WO2023013704A1 - 熱電変換素子 - Google Patents
熱電変換素子 Download PDFInfo
- Publication number
- WO2023013704A1 WO2023013704A1 PCT/JP2022/029863 JP2022029863W WO2023013704A1 WO 2023013704 A1 WO2023013704 A1 WO 2023013704A1 JP 2022029863 W JP2022029863 W JP 2022029863W WO 2023013704 A1 WO2023013704 A1 WO 2023013704A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- conversion element
- thermoelectric conversion
- less
- magnetic body
- magnetic
- Prior art date
Links
- 238000006243 chemical reaction Methods 0.000 title claims abstract description 145
- 230000005291 magnetic effect Effects 0.000 claims abstract description 111
- 239000000463 material Substances 0.000 claims abstract description 56
- 239000000696 magnetic material Substances 0.000 claims description 58
- 239000000758 substrate Substances 0.000 claims description 24
- 230000000694 effects Effects 0.000 claims description 11
- 230000005303 antiferromagnetism Effects 0.000 claims description 5
- 230000005307 ferromagnetism Effects 0.000 claims description 5
- 229920000620 organic polymer Polymers 0.000 claims description 4
- 230000005294 ferromagnetic effect Effects 0.000 abstract description 2
- 230000005290 antiferromagnetic effect Effects 0.000 abstract 1
- 239000010409 thin film Substances 0.000 description 22
- 238000000034 method Methods 0.000 description 18
- 239000000126 substance Substances 0.000 description 18
- 230000000052 comparative effect Effects 0.000 description 16
- 239000002243 precursor Substances 0.000 description 16
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 14
- 239000007789 gas Substances 0.000 description 14
- 238000004544 sputter deposition Methods 0.000 description 12
- 230000005422 Nernst effect Effects 0.000 description 11
- 230000002547 anomalous effect Effects 0.000 description 11
- 238000005452 bending Methods 0.000 description 11
- 239000012790 adhesive layer Substances 0.000 description 10
- 239000010949 copper Substances 0.000 description 9
- 238000001755 magnetron sputter deposition Methods 0.000 description 9
- 229920002799 BoPET Polymers 0.000 description 8
- 239000013078 crystal Substances 0.000 description 8
- 239000010408 film Substances 0.000 description 8
- 238000001039 wet etching Methods 0.000 description 8
- 229910052786 argon Inorganic materials 0.000 description 7
- 230000001747 exhibiting effect Effects 0.000 description 7
- 230000004907 flux Effects 0.000 description 7
- 238000004519 manufacturing process Methods 0.000 description 6
- 239000004642 Polyimide Substances 0.000 description 5
- 230000007547 defect Effects 0.000 description 5
- 238000011156 evaluation Methods 0.000 description 5
- 238000005259 measurement Methods 0.000 description 5
- 229920000139 polyethylene terephthalate Polymers 0.000 description 5
- 239000005020 polyethylene terephthalate Substances 0.000 description 5
- 229920001721 polyimide Polymers 0.000 description 5
- 238000002441 X-ray diffraction Methods 0.000 description 4
- 239000000853 adhesive Substances 0.000 description 4
- 230000001070 adhesive effect Effects 0.000 description 4
- 229910052782 aluminium Inorganic materials 0.000 description 4
- 229910052733 gallium Inorganic materials 0.000 description 4
- 229920002120 photoresistant polymer Polymers 0.000 description 4
- 239000013077 target material Substances 0.000 description 4
- 238000005229 chemical vapour deposition Methods 0.000 description 3
- 239000000203 mixture Substances 0.000 description 3
- 239000011368 organic material Substances 0.000 description 3
- 238000010248 power generation Methods 0.000 description 3
- 238000004549 pulsed laser deposition Methods 0.000 description 3
- 230000007704 transition Effects 0.000 description 3
- 229920000089 Cyclic olefin copolymer Polymers 0.000 description 2
- 230000005678 Seebeck effect Effects 0.000 description 2
- 238000001816 cooling Methods 0.000 description 2
- 238000007733 ion plating Methods 0.000 description 2
- 229910052751 metal Inorganic materials 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 238000007747 plating Methods 0.000 description 2
- -1 polyethylene terephthalate Polymers 0.000 description 2
- 229920001296 polysiloxane Polymers 0.000 description 2
- 229910052710 silicon Inorganic materials 0.000 description 2
- 239000004925 Acrylic resin Substances 0.000 description 1
- 229920000178 Acrylic resin Polymers 0.000 description 1
- 229910000838 Al alloy Inorganic materials 0.000 description 1
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 229910000881 Cu alloy Inorganic materials 0.000 description 1
- JOYRKODLDBILNP-UHFFFAOYSA-N Ethyl urethane Chemical compound CCOC(N)=O JOYRKODLDBILNP-UHFFFAOYSA-N 0.000 description 1
- 239000003522 acrylic cement Substances 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 229910052804 chromium Inorganic materials 0.000 description 1
- 230000008602 contraction Effects 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 239000003302 ferromagnetic material Substances 0.000 description 1
- 229910052732 germanium Inorganic materials 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 239000010931 gold Substances 0.000 description 1
- 239000004519 grease Substances 0.000 description 1
- 229910052735 hafnium Inorganic materials 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 230000001771 impaired effect Effects 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 230000005415 magnetization Effects 0.000 description 1
- 229910052748 manganese Inorganic materials 0.000 description 1
- 229910052750 molybdenum Inorganic materials 0.000 description 1
- 229910052758 niobium Inorganic materials 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000005408 paramagnetism Effects 0.000 description 1
- 229920003229 poly(methyl methacrylate) Polymers 0.000 description 1
- 229920000515 polycarbonate Polymers 0.000 description 1
- 239000004417 polycarbonate Substances 0.000 description 1
- 229920001225 polyester resin Polymers 0.000 description 1
- 239000004645 polyester resin Substances 0.000 description 1
- 239000011112 polyethylene naphthalate Substances 0.000 description 1
- 239000004926 polymethyl methacrylate Substances 0.000 description 1
- 238000003825 pressing Methods 0.000 description 1
- 239000002344 surface layer Substances 0.000 description 1
- 229910052715 tantalum Inorganic materials 0.000 description 1
- 229910052718 tin Inorganic materials 0.000 description 1
- 229910052719 titanium Inorganic materials 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
- 229910052720 vanadium Inorganic materials 0.000 description 1
- 229910052726 zirconium Inorganic materials 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02N—ELECTRIC MACHINES NOT OTHERWISE PROVIDED FOR
- H02N11/00—Generators or motors not provided for elsewhere; Alleged perpetua mobilia obtained by electric or magnetic means
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02N—ELECTRIC MACHINES NOT OTHERWISE PROVIDED FOR
- H02N11/00—Generators or motors not provided for elsewhere; Alleged perpetua mobilia obtained by electric or magnetic means
- H02N11/002—Generators
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N15/00—Thermoelectric devices without a junction of dissimilar materials; Thermomagnetic devices, e.g. using the Nernst-Ettingshausen effect
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N15/00—Thermoelectric devices without a junction of dissimilar materials; Thermomagnetic devices, e.g. using the Nernst-Ettingshausen effect
- H10N15/20—Thermomagnetic devices using thermal change of the magnetic permeability, e.g. working above and below the Curie point
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N19/00—Integrated devices, or assemblies of multiple devices, comprising at least one thermoelectric or thermomagnetic element covered by groups H10N10/00 - H10N15/00
Definitions
- the present invention relates to thermoelectric conversion elements.
- thermoelectric conversion elements that utilize the magneto-thermoelectric effect are known.
- Patent Document 1 describes a thermoelectric power generation device that utilizes the anomalous Nernst effect.
- the anomalous Nernst effect is a phenomenon in which a voltage is generated in a direction orthogonal to both the magnetization direction and the temperature gradient when a heat flow is applied to a magnetic material and a temperature difference is generated.
- a thermoelectric generator device includes a substrate, a generator, and a connector. At least the surface layer of the substrate is made of MgO.
- the power generator consists of a plurality of thin wires arranged parallel to each other along the surface of the substrate. Each wire is made of ferromagnetic material and is magnetized in the same direction.
- the connecting body consists of a plurality of thin wires arranged parallel to and between the thin wires of the power generating body.
- Each thin wire of the connector electrically connects one end of each thin wire of the power generating body and the other end of the adjacent thin wire on one side of each thin wire.
- thermoelectric power generation device thin wires of a ferromagnetic power generator are connected in series by a connector. This is thought to generate a high electromotive force in the thermoelectric power generation device. On the other hand, if disconnection occurs due to cracks or the like at any part of the thin wires of the heating element and the connection body, it is considered that the entire function of the thermoelectric power generating device is impaired.
- thermoelectric conversion element that uses the magneto-thermoelectric effect can be used in various environments, it is believed that the value of the thermoelectric conversion element can be further increased.
- Patent Literature 1 no study is made on the durability of the thermoelectric power generation device in a given environment.
- the present invention provides a thermoelectric conversion element that utilizes the magneto-thermoelectric effect, which is advantageous in exhibiting high durability in high-temperature and high-humidity environments.
- the present invention a substrate; and a magnetic body having ferromagnetism or antiferromagnetism disposed on the base material,
- the magnetic body has an internal stress of 900 MPa or less, A thermoelectric conversion element is provided.
- thermoelectric conversion element described above is advantageous in that it exhibits high durability in a high-temperature, high-humidity environment while utilizing the magneto-thermoelectric effect.
- FIG. 1 is a perspective view showing one example of a thermoelectric conversion element according to the present invention.
- FIG. 2 is a cross-sectional view of the thermoelectric conversion element taken along plane II shown in FIG.
- FIG. 3 is a diagram schematically showing a method of measuring internal stress in a magnetic material.
- the thermoelectric conversion element 1a includes a base material 10 and a magnetic body 21.
- the magnetic body 21 is arranged on the substrate 10 and has ferromagnetism or antiferromagnetism.
- the magnetic body 21 has an internal stress of 900 MPa or less.
- the internal stress is a tensile stress if the value of the internal stress is positive, and a compressive stress if the value of the internal stress is negative.
- thermoelectric conversion element 1a tends to exhibit high durability in a high-temperature and high-humidity environment.
- the thermoelectric conversion element 1a tends to exhibit high durability even in a state where bending stress is applied to the thermoelectric conversion element 1a.
- the internal stress of the magnetic body 21 can be measured, for example, according to the method described in Examples. 1 and 2, the X-axis, Y-axis, and Z-axis are orthogonal to each other, and the Z-axis direction is the thickness direction of the base material 10 .
- the high-temperature and high-humidity environment is not limited to a specific environment.
- a high temperature and high humidity environment is, for example, an environment having a temperature of 60° C. to 120° C. and a relative humidity of 60% or higher.
- An example of a hot and humid environment is an environment having a temperature of 85° C. and a relative humidity of 85%.
- the internal stress in the magnetic body 21 may be 800 MPa or less, 700 MPa or less, or 600 MPa or less.
- the internal stress in the magnetic body 21 is desirably 500 MPa or less.
- the thermoelectric conversion element 1a tends to more reliably exhibit high durability in a high-temperature and high-humidity environment.
- the thermoelectric conversion element 1a tends to more reliably exhibit high durability.
- the internal stress in the magnetic body 21 may be 400 MPa or less, 300 MPa or less, or 200 MPa or less.
- the internal stress in the magnetic body 21 is more desirably 100 MPa or less.
- the thermoelectric conversion element 1a tends to exhibit higher durability in a high-temperature and high-humidity environment.
- the thermoelectric conversion element 1a tends to exhibit higher durability even in a state where a bending stress is applied to the thermoelectric conversion element 1a.
- the internal stress in the magnetic body 21 may be 0 MPa or less, ⁇ 100 MPa or less, or ⁇ 200 MPa or less.
- the internal stress in the magnetic body 21 is more desirably -300 MPa or less. In this case, the thermoelectric conversion element 1a tends to exhibit higher durability even in a state where bending stress is applied to the thermoelectric conversion element 1a.
- the internal stress in the magnetic body 21 is -2000 MPa or more, for example.
- the internal stress in the magnetic body 21 may be ⁇ 1500 MPa or more, ⁇ 1000 MPa or more, or ⁇ 500 MPa or more.
- the magnetic body 21 has an internal stress of 900 MPa or less, the magnetic body 21 is not limited to a specific material.
- the magnetic body 21 generates an electromotive force in a direction orthogonal to the thickness direction of the substrate 10 when a temperature gradient ⁇ T is generated in the thickness direction (Z-axis direction) of the substrate 10, for example.
- a temperature gradient ⁇ T is generated in the thickness direction (Z-axis direction) of the substrate 10, for example.
- thermoelectric conversion element 1a For example, by increasing the dimension of the magnetic body 21 in a specific direction along the main surface of the substrate 10, the electric power generated by the temperature gradient ⁇ T in the thermoelectric conversion element 1a can be increased. Therefore, it is easy to reduce the thickness of the thermoelectric conversion element 1a.
- the magnetic body 21 generates an electromotive force by, for example, the magneto-thermoelectric effect.
- the magneto-thermoelectric effect is, for example, the anomalous Nernst effect or the spin Seebeck effect.
- the magnetic material 21 includes, for example, a material exhibiting the anomalous Nernst effect. Substances exhibiting the anomalous Nernst effect are not limited to specific substances. A material exhibiting the anomalous Nernst effect is, for example, a magnetic material having a saturation magnetic susceptibility of 5 ⁇ 10 ⁇ 3 T or more or a material having a band structure having a Weyl point near the Fermi energy.
- the magnetic body 21 contains at least one substance selected from the group consisting of the following (i), (ii), (iii), (iv), and (v) as a substance exhibiting the anomalous Nernst effect. .
- a stoichiometric substance having a composition represented by Fe 3 X (ii) an off-stoichiometric substance in which the composition ratio of Fe and X deviates from the substance (i) above (iii) the above ( A substance (iv) Fe 3 M1 1-x M2 x (iv) in which a part of the Fe site of the substance i) or part of the Fe site of the substance (ii) is replaced with a typical metal element other than X or a transition element (v) a substance having a composition represented by 0 ⁇ x ⁇ 1), wherein M1 and M2 are different representative elements; , a substance in which a part of the X site of the substance (i) above is replaced with a main group metal element other than X
- X is a typical element or a transition element.
- X is, for example, Al, Ga, Ge, Sn, Si, Ti, Zr, Hf, V, Nb, Ta, Cr, Mo, W, Sc, Ni, Mn, or Co.
- the combination of M1 and M2 is not limited to a specific combination as long as M1 and M2 are representative elements different from each other.
- the combination of M1 and M2 is Ga and Al, Si and Al, or Ga and B, for example.
- the magnetic material 21 may contain Co 2 MnGa or Mn 3 Sn as a substance exhibiting the anomalous Nernst effect.
- the magnetic body 21 is formed, for example, in a rectangular parallelepiped shape elongated in a specific direction (Y-axis direction) extending along the main surface of the base material 10 .
- the magnetic body 21 is magnetized, for example, in the negative direction of the X axis.
- the dimension of the magnetic body 21 in the Y-axis direction is larger than the dimension of the magnetic body 21 in the Z-axis and the X-axis, and the electromotive force generated by the magneto-thermoelectric effect tends to increase. Therefore, even if the magnetic body 21 does not have a large thickness, the electromotive force generated in the thermoelectric conversion element 1a tends to increase.
- the thermoelectric conversion element 1a includes, for example, conductive paths 25.
- Conductive path 25 includes magnetic material 21 and forms a meander pattern.
- the length of the conductive path 25 tends to increase, and the electromotive force generated in the thermoelectric conversion element 1a tends to increase.
- a heat flow can be generated in the thickness direction of the base material 10 by applying a voltage between the one end portion 25p and the other end portion 25q.
- the conductive path 25 includes a plurality of magnetic bodies 21.
- the plurality of magnetic bodies 21 are, for example, separated at predetermined intervals in the X-axis direction and arranged parallel to each other.
- the plurality of magnetic bodies 21 are arranged at regular intervals in the X-axis direction.
- Conductive path 25 further comprises, for example, a plurality of connectors 22 .
- the connection bodies 22 electrically connect the magnetic bodies 21 adjacent to each other in the X-axis direction.
- the connector 22 electrically connects, for example, one end of the magnetic body 21 in the Y-axis direction and the other end in the Y-axis direction of another magnetic body 21 adjacent to the magnetic body 21 .
- the plurality of magnetic bodies 21 are electrically connected in series, and the electromotive force generated in the thermoelectric conversion element 1a tends to increase.
- One end of the plurality of magnetic bodies 21 in the Y-axis direction is located at the end of the magnetic body 21 on the same side in the Y-axis direction, and the other end of the plurality of magnetic bodies 21 in the Y-axis direction is located on the same side of the magnetic body 21 . 21 in the Y-axis direction.
- connection body 22 is formed, for example, in the shape of a rectangular parallelepiped elongated in the Y-axis direction.
- the material forming the connecting body 22 is not limited to a specific material.
- the connector 22 may contain a substance that generates an electromotive force by a magneto-thermoelectric effect, and may have ferromagnetism or antiferromagnetism, for example. In this case, the connector 22 is magnetized, for example, in the positive direction of the X-axis.
- the connector 22 may contain a non-magnetic material.
- the material forming the connector 22 is, for example, a transition element having paramagnetism.
- the non-magnetic material contained in the connector 22 is, for example, gold, copper, copper alloy, aluminum, or aluminum alloy.
- the connector 22 may be a cured conductive paste.
- the base material 10 is not limited to a specific base material.
- the base material 10 has flexibility, for example. Thereby, the thermoelectric conversion elements 1a can be arranged along the curved surface.
- the base material 10 is, for example, a strip-shaped test piece made from the base material 10. When the test piece is wound around a cylindrical mandrel with a diameter of 10 cm so that both ends of the test piece in the length direction are oriented in the same direction, the The test piece has elasticity that allows it to be elastically deformed.
- the base material 10 may be a non-flexible material such as a glass base material.
- the substrate 10 When the substrate 10 has flexibility, the substrate 10 contains at least an organic polymer, for example. Thereby, it is easy to reduce the manufacturing cost of the thermoelectric conversion element 1a.
- organic polymers are polyethylene terephthalate (PET), polyethylene naphthalate (PEN), acrylic resin (PMMA), polycarbonate (PC), polyimide (PI) or cycloolefin polymer (COP).
- the coefficient of linear expansion of the base material 10 is not limited to a specific value.
- the base material 10 has, for example, a linear expansion coefficient of 1.0 ⁇ 10 ⁇ 5 /° C. or higher.
- the coefficient of linear expansion means an average value in a temperature range of 25°C to 150°C.
- the linear expansion coefficient of the base material 10 may be 1.5 ⁇ 10 -5 /°C or higher, may be 2.0 ⁇ 10 -5 /°C or higher, or may be 2.5 ⁇ 10 -5 /°C or higher. or more, may be 3.0 ⁇ 10 ⁇ 5 /° C. or more, may be 4.0 ⁇ 10 ⁇ 5 /° C. or more, or may be 5.0 ⁇ 10 ⁇ 5 /° C. or more. may be 6.0 ⁇ 10 -5 /°C or more, may be 7.0 ⁇ 10 -5 /°C or more, or may be 8.0 ⁇ 10 -5 /°C or more good too.
- the coefficient of linear expansion of the base material 10 is, for example, 15 ⁇ 10 ⁇ 5 /° C. or less. Thereby, a tensile stress is easily applied to the magnetic body 21, and the internal stress of the magnetic body 21 is easily adjusted within a desired range.
- the thickness of the base material 10 is not limited to a specific value.
- the thickness of the base material 10 is, for example, 200 ⁇ m or less.
- the thickness of the base material 10 may be 190 ⁇ m or less, 180 ⁇ m or less, 170 ⁇ m or less, or 160 ⁇ m or less.
- the thickness of the base material 10 may be 150 ⁇ m or less, 140 ⁇ m or less, 130 ⁇ m or less, 120 ⁇ m or less, or 110 ⁇ m or less.
- the thickness of the base material 10 may be 100 ⁇ m or less, 90 ⁇ m or less, 80 ⁇ m or less, 70 ⁇ m or less, or 60 ⁇ m or less.
- the thickness of the base material 10 is, for example, 10 ⁇ m or more. Thereby, the substrate 10 can be easily transported, and the substrate 10 has desired handleability.
- the thickness of the base material 10 may be 20 ⁇ m or more, or may be 30 ⁇ m or more.
- the thickness of the magnetic body 21 is not limited to a specific value.
- the magnetic body 21 has a thickness of 1000 nm or less, for example. This makes it possible to reduce the amount of material used for forming the magnetic body 21 in the thermoelectric conversion element 1a, thereby easily reducing the manufacturing cost of the thermoelectric conversion element 1a. In addition, disconnection of the conductive path 25 is less likely to occur in the thermoelectric conversion element 1a.
- the thickness of the magnetic body 21 may be 750 nm or less, 500 nm or less, 400 nm or less, 300 nm or less, or 200 nm or less.
- the thickness of the magnetic body 21 is, for example, 5 nm or more. This makes it easy for the thermoelectric conversion element 1a to exhibit high durability.
- the thickness of the magnetic body 21 may be 10 nm or more, 20 nm or more, 30 nm or more, or 50 nm or more.
- each magnetic body 21 has an internal stress of 900 MPa or less
- the width, which is the dimension in the X-axis direction, of each magnetic body 21 is not limited to a specific value.
- the width of each magnetic body 21 is, for example, 500 ⁇ m or less. This makes it possible to reduce the amount of material used for forming the magnetic body 21 in the thermoelectric conversion element 1a, thereby easily reducing the manufacturing cost of the thermoelectric conversion element 1a.
- the width of the magnetic material is small, cracks are likely to occur in the magnetic material in a high-temperature, high-humidity environment.
- the width of the magnetic material is small, defects and cracks are likely to occur in the magnetic material when a bending stress is applied to the thermoelectric conversion element including such a magnetic material.
- the magnetic body 21 has an internal stress of 900 MPa or less, even when the width is 500 ⁇ m or less, cracks are less likely to occur in the magnetic body in a high-temperature, high-humidity environment.
- bending stress is applied to the thermoelectric conversion element 1a, defects and cracks are less likely to occur in the magnetic body 21 .
- the thermoelectric conversion element 1a includes, for example, the conductive path 25, and the conductive path 25 forms a meander pattern including the magnetic material 21.
- the magnetic material 21 has a line width of 500 ⁇ m or less in the meander pattern.
- the magnetic body 21 has an internal stress of 900 MPa or less, cracks are less likely to occur in the magnetic body in a high-temperature, high-humidity environment.
- bending stress is applied to the thermoelectric conversion element 1a, defects and cracks are less likely to occur in the magnetic body 21 .
- the width of each magnetic body 21 may be 400 ⁇ m or less, 300 ⁇ m or less, 200 ⁇ m or less, 100 ⁇ m or less, or 50 ⁇ m or less.
- the width of each magnetic body 21 is, for example, 0.1 ⁇ m or more. As a result, disconnection of the conductive path 25 is less likely to occur in the thermoelectric conversion element 1a, and the thermoelectric conversion element 1a tends to exhibit high durability.
- the width of each magnetic body 21 may be 0.5 ⁇ m or more, 1 ⁇ m or more, 2 ⁇ m or more, 5 ⁇ m or more, or 10 ⁇ m or more, It may be 20 ⁇ m or more, or may be 30 ⁇ m or more.
- the thickness of the connecting body 22 is not limited to a specific value.
- the thickness of the connector 22 is, for example, 1000 nm or less. This makes it possible to reduce the amount of material used for forming the connection body 22, and it is easy to reduce the manufacturing cost of the thermoelectric conversion element 1a. In addition, disconnection of the conductive path 25 is less likely to occur in the thermoelectric conversion element 1a.
- the thickness of the connector 22 may be 750 nm or less, 500 nm or less, 400 nm or less, 300 nm or less, 200 nm or less, or 100 nm or less. There may be.
- the thickness of the connector 22 is, for example, 5 nm or more. This makes it easy for the thermoelectric conversion element 1a to exhibit high durability.
- the thickness of the connector 22 may be 10 nm or more, 20 nm or more, 30 nm or more, or 50 nm or more.
- the width which is the minimum dimension of each connecting body 22 in the X-axis direction, is not limited to a specific value.
- the width of each connector 22 is, for example, 500 ⁇ m or less.
- the width of each connector 22 may be 400 ⁇ m or less, 300 ⁇ m or less, 200 ⁇ m or less, 100 ⁇ m or less, or 50 ⁇ m or less.
- the width of each connector 22 is, for example, 0.1 ⁇ m or more. As a result, disconnection of the conductive path 25 is less likely to occur in the thermoelectric conversion element 1a, and the thermoelectric conversion element 1a tends to exhibit high durability.
- the width of each connector 22 may be 0.5 ⁇ m or more, 1 ⁇ m or more, 2 ⁇ m or more, 5 ⁇ m or more, or 10 ⁇ m or more. It may be 20 ⁇ m or more, or may be 30 ⁇ m or more.
- thermoelectric conversion element 1a An example of a method for manufacturing the thermoelectric conversion element 1a will be described.
- a thin film of a precursor of the magnetic material 21 is formed on one main surface of the base material 10 by a method such as sputtering, chemical vapor deposition (CVD), pulsed laser deposition (PLD), ion plating, and plating.
- CVD chemical vapor deposition
- PLD pulsed laser deposition
- a photoresist is then applied over the thin film, a photomask is placed over the thin film and exposed to light, followed by a wet etch. Thereby, a linear pattern of precursors of a plurality of magnetic bodies 21 arranged at predetermined intervals is formed.
- a thin film of a precursor of the connection bodies 22 is formed on one main surface of the base material 10 by sputtering, CVD, PLD, ion plating, plating, or the like.
- a photoresist is applied on the thin film of the precursor of the connection body 22, a photomask is placed on the thin film of the precursor of the connection body 22, exposure is performed, and then wet etching is performed.
- the connection body 22 is obtained, and the linear patterns of the precursor of the magnetic body 21 are electrically connected to each other.
- the magnetic body 21 is formed by magnetizing the precursor of the magnetic body 21 .
- the thermoelectric conversion element 1a is obtained.
- the connector 22 may be formed by magnetizing the precursor of the connector 22 .
- the internal stress in the magnetic body 21 can be adjusted within a desired range.
- the pressure of the atmosphere of the substrate 10 where sputtering is performed, the temperature of the substrate 10, the distance between the target and the substrate, and the magnetic flux density are By adjusting, the internal stress in the magnetic body 21 can be adjusted within a desired range.
- the pressure (process pressure) of the atmosphere of the substrate 10 where sputtering is performed is limited to a specific value as long as the internal stress of the magnetic substance 21 is 900 MPa or less. not.
- the process pressure is 1.0 Pa, for example.
- the process pressure is desirably 0.5 Pa or less, more desirably 0.3 Pa or less.
- the process pressure is, for example, 0.05 Pa or higher.
- the TS distance which is the distance between the target and the base material, is not limited to a specific value as long as the internal stress of the magnetic body 21 is 900 MPa or less.
- the TS distance is, for example, 120 mm or less. Thereby, even when the base material 10 contains an organic material, the internal stress of the magnetic body 21 is easily adjusted to 900 MPa or less.
- the TS distance is desirably 100 mm or less, may be 80 mm or less, or may be 60 mm or less.
- the TS distance is, for example, 40 mm or more.
- the magnetic field conditions are not limited to specific conditions as long as the internal stress of the magnetic body 21 is 900 MPa or less.
- the magnetic flux density in sputtering is 150 mT or less.
- the magnetic flux density may be 120 mT or less.
- the magnetic flux density is, for example, 30 mT or more.
- the magnetic flux density may be 50 mT or more, or 70 mT or more.
- the thermoelectric conversion element 1a may be provided with, for example, an adhesive layer.
- the substrate 10 is arranged between the magnetic body 21 and the adhesive layer in the thickness direction of the substrate 10 .
- the thermoelectric conversion element 1a can be attached to the article by pressing the adhesive layer against the article.
- the adhesive layer contains, for example, a rubber-based adhesive, an acrylic adhesive, a silicone-based adhesive, or a urethane-based adhesive.
- Thermoelectric conversion element 1a may be provided together with an adhesive layer and a separator.
- the separator covers the adhesive layer.
- a separator is typically a film that can maintain the adhesive strength of the adhesive layer when covering the adhesive layer and that can be easily peeled off from the adhesive layer.
- the separator is, for example, a film made of polyester resin such as PET. By peeling off the separator, the adhesive layer is exposed, and the thermoelectric conversion element 1a can be attached to an article.
- the angle ( ⁇ ) formed by the normal to the main surface of the magnetic sample Sa and the normal to the crystal plane of the crystal of the magnetic material Mb is 45°, 52°, 60°, 70°, and
- the above X-ray diffraction measurement was performed to calculate the crystal lattice strain ⁇ at each angle ( ⁇ ).
- the residual stress (internal stress) ⁇ in the in-plane direction of the magnetic material was determined from the slope of the straight line plotting the relationship between sin 2 ⁇ and the crystal lattice strain ⁇ according to the following equation (3).
- Table 1 shows the results.
- a positive value indicates tensile stress
- a negative value indicates compressive stress.
- ⁇ ⁇ (1+ ⁇ )/E ⁇ sin 2 ⁇ (2 ⁇ /E) ⁇
- E is the Young's modulus of the magnetic material (210 GPa)
- ⁇ is the Poisson's ratio of the magnetic material (0.3).
- detector 100 detects X-ray diffraction.
- thermoelectric conversion element according to each example and each comparative example was kept under conditions of a temperature of 85° C. and a relative humidity of 85% for 24 hours, and a durability test was performed.
- the electrical resistance value R 0 of the meander pattern in the thermoelectric conversion element before the durability test and the electrical resistance value R t of the meander pattern in the thermoelectric conversion element after the durability test were measured, and 100 ⁇ (R t ⁇ R 0 )/R 0 A value was obtained as a rate of change in resistance. Table 1 shows the results.
- thermoelectric conversion element according to each example and each comparative example was fixed between a pair of Cu plates having dimensions of 30 mm, 30 mm, and 5 mm using Shin-Etsu Chemical Co., Ltd.'s silicone grease KS609, and the thermoelectric properties were measured.
- a sample for evaluation was produced. The sample was placed on the cooling plate SCP-125 from AS ONE.
- a film heater manufactured by Shinwa Kiseki Co., Ltd. was fixed on the upper Cu plate with double-sided tape No. 5000NS manufactured by Nitto Denko. The heater had dimensions of 30 mm square and an electrical resistance of 20 ohms.
- thermoelectric conversion element was measured using a data logger and divided by the area of the thermoelectric conversion element to read the value of the electromotive force per unit area in the steady state. Table 1 shows the results.
- a thin film having a thickness of 96 nm was formed on a polyethylene terephthalate (PET) film having a thickness of 50 ⁇ m by DC magnetron sputtering using a target material containing Fe and Ga.
- DC magnetron sputtering the distance between the target material and the PET film was adjusted to 75 mm.
- DC magnetron sputtering a magnet having a magnetic flux density of 100 mT was used, and argon gas was supplied as a process gas at a pressure of 0.1 Pa. Also, the temperature of the PET film was adjusted to 130°C.
- the linear expansion coefficient of the PET film was 7.0 ⁇ 10 -5 /°C.
- a photoresist was applied on the thin film, a photomask was placed on the thin film, exposure was performed, and then wet etching was performed.
- 98 FeGa-containing linear patterns arranged at predetermined intervals were formed.
- the width of each FeGa-containing linear pattern was 100 ⁇ m
- the length of each FeGa linear pattern was 15 mm
- the total length of the FeGa linear patterns was 147 cm.
- a Cu thin film having a thickness of 100 nm was formed by DC magnetron sputtering using a target material containing Cu.
- thermoelectric conversion element according to Example 1 was obtained. This thermoelectric conversion element generated an electromotive force based on the anomalous Nernst effect.
- thermoelectric conversion element according to Example 2 was obtained in the same manner as in Example 1, except that argon gas was supplied as a process gas at a pressure of 0.2 Pa.
- the thickness of the magnetic material in the thermoelectric conversion element according to Example 2 was 96 nm.
- thermoelectric conversion element according to Example 3 was obtained in the same manner as in Example 1, except that argon gas was supplied as a process gas at a pressure of 0.9 Pa.
- the thickness of the magnetic material in the thermoelectric conversion element according to Example 3 was 89 nm.
- Example 4 Thermoelectric conversion according to Example 4 in the same manner as in Example 1 except that a polyimide (PI) film having a thickness of 50 ⁇ m was used instead of the PET film and the temperature of the PI film was adjusted to 25 ° C. in DC magnetron sputtering. I got the device.
- the thickness of the magnetic material in the thermoelectric conversion element according to Example 4 was 100 nm.
- thermoelectric conversion element according to Example 5 was produced in the same manner as in Example 1 except that the temperature of the PET film was adjusted to 100° C. and argon gas was supplied as the process gas at a pressure of 0.2 Pa. got The thickness of the magnetic material in the thermoelectric conversion element according to Example 5 was 96 nm.
- thermoelectric conversion element according to Example 6 was produced in the same manner as in Example 1 except that the temperature of the PET film was adjusted to 50° C. and argon gas was supplied as the process gas at a pressure of 0.2 Pa. got The thickness of the magnetic material in the thermoelectric conversion element according to Example 6 was 96 nm.
- thermoelectric conversion element according to Example 7 was obtained in the same manner as in Example 1, except that the temperature of the PET film was adjusted to 25° C. in the DC magnetron sputtering.
- the thickness of the magnetic material in the thermoelectric conversion element according to Example 7 was 96 nm.
- thermoelectric conversion element according to Example 8 was obtained in the same manner as in Example 1, except that the wet etching conditions were adjusted so that the width of each FeGa-containing linear pattern was 50 ⁇ m.
- the thickness of the magnetic material in the thermoelectric conversion element according to Example 8 was 96 nm.
- thermoelectric conversion element according to Example 9 was obtained in the same manner as in Example 1, except that the wet etching conditions were adjusted so that the width of each FeGa-containing linear pattern was 200 ⁇ m.
- the thickness of the magnetic material in the thermoelectric conversion element according to Example 9 was 96 nm.
- thermoelectric conversion element according to Example 10 was obtained in the same manner as in Example 1, except that the wet etching conditions were adjusted so that the width of each FeGa-containing linear pattern was 300 ⁇ m.
- the thickness of the magnetic material in the thermoelectric conversion element according to Example 10 was 96 nm.
- thermoelectric conversion element according to Example 11 was obtained in the same manner as in Example 1, except that the wet etching conditions were adjusted so that the width of each FeGa-containing linear pattern was 400 ⁇ m.
- the thickness of the magnetic material in the thermoelectric conversion element according to Example 11 was 96 nm.
- thermoelectric conversion element according to Comparative Example 1 was obtained in the same manner as in Example 1, except that argon gas was supplied as a process gas at a pressure of 1.6 Pa.
- the thickness of the magnetic material in the thermoelectric conversion element according to Comparative Example 1 was 85 nm.
- thermoelectric conversion element according to Comparative Example 2 was obtained in the same manner as above.
- the thickness of the magnetic material in the thermoelectric conversion element according to Comparative Example 2 was 85 nm. This thermoelectric conversion element did not exhibit an electromotive force based on the anomalous Nernst effect.
- the internal stress of the magnetic material of the thermoelectric conversion element according to each example was 900 MPa or less, and the internal stress of the magnetic material of the thermoelectric conversion element according to the comparative example exceeded 900 MPa.
- the resistance change rate in the endurance test of the thermoelectric conversion element according to each example is much lower than the resistance change rate in the endurance test of the thermoelectric conversion element according to the comparative example, and the internal stress of the magnetic material is adjusted to 900 MPa or less. This suggests that the thermoelectric conversion element can exhibit high durability in a high-temperature, high-humidity environment.
- the maximum value of the mandrel diameter at which disconnection occurs in the bending evaluation of the thermoelectric conversion element according to each example is the diameter of the mandrel at which disconnection occurs in the bending evaluation of the thermoelectric conversion element according to the comparative example. was smaller than the maximum value of It was suggested that by adjusting the internal stress of the magnetic material to 900 MPa or less, the thermoelectric conversion element can exhibit good durability when bent.
- thermoelectric force of the thermoelectric conversion element according to Example was larger than that of the thermoelectric conversion element according to Comparative Example 2.
- the internal stress of the magnetic material to 900 MPa or less and the line width of the magnetic material to be 500 ⁇ m or less, it is possible to generate an electromotive force based on the anomalous Nernst effect while exhibiting good durability when bending. It has been shown.
- a first aspect of the present invention is a substrate; and a magnetic body having ferromagnetism or antiferromagnetism disposed on the base material,
- the magnetic body has an internal stress of 900 MPa or less,
- a thermoelectric conversion element is provided.
- thermoelectric conversion element according to the first aspect,
- the substrate provides a thermoelectric conversion element having flexibility.
- thermoelectric conversion element according to the second aspect,
- the substrate provides a thermoelectric conversion element containing at least an organic polymer.
- a fourth aspect of the present invention is the thermoelectric conversion element according to any one of the first to third aspects,
- the substrate provides a thermoelectric conversion element having a coefficient of linear expansion of 1.0 ⁇ 10 ⁇ 5 /° C. or more.
- a fifth aspect of the present invention is the thermoelectric conversion element according to any one of the first to fourth aspects,
- the substrate provides a thermoelectric conversion element having a thickness of 200 ⁇ m or less.
- thermoelectric conversion element is the thermoelectric conversion element according to any one of the first to fifth aspects,
- the magnetic material provides a thermoelectric conversion element having a thickness of 1000 nm or less.
- a seventh aspect of the present invention is the thermoelectric conversion element according to any one of the first to sixth aspects,
- the magnetic material provides a thermoelectric conversion element having a width of 500 ⁇ m or less.
- thermoelectric conversion element is the thermoelectric conversion element according to any one of the first to seventh aspects,
- the magnetic material provides a thermoelectric conversion element that generates an electromotive force in a direction orthogonal to the thickness direction of the base material when a temperature gradient occurs in the thickness direction of the base material.
- thermoelectric conversion element is the thermoelectric conversion element according to any one of the first to eighth aspects,
- the magnetic material provides a thermoelectric conversion element that generates an electromotive force through a magneto-thermoelectric effect.
- thermoelectric conversion element according to any one of the first to ninth aspects, A thermoelectric conversion element is provided, which includes the magnetic material and includes a conductive path forming a meander pattern.
- thermoelectric conversion element is the thermoelectric conversion element according to the tenth aspect.
- the magnetic material provides a thermoelectric conversion element having a line width of 500 ⁇ m or less in the meander pattern.
Landscapes
- Hall/Mr Elements (AREA)
Abstract
Description
基材と、
前記基材上に配置され、強磁性又は反強磁性を有する磁性体と、を備え、
前記磁性体は、900MPa以下の内部応力を有する、
熱電変換素子を提供する。
(i)Fe3Xで表される組成を有するストイキオメトリックな物質
(ii)上記(i)の物質からFeとXとの組成比がずれたオフ・ストイキオメトリックな物質
(iii)上記(i)の物質のFeサイトの一部又は上記(ii)の物質のFeサイトの一部がX以外の典型金属元素又は遷移元素で置換された物質
(iv)Fe3M11-xM2x(0<x<1)で表される組成を有し、M1及びM2が互いに異なる典型元素である物質
(v)上記(i)の物質のFeサイトの一部がX以外の遷移元素で置換され、上記(i)の物質のXサイトの一部がX以外の典型金属元素で置換された物質
リガク社製のX線回折装置 RINT2200を用いて、40kV及び40mAの光源からCu‐Kα線を、平行ビーム光学系を通過させて試料に照射し、sin2Ψ法の原理で各実施例及び各比較例における磁性体の内部応力を評価した。Cu‐Kα線の波長λは、0.1541nmであった。sin2Ψ法は、多結晶薄膜の結晶格子歪みの角度(Ψ)に対する依存性から、薄膜の内部応力を求める手法である。上記のX線回折装置を用い、θ/2θスキャン測定によって、2θ=40°~50°の範囲において0.02°おきに回折強度を測定した。各測定点における積算時間は100秒に設定した。得られたX線回折のピーク角2θと、光源から照射されたX線の波長λとから、各測定角度(Ψ)における磁性体の結晶格子面間隔dを算出し、結晶格子面間隔dから下記の式(1)及び式(2)の関係から結晶格子歪みεを算出した。λは、光源から照射されたX線(Cu‐Kα線)の波長であり、λ=0.1541nmである。d0は、無応力状態の磁性体の格子面間隔であり、d0=0.0206nmである。
2dsinθ=λ 式(1)
ε=(d-d0)/d0 式(2)
ε={(1+ν)/E}σsin2Ψ-(2ν/E)σ 式(3)
各実施例及び各比較例に係る熱電変換素子の環境を、温度85℃及び相対湿度85%の条件に24時間保ち、耐久試験を行った。耐久試験前の熱電変換素子におけるメアンダパターンの電気抵抗値R0及び耐久試験後の熱電変換素子におけるメアンダパターンの電気抵抗値Rtを測定し、100×(Rt-R0)/R0の値を抵抗変化率として求めた。結果を表1に示す。
各実施例及び各比較例に係る熱電変換素子からストリップ状の試験片を作製した。水平に固定された以下の直径を有する円柱状のマンドレルに試験片を巻きつけ、試験片の両端に100gの錘を付けて試験片に荷重をかけた。その後、試験片におけるメアンダパターンの断線の有無について確認した。メアンダパターンの電気抵抗値が初期値の1.5倍以上になったときにメアンダパターンの断線が生じたと判断した。各実施例及び各比較例において、マンドレルの直径の降順で使用するマンドレルを選択し、メアンダパターンの断線が発生するマンドレルの直径の最大値を決定した。結果を表1に示す。
(マンドレルの直径)
21.5mm、20mm、18.5mm、17mm、15.5mm、14mm、12.5mm、11mm、9.5mm、8mm、6.5mm、5mm
50μmの厚みを有するポリエチレンテレフタレート(PET)フィルム上に、Fe及びGaを含むターゲット材を用いてDCマグネトロンスパッタリングによって96nmの厚みを有する薄膜を形成した。このターゲット材において、原子数比で、Feの含有量:Gaの含有量=3:1の関係にあった。DCマグネトロンスパッタリングにおいて、ターゲット材とPETフィルムとの距離は75mmに調整した。また、DCマグネトロンスパッタリングにおいて、100mTの磁束密度を有する磁石を用い、プロセスガスとしてアルゴンガスを0.1Paの圧力で供給した。また、PETフィルムの温度を130℃に調整した。PETフィルムの線膨張係数は、7.0×10-5/℃であった。フォトレジストを薄膜上に塗布し、フォトマスクを薄膜の上に配置して露光を行い、その後ウェットエッチングを行った。これにより、所定の間隔で配置された98本のFeGa含有線状パターンが形成された。各FeGa含有線状パターンの幅は100μmであり、各FeGa線状パターンの長さは15mmであり、FeGa線状パターンの長さの合計は147cmであった。その後、Cuを含むターゲット材を用いてDCマグネトロンスパッタリングによって100nmの厚みを有するCu薄膜を形成した。フォトレジストをCu薄膜上に塗布し、フォトマスクをCu薄膜の上に配置して露光を行い、その後ウェットエッチングを行った。これにより、40μmの幅を有するCu含有線状パターンが形成された。Cu含有線状パターンによって、隣り合う一対のFeGa含有線状パターン同士が電気的に接続されており、メアンダパターンをなす導電路が形成されていた。0.5Tの中心磁束密度を有する電磁石を用いて、PETフィルムの平面に平行であり、かつ、FeGa含有線状パターンの長さ方向と直交する方向にFeGa含有線状パターンを磁化させ、磁性体を形成した。磁性体の厚みは96nmであった。このようにして、実施例1に係る熱電変換素子を得た。この熱電変換素子は、異常ネルンスト効果に基づいて起電力を発生した。
プロセスガスとしてアルゴンガスを0.2Paの圧力で供給した以外は、実施例1と同様にして、実施例2に係る熱電変換素子を得た。実施例2に係る熱電変換素子における磁性体の厚みは96nmであった。
プロセスガスとしてアルゴンガスを0.9Paの圧力で供給した以外は、実施例1と同様にして、実施例3に係る熱電変換素子を得た。実施例3に係る熱電変換素子における磁性体の厚みは89nmであった。
PETフィルムの代わりに、50μmの厚みを有するポリイミド(PI)フィルムを用い、DCマグネトロンスパッタリングにおいてPIフィルムの温度を25℃に調整した以外は、実施例1と同様にして実施例4に係る熱電変換素子を得た。実施例4に係る熱電変換素子における磁性体の厚みは100nmであった。
DCマグネトロンスパッタリングにおいて、PETフィルムの温度を100℃に調整し、かつ、プロセスガスとしてアルゴンガスを0.2Paの圧力で供給した以外は、実施例1と同様にして実施例5に係る熱電変換素子を得た。実施例5に係る熱電変換素子における磁性体の厚みは96nmであった。
DCマグネトロンスパッタリングにおいて、PETフィルムの温度を50℃に調整し、かつ、プロセスガスとしてアルゴンガスを0.2Paの圧力で供給した以外は、実施例1と同様にして実施例6に係る熱電変換素子を得た。実施例6に係る熱電変換素子における磁性体の厚みは96nmであった。
DCマグネトロンスパッタリングにおいて、PETフィルムの温度を25℃に調整した以外は、実施例1と同様にして実施例7に係る熱電変換素子を得た。実施例7に係る熱電変換素子における磁性体の厚みは96nmであった。
各FeGa含有線状パターンの幅が50μmになるようにウェットエッチングの条件を調整したこと以外は、実施例1と同様にして実施例8に係る熱電変換素子を得た。実施例8に係る熱電変換素子における磁性体の厚みは96nmであった。
各FeGa含有線状パターンの幅が200μmになるようにウェットエッチングの条件を調整したこと以外は、実施例1と同様にして実施例9に係る熱電変換素子を得た。実施例9に係る熱電変換素子における磁性体の厚みは96nmであった。
各FeGa含有線状パターンの幅が300μmになるようにウェットエッチングの条件を調整したこと以外は、実施例1と同様にして実施例10に係る熱電変換素子を得た。実施例10に係る熱電変換素子における磁性体の厚みは96nmであった。
各FeGa含有線状パターンの幅が400μmになるようにウェットエッチングの条件を調整したこと以外は、実施例1と同様にして実施例11に係る熱電変換素子を得た。実施例11に係る熱電変換素子における磁性体の厚みは96nmであった。
プロセスガスとしてアルゴンガスを1.6Paの圧力で供給した以外は、実施例1と同様にして、比較例1に係る熱電変換素子を得た。比較例1に係る熱電変換素子における磁性体の厚みは85nmであった。
DCマグネトロンスパッタリングにおいて、プロセスガスとしてアルゴンガスを1.6Paの圧力で供給し、かつ、各FeGa含有線状パターンの幅が1000μmになるようにウェットエッチングの条件を調整したこと以外は、実施例1と同様にして比較例2に係る熱電変換素子を得た。比較例2に係る熱電変換素子における磁性体の厚みは85nmであった。この熱電変換素子は、異常ネルンスト効果に基く起電力を示さなかった。
基材と、
前記基材上に配置され、強磁性又は反強磁性を有する磁性体と、を備え、
前記磁性体は、900MPa以下の内部応力を有する、
熱電変換素子を提供する。
前記基材は、可撓性を有する、熱電変換素子を提供する。
前記基材は、有機ポリマーを少なくとも含む、熱電変換素子を提供する。
前記基材は、1.0×10-5/℃以上の線膨張係数を有する、熱電変換素子を提供する。
前記基材は、200μm以下の厚みを有する、熱電変換素子を提供する。
前記磁性体は、1000nm以下の厚みを有する、熱電変換素子を提供する。
前記磁性体は、500μm以下の幅を有する、熱電変換素子を提供する。
前記磁性体は、前記基材の厚み方向に温度勾配が生じたときに前記基材の厚み方向に直交する方向に起電力を生じさせる、熱電変換素子を提供する。
前記磁性体は、磁気熱電効果により起電力を生じさせる、熱電変換素子を提供する。
前記磁性体を含み、メアンダパターンをなしている導電路を備えた、熱電変換素子を提供する。
前記磁性体は、前記メアンダパターンにおいて500μm以下の線幅を有する、熱電変換素子を提供する。
Claims (11)
- 基材と、
前記基材上に配置され、強磁性又は反強磁性を有する磁性体と、を備え、
前記磁性体は、900MPa以下の内部応力を有する、
熱電変換素子。 - 前記基材は、可撓性を有する、請求項1に記載の熱電変換素子。
- 前記基材は、有機ポリマーを少なくとも含む、請求項2に記載の熱電変換素子。
- 前記基材は、1.0×10-5/℃以上の線膨張係数を有する、請求項1に記載の熱電変換素子。
- 前記基材は、200μm以下の厚みを有する、請求項1に記載の熱電変換素子。
- 前記磁性体は、1000nm以下の厚みを有する、請求項1に記載の熱電変換素子。
- 前記磁性体は、500μm以下の幅を有する、請求項1に記載の熱電変換素子。
- 前記磁性体は、前記基材の厚み方向に温度勾配が生じたときに前記基材の厚み方向に直交する方向に起電力を生じさせる、請求項1に記載の熱電変換素子。
- 前記磁性体は、磁気熱電効果により起電力を生じさせる、請求項1に記載の熱電変換素子。
- 前記磁性体を含み、メアンダパターンをなしている導電路を備えた、請求項1に記載の熱電変換素子。
- 前記磁性体は、前記メアンダパターンにおいて500μm以下の線幅を有する、請求項10に記載の熱電変換素子。
Priority Applications (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP22853122.4A EP4383994A1 (en) | 2021-08-06 | 2022-08-03 | Thermoelectric conversion element |
CN202280055101.1A CN117813945A (zh) | 2021-08-06 | 2022-08-03 | 热电转换元件 |
KR1020247007344A KR20240038099A (ko) | 2021-08-06 | 2022-08-03 | 열전 변환 소자 |
JP2023540400A JPWO2023013704A1 (ja) | 2021-08-06 | 2022-08-03 |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2021-130340 | 2021-08-06 | ||
JP2021130340 | 2021-08-06 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2023013704A1 true WO2023013704A1 (ja) | 2023-02-09 |
Family
ID=85156045
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/JP2022/029863 WO2023013704A1 (ja) | 2021-08-06 | 2022-08-03 | 熱電変換素子 |
Country Status (5)
Country | Link |
---|---|
EP (1) | EP4383994A1 (ja) |
JP (1) | JPWO2023013704A1 (ja) |
KR (1) | KR20240038099A (ja) |
CN (1) | CN117813945A (ja) |
WO (1) | WO2023013704A1 (ja) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2023190993A1 (ja) * | 2022-03-30 | 2023-10-05 | 日東電工株式会社 | 磁性薄膜付基材、磁気熱電変換素子、センサ、及び磁性薄膜付基材を製造する方法 |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2013508983A (ja) * | 2009-10-25 | 2013-03-07 | デストロン フィアリング コーポレイション | 平面熱電発電装置 |
JP2014072256A (ja) | 2012-09-28 | 2014-04-21 | Tohoku Univ | 熱電発電デバイス |
WO2020218613A1 (ja) * | 2019-04-26 | 2020-10-29 | 国立大学法人東京大学 | 熱電変換素子及び熱電変換装置 |
-
2022
- 2022-08-03 WO PCT/JP2022/029863 patent/WO2023013704A1/ja active Application Filing
- 2022-08-03 EP EP22853122.4A patent/EP4383994A1/en active Pending
- 2022-08-03 CN CN202280055101.1A patent/CN117813945A/zh active Pending
- 2022-08-03 JP JP2023540400A patent/JPWO2023013704A1/ja active Pending
- 2022-08-03 KR KR1020247007344A patent/KR20240038099A/ko unknown
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2013508983A (ja) * | 2009-10-25 | 2013-03-07 | デストロン フィアリング コーポレイション | 平面熱電発電装置 |
JP2014072256A (ja) | 2012-09-28 | 2014-04-21 | Tohoku Univ | 熱電発電デバイス |
WO2020218613A1 (ja) * | 2019-04-26 | 2020-10-29 | 国立大学法人東京大学 | 熱電変換素子及び熱電変換装置 |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2023190993A1 (ja) * | 2022-03-30 | 2023-10-05 | 日東電工株式会社 | 磁性薄膜付基材、磁気熱電変換素子、センサ、及び磁性薄膜付基材を製造する方法 |
Also Published As
Publication number | Publication date |
---|---|
KR20240038099A (ko) | 2024-03-22 |
JPWO2023013704A1 (ja) | 2023-02-09 |
CN117813945A (zh) | 2024-04-02 |
EP4383994A1 (en) | 2024-06-12 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
JP7276856B2 (ja) | 熱電変換素子及び熱電変換デバイス | |
US20220246820A1 (en) | Thermoelectric conversion element and thermoelectric conversion device | |
EP2110867A1 (en) | Magnetic sensor element and method for manufacturing the same | |
KR101744107B1 (ko) | 자기전기 센서 및 자기전기 센서의 생산을 위한 방법 | |
WO2023013704A1 (ja) | 熱電変換素子 | |
KR20140068005A (ko) | 자왜 층 시스템 | |
KR20160034891A (ko) | 서미스터용 금속 질화물 재료 및 그 제조 방법 그리고 필름형 서미스터 센서 | |
US20150303363A1 (en) | Thermoelectric conversion element, use of the same, and method of manufacturing the same | |
EP0618628B1 (en) | Mechanical sensor | |
WO2023013703A1 (ja) | 熱電変換素子 | |
JP7162461B2 (ja) | ヒータ用部材、ヒータ用テープ、及びヒータ用部材付成形体 | |
WO2023013702A1 (ja) | 熱電変換素子 | |
Kuts et al. | Magnetoelectric effect in three-layered gradient LiNbO3/Ni/Metglas composites | |
WO2023190993A1 (ja) | 磁性薄膜付基材、磁気熱電変換素子、センサ、及び磁性薄膜付基材を製造する方法 | |
WO2023054415A1 (ja) | 熱電変換素子及び熱電変換素子の製造方法 | |
WO2023054416A1 (ja) | 熱電変換素子及びセンサ | |
Umarov et al. | Piezophotoresistive qualities of р-TlInSe2 monocrystals | |
WO2024071419A1 (ja) | 熱電変換素子及びセンサ | |
WO2022264940A1 (ja) | 熱電発電デバイス | |
US20220349760A1 (en) | Temperature sensor film, conductive film and method for producing same | |
WO2023054583A1 (ja) | 熱電体、熱電発電素子、多層熱電体、多層熱電発電素子、熱電発電機、及び熱流センサ | |
JP2004349528A (ja) | 磁気インピーダンス素子 | |
WO2022092204A1 (ja) | 積層フィルムおよび歪みセンサ | |
Uchida et al. | Anomalous Nernst thermoelectric generation in multilayer-laminated coiled magnetic wires | |
KR100753938B1 (ko) | 초전도체의 교류자화손실 측정용 픽업코일 |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
WWE | Wipo information: entry into national phase |
Ref document number: 2023540400 Country of ref document: JP |
|
WWE | Wipo information: entry into national phase |
Ref document number: 202280055101.1 Country of ref document: CN |
|
ENP | Entry into the national phase |
Ref document number: 20247007344 Country of ref document: KR Kind code of ref document: A |
|
NENP | Non-entry into the national phase |
Ref country code: DE |
|
ENP | Entry into the national phase |
Ref document number: 2022853122 Country of ref document: EP Effective date: 20240306 |
|
121 | Ep: the epo has been informed by wipo that ep was designated in this application |
Ref document number: 22853122 Country of ref document: EP Kind code of ref document: A1 |