Framed pellicle for protection of photolithographic photomask

Radiation imagery chemistry: process – composition – or product th – Radiation modifying product or process of making – Radiation mask

Reexamination Certificate

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C428S014000, C355S075000

Reexamination Certificate

active

06593034

ABSTRACT:

BACKGROUND OF THE INVENTION
The present invention relates to a novel framed pellicle for protection of a photolithographic photomask or, more particularly, to a framed pellicle used for dustproof protection of a photomask used in the technology of photolithographic patterning by pattern-wise exposure of a photoresist layer to actinic rays such as ultraviolet light through a pattern-bearing photomask in the manufacturing processes of LSIs, VLSIs, liquid crystal display panels and the like.
Photolithography is a well established technology frequently employed in the manufacturing process of fine semiconductor devices such as LSIs and ULSIs as well as liquid crystal display panels in which a photoresist layer formed on a substrate surface is pattern-wise exposed to actinic rays such as ultraviolet light through a pattern-bearing transparency, which is called a photomask, mounted on or held above the photoresist layer and the thus pattern-wise exposed photoresist layer is then subjected to a development treatment.
One of the serious problems in the technology of photolithography is that dust particles are deposited on the pattern-bearing photomask more or less even in a clean room of the highest class of cleanness and, once dust deposition takes place on the photomask, absorption, irregular reflection and scattering of the exposure light are unavoidable thereby resulting in degradation of the quality of patterning of the resist layer hence adversely affecting the performance of the devices manufactured by utilizing the process of photolithography.
In view of the difficulty in complete prevention of dust particle deposition on the photomask even in a clean room of the highest class, a conventional measure undertaken in the photolithography is that a framed pellicle is mounted on the photomask and the pattern-wise irradiation of the photoresist layer is performed through the photomask with ultraviolet light transmitting the pellicle membrane of the framed pellicle. The framed pellicle here implied is an integral device consisting of a rectangular or circular frame of a rigid material such as stainless steel, aluminum and the like, referred to as the pellicle frame hereinafter, having a relatively small height, of which the two end surfaces are substantially parallel each to the other, and a thin, highly transparent plastic resin film, referred to as the pellicle membrane hereinafter, spread over and adhesively bonded to one of the substantially parallel end surfaces of the pellicle frame in a slack-free fashion.
FIG. 1
is a vertical cross sectional view of a conventional framed pellicle consisting of a rectangular or circular pellicle frame
2
of a rigid material and a thin, highly transparent plastic resin film
1
as the pellicle membrane which is spread over and adhesively bonded with intervention of an adhesive layer
3
to one of the end surfaces of the pellicle frame
2
in a slack-free fashion. The other end surface of the pellicle frame
2
is, though optional, coated with a pressure-sensitive adhesive to form an adhesive layer
4
by means of which the framed pellicle mounted on a photomask
5
is secured at the position in a demountable fashion.
When a framed pellicle is mounted on the photomask
5
, dust particles never fall directly onto the photomask
5
but are deposited on the upper surface of the pellicle membrane
1
. The dust particles deposited on the pellicle membrane
1
have no particularly adverse influences on the quality of patterning since the exposure light such as ultraviolet light is usually focused not to the dust particles on the pellicle membrane
1
but to the pattern-bearing photomask
5
which is at least several millimeters below the pellicle membrane
1
.
The material of the pellicle membrane
1
is not particularly limitative provided that the material is a plastic resin capable of giving a thin film of good mechanical strength having high transparency to the exposure light. Examples of suitable plastic resins include nitrocellulose, cellulose acetate and fluorocarbon resins. Examples of the material for the pellicle frame
2
include aluminum, stainless steel and polyethylene. The pellicle membrane
1
is adhesively bonded to one of the end surfaces of the pellicle frame
2
by a known method. For example, the end surface of the pellicle frame
2
is moistened with a solvent having good dissolving power to the plastic resin of the pellicle membrane
1
and the membrane
1
spread slack-free is brought into contact with the end surface of the pellicle frame
2
before complete evaporation of the solvent (see Japanese PatentKokai 58-219023). Alternatively, of course, the pellicle membrane
1
can be bonded to the end surface of the pellicle frame
2
by using an adhesive such as acrylic resin-based, epoxy resin-based and fluorocarbon polymer-based adhesives. The other end surface of the pellicle frame
2
opposite to the pellicle membrane
1
is coated with a pressure-sensitive adhesive
4
by means of which the framed pellicle is secured onto the surface of the photomask
5
. Examples of suitable pressure-sensitive adhesives include polybutene resin-based, polyvinyl acetate-based, acrylic resin-based and silicone resin-based adhesives (see U.S. Pat. No. 4,861,402, Japanese Patent Publication 63-27707 and Japanese Patent Kokai 7-168345). When the pressure-sensitive adhesive layer
4
is formed, it is preferable that the sticky surface of the adhesive layer
4
is temporarily protected by attaching a releasable paper sheet to the surface until actual use of the framed pellicle.
Along with the requirement in the photolithographic patterning technology of recent years for finer and finer pattern resolution, it is a remarkable trend in photolithography until now that, in order to satisfy this requirement, the pattern-wise light exposure of the photoresist layer is conducted by using a light source emitting a light of a shorter and shorter wavelength. To be more particular, the g-line light of 436 nm wavelength and the i-line UV light of 365 nm wavelength are now under the process of replacement with the deep UV light as the KrF excimer laser beam of 248 nm wavelength and, in the near future, with vacuum UV light as the ArF excimer laser beam of 193 nm wavelength. Even the F
2
excimer laser beam of 158 nm wavelength is already within the scope of possibility in the near future to accomplish a still finer pattern resolution.
Use of the above mentioned short-wavelength laser beams as an exposure light source for the patterning works of photoresist layers, however, is accompanied by several difficult problems. For example, a substantial portion of the laser beams is absorbed by the air present in the optical path to the photomask because oxygen in the air has an absorption band within the wavelength region of the laser beams employed. Further, the molecules of oxygen in the air eventually cause a reaction to form ozone molecules by absorbing the energy of the laser beams.
These problems accompanying the use of a short-wavelength laser beam as the exposure light source can of course be solved, in principle, by completely removing oxygen from the optical path of the exposure machine having a laser beam emitter mounted thereon or by filling the optical path with nitrogen gas. Namely, the air inside of the exposure machine should be fully replaced with nitrogen after introduction or setting of a semiconductor silicon wafer or a photomask therein to ensure such a low concentration of oxygen as not to exhibit any adverse influences.
When a framed pellicle is mounted on the photomask
5
, however, the space
10
surrounded by the pellicle membrane
1
, pellicle frame
2
and photomask
5
is necessarily a closed space so that, once a photomask
5
with a framed pellicle mounted thereon is brought into and set in an exposure machine, it is no longer possible to replace the air in the closed space with nitrogen gas to solve the problem due to oxygen in the optical path unless the air in the closed space is replaced in advance with nitrogen gas in the photomas

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