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JP7728660B2 - Co-Mn-Ga alloy powder, conductive compact, their manufacturing methods, and thermoelectric conversion element - Google Patents
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JP7728660B2 - Co-Mn-Ga alloy powder, conductive compact, their manufacturing methods, and thermoelectric conversion element - Google Patents

Co-Mn-Ga alloy powder, conductive compact, their manufacturing methods, and thermoelectric conversion element

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JP7728660B2
JP7728660B2 JP2021103682A JP2021103682A JP7728660B2 JP 7728660 B2 JP7728660 B2 JP 7728660B2 JP 2021103682 A JP2021103682 A JP 2021103682A JP 2021103682 A JP2021103682 A JP 2021103682A JP 7728660 B2 JP7728660 B2 JP 7728660B2
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王高 佐藤
翔一 公文
彰悟 加藤
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Dowa Holdings Co Ltd
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Dowa Mining Co Ltd
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Description

本発明は、熱電変換素子の素材として有用なCo-Mn-Ga系合金粉体、およびその製造方法に関する。また本発明は、Co-Mn-Ga系合金粉体の導電成形体、その製造方法、および上記導電成形体を用いた熱電変換素子に関する。 The present invention relates to a Co-Mn-Ga alloy powder useful as a material for thermoelectric conversion elements, and a method for producing the same. The present invention also relates to a conductive compact of the Co-Mn-Ga alloy powder, a method for producing the same, and a thermoelectric conversion element using the conductive compact.

近年、異常ネルンスト効果を利用した熱電変換素子の研究が進められている。異常ネルンスト効果は、自発的に磁化している磁性体に磁化と直交する向きの熱流を付与したとき、磁化と熱流の双方に垂直な方向の起電力が生じる現象である。異常ネルンスト効果を利用すると熱流と直角方向に電流が取り出せるため、ゼーベック効果を利用する場合とは異なり、薄くシート化した熱電変換デバイスが構築できるといったメリットが得られる。 In recent years, research has been progressing on thermoelectric conversion elements that utilize the anomalous Nernst effect. The anomalous Nernst effect is a phenomenon in which, when a heat flow perpendicular to the magnetization is applied to a spontaneously magnetized magnetic material, an electromotive force is generated in a direction perpendicular to both the magnetization and the heat flow. Utilizing the anomalous Nernst effect allows current to be extracted perpendicular to the heat flow, which, unlike when using the Seebeck effect, offers the advantage of being able to construct thin, sheet-like thermoelectric conversion devices.

常温で大きい異常ネルンスト効果を示す物質として、強磁性金属間化合物CoMnGaが知られている。 The ferromagnetic intermetallic compound Co 2 MnGa is known as a material that exhibits a large anomalous Nernst effect at room temperature.

特許文献1には、チョクラルスキー法によってCoMnGa単結晶を作製し、異常ネルンスト係数を測定した実験例が記載されている。CoMnGa単結晶の室温(300K)でのネルンスト係数は、磁場の付与方向が結晶の[100]、[110]、[111]方向のいずれに平行な場合も、6μV/K程度の高い値に達している(段落0021、図4)。 Patent Document 1 describes an example of an experiment in which a Co2MnGa single crystal was produced by the Czochralski method and the anomalous Nernst coefficient was measured. The Nernst coefficient of the Co2MnGa single crystal at room temperature (300 K) reached a high value of about 6 μV/K regardless of whether the magnetic field direction was parallel to the [100], [110], or [111] direction of the crystal (paragraph 0021, Figure 4).

特許文献2には、熱流センサと温度センサを有する複合センサにおいて、その熱流センサに異常ネルンスト材料膜を使用することが記載されている。異常ネルンスト材料としていくつかの物質が列挙されており、その1つとしてCoMnGaの記載がある(段落0026)。異常ネルンスト材料膜の成膜方法としてスパッタ法が示されている(段落0030)。 Patent Document 2 describes the use of an anomalous Nernst material film in a composite sensor having a heat flow sensor and a temperature sensor. Several substances are listed as anomalous Nernst materials, one of which is Co2MnGa (paragraph 0026). A sputtering method is presented as a method for forming the anomalous Nernst material film (paragraph 0030).

国際公開第2019/009308号International Publication No. 2019/009308 特開2020-153668号公報Japanese Patent Application Laid-Open No. 2020-153668

熱電変換素子の主な用途として、熱電発電デバイスおよび熱流センサが挙げられる。 The main applications of thermoelectric conversion elements include thermoelectric power generation devices and heat flow sensors.

熱電発電デバイスを実現するための熱電変換素子は、厚さ数ミリメートル程度のバルク体であることが望ましい。チョクラルスキー法による単結晶体を用いると、上記のようなサイズのバルク体を作製することは可能である。しかし、チョクラルスキー法などの単結晶製造技術はコストが高く生産性が低いので、熱電発電デバイス用素材の工業的生産においては実用的ではない。一方、スパッタ法などの成膜技術を、熱電発電デバイス用のバルク素材の工業的生産に適用することは困難である。 The thermoelectric conversion elements used to realize thermoelectric power generation devices are preferably bulk bodies with a thickness of approximately several millimeters. It is possible to produce bulk bodies of the above size using single crystals produced by the Czochralski method. However, single crystal manufacturing techniques such as the Czochralski method are expensive and have low productivity, making them impractical for the industrial production of materials for thermoelectric power generation devices. On the other hand, it is difficult to apply film formation techniques such as sputtering to the industrial production of bulk materials for thermoelectric power generation devices.

熱流センサを実現するための熱電変換素子は、微小な回路パターンの一部に組み込んで使用することを考慮すると、小サイズの素子であることが望まれる。小サイズの素子を、チョクラルスキー法などで得られる単結晶体から多数切り出すことは、コスト面で工業的に実用化することが難しい。また、所定形状の小サイズ素子をチョクラルスキー法で直接形成させることも困難である。一方、スパッタ法などの成膜技術によれば、所定の回路パターンに応じた小サイズの素子を絶縁基板上に直接形成させることは可能である。しかし、そのような成膜方法は生産性が低く、熱流センサの製造コストは高くなる。 The thermoelectric conversion elements used to create heat flow sensors are desirably small, considering that they will be incorporated into a small circuit pattern. Cutting a large number of small elements from a single crystal obtained using methods such as the Czochralski method is cost-prohibitive for industrial use. It is also difficult to directly form small elements of a specified shape using the Czochralski method. On the other hand, using film-forming techniques such as sputtering, it is possible to form small elements corresponding to a specified circuit pattern directly on an insulating substrate. However, such film-forming methods have low productivity, resulting in high manufacturing costs for heat flow sensors.

本発明は、異常ネルンスト効果を利用した、高いネルンスト係数が得られる熱電変換素子を、生産性良く製造するために適した技術であって、特に種々の形状、サイズの素子の製造に幅広く対応できる技術の提供を目的とする。また、その技術を用いて得られるネルンスト係数の高い熱電変換素子の提供を目的とする。 The present invention aims to provide technology suitable for the productive manufacture of thermoelectric conversion elements that utilize the anomalous Nernst effect and achieve a high Nernst coefficient, and in particular technology that can be widely adapted to the manufacture of elements of various shapes and sizes. It also aims to provide thermoelectric conversion elements with a high Nernst coefficient obtained using this technology.

上記目的を達成するために、本明細書では以下の発明を開示する。 To achieve the above objectives, this specification discloses the following invention.

[1]金属間化合物CoMnGaを主成分とする粉体であって、レーザー回折・散乱法による体積基準の粒度分布において、累積50%粒子径D50が1~150μm、累積90%粒子径D90が250μm以下であるCo-Mn-Ga系合金粉体。
[2]Co、MnおよびGaからなる溶融金属を凝固させ、金属間化合物CoMnGaを主成分とするCo-Mn-Ga系合金塊を得る合金塊作製工程、
前記Co-Mn-Ga系合金塊を粉砕することにより粉体を得る粉砕工程、
を有する上記[1]に記載のCo-Mn-Ga系合金粉体の製造方法。
[3]前記粉砕工程で得られた粉体を篩により分級する分級工程、
を更に有する上記[2]に記載のCo-Mn-Ga系合金粉体の製造方法。
[4]金属間化合物CoMnGaを主成分とする粉体の導電成形体。
[5]前記金属間化合物CoMnGaを主成分とする粉体は、レーザー回折・散乱法による体積基準の粒度分布において、累積50%粒子径D50が1~150μm、累積90%粒子径D90が250μm以下のものである、上記[4]に記載の導電成形体。
[6]金属間化合物CoMnGaを主成分とする粉体の焼結体である、上記[4]または[5]に記載の導電成形体。
[7]温度300Kにおいて6.0μV/K以上のネルンスト係数を呈する上記[4]~[6]のいずれかに記載の導電成形体。
[8]金属間化合物CoMnGaを主成分とする粉体を、焼結させることにより、導電成形体を得る焼結工程、を有する導電成形体の製造方法。
[9]前記金属間化合物CoMnGaを主成分とする粉体は、レーザー回折・散乱法による体積基準の粒度分布において、累積50%粒子径D50が1~150μm、累積90%粒子径D90が250μm以下のものである、上記[8]に記載の導電成形体の製造方法。
[10]上記[4]~[7]のいずれかに記載の導電成形体を用いた熱電変換素子。
[1] A Co-Mn-Ga alloy powder containing an intermetallic compound Co 2 MnGa as a main component, in which, in a volume-based particle size distribution measured by a laser diffraction/scattering method, the cumulative 50% particle diameter D50 is 1 to 150 μm and the cumulative 90% particle diameter D90 is 250 μm or less.
[2] an alloy ingot preparation step of solidifying a molten metal consisting of Co, Mn, and Ga to obtain a Co—Mn—Ga-based alloy ingot containing the intermetallic compound Co 2 MnGa as a main component;
a pulverization step of pulverizing the Co—Mn—Ga-based alloy ingot to obtain a powder;
The method for producing the Co—Mn—Ga alloy powder according to the above [1].
[3] a classification step of classifying the powder obtained in the pulverization step using a sieve;
The method for producing a Co—Mn—Ga based alloy powder according to [2] above, further comprising:
[4] A conductive compact of powder containing the intermetallic compound Co 2 MnGa as a main component.
[5] The powder mainly composed of the intermetallic compound Co 2 MnGa has a cumulative 50% particle diameter D50 of 1 to 150 μm and a cumulative 90% particle diameter D90 of 250 μm or less in a volume-based particle size distribution measured by a laser diffraction/scattering method, the conductive molded body according to [4].
[6] The conductive molded body according to the above [4] or [5], which is a sintered body of a powder containing an intermetallic compound Co 2 MnGa as a main component.
[7] The conductive molded body according to any one of the above [4] to [6], which exhibits a Nernst coefficient of 6.0 μV/K or more at a temperature of 300K.
[8] A method for producing a conductive compact, comprising a sintering step of sintering a powder containing an intermetallic compound Co 2 MnGa as a main component to obtain a conductive compact.
[9] The method for producing a conductive molded body according to the above-mentioned [8], wherein the powder mainly composed of the intermetallic compound Co 2 MnGa has a cumulative 50% particle diameter D50 of 1 to 150 μm and a cumulative 90% particle diameter D90 of 250 μm or less in a volume-based particle size distribution measured by a laser diffraction/scattering method.
[10] A thermoelectric conversion element using the conductive molded article according to any one of [4] to [7] above.

本発明によれば、ネルンスト係数の高い熱電変換素子を得ることができる。その熱電変換素子に用いる磁性材料は粉体であるため、本発明の技術は、種々の形状、サイズの素子に幅広く対応することができる。また、本発明の技術は、単結晶やスパッタ法による薄膜を用いた従来の技術と比べ、コストおよび生産性の面で優れる。 The present invention makes it possible to obtain thermoelectric conversion elements with a high Nernst coefficient. Because the magnetic material used in these thermoelectric conversion elements is a powder, the technology of the present invention can be used to produce elements of a wide variety of shapes and sizes. Furthermore, the technology of the present invention is superior in terms of cost and productivity compared to conventional technologies that use single crystals or thin films produced by sputtering.

第1分級工程後の粉体についてのX線回折パターン。X-ray diffraction pattern of the powder after the first classification step. 第1分級工程後の粉体についてのSEM写真。10 is an SEM photograph of the powder after the first classification process. 第2分級工程後の粉体についてのSEM写真。10 is an SEM photograph of the powder after the second classification process. 実施例で用いたネルンスト効果測定用試料について、電力測定用の端子、温度測定用のプローブ取り付け位置と、熱流、磁場の付与方向を模式的に示した図。FIG. 2 is a diagram schematically showing the attachment positions of terminals for power measurement and probes for temperature measurement, as well as the directions of heat flow and magnetic field application, for a sample for measuring the Nernst effect used in the examples. 第2分級工程後の粉体の導電成形体についての、ネルンスト係数の測定結果を示すグラフ。10 is a graph showing the results of measuring the Nernst coefficient of the conductive compact powder after the second classification step.

[Co-Mn-Ga系合金粉体]
本発明では熱電変換素子に適した材料として金属間化合物CoMnGaを主成分とするCo-Mn-Ga系合金粉体を適用する。CoMnGaはL2結晶構造を持つホイスラー合金の1種である。この金属間化合物はワイル強磁性体であり、常温付近でのネルンスト係数が6μV/K程度に達し、大きい異常ネルンスト効果を発現する物質であることが知られている。
[Co-Mn-Ga alloy powder]
In this invention, a Co- Mn -Ga alloy powder containing the intermetallic compound Co2MnGa as its main component is used as a material suitable for thermoelectric conversion elements. Co2MnGa is a type of Heusler alloy with an L21 crystal structure. This intermetallic compound is a Weyl ferromagnetic material, and is known to exhibit a large anomalous Nernst effect, with a Nernst coefficient of approximately 6 μV/K at room temperature.

Co、Mn、Gaの組成比がCoMnGaの化学量論組成に近い一定の組成域において、CoMnGa型の結晶構造を持つ金属間化合物が単相として安定に存在し得る。その組成域の周辺ではCoMnGa型の結晶構造を持つ金属間化合物相と異相とが混在したCo-Mn-Ga系合金が得られると考えられる。本明細書では、Co-Mn-Ga系3元合金において、CoMnGa型(すなわちL2)結晶構造を持つ金属間化合物相を「金属間化合物CoMnGa」、あるいは単に「CoMnGa相」と呼んでいる。したがって、CoMnGaの化学量論組成から少しずれた組成比の金属間化合物であっても、CoMnGa型結晶構造を持つものは、本明細書でいう「金属間化合物CoMnGa」に含まれる。 In a certain composition range where the composition ratio of Co, Mn, and Ga is close to the stoichiometric composition of Co 2 MnGa, an intermetallic compound having a Co 2 MnGa-type crystal structure can exist stably as a single phase. It is believed that a Co-Mn-Ga-based alloy can be obtained around this composition range, in which an intermetallic compound phase having a Co 2 MnGa-type crystal structure and a different phase are mixed. In this specification, an intermetallic compound phase having a Co 2 MnGa-type (i.e., L2 1 ) crystal structure in a Co-Mn-Ga-based ternary alloy is referred to as the "intermetallic compound Co 2 MnGa" or simply the "Co 2 MnGa phase." Therefore, even if an intermetallic compound has a composition ratio slightly different from the stoichiometric composition of Co 2 MnGa, one having a Co 2 MnGa-type crystal structure is included in the "intermetallic compound Co 2 MnGa" referred to in this specification.

「金属間化合物CoMnGaを主成分とする」とは、粉体に含まれる金属相のうち、質量割合が最も多い金属相がCoMnGa相であることを意味する。Co-Mn-Ga系合金粉体を用いた熱電変換素子において、CoMnGa相以外の異相が含まれていても、CoMnGa相の異常ネルンスト効果による熱電変換作用は生じる。しかし、効率の良い熱電変換特性を実現するためには、異常ネルンスト効果を示さない異相の存在量は少ないことが望ましい。例えば、粉体に占めるCoMnGa相の割合は50質量%以上であることが好ましく、90質量%以上であることがより好ましい。また、金属間化合物CoMnGaからなる粉体、すなわち、金属間化合物CoMnGa以外は不可避的不純物である粉体が特に好ましい。 "Mainly composed of the intermetallic compound Co 2 MnGa" means that the metal phase with the largest mass fraction among the metal phases contained in the powder is the Co 2 MnGa phase. In a thermoelectric conversion element using a Co-Mn-Ga alloy powder, even if a heterophase other than the Co 2 MnGa phase is contained, the thermoelectric conversion action occurs due to the anomalous Nernst effect of the Co 2 MnGa phase. However, to achieve efficient thermoelectric conversion characteristics, it is desirable that the amount of heterophases that do not exhibit the anomalous Nernst effect be small. For example, the proportion of the Co 2 MnGa phase in the powder is preferably 50 mass% or more, and more preferably 90 mass% or more. Furthermore, powders consisting of the intermetallic compound Co 2 MnGa, i.e., powders in which the intermetallic compound Co 2 MnGa and other components are unavoidable impurities, are particularly preferred.

Co-Mn-Ga系合金粉体を構成する粒子の粒度分布は、レーザー回折・散乱法による体積基準の粒度分布において、累積50%粒子径D50が1~150μm、累積90%粒子径D90が250μm以下の範囲とする。累積50%粒子径D50大きすぎる場合は、平均粒子径が大きくなるため、保磁力の低下につながる。累積90%粒子径D90が大きすぎる場合は、粗大粒子の存在割合が大きくなるため、この場合も保磁力の低下につながる。保磁力を確保する観点からは、累積50%粒子径D50が100μm以下であることが好ましく、60μm以下であることがより好ましい。 The particle size distribution of the particles that make up the Co-Mn-Ga alloy powder, measured by volumetric particle size distribution using a laser diffraction/scattering method, should be such that the cumulative 50% particle diameter D50 is 1 to 150 μm and the cumulative 90% particle diameter D90 is 250 μm or less. If the cumulative 50% particle diameter D50 is too large, the average particle diameter will be large, leading to a decrease in coercivity. If the cumulative 90% particle diameter D90 is too large, the proportion of coarse particles will increase, also leading to a decrease in coercivity. From the perspective of ensuring coercivity, the cumulative 50% particle diameter D50 is preferably 100 μm or less, and more preferably 60 μm or less.

Co-Mn-Ga系合金粉体の製造方法としては、例えば、
Co、MnおよびGaからなる溶融金属を凝固させ、金属間化合物CoMnGaを主成分とするCo-Mn-Ga系合金塊を得る合金塊作製工程、
前記Co-Mn-Ga系合金塊を粉砕することにより粉体を得る粉砕工程、
必要に応じて、前記粉砕工程で得られた粉体を篩により分級する分級工程、
を有するプロセスが適用できる。
Examples of methods for producing Co—Mn—Ga-based alloy powder include:
an alloy ingot preparation step of solidifying a molten metal consisting of Co, Mn, and Ga to obtain a Co—Mn—Ga-based alloy ingot containing an intermetallic compound Co 2 MnGa as a main component;
a pulverization step of pulverizing the Co—Mn—Ga-based alloy ingot to obtain a powder;
If necessary, a classification step of classifying the powder obtained in the pulverization step using a sieve;
A process having the following can be applied.

Co、MnおよびGaからなる溶融金属は、所定組成に秤量したCo、Mn、Gaの各原料金属をるつぼに入れ、非酸化性雰囲気中で加熱し溶融させる手法で得ることができる。その後、溶融金属を凝固させ、Co-Mn-Ga系合金塊を得る。溶融金属の凝固は、るつぼ中で冷却する方法で行ってもよいし、鋳型に鋳造する方法で行ってもよい。 Molten metal consisting of Co, Mn, and Ga can be obtained by placing the raw Co, Mn, and Ga metals, weighed to the specified composition, into a crucible and heating and melting them in a non-oxidizing atmosphere. The molten metal is then solidified to obtain a Co-Mn-Ga alloy ingot. The molten metal can be solidified by cooling it in the crucible or by casting it into a mold.

次に、Co-Mn-Ga系合金塊を粉砕することにより粉体を得る。粉砕手段としては、例えばスタンプミル、ハンマーミル、サンプルミルなど、公知の機械的粉砕装置が適用できる。複数の粉砕手段を組み合わせて段階的に粒子径を減じていくことが効率的である。粉砕工程を段階的に行う場合、各粉砕段階の間で篩などによる分級を実施しても構わない。また、最終的な粒度分布の調整のために、最後の粉砕手段を終了して得られた粉体に対して、篩による分級を行うことが好ましい。 The Co-Mn-Ga alloy ingot is then pulverized to obtain a powder. Known mechanical pulverizers, such as stamp mills, hammer mills, and sample mills, can be used as the pulverizing means. It is more efficient to combine multiple pulverizing means to gradually reduce the particle size. When the pulverizing process is carried out in stages, classification using a sieve or other method may be performed between each pulverizing stage. Furthermore, to adjust the final particle size distribution, it is preferable to classify the powder obtained after the final pulverizing step using a sieve.

[導電成形体]
本明細書では、粉体を材料に用いて所定形状に成形され、使用環境においてその形状を維持できる定形性を備えた物体を、「粉体の成形体」と呼ぶ。特に、導電性を有する粉体の成形体を「粉体の導電成形体」と呼ぶ。上記のCo-Mn-Ga系合金粉体を材料に用いた、金属間化合物CoMnGaを主成分とする粉体の導電成形体は、熱電変換素子として有用である。
[Conductive molded body]
In this specification, an object that is formed into a predetermined shape using powder as a material and has the definite shape to maintain that shape in the usage environment is called a "powder compact." In particular, a powder compact that has conductivity is called a "conductive powder compact." A conductive powder compact that uses the above Co-Mn-Ga alloy powder as a material and contains the intermetallic compound Co 2 MnGa as its main component is useful as a thermoelectric conversion element.

粉体の導電成形体の代表的な形態として、圧粉体、焼結体が挙げられる。圧粉体であっても、使用環境で定形性を維持できるようにしてデバイスに組み込むことにより、熱電変換素子として使用可能である。安定した定形性を確保するためには、焼結体が好ましい。 Typical forms of conductive powder compacts include green compacts and sintered compacts. Green compacts can also be used as thermoelectric conversion elements by incorporating them into devices in a way that allows them to maintain their shape in the usage environment. Sintered compacts are preferred to ensure stable shapeability.

粉体の導電成形体の、圧粉体、焼結体以外の形態としては、例えば樹脂等のバインダー成分により粉体を所定形状に固形化した成形体を挙げることができる。導電性のないバインダー成分を使用する場合は、粉体粒子同士が接触する状態で固形化させる必要がある。導電性を有するバインダー成分を使用する場合は、粉体粒子同士の接触は必須ではない。 An example of a form of conductive powder compact other than a compact or sintered compact is a compact formed by solidifying powder into a predetermined shape using a binder component such as a resin. When a non-conductive binder component is used, the powder particles must be solidified in a state where they are in contact with each other. When a conductive binder component is used, contact between the powder particles is not essential.

金属間化合物CoMnGaを主成分とする粉体の導電成形体として、焼結体を適用する場合は、公知の焼結手法を利用して金属間化合物CoMnGaを主成分とする粉体の焼結体を作製することができる。絶縁基板上に形成された回路パターンの一部または全部を、金属間化合物CoMnGaを主成分とする粉体の導電成形体として使用する場合は、当該粉体をフィラーとする塗料により絶縁基板上に回路パターンの塗膜を形成したのち、その塗膜を加熱して焼結させる方法が適用できる。 When a sintered body is used as a conductive compact of a powder containing the intermetallic compound Co 2 MnGa as the main component, a sintered body of a powder containing the intermetallic compound Co 2 MnGa as the main component can be produced by using a known sintering method.When a part or all of a circuit pattern formed on an insulating substrate is used as a conductive compact of a powder containing the intermetallic compound Co 2 MnGa as the main component, a method can be applied in which a coating film of the circuit pattern is formed on the insulating substrate using a paint containing the powder as a filler, and then the coating film is heated and sintered.

上述した粒度分布に調整されたCo-Mn-Ga系合金粉体を材料に用いることによって、温度300Kにおいて6.0μV/K以上のネルンスト係数を呈する粉体の導電成形体を構築することが可能である。 By using Co-Mn-Ga alloy powder adjusted to the particle size distribution described above, it is possible to create a conductive powder compact that exhibits a Nernst coefficient of 6.0 μV/K or more at a temperature of 300 K.

[実施例1]
(Co-Mn-Ga系合金塊の作製)
原料である金属Co(株式会社レアメタリック製、純度3N)、金属Mn(株式会社レアメタリック製、純度3N)および金属Ga(株式会社レアメタリック製、純度6N)を、モル比においてCo:Mn:Ga=2:1:1となるように秤量してアルミナるつぼに入れた。このるつぼを縦型電気炉に装入し、Arガス雰囲気下において、常温から1000℃まで4時間かけて昇温、1000℃から1250℃まで2時間かけて昇温、1250℃で12時間保持、その後、炉内で5時間放冷、というヒートパターンにより、Co-Mn-Ga系合金の溶融金属をるつぼ中で凝固させ、Co-Mn-Ga系合金塊を得た。
[Example 1]
(Production of Co—Mn—Ga-based alloy ingot)
The raw materials, metallic Co (manufactured by Rare Metallic Co., Ltd., purity 3N), metallic Mn (manufactured by Rare Metallic Co., Ltd., purity 3N), and metallic Ga (manufactured by Rare Metallic Co., Ltd., purity 6N), were weighed out to a molar ratio of Co:Mn:Ga = 2:1:1 and placed in an alumina crucible. This crucible was placed in a vertical electric furnace and, under an Ar gas atmosphere, the temperature was raised from room temperature to 1000°C over 4 hours, raised from 1000°C to 1250°C over 2 hours, held at 1250°C for 12 hours, and then allowed to cool in the furnace for 5 hours. This heating pattern allowed the molten metal of the Co—Mn—Ga alloy to solidify in the crucible, yielding a Co—Mn—Ga alloy ingot.

(粉体の作製)
得られたCo-Mn-Ga系合金塊553.47gを用いて、以下の3段階の粉砕工程および2段階の分級工程により粉体を作製した。
(Powder preparation)
553.47 g of the obtained Co—Mn—Ga alloy ingot was subjected to the following three-stage pulverization process and two-stage classification process to produce powder.

(第1粉砕工程)
上記のCo-Mn-Ga系合金塊をスタンプミル(日陶科学株式会社製、ANS-143PS)により大気雰囲気下で約5mm以下の粒子に粉砕した。
(First pulverization step)
The above Co-Mn-Ga alloy ingot was pulverized into particles of about 5 mm or less in an air atmosphere using a stamp mill (ANS-143PS, manufactured by Nitto Kagaku Co., Ltd.).

(第2粉砕工程)
第1粉砕工程で得られた粉砕物を、ハンマーミル(三庄インダストリー株式会社製、ハンマークラッシャーNH-34S、スクリーンメッシュ:0.3mm)により、グローブボックス中、窒素ガス雰囲気下で粉砕した。粉砕中の雰囲気における酸素濃度は0.0体積%未満であった。粉砕終了後、徐々に大気開放し、粉砕物を回収した。
(Second pulverization step)
The pulverized material obtained in the first pulverization step was pulverized in a glove box under a nitrogen gas atmosphere using a hammer mill (Hammer Crusher NH-34S, manufactured by Sansho Industry Co., Ltd., screen mesh: 0.3 mm). The oxygen concentration in the atmosphere during pulverization was less than 0.0% by volume. After pulverization was completed, the container was gradually opened to the atmosphere, and the pulverized material was collected.

(第3粉砕工程)
第2粉砕工程で得られた粉砕物を、サンプルミル(協立理工株式会社製、SK-M10型)により、グローブボックス中、窒素ガス雰囲気下で粉砕した。粉砕手順は、「30秒粉砕処理→放冷」を4サイクル繰り返す方法とした。粉砕、放冷サイクル中の雰囲気における酸素濃度は0.0体積%未満であった。最後の放冷終了後、徐々に大気開放し、粉砕物である粉体を回収した。
(Third pulverization step)
The pulverized material obtained in the second pulverization step was pulverized in a glove box under a nitrogen gas atmosphere using a sample mill (SK-M10 model, manufactured by Kyoritsu Riko Co., Ltd.). The pulverization procedure consisted of repeating four cycles of "30-second pulverization treatment → cooling." The oxygen concentration in the atmosphere during the pulverization and cooling cycles was less than 0.0% by volume. After the final cooling period, the container was gradually opened to the atmosphere, and the pulverized powder was collected.

(第1分級工程)
第3粉砕工程で得られた粉体を目開き100μmの篩で分級し、篩を通過した粉体を得た。
(1st classification process)
The powder obtained in the third pulverization step was classified using a sieve with 100 μm openings, and the powder that passed through the sieve was obtained.

(第2分級工程)
第1分級工程で得られた粉体を目開き45μmの篩で更に分級し、篩を通過した粉体を得た。
(Second classification process)
The powder obtained in the first classification step was further classified using a sieve with 45 μm openings, and the powder that passed through the sieve was obtained.

(粒度分布の測定)
上記の第2粉砕工程後の粉砕物、第3粉砕工程後の粉体、第1分級工程後の粉体、および第2分級工程後の粉体について、乾式レーザー回折式粒度分布測定装置(株式会社日本レーザー製、HELOS & RODOS)により、焦点距離1000mmのレンズを用いてレーザー回折・散乱法による体積基準の粒度分布を測定した。得られた粒度分布に基づき算出された累積10%粒子径D10、累積50%粒子径D50、および累積90%粒子径D90を表1に示す。
(Measurement of particle size distribution)
The pulverized material after the second pulverization step, the powder after the third pulverization step, the powder after the first classification step, and the powder after the second classification step were measured for volumetric particle size distribution by laser diffraction/scattering using a dry laser diffraction particle size distribution analyzer (HELOS & RODOS, manufactured by Japan Laser Co., Ltd.) with a lens having a focal length of 1000 mm. The cumulative 10% particle diameter D10, cumulative 50% particle diameter D50, and cumulative 90% particle diameter D90 calculated based on the obtained particle size distribution are shown in Table 1.

(X線回折パターンの測定)
上記の第1分級工程後の粉体について、X線回折装置(株式会社島津製作所製、XRD-6100 LabX)により、Cu-Kα線でのX線回折パターンを測定した。図1に、そのX線回折パターンを例示する。図1中には格子定数a=0.578nmのCoMnGa結晶で現れる計算上の回折ピーク位置を併せて掲載してある。当該粉体試料のX線回折パターンはCoMnGa結晶の計算上の回折パターンと良く一致している。
(Measurement of X-ray diffraction pattern)
The powder after the first classification step was subjected to measurement of an X-ray diffraction pattern using Cu-Kα radiation using an X-ray diffractometer (Shimadzu Corporation, XRD-6100 LabX). An example of the X-ray diffraction pattern is shown in Figure 1. Figure 1 also shows the calculated diffraction peak positions that appear in a Co 2 MnGa crystal with a lattice constant a = 0.578 nm. The X-ray diffraction pattern of the powder sample is in good agreement with the calculated diffraction pattern of a Co 2 MnGa crystal.

(粉体磁気特性の測定)
上記の第3粉砕工程後の粉体、第1分級工程後の粉体、および第2分級工程後の粉体について、SQUID(Super Quantum Interference Device)磁束計により、以下の方法で300Kにおける磁気特性を測定した。すなわち、粉体試料の温度を300Kとし、SQUID磁束計に付属の超伝導マグネットにより最大磁場3T(30000Oe)を印可した後、3Tから-3T、-3Tから3Tの磁場掃引過程において、各測定点で磁場を固定し、磁化(μ/f.u.)を測定した。その磁化曲線に基づき、飽和磁化および保磁力を求めた。その結果を表1に示す。
(Measurement of powder magnetic properties)
The magnetic properties of the powders after the third pulverization step, the powders after the first classification step, and the powders after the second classification step were measured at 300 K using a SQUID (Super Quantum Interference Device) magnetometer in the following manner. That is, the temperature of the powder samples was set to 300 K, and a maximum magnetic field of 3 T (30,000 Oe) was applied using a superconducting magnet attached to the SQUID magnetometer. Then, the magnetic field was swept from 3 T to -3 T and from -3 T to 3 T, with the magnetic field fixed at each measurement point, and the magnetization (μ B /fu) was measured. The saturation magnetization and coercivity were calculated based on the magnetization curves. The results are shown in Table 1.

(粉体のSEM写真)
上記の第1分級工程後の粉体および第2分級工程後の粉体についてのSEM(走査型電子顕微鏡)写真を、それぞれ、図2および図3に例示する。写真の下部に表示される白いスケールバーの長さが10μmに相当する。使用したSEMは、日本電子株式会社製、FE-SEM JSM-7200Fである。
(SEM photo of powder)
SEM (scanning electron microscope) photographs of the powder after the first classification step and the powder after the second classification step are shown in Figures 2 and 3, respectively. The length of the white scale bar displayed at the bottom of the photograph corresponds to 10 μm. The SEM used was an FE-SEM JSM-7200F manufactured by JEOL Ltd.

(EDXによる粉体の組成分析)
上記の第1分級工程後の粉体について、SEMに付属のEDX(エネルギー分散型X線分析)装置(Oxford Instruments製、X-Max20)により組成分析を行ったところ、原子比でCo:Mn:Mg=51.0:29.1:19.9であった。
(Powder Composition Analysis by EDX)
The powder after the first classification step was subjected to composition analysis using an EDX (energy dispersive X-ray analysis) device (X-Max20, manufactured by Oxford Instruments) attached to an SEM, and the atomic ratio was found to be Co:Mn:Mg=51.0:29.1:19.9.

(導電成形体の作製)
ここでは粉体の導電成形体として上記の第2分級工程後の粉体を用いた焼結体を以下のように作製した。第2分級工程後の粉体約5.9gを、内径10mmの円筒形グラファイトセルのシリンダー中で上下のピストンにより90MPa(7.065kN)の圧力を付与した状態として、約1Paの真空雰囲気下で放電プラズマ焼結装置により加熱することによって、直径10mm、高さ約8mmの円柱形状の焼結体を得た。ヒートパターンは、650℃まで昇温、650℃で10分間保持、750℃まで昇温、750℃で10分間保持、放冷とした。
(Preparation of conductive molded body)
Here, a sintered body was produced as a conductive powder compact using the powder after the second classification process described above as follows: Approximately 5.9 g of the powder after the second classification process was placed in a cylindrical graphite cell cylinder with an inner diameter of 10 mm, and heated in a spark plasma sintering apparatus under a vacuum atmosphere of approximately 1 Pa while applying a pressure of 90 MPa (7.065 kN) using upper and lower pistons. This produced a cylindrical sintered body with a diameter of 10 mm and a height of approximately 8 mm. The heating pattern was as follows: the temperature was raised to 650°C, held at 650°C for 10 minutes, raised to 750°C, held at 750°C for 10 minutes, and then allowed to cool.

(異常ネルンスト効果の測定)
上記の導電成形体(焼結体)から、長さ(L)8.269mm、幅(W)1.460mm、厚さ(H)0.624mmの直方体試料を切り出した。図4に、起電力測定用の端子、温度測定用のプローブ取り付け位置と、熱流、磁場の付与方向を模式的に示す。ネルンスト効果測定用試料1の対向する側面中央位置に、起電力測定用の端子2a、2bを導電性エポキシ接着剤で取り付け、電圧計で両端子間に生じる電圧(V)を測定できるようにした。この電圧は異常ネルンスト効果によって生じるものであるので、VANEと表示する。試料1の上面2箇所(符号31、32で示す位置)に5.0mmの間隔(L)をあけて温度測定用プローブを導電性エポキシ接着剤で取り付けてその間の温度差ΔTをモニターできるようにし、Quantum Design社製、物理特性測定システムPPMS装置内で試料長手方向に熱流を生じさせながら、試料の厚さ方向に磁場を付与し、試料の幅方向両端の間に生じる起電力を室温(300K)において測定した。図4中の黒塗り矢印(符号4)が試料中の熱流方向を表す。温度TおよびTが安定した後、試料に磁場を付与し、電圧VANE(V)を測定した。図4中の白抜き矢印(符号5)が磁場の方向を表す。磁場は3Tから-3T、-3Tから3Tの間で掃引した。
下記(1)式によりネルンスト係数SANE(μV/K)を求めた。
ANE(μV/K)=VANE(V)/W/ΔT(K)/L …(1)
ここで、
ANE:試料幅方向両端に生じる起電力(V)、
W:試料の幅方向長さ(mm)、
ΔT:温度プローブ取り付け位置2箇所の温度差(K)、
:2箇所の温度プローブ取り付け位置の試料長手方向距離(mm)、
である。
(Measurement of the anomalous Nernst effect)
A rectangular parallelepiped sample with a length ( L1 ) of 8.269 mm, a width (W) of 1.460 mm, and a thickness (H) of 0.624 mm was cut out from the above-mentioned conductive molded body (sintered body). Figure 4 shows the attachment positions of the terminals for measuring electromotive force and the probes for measuring temperature, as well as the directions of heat flow and magnetic field application. Terminals 2a and 2b for measuring electromotive force were attached to the center of opposite sides of the Nernst effect measurement sample 1 with conductive epoxy adhesive, so that the voltage (V) generated between the two terminals could be measured with a voltmeter. This voltage is generated by the anomalous Nernst effect, and is therefore designated as V ANE . Two temperature measurement probes were attached to the top surface of sample 1 at two locations (positions indicated by reference numerals 31 and 32) with a 5.0 mm gap (L 2 ) between them using conductive epoxy adhesive, allowing the temperature difference ΔT between them to be monitored. A magnetic field was applied in the thickness direction of the sample while a heat flow was generated in the longitudinal direction of the sample in a Quantum Design Physical Property Measurement System (PPMS) device. The electromotive force generated between both ends of the sample in the width direction was measured at room temperature (300 K). The solid arrow (reference numeral 4) in Figure 4 indicates the direction of heat flow in the sample. After temperatures T1 and T2 stabilized, a magnetic field was applied to the sample, and the voltage V ANE (V) was measured. The open arrow (reference numeral 5) in Figure 4 indicates the direction of the magnetic field. The magnetic field was swept between 3 T and -3 T and between -3 T and 3 T.
The Nernst coefficient S ANE (μV/K) was calculated using the following formula (1).
S ANE (μV/K)=V ANE (V)/W/ΔT(K)/L 2 ...(1)
where:
V ANE : electromotive force (V) generated at both ends of the sample in the width direction,
W: width of sample (mm),
ΔT: temperature difference between the two temperature probe mounting positions (K),
L2 : Distance in the longitudinal direction of the sample between the two temperature probe attachment positions (mm),
is.

図5に、ネルンスト係数の測定結果を示す。温度300Kにおけるネルンスト係数は6.68μV/Kに達した。本発明に従う金属間化合物CoMnGaを主成分とする粉体の導電成形体は、単結晶CoMnGaと同等以上のネルンスト係数を呈することが確認された。 The measurement results of the Nernst coefficient are shown in Figure 5. The Nernst coefficient at a temperature of 300 K reached 6.68 μV/K. It was confirmed that the conductive compact of powder containing the intermetallic compound Co2MnGa as the main component according to the present invention exhibits a Nernst coefficient equal to or greater than that of single crystal Co2MnGa .

1 ネルンスト効果測定用試料
2a、2b 起電力測定端子
31、32 測温位置
4 試料中の熱流方向
5 磁場の方向
1 Nernst effect measurement sample 2a, 2b electromotive force measurement terminals 31, 32 temperature measurement positions 4 heat flow direction in sample 5 magnetic field direction

Claims (20)

金属間化合物CoMnGaを主成分とする粉体であって、当該粉体に占めるCo MnGa相の割合が90質量%以上であり、レーザー回折・散乱法による体積基準の粒度分布において、累積50%粒子径D50が1~150μm、累積90%粒子径D90が250μm以下であるCo-Mn-Ga系合金粉体。 A Co-Mn-Ga-based alloy powder containing an intermetallic compound Co 2 MnGa as a main component , in which the proportion of the Co 2 MnGa phase in the powder is 90 mass % or more, and in a volume-based particle size distribution measured by a laser diffraction/scattering method, the cumulative 50% particle diameter D50 is 1 to 150 μm and the cumulative 90% particle diameter D90 is 250 μm or less. Co、MnおよびGaからなる溶融金属を凝固させ、金属間化合物CoMnGaを主成分とし、Co MnGa相の割合が90質量%以上であるCo-Mn-Ga系合金塊を得る合金塊作製工程、
前記Co-Mn-Ga系合金塊を粉砕することにより粉体を得る粉砕工程、
を有する請求項1に記載のCo-Mn-Ga系合金粉体の製造方法。
an alloy ingot preparation step of solidifying a molten metal composed of Co, Mn, and Ga to obtain a Co—Mn—Ga-based alloy ingot containing an intermetallic compound Co 2 MnGa as a main component and having a proportion of the Co 2 MnGa phase of 90 mass % or more ;
a pulverization step of pulverizing the Co—Mn—Ga-based alloy ingot to obtain a powder;
2. The method for producing Co—Mn—Ga based alloy powder according to claim 1, wherein the
前記粉砕工程で得られた粉体を篩により分級する分級工程、
を更に有する請求項2に記載のCo-Mn-Ga系合金粉体の製造方法。
a classification step of classifying the powder obtained in the pulverization step using a sieve;
3. The method for producing Co-Mn-Ga based alloy powder according to claim 2, further comprising:
金属間化合物CoMnGaを主成分とし、Co MnGa相の割合が90質量%以上である粉体の導電成形体。 A conductive compact of powder containing an intermetallic compound Co 2 MnGa as a main component , with the proportion of the Co 2 MnGa phase being 90 mass % or more . 前記金属間化合物CoMnGaを主成分とし、Co MnGa相の割合が90質量%以上である粉体は、レーザー回折・散乱法による体積基準の粒度分布において、累積50%粒子径D50が1~150μm、累積90%粒子径D90が250μm以下のものである、請求項4に記載の導電成形体。 The powder, which is mainly composed of the intermetallic compound Co 2 MnGa and has a ratio of 90 mass% or more of the Co 2 MnGa phase , has a cumulative 50% particle diameter D50 of 1 to 150 μm and a cumulative 90% particle diameter D90 of 250 μm or less in a volume-based particle size distribution measured by a laser diffraction/scattering method. The conductive molded body according to claim 4. 金属間化合物CoMnGaを主成分とし、Co MnGa相の割合が90質量%以上である粉体の焼結体である、請求項4または5に記載の導電成形体。 6. The conductive molded body according to claim 4, which is a sintered body of powder containing the intermetallic compound Co2MnGa as a main component , with the proportion of the Co2MnGa phase being 90 mass % or more . 温度300Kにおいて6.0μV/K以上のネルンスト係数を呈する請求項4~6のいずれか1項に記載の導電成形体。 The conductive molded article according to any one of claims 4 to 6, exhibiting a Nernst coefficient of 6.0 μV/K or greater at a temperature of 300 K. 金属間化合物CoMnGaを主成分とし、Co MnGa相の割合が90質量%以上である粉体を、焼結させることにより、導電成形体を得る焼結工程、を有する導電成形体の製造方法。 A method for producing a conductive molded body, comprising: a sintering step of sintering a powder containing an intermetallic compound Co 2 MnGa as a main component , with the proportion of the Co 2 MnGa phase being 90 mass % or more, to obtain a conductive molded body. 前記金属間化合物CoMnGaを主成分とし、Co MnGa相の割合が90質量%以上である粉体は、レーザー回折・散乱法による体積基準の粒度分布において、累積50%粒子径D50が1~150μm、累積90%粒子径D90が250μm以下のものである、請求項8に記載の導電成形体の製造方法。 The powder, which is mainly composed of the intermetallic compound Co 2 MnGa and has a ratio of 90 mass% or more of the Co 2 MnGa phase , has a cumulative 50% particle diameter D50 of 1 to 150 μm and a cumulative 90% particle diameter D90 of 250 μm or less in a volume-based particle size distribution measured by a laser diffraction/scattering method. The method for producing a conductive molded body according to claim 8. 請求項4~7のいずれか1項に記載の導電成形体を用いた熱電変換素子。 A thermoelectric conversion element using the conductive molded article described in any one of claims 4 to 7. 金属間化合物CoMnGaからなる粉体であって、レーザー回折・散乱法による体積基準の粒度分布において、累積50%粒子径D50が1~150μm、累積90%粒子径D90が250μm以下であるCo-Mn-Ga系合金粉体。 A Co-Mn-Ga alloy powder is a powder made of an intermetallic compound Co 2 MnGa, and has a cumulative 50% particle diameter D50 of 1 to 150 μm and a cumulative 90% particle diameter D90 of 250 μm or less in a volume-based particle size distribution measured by a laser diffraction/scattering method. Co、MnおよびGaからなる溶融金属を凝固させ、金属間化合物CoMnGaからなるCo-Mn-Ga系合金塊を得る合金塊作製工程、
前記Co-Mn-Ga系合金塊を粉砕することにより粉体を得る粉砕工程、
を有する請求項11に記載のCo-Mn-Ga系合金粉体の製造方法。
an alloy ingot preparation step of solidifying a molten metal consisting of Co, Mn, and Ga to obtain a Co—Mn—Ga-based alloy ingot consisting of an intermetallic compound Co 2 MnGa;
a pulverization step of pulverizing the Co—Mn—Ga-based alloy ingot to obtain a powder;
The method for producing Co-Mn-Ga based alloy powder according to claim 11 , which comprises:
前記粉砕工程で得られた粉体を篩により分級する分級工程、
を更に有する請求項12に記載のCo-Mn-Ga系合金粉体の製造方法。
a classification step of classifying the powder obtained in the pulverization step using a sieve;
The method for producing Co-Mn-Ga based alloy powder according to claim 12 , further comprising:
金属間化合物CoMnGaからなる粉体の導電成形体。 A conductive compact of powder made of the intermetallic compound Co 2 MnGa. 前記金属間化合物CoMnGaからなる粉体は、レーザー回折・散乱法による体積基準の粒度分布において、累積50%粒子径D50が1~150μm、累積90%粒子径D90が250μm以下のものである、請求項14に記載の導電成形体。 The powder made of the intermetallic compound Co 2 MnGa has a cumulative 50% particle diameter D50 of 1 to 150 μm and a cumulative 90% particle diameter D90 of 250 μm or less in a volume-based particle size distribution measured by a laser diffraction/scattering method. 金属間化合物CoMnGaからなる粉体の焼結体である、請求項14または15に記載の導電成形体。 The conductive molded body according to claim 14 or 15 , which is a sintered body of powder made of the intermetallic compound Co 2 MnGa. 温度300Kにおいて6.0μV/K以上のネルンスト係数を呈する請求項1416のいずれか1項に記載の導電成形体。 The conductive molded article according to any one of claims 14 to 16 , which exhibits a Nernst coefficient of 6.0 µV/K or more at a temperature of 300K. 金属間化合物CoMnGaからなる粉体を、焼結させることにより、導電成形体を得る焼結工程、を有する導電成形体の製造方法。 A method for producing a conductive compact, comprising: a sintering step of sintering powder made of an intermetallic compound Co 2 MnGa to obtain a conductive compact. 前記金属間化合物CoMnGaからなる粉体は、レーザー回折・散乱法による体積基準の粒度分布において、累積50%粒子径D50が1~150μm、累積90%粒子径D90が250μm以下のものである、請求項18に記載の導電成形体の製造方法。 The powder made of the intermetallic compound Co 2 MnGa has a cumulative 50% particle diameter D50 of 1 to 150 μm and a cumulative 90% particle diameter D90 of 250 μm or less in a volume - based particle size distribution measured by a laser diffraction/scattering method. 請求項1417のいずれか1項に記載の導電成形体を用いた熱電変換素子。 A thermoelectric conversion element using the conductive molded article according to any one of claims 14 to 17 .
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