JPS60222849A - X-ray exposure method - Google Patents
X-ray exposure methodInfo
- Publication number
- JPS60222849A JPS60222849A JP59079498A JP7949884A JPS60222849A JP S60222849 A JPS60222849 A JP S60222849A JP 59079498 A JP59079498 A JP 59079498A JP 7949884 A JP7949884 A JP 7949884A JP S60222849 A JPS60222849 A JP S60222849A
- Authority
- JP
- Japan
- Prior art keywords
- ray
- resist
- exposure
- film
- air
- 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
Links
- 238000000034 method Methods 0.000 title claims description 13
- 229910052751 metal Inorganic materials 0.000 claims abstract description 19
- 239000002184 metal Substances 0.000 claims abstract description 19
- 239000010408 film Substances 0.000 abstract description 24
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 abstract description 13
- 229910052760 oxygen Inorganic materials 0.000 abstract description 13
- 239000001301 oxygen Substances 0.000 abstract description 13
- 230000035945 sensitivity Effects 0.000 abstract description 10
- 229920002120 photoresistant polymer Polymers 0.000 abstract description 8
- 230000004907 flux Effects 0.000 abstract description 3
- 150000002739 metals Chemical class 0.000 abstract description 3
- 239000003638 chemical reducing agent Substances 0.000 abstract description 2
- 238000013461 design Methods 0.000 abstract description 2
- 238000011161 development Methods 0.000 abstract description 2
- 230000001681 protective effect Effects 0.000 abstract description 2
- 239000010409 thin film Substances 0.000 abstract description 2
- 230000007423 decrease Effects 0.000 description 6
- 238000005516 engineering process Methods 0.000 description 6
- 230000000694 effects Effects 0.000 description 4
- 238000010586 diagram Methods 0.000 description 3
- 239000007789 gas Substances 0.000 description 3
- 230000008901 benefit Effects 0.000 description 2
- 238000006243 chemical reaction Methods 0.000 description 2
- 238000004132 cross linking Methods 0.000 description 2
- 230000007246 mechanism Effects 0.000 description 2
- 229920002189 poly(glycerol 1-O-monomethacrylate) polymer Polymers 0.000 description 2
- 230000005855 radiation Effects 0.000 description 2
- 238000006722 reduction reaction Methods 0.000 description 2
- 239000006096 absorbing agent Substances 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 238000001312 dry etching Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 230000000149 penetrating effect Effects 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 238000012827 research and development Methods 0.000 description 1
- 230000004044 response Effects 0.000 description 1
- 238000012546 transfer Methods 0.000 description 1
- 238000001039 wet etching Methods 0.000 description 1
- 229910052725 zinc Inorganic materials 0.000 description 1
Classifications
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03F—PHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
- G03F7/00—Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
- G03F7/20—Exposure; Apparatus therefor
- G03F7/2037—Exposure with X-ray radiation or corpuscular radiation, through a mask with a pattern opaque to that radiation
- G03F7/2039—X-ray radiation
Landscapes
- Health & Medical Sciences (AREA)
- Toxicology (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Exposure Of Semiconductors, Excluding Electron Or Ion Beam Exposure (AREA)
- Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)
Abstract
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は、1μフn以下の微細パターンの転写に威力を
・発揮するX線リングラフィの分野におけるX線露光方
法に関する。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an X-ray exposure method in the field of X-ray phosphorography, which is effective in transferring fine patterns of 1 μf or less.
(従来技術とその問題点)
X線露光技術は、サブミクロン幅パターンの確実な高解
像性の故に、将来の極めて有望な転写技術として期待さ
れ、現在各所で精力的な研究、開発が行われている。本
発明者も、長らくX線露光技術の研究に携わってきたが
、一つの重要な問題点を見出した。第1図に、問題点と
思われる実験事実を示す特性を示す。本図は、特性X線
(この場合は波長5.41XのM 01iα線)をネガ
レジストP GMAにX線マスクを介さないで直接照射
した場合における、PGMAの残存膜厚の露光雰囲気(
この場合は空気)圧力依存性を示している。(Prior art and its problems) X-ray exposure technology is expected to be an extremely promising transfer technology in the future due to its reliable high resolution of submicron width patterns, and active research and development is currently being carried out in various places. It is being said. The present inventor has been involved in research on X-ray exposure technology for a long time, and has discovered one important problem. Figure 1 shows characteristics that indicate experimental facts that are considered to be problematic. This figure shows the exposure atmosphere for the remaining film thickness of PGMA (
In this case, air) shows pressure dependence.
MoLα線のドース量によ、低圧空気雰囲気において〜
60チの残存膜厚を得る5 5 mlT/C<に設定し
た。Depending on the dose of MoLα radiation, in a low pressure air atmosphere ~
It was set at 5 5 ml T/C< to obtain a residual film thickness of 60 inches.
圧力が増加すると、その空気雰囲気での特性X線の吸収
が多くなるから、その場合は55mJy(iのドース量
がP()MAレジストに与えられるように露光時間を多
くして調整した。As the pressure increases, absorption of characteristic X-rays increases in the air atmosphere, so in that case, the exposure time was increased so that a dose of 55 mJy(i) was applied to the P()MA resist.
図から分かるように、圧力が増加すると、P(IMAの
残存膜厚は、かなり減少している。ネガレジストのこの
ような現象、すなわち空気圧力の増加による架橋の減退
反応は、詳細な機構については解明されてい々いが、空
気中の酸素による効果であることが実験的に認められて
いる。例えば、1975年に発行された刊行物ジャーナ
ル・オブ・バキュウム・サイエンス−アンド・テクノロ
ジー(・工。As can be seen from the figure, as the pressure increases, the residual film thickness of P(IMA) decreases considerably.This phenomenon of negative resist, that is, the reduction reaction of crosslinking due to increase in air pressure, is explained in detail by the mechanism. Although this has not been fully elucidated, it has been experimentally confirmed that it is an effect of oxygen in the air.For example, in the 1975 publication Journal of Vacuum Science and Technology, .
Vac、Sci 、Technol、)第12巻、第1
329頁に同様の効果が指摘されている。第1図におい
て、空気圧力の増加に対してPGMA残存膜厚が減少す
るということは、圧力の増加とともにP(3MAレジス
トの感度が減少していくことを意味する。図で最高圧力
は2670Paであり、そのときの残存膜厚は、圧力に
おける約55チの値から約35%まで落ちている。Vac, Sci, Technol,) Volume 12, No. 1
A similar effect is pointed out on page 329. In Figure 1, the fact that the PGMA residual film thickness decreases as the air pressure increases means that the sensitivity of the P (3MA resist) decreases as the pressure increases. The remaining film thickness at that time was reduced to about 35% from the value of about 55 inches at pressure.
このような現象は次のような観点から、X線露光技術に
おいて大きな問題である。現状においてX線露光システ
ムの露光雰囲気は真空、Heガス、あるいは大気(空気
)においてそれぞれ可能であるが、どれか一つというよ
うには定まっていない。Such a phenomenon is a major problem in X-ray exposure technology from the following viewpoints. Currently, the exposure atmosphere of the X-ray exposure system can be vacuum, He gas, or atmosphere (air), but it has not been determined that only one of them is possible.
第1図の圧力範囲け67〜2670pa の低真空領域
であるが、残存膜厚が圧力変化に対して変動することは
、定められた残存膜厚全稈る必要があるデバイス作製に
おいて支障となる。もっとも、露光雰囲気の圧力を定め
てやれば、常に一定の残存膜厚が得られるが、この場合
は雰囲気の圧力を一定に制御する機構を余分に装備して
おく必要がある。以上が第一の観、点である。The pressure range shown in Figure 1 is in the low vacuum region of 67 to 2670 pa, but the fact that the residual film thickness fluctuates in response to pressure changes is a problem in the fabrication of devices that require the entire culm to have a specified residual film thickness. . However, if the pressure of the exposure atmosphere is determined, a constant residual film thickness can always be obtained, but in this case, it is necessary to provide an additional mechanism for controlling the pressure of the atmosphere to a constant value. The above is the first point.
第二の観点として、大気中露光方式に関連した事項があ
る。大気中露光方式は、Xi露光システムの設計及び構
成のしやすさにおいて優れており、将来の相当に有望庁
露光方式と考えられる。特にステップ・アンド・リピー
ト型のシステムにおいて一層そのメリットが生かされや
すい。ところが第1図から分かるように、大気中(〜1
0 ’ 、Pa )では、感度が相当低下することが予
想される。前述のように酸素による架橋減退反応が堕め
て犬きくなるからであン)。レジストの感度の低下は、
X紳露光シておけるスループットに直接関係してくるた
め、重大な問題点である。X紳露光の将来に渡る大きな
課題は高スループツト化であるが、その高スルーブツト
達成の一つの大きな手段H1高感度X線レジストの開発
である。高感度t/レジスト、BVCネガレジストにお
いて得らハることが多い。The second point is related to the atmospheric exposure method. The atmospheric exposure method is superior in the ease of designing and configuring the Xi exposure system, and is considered to be a very promising exposure method in the future. This advantage is particularly easy to take advantage of in step-and-repeat systems. However, as can be seen from Figure 1, in the atmosphere (~1
0', Pa), the sensitivity is expected to decrease considerably. This is because, as mentioned above, the cross-linking reduction reaction caused by oxygen slows down, resulting in a dog-like appearance). The decrease in resist sensitivity is
This is a serious problem because it is directly related to the throughput of X-ray exposure. A major challenge for the future of X-ray exposure is to increase throughput, and one major means of achieving this high throughput is the development of H1 high-sensitivity X-ray resists. It is often obtained in high-sensitivity t/resists and BVC negative resists.
ところが、その高感度ネガレジストにおいて、第1図の
ようなy囲気依存性による感度の低下現象がみられると
なると、大きな問題点である。However, if such a high-sensitivity negative resist exhibits a decrease in sensitivity due to the y-ambience dependence as shown in FIG. 1, it is a major problem.
第2図において、特性X線としてPdLa線(波長4.
37A)を用いた場合の上述と同様の圧力依存性が示さ
れている。ドーズ量は130mり侃、レジストは第1図
と同じ< P()MAである。この場合も同様の現象が
みられており、上述の解釈がそのまま当てはまる。In FIG. 2, PdLa rays (wavelength 4.
A pressure dependence similar to that described above with 37A) is shown. The dose amount was 130 m and the resist was <P()MA, the same as in FIG. A similar phenomenon is observed in this case as well, and the above interpretation applies as is.
(発明の目的)
本発明の目的は、このような従来の欠点を除去せしめて
、露光雰囲気に拘わらず一定の高感度を示すネガレジス
トを用いることが出来る新た々X線露光方法を提供する
ことにある。(Object of the Invention) An object of the present invention is to provide a new X-ray exposure method that eliminates such conventional drawbacks and can use a negative resist that exhibits a constant high sensitivity regardless of the exposure atmosphere. It is in.
(発明の構成)
すなわち本発明によれば、X線源から放射されるX線を
X線マスクを通してX線レジストを塗布した被加工物に
照射するX線露光方法において、前記X線レジストの上
層としてに* Ca p N a r M g *A
4.Zn 、F e、 N i + 3 n + P
d #あるいはCuなどのイオン化傾向の大きい薄い金
属膜を形成して露光することを特徴とするX線露光方法
が得られる。(Structure of the Invention) That is, according to the present invention, in an X-ray exposure method in which a workpiece coated with an X-ray resist is irradiated with X-rays emitted from an X-ray source through an X-ray mask, the upper layer of the X-ray resist is As* Cap N a r M g *A
4. Zn, Fe, N i + 3 n + P
An X-ray exposure method is obtained which is characterized in that a thin metal film having a high ionization tendency, such as d# or Cu, is formed and exposed.
(実施例)
以下本発明の構成について、図面を参照しながら説明す
る。(Example) The configuration of the present invention will be described below with reference to the drawings.
第3:図は、本発明に係るX線露光方法の一実施例を示
す概略図である。基本構成としては、X線源1と、X線
マスク2と、X線レジスト3が塗布された被加工物4か
ら成る。X線源1から放射されるX′a束5がX線マス
ク2を通してX線レジスト3上に照射される。このとき
X糾マスク上の吸収体パターン部6(通常はAu)にお
いてはX線束は吸収され、下のレジスト面には達しない
。ここで、X線マスク2とX線レジスト3との間の露光
雰囲気は、真空、)Ieガス、あるいは大気いずれでも
よいが、前述の問題点のところで詳述したように大気(
空気)の場合について述べる。Third: The figure is a schematic diagram showing an embodiment of the X-ray exposure method according to the present invention. The basic configuration consists of an X-ray source 1, an X-ray mask 2, and a workpiece 4 coated with an X-ray resist 3. An X'a flux 5 emitted from an X-ray source 1 is irradiated onto an X-ray resist 3 through an X-ray mask 2. At this time, the X-ray flux is absorbed by the absorber pattern portion 6 (usually made of Au) on the X-ray mask and does not reach the resist surface below. Here, the exposure atmosphere between the X-ray mask 2 and the X-ray resist 3 may be vacuum, ) Ie gas, or air;
Let us discuss the case of air).
大気の場合、多量の酸素の影響によって高感度X線ネガ
レジストの感度の低下が著しい。そこで本発明では、新
たにX線レジスト3の上に薄い金属膜7を形成するとい
う構成をとる。この金属膜としては、K、Ca + N
a * Mg 、A l* Znr F e + N
1rPdあるいはCu などが用いられる。これらの
金属はイオン化傾向が大きく、空気中において表面に酸
化物が出来やすい。この点が要点であるが、こね、らの
金属の薄い膜をX線レジスト上に形成して、空気中の酸
素と金属膜とを反応させ、反応を金属の表面(あるいは
薄い金属層全体)でくい止めX1liIレジストまで酸
素を通過させないようにするわけである。言い換えると
、これら薄い金属膜は一種の還元剤として働き、空気中
の酸素を吸収して安定な酸化物となって一種の保護膜と
なって内側のX線レジスト層への酸素の侵入を防ぐ。と
のように、イオン化傾向の大きい金属の特性を巧みに利
用することによって、薄い金属膜のみにおいて酸素を取
り込み、X線レジストへの酸素の侵入を防ぐことが出来
、本発明の目的は達成される。In the case of the atmosphere, the sensitivity of high-sensitivity X-ray negative resists is significantly reduced due to the influence of a large amount of oxygen. Therefore, the present invention adopts a configuration in which a thin metal film 7 is newly formed on the X-ray resist 3. As this metal film, K, Ca + N
a * Mg , A l * Znr F e + N
1rPd or Cu is used. These metals have a strong tendency to ionize and easily form oxides on their surfaces in the air. The key point here is that by forming a thin film of metal on an X-ray resist, oxygen in the air reacts with the metal film, and the reaction occurs on the surface of the metal (or the entire thin metal layer). This prevents oxygen from passing through to the X1liI resist. In other words, these thin metal films act as a kind of reducing agent, absorbing oxygen from the air and turning into stable oxides, forming a kind of protective film that prevents oxygen from penetrating into the inner X-ray resist layer. . By skillfully utilizing the characteristics of metals that have a strong tendency to ionize, oxygen can be taken in only in a thin metal film and oxygen can be prevented from entering the X-ray resist, and the object of the present invention has been achieved. Ru.
すなわち最悪の争件である大気(空気)に卦いて酸素の
影響を受けないX線レジストの状態が7iられるという
ことは、露光雰囲気によらず一定の高感度を示すネガレ
ジストを得ることが出来る。In other words, the fact that the condition of the X-ray resist, which is unaffected by oxygen in the atmosphere (air), which is the worst issue, can be improved to 7i means that it is possible to obtain a negative resist that exhibits a constant high sensitivity regardless of the exposure atmosphere. .
薄い金属膜の膜厚は、金属の種類によって若干異なると
思われるが数十へ〜数千Aの範囲内である。またX線露
光後において、X線レジストを現像する前に、薄い金属
膜を除去する必要がある場合には、適当なドライエツチ
ング(例えば0□。The thickness of the thin metal film may vary slightly depending on the type of metal, but it is in the range of several tens to several thousand amps. If it is necessary to remove a thin metal film after X-ray exposure and before developing the X-ray resist, appropriate dry etching (for example, 0□.
Arガスを用いて)、あるいはウェットエツチング等の
手法によって容易に可能である。This can easily be done by a method such as using Ar gas) or wet etching.
(発明の効果)
以上説明したように本発明によれば、第1に露光雰囲気
によらず高感度ネガ型X線レジストを用いた高スループ
ットX紳バ光がより確実になり、第2に高感度X線レジ
ストを開発する際により大きな許容度(すなわち酸素と
の反応による低感度化は考慮する必要がない)を与える
ことが出来、第3にX線露光の露光雰囲気等のシステム
設計に自由度を与えることが出来る効果を有するもので
ある。(Effects of the Invention) As explained above, according to the present invention, firstly, high-throughput X-ray radiation using a high-sensitivity negative X-ray resist can be achieved regardless of the exposure atmosphere; Greater tolerance can be given when developing sensitive X-ray resists (i.e., there is no need to consider lower sensitivity due to reaction with oxygen), and thirdly, there is greater freedom in system design such as the exposure atmosphere for X-ray exposure. It has the effect of giving strength.
第1図、第2図は、従来技術の問題点であるネガ型レジ
ストの残存膜厚(すなわち感度)の露光雰囲気(空気)
圧力依存性を示した図、第3図は本発明にがかる一実施
例であるX線露光方法を説明するための饋略図である。Figures 1 and 2 show the exposure atmosphere (air) of the remaining film thickness (i.e. sensitivity) of the negative resist, which is a problem with the conventional technology.
FIG. 3, a diagram showing pressure dependence, is a schematic diagram for explaining an X-ray exposure method that is an embodiment of the present invention.
Claims (1)
通じてX線レジストを塗布した被加工物に照射するX線
露光方法において、前記X線レジストの上層としてイオ
ン化傾向の大きい薄い金属膜を形成して露光することを
特徴とするX線鯖光方法。(1) X1FJ emitted from the X-ray source! An X-ray exposure method in which a workpiece coated with an X-ray resist is irradiated with X-rays through an X-ray mask, the X-rays being exposed after forming a thin metal film with a high ionization tendency as an upper layer of the X-ray resist. Sabamitsu method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59079498A JPS60222849A (en) | 1984-04-20 | 1984-04-20 | X-ray exposure method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59079498A JPS60222849A (en) | 1984-04-20 | 1984-04-20 | X-ray exposure method |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS60222849A true JPS60222849A (en) | 1985-11-07 |
Family
ID=13691584
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59079498A Pending JPS60222849A (en) | 1984-04-20 | 1984-04-20 | X-ray exposure method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60222849A (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62206546A (en) * | 1986-03-07 | 1987-09-11 | Nec Corp | Method for forming x-ray resist film |
| WO2004047155A1 (en) * | 2002-11-19 | 2004-06-03 | Nikon Corporation | Euv exposure method, euv exposure system and euv exposure substrate |
| EP1480078A1 (en) * | 2003-05-21 | 2004-11-24 | ASML Netherlands B.V. | Method for coating a substrate for EUV lithography and substrate with photoresist layer |
| WO2015046327A1 (en) * | 2013-09-26 | 2015-04-02 | 独立行政法人物質・材料研究機構 | Highly sensitive multilayer resist film and method for improving photosensitivity of resist film |
-
1984
- 1984-04-20 JP JP59079498A patent/JPS60222849A/en active Pending
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62206546A (en) * | 1986-03-07 | 1987-09-11 | Nec Corp | Method for forming x-ray resist film |
| WO2004047155A1 (en) * | 2002-11-19 | 2004-06-03 | Nikon Corporation | Euv exposure method, euv exposure system and euv exposure substrate |
| EP1480078A1 (en) * | 2003-05-21 | 2004-11-24 | ASML Netherlands B.V. | Method for coating a substrate for EUV lithography and substrate with photoresist layer |
| WO2015046327A1 (en) * | 2013-09-26 | 2015-04-02 | 独立行政法人物質・材料研究機構 | Highly sensitive multilayer resist film and method for improving photosensitivity of resist film |
| JPWO2015046327A1 (en) * | 2013-09-26 | 2017-03-09 | 国立研究開発法人物質・材料研究機構 | High-sensitivity laminated resist film and method for improving sensitivity of resist film |
| US9703197B2 (en) | 2013-09-26 | 2017-07-11 | National Institute For Materials Science | High-sensitivity multilayer resist film and method of increasing photosensitivity of resist film |
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