JP2779040B2 - Method and apparatus for supplying vapor deposition material - Google Patents
Method and apparatus for supplying vapor deposition materialInfo
- Publication number
- JP2779040B2 JP2779040B2 JP2075218A JP7521890A JP2779040B2 JP 2779040 B2 JP2779040 B2 JP 2779040B2 JP 2075218 A JP2075218 A JP 2075218A JP 7521890 A JP7521890 A JP 7521890A JP 2779040 B2 JP2779040 B2 JP 2779040B2
- Authority
- JP
- Japan
- Prior art keywords
- deposition material
- vapor deposition
- transfer
- liquid surface
- 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.)
- Expired - Fee Related
Links
- 239000000463 material Substances 0.000 title claims description 180
- 238000007740 vapor deposition Methods 0.000 title claims description 83
- 238000000034 method Methods 0.000 title claims description 23
- 239000007788 liquid Substances 0.000 claims description 92
- 230000008021 deposition Effects 0.000 claims description 43
- 238000001704 evaporation Methods 0.000 claims description 36
- 230000008020 evaporation Effects 0.000 claims description 35
- 239000010409 thin film Substances 0.000 claims description 32
- 238000001816 cooling Methods 0.000 claims description 20
- 239000000155 melt Substances 0.000 claims description 20
- 239000000758 substrate Substances 0.000 claims description 18
- 230000008018 melting Effects 0.000 claims description 17
- 238000002844 melting Methods 0.000 claims description 17
- 230000026058 directional locomotion Effects 0.000 claims description 6
- 238000010438 heat treatment Methods 0.000 claims description 5
- 238000000151 deposition Methods 0.000 description 24
- 239000010408 film Substances 0.000 description 21
- 230000007423 decrease Effects 0.000 description 15
- 239000000203 mixture Substances 0.000 description 11
- 230000015572 biosynthetic process Effects 0.000 description 7
- 238000010586 diagram Methods 0.000 description 5
- 238000010894 electron beam technology Methods 0.000 description 3
- 229910000599 Cr alloy Inorganic materials 0.000 description 2
- 230000001133 acceleration Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000002195 synergetic effect Effects 0.000 description 2
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 230000006399 behavior Effects 0.000 description 1
- 239000003990 capacitor Substances 0.000 description 1
- 239000012809 cooling fluid Substances 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 229910000701 elgiloys (Co-Cr-Ni Alloy) Inorganic materials 0.000 description 1
- 229910002804 graphite Inorganic materials 0.000 description 1
- 239000010439 graphite Substances 0.000 description 1
- 239000011344 liquid material Substances 0.000 description 1
- 230000033001 locomotion Effects 0.000 description 1
- CWQXQMHSOZUFJS-UHFFFAOYSA-N molybdenum disulfide Chemical compound S=[Mo]=S CWQXQMHSOZUFJS-UHFFFAOYSA-N 0.000 description 1
- 229910052982 molybdenum disulfide Inorganic materials 0.000 description 1
- 238000001771 vacuum deposition Methods 0.000 description 1
- 238000007738 vacuum evaporation Methods 0.000 description 1
- 238000009834 vaporization Methods 0.000 description 1
- 230000008016 vaporization Effects 0.000 description 1
- 239000011364 vaporized material Substances 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Physical Vapour Deposition (AREA)
Description
【発明の詳細な説明】 産業上の利用分野 本発明は、基板に薄膜を形成する際に、蒸着材料を被
加熱位置に供給する蒸着材料供給方法及びその装置に関
するものである。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method and apparatus for supplying a vapor deposition material to a heated position when a thin film is formed on a substrate.
従来の技術 例えば長尺フィルム上へ薄膜を形成して、コンデンサ
や磁気テープ等の素材となる機能性フィルムなどを真空
蒸着などによって作製するためには、長時間に亘って大
量の蒸気を発生させる必要がある。そのためには蒸発坩
堝などの被加熱位置において蒸着材料を連続的に供給す
ることが必要となってくる。その一つの方法に、例えば
日本学術振興会編「薄膜ハンドブック」(昭和58年発
行、オーム社刊、第105頁)に示されているように蒸着
材料を線材にして坩堝へ供給する方法がある。2. Description of the Related Art For example, in order to form a thin film on a long film and to produce a functional film or the like to be a material of a capacitor or a magnetic tape by vacuum deposition or the like, a large amount of steam is generated for a long time. There is a need. For that purpose, it is necessary to continuously supply the deposition material at a heated position such as an evaporation crucible. As one of the methods, there is a method in which a vapor-deposited material is supplied as a wire into a crucible as shown in, for example, “The Thin Film Handbook” edited by the Japan Society for the Promotion of Science (published in 1983, Ohmsha, p. 105). .
この方法は、蒸着材料がAl、Ni、Cuのように延性材料
であれば容易に線材化して適用できるが、Crのような脆
性材料では線材化は極めて困難である。This method can be easily applied to a wire if the deposition material is a ductile material such as Al, Ni, or Cu, but it is extremely difficult to apply a wire to a brittle material such as Cr.
また脆性材料でなくとも例えば磁性膜材料であるCo−
Cr合金あるいはCo−Cr−Ni合金のような硬質の材料は、
線材化できないことはないが加工性がよくないため加工
費が高価になり、実用的ではない。従ってこのような材
料は棒材で供給することになる。Further, even if it is not a brittle material, for example, Co-
Hard materials such as Cr alloy or Co-Cr-Ni alloy,
It is not impossible to make a wire rod, but the workability is not good, so the processing cost is high and it is not practical. Therefore, such a material is supplied in the form of a bar.
棒材で材料供給する場合の問題を第4図〜第10図を用
いて説明する。第4図において、1は坩堝2に収納され
た蒸着材料で、図示しない例えば公知の電子ビーム加熱
手段により加熱されて溶融している。3は棒状供給用蒸
着材料(以下棒材と略す)で、11、12、13はそれぞれ棒
材3を、案内する回転ローラ、14は駆動ローラである。
駆動ローラ14は、例えば図示しない公知のモータ等によ
り駆動されて、前記回転ローラ11との間に前記棒材3を
挟み込んで前記棒材3を矢印A方向に一定速度で、溶融
した蒸着材料1の液面4に向かって移送する。15、16
は、蒸着材料1の蒸気が前記各ローラ11、12、13、14に
付着することを防止するカバーである。The problem in the case where the material is supplied by a bar will be described with reference to FIGS. In FIG. 4, reference numeral 1 denotes a vapor deposition material contained in the crucible 2, which is heated and melted by, for example, a known electron beam heating means (not shown). Reference numeral 3 denotes a bar-shaped supply vapor deposition material (hereinafter abbreviated as a bar). Reference numerals 11, 12, and 13 denote rotating rollers for guiding the bar 3, respectively, and 14 denotes a driving roller.
The drive roller 14 is driven by, for example, a known motor (not shown) or the like, and sandwiches the bar 3 with the rotary roller 11 to melt the bar 3 at a constant speed in the direction of arrow A. To the liquid level 4. 15, 16
Is a cover for preventing the vapor of the vapor deposition material 1 from adhering to the rollers 11, 12, 13, and 14.
以上の構成により、長時間に亘って薄膜を形成するた
めに、坩堝2内の蒸着材料1が蒸発によって減少しない
ように棒材3が供給される。With the above configuration, in order to form a thin film over a long period of time, the rod material 3 is supplied so that the evaporation material 1 in the crucible 2 does not decrease due to evaporation.
棒材3の先端5が液面4に接した後の先端5の挙動
を、第5図〜第8図に基づいて説明する。The behavior of the tip 5 after the tip 5 of the bar 3 contacts the liquid level 4 will be described with reference to FIGS.
第5図は棒材3の先端5が液面4に接した瞬間の図
で、この瞬間を状態aとする。この状態aにおいて先端
5は液面4から熱を吸収して溶融を始め、溶液6となっ
て第6図に示す状態bの矢印Rのように蒸着材料1の溶
液に溶け込む。この時矢印Rと逆方向に熱が先端5に伝
わり先端5の溶融が進む。溶融が進につれて液面4と棒
材3の先端5の距離gが長くなるので液面4からの熱が
先端5に伝わりにくくなり、第7図の状態cのように先
端5の溶融量が減少して前記溶融6の量が少なくなる。
そうするとますます先端5は溶融しにくくなってついに
は第8図の状態dのように溶融が停止する。FIG. 5 is a view at the moment when the tip 5 of the bar 3 comes into contact with the liquid surface 4, and this moment is referred to as a state a. In this state a, the tip 5 absorbs heat from the liquid level 4 and starts to melt, becoming a solution 6 and dissolving in the solution of the vapor deposition material 1 as indicated by the arrow R in the state b shown in FIG. At this time, heat is transmitted to the tip 5 in a direction opposite to the arrow R, and the melting of the tip 5 proceeds. As the melting progresses, the distance g between the liquid surface 4 and the tip 5 of the rod 3 increases, so that heat from the liquid surface 4 is less likely to be transmitted to the tip 5, and the amount of melting at the tip 5 as shown in state c in FIG. The amount of the melt 6 decreases and decreases.
Then, the tip 5 becomes more difficult to melt, and finally the melting stops as shown in the state d in FIG.
この間棒材3は前記矢印A方向に連続して送られてい
るがその速さよりも状態aから状態dまでの先端5の溶
融速度の方が速いので状態dのようにスキマDが生じる
ことになる。そして連続して棒材3が送られてくるので
時間が経過するにつれてスキマDが小さくなってついに
は状態aとなり、順次以上のサイクルが繰り返されるこ
とになる。すなわち棒材3の送りは連続であっても液面
4への棒材3の供給は間欠的なものとなる。During this time, the rod material 3 is continuously fed in the direction of the arrow A. However, since the melting speed of the tip 5 from the state a to the state d is faster than the speed, the gap D occurs as in the state d. Become. Since the bars 3 are continuously fed, the gap D becomes smaller as time elapses, and finally reaches the state a, and the above cycle is repeated sequentially. That is, even though the feed of the bar 3 is continuous, the supply of the bar 3 to the liquid surface 4 is intermittent.
先端5が液面に溶け込んでいる間は液面4から熱を奪
うので液面4の温度が低下する。そうすると蒸発速度が
低下することになり、蒸発速度は第9図に示すように時
間経過と共に周期的に変動することになる。状態dの距
離Dは棒材3の径が太くなるほど大きくなる。その理由
は前記溶液6を略円筒とした場合、径が太くなるほど
(円筒表面積/円筒容積)が小さくなるので液面4から
先端5へ溶液6を通って伝わる熱量に対して円筒表面か
ら輻射で逃げる熱量の割合が少なくなってより長く溶融
するためである。従って棒材の径が太くなると第9図の
周期TL及び蒸発速度の変動幅HL共に大きくなる。While the tip 5 is melting into the liquid surface, heat is taken from the liquid surface 4, so that the temperature of the liquid surface 4 decreases. Then, the evaporation rate decreases, and the evaporation rate periodically fluctuates with time as shown in FIG. The distance D in the state d increases as the diameter of the bar 3 increases. The reason is that, when the solution 6 is substantially cylindrical, the larger the diameter is, the smaller (cylindrical surface area / cylindrical volume) is, so the amount of heat transmitted from the liquid surface 4 to the tip 5 through the solution 6 is radiated from the cylindrical surface. This is because the ratio of the amount of heat that escapes is reduced and the material is melted for a longer time. Thus the diameter of the bar is the both larger Figure 9 period T L and fluctuations in evaporation rate width H L thick.
蒸発速度が変動すると坩堝2の上方を、図示しない基
板やフィルム等を移動させながら蒸着するいゆる通過製
膜するときに通過方向の膜厚の変動が発生するという大
きな問題があった。If the evaporation rate fluctuates, there is a serious problem that the thickness of the film in the passing direction fluctuates when performing vapor deposition while moving a substrate or a film (not shown) above the crucible 2 while moving the substrate or film.
この問題に対応するために従来は棒材を溶融した後坩
堝へ供給するという第10図に示す方法が用いられること
がある。この方法を第4図と同一構成要素は同番号にて
説明する。第10図において棒材3の先端5に公知の電子
ビーム7を照射して溶融し、その溶液6を液面に供給す
ると液面4の温度が前例のように低下しないので蒸発速
度が変動することはない。従って坩堝2の上方で基板8
に紙面に垂直方向に通過製膜しても薄膜9の膜厚が変動
することはない。To cope with this problem, a method shown in FIG. 10 in which a bar is melted and then supplied to a crucible is conventionally used in some cases. This method will be described with the same reference numerals as those of FIG. In FIG. 10, when the tip 5 of the bar 3 is irradiated with a known electron beam 7 and melted, and the solution 6 is supplied to the liquid surface, the evaporation rate fluctuates because the temperature of the liquid surface 4 does not decrease as in the previous example. Never. Therefore, the substrate 8 is placed above the crucible 2.
The thickness of the thin film 9 does not fluctuate even when the film is formed in the direction perpendicular to the paper surface.
しかしながら蒸着材料1が、蒸発速度が相異なる成分
から成る例えば磁性膜材料であるCo−Cr合金の場合、Cr
はCoよりも蒸発速度が高いので目的とする薄膜のCr含有
量をMとし、その含有量Mの薄膜が得られる時の薄膜材
料1のCr含有量をYとするM>Yである。また液面4か
ら発生する蒸気のCr含有量はMに等しい。従って蒸発し
た量だけCr含有量Mの材料を供給してやれば坩堝2内の
薄膜材料1の量を一定に保ちつつCr含有量Mの薄膜を連
続して蒸着できることになる。However, when the vapor deposition material 1 is, for example, a Co—Cr alloy that is a magnetic film material composed of components having different evaporation rates,
Since the evaporation rate is higher than that of Co, M> Y where Cr is the content of the target thin film and Y is the Cr content of the thin film material 1 when a thin film having the content M is obtained. The Cr content of the vapor generated from the liquid level 4 is equal to M. Therefore, if a material having a Cr content of M is supplied by the amount evaporated, a thin film having a Cr content of M can be continuously deposited while the amount of the thin film material 1 in the crucible 2 is kept constant.
しかしながら第10図の構成では電子ビーム7で溶融さ
れた溶液6のCr含有量はMであるから溶液6から発生す
る蒸気のCr含有量はMよりも大きくなる。However, in the structure of FIG. 10, the Cr content of the solution 6 melted by the electron beam 7 is M, so that the Cr content of the vapor generated from the solution 6 is larger than M.
そうすると基板8の向かって右方に形成される薄膜の
Cr含有量は溶液6に近いので多くなり、左方に形成され
る薄膜のCr含有量はその逆に少なくなるため、基板8の
全幅に亘って一定組成の薄膜9が形成できないという大
きな問題があった。Then, the thin film formed on the right side of the substrate 8
Since the Cr content is high because it is close to the solution 6, the Cr content of the thin film formed on the left is conversely small, and there is a major problem that the thin film 9 having a constant composition cannot be formed over the entire width of the substrate 8. there were.
そこで本発明者は、真空蒸着する際に蒸着速度変動が
小さく、また蒸発速度が相異なる複数の成分から成る薄
膜を形成する場合にも基板上にその面方向に成分の含有
量の差の小さい薄膜を形成できる蒸着材料供給方法及び
その装置を発明し、出願した(特願平1−156520)。そ
の発明の骨子は、坩堝内で溶融された蒸着材料に向かっ
て移送される供給用長尺蒸着材料の移送速度を、前記蒸
着材料に向かう方向を+、前記蒸着材料から遠ざかる方
向を−としたとき、交互に+方向と−方向に切り替え、
すなわち往復動作させ、平均として+方向とするもので
ある。Therefore, the present inventor has found that, when forming a thin film composed of a plurality of components having different evaporation rates during vacuum evaporation, the difference in the content of components in the plane direction is small even when a thin film composed of a plurality of components having different evaporation rates is formed. The inventors of the present invention have invented a method and apparatus for supplying a deposition material capable of forming a thin film, and have filed an application (Japanese Patent Application No. 1-156520). The gist of the invention is as follows. The transfer speed of the supply long vapor deposition material transferred toward the vapor deposition material melted in the crucible is defined as + in the direction toward the vapor deposition material and − in the direction away from the vapor deposition material. At that time, it alternately switches between + direction and-direction,
That is, the reciprocating operation is performed, and the average is set to the + direction.
その内容の1例を第11図に於て説明する。尚、従来と
同一構成要素は従来例と同一番号で示すものである。第
11図はその発明の1実施例を示す図である。第11図にお
いて、20はモータで、駆動回路21により駆動されて前記
駆動ローラ14を回転させる。モータ20は図示しない真空
チャンバ内に設置しても、あるいは外部に設置し、公知
の回転導入器を介して駆動ローラ14を回転させてもよ
い。22は演算回路で、棒材3の平均移送速度指令
(VAV)24とメモリ23のデータに基づいて前記モータ20
の速度パターンを演算し、それを速度指令25として前記
駆動回路21に送出する。One example of the contents will be described with reference to FIG. The same components as those of the conventional example are indicated by the same numbers as those of the conventional example. No.
FIG. 11 shows an embodiment of the present invention. In FIG. 11, reference numeral 20 denotes a motor, which is driven by a drive circuit 21 to rotate the drive roller 14. The motor 20 may be installed in a vacuum chamber (not shown) or may be installed outside, and the driving roller 14 may be rotated via a known rotation introducing device. Numeral 22 denotes an arithmetic circuit which controls the motor 20 based on an average transfer speed command (V AV ) 24 of the bar 3 and data in the memory 23.
And sends it to the drive circuit 21 as a speed command 25.
次に速度パターン演算の一例を第12図に示す。第12図
に於て移送速度vは第11図の前記棒材3の移送速度を示
し、+は矢印A方向、−は矢印Aと逆方向の速度をそれ
ぞれ示すものとする。速度パターンは+方向、−方向共
に台形波状である。演算を簡単にするため+方向、−方
向共に最高速度(VMAX)は同一であり、速度0から速度
VMAXまでの加減速、すなわち角度α1、α2、α3、α
4も共に同一とする。また移送速度が+方向から−方向
に転じる時及びその逆の時、第11図に示す各ローラやモ
ータ等からなる棒材供給機構に過大な力がかからないよ
うに、あるいは前記演算に必要な時間として休止時間T
FS、TBSをそれぞれ設けてあるが必ずしも必要ではな
い。Next, an example of the speed pattern calculation is shown in FIG. In FIG. 12, the transfer speed v indicates the transfer speed of the bar 3 in FIG. 11, and + indicates the speed in the direction of arrow A, and-indicates the speed in the direction opposite to arrow A. The speed pattern has a trapezoidal wave shape in both the + and-directions. In order to simplify the calculation, the maximum speed (V MAX ) is the same in both the + direction and the-direction.
Acceleration / deceleration to V MAX , that is, angles α 1 , α 2 , α 3 , α
4 are the same. Also, when the transfer speed changes from the + direction to the-direction and vice versa, the bar supply mechanism including the rollers and motors shown in FIG. Pause time T as
FS, but are provided respectively T BS is not always necessary.
速度が+方向の台形波の面積が矢印A方向への移送量
Fを、一方向の台形波の面積が矢印Aと逆方向への移送
量Bをそれぞれ表わすことになる。TFD、TBDはそれぞれ
+方向移送正味時間、一方向移送正味時間である。以上
に於て平均移送速度(VAV)は式(1)で表わされる。The area of the trapezoidal wave whose velocity is in the positive direction indicates the amount of transfer F in the direction of arrow A, and the area of the trapezoidal wave in one direction indicates the amount of transfer B in the direction opposite to arrow A. T FD and T BD are the net time for one-way transfer and the net time for one-way transfer, respectively. In the above, the average transfer speed (V AV ) is represented by equation (1).
VAV=(F−B)/(TFD+TBD+TFS+TBS) …(1) またTFDは(2)式より算出することができる。V AV = (F−B) / (T FD + T BD + T FS + T BS ) (1) Further, T FD can be calculated from the equation (2).
TFD=TBD+[(F−B)/VMAX] …(2) 尚,VAVは従来と同様に坩堝2内の蒸着材料1が蒸発に
よって減少しないように、すなわち蒸発した量を補える
よう設定される。T FD = T BD + [(F−B) / V MAX ] (2) Note that V AV can compensate for the evaporation amount of the evaporation material 1 in the crucible 2 as in the related art, that is, the evaporation amount. It is set as follows.
距離Bを第12図の距離K1(=D/sinθ1)と同一ある
いはK1よりも大きくしておいて、すなわち棒材の先端5
と液面4が分離するまで−方向に送るようにして第12図
の速度パターンで棒材を駆動すると、第12図の時間0で
棒材3が第8図状態dにあったとすると時間T1で第5図
状態aとなり、時間がT1からT2まで経過するにつれて第
6図状態b、第7図状態c、第8図状態dの順に棒材3
は前記蒸着材料1の溶液に溶け込む。前記速度パターン
の1周期TSが従来の第9図の1周期TLの例えば1/10とな
るようにその速度パターンが設定されているとする。そ
うすると1周期に前記蒸着材料1の溶液に溶け込む棒材
3の量を、従来の1/10とすることができる。溶け込む量
が少なくなると液面4から奪う熱量も少なくなるので液
面4の温度低下も少なくなる。そうすると蒸発速度の低
下も少なくなり、蒸発速度は第13図に示すように時間経
過と共に周期TSで変動するがその変動幅HSは従来のそれ
HLの約1/10にすることができる。従って通過製膜におけ
る膜厚の均一性を向上させることができる。Distance the distance B of Fig. 12 K 1 (= D / sinθ 1 ) in advance to be larger than the same or K 1 and, namely the tip of the bar 5
When the bar is driven in the speed pattern of FIG. 12 so that the bar 3 is moved in the negative direction until the liquid level 4 is separated from the liquid surface 4, if the bar 3 is in the state d in FIG. 8 at time 0 in FIG. 1 in FIG. 5 state a, and the Figure 6 condition b as time elapses from T 1 to T 2, Fig. 7 state c, the bar 3 in the order of FIG. 8 state d
Dissolves in the solution of the vapor deposition material 1. It is assumed that the speed pattern is set such that one cycle T S of the speed pattern is, for example, 1/10 of one cycle T L of the related art in FIG. Then, the amount of the rod 3 dissolved in the solution of the vapor deposition material 1 in one cycle can be reduced to 1/10 of the conventional amount. When the amount of the melt decreases, the amount of heat taken from the liquid surface 4 also decreases, so that the temperature decrease of the liquid surface 4 also decreases. Then reduction in evaporation rate is also reduced, the evaporation rate is the variation width H S varies period T S with time lapse as shown in FIG. 13 that of the prior
It can be about 1/10 of H L. Therefore, the uniformity of the film thickness in the pass film formation can be improved.
また第14図に示すように先端5が液面4に接すると先
端5は融けて溶液6となる。棒材3が前記した蒸発速度
の相異なる成分から成る例えばCoとCrの合金である場
合、前記したように溶液6中のCrの含有量は蒸着材料1
の溶液のそれよりも多いが溶液6は蒸着材料1中に矢印
Eに示すように拡散して薄められる。従って溶液6から
直接蒸発するCr含有量の多い蒸気の発生は少なくなるの
で、第11図において基板8に形成される薄膜9の向かっ
て右側の部分のCr含有量の増加を抑制することができ、
薄膜の幅方向の成分の含有量の均一性を向上させること
ができる等の効果を有するものである。When the tip 5 contacts the liquid surface 4 as shown in FIG. 14, the tip 5 melts and becomes a solution 6. When the rod 3 is, for example, an alloy of Co and Cr composed of components having different evaporation rates as described above, the content of Cr in the solution 6 depends on the deposition material 1 as described above.
Although the solution 6 is larger than that of the above solution, the solution 6 is diffused into the vapor deposition material 1 as shown by an arrow E and is diluted. Therefore, since the generation of the vapor having a high Cr content that evaporates directly from the solution 6 is reduced, the increase in the Cr content in the right portion of the thin film 9 formed on the substrate 8 in FIG. 11 can be suppressed. ,
This has the effect that the uniformity of the content of the component in the width direction of the thin film can be improved.
発明が解決しようとする課題 その後の当発明者による研究の結果、蒸着速度変動を
小さくするには、「供給材料が液面に接して溶融する時
に一時に大量に供給材料が液面に溶け込まないように
し、液面の温度低下を小さくして蒸発速度の低下を小さ
くする」すなわち第12図においてVAVを同一とすれば1
周期TS(=TFD+TBD+TFS+TBS)を小さくする、すなわ
ち1往復当りの送り量(F−B)を小さくする」という
条件の他に更に一つの条件「供給材料が前記液面に接し
て溶融しその液面にとけ込む量が、1+−方向動作、す
なわち1往復動作当りの前記供給材料の前進量を越えな
い」すなわち「往復動作毎に供給材料が略等量液面に接
触する」を満たす必要があるとの新たな知見を得た。Problems to be Solved by the Invention As a result of research conducted by the present inventors, it was found that, in order to reduce the variation in deposition rate, `` a large amount of the feed material does not dissolve into the liquid surface at a time when the feed material comes into contact with the liquid surface and melts. and so, to reduce the decrease in the evaporation rate by decreasing the temperature drop of the liquid surface "or if the V AV the same in Figure 12 1
In addition to the condition that the period T S (= T FD + T BD + T FS + T BS ) is reduced, that is, the feed amount per reciprocation (F−B) is reduced ”, one more condition“ the feed material is the liquid level The amount of material that melts and melts on the liquid surface does not exceed the 1 + -direction operation, that is, does not exceed the advancing amount of the feed material per one reciprocating operation. To do so ".
この条件を満たさない場合は、次に説明するような蒸
着速度変動を生じることがわかった。棒材3を坩堝2内
の蒸着材料1の液面4に前記の方法で往復動供給させて
棒材3の溶解する様子を観察すると第15図(a′)、
(b′),(c′),(d′)に示すように棒材3は状
態a′,b′,c′,d′の順に液面4に接触してから後退す
る。この時状態d′においては、棒材3の下部に滴3′
が垂れているのが観察される。この滴3′が原因となっ
て第16図(f′)、(g′)、(h′)・・・
(p′)、(q′)、(f′)、(g′)、(h′)・
に示すような現象が発生する。第16図は往復動供給され
る棒材3の溶融状態を示す図で、状態f′、g′、h′
・・・p′、q′、f′、g′、h′・・・の順に動作
が繰り返される。状態f′、h′、j′・・・が第12図
のT1、すなわち棒材が前進を終了した状態であり、状態
g′、i′、k′・・・が第12図のT2、すなわち棒材が
後退を終了した状態を示す。状態f′とg′の間、h′
とi′の間等の滴3′と液面4が接触して後退するとき
はいずれも第15図の経過をたどるものとする。第16図に
おいては説明をわかりやすくするために第15図よりも滴
3′の垂れ量を大きく誇張して示してある。ここでMeは
棒材3が液面4と接触して液面4と離れるまでに液面4
にとけ込む量であり、第16図に示すようにMe>(F−
B)、すなわち「供給材料が前記液面に接して溶融しそ
の液面にとけ込む量が、1+−方向動作、すなわち1往
復動作当りの前記供給材料の前進量を越える」条件にあ
るとする。そうすると棒材3が往復動作を繰り返すから
第15図のa′からd′の動作が繰り返される。Me>(F
−B)であるから徐々に液面4と棒材3の接触量が少な
くなりついには状態p′のように接触しなくなる。接触
量が多いときはとけ込み量が多くなり液面4の温度低下
が大きくなって蒸発速度が下がり、少なくなるにつれて
とけ込み量が少なくなって温度が上昇して蒸発速度が上
がり、蒸発速度は第13図の周期TAで振幅HAのように変動
するという大きな問題が発生する。また供給材料が相異
なる蒸発速度の複数の成分から構成されている場合にお
いては、前記したように供給材料には蒸発速度の高い材
料を溶液よりもより多く含有させることになる。従って
前記のように棒材と液面の接触量が変化して棒材が液面
にとけ込む量が変化すると液面から発生す蒸気の組成比
も変化し、通過製膜するときに通過方向の組成比の変動
が発生するという大きな問題があった。When this condition is not satisfied, it has been found that the evaporation rate fluctuation as described below occurs. FIG. 15 (a ′) shows that the rod 3 is reciprocated and supplied to the liquid surface 4 of the vapor deposition material 1 in the crucible 2 by the above-described method and the rod 3 is melted.
As shown in (b '), (c'), and (d '), the rod 3 comes into contact with the liquid surface 4 in the order of states a', b ', c', and d 'and then recedes. At this time, in the state d ', the drop 3'
Is observed to hang. 16 (f '), (g'), (h ')... Due to the drop 3'.
(P '), (q'), (f '), (g'), (h ')
The phenomenon shown in FIG. FIG. 16 is a view showing a molten state of the bar material 3 supplied in a reciprocating motion, and states f ', g', and h '.
The operation is repeated in the order of p ', q', f ', g', h ',. State f ', h', j '... Is T 1 in FIG. 12, that is, the state in which the bar has finished moving forward, and states g ′, i ′, k ′. 2 , that is, a state in which the bar has finished retreating. Between states f 'and g', h '
When the drop 3 'and the liquid surface 4 between the positions i and i' come back in contact with each other, the course shown in FIG. 15 is followed. In FIG. 16, the amount of dripping of the droplet 3 'is exaggerated more than in FIG. 15 for easy understanding. Here, Me is the liquid surface 4 until the rod 3 comes into contact with the liquid surface 4 and separates from the liquid surface 4.
And Me> (F−
B), i.e., the condition that "the amount of the supplied material which is in contact with the liquid level and melts and melts at the liquid level exceeds the 1 + -direction operation, that is, exceeds the advance amount of the supplied material per one reciprocating operation". Then, since the bar 3 repeats the reciprocating operation, the operations from a 'to d' in FIG. 15 are repeated. Me> (F
-B), the contact amount between the liquid surface 4 and the rod 3 gradually decreases, and finally the contact stops as in the state p '. When the contact amount is large, the melting amount increases, the temperature drop of the liquid surface 4 increases, and the evaporation rate decreases. As the contact amount decreases, the melting amount decreases, the temperature increases, the evaporation rate increases, and the evaporation rate increases. major problem of variation as the amplitude H a generated in the period T a of FIG. 13. When the feed material is composed of a plurality of components having different evaporation rates, as described above, the feed material contains a material having a high evaporation rate more than the solution. Therefore, as described above, when the amount of contact between the rod and the liquid surface changes and the amount of the rod that melts into the liquid surface changes, the composition ratio of the vapor generated from the liquid surface also changes, and when passing through the film, the composition ratio in the passing direction changes. There was a big problem that the composition ratio fluctuated.
そこで本発明は、このような課題を解決するものであ
って、真空蒸着する際に蒸着速度変動が小さく、また蒸
発速度が相異なる複数の成分から成る薄膜を形成する場
合にも蒸気の組成比の変動の小さい薄膜を形成できる蒸
着材料供給方法及びその装置を提供することを目的とす
るものである。Therefore, the present invention is to solve such a problem, and the vapor deposition rate fluctuation during vacuum vapor deposition is small, and the vapor composition ratio can be reduced even when a thin film composed of a plurality of components having different vaporization rates is formed. It is an object of the present invention to provide a method and an apparatus for supplying a vapor deposition material capable of forming a thin film having a small fluctuation in the material.
課題を解決するための手段 請求項1の本発明は、坩堝に収納された蒸着材料を加
熱して溶融し、その蒸着材料から発生する蒸気を基板に
付着せしめて薄膜を形成するため、前記蒸着材料を蒸着
材料液面に向かって供給する蒸着材料供給方法におい
て、前記坩堝内で溶融された蒸着材料液面に向かって移
送される供給用長尺蒸着材料の移送速度を、前記液面に
向かう方向を+、前記液面から遠ざかる方向を−とした
とき、交互に+方向と−方向に切り替え、平均として+
方向とすると共に、前記蒸着材料が前記液面に接して溶
融しその液面にとけ込む量が、1+−方向動作当りの前
記蒸着材料の前進量を越えないように前記移動量を設定
することを特徴とする蒸着材料供給方法である。Means for Solving the Problems According to the present invention, the vapor deposition material contained in a crucible is heated and melted, and vapor generated from the vapor deposition material is attached to a substrate to form a thin film. In a vapor deposition material supply method for supplying a material toward a liquid surface of a vapor deposition material, a transfer speed of a long evaporating material for supply transferred toward a liquid surface of the vaporized material melted in the crucible is increased toward the liquid surface. When the direction is + and the direction away from the liquid surface is-, the direction is alternately switched to the + and-directions, and the average is +
The moving amount is set so that the amount of the vapor deposition material in contact with the liquid surface and melting and melting into the liquid surface does not exceed the advance amount of the vapor deposition material per 1 + -direction operation. This is a characteristic method of supplying a deposition material.
請求項2の本発明は、坩堝に収納された蒸着材料を加
熱して溶融し、その蒸着材料から発生する蒸気を基板に
付着せしめて薄膜を形成する際、前記坩堝内で溶融され
た蒸着材料に向かって移送される供給用長尺蒸着材料の
移送速度を、前記蒸着材料に向かう方向を+、前記蒸着
材料から遠ざかる方向を−としたとき、交互に+方向と
−方向に切り替えて蒸着材料を坩堝に供給する蒸着材料
供給装置であって、前記供給用長尺蒸着材料の平均移送
速度(VAV)指令に基づいて VAV=(F−B)/(TFD+TBD+TFS+TBS) …(1) なお、F :+方向移送量 B :−方向移送量(一定) TFD:+方向移送正味時間 TFS:+方向移送休止時間(一定) TFS≧0 TBD:−方向移送正味時間(一定) TBS:−方向移送休止時間(一定) TBS>TFS なる演算を行い、算出されたFとTFDにて供給用長尺蒸
着材料を駆動する制御手段を備えたことを特徴とする蒸
着材料供給装置である。The present invention according to claim 2 is that, when the vapor deposition material stored in the crucible is heated and melted, and the vapor generated from the vapor deposition material is attached to the substrate to form a thin film, the vapor deposition material melted in the crucible When the transfer speed of the supply long deposition material transferred toward the deposition material is + in the direction toward the deposition material and-in the direction away from the deposition material, the deposition material is alternately switched to the + and-directions. the a deposition material supplying device for supplying to the crucible, the average transfer rate of supply long deposition material (V AV) V on the basis of a command AV = (F-B) / (T FD + T BD + T FS + T BS ) ... (1) F: + direction transfer amount B:-direction transfer amount (constant) T FD : + direction transfer net time T FS : + direction transfer pause time (constant) T FS ≥ 0 T BD :-direction transferring the net time (constant) T BS: - directional movement quiescent time (constant) performed T BS> T FS becomes operational, calculated Is an evaporation material supply apparatus characterized by comprising a control means for driving the feed long deposition material at have been F and T FD.
請求項3の本発明は、坩堝に収納された蒸着材料を加
熱して溶融し、その蒸着材料から発生する蒸気を基板に
付着せしめて薄膜を形成する際に坩堝内で溶融された蒸
着材料に向かって移送される供給用長尺蒸着材料の移送
速度を、前記蒸着材料に向かう方向を+、前記蒸着材料
から遠ざかる方向を−としたとき、交互に+方向と−方
向に切り替えて蒸着材料を坩堝に供給する蒸着材料供給
装置であって、供給用長尺蒸着材料の平均移送速度(V
AV)指令に基づいて VAV=(F−B)/(TFD+TBD+TFS+TBS) …(1) なお、F :+方向移送量(一定) B :−方向移送量(一定) TFD:+方向移送正味時間(一定) TFS:+方向移送休止時間(一定) TFS≧0 TBD:−方向移送正味時間(一定) TBS:−方向移送休止時間 TBS>TFS なる演算を行い、算出されたTBSにて供給用長尺蒸着材
料を駆動する制御手段を備えたことを特徴とする蒸着材
料供給装置である。According to the present invention of claim 3, the vapor deposition material contained in the crucible is heated and melted, and the vapor generated from the vapor deposition material is attached to the substrate to form a thin film. When the transfer speed of the supply long deposition material transferred toward the deposition material is +, the direction toward the deposition material is +, and the direction away from the deposition material is-, the deposition material is alternately switched to the + direction and the-direction. An apparatus for supplying a vapor deposition material to a crucible, wherein the average transport speed (V
AV ) Based on the command, VAV = (FB) / ( TFD + TBD + TFS + TBS ) (1) where F: positive direction transfer amount (constant) B: negative direction transfer amount (constant) T FD : + direction net transfer time (constant) T FS : + direction transfer pause time (constant) T FS ≥ 0 T BD :-direction transfer net time (constant) T BS :-direction transfer pause time T BS > T FS performs the operation, a vapor deposition material supply apparatus characterized by comprising a control means for driving the feed long deposition material at the calculated T BS.
請求項4の本発明は、坩堝に収納された蒸着材料を加
熱して溶融し、その蒸着材料から発生する蒸気を基板に
付着せしめて薄膜を形成する手段と、前記坩堝内で溶融
された蒸着材料液面に向かって移送される供給用長尺蒸
着材料の移送速度を、前記液面に向かう方向を+、前記
液面から遠ざかる方向を−としたとき、交互に+方向と
−方向に切り替え、平均として+方向として前記蒸着材
料を移送するする蒸着材料移送手段と、前記液面に向か
う前記蒸着材料の先端部近傍を冷却する手段とを備えた
ことを特徴とする蒸着材料供給装置である。The present invention according to claim 4 is a means for heating and melting a vapor deposition material contained in a crucible, adhering vapor generated from the vapor deposition material to a substrate to form a thin film, and a vapor deposition material melted in the crucible. When the transfer speed of the supply long vapor deposition material transferred toward the material liquid level is + in the direction toward the liquid surface and-in the direction away from the liquid surface, the transfer speed is alternately switched between the + direction and the-direction. A vapor deposition material transporting means for transporting the vapor deposition material as a + direction on average, and a means for cooling the vicinity of the tip end of the vapor deposition material toward the liquid level. .
請求項5の本発明は、坩堝に収納された蒸着材料を加
熱して溶融し、その蒸着材料から発生する蒸気を基板に
付着せしめて薄膜を形成する手段と、前記坩堝内で溶融
された蒸着材料液面に向かって移送される供給用長尺蒸
着材料の移送速度を、前記液面に向かう方向を+、前記
液面から遠ざかる方向を−としたとき、交互に+方向と
−方向に切り替え、平均として+方向として前記蒸着材
料を移送するする蒸着材料移送手段と、前記液面に向か
う前記蒸着材料の先端部近傍を冷却する手段とを備えた
蒸着材料供給装置であって、供給用長尺蒸着材料の平均
移送速度(VAV)指令に基づいて VAV=(F−B)/(TFD+TBD+TFS+TBS) …(1) F :+方向移送量 B :−方向移送量 TFD:+方向移送正味時間 TFS:+方向移送休止時間 TFS≧0 TBD:−方向移送正味時間 TBS:−方向移送休止時間 TBS>TFS なる演算を行い、算出された各々の値にて供給用長尺蒸
着材料を駆動する制御手段を備えたことを特徴とする蒸
着材料供給装置である。The present invention according to claim 5 is a means for heating and melting a vapor deposition material stored in a crucible, attaching vapor generated from the vapor deposition material to a substrate to form a thin film, and forming a thin film in the crucible. When the transfer speed of the supply long vapor deposition material transferred toward the material liquid level is + in the direction toward the liquid surface and-in the direction away from the liquid surface, the transfer speed is alternately switched between the + direction and the-direction. A vapor deposition material supply device comprising: a vapor deposition material transporting means for transporting the vapor deposition material as a + direction on average; and a means for cooling the vicinity of the tip of the vapor deposition material toward the liquid level, wherein the average transfer rate of scale deposition material (V AV) V AV = ( F-B) based on the command / (T FD + T BD + T FS + T BS) ... (1) F: + directional movement amount B: - directional movement amount T FD : + direction transfer net time T FS : + direction transfer pause time T FS ≧ 0 T BD : − Direction transfer net time T BS : −direction transfer pause time T BS > T FS calculation, and control means for driving the supply long deposition material at each calculated value is provided. It is a material supply device.
作用 請求項1記載の本発明は上記構成により、往復動作毎
に供給材料が略等量液面に接触させることができるの
で、毎回等量供給材料を溶液に溶け込ませることが可能
となるので液面の温度変動が小さくなり蒸発速度変動も
小さくなる。その結果通過製膜における膜厚の変動が小
さくなるので膜厚の均一性を向上させることができる。According to the present invention, the supply material can be brought into contact with the liquid surface at substantially the same amount for each reciprocating operation, so that the same amount of the supply material can be dissolved in the solution each time. Surface temperature fluctuations are reduced, and evaporation rate fluctuations are also reduced. As a result, the variation of the film thickness in the pass-through film formation is reduced, so that the uniformity of the film thickness can be improved.
また棒材が相異なる蒸発速度の複数の成分から構成さ
れている場合においても、上記の組成比の変動を小さく
できる。その結果、通過製膜するときに通過方向の組成
比の均一性を向上させることができる。In addition, even when the bar is composed of a plurality of components having different evaporation rates, the above-described variation in the composition ratio can be reduced. As a result, it is possible to improve the uniformity of the composition ratio in the passing direction when performing the passing film formation.
請求項2記載の本発明は上記したように、TFSを短く
しているので液面と棒材との接触時間が短くなるので両
者の接触時に棒材が液面にとけ込む量を少なくすること
ができる。一方、TBSを長くしているのでVAVが同一であ
れば式(1)の分母が大きくなり式(1)の(F−B)
すなわち棒材1往復当りの供給量を大きくすることがで
きる。従って、それらの相乗効果で容易に前記条件「供
給材料が前記液面に接して溶融しその液面にとけ込む量
が、1+−方向動作、すなわち1往復動作当りの前記供
給材料の前進量を越えない」すなわち「往復動作毎に供
給材料が略等量液面に接触する」を満たすことが出来る
ようになり、上記優れた特徴を有する材料供給を実現す
ることができる。As described above, according to the present invention, since the contact time between the liquid surface and the bar is shortened because the T FS is shortened, the amount of the bar material that melts into the liquid surface at the time of contact between the two is reduced. Can be. On the other hand, if V AV is the same because T BS is lengthened, the denominator of equation (1) becomes large and (FB) of equation (1)
That is, the supply amount per reciprocation of the bar can be increased. Therefore, due to their synergistic effect, the condition “the amount of the supplied material that comes into contact with the liquid surface and melts and melts into the liquid surface exceeds the amount of advance of the supplied material per 1 + -direction operation, that is, one reciprocating operation. No ", that is," the supply material comes into contact with the liquid surface at substantially the same amount for each reciprocating operation "can be satisfied, and material supply having the above-mentioned excellent characteristics can be realized.
請求項3記載の本発明は上記したように、前記請求項
2と同様に前記条件を満たすことが出来るようになる。
更に(F−B)を一定としているから(F−B)が前記
条件を満たすようにさえしておけばVAVが小さい領域に
おいても式(1)の分母が大きくなるだけであるから前
記条件を同様に容易に満たすことが出来るようになる。
従ってVAVが小さい領域で上記優れた特徴を有する材料
供給を実現することができる。According to the third aspect of the present invention, as described above, the condition can be satisfied in the same manner as in the second aspect.
Further, since (FB) is fixed, if the condition (FB) satisfies the above condition, the denominator of the equation (1) will only increase even in a region where VAV is small. Can be easily satisfied as well.
Therefore, material supply having the above-described excellent characteristics can be realized in a region where VAV is small.
請求項4記載の本発明は上記構成により、蒸着材料の
先端部が冷却されて温度が下がるので、液面と棒材との
接触時に棒材の温度が上りにくくなり、棒材が液面にと
け込む量を少なくすることができる。従って同様に上記
優れた特徴を有する材料供給を実現することができる。According to the fourth aspect of the present invention, since the temperature of the vapor-deposited material is reduced by cooling the leading end of the vapor-deposited material, the temperature of the rod hardly rises at the time of contact between the liquid surface and the rod, so that the rod has a liquid surface. The amount of melting can be reduced. Accordingly, material supply having the above-mentioned excellent characteristics can be realized.
請求項5記載の本発明は上記したように、棒材が液面
から遠ざかって停止している時間TBSが長いので冷却手
段により棒材先端部が充分に冷却され、棒材が液面にと
け込む量をより効果的に少なくすることができる。従っ
て同様に上記優れた特徴を有する材料供給を実現するこ
とができる。In order that the invention described in claim 5 above, the time T BS which bar is stopped away from the liquid surface is long been the bar tip is sufficiently cooled by the cooling means, the bar has a liquid surface The amount of melting can be reduced more effectively. Accordingly, material supply having the above-mentioned excellent characteristics can be realized.
実施例 以下に本発明の実施例を図面を参照して説明する。
尚、従来と同一構成要素には従来例と同一番号を付して
いる。第1図は本発明の一実施例を示す棒材の移送速度
パターン図である。棒材を移送させるには、例えば、す
でに当発明者が出願した第4図の構成を適用することが
出来る。第4図の構成及び動作についてはすでに説明し
たので省略する。Embodiments Embodiments of the present invention will be described below with reference to the drawings.
The same components as those of the conventional example are denoted by the same reference numerals as those of the conventional example. FIG. 1 is a pattern diagram of the transfer speed of a bar showing one embodiment of the present invention. In order to transfer the bar, for example, the configuration shown in FIG. 4 filed by the present inventors can be applied. The configuration and operation of FIG. 4 have already been described, and a description thereof will not be repeated.
本発明の第1実施例は、第1図における移送速度パタ
ーン図において、棒材3が前記液面4に接して溶融しそ
の液面4にとけ込む量が、1+−方向動作、すなわち1
往復動作当りの前記供給材料3の前進量(F−B)越え
ないように移送速度パターンが設定されているものであ
る。In the first embodiment of the present invention, in the transfer speed pattern diagram shown in FIG. 1, the amount by which the rod 3 contacts and melts into the liquid surface 4 and melts into the liquid surface 4 is 1 + -direction operation, that is, 1
The transfer speed pattern is set so as not to exceed the advance amount (FB) of the supply material 3 per reciprocating operation.
従って、往復動作毎に供給材料3が略等量液面4に接
触させることができるので、毎回等量供給材料3の溶液
に溶け込ませることが可能となるので液面4の温度変動
が小さくなり蒸発速度変動も小さくなる。その結果通過
製膜における膜厚の変動が小さくなるので膜厚の均一性
を向上させることができる。Accordingly, the supply material 3 can be brought into contact with the liquid surface 4 of substantially the same amount each time the reciprocating operation is performed, and the liquid material 4 can be dissolved in the solution of the same amount of the supply material 3 each time, so that the temperature fluctuation of the liquid surface 4 is reduced. Evaporation rate fluctuations are also reduced. As a result, the variation of the film thickness in the pass-through film formation is reduced, so that the uniformity of the film thickness can be improved.
また棒材3が相異なる蒸発速度の複数の成分から構成
されている場合においても、上記の組成比の変動を小さ
くできる。その結果、通過製膜するときに通過方向の組
成比の均一性を向上させることができる。Further, even when the bar 3 is composed of a plurality of components having different evaporation rates, the above-described variation in the composition ratio can be reduced. As a result, it is possible to improve the uniformity of the composition ratio in the passing direction when performing the passing film formation.
本発明の第2実施例は、第1図における移動速度パタ
ーン図において、供給用長尺蒸着材料3の平均移送速度
(VAV)指令に基づいて VAV=(F−B)/(TFD+TBD+TFS+TBS) …(1) F :+方向移送量 B :−方向移送量(一定) TFD:+方向移送正味時間 TFS:+方向移送休止時間(一定) TFS≧0 TBD:−方向移送正味時間(一定) TBS:−方向移送休止時間(一定) TBS>TFS なる演算を行い、算出されたFとTFDにて供給用長尺蒸
着材料3を駆動する制御手段100を備えたものである
(第2図参照)。In the second embodiment of the present invention, in the moving speed pattern diagram in FIG. 1, V AV = (FB) / (T FD ) based on the average moving speed (V AV ) command of the supply long vapor deposition material 3. + T BD + T FS + T BS )… (1) F: + direction transfer amount B: − direction transfer amount (constant) T FD : + direction transfer net time T FS : + direction transfer pause time (constant) T FS ≧ 0 T BD :-direction transfer net time (constant) T BS :-direction transfer pause time (constant) TBS > T FS is calculated, and the calculated F and T FD are used to drive the long deposition material 3 for supply. It is provided with control means 100 (see FIG. 2).
従って、TFSを短くしているので液面4と棒材3との
接触時間が短くなるので両者の接触時に棒材3が液面4
にとけ込む量を少なくすることができる。一方、TBSを
長くしているので式(1)の分母が大きくなり式(1)
の(F−B)すなわち棒材1往復当りの供給量を大きく
することができる。従って、それらの相乗効果で容易に
前記条件「前記材料が前記液面に接して溶融しその液面
にとけ込む量が、1+−方向動作、すなわち1往復動作
当りの前記供給材料の前進量を越えない」すなわち「往
復動作毎に供給材料が略等量液面に接触する」を満たす
ことが出来るようになる。Therefore, the contact time between the liquid surface 4 and the rod 3 is shortened because the T FS is shortened.
It is possible to reduce the amount of melting. On the other hand, since the longer T BS denominator becomes large and expression of the formula (1) (1)
(FB), that is, the supply amount per reciprocation of the bar can be increased. Therefore, due to their synergistic effect, the condition “the amount of the material that comes into contact with the liquid surface and melts and melts into the liquid surface exceeds the amount of advance of the supply material per 1 + -direction operation, that is, one reciprocating operation. No ", that is," the feed material comes into contact with the liquid surface at substantially the same amount for each reciprocating operation ".
本発明の第3実施例は、供給用長尺蒸着材料3の平均
移送速度(VAV)指令に基づいて VAV=(F−B)/(TFD+TBD+TFS+TBS) …(1) F :+方向移送量(一定) B :−方向移送量(一定) TFD:+方向移送正味時間(一定) TFS:+方向移送休止時間(一定) TFS≧0 TBD:−方向移送正味時間(一定) TBS:−方向移送休止時間 TBS>TFS なる演算を行い、算出されたTBSにて供給用長尺蒸着材
料を駆動する制御手段100を備えたものである。Third embodiment of the present invention, V AV = (F-B ) based on the average transfer rate of supply long deposition material 3 (V AV) Directive / (T FD + T BD + T FS + T BS) ... (1 ) F: + direction transfer amount (constant) B:-direction transfer amount (constant) T FD : + direction transfer net time (constant) T FS : + direction transfer pause time (constant) T FS ≥ 0 T BD :-direction Net transfer time (constant) T BS : − direction transfer pause time An arithmetic operation of T BS > T FS is performed, and the control means 100 is provided to drive the supply long evaporation material at the calculated T BS .
従って、上記と同様に前記条件を満たすことが出来る
ようになる。更に(F−B)を一定としているから(F
−B)が前記条件を満たすようにさえしておけばVAVが
小さい領域においても式(1)の分母が大きくなるだけ
であるから前記条件を同様に容易に満たすことが出来る
ようになる。従ってVAVが小さい領域で有利な方法であ
る。Therefore, the above condition can be satisfied in the same manner as described above. Further, since (FB) is fixed, (F
As long as -B) satisfies the above condition, the denominator of the equation (1) only increases in the region where VAV is small, so that the above condition can be easily satisfied. Thus an advantageous way in the area V AV is small.
本発明の第4実施例を添え付け図面に基づいて説明す
る。尚、従来と同一構成要素には従来側と同一番号を付
している。第2図、第3図において30は前記モータ20に
より駆動される駆動ローラで、31は棒材3を案内する回
転ローラである。32、33はそれぞれ冷却流体通路34、35
を中心に形成した軸36、37に回転自在に支持された冷却
回転ローラである。図示しないが冷却回転ローラ33は冷
却回転ローラ32にバネあるいは自重により押しつけられ
ている。各々の冷却回転ローラ32、33の外形は前記棒材
3との接触面積を大きくして棒材の冷却効率を高めるた
めに鼓型としてある。前記軸36、37と冷却回転ローラ3
2、33間は必要に応じてグラファイトや二硫化モリブデ
ン等により潤滑される。A fourth embodiment of the present invention will be described with reference to the accompanying drawings. Note that the same components as those in the related art are denoted by the same reference numerals as those in the related art. 2 and 3, reference numeral 30 denotes a driving roller driven by the motor 20, and reference numeral 31 denotes a rotating roller for guiding the bar 3. 32 and 33 are cooling fluid passages 34 and 35, respectively.
This is a cooling rotary roller rotatably supported by shafts 36 and 37 formed around the center. Although not shown, the cooling rotary roller 33 is pressed against the cooling rotary roller 32 by a spring or its own weight. The outer shape of each of the cooling rotary rollers 32 and 33 is shaped like a drum in order to increase the contact area with the bar 3 and increase the cooling efficiency of the bar. The shafts 36 and 37 and the cooling rotary roller 3
The space between 2 and 33 is lubricated with graphite or molybdenum disulfide as necessary.
このように構成すると第2図において、棒材3が前記
液面4から後退してその先端5はR位置にて休止し、先
端5は前記各々の冷却回転ローラ32、33により冷却され
ることになる。冷却されると、次に棒材3が前記液面4
に向かって送られて液面4と接触したとき先端5の温度
が上りにくくなり、先端が液面4にとけ込む量を少なく
することができる。In this configuration, in FIG. 2, the rod 3 retreats from the liquid surface 4 and its tip 5 rests at the R position, and the tip 5 is cooled by the cooling rollers 32 and 33, respectively. become. When cooled, the rod 3 is then moved to the liquid level 4
The temperature of the tip 5 becomes hard to rise when it is sent toward the liquid surface 4 and comes into contact with the liquid surface 4, and the amount of the tip that melts into the liquid surface 4 can be reduced.
この時、式(1)においてTBS>TFSとし、TBSすなわ
ち棒材3が液面4から後退して停止している時間を長く
すると前記各々の冷却回転ローラ32、33により棒材先端
部が充分に冷却され、棒材3が液面4にとけ込む量をよ
り効果的に少なくすることができる。At this time, the bar tip by T BS> T FS and, T BS i.e. wherein each of the cooling rollers 32, 33 and bars 3 to lengthen the time that the stop retracted from the liquid surface 4 in the formula (1) The portion is sufficiently cooled, and the amount of the rod material 3 that melts into the liquid surface 4 can be reduced more effectively.
上記例では棒材3に当接する冷却部材は2個の回転ロ
ーラとしたが、冷却能力が充分であれば冷却回転ローラ
は1個でもよい。また冷却部材は必ずしも回転させる必
要はなく冷却部材の棒材3との摩耗が問題にならなけれ
ば水等で冷却された固定部材でもよい。In the above example, the cooling member that contacts the bar 3 is two rotating rollers. However, if the cooling capacity is sufficient, one cooling rotating roller may be used. The cooling member does not necessarily need to be rotated, and may be a fixed member cooled with water or the like if wear of the cooling member with the bar 3 does not matter.
以上の例では、速度パターンは台形波状で説明したが
それに限るものではなく、制御が簡単になる矩形波状、
あるいは加減速が滑らかな正弦波状、またはその他であ
ってもよい。In the above example, the speed pattern has been described in the form of a trapezoidal wave, but the present invention is not limited to this.
Alternatively, the acceleration / deceleration may be a smooth sinusoidal wave or the like.
また棒材3を移送する方法は以上のように駆動ローラ
に限るものではなく、チェーン、ベルトあるいはロープ
等を駆動し、それらに棒材を係合せしめる方法であって
もまた、送りネジを用いる方法であってもよい。Further, the method of transferring the bar 3 is not limited to the drive roller as described above, and a method of driving a chain, a belt, a rope, or the like and engaging the bar with them may also use a feed screw. It may be a method.
以上全て棒材の形状は円柱状、数量は1本を1例とし
てとして説明したが形状は長尺材であれば角柱状、板状
他であっても、また数量は複数であってもよい。As described above, the shape of the rod is all cylindrical and the number is one as an example. However, the shape may be prismatic, plate, or the like as long as the material is long, or the number may be plural. .
発明の効果 以上説明したところから明らかなように、本発明の蒸
着材料供給方法及びその装置は、蒸着材料供給時の液面
の温度変動が小さく、蒸着速度変動も小さいものとする
ことが出来る。その結果、通過製膜における膜厚の均一
性を向上させることができる。EFFECT OF THE INVENTION As is clear from the above description, the vapor deposition material supply method and apparatus of the present invention can reduce the temperature fluctuation of the liquid surface during the vapor deposition material supply and the fluctuation of the vapor deposition rate. As a result, the uniformity of the film thickness in the pass film formation can be improved.
また棒材が相異なる蒸発速度の複数の成分から構成さ
れている場合においても、蒸気の組成比の変動を小さく
できる。その結果、通過製膜するときに通過方向の組成
比の均一性を向上させることができる。Further, even when the rod is composed of a plurality of components having different evaporation rates, the variation in the composition ratio of the steam can be reduced. As a result, it is possible to improve the uniformity of the composition ratio in the passing direction when performing the passing film formation.
第1図は、本発明の第1、第2、第3、第5実施例にお
ける棒材の移送速度パターン図、第2図は本発明におけ
る第4実施例を示す一部断面図、第3図は第2図のY−
Y′矢視断面図、第4図は従来の蒸着材料供給方法及び
その装置を示す一部断面図、第5図、第6図、第7図、
第8図は従来の蒸着材料供給方法における棒材の先端部
の溶融状態を示す側断面図、第9図は従来の蒸着材料供
給方法における蒸発速度変動を示すグラフ、第10図は従
来の蒸着材料供給装置のその他の例を示す1部断面図、
第11図は本発明者が出願した発明の1実施例における蒸
着材料供給装置を示す一部断面図、第12図は本発明者が
出願した発明の1実施例における棒材の移送速度パター
ン図、第13図は各供給方法の蒸発速度変動を比較して示
すグラフ、第14図は第11図の要部を拡大して示す側断面
図、第15図、第16図は棒材先端部の溶融状態を示す側断
面図である。 1……蒸着材料、2……坩堝、3……棒材、8……基
板、9……薄膜、14、30……駆動ローラ、32、33……冷
却回転ローラ、20……モータ、21……駆動回路、22……
演算回路、23……メモリ、24……平均移送速度指令、10
0……制御手段。FIG. 1 is a diagram showing a transfer speed pattern of a bar in the first, second, third and fifth embodiments of the present invention. FIG. 2 is a partial sectional view showing a fourth embodiment of the present invention. The figure shows Y- in FIG.
FIG. 4 is a partial sectional view showing a conventional vapor deposition material supply method and its apparatus, and FIG. 5, FIG. 6, FIG.
FIG. 8 is a side sectional view showing the molten state of the tip of the rod in the conventional vapor deposition material supply method, FIG. 9 is a graph showing the evaporation rate fluctuation in the conventional vapor deposition material supply method, and FIG. 1 is a partial cross-sectional view illustrating another example of a material supply device,
FIG. 11 is a partial cross-sectional view showing a vapor deposition material supply apparatus according to one embodiment of the invention filed by the inventor, and FIG. 12 is a diagram showing a transfer speed pattern of a bar in one embodiment of the invention filed by the inventor. , FIG. 13 is a graph showing a comparison of the evaporation rate fluctuation of each supply method, FIG. 14 is a side sectional view showing an enlarged main part of FIG. 11, FIG. 15 and FIG. 3 is a side sectional view showing a molten state of FIG. DESCRIPTION OF SYMBOLS 1 ... Vapor deposition material, 2 ... Crucible, 3 ... Bar material, 8 ... Substrate, 9 ... Thin film, 14, 30 ... Drive roller, 32, 33 ... Cooling rotation roller, 20 ... Motor, 21 …… Drive circuit, 22 ……
Arithmetic circuit, 23: Memory, 24: Average transfer speed command, 10
0 ... Control means.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 児玉 佳代子 大阪府門真市大字門真1006番地 松下電 器産業株式会社内 (56)参考文献 特公 昭53−33873(JP,B2) (58)調査した分野(Int.Cl.6,DB名) C23C 14/00 - 14/58────────────────────────────────────────────────── ─── Continued on the front page (72) Inventor Kayoko Kodama 1006 Kazuma Kadoma, Kadoma City, Osaka Inside Matsushita Electric Industrial Co., Ltd. Field (Int. Cl. 6 , DB name) C23C 14/00-14/58
Claims (5)
し、その蒸着材料から発生する蒸気を基板に付着せしめ
て薄膜を形成するため、前記蒸着材料を蒸着材料液面に
向かって供給する蒸着材料供給方法において、前記坩堝
内で溶融された蒸着材料液面に向かって移送される供給
用長尺蒸着材料の移送速度を、前記液面に向かう方向を
+、前記液面から遠ざかる方向を−としたとき、交互に
+方向と−方向に切り替え、平均として+方向とすると
共に、前記蒸着材料が前記液面に接して溶融しその液面
にとけ込む量が、1+−方向動作当りの前記蒸着材料の
前進量を越えないように前記移動速度を設定することを
特徴とする蒸着材料供給方法。1. A vapor deposition material contained in a crucible is heated and melted, and the vapor generated from the vapor deposition material is attached to a substrate to form a thin film. In the method of supplying a deposition material, the transfer speed of the supply long deposition material transferred toward the liquid surface of the deposition material melted in the crucible is set such that the direction toward the liquid surface is +, and the direction away from the liquid surface is +. When-is set to-, the direction is alternately switched to the + direction and the-direction, and the + direction is averaged, and the amount of the vapor deposition material which is in contact with the liquid surface and melts and melts into the liquid surface is determined per 1 +-direction operation. A method of supplying a deposition material, wherein the moving speed is set so as not to exceed an advance amount of the deposition material.
し、その蒸着材料から発生する蒸気を基板に付着せしめ
て薄膜を形成する際、前記坩堝内で溶融された蒸着材料
に向かって移送される供給用長尺蒸着材料の移送速度
を、前記蒸着材料に向かう方向を+、前記蒸着材料から
遠ざかる方向を−としたとき、交互に+方向と−方向に
切り替えて蒸着材料を坩堝に供給する蒸着材料供給装置
であって、前記供給用長尺蒸着材料の平均移送速度(V
AV)指令に基づいて VAV=(F−B)/(TFD+TBD+TFS+TBS) …(1) なお、F:+方向移送量 B:−方向移送量(一定) TFD:+方向移送正味時間 TFS:+方向移送休止時間(一定) TFS≧0 TBD:−方向移送正味時間(一定) TBS:−方向移送休止時間(一定) TBS>TFS なる演算を行い、算出されたFとTFDにて供給用長尺蒸
着材料を駆動する制御手段を備えたことを特徴とする蒸
着材料供給装置。2. The method according to claim 1, wherein the vapor deposition material contained in the crucible is heated and melted, and vapor generated from the vapor deposition material is adhered to a substrate to form a thin film. When the transfer speed of the supplied long deposition material for transfer is + in the direction toward the deposition material and-in the direction away from the deposition material, the deposition material is alternately switched to the + and-directions, and the deposition material is placed in the crucible. A vapor deposition material supply device for supplying the long vapor deposition material for supply (V
AV ) Based on the command, V AV = (FB) / ( TFD + TBD + TFS + TBS ) (1) where F: + direction transfer amount B:-direction transfer amount (constant) TFD : + Direct transfer net time T FS : + direction transfer pause time (constant) T FS ≧ 0 T BD : − direction transfer net time (constant) T BS : − direction transfer pause time (constant) T BS > T FS And a control means for driving the supply long evaporation material based on the calculated F and TFD .
し、その蒸着材料から発生する蒸気を基板に付着せしめ
て薄膜を形成する際に前記坩堝内で溶融された蒸着材料
に向かって移送される供給用長尺蒸着材料の移送速度
を、前記蒸着材料に向かう方向を+、前記蒸着材料から
遠ざかる方向を−としたとき、交互に+方向と−方向に
切り替えて蒸着材料を坩堝に供給する蒸着材料供給装置
であって、供給用長尺蒸着材料の平均移送速度(VAV)
指令に基づいて VAV=(F−B)/(TFD+TBD+TFS+TBS) …(1) なお、F:+方向移送量(一定) B:−方向移送量(一定) TFD:+方向移送正味時間(一定) TFS:+方向移送休止時間(一定) TFS≧0 TBD:−方向移送正味時間(一定) TBS:−方向移送休止時間 TBS>TFS なる演算を行い、算出されたTBSにて供給用長尺蒸着材
料を駆動する制御手段を備えたことを特徴とする蒸着材
料供給装置。3. A vapor deposition material contained in a crucible is heated and melted, and vapor generated from the vapor deposition material is adhered to a substrate to form a thin film toward the vapor deposition material melted in the crucible. When the transfer speed of the supplied long deposition material for transfer is + in the direction toward the deposition material and-in the direction away from the deposition material, the deposition material is alternately switched to the + and-directions, and the deposition material is placed in the crucible. An apparatus for supplying a deposition material to be supplied, wherein the average transport speed (V AV ) of the long deposition material for supply is provided.
Based on the command, VAV = (FB) / ( TFD + TBD + TFS + TBS ) (1) where F: + direction transfer amount (constant) B:-direction transfer amount (constant) TFD : + Direction transfer net time (constant) T FS : + direction transfer pause time (constant) T FS ≥ 0 T BD :-direction transfer net time (constant) T BS :-direction transfer pause time T BS > T FS performed, the vapor deposition material supply apparatus characterized by comprising a control means for driving the feed long deposition material at the calculated T BS.
し、その蒸着材料から発生する蒸気を基板に付着せしめ
て薄膜を形成する手段と、前記坩堝内で溶融された蒸着
材料液面に向かって移送される供給用長尺蒸着材料の移
送速度を、前記液面に向かう方向を+、前記液面から遠
ざかる方向を−としたとき、交互に+方向と−方向に切
り替え、平均として+方向として前記蒸着材料を移送す
るする蒸着材料移送手段と、前記液面に向かう前記蒸着
材料の先端部近傍を冷却する手段とを備えたことを特徴
とする蒸着材料供給装置。4. A means for heating and melting a vapor deposition material contained in a crucible and adhering vapor generated from the vapor deposition material to a substrate to form a thin film, and a liquid surface of the vapor deposition material melted in the crucible. When the transfer speed of the supply long vapor deposition material transferred toward the liquid surface is + in the direction toward the liquid surface and-in the direction away from the liquid surface, the transfer direction is alternately switched between the + direction and the-direction, and on average. A vapor deposition material supply device, comprising: a vapor deposition material transporting means for transporting the vapor deposition material as a + direction; and a means for cooling the vicinity of the tip of the vapor deposition material toward the liquid surface.
し、その蒸着材料から発生する蒸気を基板に付着せしめ
て薄膜を形成する手段と、前記坩堝内で溶融された蒸着
材料液面に向かって移送される供給用長尺蒸着材料の移
送速度を、前記液面に向かう方向を+、前記液面から遠
ざかる方向を−としたとき、交互に+方向と−方向に切
り替え、平均として+方向として前記蒸着材料を移送す
るする蒸着材料移送手段と、前記液面に向かう前記蒸着
材料の先端部近傍を冷却する手段とを備えた蒸着材料供
給装置であって、供給用長尺蒸着材料の平均移送速度
(VAV)指令に基づいて VAV=(F−B)/(TFD+TBD+TFS+TBS) …(1) F:+方向移送量 B:−方向移送量 TFD:+方向移送正味時間 TFS:+方向移送休止時間 TFS≧0 TBD:−方向移送正味時間 TBS:−方向移送休止時間 TBS>TFS なる演算を行い、算出された各々の値にて供給用長尺蒸
着材料を駆動する制御手段を備えたことを特徴とする蒸
着材料供給装置。5. A means for heating and melting a vapor deposition material contained in a crucible and adhering vapor generated from the vapor deposition material to a substrate to form a thin film, and a liquid surface of the vapor deposition material melted in the crucible. When the transfer speed of the supply long vapor deposition material transferred toward the liquid surface is + in the direction toward the liquid surface and-in the direction away from the liquid surface, the transfer direction is alternately switched between the + direction and the-direction, and on average. A vapor deposition material transporting device for transporting the vapor deposition material as a positive direction, and a device for cooling the vicinity of the tip end of the vapor deposition material toward the liquid level, wherein a long vapor deposition material for supply is provided. the average transfer rate of (V AV) V AV = ( F-B) based on the command / (T FD + T BD + T FS + T BS) ... (1) F: + directional movement amount B: - directional movement amount T FD: + direction transfer net time T FS: + direction transfer pause time T FS ≧ 0 T BD: - direction transfer Taste Time T BS: - perform directional movement quiescent time T BS> T FS becomes operational, the vapor deposition material supply, characterized in that it comprises a control means for driving the feed long deposition material at calculated each value apparatus.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2075218A JP2779040B2 (en) | 1990-03-22 | 1990-03-22 | Method and apparatus for supplying vapor deposition material |
| DE69012667T DE69012667T2 (en) | 1989-06-19 | 1990-06-16 | Process for supplying vacuum evaporation material and device for carrying it out. |
| EP90111384A EP0403987B1 (en) | 1989-06-19 | 1990-06-16 | Method for supplying vacuum evaporation material and apparatus therefor |
| US07/539,740 US5098742A (en) | 1989-06-19 | 1990-06-18 | Method for supplying vacuum evaporation material |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2075218A JP2779040B2 (en) | 1990-03-22 | 1990-03-22 | Method and apparatus for supplying vapor deposition material |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH03274263A JPH03274263A (en) | 1991-12-05 |
| JP2779040B2 true JP2779040B2 (en) | 1998-07-23 |
Family
ID=13569859
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2075218A Expired - Fee Related JP2779040B2 (en) | 1989-06-19 | 1990-03-22 | Method and apparatus for supplying vapor deposition material |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2779040B2 (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5910764B2 (en) * | 1976-08-30 | 1984-03-12 | ヤンマー農機株式会社 | hay tower |
-
1990
- 1990-03-22 JP JP2075218A patent/JP2779040B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH03274263A (en) | 1991-12-05 |
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