JPH05339714A - Electron beam evaporation method - Google Patents

Electron beam evaporation method

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Publication number
JPH05339714A
JPH05339714A JP4168402A JP16840292A JPH05339714A JP H05339714 A JPH05339714 A JP H05339714A JP 4168402 A JP4168402 A JP 4168402A JP 16840292 A JP16840292 A JP 16840292A JP H05339714 A JPH05339714 A JP H05339714A
Authority
JP
Japan
Prior art keywords
electron beam
evaporation
evaporation material
magnetic pole
crucible
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.)
Granted
Application number
JP4168402A
Other languages
Japanese (ja)
Other versions
JP3244532B2 (en
Inventor
Toshio Rikitake
利夫 力武
Shigehisa Hashimoto
恵久 橋本
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.)
Jeol Ltd
Original Assignee
Jeol 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 Jeol Ltd filed Critical Jeol Ltd
Priority to JP16840292A priority Critical patent/JP3244532B2/en
Publication of JPH05339714A publication Critical patent/JPH05339714A/en
Application granted granted Critical
Publication of JP3244532B2 publication Critical patent/JP3244532B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

(57)【要約】 【目的】 蒸発材料を回転させながら電子ビームにより
加熱蒸発させるにあたり、蒸発ムラをなくして均一な蒸
着膜を形成すると共に蒸発材料を一様に蒸発させること
のできる蒸発方法を提供するものである。 【構成】 蒸発源本体1上部に電子銃2と回転可能な蒸
発材料5を収容したルツボ4を設置する。該電子銃とル
ツボをその間に挾むように磁極6a,6bを設置し、各
磁極の両端に第1,第2の磁極片8a,8b及び9a,
9bを固定する。更に、前記磁極の相対向する部分に補
助磁極片11a,11bを固定する。電子銃2からの電
子ビームEは偏向系10により蒸発材料5上において、
回転中心Oを中心にしてX方向に沿って往復動する。こ
のように補助磁極片を追加することにより蒸発材料上で
の電子ビームの形状が回転中心O部分とその外周部分と
で変化して電流密度が変わるため、蒸発材料を均一に加
熱することができる。
(57) [Abstract] [Purpose] A method for evaporating a vaporized material by rotating the vaporized material with an electron beam to evaporate the vaporized material uniformly while forming a uniform vapor deposition film by eliminating vaporization unevenness. Is provided. [Structure] An electron gun 2 and a crucible 4 containing a rotatable evaporation material 5 are installed above an evaporation source main body 1. Magnetic poles 6a and 6b are installed so as to sandwich the electron gun and the crucible, and first and second magnetic pole pieces 8a, 8b and 9a are provided at both ends of each magnetic pole.
Fix 9b. Further, the auxiliary magnetic pole pieces 11a and 11b are fixed to the opposing portions of the magnetic poles. The electron beam E from the electron gun 2 is deflected on the evaporation material 5 by the deflection system 10,
It reciprocates around the rotation center O along the X direction. By adding the auxiliary magnetic pole piece in this way, the shape of the electron beam on the evaporation material changes between the rotation center O portion and the outer peripheral portion thereof to change the current density, so that the evaporation material can be uniformly heated. ..

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、真空蒸着装置やイオン
プレーティング装置における蒸発源の電子ビーム蒸発方
法に関し、特に、蒸発物質を回転させながら蒸発させる
場合に使用して有効な電子ビーム蒸発方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electron beam evaporation method of an evaporation source in a vacuum evaporation apparatus or an ion plating apparatus, and more particularly, an electron beam evaporation method effective when used for evaporating while rotating an evaporation substance. Regarding

【0002】[0002]

【従来の技術】かかる装置に用いられる電子ビーム蒸発
源としては、図1及び図2に示すような例えば180度
の偏向型の構造のものが広く使用されている。同図にお
いて、1は蒸発源本体、2はこの本体の上面に載置され
た電子銃で、図示しないがフィラメントとグリッドと陽
極とから構成されている。この電子銃2の上面にはフィ
ラメントから発生した電子ビームEを通過させるための
ビーム通過孔3が形成されている。4はこの電子銃と同
様に本体1の上面に載置された有底筒状のルツボで、内
部に蒸発物質5が装填されている。前記電子銃2とルツ
ボ4とはX方向に沿って適当な間隔をおいて配置されて
いる。6a及び6bは電子銃2から発生した電子ビーム
Eを偏向させて蒸発材料5上に照射するための偏向磁場
Bを発生する一対の磁極で、各磁極はその間に前記電子
銃2及びルツボ4を挾むようにしてY方向に沿って互い
に対向するように配置されている。また、この各磁極は
前記本体1に取り付けられた断面コの字状のヨーク7の
両端に夫々固定されている。前記ヨークの途中には図示
しないが磁束を発生するためのコイルが巻回されてい
る。
2. Description of the Related Art As an electron beam evaporation source used in such an apparatus, a structure having a deflection type of, for example, 180 degrees as shown in FIGS. 1 and 2 is widely used. In the figure, 1 is an evaporation source main body, 2 is an electron gun mounted on the upper surface of the main body, and is composed of a filament, a grid and an anode (not shown). A beam passage hole 3 for passing the electron beam E generated from the filament is formed on the upper surface of the electron gun 2. Reference numeral 4 denotes a bottomed cylindrical crucible placed on the upper surface of the main body 1 similarly to this electron gun, and an evaporation substance 5 is loaded inside. The electron gun 2 and the crucible 4 are arranged at appropriate intervals along the X direction. Reference numerals 6a and 6b denote a pair of magnetic poles for deflecting the electron beam E generated from the electron gun 2 to generate a deflection magnetic field B for irradiating the evaporation material 5 on the evaporation material 5, and each magnetic pole holds the electron gun 2 and the crucible 4 between them. They are arranged so as to sandwich each other and face each other along the Y direction. The magnetic poles are fixed to both ends of a yoke 7 having a U-shaped cross section attached to the main body 1. A coil (not shown) for generating magnetic flux is wound around the yoke.

【0003】8a,8b及び9a,9bは前記磁極6a
及び6bに夫々固定されたビーム成形用の第1,第2の
磁極片で、第1の磁極片8a,8bは各開放端部が電子
銃2に接近するように配置され、それによって電子銃の
ビーム通過孔3から出射した電子ビームEを発散させる
ことなく集束させながらルツボ4方向に向けて偏向させ
る役目を果たすものである。また、第2の磁極片9a,
9bも同様に各開放端部がルツボ4(蒸発材料5)に接
近するように配置され、蒸発材料上に照射される電子ビ
ームEの形状をできるだけ小さいスポット状に集束する
役目を果たすものである。ここで、蒸発材料5を照射す
る電子ビームの形状をできるだけ小さい径のスポット状
にするのは、電流密度をできるだけ高くして効率良く加
熱蒸発させるためである。
8a, 8b and 9a, 9b are the magnetic poles 6a
And 6b are beam-forming first and second pole pieces fixed respectively, and the first pole pieces 8a and 8b are arranged so that their respective open ends are close to the electron gun 2, whereby the electron gun 2 is provided. It serves to deflect the electron beam E emitted from the beam passage hole 3 toward the crucible 4 while converging it without diverging it. In addition, the second pole piece 9a,
Similarly, 9b is also arranged such that each open end approaches the crucible 4 (evaporation material 5), and serves to focus the shape of the electron beam E with which the evaporation material is irradiated in a spot shape as small as possible. .. Here, the shape of the electron beam for irradiating the evaporation material 5 is made into a spot shape having a diameter as small as possible in order to increase the current density as much as possible and efficiently heat and evaporate.

【0004】10は電子ビームEを蒸発材料5上で2次
元的に走査するための例えばトロイダルコイル等からな
る偏向系である。
Reference numeral 10 is a deflecting system for two-dimensionally scanning the electron beam E on the evaporation material 5, which is composed of, for example, a toroidal coil.

【0005】いま、図1及び図2で示すように各磁極6
a,6bにより矢印方向の磁場Bを形成した状態におい
て電子銃2から電子ビームEを発生すれば、電子ビーム
は磁場Bにより180度偏向されて蒸発材料5上を照射
するため、蒸発材料が加熱蒸発される。このとき、偏向
系10により電子ビームEを蒸発材料5上で2次元的に
走査すれば、蒸発材料領域を広げることができる。
Now, as shown in FIGS. 1 and 2, each magnetic pole 6
When the electron beam E is generated from the electron gun 2 in the state where the magnetic field B in the arrow direction is formed by a and 6b, the electron beam is deflected by 180 degrees by the magnetic field B and irradiates the evaporation material 5, so that the evaporation material is heated. Is evaporated. At this time, if the electron beam E is two-dimensionally scanned on the evaporation material 5 by the deflection system 10, the evaporation material region can be expanded.

【0006】しかしながら、このように偏向系により蒸
発材料上で電子ビームを2次元的に走査する方式では、
一般にはルツボの形状は円筒状のものが使用されるのに
対して電子ビームの走査は矩形状に行われるため、蒸発
材料状で走査されない部分ができ、走査されない部分に
は蒸発材料が残る。従って、蒸発されずに残っている部
分があるにもかかわらず蒸発材料を交換しなければなら
ないため、蒸発材料の利用効率が悪い。また、電子ビー
ムによる蒸発材料の走査範囲にも限界があり、一度に蒸
発させる量に限界がある。
However, in the system in which the electron beam is two-dimensionally scanned on the evaporation material by the deflection system as described above,
Generally, the crucible has a cylindrical shape, whereas the electron beam is scanned in a rectangular shape. Therefore, a portion of the evaporation material that is not scanned is formed, and the evaporation material remains in the portion that is not scanned. Therefore, the evaporation material has to be exchanged even though there is a portion that has not been evaporated, so that the utilization efficiency of the evaporation material is poor. Also, there is a limit to the scanning range of the evaporation material by the electron beam, and there is a limit to the amount of evaporation at one time.

【0007】そこで、近時図3に示すように蒸発材料5
(ルツボ4)を矢印C方向に回転させた状態において、
電子ビームEを蒸発材料5の回転中心Oから半径方向
(X方向)に沿って同図中点線Saで示すように蒸発材
料の外周部分までを往復動させながら蒸発材料を加熱蒸
発することが行われている。
Therefore, recently, as shown in FIG.
With the (crucible 4) rotated in the direction of arrow C,
The electron beam E is heated and vaporized while reciprocating from the rotation center O of the vaporized material 5 along the radial direction (X direction) to the outer peripheral portion of the vaporized material as shown by the dotted line Sa in the figure. It is being appreciated.

【0008】このようになせば、電子ビームEを蒸発材
料5全体に照射させることができるため、蒸発材料を無
駄なく消費することができる。また、電子ビームの走査
は2次元的ではなく往復動であるため、その移動距離を
長くすることは比較的容易である。従って、大径のルツ
ボを使用することが可能となるため、一度に多量の蒸発
材料を加熱蒸発させることができる。
In this way, the electron beam E can be irradiated to the entire evaporation material 5, so that the evaporation material can be consumed without waste. Further, since the scanning of the electron beam is not a two-dimensional scan but a reciprocating motion, it is relatively easy to increase the moving distance. Therefore, a crucible having a large diameter can be used, and a large amount of evaporation material can be heated and evaporated at one time.

【0009】[0009]

【発明が解決しようとする課題】ところで、蒸発材料5
上を照射する電子ビームEの形状は、図3中実線Saと
点線Sbで示すように電子ビームの移動範囲内で変える
ことなく一定であり、また、その大きさは前述した理由
により非常に小さいスポット上のものを使用している。
つまり、非常に大きな一定の電流密度の電子ビームでも
って蒸発材料上を往復動させている。
By the way, the evaporation material 5
The shape of the electron beam E for irradiating the upper part is constant without changing within the moving range of the electron beam as shown by the solid line Sa and the dotted line Sb in FIG. 3, and the size thereof is very small for the reason described above. You are using the one on the spot.
In other words, it reciprocates on the evaporation material with an electron beam having a very large constant current density.

【0010】一方、蒸発材料5を回転させた場合、その
周速度は回転中心からの距離に比例して速くなる。つま
り蒸発材料の回転中心O部分はほとんど回転していな
い。従って、蒸発材料上を上述のように非常に大きな一
定の電流密度の電子ビームで移動させると、ほとんど回
転していない回転中心部分がその外周部分よりも強く加
熱されて早く蒸発するため、蒸発材料上において蒸発の
ムラが生じて均一な蒸着膜を形成することができなくな
ると共に、蒸発材料を一様に蒸発させることができなく
なる。また、最悪の場合には蒸発材料の回転中心部分に
ルツボ底部に到達する穴が形成されて蒸発作業ができな
くなる恐れがある。
On the other hand, when the evaporation material 5 is rotated, its peripheral speed increases in proportion to the distance from the center of rotation. That is, the center O of rotation of the evaporation material hardly rotates. Therefore, when the electron beam with a very large constant current density is moved on the evaporation material as described above, the rotation center part which is hardly rotating is heated more strongly than the outer peripheral part and evaporates earlier, so that the evaporation material As a result, uneven evaporation occurs, making it impossible to form a uniform evaporated film, and it becomes impossible to evenly evaporate the evaporation material. In the worst case, a hole reaching the bottom of the crucible may be formed in the center of rotation of the evaporation material, and evaporation work may not be possible.

【0011】そこで、本発明はかかる不都合を解決する
ために、蒸発材料を回転させながら電子ビームにより加
熱蒸発させるにあたり、蒸発ムラをなくして均一な蒸着
膜を形成すると共に蒸発材料を一様に蒸発させることの
できる蒸発方法を提供することを目的とするものであ
る。
Therefore, in order to solve such a problem, the present invention eliminates uneven evaporation and forms a uniform vapor deposition film when the evaporation material is heated and vaporized while being rotated, and the evaporation material is evenly vaporized. It is an object of the present invention to provide an evaporation method that can be performed.

【0012】[0012]

【課題を解決するための手段】上記目的を達成するた
め、本発明は回転している蒸発物質に電子ビームを照射
して蒸発させるにあたって、前記電子ビームを蒸発物質
の回転中心から半径方向に往復動させながら蒸発させる
方法において、前記蒸発物質に照射する電子ビームの形
状を蒸発物質の回転中心部とその外周部とで変化させる
ことにより蒸発物質上での電子ビームの電流密度を変化
させて蒸発させることを特徴とするものである。
In order to achieve the above object, the present invention irradiates a rotating vaporized substance with an electron beam to vaporize the vaporized substance, and reciprocates the electron beam in a radial direction from a rotation center of the vaporized substance. In the method of evaporating while moving, the shape of the electron beam with which the evaporative substance is irradiated is changed between the rotation center part of the evaporating substance and the outer peripheral part thereof to change the current density of the electron beam on the evaporating substance and evaporate. It is characterized by that.

【0013】[0013]

【実施例】以下、図面に基づいて本発明の実施例を詳説
する。
Embodiments of the present invention will be described below in detail with reference to the drawings.

【0014】図4は本発明に係る電子ビーム蒸発方法を
実施するための装置の一例を示す構成概略図であり、図
1,図2及び図3と同一番号のものは同一構成要素を示
すものである。
FIG. 4 is a schematic structural view showing an example of an apparatus for carrying out the electron beam evaporation method according to the present invention. The same reference numerals as those in FIGS. 1, 2 and 3 indicate the same constituent elements. Is.

【0015】該実施例において、図1及び図2と相違す
るところは蒸発源本体1に対してルツボ4を図示外のモ
ータ等により回転可能に組み込むと共に、一対の磁極6
a,6bの相対向する面に補助磁極片11a,11bを
夫々対向するように取り付けた点である。
In this embodiment, what is different from FIGS. 1 and 2 is that the crucible 4 is rotatably incorporated into the evaporation source body 1 by a motor or the like (not shown), and a pair of magnetic poles 6
The auxiliary magnetic pole pieces 11a and 11b are attached to the surfaces of a and 6b facing each other so as to face each other.

【0016】このように補助磁極片11a,11bを設
けることにより電子ビームが走査されるX方向のルツボ
4(蒸発材料5)の外周付近に形成される磁場が強くな
る。また、この各補助磁極片間に流れる磁束により第2
磁極片9a,9bの各開放端部間に形成される磁場が弱
くなる。その結果、磁極6a,6b及び第2の磁極片9
a,9bとの間に形成される偏向磁場BはX方向におい
て蒸発材料5の回転中心O部分が小さくて外周に向かう
につれて次第に高くなるような分布となる。従って、図
5に示すように偏向系10により電子ビームEが蒸発材
料5の回転中心O付近に近づくと、第2の磁極片9a,
9bの開放端に形成される磁場が弱いため、電子ビーム
に対するX方向の集束作用が弱まり、電子ビームの形状
は実線Sb´で示すように楕円状となるので電流密度は
小さくなる。そして、逆に電子ビームがX方向に沿って
蒸発材料5の外周部に近づくと補助磁極片11a,11
bにより磁場の強さが次第に増大するため、電子ビーム
に対するX方向の集束作用が徐々に強くなり、電子ビー
ムの形状は点線Sa´で示すようにスポット状になるの
で電流密度は高くなる。従って、蒸発材料上での電子ビ
ームの電流密度を回転中心から離れるに従って大きくな
るように連続的に変化させることができるため、回転し
ている蒸発材料に電子ビームを照射させても蒸発材料を
均一に加熱蒸発させることができる。
By thus providing the auxiliary magnetic pole pieces 11a and 11b, the magnetic field formed near the outer circumference of the crucible 4 (evaporation material 5) in the X direction scanned by the electron beam becomes strong. In addition, the magnetic flux flowing between the auxiliary pole pieces causes the second
The magnetic field formed between the open ends of the pole pieces 9a, 9b is weakened. As a result, the magnetic poles 6a and 6b and the second magnetic pole piece 9
The deflection magnetic field B formed between a and 9b has such a distribution that the rotation center O of the evaporation material 5 is small in the X direction and gradually increases toward the outer circumference. Therefore, as shown in FIG. 5, when the electron beam E approaches the rotation center O of the evaporation material 5 by the deflection system 10, the second pole piece 9a,
Since the magnetic field formed at the open end of 9b is weak, the focusing action in the X direction on the electron beam is weakened, and the shape of the electron beam becomes elliptic as shown by the solid line Sb ', so that the current density becomes small. On the contrary, when the electron beam approaches the outer peripheral portion of the evaporation material 5 along the X direction, the auxiliary magnetic pole pieces 11a, 11
Since the strength of the magnetic field gradually increases due to b, the focusing action in the X direction on the electron beam gradually becomes stronger, and the shape of the electron beam becomes a spot shape as shown by the dotted line Sa ′, so that the current density becomes high. Therefore, the current density of the electron beam on the evaporation material can be continuously changed so as to increase as the distance from the rotation center increases, so that the evaporation material can be made uniform even if the rotating evaporation material is irradiated with the electron beam. It can be heated and evaporated.

【0017】以上の説明は本発明の一例であり、実施に
あたっては幾多の変形が考えられる。例えば、図6に示
すように補助磁極片11a,11bを設けた状態で第2
の磁極片9a,9bを取り外しても、図5で示したよう
に電子ビームEの形状を蒸発材料5の回転中心O部分で
楕円上に照射させると共にその外周部分でスポット上に
照射させるようにすることができることが実験により確
認された。このように第2の磁極片がなくなれば、蒸発
材料動供給の自動化を容易に行うことが可能となり、ま
た、第2の磁極片に付着した蒸発物質が剥離してルツボ
内に落下することによるコンタミを防止することができ
る効果を有する。
The above description is one example of the present invention, and various modifications can be considered in the implementation. For example, when the auxiliary magnetic pole pieces 11a and 11b are provided as shown in FIG.
Even if the magnetic pole pieces 9a and 9b are removed, the shape of the electron beam E is irradiated on the ellipse at the rotation center O portion of the evaporation material 5 and on the spot at the outer peripheral portion thereof as shown in FIG. It was confirmed by experiments that this can be done. If the second magnetic pole piece is eliminated in this way, it becomes possible to easily automate the dynamic supply of the vaporized material, and the vaporized substance adhering to the second magnetic pole piece is separated and falls into the crucible. It has the effect of preventing contamination.

【0018】また、上記実施例では、蒸発材料上を走査
する電子ビームの形状を変化させるために、磁極6a,
6bに補助磁極片11a,11bを追加した場合を示し
たが、これに限定されることなく、例えば補助磁極片を
設けないで第2の磁極片の開放端の間隔を拡げても良
い。これは磁極片の間隔が広くなるにつれてその間に生
じる磁場が弱くなり、電子ビームEがルツボ5の外周部
から回転中心Oに向かうにつれてX方向の集束作用が弱
まるためである。
Further, in the above embodiment, in order to change the shape of the electron beam scanning the evaporation material, the magnetic poles 6a,
Although the case where the auxiliary magnetic pole pieces 11a and 11b are added to 6b is shown, the present invention is not limited to this, and the gap between the open ends of the second magnetic pole pieces may be widened without providing the auxiliary magnetic pole piece, for example. This is because the magnetic field generated between the magnetic pole pieces becomes weaker as the distance between the magnetic pole pieces becomes wider, and the focusing action in the X direction becomes weaker as the electron beam E moves from the outer peripheral portion of the crucible 5 toward the rotation center O.

【0019】さらに、上記の実施例では、180度偏向
型の電子ビーム蒸発源について述べたが、これに限定さ
れることなく270度偏向型にも同様に実施することが
できる。
Further, in the above-mentioned embodiment, the electron beam evaporation source of the 180-degree deflection type is described, but the present invention is not limited to this, and the electron beam evaporation source of the 270-degree deflection type can be similarly applied.

【0020】[0020]

【発明の効果】以上のようになせば、電子ビームの電流
密度を蒸発材料の回転中心とその外周部において変化さ
せることができるため、従来のように蒸発材料の回転中
心部が強く加熱されるのを防止することができる。その
結果、蒸発材料上において蒸発のムラが生じることなく
均一な蒸着膜を形成することができると共に、蒸発材料
を一様に蒸発させることができる。また、蒸発材料の回
転中心部分にルツボ底部に到達する穴が形成されて蒸発
作業ができなくなるという最悪の状態をなくすることが
できる。
As described above, since the current density of the electron beam can be changed at the rotation center of the evaporation material and its outer peripheral portion, the rotation center of the evaporation material is heated strongly as in the conventional case. Can be prevented. As a result, it is possible to form a uniform vapor deposition film on the evaporation material without causing unevenness of evaporation and to evaporate the evaporation material uniformly. Further, it is possible to eliminate the worst condition in which a hole reaching the bottom of the crucible is formed at the center of rotation of the evaporation material and the evaporation work cannot be performed.

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

【図1】従来装置を説明するための平面図である。FIG. 1 is a plan view for explaining a conventional device.

【図2】図1のAA断面図である。FIG. 2 is a sectional view taken along the line AA in FIG.

【図3】従来装置の動作を説明するための図である。FIG. 3 is a diagram for explaining the operation of the conventional device.

【図4】本発明に係る電子ビーム蒸発方法を実施するた
めの装置の一例を示す構成概略図である。
FIG. 4 is a schematic configuration diagram showing an example of an apparatus for carrying out the electron beam evaporation method according to the present invention.

【図5】本発明における動作を説明するための図であ
る。
FIG. 5 is a diagram for explaining the operation in the present invention.

【図6】本発明に係る電子ビーム蒸発方法を実施するた
めの装置の他の例を示す構成概略図である。
FIG. 6 is a schematic configuration view showing another example of the apparatus for carrying out the electron beam evaporation method according to the present invention.

【符号の説明】[Explanation of symbols]

1 蒸発源本体 2 電子銃 3 ビーム通過孔 4 ルツボ 5 蒸発物質 6a,6b 磁極 7 ヨーク 8a,8b 第1の磁極片 9a,9b 第2の磁極片 10 偏向系 11a,11b 補助磁極片 DESCRIPTION OF SYMBOLS 1 evaporation source main body 2 electron gun 3 beam passage hole 4 crucible 5 evaporation material 6a, 6b magnetic pole 7 yokes 8a, 8b first magnetic pole piece 9a, 9b second magnetic pole piece 10 deflection system 11a, 11b auxiliary magnetic pole piece

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 回転している蒸発物質に電子ビームを照
射して蒸発させるにあたって、前記電子ビームを蒸発物
質の回転中心から半径方向に往復動させながら蒸発させ
る方法において、前記蒸発物質に照射する電子ビームの
形状を蒸発物質の回転中心部とその外周部とで変化させ
ることにより蒸発物質上での電子ビームの電流密度を変
化させて蒸発させることを特徴とする電子ビーム蒸発方
法。
1. When irradiating a rotating evaporation material with an electron beam to evaporate the same, the method is to evaporate the electron beam while reciprocating in the radial direction from the rotation center of the evaporation material, and irradiating the evaporation material. An electron beam evaporation method, characterized in that the shape of an electron beam is changed between a rotation center part and an outer peripheral part of the evaporation substance to change the current density of the electron beam on the evaporation substance to evaporate.
JP16840292A 1992-06-03 1992-06-03 Electron beam evaporation method Expired - Fee Related JP3244532B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16840292A JP3244532B2 (en) 1992-06-03 1992-06-03 Electron beam evaporation method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16840292A JP3244532B2 (en) 1992-06-03 1992-06-03 Electron beam evaporation method

Publications (2)

Publication Number Publication Date
JPH05339714A true JPH05339714A (en) 1993-12-21
JP3244532B2 JP3244532B2 (en) 2002-01-07

Family

ID=15867460

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16840292A Expired - Fee Related JP3244532B2 (en) 1992-06-03 1992-06-03 Electron beam evaporation method

Country Status (1)

Country Link
JP (1) JP3244532B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2025105403A1 (en) * 2023-11-14 2025-05-22 株式会社オリジン Electron gun device for vapor deposition
CN120026284A (en) * 2025-04-23 2025-05-23 蒙城繁枫真空科技有限公司 An independent double-chamber electron gun evaporation coating equipment

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2025105403A1 (en) * 2023-11-14 2025-05-22 株式会社オリジン Electron gun device for vapor deposition
CN120026284A (en) * 2025-04-23 2025-05-23 蒙城繁枫真空科技有限公司 An independent double-chamber electron gun evaporation coating equipment

Also Published As

Publication number Publication date
JP3244532B2 (en) 2002-01-07

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