The accompanying drawings, which are incorporated in and constitute a part of the specification, illustrate exemplary embodiments of the invention and, together with the description, serve to explain the principles of the invention.
Exemplary embodiments, features and aspects of the present invention will now be described in detail in accordance with the accompanying drawings.
The illumination optical system according to the first exemplary embodiment includes a rod integrator 1, a prism unit 2, a zoom lens 5, a fly-eye integrator 6 serving as an optical integrator, and an aperture stop 12.
The optical integrator 6 is constituted by a plurality of small lenses which are two-dimensionally arranged, and it forms a plurality of secondary light sources near an emergent surface thereof. The optical integrator can be constituted, for example, by a fly-eye lens, a cylindrical lens array, a microlens array, or an optical pipe (rod).
The illumination optical system according to the first exemplary embodiment further includes an optical system for illuminating the original 9, which is disposed in an illumination target plane, with light emerging from the optical integrator. Such an optical system includes a condenser lens 7 and a masking imaging lens 8.
The prism unit 2 is made up of a first subunit comprising a prism 3a having a conical concave refractive surface and a prism 4a having a pyramidal concave refractive surface, and a second subunit comprising a prism 3b having a conical convex refractive surface and a prism 4b having a pyramidal convex refractive surface.
The rod integrator 1 converts light emitted from a light source (not shown) to light having a substantially uniform light intensity distribution at an emergent surface thereof. The rod integrator 1 is disposed with intent to suppress unevenness in the light intensity distribution of an effective light source. A similar effect to that of the rod integrator 1 can also be obtained by, instead of using the rod integrator 1, arranging a microlens unit or a diffraction optical element and placing a condenser lens behind it. A light beam emerging from the rod integrator 1 enters the prism unit 2, and the prism unit 2 produces multipole illumination. Details of the multipole illumination will be described later.
After the multipole illumination has been produced by the prism unit 2, the light beam enters the zoom lens 5. The zoom lens 5 enlarges and reduces the size of the effective light source without changing the shape of the effective light source.
Further, the fly-eye integrator 6 forms a plurality of secondary light sources to illuminate the original 9 in a superimposed manner through the condenser lens 7 and the masking imaging lens 8. A pattern of the original 9 is transferred to the substrate 11 through the projection optical system 103.
Prior to describing a method of producing the multipole illumination, an effective light source distribution formed by a pair of concave and convex pyramidal refractive surfaces 21 and 22 with complementary refracting actions is described with reference to
As illustrated in
On the other hand, because a radial width of the distribution is substantially constant, the annular ratio defined by (inner radius 13/outer radius 14) is increased consequently.
Also, as illustrated in
Thus, as the interval between the pair of concave and convex pyramidal refractive surfaces 21 and 22 with complementary refracting actions increases, the annular ratio is increased and the opening angle 15 is reduced.
Next, an effective light source distribution formed by a pair of concave and convex conical refractive surfaces 24 and 25 with complementary refracting actions is described with reference to
Thus, as seen from
In this first exemplary embodiment, the prism unit 2 includes the prism 3a having the conical concave refractive surface, the prism 4a having the pyramidal concave refractive surface, the prism 3b having the conical convex refractive surface, and the prism 4b having the pyramidal convex refractive surface, which are arranged in the order named from the light source side. The conical concave refractive surface and the pyramidal concave refractive surface are each a refractive surface having a concave refracting action, and the conical convex refractive surface and the pyramidal convex refractive surface are each a refractive surface having a convex refracting action. Herein, the conical refractive surfaces are formed such that the pair of concave and convex refractive surfaces has complementary refracting actions. The pyramidal refractive surfaces are also formed in a similar manner. The term “complementary” means that refractive indices are substantially the same, and that the convex surface and the concave surface have substantially the same shape in match with each other.
In this first exemplary embodiment, each concave refractive surface is formed on the side of the prism closer to the light source, and each convex refractive surface is formed on the side of the prism closer to the illumination target plane. Thus, the concave refractive surface is an incident surface, and the convex refractive surface is an emergent surface. Such an arrangement is advantageous in reducing the size of a spot generated by the refracting actions of the refractive surfaces.
However, a more compact optical system can be constituted by arranging the pyramidal concave refractive surface on the side of the prism closer to the illumination target plane and forming that prism to be integral with the prism having the conical concave refractive surface. In other words, the side on which the refractive surface is arranged is not necessarily limited to that illustrated in the first exemplary embodiment.
In the first exemplary embodiment, the second subunit comprising the prism 3b having the conical convex refractive surface and the prism 4b having the pyramidal convex refractive surface is movable in the direction of the optical axis of the illumination optical system such that the interval (relative distance) between the second subunit and the first subunit, which comprises, the prism 3a having the conical concave refractive surface and the prism 4a having the pyramidal concave refractive surface, is variable.
Although two pairs of concave and convex refractive surfaces are used, zooming is performed only by a single operation and a comparatively compact optical system is realized.
The shape of the effective light source formed by the prism unit 2 in the first exemplary embodiment will now be described with reference to
On the other hand, when the distance between the concave refractive surface and the convex refractive surface is increased, the pair of conical refractive surfaces develops an effect of increasing the opening angle 15, while the pair of pyramidal refractive surfaces develops an effect of reducing the opening angle 15.
Therefore, even when the distance between the first subunit and the second subunit is changed, influences of the pair of conical refractive surfaces and the pair of pyramidal refractive surfaces upon the opening angle 15 are cancelled and an overall change of the opening angle 15 is reduced.
Thus, according to the first exemplary embodiment, the annular ratio can be changed while suppressing the change of the opening angle 15 of the effective light source formed in the pupil plane of the projection optical system 13.
In the first exemplary embodiment described above, the prism 3a having the conical concave refractive surface, the prism 4a having the pyramidal concave refractive surface, the prism 3b having the conical convex refractive surface, and the prism 4b having the pyramidal convex refractive surface are arranged in the order named.
However, even when the four prisms are arranged as a modified example in the order of the prism 3a having the conical concave refractive surface, the prism 4a having the pyramidal concave refractive surface, the prism 4b having the pyramidal convex refractive surface, and the prism 3b having the conical convex refractive surface, an essentially similar effect can also be obtained although a difference is caused in the effective light source distribution.
While the first exemplary embodiment is able to suppress the change of the opening angle 15 smaller, the aperture stop 12 for blocking a part of the light beam can be disposed between the prism unit and the optical integrator in order to further reduce the change of the opening angle 15. The aperture stop 12 can also be disposed on the side of the zoom lens 5 closer to the light source. Although the aperture stop 12 causes a slight loss of light quantity, the opening angle 15 can be held substantially constant.
A second exemplary embodiment of the present invention will now be described with reference to
An effective light source formed in the second exemplary embodiment is illustrated in
On the other hand, as illustrated in
As described above, in each of the pair of conical refractive surfaces and the pair of pyramidal refractive surfaces, as the distance between the concave refractive surface and the convex refractive surface increases, the annular ratio is increased. In the second exemplary embodiment, when the distance between one pair of refractive surfaces is increased with zoom-moving of the second subunit, the distance between the other pair of refractive surfaces is reduced. As a result, changes of the annular ratio are canceled and maintained small. Regarding the opening angle 15, as the interval between the concave refractive surface and the convex refractive surface increases, the opening angle 15 is increased in the case of the conical refractive surfaces, but it is reduced in the case of the pyramidal refractive surfaces. Accordingly, influences of the two pairs of conical and pyramidal refractive surfaces upon the opening angle are additively generated with the movement of the second subunit.
Thus, when the second subunit is positioned close to the first subunit, the opening angle 15 is reduced, and when the second subunit is positioned close to the third subunit, the opening angle 15 is increased. Consequently, according to the second exemplary embodiment, the opening angle 15 can be changed while maintaining small the change of the annular ratio of the effective light source.
In the illustrated second exemplary embodiment, the second subunit comprises two prisms, i.e., the prism 4a having the pyramidal concave refractive surface and the prism 3b having the conical convex refractive surface. However, a more compact optical system can be constituted by forming opposite surfaces of a single prism to serve as the pyramidal concave refractive surface and the conical convex refractive surface, respectively.
The above-described exemplary embodiments are illustrated such that each refractive surface has an apex positioned near the optical axis. However, a more compact optical system can be constituted by chamfering a part of the refractive surface near the apex thereof so as to reduce the thickness of the prism having the relevant refractive surface in the direction of the optical axis.
Also, while the exemplary embodiments have been described above in connection with the case that a circular light beam enters the refractive surface, a light beam having an annular shape or a multipole shape can also be introduced by using, e.g., a diffraction optical element. In such a case, the degree of freedom in forming the effective light source distribution is further increased. In other words, the effective light source can be formed in a more variety of shapes.
According to the exemplary embodiments described above, the shape of the effective light source can be adjusted while suppressing a reduction of illumination efficiency. Further, by adjusting the positions of the subunits constituting the prism unit, one of the annular ratio and the opening angle of the effective light source can be changed while suppressing a change of the other.
An exemplary embodiment of a device manufacturing method utilizing the foregoing exposure apparatus will now be described with reference to
As many apparently widely different embodiments of the present invention can be made without departing from the sprit and scope thereof, it is to be understood that the invention is not limited to the specific embodiments thereof except as defined in the claims.
The entire disclosure of Japanese Patent Application No. 2006-246590 filed on Sep. 12, 2006 including claims, specification, drawings, and abstract is incorporated herein by reference in its entirety.
Number | Date | Country | Kind |
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2006-246590 | Sep 2006 | JP | national |