1. Field of the Invention
The present disclosure relates to a mirror arrangement for reflecting electromagnetic radiation, and to a method for manufacturing such a mirror arrangement. The present disclosure further relates to an optical system having a mirror arrangement and to a lithographic method of manufacturing a miniaturized device using a projection exposure system.
2. Brief Description of Related Art
A mirror arrangement has a mirror surface the geometry of which determines the optical properties of the mirror. The mirror arrangement can be integrated within an optical system and determine a path of rays therein. In particular, the optical system may comprise a projection optical system as it is used in lithographical methods for imaging a reticle onto a photosensitive layer for manufacturing of miniaturized components.
A success of such optical systems depends among other things on the precision in which the shape of the mirror surface of the mirror arrangement matches a predefined shape of the mirror surface.
From U.S. Pat. No. 5,986,795 a mirror arrangement is known the mirror surface of which is deformable to form the optical properties of the mirror variably and to particularly be able to adapt these to desired optical properties. According to this the mirror arrangement of the art comprises a substrate having a mirror side facing towards the radiation to be reflected, where a mirror surface is provided and a back side facing away from the mirror side. Further, a reaction plate is arranged in a distance apart from the back side and between the substrate and the reaction plate a plurality of actuators arranged with a distance from each other is provided, which actuators are hold with one end to the substrate and with the other end to the reaction plate. By operation of the actuators it is possible to deform the substrate and by this the mirror surface in a predefined manner. Concerning the arrangement of the art it is further provided to keep the layer thickness of the substrate and the thickness of the reaction plate over the cross section of the mirror surface not constant but to design the thicknesses variably in order to manipulate the bending characteristics of the substrate.
The arrangement of the related art is complicated with respect to its assembly having a plurality of actuators and with respect to the control of the actuators during operation.
It is further known to provide deformable mirror arrangements by applying a piezoelectric layer onto a back side of a substrate providing a mirror surface. By triggering of a piezoeffect in such a layer consequently the mirror surface is deformable. Nevertheless a bending characteristics of the mirror surface cannot be adapted to a desired characteristic.
The present invention has been accomplished taking the above problems into consideration.
It is an object of the present invention to provide a mirror arrangement having a deformable mirror surface and which is adaptable to a desired characteristic with respect to a bending characteristic of the mirror surface on operation of an actuator.
Further it is an object of the present invention to provide an optical system having the aforementioned mirror arrangement.
Still further it is an object of the present invention to provide a lithographic method of manufacturing a miniaturized device using a projection exposure system.
In order to achieve such object, the present invention provides a mirror arrangement for reflecting electromagnetic radiation, the mirror arrangement comprising a substrate having a mirror side facing towards the radiation to be reflected and a back side opposite to the mirror side, wherein a mirror surface is provided on the mirror side and wherein an actuator arrangement for generating a deformation of the substrate is mounted on the back side of the substrate, wherein the actuator arrangement comprises at least one active layer having an areal adhering contact with a portion of the back side of the substrate.
The at least one active layer has a first layer thickness at a first location within the portion and a second layer thickness at a second location disposed at a distance from the first location within the portion, wherein the first layer thickness differs from the second layer thickness by more than 1%. Because of the locally different layer thicknesses of the active layer the actuator provides locally different operational forces for deformation of the substrate. By an appropriate selection of the layer thickness distribution of the active layer on the substrate it is thereby possible to set a distribution of deformation force of the actuator on the substrate.
Between the two locations being disposed within a distance from each other the layer thickness changes preferably continuously and continually. In particular the active layer can be made from a material which comprises a ferroelectric material, a piezoelectric material, a magnetostrictive material, an electrostrictive material and a memory metal alloy.
According to one embodiment of the invention the layer thicknesses at the both locations differ by more than 1%. Further the layer thicknesses can have bigger differences at the both locations. As for example 2%, 3%, 4%, 5%, 6%, 7%, 8%, 9% ore more.
According to a further embodiment of the invention the at least one active layer has a rotational symmetric distribution of layer thickness with respect to an axis of symmetry. According to an alternative embodiment the distribution of layer thickness of the active layer is rotationally unsymmetric; which is, at all locations within the portion, rotationally non-symmetric with respect to all lines extending through each respective location.
According to a further embodiment of the invention the distribution of the layer thickness is substantially representable by one single Zernike polynomial. With such a distribution of layer thickness it is possible to set wavefront variations using the mirror surface which also correspond to the corresponding Zernike polynomial, when the mirror stands in the pupil, respectively, correspond to polynomials, which are determined by the position of the mirror and by the transfer behaviour of the optical system. Such wavefront variations are desired in optical systems for further compensation of aberrations. In alternative for the description of the distribution of the layer thickness based on Zernike polynomials also other appropriate functional systems are possible as for example splines, Tschebyscheff polynomials, modular descriptions, free surface forms.
According to a further embodiment of the invention the substrate has a first substrate thickness at the first location within the portion and a second substrate thickness at the second location within the portion, and wherein the first substrate thickness differs from the second substrate thickness by more than 1%. Also bigger differences as for example 2%, 3%, 4%, 5%, 6%, 7%, 8%, 9%, 10%, 11%, 12%, 13%, 14% or more are provided.
According to an embodiment the actuator arrangement comprises one single active layer, wherein the areal adhering contact of the active layer with the portion of the back side of the substrate is mediated by an intermediate adhesion layer firmly joining the active layer to the back side of the substrate. The intermediate adhesion layer can comprise an adhesive, a solder, an eutecticum, a paste and other layers. According to an embodiment the adhesion mediation layer also provides an electrode layer for exciting the active layer. According to an alternative embodiment an electrode layer is a supplement to the adhesion mediation layer as a further layer arranged between the active layer and the substrate. According to an embodiment of the invention the electrode layer continuously extends over the portion of the back side of the substrate.
According to an embodiment of the invention the actuator arrangement comprises a plurality of active layers which are stacked one above the other, wherein each pair of active layers are joined to each other by an areal adhering contact.
According to an embodiment of the invention the mirror arrangement comprises a bottom layer of the plurality of active layers and arranged closest to the substrate, wherein the areal adhering contact of the bottom active layer with the portion of the back side of the substrate is mediated by an intermediate adhesion layer firmly joining the active layer to the back side of the substrate. According to an embodiment of the invention an electrode layer for exciting the active layer is disposed between the bottom active layer and the substrate. According to an embodiment of the invention the electrode layer comprises the adhesion mediating layer.
According to an embodiment of the invention at least one electrode layer for exciting at least one active layer of a pair of adjacent layers is disposed between said pair of adjacent active layers. According to an embodiment of the invention the electrode layer continuously extends over the portion of the back side of the substrate.
According to an alternative embodiment of the invention the electrode layer comprises a plurality of non-overlapping partial electrodes, distributed over the portion of the back side of the substrate. According to a further embodiment of the invention first and second partial electrodes of each pair of partial electrodes are electrically insulated from each other. Still further according to an embodiment of the invention an electrical resistance between first and second partial electrodes of each pair of partial electrodes is greater than 1 M Ω. According to an exemplary embodiment the plurality of partial electrodes are arranged in a hexagonal pattern. The plurality of partial electrodes is groupable into electrode groups, wherein the electrode groups are arranged in a hexagonal pattern.
The invention further provides a method of manufacturing a mirror arrangement for reflecting electromagnetic radiation, wherein the method comprises:
According to an exemplary embodiment the distributing of the precursor material comprises rotating of the substrate about an axis of rotation. The rotating proceeds such that the precursor material distributes according to an equilibrium between the centripetal force and the gravitational force at the different locations of the precursor material. Also a viscosity of the precurser material can provide a force affecting the shape of the surface, the layer thicknesses respectively.
According to another embodiment the distributing of the precursor material comprises pressing a shaped stamp into the layer to shape the layer according to a surface shape of the stamp. By this also the desired layer thicknesses distribute according to the shape of the surface shape of the stamp. According to an exemplary embodiment the surface shape of the stamp comprises at least one of a concave portion and a convex portion. According to another exemplary embodiment the surface shape of the stamp comprises at least one of plural concave portions and plural convex portions.
The invention further provides an optical system having a plurality of optical elements, wherein at least one of the optical element comprises a mirror arrangement as described above.
According to another embodiment of the invention an optical system is provided, the optical system having a plurality of optical elements, wherein at least one of the optical elements comprises a mirror arrangement for reflecting electromagnetic radiation, wherein the mirror arrangement comprises a substrate having a mirror side facing towards the radiation to be reflected and a back side opposite to the mirror side, wherein a mirror surface is provided on the mirror side and wherein an actuator arrangement for generating a deformation of the substrate is mounted on the back side of the substrate, wherein the actuator arrangement comprises at least one active layer having an areal adhering contact with a portion of the back side of the substrate; wherein the at least one active layer has a first layer thickness at a first location within the portion and a second layer thickness at a second location disposed at a distance from the first location within the portion, wherein the first layer thickness differs from the second layer thickness by more than 1%; and wherein the at least one active layer comprises at least one of a ferroelectric material, a piezoelectric material, a magnetostrictive material, an electrostrictive material and a memory metal alloy.
According to another embodiment of the invention the optical system can also be a catadioptrical system wherein at least one of the optical elements comprises a refractive lens. In an alternative embodiment the optical system comprises only mirrors as the optical elements.
According to another embodiment of the invention the optical system further comprises a mount for mounting a patterning structure to be imaged in a region of an object plane of the optical system, and a mount for mounting a substrate having a radiation sensitive layer in an image plane of the optical system.
According to an embodiment the optical system comprises an objective of a lithographic system for imaging a pattern forming structure (reticle) onto a photosensitive layer (resist), which is provided on a substrate (wafer).
According to another embodiment of the invention lithographic method of manufacturing a miniaturized device using a projection exposure system optical system is provided, wherein the method comprises: disposing a patterning structure to be imaged in a region of an object plane of an imaging optics of the projection exposure system; disposing a substrate carrying a resist in a region of an image plane of the imaging optics and exposing portions of the substrate with images of the patterning structure using the projection exposure system; wherein the projection exposure system comprises a plurality of optical elements, and wherein at least one of the optical elements comprises a mirror arrangement as described above.
The forgoing as well as other advantageous features of the invention will be more apparent from the following detailed description of exemplary embodiments of the invention with reference to the accompanying drawings, wherein
a-6d,
a and
b show lines of height of a thickness distribution of an active layer according to further embodiments of mirror arrangements according to the present invention;
It is noted that not all possible embodiments of the present invention necessarily exhibit each and every, or any, of the advantages described herein.
In the exemplary embodiments described below, components that are alike in function and structure are designated as far as possible by alike reference numerals. Therefore, to understand the features of the individual components of a specific embodiment, the descriptions of other embodiments and of the summary of the invention should be referred to.
In
The back side 7 of the substrate 3 is firmly joint to the active layer 13 made of a piezomaterial as for example lead-circonate-titanate (PZT). Also the layer 13 made of piezomaterial is rotationally symmetric with respect to axis 9, wherein the back side 0.15 facing away from the substrate is a flat surface.
The front side 5 of the substrate 3, respectively, the mirror surface 11 has a concave parabolic shape. The back side 7 of the substrate 3 exhibits a similar form so that the substrate exhibits a same thickness (a1, a2) at each location on the substrate.
Nevertheless a layer thickness of layer 13 made of piezomaterial is dependent on location. It thus exhibits at a location I, a thickness b1 which is greater than a thickness b2 at a location II.
For the operation of the layer 13 as actuator an electrical potential generated by a controlled voltage supply 16 is applied to an electrode 12 provided between the substrate 3 and the layer 13 and to a further electrode 14 provided at a back side 15 of the layer 13, so that based on the piezoelectrical effect in layer 13 this layer generates a mechanical force which leads to deformation of the substrate as well as the mirror surface 11. In the illustrated exemplary embodiment the electrodes 12 and 14 are area electrodes extending continuously over the whole surface of the active layer 13. The electrode 12 by this forms also a intermediate adhesion layer between the substrate 3 and the active layer 13. For this the electrode 12, the intermediate adhesion layer, respectively, can be formed by a gold paste.
This deformation is determined by the thickness and rigidity of the substrate 3, the thickness and rigidity of the layer 13 made of piezomaterial and the location dependency of the layer thickness of the layer 13. Depending on the location dependent layer thickness of layer 13 the location dependency of the piezo force is determined.
In the following further variants of the embodiment illustrated in
The mirror arrangement 1a shown in
The geometrical relations of the mirror arrangement in
The mirror arrangement 1b shown in
Concerning the mirror arrangement 1c shown in
The mirror arrangement id shown in
The process uses a mould 21 into which at the beginning of the process (
Onto the back side 7 of the substrate 3 a piece 25 of PZT-paste, the precursor material of the piezoelectric layer 13 to be produced, will be applied. Then the form 21 will be put into rotation around the axis 9, so that the piece 25 of PZT-paste spreads on the back side 7 of the substrate 3 (
Then the PZT-paste 25 is heated (arrows ˜27 in
According to a further embodiment of the method of manufacturing a piezoelectric layer a so-called Mandrel technique is employed. A polished and with gold (Au) vapor-deposited stamp 30 having a predetermined geometric shape of a stamp surface 33 fits into the form and is pressed into the latter such forming the shape of the PZT-paste 25. Thereafter the PZT-paste 25 is sintered at temperatures in a range of 400° C. to 900° C. In the subsequent process of cooling the vapor-deposited gold peels from stamp 30 and remains at the PZT-layer 25 because a coefficient of thermal expansion of the stamp 30 is considerably larger than a coefficient of thermal expansion of the PZT-layer 25. A temperature at which such peeling takes place can be determined empirically. In the vicinity of the peeling temperature a temperature cooling speed, with which the stamp and the sintered layer are being cooled during a process of cooling, is reduced essentially so that internal tensions in the arrangement distribute as even as possible.
a shows a top view onto an active layer 15e of a mirror arrangement 1e. Here, the lines 31 and 32 represent lines of height of a distribution of layer thickness of the active layer. Differently from the embodiments explained above the distribution of layer thickness of the active layer 13e of the mirror arrangement 1e is not rotational symmetric to an axis. Rather the lines of height 31 represent a reduced layer thickness of the active layer and the lines of height 32 represent a enlarged layer thickness of the active layer. By this a symmetry of the distribution of thickness is a two-fold symmetry around an axis 9e, wherein main axis of this symmetry in
Such a distribution of layer thickness generates, with a corresponding excitation of the active layer, a deformation of the mirror surface which again is representable by a Zernike polynomial, so that also wavefronts of the light being reflected from the mirror surface suffer an according deformation in the wavefront. The deformation generated by the mirror surface of the mirror arrangement 1e can thus serve for the specific generation or compensation of an astigmatism in an optical system.
The distribution in layer thickness of the active layer as explained according to
The distribution in layer thickness as explained according to
A structure of the electrode layer 14f1 is schematically illustrated in
Background information for the optical system shown in
Besides the employment of the deformable mirror in a pure reflective optical system also an employment of the deformable mirror is provided in a katadioptrical system. Background information concerning katadioptrical imaging systems can for example be obtained from U.S. Pat. No. 6,229,647 B1 and EP 1069448 B1. By this it is possible to provide the deformation of the mirror surface such that the wavefront deviations are generated by the deformation are representable by Zernike polynomials. In this case the deformable mirror is particularly well suited for the compensation of aberrations of the optical system. But it is also possible to provide deformations of the mirror surface deviating from the latter. Examples for this are compensations of non-homogeneous heat transfers into the mirror caused by radiation. Then the distribution of layer thickness of the active layer is preferably adjusted such that it is adjusted to the location dependent heat transfer caused by radiation that provided an according control of the actuators a deformation caused by the heat absorption is compensable. Also other effects induced by radiation as for example Compaction, Lens Heating or similar is thus compensable.
An example for an exemplary embodiment of the mirror arrangement of the present invention is explained in
In order to adjust the form of the piezoelectric layer of the above explained embodiment according to
Besides the application of the piezomaterial as precursor material onto the substrate it is also possible to apply piezoceramics directly onto the substrate (direct application). It is also possible to provide adhesion mediation between the substrate and the piezolayer as for example pastes particularly a gold paste, and adhesive or a solder. The piezolayer can also be formed by grinding. The grinding can be conducted on the accomplished ceramics or a green mood of the same. The piezoceramics can be formed by any production process for ceramics as for example a sol-gel-process.
In the above described embodiments the active layer consist of a piezoelectric material. Nevertheless it is also possible to use other active materials for the manufacturing of the active layer as for example a ferroelectric material, a piezoelectric material, a magnetostrictive material, an electrostrictive material or a memory metal alloy. Magnetostrictive materials for example can be formed on the basis of Lanthanit-ferrum-alloys as for example Terfenol or Terfenol-D, and electrostrictive materials can for example be formed on the basis of Lead-magnesium-niobate as for example PMN or Lanthanum-circonate-titanate as for example PLZT. These materials can be employed in the same manner as in the above described embodiments thus forming the active layer formed according to the present invention. Further information concerning appropriate active materials can be obtained from the PhD-thesis “Ein Beitrag zur Untersuchung von Bimorphspiegeln für die Präzisionsoptik”, by Timo Richard Möller, published in Shaker Verlag 2002, ISBN 3-8322-0555-1.
While the invention has been described also with respect to certain specific embodiments thereof, it is evident that many alternatives, modifications and variations will be apparent to those skilled in the art. Accordingly, the exemplary embodiments of the invention set forth herein are intended to be illustrative and not limiting in any way. Various changes may be made without departing from the spirit and scope of the present invention as defined in the following claims.
Summarized, described herein is a mirror arrangement for reflecting electromagnetic radiation, the mirror arrangement comprising: a substrate having a mirror side facing towards the radiation to be reflected and a back side opposite to the mirror side, wherein a mirror surface is provided on the mirror side and wherein an actuator arrangement for generating a deformation of the substrate is mounted on the back side of the substrate, wherein the actuator arrangement comprises at least one active layer having an areal adhering contact with a portion of the back side of the substrate; wherein the at least one active layer has a first layer thickness at a first location within the portion and a second layer thickness at a second location disposed at a distance from the first location within the portion, wherein the first layer thickness differs from the second layer thickness by more than 1%; and wherein the at least one active layer comprises at least one of a ferroelectric material, a piezoelectric material, a magnetostrictive material, an electrostrictive material and a memory metal alloy.
Number | Date | Country | Kind |
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103 49 290.9 | Oct 2003 | DE | national |