JPH0524972B2 - - Google Patents
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- Publication number
- JPH0524972B2 JPH0524972B2 JP4854487A JP4854487A JPH0524972B2 JP H0524972 B2 JPH0524972 B2 JP H0524972B2 JP 4854487 A JP4854487 A JP 4854487A JP 4854487 A JP4854487 A JP 4854487A JP H0524972 B2 JPH0524972 B2 JP H0524972B2
- Authority
- JP
- Japan
- Prior art keywords
- temperature
- vanadium
- type
- germanium
- vge
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Fee Related
Links
- -1 vanadium digermanide Chemical compound 0.000 claims description 13
- 229910052732 germanium Inorganic materials 0.000 claims description 12
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 claims description 10
- 239000000203 mixture Substances 0.000 claims description 6
- 238000004519 manufacturing process Methods 0.000 claims description 4
- 229910052720 vanadium Inorganic materials 0.000 claims description 4
- LEONUFNNVUYDNQ-UHFFFAOYSA-N vanadium atom Chemical compound [V] LEONUFNNVUYDNQ-UHFFFAOYSA-N 0.000 claims 1
- 238000006243 chemical reaction Methods 0.000 description 15
- 150000001875 compounds Chemical class 0.000 description 12
- 239000000843 powder Substances 0.000 description 8
- 239000000463 material Substances 0.000 description 7
- 239000000126 substance Substances 0.000 description 6
- 238000004458 analytical method Methods 0.000 description 5
- 229910019974 CrSi Inorganic materials 0.000 description 4
- 239000013078 crystal Substances 0.000 description 4
- 230000000704 physical effect Effects 0.000 description 4
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 3
- 230000000052 comparative effect Effects 0.000 description 3
- 229910052802 copper Inorganic materials 0.000 description 3
- 239000010949 copper Substances 0.000 description 3
- 150000002291 germanium compounds Chemical class 0.000 description 3
- 230000005291 magnetic effect Effects 0.000 description 3
- 239000012071 phase Substances 0.000 description 3
- 239000002994 raw material Substances 0.000 description 3
- 229910052723 transition metal Inorganic materials 0.000 description 3
- 150000003624 transition metals Chemical class 0.000 description 3
- GPPXJZIENCGNKB-UHFFFAOYSA-N vanadium Chemical compound [V]#[V] GPPXJZIENCGNKB-UHFFFAOYSA-N 0.000 description 3
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- 229910001006 Constantan Inorganic materials 0.000 description 2
- GRYLNZFGIOXLOG-UHFFFAOYSA-N Nitric acid Chemical compound O[N+]([O-])=O GRYLNZFGIOXLOG-UHFFFAOYSA-N 0.000 description 2
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 238000002441 X-ray diffraction Methods 0.000 description 2
- RQNKKHCCPWBTIM-UHFFFAOYSA-N [V].[Ge] Chemical class [V].[Ge] RQNKKHCCPWBTIM-UHFFFAOYSA-N 0.000 description 2
- 239000011572 manganese Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 229910017604 nitric acid Inorganic materials 0.000 description 2
- 238000011160 research Methods 0.000 description 2
- 229910000809 Alumel Inorganic materials 0.000 description 1
- 229910005329 FeSi 2 Inorganic materials 0.000 description 1
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 description 1
- PWHULOQIROXLJO-UHFFFAOYSA-N Manganese Chemical compound [Mn] PWHULOQIROXLJO-UHFFFAOYSA-N 0.000 description 1
- 229910016006 MoSi Inorganic materials 0.000 description 1
- 229910008484 TiSi Inorganic materials 0.000 description 1
- TZHYBRCGYCPGBQ-UHFFFAOYSA-N [B].[N] Chemical compound [B].[N] TZHYBRCGYCPGBQ-UHFFFAOYSA-N 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 238000001479 atomic absorption spectroscopy Methods 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 239000006227 byproduct Substances 0.000 description 1
- RKTYLMNFRDHKIL-UHFFFAOYSA-N copper;5,10,15,20-tetraphenylporphyrin-22,24-diide Chemical compound [Cu+2].C1=CC(C(=C2C=CC([N-]2)=C(C=2C=CC=CC=2)C=2C=CC(N=2)=C(C=2C=CC=CC=2)C2=CC=C3[N-]2)C=2C=CC=CC=2)=NC1=C3C1=CC=CC=C1 RKTYLMNFRDHKIL-UHFFFAOYSA-N 0.000 description 1
- 238000007872 degassing Methods 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 230000005292 diamagnetic effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005307 ferromagnetism Effects 0.000 description 1
- YBMRDBCBODYGJE-UHFFFAOYSA-N germanium oxide Inorganic materials O=[Ge]=O YBMRDBCBODYGJE-UHFFFAOYSA-N 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 239000001257 hydrogen Substances 0.000 description 1
- 229910052739 hydrogen Inorganic materials 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 230000003993 interaction Effects 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 229910052748 manganese Inorganic materials 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 150000002738 metalloids Chemical group 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- PVADDRMAFCOOPC-UHFFFAOYSA-N oxogermanium Chemical compound [Ge]=O PVADDRMAFCOOPC-UHFFFAOYSA-N 0.000 description 1
- 239000002907 paramagnetic material Substances 0.000 description 1
- 230000005408 paramagnetism Effects 0.000 description 1
- 230000000737 periodic effect Effects 0.000 description 1
- PXXKQOPKNFECSZ-UHFFFAOYSA-N platinum rhodium Chemical compound [Rh].[Pt] PXXKQOPKNFECSZ-UHFFFAOYSA-N 0.000 description 1
- 238000000634 powder X-ray diffraction Methods 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 230000027756 respiratory electron transport chain Effects 0.000 description 1
- 238000007789 sealing Methods 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 229910021332 silicide Inorganic materials 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
- 150000003377 silicon compounds Chemical class 0.000 description 1
- 239000000377 silicon dioxide Substances 0.000 description 1
- 238000003746 solid phase reaction Methods 0.000 description 1
- 238000002798 spectrophotometry method Methods 0.000 description 1
- 239000002887 superconductor Substances 0.000 description 1
- 238000003786 synthesis reaction Methods 0.000 description 1
- 230000002194 synthesizing effect Effects 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
Landscapes
- Powder Metallurgy (AREA)
Description
本発明はC40型の結晶構造をもつ新規な導電性
バナジウム二ゲルマニウム化物(化学組成VGe2)
とその製造方法に関する。
従来の技術
遷移金属の珪化物やゲルマニウム化物には、電
気伝導度の高い金属的性質を示すものや、半導
体、半金属、超伝導体などの特徴ある性質を示す
ものが多く、又磁気的にもパウリ常磁性、ヘリカ
ル磁性、弱い強磁性、反磁性など多彩な性質を示
すことから、これまでに結晶化学的、物理的な興
味と相俟つて広範な基礎研究及び応用研究がなさ
れてきた。例えば半導体的な性質を示すCrSi2、
FeSi2などは低い抵抗率と大きな熱電能を有して
おり熱電変換材料として使用されている。
ところでゲルマニウム化物にも同様な性質が期
待され、更に優れた性質を備えた新規化合物が見
出される可能性がある。即ちゲルマニウムは珪素
に比べて電気伝導度が大きく、又電子と正孔の移
動度も大きいので、遷移金属と化合物を作ること
により珪素化合物に比して電気伝導度の高いもの
が得られる可能性があり、又エネルギーバンドギ
ヤツプの調整が容易にできると考えられ、いろい
ろな特性を有する化合物を多様に設計し得るもの
と予測される。そこで現在多くのゲルマニウム化
物について研究が行われている。
例えばバナジウムのゲルマニウム化物として
は、これまで4つの相が報告されている。H.
Holleck等によつて開示されたV3Ge(Monatsh
Chem.、94、473(1963))及びV5Ge3(Monatsh
Chem.、94、497(1963))、H.Vollenkle等の
V11Ge8(Monatsh Chem.、95、1544(1964))及
びV17Ge31(Z.Krist.、124、9(1967))である。
これらはいずれもGe/V比が0.3〜2の原料粉末
を真空中、600〜1000℃の温度条件で処理するこ
とによつて製造されるものであるが、これまでV
とGeの比が1:2の定比組成を有するものは知
られていない。
遷移金属−ゲルマニウム化物においてはゲルマ
ニウムの割合が大きくなるにつれてバンドギヤツ
プが大きくなるため、従来知られていない熱的・
電気的性質が得られるものと考えられるが、遷移
金属のゲルマニウム化物では1:2の定比組成を
有するものを合成することが難しく、特にバナジ
ウム−ゲルマニウム系ではゲルマニウム含有率の
高い相など生成自由エネルギーが大きくなるた
め、常圧下ではゲルマニウム化物の生成が不可能
であつた。
発明の目的
本発明は、従来知られているものよりゲルマニ
ウムの比率が高い、新規な導電性バナジウム二ゲ
ルマニウム化物及びその合成方法を提供するもの
である。
発明の構成
本発明はC40型構造を有し、組成式VGe2で表
される新規な導電性バナジウム二ゲルマニウム化
物である。このバナジウム二ゲルマニウム化物
は、実施例において詳細に説明するように単一の
化合物であつて、一つの物性を示す。C40型構造
はZeitschrift fu¨r Kristallogrophieの
Erga¨nzungsbandのStrukturberichteに登録され
た結晶格子型番号で表わされた格子型で、CrSi2
型とも言う。これは金属原子Tとメタロイド原子
Xが密にパツキングしたTX2原子平面が一定の
規則で積重なつて構成された六方晶系空間群D4 6
(P6222)の構造である。
二珪化物、二ゲルマニウム化物の中では最も緻
密な構造である。
したがつて、本発明で言うC40型構造を有する
バナジウム二ゲルマニウム化物は六方晶系で空間
群D4 6(P6222)の結晶格子型を有する化合物であ
る。
本発明のC40型構造の導電性バナジウム二ゲル
マニウム化物は、バナジウムとゲルマニウムを高
温高圧下で反応させて合成する。即ち第二の発明
は、バナジウムとゲルマニウムを1:1〜1:3
のモル比で混合し、圧力1GPa以上、温度600〜
1300℃の条件下で反応させることを特徴とする、
C40型構造を有する導電性バナジウム二ゲルマニ
ウム化物の製造方法である。原料であるバナジウ
ムとゲルマニウムは、高純度のものを用いるのが
望ましい。特に酸化物が不純物として存在すると
ゲルマニウム酸化物が生成して分離が困難になる
ので、酸化物が極力少ないものを使用する必要が
ある。場合によつては水素などで還元処理を行つ
た原料を用いることが好ましい。反応温度が600
℃より低いとゲルマニウムが溶解せず反応が起こ
らない。又、1300℃を越えると蒸発するので、固
相反応に近い状態で反応させるために1GPa以上、
好ましくは3GPa以上で、温度600〜1300℃の条件
が必要である。尚、反応温度が低いと一部ゲルマ
ニウムが未反応のまま残存し、又高温であると一
部V5Ge3の生成が認められるようになるので、
VGe2の単一相を得るためには850〜1250℃の温度
範囲が望ましい。これら未反応物や副生成物は硝
酸などで処理することにより除去することも可能
である。
高温高圧合成には例えばベルト型高圧装置な
ど、所定の反応に必要な時間中、前記条件を保持
し得るような高圧、高温発生装置を用いる。
TG2型化合物にはTX2平面の積重り方の違いに
よりC54型(TiSi2型、斜方晶系)、C40型(CrSi2
型、六方晶系)C11b型(MoSi2型、正方晶系)の
いずれかになるが、周期律表第属元素の二ゲル
マニウム化物はC40型になると考えられている。
本発明の高温高圧反応で製造されるバナジウム
二ゲルマニウム化物は全てC40型のVGe2である。
実施例
実施例 1
純度99.99%以上のV粉末及びGe粉末を窒素中
ほぼ1:2のモル比で充分混合した後、4.0t/cm2
の荷重をかけて5φ×3mmの円板状に成形した。
これを窒素硼素の反応容器に充填し、ベルト型高
圧装置により5.5GPa、850℃の条件で2時間処理
を行つた。反応終了後、加熱電力を遮断して急冷
した。
得られた化合物は、暗灰色を呈しており、原子
吸光分析及び吸光光度分析の結果VGe2であるこ
とが確認された。
表1は、実施例1で得られたバナジウム二ゲル
マニウム化物の粉末X線回析の結果を示したもの
である。この回折図形は、VSi2、CrSi2のものと
類似しており、各ピークの回折強度もほぼ一致し
C40型構造であることを示している。又六方晶
系、空間群D4 6に属し、格子定数a=0.4806nm、
c=0.6634nmとして決定された。
The present invention is a novel conductive vanadium digermanide with a C40 type crystal structure (chemical composition VGe 2 ).
and its manufacturing method. Prior Art Many of the silicides and germanides of transition metals exhibit metallic properties with high electrical conductivity, as well as characteristic properties such as semiconductors, semimetals, and superconductors. Because magnets exhibit a wide variety of properties, including Pauli paramagnetism, helical magnetism, weak ferromagnetism, and diamagnetic properties, a wide range of basic and applied research has been conducted on them, with interest in crystal chemistry and physics. For example, CrSi 2 , which exhibits semiconducting properties,
FeSi 2 and other materials have low resistivity and large thermoelectric power, and are used as thermoelectric conversion materials. By the way, similar properties are expected for germanium compounds, and there is a possibility that new compounds with even better properties will be discovered. In other words, germanium has higher electrical conductivity than silicon, and also has higher mobility of electrons and holes, so it is possible that by creating a compound with a transition metal, it is possible to obtain something with higher electrical conductivity than silicon compounds. It is also believed that the energy band gap can be easily adjusted, and it is predicted that a wide variety of compounds with various properties can be designed. Therefore, research is currently being conducted on many germanium compounds. For example, four phases of vanadium germanium compounds have been reported so far. H.
V 3 Ge (Monatsh
Chem., 94, 473 (1963)) and V 5 Ge 3 (Monatsh
Chem., 94, 497 (1963)), H. Vollenkle et al.
V 11 Ge 8 (Monatsh Chem., 95, 1544 (1964)) and V 17 Ge 31 (Z. Krist., 124, 9 (1967)).
All of these are manufactured by processing raw material powder with a Ge/V ratio of 0.3 to 2 in a vacuum at a temperature of 600 to 1000°C, but until now V
There is no known material having a stoichiometric composition in which the ratio of Ge and Ge is 1:2. In transition metal-germanium compounds, the band gap increases as the proportion of germanium increases, so a previously unknown thermal
It is thought that electrical properties can be obtained, but it is difficult to synthesize transition metal germanides with a stoichiometric ratio of 1:2, and especially in the vanadium-germanium system, phases with a high germanium content cannot be formed freely. Because of the increased energy, it was impossible to generate germanium compounds under normal pressure. OBJECTS OF THE INVENTION The present invention provides a novel conductive vanadium digermanide having a higher proportion of germanium than those conventionally known, and a method for synthesizing the same. Structure of the Invention The present invention is a novel conductive vanadium digermanide having a C40 type structure and represented by the compositional formula VGe 2 . This vanadium digermanide is a single compound and exhibits one physical property, as will be explained in detail in Examples. The C40 type structure is of Zeitschrift fu¨r Kristallogrophie.
CrSi 2
Also called type. This is a hexagonal space group D 4 6 consisting of TX 2 atomic planes stacked with a certain regularity, in which metal atoms T and metalloid atoms X are tightly packed.
The structure is (P6 2 22). It has the most dense structure among disilicides and digermanides. Therefore, the vanadium digermanide having the C40 type structure referred to in the present invention is a compound having a hexagonal system and a crystal lattice type of space group D 4 6 (P6 2 22). The conductive vanadium digermanide having a C40 type structure of the present invention is synthesized by reacting vanadium and germanium under high temperature and high pressure. That is, in the second invention, vanadium and germanium are mixed in a ratio of 1:1 to 1:3.
Mix at a molar ratio of , pressure 1GPa or more, temperature 600~
Characterized by reacting under conditions of 1300℃,
This is a method for producing conductive vanadium digermanide having a C40 type structure. It is desirable to use highly purified vanadium and germanium as raw materials. In particular, if an oxide is present as an impurity, germanium oxide is generated and separation becomes difficult, so it is necessary to use a material containing as little oxide as possible. In some cases, it is preferable to use a raw material that has been subjected to a reduction treatment with hydrogen or the like. Reaction temperature is 600
If the temperature is lower than ℃, germanium will not dissolve and no reaction will occur. Also, since it will evaporate if the temperature exceeds 1300℃, the temperature should be set at 1GPa or higher to allow the reaction to occur in a state close to that of a solid phase reaction.
Preferably, conditions of 3 GPa or higher and a temperature of 600 to 1300°C are required. Note that if the reaction temperature is low, some germanium will remain unreacted, and if the reaction temperature is high, some V 5 Ge 3 will be produced.
A temperature range of 850-1250°C is desirable to obtain a single phase of VGe2 . These unreacted substances and by-products can also be removed by treatment with nitric acid or the like. For high-temperature, high-pressure synthesis, a high-pressure and high-temperature generating device such as a belt-type high-pressure device that can maintain the above-mentioned conditions for the time required for a predetermined reaction is used. TG 2 type compounds include C54 type (TiSi 2 type, orthorhombic system) and C40 type (CrSi 2 type) depending on the stacking method of the TX 2 planes.
Type, hexagonal system) C11 b type (MoSi 2 type, tetragonal system), but digermanides of group elements of the periodic table are thought to be C40 type. The vanadium digermanium compound produced by the high temperature and high pressure reaction of the present invention is all C40 type VGe 2 . Examples Example 1 After thoroughly mixing V powder and Ge powder with a purity of 99.99% or more in nitrogen at a molar ratio of approximately 1:2, 4.0 t/cm 2
It was molded into a disc shape of 5φ x 3mm by applying a load of .
This was filled into a nitrogen-boron reaction vessel, and treated for 2 hours at 5.5 GPa and 850°C using a belt-type high-pressure device. After the reaction was completed, the heating power was cut off and the mixture was rapidly cooled. The obtained compound had a dark gray color and was confirmed to be VGe 2 by atomic absorption spectrometry and spectrophotometric analysis. Table 1 shows the results of powder X-ray diffraction of the vanadium digermanium compound obtained in Example 1. This diffraction pattern is similar to that of VSi 2 and CrSi 2 , and the diffraction intensity of each peak is also almost the same.
This indicates a C40 type structure. It also has a hexagonal crystal system, belongs to space group D 4 6 , and has a lattice constant a = 0.4806 nm.
It was determined that c=0.6634 nm.
【表】
第1図、第2図にそれぞれ実施例1で得られた
VGe2の抵抗率の温度依存性と熱電能の温度依存
性とを示した。これらの図によれば抵抗率は金属
的で1.5×10-4〜4×10-4Ωcmの範囲で温度と共に
直線的に増加するが、その増加率は1.1×10-6Ω
cm/Kである。又熱電能は80〜300Kの範囲で−
4〜−5μV/Kと、通常熱電対に用いられる白金
ロジウム、クロメルアルメル、コンスタンタンな
どの合金と比較して小さな値を示し、かつ温度変
化が少ないことが特徴的である。
第3図はVGe2の磁化率の温度変化を示したも
のである。磁化率は80K以上では特別な相互作用
を示さず、小さな磁化率を有しており、キユー
リ・ワイス則に従う常磁性体であることがわかつ
た。ちなみに有効ポーア磁子数及びキユーリ・ワ
イス温度はそれぞれ0.82μB及び−32Kと定まつ
た。この値は1個の不対電子をもつと考えた際の
値、1.73μBに比べて小さい。これは、V−Ge結合
距離が2.61Aであり、原子半径の和である2.64A
より短くなつていることから、GeからVへの電
子移動によつてスピンが一部相殺された結果と考
えれば説明できる。
実施例 2
反応条件を4GPa、1000℃、1時間とする以外
は実施例1と同様にして処理を行つた。得られた
化合物は化学分析及びX線回折の結果、実施例1
と同じC40型のVGe2であり、同一の物性を示し
た。
実施例 3
反応条件を4GPa、800℃、2時間とする以外は
実施例1と同様にして処理を行つた。得られた化
合物は、分析の結果VGe2の他に微量の未反応Ge
が存在することが明らかになつた。そこでこれを
1規定硝酸で処理しGeを除去した。得られた試
料は実施例1と同じC40型のVGe2であり、同一
の物性を示すことが確認された。
実施例 4
反応条件を5.5GPa、1100℃、30分とする以外
は実施例1と同様にして処理を行つた。得られた
化合物は化学分析及びX線回折の結果、実施例1
と同じC40型のVGe2であり、同一の物性を示し
た。
比較例 1
V粉末及びGe粉末をほぼ2:1のモル比で充
分混合した後シリカチユーブに入れ、10-3mmHg
で脱気後溶封し、880℃の温度条件下で40時間反
応を行つた。得られた試料は化学分析及び粉末X
線回折の結果、Mn11Si19型構造のV17Ge31と未反
応Geであつた。
比較例 2
V粉末及びGe粉末をほぼ1:1のモル比で混
合し比較例1と同様に真空中900℃の温度条件下
で20時間反応を行つた。得られた試料は分析の結
果、V17Ge31とV11Ge8であつた。
効 果
本発明は新規かつ有用なC40型構造のバナジウ
ム二ゲルマニウム化物を提供し、併せてその製造
方法を確立したものである。この化合物は実施例
に示されたとおり熱電能が小さく、外気の変化特
に熱や雰囲気に対して極めて安定した電気的抵抗
特性を備えることから、超精密抵抗、電流制御用
抵抗材料などとして幅広い用途開発の期待できる
物質である。例えば現在一般に電流制御用抵抗体
としては体積抵抗率50μΩcm、抵抗値の温度変化
率2×10-5Ωcm/Kのコンスタンタン線が多用さ
れているが、銅に対する熱起電力が40μVと大き
く、超精密抵抗材料としてはむしろ体積抵抗率44
±3μΩcm、抵抗値の温度変化率(5〜100)×
10-6Ωcm/K、銅に対する熱起電力2μVと、より
優れたマンガン線が標準抵抗などに利用されてい
る。しかし本発明で得られた新規化合物VG2は、
体積抵抗率1.5×10-4Ωcm、抵抗値の温度変化率は
1.1×10-6Ωcm/K、銅に対する熱起電力が−4〜
−5μVでしかもその温度依存性が小さいので、よ
り優れた低抗体としての利用が期待され、産業上
極めて有用である。[Table] Figures 1 and 2 show the results obtained in Example 1, respectively.
The temperature dependence of resistivity and the temperature dependence of thermopower of VGe 2 are shown. According to these figures, resistivity is metallic and increases linearly with temperature in the range of 1.5 × 10 -4 to 4 × 10 -4 Ωcm, but the rate of increase is 1.1 × 10 -6 Ω.
cm/K. The thermoelectric power is - in the range of 80 to 300K.
It exhibits a small value of 4 to -5 μV/K compared to alloys such as platinum-rhodium, chromel-alumel, and constantan that are normally used in thermocouples, and is characterized by small temperature changes. Figure 3 shows the change in magnetic susceptibility of VGe 2 with temperature. It was found that the material exhibits no special interaction above 80K, has a small magnetic susceptibility, and is a paramagnetic material that follows the Cuyrie-Weiss law. By the way, the effective Pohr magneton number and the Cuyuri-Weiss temperature were determined to be 0.82μ B and -32K, respectively. This value is smaller than 1.73μ B , which is the value when considering one unpaired electron. This means that the V-Ge bond distance is 2.61A, and the sum of the atomic radii is 2.64A.
Since it is shorter, this can be explained by considering that the spin is partially canceled out by electron transfer from Ge to V. Example 2 The treatment was carried out in the same manner as in Example 1, except that the reaction conditions were 4 GPa, 1000° C., and 1 hour. As a result of chemical analysis and X-ray diffraction, the obtained compound was found to be Example 1.
It is the same C40 type VGe 2 and showed the same physical properties. Example 3 The treatment was carried out in the same manner as in Example 1, except that the reaction conditions were 4 GPa, 800° C., and 2 hours. As a result of analysis, the obtained compound contained VGe 2 and a trace amount of unreacted Ge.
It has become clear that there is. Therefore, this was treated with 1N nitric acid to remove Ge. It was confirmed that the obtained sample was the same C40 type VGe 2 as in Example 1 and exhibited the same physical properties. Example 4 The treatment was carried out in the same manner as in Example 1, except that the reaction conditions were 5.5 GPa, 1100° C., and 30 minutes. As a result of chemical analysis and X-ray diffraction, the obtained compound was found to be Example 1.
It is the same C40 type VGe 2 and showed the same physical properties. Comparative Example 1 V powder and Ge powder were thoroughly mixed at a molar ratio of approximately 2:1, then placed in a silica tube and heated to 10 -3 mmHg.
After degassing and sealing, the reaction was carried out at a temperature of 880°C for 40 hours. The obtained sample was subjected to chemical analysis and powder
As a result of line diffraction, it was found to be V 17 Ge 31 with a Mn 11 Si 19 type structure and unreacted Ge. Comparative Example 2 V powder and Ge powder were mixed at a molar ratio of approximately 1:1, and as in Comparative Example 1, a reaction was carried out in vacuum at a temperature of 900° C. for 20 hours. Analysis of the obtained sample revealed that it was V 17 Ge 31 and V 11 Ge 8 . Effects The present invention provides a novel and useful vanadium digermanide having a C40 type structure, and also establishes a method for producing the same. As shown in the examples, this compound has low thermoelectric power and has extremely stable electrical resistance characteristics against changes in the outside air, especially heat and atmosphere, so it has a wide range of applications such as ultra-precision resistors and resistance materials for current control. This is a promising substance for development. For example, constantan wire with a volume resistivity of 50 μΩcm and a temperature change rate of resistance value of 2 × 10 -5 Ωcm/K is currently widely used as a resistor for current control, but the thermoelectromotive force against copper is as large as 40 μV, As a precision resistance material, the volume resistivity is rather 44.
±3μΩcm, temperature change rate of resistance value (5 to 100) ×
10 -6 Ωcm/K, thermal electromotive force of 2 μV compared to copper, and superior manganese wire is used for standard resistors. However, the new compound VG 2 obtained by the present invention is
Volume resistivity is 1.5×10 -4 Ωcm, and the temperature change rate of resistance is
1.1×10 -6 Ωcm/K, thermoelectromotive force against copper is -4~
-5 μV and its temperature dependence is small, so it is expected to be used as a superior low-voltage antibody and is extremely useful industrially.
第1図は、本発明のC40型構造を有するVGe2
抵抗率を測定結果示すグラフ、第2図及び第3図
は同じく熱電能及び磁化率の測定結果を示すグラ
フである。
Figure 1 shows VGe 2 having a C40 type structure according to the present invention.
The graphs showing the results of measuring resistivity, and FIGS. 2 and 3, are also graphs showing the results of measuring thermoelectric power and magnetic susceptibility.
Claims (1)
導電性バナジウム二ゲルマニウム化物。 2 バナジウムとゲルマニウムを1:1〜1:3
のモル比で混合し、圧力1GPa以上、温度600〜
1300℃の条件下で反応させることを特徴とする、
C40型構造を有する組成式VGe2の導電性バナジ
ウム二ゲルマニウム化物の製造方法。[Claims] 1. A conductive vanadium digermanide having a C40 type structure and represented by the compositional formula VGe 2 . 2 Vanadium and germanium 1:1 to 1:3
Mix at a molar ratio of , pressure 1GPa or more, temperature 600~
Characterized by reacting under conditions of 1300℃,
A method for producing conductive vanadium digermanide having a composition formula VGe 2 and having a C40 type structure.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4854487A JPS63216940A (en) | 1987-03-03 | 1987-03-03 | Vanadium digermanium compound and its manufacturing method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4854487A JPS63216940A (en) | 1987-03-03 | 1987-03-03 | Vanadium digermanium compound and its manufacturing method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63216940A JPS63216940A (en) | 1988-09-09 |
| JPH0524972B2 true JPH0524972B2 (en) | 1993-04-09 |
Family
ID=12806310
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4854487A Granted JPS63216940A (en) | 1987-03-03 | 1987-03-03 | Vanadium digermanium compound and its manufacturing method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS63216940A (en) |
-
1987
- 1987-03-03 JP JP4854487A patent/JPS63216940A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63216940A (en) | 1988-09-09 |
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