JPH10106818A - Permanent magnet for ultra high vacuum and method for manufacturing the same - Google Patents

Permanent magnet for ultra high vacuum and method for manufacturing the same

Info

Publication number
JPH10106818A
JPH10106818A JP8277202A JP27720296A JPH10106818A JP H10106818 A JPH10106818 A JP H10106818A JP 8277202 A JP8277202 A JP 8277202A JP 27720296 A JP27720296 A JP 27720296A JP H10106818 A JPH10106818 A JP H10106818A
Authority
JP
Japan
Prior art keywords
magnet
permanent magnet
high vacuum
film
thickness
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.)
Pending
Application number
JP8277202A
Other languages
Japanese (ja)
Inventor
Fumiaki Kikui
文秋 菊井
Masako Suzuki
雅子 鈴木
Masayuki Yoshimura
吉村  公志
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Proterial Ltd
Original Assignee
Sumitomo Special Metals Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Sumitomo Special Metals Co Ltd filed Critical Sumitomo Special Metals Co Ltd
Priority to JP8277202A priority Critical patent/JPH10106818A/en
Publication of JPH10106818A publication Critical patent/JPH10106818A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F41/00Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
    • H01F41/02Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets
    • H01F41/0253Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets for manufacturing permanent magnets
    • H01F41/026Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets for manufacturing permanent magnets protecting methods against environmental influences, e.g. oxygen, by surface treatment

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Environmental & Geological Engineering (AREA)
  • Manufacturing & Machinery (AREA)
  • Manufacturing Cores, Coils, And Magnets (AREA)
  • Physical Vapour Deposition (AREA)
  • Hard Magnetic Materials (AREA)

Abstract

PROBLEM TO BE SOLVED: To provide a permanent magnet for ultra high vacuum which has good adhesion of a coating film thereon, is tight, can prevent the generation and release of gas from the magnet body, and has a high magnetic characteristic used for an undulator, etc., in the ultra high vacuum of below 1×10<-9> Pa. SOLUTION: After the surface of an Fe-B-R permanent magnet body is cleaned by an ion sputtering method, etc., an aluminum coating film of 0.06 to 5.0×m thickness is formed on the surface of the permanent magnet body by a method for firming a thin film such as an ion plating method, etc. An AlN coating film of 5.0 to 20μm thickness is formed on the aluminum coating film in an atmosphere of N2 gas by a method for forming a thin film such as an ion reaction plating method, etc. The can prevent the generation of a gas adhering to the magnet or absorbed by the magnet, and enables effective use of high magnetic characteristics of the magnet.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】この発明は、超高真空雰囲気
のアンジュレーター等に使用可能な高磁気特性を有した
超高真空用永久磁石に係り、磁石体表面にAl被膜を介
してAlN被膜層を形成することにより、被膜の密着性
に優れ、緻密で磁石体からのガス発生、放出を防止し
て、1×10-9Pa以下の超高真空に使用でき、極めて
安定した磁気特性を有する超高真空用永久磁石およびそ
の製造方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an ultra-high vacuum permanent magnet having high magnetic properties which can be used for an undulator or the like in an ultra-high vacuum atmosphere. By forming a film, it is excellent in adhesion of the film, is dense, prevents gas generation and release from the magnet body, can be used in an ultra-high vacuum of 1 × 10 −9 Pa or less, and has extremely stable magnetic properties. The present invention relates to an ultra-high vacuum permanent magnet and a method for manufacturing the same.

【0002】[0002]

【従来の技術】先に、NdやPrを中心とする資源的に
豊富な軽希土類を用いてB,Feを主成分とし、高価な
SmやCoを含有せず、従来の希土類コバルト磁石の最
高特性を大幅に超える新しい高性能永久磁石として、F
e−B−R系永久磁石が提案されている(特開昭59−
46008号公報、特開昭59−89401号公報)。
2. Description of the Related Art First, using rare earths, which are abundant in resources, mainly Nd and Pr, B and Fe as main components, do not contain expensive Sm and Co, and are the highest among conventional rare earth cobalt magnets. As a new high-performance permanent magnet that greatly exceeds the characteristics,
e-B-R permanent magnets have been proposed (Japanese Patent Laid-Open No. 59-1984).
46008, JP-A-59-89401).

【0003】前記磁石合金のキュリー点は、一般に30
0℃〜370℃であるが、Feの一部をCoにて置換す
ることにより、より高いキュリー点を有するFe−B−
R系永久磁石(特開昭59−64733号、特開昭59
−132104号)を得られる。
The Curie point of the above magnet alloy is generally 30
0 ° C. to 370 ° C., but having a higher Curie point by substituting a part of Fe with Co
R-based permanent magnets (JP-A-59-64733, JP-A-59-64733)
-132104).

【0004】前記Co含有のFe−B−R系希土類永久
磁石と同等以上のキュリー点並びにより高い(BH)m
axを有し、その温度特性、特にiHcを向上させるた
め、希土類元素(R)としてNdやPr等の軽希土類を
中心としたCo含有のFe−B−R系希土類永久磁石の
Rの一部にDy、Tb等の重希土類のうち少なくとも1
種を含有することにより、25MGOe以上の極めて高
い(BH)maxを保有したままで、iHcをさらに向
上させたCo含有のFe−B−R系希土類永久磁石が提
案(特開昭60−34005号)されている。
[0004] The Curie point is higher than or equal to that of the Co-containing Fe-BR based rare earth permanent magnet and the (BH) m is higher.
ax and a part of R of a Co-containing Fe-BR-based rare earth permanent magnet mainly containing light rare earths such as Nd and Pr as rare earth elements (R) in order to improve its temperature characteristics, particularly iHc. At least one of heavy rare earths such as Dy and Tb.
Proposal of a Co-containing Fe-BR based rare earth permanent magnet further improved in iHc while retaining a very high (BH) max of 25 MGOe or more by containing a seed (Japanese Patent Application Laid-Open No. 60-34005) ) Has been.

【0005】従来、真空雰囲気用磁石としては、フェラ
イト磁石が10-3Paオーダーの真空で使用されている
が、フェライト磁石は磁気特性が低く、アンジュレータ
ー等に使用するには磁気特性が十分でない。
Conventionally, as a magnet for a vacuum atmosphere, a ferrite magnet has been used in a vacuum of the order of 10 −3 Pa. However, the ferrite magnet has low magnetic properties and does not have sufficient magnetic properties to be used for an undulator or the like. .

【0006】すなわち、1×10-9Pa以下の超高真空
に使用できる超高真空用磁石としては、(1)磁石特性
が優れること、(2)磁石よりの内蔵ガス、付着ガスの
放出、放散がないこと、(3)装置内に取り付けて1×
10-9Pa以下が、達成できることが重要である。
That is, as a magnet for an ultra-high vacuum that can be used in an ultra-high vacuum of 1 × 10 −9 Pa or less, (1) excellent magnet properties, (2) release of a built-in gas and an attached gas from the magnet, No radiation, (3) 1 ×
It is important that 10 -9 Pa or less can be achieved.

【0007】そこで、前記のごとくFe−B−R系磁石
が高磁気特性のため、1×10-9Pa以下の超高真空用
アンジュレーターへの使用が考えられるが、前記Fe−
B−R系磁石はガスの吸着、吸蔵が生じるため、真空雰
囲気での磁石からの発生、放出ガスにより、真空度1×
10-9Pa以下の超高真空雰囲気には、Fe−B−R系
磁石の使用は困難であった。
Therefore, as described above, since the Fe-BR based magnet has high magnetic properties, it can be used for an undulator for ultra-high vacuum of 1 × 10 −9 Pa or less.
Because the BR magnet absorbs and absorbs gas, the degree of vacuum is 1 × due to the gas generated and released from the magnet in a vacuum atmosphere.
In an ultra-high vacuum atmosphere of 10 −9 Pa or less, it was difficult to use a Fe—BR magnet.

【0008】[0008]

【発明が解決しようとする課題】従来、防食用にNiメ
ッキ処理したFe−B−R系磁石を超高真空に用いる場
合、磁石は超高真空チャンバー中には入れられず、外部
より磁石を取付け、アンジュレーター等を作製していた
ため、装置が大型化し、Fe−B−R系磁石の高磁気特
性を有効に利用できなかった。
Conventionally, when a Ni-plated Fe-BR-based magnet for corrosion protection is used in an ultra-high vacuum, the magnet cannot be placed in an ultra-high vacuum chamber, Since the mounting, the undulator, and the like were manufactured, the size of the apparatus was increased, and the high magnetic characteristics of the Fe-BR-based magnet could not be effectively used.

【0009】従来のFe−B−R系磁石体の耐食性の改
善を目的とした各種被膜を有する耐食性Fe−B−R系
永久磁石でも、真空雰囲気での磁石からの発生、放出ガ
スにより、真空度1×10-9Pa以下の超高真空雰囲気
での使用が困難であった。
[0009] Even a conventional corrosion-resistant Fe-BR permanent magnet having various coatings for the purpose of improving the corrosion resistance of a conventional Fe-BR-based magnet body, the vacuum generated by the magnet in a vacuum atmosphere and the gas released therefrom cause a vacuum. It was difficult to use it in an ultra-high vacuum atmosphere having a degree of 1 × 10 −9 Pa or less.

【0010】この発明は、従来、Fe−B−R系磁石体
の耐食性の改善を目的とした各種被膜を有する耐食性F
e−B−R系永久磁石とは全く異なり、磁石体表面との
密着性に優れる上、被膜は緻密で磁石体からのガス発
生、放出を防止する働きがあり、超高真空雰囲気のアン
ジュレーター等に使用可能な高磁気特性を有した超高真
空用永久磁石の提供を目的としている。
The present invention relates to a conventional corrosion-resistant F-B-R magnet having various coatings for the purpose of improving the corrosion resistance.
Unlike e-B-R permanent magnets, they have excellent adhesion to the surface of the magnet body and have a dense coating that prevents gas generation and release from the magnet body. It is an object of the present invention to provide an ultra-high vacuum permanent magnet having high magnetic properties that can be used for such purposes.

【0011】[0011]

【課題を解決するための手段】発明者らは、下地との密
着性がすぐれ、被着した緻密な金属被膜により、磁石に
付着あるいは吸蔵するガスの発生を防止することがで
き、その磁石特性の安定したFe−B−R系永久磁石を
目的に、永久磁石体表面へのAlN被膜形成法について
種々検討した結果、磁石体表面をイオンスパッター法等
により清浄化した後、前記磁石体表面にイオンプレーテ
ィング法等の薄膜形成法により特定膜厚のAl被膜を形
成後、N2ガス中にてイオン反応プレーティング等の薄
膜形成法を行って、特定膜厚のAlNを形成することに
より、Alは下地との密着性に優れ、また、Al被膜上
にAlN被膜を形成するに際し、界面にはAlNxなる
Al,Nの複合被膜が生成し、このAlNxの組成、膜
厚は、基板温度、バイアス電圧、成膜スピード等によっ
て変化し、AlN界面に向かって、Nが連続的に増加す
る組成となっており、これによりAl被膜とAlN被膜
との密着性は著しく改善できること、この磁石を装置内
に取り付けて1×10-9Pa以下の真空度を達成でき、
超高真空用アンジュレーターに最適であることを知見
し、この発明を完成した。
Means for Solving the Problems The inventors of the present invention have excellent adhesion to a base and can prevent generation of gas adhering to or occluded by a magnet by a dense metal coating applied thereto. As a result of various studies on a method of forming an AlN coating on the surface of the permanent magnet body for the purpose of producing a stable Fe-BR-based permanent magnet, the magnet body surface was cleaned by an ion sputtering method or the like, and then the magnet body surface was cleaned. After forming an Al film having a specific thickness by a thin film forming method such as an ion plating method, a thin film forming method such as an ion reaction plating is performed in N 2 gas to form AlN having a specific thickness. Al has excellent adhesion to the base, and when an AlN film is formed on the Al film, a composite film of Al and N, which is AlNx, is formed at the interface. Ba The composition is such that N changes continuously depending on the ass voltage, the film forming speed, etc., and N continuously increases toward the AlN interface, whereby the adhesion between the Al film and the AlN film can be significantly improved. To achieve a degree of vacuum of 1 × 10 -9 Pa or less,
The present inventors have found that the present invention is most suitable for an undulator for ultra-high vacuum, and have completed the present invention.

【0012】すなわち、この発明は、主相が正方晶相か
らなるFe−B−R系永久磁石体表面に、膜厚0.06
μm〜5.0μmのAl被膜を形成して膜厚0.5μm
〜10μmのAlN被膜層を有することを特徴とする超
高真空用永久磁石である。
That is, according to the present invention, a film having a thickness of 0.06 mm is formed on the surface of an Fe—BR-based permanent magnet body whose main phase is a tetragonal phase.
forming an Al coating having a thickness of 0.5 μm to 5.0 μm
An ultrahigh vacuum permanent magnet having an AlN coating layer of 10 to 10 μm.

【0013】また、この発明は、主相が正方晶相からな
るFe−B−R系永久磁石体表面を清浄化した後、前記
磁石体表面に膜厚0.06μm〜5.0μmのAl被膜
を気相成膜法により形成後、N2ガス雰囲気中で気相成
膜法により膜厚0.5μm〜10μmのAlN被膜層を
形成することを特徴とする超高真空用永久磁石の製造方
法である。
Further, according to the present invention, an Al coating having a thickness of 0.06 μm to 5.0 μm is formed on the surface of the permanent magnet body after cleaning the surface of the Fe—BR based permanent magnet body having a tetragonal phase as a main phase. Forming an AlN coating layer having a film thickness of 0.5 μm to 10 μm in a N 2 gas atmosphere by a gas phase film forming method after forming the AlN film layer by a gas phase film forming method. It is.

【0014】[0014]

【発明の実施の形態】この発明において、Fe−B−R
系永久磁石体表面に被着するAl被膜、AlN被膜の形
成方法としてはイオンプレーティング法、イオンスパッ
タリング法、蒸着法等のいわゆる気相成膜法が適宜利用
できるのが、被膜緻密性、均一性、被膜形成速度などの
理由からイオンプレーティング、反応イオンプレーティ
ングが好ましい。
BEST MODE FOR CARRYING OUT THE INVENTION In the present invention, Fe-BR
As a method for forming the Al film and the AlN film to be adhered to the surface of the permanent magnet body, a so-called gas-phase film forming method such as an ion plating method, an ion sputtering method, and a vapor deposition method can be appropriately used. Ion plating and reactive ion plating are preferred from the viewpoints of properties, film formation speed, and the like.

【0015】また、反応被膜生成時の基板となる永久磁
石の温度は200℃〜500℃に設定するのが好まし
く、200℃未満では基板磁石との反応密着が十分でな
く、また500℃を超えると常温(25℃)との温度差
が大きくなり、処理後の冷却過程で被膜に亀裂が入り、
一部基板より剥離を発生するため、基板磁石の温度を2
00℃〜500℃に設定するとよい。
The temperature of the permanent magnet serving as the substrate when the reaction film is formed is preferably set to 200 ° C. to 500 ° C. If the temperature is lower than 200 ° C., the reaction adhesion with the substrate magnet is not sufficient, and the temperature exceeds 500 ° C. The temperature difference between the temperature and normal temperature (25 ° C) increases, and the coating cracks in the cooling process after the treatment,
The temperature of the substrate magnet is set to 2
It is good to set to 00 degreeC-500 degreeC.

【0016】Fe−B−R系永久磁石体表面にAl被膜
層を介してAlN被膜層を設けたことを特徴とするこの
発明の超高真空用永久磁石の製造方法の一例を以下に詳
述する。1)アークイオンプレーティング装置を用い
て、真空容器を到達真空度が、1×10-3pa以下まで
真空排気した後、Arガス圧10pa、−500VでA
rイオンによる表面スパッターにてFe−B−R系磁石
体表面を清浄化する。
An example of the method for manufacturing a permanent magnet for ultra-high vacuum of the present invention, characterized in that an AlN coating layer is provided on the surface of the Fe-BR-based permanent magnet body via an Al coating layer, will be described in detail below. I do. 1) After evacuating the vacuum vessel to an ultimate vacuum of 1 × 10 −3 pa or less using an arc ion plating apparatus, the vacuum vessel is evacuated at an Ar gas pressure of 10 pa and −500 V.
The surface of the Fe-BR-based magnet body is cleaned by surface sputtering using r ions.

【0017】2)次に、Arガス圧0.1pa、バイア
ス電圧−50Vにより、ターゲットのAlを蒸発させ
て、アークイオンプレーティング法にて、磁石体表面に
0.06μm〜5.0μm膜厚のAl被膜層を形成す
る。
2) Next, the target Al is evaporated by an Ar gas pressure of 0.1 pa and a bias voltage of −50 V, and the thickness of the target is 0.06 μm to 5.0 μm on the surface of the magnet body by an arc ion plating method. Is formed.

【0018】3)続いて、基板の磁石温度を250℃に
保持し、N2ガス圧1pa、バイアス電圧−100Vの
条件にて、Al被膜層上に特定厚のAlN被膜層を形成
する。
3) Subsequently, an AlN coating layer having a specific thickness is formed on the Al coating layer under the conditions that the magnet temperature of the substrate is maintained at 250 ° C., the N 2 gas pressure is 1 pa, and the bias voltage is −100 V.

【0019】この発明において、Fe−B−R系永久磁
石体表面のAl被膜厚を0.06μm〜5.0μmに限
定した理由は、0.06μm未満では磁石体表面にAl
が均一に被着し難く、下地膜としての効果が十分でな
く、5.0μmを超えると効果的には問題ないが、下地
膜としてはコスト上昇を招来して、実用的でなく好まし
くないので、Al被膜厚は0.06μm〜5.0μmと
する。特に、Al被膜厚は磁石体の表面粗度によって選
定され、表面粗度が0.1μm以下の場合、Al被膜厚
は0.06μm〜5.0μmが好ましく、また表面粗度
が0.1μm〜1.2μmの場合、望ましい膜厚は0.
1μm〜5.0μmである。
In the present invention, the reason why the thickness of the Al coating on the surface of the Fe—BR type permanent magnet body is limited to 0.06 μm to 5.0 μm is that if the thickness is less than 0.06 μm, the surface of the magnet body has an aluminum coating.
Is difficult to apply uniformly, and the effect as a base film is not sufficient. When the thickness exceeds 5.0 μm, there is no problem. However, the cost of the base film is increased, which is not practical and not preferable. , Al coating thickness is set to 0.06 μm to 5.0 μm. In particular, the Al coating thickness is selected according to the surface roughness of the magnet body. When the surface roughness is 0.1 μm or less, the Al coating thickness is preferably 0.06 μm to 5.0 μm, and the surface roughness is 0.1 μm to In the case of 1.2 μm, the desired film thickness is 0.1 μm.
It is 1 μm to 5.0 μm.

【0020】また、AlN被膜厚を0.5μm〜10μ
mに限定した理由は、0.5μm未満ではAlNとして
の耐食性、耐摩耗性が十分でなく、10μmを超えると
効果的には問題ないが、製造コスト上昇を招来するので
好ましくない。
The AlN film thickness is set to 0.5 μm to 10 μm.
The reason for limiting to m is that if it is less than 0.5 μm, the corrosion resistance and abrasion resistance as AlN are not sufficient, and if it exceeds 10 μm, there is no problem effectively, but it is not preferable because it increases the manufacturing cost.

【0021】この発明において、永久磁石に用いる希土
類元素Rは、組成の10原子%〜30原子%を占める
が、Nd、Pr、Dy、Ho、Tbのうち少なくとも1
種、あるいはさらに、La、Ce、Sm、Gd、Er、
Eu、Tm、Yb、Lu、Yのうち少なくとも1種を含
むものが好ましい。また、通常Rのうち1種をもって足
りるが、実用上は2種以上の混合物(ミッシュメタル、
ジジム等)を入手上の便宜等の理由により用いることが
できる。なお、このRは純希土類元素でなくてもよく、
工業上入手可能な範囲で製造上不可避な不純物を含有す
るものでも差支えない。
In the present invention, the rare earth element R used in the permanent magnet occupies 10 to 30 atomic% of the composition, but at least one of Nd, Pr, Dy, Ho, and Tb.
Species, or additionally, La, Ce, Sm, Gd, Er,
Those containing at least one of Eu, Tm, Yb, Lu, and Y are preferable. Usually, one kind of R is sufficient, but in practice, a mixture of two or more kinds (Misch metal,
Jijim etc.) can be used for reasons such as convenience in obtaining. Note that this R may not be a pure rare earth element,
It may be one containing impurities that are unavoidable in production as far as it is industrially available.

【0022】Rは、上記系永久磁石における必須元素で
あって、10原子%未満では結晶構造がα−鉄と同一構
造の立方晶組織となるため、高磁気特性、特に高保磁力
が得られず、30原子%を超えるとRリッチな非磁性相
が多くなり、残留磁束密度(Br)が低下してすぐれた
特性の永久磁石が得られない。よって、R10原子%〜
30原子%の範囲が望ましい。
R is an essential element in the above-mentioned permanent magnets. If it is less than 10 atomic%, the crystal structure becomes a cubic structure having the same structure as that of α-iron, so that high magnetic properties, particularly high coercive force cannot be obtained. , More than 30 atomic%, the R-rich nonmagnetic phase increases, the residual magnetic flux density (Br) decreases, and a permanent magnet having excellent characteristics cannot be obtained. Therefore, R10 atomic% or more
A range of 30 atomic% is desirable.

【0023】Bは、上記系永久磁石における必須元素で
あって、2原子%未満では菱面体構造が主相となり、高
い保磁力(iHc)は得られず、28原子%を超えると
Bリッチな非磁性相が多くなり、残留磁束密度(Br)
が低下するため、すぐれた永久磁石が得られない。よっ
て、Bは2原子%〜28原子%の範囲が望ましい。
B is an essential element in the above permanent magnets. If it is less than 2 atomic%, the rhombohedral structure becomes the main phase, and a high coercive force (iHc) cannot be obtained. If it exceeds 28 atomic%, B becomes rich. Increase in non-magnetic phase, residual magnetic flux density (Br)
, The excellent permanent magnet cannot be obtained. Therefore, B is desirably in the range of 2 to 28 atomic%.

【0024】Feは、上記系永久磁石において必須元素
であり、65原子%未満では残留磁束密度(Br)が低
下し、80原子%を超えると高い保磁力が得られないの
で、Feは65原子%〜80原子%の含有が望ましい。
また、Feの一部をCoで置換することは、得られる磁
石の磁気特性を損うことなく、温度特性を改善すること
ができるが、Co置換量がFeの20%を超えると、逆
に磁気特性が劣化するため、好ましくない。Coの置換
量がFeとCoの合計量で5原子%〜15原子%の場合
は、Brは置換しない場合に比較して増加するため、高
磁束密度を得るために好ましい。
Fe is an essential element in the above-mentioned permanent magnets. When the content is less than 65 atomic%, the residual magnetic flux density (Br) decreases, and when it exceeds 80 atomic%, a high coercive force cannot be obtained. % To 80 atomic%.
Further, substituting a part of Fe with Co can improve the temperature characteristics without impairing the magnetic characteristics of the obtained magnet. However, when the Co substitution amount exceeds 20% of Fe, conversely, It is not preferable because the magnetic properties deteriorate. When the substitution amount of Co is 5 atomic% to 15 atomic% in the total amount of Fe and Co, Br is increased as compared with the case where no substitution is made, and thus it is preferable to obtain a high magnetic flux density.

【0025】また、R、B、Feの他、工業的生産上不
可避的不純物の存在を許容でき、例えば、Bの一部を
4.0wt%以下のC、2.0wt%以下のP、2.0
wt%以下のS、2.0wt%以下のCuのうち少なく
とも1種、合計量で2.0wt%以下で置換することに
より、永久磁石の製造性改善、低価格化が可能である。
In addition to R, B, and Fe, the presence of unavoidable impurities in industrial production can be tolerated. For example, part of B may be 4.0 wt% or less of C, 2.0 wt% or less of P, .0
By replacing at least one of S by wt% or less and Cu by 2.0 wt% or less with a total amount of 2.0 wt% or less, it is possible to improve the productivity and reduce the cost of the permanent magnet.

【0026】さらに、Al、Ti、V、Cr、Mn、B
i、Nb、Ta、Mo、W、Sb、Ge、Sn、Zr、
Ni、Si、Zn、Hf、のうち少なくとも1種は、F
e−B−R系永久磁石材料に対してその保磁力、減磁曲
線の角型性を改善あるいは製造性の改善、低価格化に効
果があるため添加することができる。なお、添加量の上
限は、磁石材料の(BH)maxを20MGOe以上と
するには、Brが少なくとも9kG以上必要となるた
め、該条件を満す範囲が望ましい。
Further, Al, Ti, V, Cr, Mn, B
i, Nb, Ta, Mo, W, Sb, Ge, Sn, Zr,
At least one of Ni, Si, Zn, and Hf is F
It can be added to the e-B-R permanent magnet material because it has the effect of improving the coercive force and the squareness of the demagnetization curve, improving the productivity, and reducing the price. The upper limit of the addition amount is preferably in a range that satisfies the above condition, since Br needs to be at least 9 kG or more in order to make (BH) max of the magnet material 20 MGOe or more.

【0027】また、Fe−B−R系永久磁石は平均結晶
粒径が1〜80μmの範囲にある正方晶系の結晶構造を
有する化合物を主相とし、体積比で1%〜50%の非磁
性相(酸化物相を除く)を含むことを特徴とする。Fe
−B−R系永久磁石は、保磁力iHc≧1kOe、残留
磁束密度Br>4kG、を示し、最大エネルギー積(B
H)maxは、(BH)max≧10MGOeを示し、
最大値は25MGOe以上に達する。
The Fe-BR-based permanent magnet has a main phase of a compound having a tetragonal crystal structure having an average crystal grain size in a range of 1 to 80 μm, and has a non-volume of 1% to 50% by volume. It is characterized by containing a magnetic phase (excluding an oxide phase). Fe
The -BR type permanent magnet has a coercive force iHc ≧ 1 kOe, a residual magnetic flux density Br> 4 kG, and a maximum energy product (B
H) max indicates (BH) max ≧ 10MGOe,
The maximum reaches 25 MGOe or more.

【0028】[0028]

【実施例】【Example】

実施例1 公知の鋳造インゴットを粉砕し、微粉砕後に成形、焼結
し、熱処理を施して16Nd−1Pr−76Fe−7B
組成の径12mm×厚み2mm寸法の磁石体試験片を得
た。その磁石を真空容器内に入れ、真空容器内を1×1
-3pa以下に排気してArガス圧5pa、−600V
で20分間、表面スパッターを行って磁石体表面を清浄
化した後、Arガス圧0.2pa、バイアス電圧−80
V、基板磁石温度を250℃にてターゲットとして金属
Alをアークイオンプレーティング法にて磁石体表面に
1.5μm厚のAl被膜層を形成する。
Example 1 A known casting ingot was pulverized, finely pulverized, molded, sintered, and heat-treated to obtain 16Nd-1Pr-76Fe-7B.
A magnet test piece having a composition having a diameter of 12 mm and a thickness of 2 mm was obtained. Put the magnet in a vacuum vessel,
Exhaust to 0 -3 pa or less, Ar gas pressure 5 pa, -600 V
After performing surface sputtering for 20 minutes to clean the surface of the magnet body, an Ar gas pressure of 0.2 pa and a bias voltage of −80 were applied.
V. A 1.5 μm thick Al coating layer is formed on the surface of the magnet body by arc ion plating using metal Al as a target at a substrate magnet temperature of 250 ° C.

【0029】次に基板磁石を350℃、バイアス電圧−
100V、アーク電流100Aで、N2ガス1paに
て、アークイオンプレーティング法にてAl被膜表面に
膜厚3μmののAlN被膜層を形成した。その後、放冷
後、得られたAlN被膜を有する永久磁石の磁気特性を
測定し、その結果を表1に示す。得られた永久磁石を図
1に示す超高真空装置で到達真空度を測定した。その測
定結果を図2に示す。
Next, the substrate magnet was heated at 350 ° C.
An AlN coating layer having a thickness of 3 μm was formed on the surface of the Al coating by arc ion plating at 100 V and an arc current of 100 A with N 2 gas at 1 pa. Thereafter, after cooling, the magnetic properties of the obtained permanent magnet having an AlN coating were measured, and the results are shown in Table 1. The ultimate vacuum degree of the obtained permanent magnet was measured by the ultrahigh vacuum apparatus shown in FIG. FIG. 2 shows the measurement results.

【0030】図1に示す超高真空装置による到達真空度
の測定方法を説明すると、超高真空装置1は、長尺筒状
からなる本体2にはTiゲッターポンプ4、イオンポン
プ5並びにBAゲージ6とエクストラクターゲージ7が
それぞれ配設されており、本体2の一方端には試料室3
が設けてある。
The method of measuring the ultimate vacuum by the ultra-high vacuum apparatus shown in FIG. 1 will be described. The ultra-high vacuum apparatus 1 has a long cylindrical body 2 having a Ti getter pump 4, an ion pump 5, and a BA gauge. 6 and an extractor gauge 7 are provided, respectively.
Is provided.

【0031】まず、試料室3に磁石試料8を挿入しない
で、Tiゲッターポンプ4、イオンポンプ5を作動させ
て真空引きしながら、150〜200℃に48時間ベー
キングした後、放冷して本体2内の温度が70℃以下に
なった後、BAゲージ6とエクストラクターゲージ7を
作動させて、最終到達真空度を測定する。この最終到達
真空度は7×10-10Paであった。図2中のaに示
す。
First, without inserting the magnet sample 8 into the sample chamber 3, the Ti getter pump 4 and the ion pump 5 are operated and evacuated, baked at 150 to 200 ° C. for 48 hours, and then cooled and cooled. After the temperature in 2 becomes 70 ° C. or lower, the BA gauge 6 and the extractor gauge 7 are operated to measure the ultimate vacuum degree. The final vacuum degree was 7 × 10 −10 Pa. This is indicated by a in FIG.

【0032】次に、試料室3に寸法、高さ8mm×幅8
mm×長さ50mm、数量60個の磁石試料8を挿入し
て、Tiゲッターポンプ4、イオンポンプ5を作動させ
て真空引きしながら、150〜200℃に48時間ベー
キングした後、放冷して本体2内の温度が70℃以下に
なった後、BAゲージ6とエクストラクターゲージ7を
作動させて、到達真空度を測定する。この際の最終到達
真空度とそれに至るまでの経過時間との関係を図2の曲
線bに示す。なお、○印はBAゲージ、□印はエクスト
ラクターゲージによる測定値を示す。
Next, the size, height 8 mm × width 8 are set in the sample chamber 3.
The magnet sample 8 having a size of 50 mm × length 50 mm and a quantity of 60 was inserted, and the Ti getter pump 4 and the ion pump 5 were operated and evacuated, baked at 150 to 200 ° C. for 48 hours, and then allowed to cool. After the temperature in the main body 2 becomes 70 ° C. or lower, the ultimate vacuum degree is measured by operating the BA gauge 6 and the extractor gauge 7. At this time, the relationship between the ultimate vacuum degree and the elapsed time until reaching the final vacuum degree is shown by a curve b in FIG. In addition, ○ indicates a measurement value using a BA gauge, and □ indicates a measurement value using an extractor gauge.

【0033】比較例1 実施例1と同一組成の表面にAl被膜、AlN被膜を有
しない磁石体試験片の磁気特性を第1表に表す。実施例
1と同一寸法、数量の磁石体試験片を実施例1と同一条
件にて表面清浄化した後、図1の超高真空装置で実施例
1と同一条件にて到達真空度を測定した。その結果を図
2の曲線cに示す。
Comparative Example 1 Table 1 shows the magnetic properties of a magnet test piece having the same composition as in Example 1 but without an Al film or an AlN film on the surface. After cleaning the surface of a magnet body test piece having the same size and quantity as in Example 1 under the same conditions as in Example 1, the ultimate vacuum degree was measured using the ultrahigh vacuum apparatus of FIG. 1 under the same conditions as in Example 1. . The result is shown by curve c in FIG.

【0034】比較例2 実施例1と同一組成、同一寸法、数量の磁石体試験片を
実施例1と同一条件にて表面清浄化した後、通常の電気
メッキにてNi膜を20μm形成した。得られたNiメ
ッキ磁石の磁気特性を測定し、その結果を第1表に表
す。その後、Niメッキ磁石を表面洗浄後、図1の超高
真空装置で実施例1と同一条件にて到達真空度を測定し
た。その結果を図2の曲線dに示す。
Comparative Example 2 A magnet test piece having the same composition, the same dimensions and the same number as in Example 1 was cleaned under the same conditions as in Example 1, and then a Ni film was formed to 20 μm by ordinary electroplating. The magnetic properties of the obtained Ni-plated magnet were measured, and the results are shown in Table 1. Then, after the surface of the Ni-plated magnet was washed, the ultimate vacuum degree was measured using the ultrahigh vacuum apparatus of FIG. 1 under the same conditions as in Example 1. The result is shown by a curve d in FIG.

【0035】この発明による磁石表面にAl被膜を形成
後、このAl被膜の上にAlN被膜層を設けたFe−B
−R系永久磁石体は、実施例の如く、磁石体からのガス
の発生がなく、真空度1×10-9Pa以下を達成できる
が、磁石素材そのまま、あるいはNiメッキ膜を設けた
磁石体では磁石体からのガスの発生により、目的の到達
真空度が達成できないことが分かる。
After forming an Al coating on the magnet surface according to the present invention, Fe-B having an AlN coating layer on the Al coating is provided.
The -R permanent magnet body can achieve a degree of vacuum of 1 × 10 −9 Pa or less without generating gas from the magnet body as in the embodiment, but the magnet body as it is or a magnet body provided with a Ni plating film It can be seen that the target ultimate vacuum cannot be achieved due to the generation of gas from the magnet body.

【0036】[0036]

【表1】 [Table 1]

【0037】[0037]

【発明の効果】この発明は、Fe−B−R系永久磁石体
表面をイオンスパッター法等により清浄化した後、前記
磁石体表面にイオンプレーティング法等の薄膜形成法に
よりAl被膜を形成後、N2ガス中にてイオン反応プレ
ーティング等の薄膜形成法を行って、AlN被膜を形成
したことを特徴とし、被膜は緻密で、密着性に優れ、磁
石体からのガスの発生を防止する働きがあり、超高真空
雰囲気のアンジュレーター等に使用可能な高磁気特性を
有した超高真空用Fe−B−R系永久磁石が得られる。
According to the present invention, after the surface of an Fe-BR based permanent magnet is cleaned by an ion sputtering method or the like, an Al film is formed on the surface of the magnet by a thin film forming method such as an ion plating method. And an AlN film formed by performing a thin film forming method such as ion reaction plating in N 2 gas. The film is dense, has excellent adhesion, and prevents generation of gas from the magnet body. An Fe-BR-based permanent magnet for ultra-high vacuum that has a function and has high magnetic properties and can be used for an undulator or the like in an ultra-high vacuum atmosphere is obtained.

【図面の簡単な説明】[Brief description of the drawings]

【図1】到達真空度の測定に用いた超高真空装置の構成
説明図である。
FIG. 1 is an explanatory diagram of a configuration of an ultra-high vacuum device used for measuring a degree of ultimate vacuum.

【図2】到達真空度と時間の関係を示すグラフである。FIG. 2 is a graph showing the relationship between ultimate vacuum and time.

【符号の説明】[Explanation of symbols]

1 超高真空装置 2 本体 3 試料室 4 Tiゲッターポンプ 5 イオンポンプ 6 BAゲージ 7 エクストラクターゲージ 8 磁石試料 DESCRIPTION OF SYMBOLS 1 Ultra-high vacuum apparatus 2 Main body 3 Sample chamber 4 Ti getter pump 5 Ion pump 6 BA gauge 7 Extractor gauge 8 Magnet sample

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 主相が正方晶相からなるFe−B−R系
永久磁石体表面に、膜厚0.06μm〜5.0μmのA
l被膜を介して膜厚0.5μm〜10μmのAlN被膜
層を有する超高真空用永久磁石。
1. A 0.06 μm-5.0 μm thick A—B—R based permanent magnet body having a tetragonal phase as a main phase.
(1) An ultra-high vacuum permanent magnet having an AlN coating layer having a thickness of 0.5 μm to 10 μm via a coating.
【請求項2】 主相が正方晶相からなるFe−B−R系
永久磁石体表面を清浄化した後、前記磁石体表面に膜厚
0.06μm〜5.0μmのAl被膜を気相成膜法によ
り形成後、N2ガス雰囲気中で気相成膜法により膜厚
0.5μm〜10μmのAlN被膜層を形成する超高真
空用永久磁石の製造方法。
2. After cleaning the surface of a Fe-BR-based permanent magnet whose main phase is a tetragonal phase, an Al film having a thickness of 0.06 μm to 5.0 μm is formed on the surface of the magnet by vapor phase deposition. A method for manufacturing an ultra-high vacuum permanent magnet in which an AlN coating layer having a thickness of 0.5 μm to 10 μm is formed by a vapor phase film forming method in an N 2 gas atmosphere after being formed by a film method.
JP8277202A 1996-09-26 1996-09-26 Permanent magnet for ultra high vacuum and method for manufacturing the same Pending JPH10106818A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8277202A JPH10106818A (en) 1996-09-26 1996-09-26 Permanent magnet for ultra high vacuum and method for manufacturing the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8277202A JPH10106818A (en) 1996-09-26 1996-09-26 Permanent magnet for ultra high vacuum and method for manufacturing the same

Publications (1)

Publication Number Publication Date
JPH10106818A true JPH10106818A (en) 1998-04-24

Family

ID=17580238

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8277202A Pending JPH10106818A (en) 1996-09-26 1996-09-26 Permanent magnet for ultra high vacuum and method for manufacturing the same

Country Status (1)

Country Link
JP (1) JPH10106818A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110310795A (en) * 2019-06-25 2019-10-08 宁波合力磁材技术有限公司 A kind of anti-corrosion neodymium iron boron magnetic body and preparation method thereof

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110310795A (en) * 2019-06-25 2019-10-08 宁波合力磁材技术有限公司 A kind of anti-corrosion neodymium iron boron magnetic body and preparation method thereof

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