JPS592046A - Object to be irradiated with x rays - Google Patents

Object to be irradiated with x rays

Info

Publication number
JPS592046A
JPS592046A JP57111103A JP11110382A JPS592046A JP S592046 A JPS592046 A JP S592046A JP 57111103 A JP57111103 A JP 57111103A JP 11110382 A JP11110382 A JP 11110382A JP S592046 A JPS592046 A JP S592046A
Authority
JP
Japan
Prior art keywords
mask
ray
resist
ray mask
exposure
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
JP57111103A
Other languages
Japanese (ja)
Inventor
Koichi Okada
浩一 岡田
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.)
NEC Corp
Original Assignee
NEC Corp
Nippon Electric 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 NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP57111103A priority Critical patent/JPS592046A/en
Publication of JPS592046A publication Critical patent/JPS592046A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03FPHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
    • G03F7/00Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
    • G03F7/20Exposure; Apparatus therefor
    • G03F7/2037Exposure with X-ray radiation or corpuscular radiation, through a mask with a pattern opaque to that radiation
    • G03F7/2039X-ray radiation

Landscapes

  • Health & Medical Sciences (AREA)
  • Toxicology (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Preparing Plates And Mask In Photomechanical Process (AREA)
  • Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)
  • Exposure Of Semiconductors, Excluding Electron Or Ion Beam Exposure (AREA)

Abstract

PURPOSE:To make secure further the copying of a pattern having a submicron width and to provide a large degree of technical freedom to an X-ray mask and an exposure atmosphere by providing electrode impressed with positive and negative potential near the X-ray mask and the work. CONSTITUTION:Electrodes 7, 8 are installed near an X-ray mask and the work, and positive and negative potentials are applied thereto to form the electric field region between the electrodes 7 and 8 within an exposure atmosphere. Then, all the generated secondary electrons 9 are gathered to an anode 10 and do not arrive on a resist surface; therefore, the over-exposure of the resist is obviated. The fine patterning of the resist is thus further made secure.

Description

【発明の詳細な説明】 本発明は、1μn1以1′の微細パターンの複ダに威力
を元押するXiクリソラフィの分野におけるX線剣光彼
jにi射体に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an X-ray beam projector in the field of XI chrysometry, which is effective in producing multiples of fine patterns of 1μn1 to 1'.

軟X mAを用いだX緑すソグラフィによれば、高解像
度パターンの枚写がLif能であることがエレク)u、
=、クス・レターズ(Electronics Let
ters)第8巻第4号第102−104頁(1972
年)に発表されて以来、X線リングラフィに関する研究
開発が精力的に進められてきた。X線源、X線マスク、
アライメント方式、X線レジスト、そしてX祿M光装置
とその各々において技術の畜檀がlさ7L、実用Jψ紡
にかなり近付(へCきてのると言える。
According to X-green lithography using soft X mA, it is possible to copy high-resolution patterns with ease.
=, Kuss Letters (Electronics Let
ters) Vol. 8, No. 4, pp. 102-104 (1972
Since its publication in 2010, research and development on X-ray phosphorography has been vigorously pursued. X-ray source, X-ray mask,
The technology in each of the alignment methods, X-ray resists, and X-ray M optical devices is 17L, and it can be said that we have come quite close to practical Jψ spinning.

本発明は、X、l1lilマスク、11にマスク上のA
n 1+!を数体から放出される光電子・オージヱ電子
の効果に関する。光゛成子・オージェ戊子放出に1゛超
する指摘は、1975年に発行された刊行セグジャーナ
ル・オブ・バキュウム・サイエンス・アンド・テクノロ
ジー(Journal of Vacuum 5cie
nce andTechnology)第12着第6号
第x32c>J3:n BYになされている。すなわち
、RhLa、$(波長4.6特性X廉を使用する場合に
、A/’にα線(波長8.34A)使用の場汗に比べて
、より多く放出される高エネルギー成分である連続X、
顧にょる影ぜが指摘されている。この連続X線によって
マスクコントラストが低Fし、さらにはマスク上のAu
吸収体パターン及びレジスト基板から光゛丸干・オ−ジ
ェ電子が放出され、レジストのパターンニングに影響を
与えることが報告されている。
The present invention uses X, l1lil mask, 11 and A on the mask.
n1+! Regarding the effects of photoelectrons and audioelectrons emitted from several bodies. The point that exceeds the Mitsunari-Auger Boron emission by 1 degree was found in a publication published in 1975, Journal of Vacuum Science and Technology (Journal of Vacuum 5cie).
nce and Technology) No. 12, No. 6, x32c>J3:n BY. That is, when RhLa, $ (wavelength 4.6 characteristic X,
It has been pointed out that there are shadows. This continuous X-ray causes the mask contrast to be low F, and furthermore, the Au on the mask
It has been reported that light and Auger electrons are emitted from the absorber pattern and the resist substrate and affect the patterning of the resist.

ところが、本発明者はA7?ターゲットを用いたX線露
光にネtいて、次の所しい実験事実を見出した。第1図
にその特性が示されてl/+る。
However, the inventor is A7? By studying X-ray exposure using targets, we discovered the following interesting experimental facts. Its characteristics are shown in FIG.

本図は、ネガレジス)PG〜IAの残存膜)Vの露光雰
囲気真空度依イr性を示している。露光z< 1141
気とは、マスクとウェハーとの間の空間のMFin気を
意味する。第1図マ′!1ら露光雰囲気真イF度依存性
を示し−Cいる。シ゛、9光W!i1J気と11、マス
クとウェハーとの四(の空間の雰囲気を意味する。第1
. IAから露::1雰囲気真鴛度が悪化すると、X線
マスク無しの場合口り印のデータ)は、PGM人残存膜
厚は次第に減少し、厚さ]、7n+馬のAu膜を有する
マスクを用いた場合(・印のデータ)は、P(Jλ、I
A残イ月摸1pは次第に増加することが分かる。このと
きPGんIAに対するklKait#oドース量は3 
Q !nJ/7 、−q スフとウェハーとのギャップ
は20μff+に固定された。X線マスク無し、の場合
の傾向によ、空気中の酸素による架橋反応阻止効果であ
ることが、はぼ詔められている。問題は厚さ17nmの
Au膜を有するマスクを用いた場合である。露光雰囲気
真空度の悪化によるP GM、A 浅イJ膜厚(9顕著
な増加傾向は新たに見出された実験事実でンらり、かつ
、し・シストのバターニングの′frIJf:向−トに
対しで、一つの大きな8題点である。つまり、残存膜厚
が増加するとマスク上のパターン全精度良く転写できな
くなる。特に、サブミクロン幅のパターンの旧確な複写
を実現するという観点において、このようなPGMA残
存膜厚の増加は、重大な間頓点である。
This figure shows the dependence of the residual film (V) of the negative resists (PG) to (IA) on the vacuum degree of the exposure atmosphere. Exposure z< 1141
Air means MFin air in the space between the mask and the wafer. Figure 1 Ma'! 1 shows exposure atmosphere true F degree dependence -C. Wow, 9 light W! i1J Qi and 11, meaning the atmosphere of the space between the mask and the wafer. 1st
.. From IA to Dew::1 When the atmospheric density deteriorates, the PGM residual film thickness gradually decreases (without X-ray mask), the thickness], 7n + mask with Au film When using (data marked with ・), P(Jλ, I
It can be seen that the amount of A remaining month 1p gradually increases. At this time, the dose of klKait#o for PGIA is 3
Q! nJ/7, -q The gap between the fabric and the wafer was fixed at 20 μff+. Due to the tendency in the case without an X-ray mask, it is rumored that the crosslinking reaction is inhibited by oxygen in the air. The problem occurs when a mask having a 17 nm thick Au film is used. The remarkable increasing tendency of PGM,A shallow AJ film thickness (9) due to the deterioration of the vacuum degree of the exposure atmosphere is a newly discovered experimental fact, and the tendency for the patterning of cysts to increase. There are 8 major issues regarding the above.In other words, as the remaining film thickness increases, it becomes impossible to transfer the pattern on the mask with high accuracy.Especially, from the perspective of realizing accurate reproduction of sub-micron width patterns. In this case, such an increase in the remaining PGMA film thickness is a serious point of failure.

前2者の実験(・印と○印)条件の大きな違1ρは薄い
Au膜の存在の有無である。幼いAu膜が有るというこ
とは、AIケタ−ットから放射されるX線(主ど士、て
1(α線〕が、Au膜に吸収されて、A11膜−1,1
・ら光を子・オージェ゛電子が放出され、ζ゛)ことを
意味する。この−ρわゆる光電効果による光電子・オー
ジェ電子の放出1″Cは、全ての拳印のデータ点におい
て同一である。にもかかわらず、露光雰囲気真空度の悪
化によって、PGMA残存膜厚が増加するという事は、
光電子・オージェ成子による露光雰囲気内の空気の電離
が、真空度の悪化に従って増加するためと考えられる。
The major difference 1ρ between the experimental conditions of the former two experiments (marked with * and marked with ○) is the presence or absence of a thin Au film. The presence of a young Au film means that the X-rays (alpha rays) emitted from the AI digits are absorbed by the Au film and
・This means that light is emitted from Auger electrons (ζ゛). This -ρ emission of photoelectrons and Auger electrons due to the so-called photoelectric effect 1''C is the same for all fist data points.Nevertheless, as the vacuum level of the exposure atmosphere worsens, the remaining PGMA film thickness increases. To do it means
This is thought to be because the ionization of the air in the exposure atmosphere by photoelectrons and Auger Seiko increases as the degree of vacuum deteriorates.

真空度の悪化は、空気の密度の増加を意味するから、こ
の考えは極めて妥当である。
This idea is extremely reasonable because a deterioration in the degree of vacuum means an increase in the density of air.

すなわち、ALL膜から放出される光電子・オージェ電
子が露光雰囲気中の空気を電離し、その結果、発生した
全二次電子がPGllviAの架橋を促進する効果が前
記の空気中の酸素による架橋阻止の効果を上まわるため
であると解釈される。
That is, the photoelectrons and Auger electrons emitted from the ALL film ionize the air in the exposure atmosphere, and as a result, all the secondary electrons generated promote crosslinking of PGllviA, which is due to the effect of inhibiting crosslinking due to oxygen in the air. It is interpreted that this is to outweigh the effects.

本発明の目的は、このような従来の問題点を除去せしめ
てX線マスクから発生する光電子・オージェ電子による
悪影響を回避し、X騙すソグラフィにおける微細パター
ン複写を、より精度良く行なうことのできるX#jI屋
光被射光被射体することにある。
The object of the present invention is to eliminate such conventional problems, avoid the adverse effects of photoelectrons and Auger electrons generated from an #jI The object is to be exposed to light.

本発明によれば、Xfj!吸収体パターン及びマスク基
板から成るX線マスクと、該x、1マスクと一定の間隔
を保って相対する被加工物と前記Xdマスク及び前記被
加物の周囲に近接して設置された正負の電圧を印加され
た、少くとも一対の電極とを含むX巌露光被照射体が得
られる。
According to the invention, Xfj! An X-ray mask consisting of an absorber pattern and a mask substrate, a workpiece facing the x,1 mask at a constant distance, and positive and negative An object to be exposed to X-rays is obtained which includes at least one pair of electrodes to which a voltage is applied.

以下、本発明について、実施例を示す図面を参照して詳
しく説明する。第2図は、一実施例を示すX機側光被照
射体の概略図である。X線マスク基板1上にAuXd吸
収体バ数体ン2を有するX線マスク3と、レジスト4を
コートされたウェハ−5から成る被加工物とが、一定の
設定された間隔に保たれている。この状態でX線6が照
射されX111!マスク上のパターンがレジストに複写
される。
EMBODIMENT OF THE INVENTION Hereinafter, the present invention will be described in detail with reference to drawings showing embodiments. FIG. 2 is a schematic diagram of a light irradiated object on the X machine side, showing one embodiment. An X-ray mask 3 having an AuXd absorber band 2 on an X-ray mask substrate 1 and a workpiece consisting of a wafer 5 coated with a resist 4 are kept at a predetermined distance. There is. In this state, X-ray 6 is irradiated and X111! The pattern on the mask is copied into the resist.

このとき、X線マスク3と被加工物との間の空間すなわ
ち、露光雰囲気は、通常大気まだはHe、N。
At this time, the space between the X-ray mask 3 and the workpiece, that is, the exposure atmosphere is usually atmospheric air or He or N.

等の不活性ガスである。そこで、前述したようにX11
Mマスク上のAu吸収体パターンから光電子・オージェ
電子が放出され、これらの電子によって露光雰囲気が電
離、され、多数の二次電子が発生する。
Inert gas such as Therefore, as mentioned above,
Photoelectrons and Auger electrons are emitted from the Au absorber pattern on the M mask, the exposure atmosphere is ionized by these electrons, and a large number of secondary electrons are generated.

この全二次′電子の作用によってレジストの過剰の露光
が生ずることは、第1図で説明した通りである。これを
回避するだめに、本発明では第2図に示す様にX線マス
クと被加工物の近傍に、電極78を設置した。これら電
極に正・負の電位を与えて、電極7.8間に電場領域を
露光雰囲気内に作る。
As explained in FIG. 1, overexposure of the resist occurs due to the action of all the secondary electrons. In order to avoid this, in the present invention, as shown in FIG. 2, an electrode 78 is installed near the X-ray mask and the workpiece. Positive and negative potentials are applied to these electrodes to create an electric field region in the exposure atmosphere between the electrodes 7 and 8.

このようにすると、第3図に示すように発生した全・二
次電子9は陽極10に集められる。11は電位を与える
電源である。従って、全二次電子は、レジスト面上に到
達することが無いので、レジストの過剰露光は生じない
。。
In this way, all the secondary electrons 9 generated are collected at the anode 10 as shown in FIG. Reference numeral 11 is a power source that provides a potential. Therefore, all secondary electrons do not reach the resist surface, so overexposure of the resist does not occur. .

以上説、明したように、光電子・オージェ電子を収集す
る電極を設置したX線露光被照射体を用いることによっ
て、レジストの過剰露光を回避できレジストの微細パタ
ーン加工を、より確実し、本発明の目的を達成できる。
As explained and clarified above, by using an X-ray exposed object equipped with an electrode for collecting photoelectrons and Auger electrons, overexposure of the resist can be avoided and fine pattern processing of the resist can be made more reliable, and the present invention can achieve the purpose of

本発明の他の実施例を第4図に示す。Another embodiment of the invention is shown in FIG.

第3図では、電極の配置の仕方が二電極であったが、第
4図では、四電極となっている。このようにすると、二
次電子12の陽極13.14への移動距離が縮まり、結
局全二次電子の収集効率を増加させることができる。本
構成によっても、本発明の目的を達成することができる
In FIG. 3, two electrodes are arranged, but in FIG. 4, four electrodes are arranged. In this way, the travel distance of the secondary electrons 12 to the anode 13.14 is reduced, and the overall collection efficiency of the secondary electrons can be increased. With this configuration as well, the object of the present invention can be achieved.

以上、説明したように本発明を適用するならば第一にX
繊すソグラフィにおけるサブミクロン幅パターンの複写
をより確実にでき、第2にX線マス゛り及び露光雰囲気
に対して大きな技術上の自由度を与えることができる。
As explained above, if the present invention is applied, first
It is possible to more reliably reproduce submicron width patterns in fiber lithography, and secondly, it is possible to provide a greater degree of technical freedom regarding the X-ray mask and exposure atmosphere.

なお、電界の印加によって、X線が影響を受けることが
熱いことは言うまでもない。
It goes without saying that the X-rays are hotly affected by the application of the electric field.

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

第1図は、従来技術の問題点であるPGMA残存膜厚の
露光雰囲気真空度依存性を示した図、第2図は本発明に
かかる一実施例であるX線露光被照射体の概略図、第3
図は同実施例における電極構成図、第4図は他の実施例
における電極構成を示した図である◇ l・・・・・・・・・マスク基板、2・・・・・・・・
・Au吸収体パターン、3・・・・・・・・・)lマス
ク、4・・・・・・・・・レジスト、5・・・・・・・
・・ウェハー、6・・・・・・・・・X線、7,8・・
・・・・・・・電極、9. 12・・・・・・・・・全
二次電子、10.13.14・・・・・・・・・陽極、
11・・・・・・・・・電源。 卦 2 図 号 J ロ 牙4μs
FIG. 1 is a diagram showing the dependence of the PGMA residual film thickness on the vacuum degree of the exposure atmosphere, which is a problem in the prior art, and FIG. 2 is a schematic diagram of an object to be exposed to X-rays, which is an embodiment of the present invention. , 3rd
The figure is a diagram showing the electrode configuration in the same embodiment, and FIG. 4 is a diagram showing the electrode configuration in another embodiment.
・Au absorber pattern, 3・・・・・・・・・)l mask, 4・・・・・・・・・Resist, 5・・・・・・・・・
...Wafer, 6...X-ray, 7,8...
...... Electrode, 9. 12......All secondary electrons, 10.13.14...Anode,
11......Power supply. Trigram 2 Symbol J Roga 4μs

Claims (1)

【特許請求の範囲】[Claims] X線吸tB体パターン及びマスク基板から成るX線マス
クと、該X線マスクと一定のff1l隔を保って相対す
る被加工物と、前記X線マスク及び前記被加工物の周囲
に近接して設置された正負の電圧を印加さIした少なく
とも1対のLL桶とを含bX線露光被照射体。
An X-ray mask consisting of an X-ray absorption body pattern and a mask substrate, a workpiece facing the X-ray mask with a constant distance of ff1l, and a workpiece adjacent to the X-ray mask and the workpiece. and at least one pair of LL buckets to which positive and negative voltages are applied.
JP57111103A 1982-06-28 1982-06-28 Object to be irradiated with x rays Pending JPS592046A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57111103A JPS592046A (en) 1982-06-28 1982-06-28 Object to be irradiated with x rays

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57111103A JPS592046A (en) 1982-06-28 1982-06-28 Object to be irradiated with x rays

Publications (1)

Publication Number Publication Date
JPS592046A true JPS592046A (en) 1984-01-07

Family

ID=14552469

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57111103A Pending JPS592046A (en) 1982-06-28 1982-06-28 Object to be irradiated with x rays

Country Status (1)

Country Link
JP (1) JPS592046A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6118010A (en) * 1984-07-04 1986-01-25 Toyoda Mach Works Ltd Manual teaching method of robot
WO2019166318A1 (en) * 2018-03-02 2019-09-06 Asml Netherlands B.V. Method and apparatus for forming a patterned layer of material

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6118010A (en) * 1984-07-04 1986-01-25 Toyoda Mach Works Ltd Manual teaching method of robot
JPH0562369B2 (en) * 1984-07-04 1993-09-08 Toyoda Machine Works Ltd
US20210079519A1 (en) * 2018-02-03 2021-03-18 Asml Netherlands B.V. Method and apparatus for forming a patterned layer of material
WO2019166318A1 (en) * 2018-03-02 2019-09-06 Asml Netherlands B.V. Method and apparatus for forming a patterned layer of material
KR20200118119A (en) * 2018-03-02 2020-10-14 에이에스엠엘 네델란즈 비.브이. Method and apparatus for forming a patterned layer of material
JP2021515264A (en) * 2018-03-02 2021-06-17 エーエスエムエル ネザーランズ ビー.ブイ. Methods and equipment for forming patterned layers of material

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