layer 33 from the outside. In this embodiment, a layer containing Ta, that is, each of oxidation-inhibiting layers 20a and 20b, has a thickness of about 10 nm in stacking direction D1, but may have a smaller thickness as long as the functions described above are obtained.
In
On the other hand, at point F, the concentration of Co is about 90% while the concentration of Sm is about 10%. It is confirmed that this configuration is a crystal structure similar to Sm2Co17. It is also confirmed that films having different thicknesses in intermediate layer 32 have other crystal structures, such as SmCo5. In the forming of thin film magnet 100a, in that case where Co as a main component of intermediate layer 32 has a large thickness, intermediate layer 32 includes a crystal of a cubic crystal, Co before the heat treatment, in addition to a crystal having a crystal structure. Point F is a location corresponding to intermediate layer 32, and is a phase including Co only or the same constituent element as magnetic layers 31 and 33 and has a composition and crystal structure different from that of Co only or magnetic layers 31 and 33. This phase is a phase having a higher residual flux density and a lower coercive force than magnetic layers 31 and 33 in terms of magnetic properties.
The reason why the Co percentage is not 100%, Sm is detected, and the Co concentration is about 90% accordingly at point F corresponding to intermediate layer 32 is because Sm at the boundary between intermediate layer 32 and each of magnetic layers 31 and 33 is diffused in the heat treatment process.
Next, magnetic properties of thin film magnet 100a were evaluated. The crystal structure of thin film magnet 100a in the case of using Co oriented in the (110) direction for intermediate layer 32 will be described below.
An area surrounded by B-H curve 64 of thin film magnet 100a according to Embodiment 4 is larger than an area surrounded by B-H curve 65 of the comparative example of the thin film magnet. Thus, thin film magnet 100a has a larger BH product indicating energy of a magnet than in the comparative example of the thin film magnet. This also shows that a maximum energy product, one of important properties of a magnet, of the thin film magnet according to Embodiment 4 is large.
The crystal of SmCo5 constituting magnetic body 30 is a hexagonal crystal, the crystal of Sm2Co17 is a rhombohedral crystal, and magnetic body 30 of thin film magnet 100a according to this embodiment is oriented in the (11-20) direction of SmxCoy as a hexagonal crystal or a rhombohedral crystal. Thus, the c axis of the crystal of magnetic body 30 is parallel to in-plane direction D10a. Since magnetocrystalline anisotropy of SmCo5 is in the c axis direction, magnetic body 30 has magnetocrystalline anisotropy in in-plane direction D10a.
As shown in
In the case of using Cu oriented in the (111) direction for intermediate layer 32 instead of Co oriented in the (110) direction, in thin film magnet 100a after the heat treatment, magnetic layers 31 and 33 have magnetocrystalline anisotropy in normal direction D10b and generate strong magnetic fields in normal direction D10b.
As described above, in thin film magnet 100a according to Embodiment 4, SmxCoy having a high energy product is used for magnetic layers 31 and 33, Co or Cu is used as intermediate layer 32. Thus, thin film magnet 100a has magnetocrystalline anisotropy in predetermined directions, such as in-plane direction D10a and normal direction D10b, a sufficiently large coercive force, and a high residual flux density.
The c axes of crystalline particles of magnetic body 30 are generally oriented in in-plane direction D10a. However, magnetic body 30 according to Embodiment 4 has a polycrystalline structure and includes crystalline dispersion, and thus, it is not intended that the c axes of all the crystalline particles are completely oriented in the same direction. For example, in the case of using Co as intermediate layer 42, magnetic body 30 has magnetic anisotropy in in-plane direction D10a. This means that the c axes of crystalline particles in magnetic body 30 are generally oriented in in-plane direction D10a and does not mean that the c axes of all the crystalline particles are completely oriented in in-plane direction D10a. In magnetic body 30 in accordance with Embodiment 4, the crystal direction is oriented in the c axis direction as a whole. As long as the number of crystalline particles having c axes at angles ranging from 0° to 45° with respect to in-plane direction D10a is larger than the number of crystalline particles having c axes at angles ranging from 45° to 90° with respect to in-plane direction D10a, similar advantages can be obtained although the degree of the advantages are different.
In accordance with Embodiment 4, magnetic layers 31 and 33 are made of SmxCoy, but are not limited to SmxCoy. For example, part of Co may be replaced by Fe and Cu to enhance magnetization as a material. In order to increase the effect of replacement between Co and other elements, Zr or other elements may be mixed into magnetic layers 31 and 33 as an additive. In magnetic layers 31 and 33, Co of SmxCoy may be replaced by Fe so that Sm2Fe14N3 containing N, which is an interstitial material, is obtained. In this case, magnetic layers 31 and 33 may be formed in an atmosphere subjected to nitrogen replacement in crystallization to cause nitrogen to enter. Specifically, an amorphous SmxFeyNz layer may be formed above substrate 10 by performing low-temperature sputtering of a SmaFebNc target in a mixed atmosphere of Ar gas and N2 gas, or an amorphous SmxFeyNz layer may be formed above substrate 10 by performing low-temperature sputtering on a SmFe target in a mixed atmosphere of Ar gas and N2 gas. After that, the heat treatment is performed in high-purity nitrogen in which replacement is performed after the back pressure of the SmFeN layer formed above substrate 10 is evacuated to a vacuum atmosphere or an extremely high vacuum. This configuration crystallizes Sm2Fe14N3.
Instead of Co, intermediate layer 32 may use Fe that is a cubic crystal having a (110) plane oriented in parallel with surface 810 of substrate 10. Similarly, instead of Co, CoFe that is a cubic crystal having a (110) plane oriented in parallel with surface 810 of substrate 10 may be used. As intermediate layer 32, Cu may be replaced by Ni having a (111) plane in which crystalline is oriented. As intermediate layer 32, Cu may be replaced by metal particles 32p of a hexagonal crystal having a (0001) plane in which crystalline is oriented. As metal particles 32p of this hexagonal crystal, Ti, Co, Zr, Mg, or Hf may be used. In particular, Ti is preferable because of a small amount of lattice mismatch. Co as a hexagonal crystal can be obtained by controlling conditions of sputtering.
Oxidation-inhibiting layer 20a may include Nb, W, or Mo, instead of Ta. Oxidation-inhibiting layer 20a is required to be non-magnetic and have a high melting point. In particular, oxidation-inhibiting layer 20a preferably has a melting point higher than or equal to three times as large as a heat treatment temperature at which SmCo5 films of magnetic layers 31 and 33 are crystallized. This configuration effectively suppresses recrystallization of oxidation-inhibiting layer 20a in the crystallizing of magnetic layers 31 and 33. Oxidation-inhibiting layer 20a includes at least one of Ta, Nb, W, and Mo.
Oxidation-inhibiting layer 20b is similar to oxidation-inhibiting layer 20a.
Oxidation-inhibiting layers 20a and 20b do not necessarily be made of the same material, but are made of the same material in accordance with this embodiment from the viewpoint of reduction of materials to be used.
Intermediate layer 32 does not necessarily be continuous in in-plane direction D10a of substrate 10, and may partially has island shapes or interrupted. In this case, no problems arise in terms of function. That is, in accordance with this embodiment, the “intermediate layer” includes any layer disposed between magnetic layers including not only a case where the intermediate layer is continuous in in-plane direction D10a of substrate 10 but also a case where the intermediate layer has partially an island shape or interrupted. That is, in the magnetic layer, a region where a distribution concentration of metal particles 32p is higher than its surrounding portions will be hereinafter referred to as an “intermediate layer.”
The presence of intermediate layer 32 is detected by an observation with a transmission electron microscope. In addition to the observation with a transmission electron microscope, a method of measuring the concentration of metal particles 32p constituting intermediate layer 32 and determining, as intermediate layer 32, a region where the distribution concentration of metal particles 32p is locally higher than its surrounding portions, may be employed.
It was confirmed that similar advantages can be obtained in the case where the thickness of intermediate layer 32 in stacking direction D1 is changes within the range from 1 nm to 30 nm. Observation with a scanning-type transmission electron microscope confirmed a structure in which intermediate layer 32 spreads into magnetic layers 31 and 33 to partially have island shapes. Thus, it can be concluded that the same advantages can be obtained when the thicknesses changes as described above.
Thin film magnet 200a according to Embodiment 5 is different from thin film magnet 100a according to Embodiment 4 in the structure of magnetic layers. Thin film magnet 200a includes magnetic body 230 provided on upper surface 820a of oxidation-inhibiting layer 20a, instead of magnetic body 30 of thin film magnet 100a illustrated in
As illustrated in
That is, in magnetic body 230 according to Embodiment 5, magnetic layers 231 and 233 correspond to magnetic layers 31 and 33 of magnetic body 30 in accordance with Embodiment 4, respectively. Intermediate layer 232 in accordance with Embodiment 5 corresponds to intermediate layer 32 in accordance with Embodiment 4. In magnetic body 230 according to Embodiment 5, intermediate layer 234 and magnetic layer 235 are stacked on magnetic layer 33 of thin film magnet 100a according to Embodiment 4. Magnetic layer 235 has the same composition as magnetic layers 31 and 33, and can be obtained by a manufacturing process similar to that of magnetic layers 31 and 33. Intermediate layer 234 can be obtained by a manufacturing process similar to that of intermediate layer 32.
Thin film magnet 200a according to the present embodiment also has the same advantages as those of thin film magnet 100a according to Embodiment 4. In addition, since plural intermediate layers 232 and 234 and plural magnetic layers 231, 233, and 235 are stacked, thin film magnet 200a reduces continuous growth of particles, thereby improving a coercive force.
Although the foregoing description is directed to thin film magnets according to exemplary embodiments of the present disclosure, the present disclosure is not limited to the embodiments.
For example, in the exemplary embodiment described above, SmxCoy is used as a material constituting magnetic layers 31, 33, 231, 233, and 235, but the materials constituting magnetic layers 31 and 33, 231, 233, and 235 are not limited to these examples, and a material in which part of Co is replaced by Fe and Cu or a material in which Zr or other elements are mixed as an additive. The material may be, e.g. Sm2Fe14N3.
Oxidation-inhibiting layers 20a and 20b are not limited to the material containing Ta as described above, and may include Nb, W, or Mo, instead of Ta. The same material may be used for all the oxidation-inhibiting layers 20a and 20b, or different materials may be used for the oxidation-inhibiting layers.
Oxidation-inhibiting layers 20a and 20b, magnetic layers 31, 33, 231, 233, and 235, and intermediate layers 32, 232, and 234 may be formed by sputtering as described in the above exemplary embodiment or may be formed by other methods. The heat treatment temperature is not limited to the temperatures described above, and may be changed appropriately depending on materials.
The present disclosure is not limited to the exemplary embodiments. Embodiments in which variations conceivable to those skilled in the art are made on the exemplary embodiments and embodiments using combinations of components of different exemplary embodiments may be included within the range of one or more aspect, as long as these embodiments are within the gist of the present disclosure.
As described above, thin film magnet 100a (200a) includes substrate 10, oxidation-inhibiting layer 20a in an amorphous state provided on upper surface 810 of the substrate, magnetic material layer 31 (231) provided on oxidation-inhibiting layer 20a, intermediate layer 32 (232) provided on magnetic layer 31 (231), magnetic layer 33 (233) provided on intermediate layer 32 (232), and oxidation-inhibiting layer 20b in an amorphous state provided above magnetic layer 33 (233). Intermediate layer 32 includes metal particles 32p. Metal particles 32p are diffused in magnetic layers 31 and 33 (231 and 233). The concentration of metal particles 32p at a part of magnetic layers 31 (231) decreases as the distance from intermediate layer 32 (232) to the part of magnetic layers 31 (231) increases. The concentration of metal particles 32p at a part of magnetic layers 33 (233) decreases as the distance from intermediate layer 32 (232) to the part of magnetic layers 33 (233) increases.
This configuration provides thin film magnet 100a (200a) with magnetic anisotropy in a predetermined direction, for example, in-plane direction D10a or normal direction D10b, a high energy product, a sufficiently large coercive force, and a high residual flux density.
Magnetic layers 31 and 33 (231 and 233) may have magnetocrystalline anisotropy in in-plane direction D10a parallel to upper surface 810 of substrate 10.
With this configuration, magnetic layers 31 and 33 (231 and 233) are formed such that magnetic layers 31 and 33 (231 and 233) are oriented in-plane direction D10a. Thin film magnet 100a having magnetic anisotropy in in-plane direction D10a can thus be obtained.
Intermediate layer 32 (232) may be constituted by a crystal having a cubic crystal structure oriented in the (110) direction or by a crystal having a hexagonal crystal oriented in the (11-20) direction.
This configuration allows orientations of magnetic layers 31 and 33 (231 and 233) to be easily controlled in in-plane direction D10a in accordance with orientation of intermediate layer 32 (232).
Intermediate layer 32 (232) may contain at least one of cobalt (Co) and iron (Fe).
With this configuration, Co for intermediate layers 32 (232) allows orientations of magnetic layers 31 and 33 (231 and 233) to be easily controlled in in-plane direction D10a.
Magnetic layers 31 and 33 (231 and 233) may have magnetocrystalline anisotropy in normal direction D10b perpendicular to upper surface 810 of substrate 10.
With this configuration, magnetic layers 31 and 33 (231 and 233) are formed such that magnetic layers 31 and 33 (231 and 233) are oriented in normal direction D10b. Thin film magnet 100a (200a) having magnetic anisotropy in normal direction D10b can thus be obtained.
Intermediate layer 32 (232) may be constituted by a crystal having a cubic crystal structure oriented in the (111) direction.
This configuration allows orientations of magnetic layers 31 and 33 (231 and 233) to be easily controlled in normal direction D10b in accordance with orientation of intermediate layer 32 (232).
Intermediate layer 32 (232) may contain copper (Cu).
With this configuration, Cu for intermediate layers 32 (232) allows orientations of magnetic layers 31 and 33 (231 and 233) to be easily controlled in normal direction D10b.
Intermediate layer 32 (232) may be constituted by a crystal having a hexagonal crystal structure oriented in the (0001) direction.
This configuration allows orientations of magnetic layers 31 and 33 (231 and 233) to be easily controlled in normal direction D10b in accordance with orientation of intermediate layer 32 (232).
Intermediate layer 32 (232) may contain titanium (Ti) or zirconium (Zr).
With this configuration, Ti or Zr for intermediate layers 32 (232) allows orientations of magnetic layers 31 and 33 (231 and 233) to be easily controlled in normal direction D10b.
Intermediate layer 32 (232) may have lower crystallization temperature than magnetic layers 31 and 33 (231 and 233).
With this configuration, even when intermediate layer 32 (232) is crystallized, magnetic layer 31 (231) can be maintained in an amorphous state.
Magnetic layers 31 and 33 (231 and 233) may contain samarium (Sm).
With this configuration, a material, such as SmxCoy, containing Co and at least one of Sm, Pr, Nd, Y, La, and Gd for magnetic layers 31 and 33 (231 and 233) provides thin film magnet 100a (200a) with a high energy product.
Each of oxidation-inhibiting layers 20a and 20b may contain at least one of tantalum (Ta), niobium (Nb), tungsten (W), and molybdenum (Mo).
This configuration provides oxidation-inhibiting layers 20a and 20b with high oxidation suppressing function.
Thin film magnet 200a may further include magnetic layer 234 provided on magnetic layer 233 and magnetic layer 235 provided on intermediate layer 234. Intermediate layer 234 includes metal particles 234p. Metal particles 234p are diffused in magnetic layers 233 and 235. The concentration of metal particles 234p in a part of magnetic layer 233 decreases as the distance from intermediate layer 234 to the part of magnetic layer 233 increases. The concentration of metal particles 234p in a part of magnetic layer 235 decreases as the distance from intermediate layer 234 to the part of magnetic layer 235 increases.
Magnetic layer 235 may have magnetocrystalline anisotropy in in-plane direction D10a parallel to upper surface 810 of substrate 10.
Intermediate layer 234 may be constituted by a crystal having a cubic crystal structure oriented in the (110) direction or by a crystal having a hexagonal crystal oriented in the (11-20) direction.
Intermediate layer 234 may contain at least one of cobalt (Co) and iron (Fe).
Magnetic layer 235 may have magnetocrystalline anisotropy in normal direction D10b perpendicular to upper surface 810 of substrate 10.
Intermediate layer 234 may be constituted by a crystal having a cubic crystal structure oriented in the (111) direction.
Intermediate layer 234 may contain copper (Cu).
Intermediate layer 234 may be constituted by a crystal having a hexagonal crystal structure oriented in the (0001) direction.
Intermediate layer 234 may contain titanium (Ti) or ruthenium (Zr).
Each of intermediate layers 232 and 234 may have a crystallization temperature lower than those of magnetic layers 231, 233, and 235.
Each of magnetic layers 231, 233, and 235 may be made of a material containing Co and at least one of Sm, Pr, Nd, Y, La, and Gd.
Thin film magnet 100a (200a) can be manufactured by the following method. Oxidation-inhibiting layer 20a in an amorphous state is formed on upper surface 810 of substrate 10. Magnetic layer 31 (231) is formed on oxidation-inhibiting layer 20a. Intermediate layer 32 including metal particles 32p is formed on magnetic layer 31 (231). Intermediate layer 33 (233) is formed on magnetic layer 32. Oxidation-inhibiting layer 20b in an amorphous state is formed above magnetic layer 33 (233). A heat treatment is performed on oxidation-inhibiting layers 20a and 20b, magnetic layers 31 and 33 (231 and 233), and intermediate layer 32.
This configuration provides thin film magnet 100a (200a) having magnetic anisotropy in a predetermined direction, for example, in-plane direction D10a or normal direction D10b, a high energy product, a sufficiently large coercive force, and a high residual flux density.
In the process for forming magnetic layers 31 and 33 (231 and 233), magnetic layers 31 and 33 (231 and 233) may be formed in an amorphous state. In the process of forming intermediate layer 32 (232), intermediate layer 32 (232) may be formed by crystallization. In the heat treatment, magnetic layers 31 and 33 (231 and 233) may be crystallized.
This configuration allows orientations of magnetic layers 31 and 33 (231 and 233) to be easily controlled in accordance with orientation of intermediate layer 32 (232).
In the process of forming magnetic layers 31 and 33 (231 and 233), magnetic layers 31 and 33 (231 and 233) may be made of a material containing Co and at least one of Sm, Pr, Nd, Y, La, and Gd.
With this configuration, a material, such as SmxCoy, containing Sm for magnetic layers 31 and 33 (231 and 233) provides thin film magnet 100a (200a) with a high energy product to be obtained.
In the process of forming magnetic layers 31 and 33 (231 and 233), magnetic layers 31 and 33 (231 and 233) may be formed in an amorphous state with the surface temperature of substrate 10 equal to or lower than 400° C. In the process for forming intermediate layer 32 (232), magnetic layer 32 (232) may be formed at the surface temperature of substrate 10 equal to or lower than 400° C. The heat treatment may be performed on oxidation-inhibiting layers 20a and 20b, magnetic layers 31 and 33 (231 and 233), and intermediate layers 32 (232) at the surface temperature of substrate 10 equal to or higher than 500° C.
With this configuration, in the forming of intermediate layer 32 (232), intermediate layer 32 (232) can be crystallized while magnetic layer 31 (231) can be in an amorphous state. This configuration allows orientations of magnetic layers 31 and 33 (231 and 233) to be easily controlled in accordance with orientation of intermediate layer 32 (232).
In the process for forming oxidation-inhibiting layers 20a and 20b, oxidation-inhibiting layers 20a and 20b may be made of material containing at least one of Ta, Nb, W, and Mo.
This configuration provides oxidation-inhibiting layers 20a and 20b with high oxidation suppressing function.
In the foregoing exemplary embodiments, terms, such as “upper surface,” “above,” and “below,” indicating directions indicate relative directions determined based on relative positional relationships among components of a thin film magnet, and do not indicate absolute directions, such as a vertical direction.
A thin film magnet according to the present invention is useful as, for example, a permanent magnet required to have a high energy product, such as a sensor, an actuator, or a motor.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2015-073127 | Mar 2015 | JP | national |
| 2015-073247 | Mar 2015 | JP | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/JP2016/001420 | 3/14/2016 | WO | 00 |
