CN1894632A - Projection objective having a high aperture and a planar end surface - Google Patents

Projection objective having a high aperture and a planar end surface Download PDF

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Publication number
CN1894632A
CN1894632A CN 200480037372 CN200480037372A CN1894632A CN 1894632 A CN1894632 A CN 1894632A CN 200480037372 CN200480037372 CN 200480037372 CN 200480037372 A CN200480037372 A CN 200480037372A CN 1894632 A CN1894632 A CN 1894632A
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projection objective
optical unit
lens
index
refractive index
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S·贝德尔
W·辛格尔
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Carl Zeiss SMT GmbH
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Carl Zeiss SMT GmbH
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Priority claimed from US10/734,623 external-priority patent/US6995930B2/en
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Abstract

age plane of the projection objective suitable for microlithography projection exposure machines has a plurality of optical elements transparent for radiation at an operating wavelength of the projection objective. At least one optical element is a high-index optical element made from a high-index material with a refractive index n = 1.6 at the operating wavelength.

Description

The projection objective that high aperture and planar end surface are arranged
The background of invention
Invention field
The present invention relates to be used for the projection objective on the image surface that projection objective is provided at the pattern that provides on the object plane of projection objective.Projection objective can be used in the microlithographic projection exposure machine.The present invention be more particularly directed to be used for the exposure machine that those are designed to the semiconductor structure of submergence operation, that is to say, its image-side numerical aperture NA greater than 1.0 pore diameter range among.
Description of Related Art
Under the situation of dwindling optical imagery of projection lithography particularly, the refractive index restriction of the medium around image-side numerical aperture NA is subjected in the image space.In immersion lithographic, possible in theory numerical aperture NA is limited by the refractive index of submergence medium.The submergence medium can be liquid or solids.Under the latter's situation, be also referred to as solid immersion.
Yet, because actual cause, the refractive index of the medium (that is, approaching the medium of image most) that the aperture is should be not approaching arbitrarily not last.Because at this moment angle of propagation becomes very big with respect to optical axis.Verified, about 95% of the refractive index of last above image-side significantly medium aperture does not gear to actual circumstances.This is corresponding to the angle of propagation about 72 ° with respect to optical axis.For 193nm, this is at Yi Shui (n H2O=1.43) as under the situation of submergence medium corresponding to NA=1.35.
The liquid that is higher than the refractive index of last lens material for refractive index, or under the situation of solid immersion, if the design of last end face (exit face of projection objective) be the plane or slight curvature only, then the material of last lens unit (that is the last optical unit of the projection objective of adjacent image) plays the effect of restriction.Planar design is being favourable under the following situation for example: for the characteristic of the fluid of the submergence medium between wafer that will be exposed and last object lens face and for they cleaning and measure distance between wafer and object lens.For solid immersion, be the wafer on plane equally particularly in order to expose, last end face must be planar design,
For DUV (operation wavelength of 248nm or 193nm), the material that is generally used for last lens is to have refractive index n SiO2=1.56 fused quartz (synthetic quartz glass, SiO 2) or have refractive index n CaF2=1.50 CaF 2The synthetic quartz glass material also is called " quartz " below for short.Because the high radiation load in last lens unit particularly preferably uses calcium fluoride as last lens at 193nm, because synthetic quartz glass will be owing to radiation load damages for a long time.The numerical aperture that this causes reaching is about 1.425 (n=1.5 95%).If accept the shortcoming of radiation damage, then quartz glass still allow 1.48 (193nm corresponding to the refractive index of quartz about 95%) numerical aperture.This pass is similar when tying up to 248nm.
Brief summary of the invention
An object of the present invention is to provide high aperture projection objective, it prevents to have such as the submergence medium of water or has such as fused quartz and CaF 2The shortcoming of traditional design of lens material.Another object of the present invention provide size with appropriateness and material consumption, be suitable for the image-side immersion lithographic, numerical aperture is at least the projection objective of NA=1.35.
Solution as this and other purpose, according to a formula, the invention provides a kind of being used for the projection objective on the image surface that the projection objective that is suitable for the microlithographic projection exposure machine is provided at the pattern that provides on the object plane of projection objective, comprising: to the radiation in the projection objective operation wavelength is transparent a plurality of optical units; Wherein at least one optical unit is the high index of refraction optical unit of being made by the high-index material with refractive index n on operation wavelength 〉=1.6.
An embodiment comprises the radiation proof lithographic objective with the image-side numerical aperture that is preferably more than or equals NA=1.35, and for it, last at least lens unit comprises high-index material (refractive index n>1.6, particularly n>1.8).Thereby under the situation of the minification of (absolute value) of the convention of photoetching 4: 1 (| β |=0.25), object side (mask side) numerical aperture is NA Obj〉=0.33, NA preferably Obj〉=0.36.
Exemplary embodiment below by using for 193nm illustrates in greater detail various aspect of the present invention.In example, the material that is used for last lens unit or its parts is sapphire (Al 2O 3), and all the other lens are made by fused quartz.Yet these examples can be transferred to other high refractive index lens material and other wavelength.For example, for 248nm, might use germanium dioxide (GeO 2) as the material that is used for last lens or its parts.Compare with sapphire, this material has advantage: it is not birefringent.Yet this material no longer is transparent at 193nm.
Under liquid-immersed situation,, then can reach NA>1.35 if use immersion liquid with refractive index higher than water.In some example application, use cyclohexane (refractive index n=1.556).
Has the current reality of being considered to of the submergence medium of n>1.6.
If the thickness that use immersion liquid, then high refractive index liquid--that is to say immersion liquid--preferably can be 0.1 and 10mm between.Less thickness in this scope can be favourable, because high index of refraction submergence medium also present higher absorption usually.
The above characteristic with other singly can in the claims and can not seen in explanation and accompanying drawing, wherein each characteristic can be individually or is divided and be used as embodiments of the invention in combination, and can express embodiment favourable and can patent in other field individually.
The accompanying drawing summary
Fig. 1 is the longitdinal cross-section diagram according to first embodiment of Catadioptric projection objective of the present invention;
Fig. 2 is the longitdinal cross-section diagram according to second embodiment of Catadioptric projection objective of the present invention;
Fig. 3 is the longitdinal cross-section diagram according to the 3rd embodiment of Catadioptric projection objective of the present invention;
Fig. 4 is the longitdinal cross-section diagram according to the 4th embodiment of Catadioptric projection objective of the present invention;
Fig. 5 is the longitdinal cross-section diagram according to the 5th embodiment of Catadioptric projection objective of the present invention.
Preferred embodiment describes in detail
In the explanation of following the preferred embodiments of the present invention, term " optical axis " is meant straight line or a series of straight-line segment that passes involved optical unit center of surface.Optical axis can be folding by folding mirror (deflection mirror).Under the situation of these examples that here provide, related object is the mask (reticle) that is loaded with the pattern of integrated circuit, or certain other pattern, for example grating pattern.In these examples that here provide, the image of object is projected to the wafer that is used as substrate, is applying one deck photoresists on it, though the substrate of other type such as the element of LCD or be used for the substrate of grating, also is feasible.
Be provided at form under the occasion of technical manual of open design as shown in the figure, form is represented by the numeral identical with each accompanying drawing.
Fig. 1 show be designed to about 193nm UV operation wavelength, according to the longitdinal cross-section diagram of first embodiment of Catadioptric projection objective 100 of the present invention.It is designed to the ratio of image to dwindle of the pattern on the master (or mask) that is arranged at object plane OP for example projected to image surface IP at 4: 1, and accurately creates two real intermediate image IMI1 and IMI2 simultaneously.The first refractive objective lens part ROP1 is designed to the pattern on the object plane is imaged as the first intermediate image IMI1, second reflective (pure reflection) object lens part COP2 is imaged as the second intermediate image IMI2 to the first intermediate image IMI1 with the magnification that approached 1: 1, and third reflect object lens part ROP3 is imaged onto image surface to the second intermediate image IMI2 with very high minification.The second reflective object lens part COP2 comprises the first concave mirror CM1 that has in the face of the concave reflection minute surface of object side, and has the second concave mirror CM2 in the face of the concave reflection minute surface of image-side.Mirror surface is continuous or does not rupture that promptly they do not have hole or hole.The mirror surface that faces one another has been stipulated space between a mirror, i.e. the space that curved surface surrounded of being stipulated by the concave reflection minute surface.Two intermediate image IMI1, IMI2 are positioned at space between mirror on how much, paraxial at least intermediate image almost is in the centre away from this space of mirror surface.
One " curved surface " or " flexure plane " of each mirror surface regulation of concave mirror, it is the mathematics surface that extends to beyond the edge of physics mirror surface and comprise mirror surface.First and second concave mirrors are the parts with rotation symmetroid of public rotation axes of symmetry.
System 100 is rotational symmetric, and has one for all refraction and the common direct light axle AX in catoptrics unit.There is not folding mirror.Concave mirror has little diameter, allow them to be close together and and the intermediate image between them quite approaching.Concave mirror is building with irradiated from the axle segmentation as the rotational symmetry face.Light beam transmits by not fogging towards the edge of the concave mirror of optical axis.
That Catadioptric projection objective with this general structure is for example submitted on January 14th, 2004, sequence number 60/536,248; In U.S. Provisional Patent Application that submit to, sequence number 60/587,504 on July 14th, 2004; And be disclosed in the application of the later expansion of submitting on October 13rd, 2004.The content of these applications is integrated into the application, for your guidance.The characteristic of a characterization of such Catadioptric projection objective is: between the object plane and first intermediate image, between first and second intermediate image and on formation each perforation hole surface (on principal ray and optical axis intersecting axis position) between second intermediate image and the image surface, and all concave mirrors are arranged to optically away from the perforation hole surface, especially on the position of principal ray height above the marginal ray height of imaging processing process of imaging processing process.And, at least the first intermediate image space between the mirror that is located on how much between first concave mirror and second concave mirror preferably.Preferably, first intermediate image and second intermediate image are located on how much between mirror between the concave mirror in the space.
The illustrative example that describes below is shared these characteristics, and they allow to carry out with the optical system of the optical material structure of relatively small amount the immersion lithographic of numerical aperture NA>1.
Fig. 1 shows the 193nm lithographic objective as first exemplary embodiment, has sapphire lens and cyclohexane give and is the submergence medium and combine with the image-side numerical aperture of NA=1.45.The sapphire lens are the last optical unit LOE that approach image surface most.The image-side operating distance is 1mm.Catadioptric design has two concave mirrors, and be mainly used in chromaticity correction and Petzval and proofread and correct, and an intermediate image, be in this upstream and downstream respectively to catoptron.Yet these intermediate images are not corrected fully, and are mainly used in how much restrictions of design and are used to isolate two beam paths of advancing and advancing from catoptron at the mirror reflection back that is reflected to catoptron.Picture field (on wafer) is a rectangle.Outfield radius (on the wafer limit) is 15.5mm, and the internal field radius is 4.65mm.Such result is the rectangular field of 26 * 3.8mm.
In first exemplary embodiment, aperture diaphragm (aperture diaphragm AS, system aperture) is arranged at the first refractive objective lens part ROP1.This is favourable, on the one hand in order to make less variable aperture diaphragm, and on the other hand, when the diaphragm of reduced bore, mainly protects later object lens parts (seeing from object plane (mask face)) to avoid useless and the radiation load that disturbs.Caudacoria in image-side object lens part ROP3 is unilateral, can place the aperture location of aperture therein, is positioned in the zone between the lens LMD of maximum gauge and the image surface IP on the converging beam path.
A contraction section (contraction of light beam and lens diameter) is formed among the local object lens ROP1 that reflects before the object side, and this contraction section is mainly used in correcting image curvature of field face (Petzval summation).Aperture diaphragm AS is arranged at contraction section.
CaF 2It is not preferred being used for last lens, because this need be not more than 1.425 (CaF as far as possible 2Refractive index about 95%) numerical aperture.In this example, sapphire (Al 2O 3) be used as high-index material among the last lens unit LOE at 193mm.In all embodiment as shown in the figure, the optical unit of being made by sapphire draws hacures becomes grey, so that reference.
The birefringence that takes place when using sapphire is by being separated into last lens two lens unit LOE1 and LOE2 and rotating two lens units relative to each other and compensated to a great extent around optical axis.In this case, separate interface S1 (surface of contact of two lens unit LOE1 and LOE2) and preferably be bent, so that two lens units have similar refracting power.Alternatively, might use the Unit of being made by sapphire second that is arranged near near position of object lens (for example the intermediate image or object plane) for compensation, it plays similar effect aspect optics.In this example, last sapphire lens LOE is separated into two lens unit LOE1 and the LOE2 that in fact plays same function.The preceding radius surface of sapphire lens LOE (promptly, the radius of light approaching side) is designed such that the aperture light beam, promptly the center of the light beam trend picture field of advancing to image with the circumference (parimeter) of assembling light beam is passed interface and is actually aclastic, that is to say, in fact vertically project interface (in fact lens radius is concentric with the point of crossing of image surface and optical axis).At the radius of cutting apart interface SI between two lens units of this sapphire split lens (split lens) is more smooth (distance between image surface of wafer be multiply by and can be placed on it in radius>1.3).
For example in by the applicant's patented claim DE 101 23 725 A1 (for example corresponding to US 2004/0190151 A1) or WO 03/077007 A2, the describing in more detail by the relative rotation of the unit made by birefringent material to the birefringence effect redeeming.Have be designed to the last lens of cutting open made by birefringent material (calcium fluoride), with the Catadioptric projection objective of the hithermost last lens unit of image surface be that 722B is known from US 6,717.
The technical manual of the design of Fig. 1 is summarized in table 1.The row on the left side are listed plane of refraction, reflecting surface or the number of the face of appointment in addition, secondary series is listed the radius r [mm] of this face, the 3rd be listed between this face and the next face apart from d[mm], it is called as the parameter of optical unit " thickness ", the 4th lists and is used to make the material that optical unit adopts, and the 5th refractive index of listing the material that the manufacturing that is used for it adopts.The 6th lists available on the optics of optics, semidiameter [mm] clearly.On this table, the radius value r=0 that provides for plane with infinitely great radius.
Under the situation of this certain embodiments, 15 faces are faces of aspheric surface.Table 1A lists for these aspheric relevant data, and thus, the curved arrow of their surface number can utilize following formula to calculate as the function of height h:
P (h)=[((1/r) h 2(1-(1+K) (1/r) for)/(1+SQRT 2h 2)]+C1h 4+ C2h 6+ ...., wherein the reciprocal value of radius (1/r) is the surface of the being discussed curvature at surperficial top, and h is that thereon a point is from the distance of optical axis.Therefore curvedly vow that p (h) representative is along the z direction--promptly along optical axis--measurement, this distance from the top on the surface of being discussed.Constant K, C1, C2 or the like lists on table 1A.
Similarly, the technical manual of following embodiment is for the table 2 of Fig. 2,2A; For the table 3 of Fig. 3,3A; For the table 4 of Fig. 4,4A; With table 5, represent in a similar fashion among the 5A for Fig. 5.
According to the projection objective on Fig. 2 200, the last optical unit LOE on image surface has total shape of planar convex lens.Lens are divided into two optical unit LOE1 and LOE2 again, and they are cut apart interface S1 and contact with each other along the plane.Especially, has the positive curvature radius of entering surface and be thereafter that the quartz glass lens LOE1 on plane is bonded on (or two) planopaallel plate LOE2 who is made by sapphire.This produces the numerical value be not higher than NA possible in the quartz glass, but it has such advantage, and promptly the angle of propagation of light beam is reduced in last objection lens portion office, and there the aperture because the medium of high index of refraction but maximum.When considering that this is favourable when the reflection loss on the possible protective seam and scattered light effect at interface with on last end face, these scattered light effects are for those otherwise will be that very large propagation angle will constitute problem.Like this, Zui Da angle only takes place on the bonding surface between the quartz lens LOE1 and the first high index of refraction planopaallel plate LOE2.This bonding surface (wherein adjacent optical unit is by bonding and adhered to one another surface of contact) is protected to be avoided polluting and damaging, and available have the also responsive coating of environmental impact is designed.If two planopaallel plates are used for forming parallel plane high index of refraction element LOE2, then two planopaallel plates being made by sapphire can rotate relatively around optical axis, and the compensation S in the x and y direction and the birefringence effect of P polarization ideally actually, this is at first to need for making the semiconductor structure imaging.
Yet, because its lower refractive index, quartz lens LOE1 has following effect here, even--because its less concentration effect--is for the image-side numerical aperture of the projection objective of limited total length, need very large lens diameter, and in fact these diameters not so big yet.In second exemplary embodiment (Fig. 2), the aperture is NA=1.35, but lens diameter bigger compared with among first embodiment.Here, lens diameter has surpassed 143mm, therefore is actually 212 times of numerical aperture, and only reaches 200 times numerical aperture in first embodiment.Particularly, in the exemplary embodiment of Fig. 2, maximum half lens diameter under 143mm even greater than the catoptron semidiameter under about 136mm.
Diameter for the maximum lens unit that minimizes projection objective, and minimize birefringent effect simultaneously, in the alternative embodiment (projection objective 300) of the design example with NA=1.45, last lens unit LOE comprises the entering surface of thin sapphire lens LOE1 with positive refracting power, spherical curve and is bonded to appear outside the plane on the thin quartz glass plate LOE2 (exemplary embodiment 3 of Fig. 3).Provide the outer parallel plane quartz glass plate of appearing of object lens can take place then owing to exchanged after the damage that radiation load causes.Therefore bonding quartz plate also is used as tradable protective seam, and protection sapphire lens LOE1 avoids pollution and/or scratch or destruction.It is immersion fluid that embodiment 3 adapts to cyclohexane give, and it has and is used for and the similar refractive index (n=1.566) of the refractive index (n=1.560) of the fused quartz of the contacted plate of immersion fluid.
Under these situations, NA is limited by the refractive index of quartz glass.Yet, compare with design with last lens of making by pure quartz glass, in the end the result of the upstream of lens is less beam angles, so also be the lower sensitivity (to the susceptibility of fabrication tolerance) of the less diameter and the last lens unit of total object lens.In embodiment 3, maximum lens diameter is about 186 times of numerical aperture now under 135mm.
Certainly, the present invention also can be used for the object lens of low numerical aperture, so that reduce the diameter of former projection objective significantly.This advantageously influences the price of projection objective, because quantity of material can be reduced significantly.
The 4th exemplary embodiment (Fig. 4) shows the lithographic objective 400 be used for 193nm, it have by sapphire make but the last lens and the Yi Shui (n of monolithic H2O=1.43) as the submergence medium, NA=1.35 and operating distance are 1mm.Monolithic (parts, ameristic) top surface (entering surface) of sapphire lens LOE is aspheric surface, and in the zone of the zone of the largest beam diameter of aperture diaphragm AS in the 3rd object lens part ROP3 that is in the biconvex lens LMD with maximum gauge and the collected radiation between the image surface IP in the aft section of image surface refractive objective lens part ROP3.Maximum lens diameter is limited to 190 times less than numerical aperture.
By means of the high-index material of last at least lens unit, even the numerical aperture higher than NA=1.45 also is possible.
The 5th exemplary embodiment 500 (Fig. 5) be designed for NA=1.6 have a plane convex surface sapphire lens (n Sapphire=1.92) solid immersion (photoetching of contact object lens).Therefore, even also be feasible on principle up to the numerical aperture of NA>1.8.In this example, be 15.53mm at the external field radius of wafer side, and the fields inside radius is 5.5mm, that is to say that the size of rectangular field is 26 * 3mm.
Since have NA>0.52 the high aperture light beam in aperture at plane exit face place when when sapphire is transferred to air, standing total reflection, so must realize operating distance for solid immersion, so that the service wear ripple makes wafer exposure effectively less than wavelength.This can be achieved like this: wafer is placed in the end near the lens surface for example 100nm (≈ λ/2) is exposed consistently in a vacuum.
Yet, because the through-put power by evanescent field (evanescent field) is pressed index decreased with distance, the minor alteration of distance also will cause inhomogeneity surging, be favourable so wafer is contacted with last end face (exit face) direct mechanical of projection objective.In order to expose, wafer can be adhered on the last planar lens face (surface of contact CS), so that reach the Mechanical Contact between the exit face of projection objective and the interior coupling surface that is associated with substrate.The exposure method of substep scan pattern or splicing is preferred in this case, that is to say, the zone bigger than picture field is exposed in each step respectively, and reticle also correspondingly is adjusted so that aim at, rather than as former convention to the wafer adjustment.Because the imaging of having dwindled is adjusted master and can be used than adjusting the lower precision of wafer, this also is favourable.The follow-up level of the semiconductor structure of exposure area adjacent to each other (target area) or step of exposure subsequently thus by reticle laterally and axially-movable and rotation obtain good overlappingly, with the overlapping accuracy that is better than several nanometers semiconductor structure is exposed to the wafer of also defective applying thus.For example the alignment mark of master also aligns with the alignment mark that has exposed on wafer for this reason
Wafer takes out from last surface and preferably carries out in a vacuum.If desired, place a thin layer (film/membrane sheet) between wafer and last planar lens face, it can for example exchanged after each step of exposure.This diaphragm for example also can keep being engaged with on the wafer and help separating, and is used as the protective seam for last planar lens face especially.The latter can randomly be protected by thin protective layer in addition.
Under the situation of solid immersion, because the situation that imaging is disturbed, the fringe region at last lens face between exposure period can produce high-intensity standing wave.So, when wafer because how much bonding out of true once in a while ground when being placed on certain scope of several microns, for structure repeated exposure on wafer, can be compensated it by using master to adjust, being burnt on the last lens so that prevent systematic structure, is more favourable.
All exemplary embodiments discussed above are to have just in time two concave mirrors and the Catadioptric projection objective of two intermediate images just in time, and wherein all optical units are aimed at along folding straight line optical axis.The projection objective that is selected to illustrate the unified fundamental type of preferred variation of the present invention plan to help explanation some become substantially example and with different relevant technique effect and the advantages of change example of the present invention.Yet the illustrative of the lens unit of being made by high-index material (for example n 〉=1.6 or even n 〉=1.8) in the projection objective of the operation wavelength in being specifically used for deep UV (DUV) scope is used and is not limited to this projection objective.The present invention also be directed into pure refraction projection object lens.In these types, the last lens unit that approaches image surface most usually is a plano-convex lens, and it for example can be designed by each the rule of last optical unit LOE above-mentioned, that be used for first to the 5th embodiment.Some examples for example have a sequence number 10/931 the applicant, 051 (also seeing WO 03/075049 A), 10/931,062 (also seeing US 2004/0004757 A1), 10/379,809 (also seeing US 2004/0004757A1), in the U.S. Patent application or in WO 03/077036A, provide.The disclosure of these documents is being hereby incorporated by reference.
Similarly, the present invention may be embodied as the Catadioptric projection objective that only has a concave mirror, or is embodied as Catadioptric projection objective in a device that is different from accompanying drawing with two above concave mirrors or embodiment, that have two concave mirrors.In addition, use of the present invention can irrespectively be implemented with whether there is folding mirror in optical design.The example of reflected refraction system is in the U.S. Patent application of the applicant with sequence number 60/511,673,10/743,623,60/530,622,60/560,267 or describe in US2002/0012100.The disclosure of these documents is being hereby incorporated by reference.Other example shows in US 2003/0011755 A1 and relevant application.
Similarly, the present invention may be implemented as and not have projection objective intermediate image or that have the intermediate image of any proper number on request.
Table 1
Embodiment 1:NA=1.45, β=-0.25, λ=193.4nm
The surface Radius Thickness Material Refractive index Semidiameter
0 0.000000 37.647680 62.000
1 200.438805 20.912608 SIO2HL 1.56018811 83.110
2 747.538013 7.881173 83.845
3 317.250503 20.945704 SIO2HL 1.56018811 86.831
4 22587.222465 11.951766 86.988
5 -354.957551 49.505975 SIO2HL 1.56018811 87.016
6 -278.404969 31.885410 92.050
7 133.981210 32.856595 SIO2HL 1.56018811 92.150
8 186.155059 11.833855 85.480
9 260.034334 38.111988 SIO2HL 1.56018811 85.440
10 -248.127931 0.945803 84.087
11 97.319012 29.863172 SIO2HL 1.56018811 63.308
12 247.011352 15.182258 54.518
13 0.000000 13.667911 46.858
14 -118.535589 9.039902 SIO2HL 1.56018811 47.472
15 -136.528381 10.289540 49.929
16 -117.640924 9.240335 SIO2HL 1.56018811 50.901
17 -267.170322 7.604882 57.478
18 -147.424814 27.658175 SIO2HL 1.56018811 58.338
19 -83.904407 29.670597 63.295
20 -79.022234 16.329258 SIO2HL 1.56018811 66.670
21 -99.429984 38.001255 76.192
22 -111.093244 49.234984 SIO2HL 1.56018811 86.007
23 -144.921986 0.952550 108.817
24 -6366.151454 44.409555 SIO2HL 1.56018811 119.243
25 -217.880653 270.750636 120.802
26 -219.739583 -239.183412 REFL 145.235
27 184.636114 269.507816 REFL 128.436
28 197.874974 37.626342 SIO2HL 1.56018811 86.078
29 524.125561 15.614096 81.840
30 -406.239674 8.985971 SIO2HL 1.56018811 81.383
31 106.800601 32.709694 77.510
32 -1162.346319 30.365146 SIO2HL 1.56018811 78.287
33 -161.881438 8.348534 81.54
34 -166.445156 11.418724 SIO2HL 1.56018811 81.127
35 -1076.211334 42.927908 95.134
36 -546.503260 41.443273 SIO2HL 1.56018811 113.022
37 -173.835591 0.952741 119.110
38 -372.875307 32.537548 SIO2HL 1.56018811 128.490
39 -210.380863 1.042699 131.802
40 303.213120 50.564746 SIO2HL 1.56018811 145.286
41 5346.623071 0.921057 144.413
42 262.055999 33.924688 SIO2HL 1.56018811 133.743
43 733.81 3747 0.928913 130.461
44 163.353186 39.409378 SIO2HL 1.56018811 116.482
45 349.938998 0.920003 111.971
46 279.917107 28.062402 SIO2HL 1.56018811 109.138
47 11299.235097 0.896338 104.077
48 88.608734 39.730068 SIO2HL 1.56018811 73.896
49 114.264419 0.751321 56.000
50 65.720894 25.021454 SAPHIR 1.92674849 49.523
51 131.441788 25.021469 SAPHIR 1.92674849 39.659
52 0.000000 1.000000 HKIINDEX 1.55600000 18.066
53 0.000000 0.000000 Air 0.00000000 15.503
Table 1A
Aspheric constants
SRF 1 6 8 12 16
K 0 0 0 0 0
C1 -2.263569e-08 5.432610e-08 -7.143508e-09 2.619298e-07 -3.184960e-07
C2 -9.879901e-13 -7.797101e-12 1.564097e-11 -3.814641e-11 -3.142211e-11
C3 3.070713e-17 8.455873e-16 -1.599946e-15 1.148617e-14 -1.728296e-15
C4 -6.018627e-21 -6.875038e-20 3.060476e-19 -4.506119e-18 -1.249207e-18
C5 4.073174e-26 3.863488e-24 -2.788321e-23 -5.794434e-23 -9.678014e-24
C6 1.391778e-29 -1.112310e-28 1.126553e-27 4.244063e-26 -4.921692e-26
C7 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00
SRF 22 26 27 28 31
K 0 0 0 0 0
C1 2.863527e-08 8.694636e-09 -6.654566e-09 5.614883e-08 -1.288689e-07
C2 1.884154e-12 1.385871e-13 -1.686449e-13 1.450774e-12 -4.820574e-12
C3 1.636375e-17 1.727286e-18 -2.470942e-18 1.892047e-16 5.082977e-16
C4 1.888300e-20 4.461465e-23 -2.362157e-22 6.954696e-21 -1.375138e-19
C5 -2.021635e-24 -7.172318e-28 7.757389e-7 -1.108417e-24 1.555422e-23
C6 1.591959e-28 3.081240e-32 -3.330142e-31 2.459404e-28 -2.481857e-28
C7 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00
SRF 34 36 41 47 49
K 0 0 0 0 0
C1 -1.177998e-07 -2.187776e-08 -1.577571e-08 -8.244653e-09 2.024084e-07
C2 -5.683441e-12 -8.068584e-14 3.706857e-13 4.957466e-12 1.422789e-11
C3 -5.647064e-16 8.600815e-17 -1.492063e-17 -2.442972e-16 3.923209e-15
C4 -7.031797e-21 -2.071494e-20 -9.742126eI 6.741381e-21 4.845684e-19
C5 -1.902336e-24 1.290940e-24 6.498365e-26 2.034640e-25 -2.134986e-22
C6 2.891112e-29 -3.884318e-29 -9.630077e-31 -2.570056e-29 5.591977e-26
C7 0.000000e+00 0.000000e+00 0.000000e+00 9.579172e-34 0.000000e+00
Table 2
Embodiment 2 (b037b): NA=1.35, β=-0.25, λ=193.4nm
The surface Radius Thickness Material Refractive index Semidiameter
0 0.000000 37.647680 62.000
1 526.196808 49.977602 SIO2HL 1.56018811 75.944
2 -256.668548 1.120100 85.473
3 696.160336 28.649736 SIO2HL 1.56018811 90.668
4 -2056.955285 22.244610 92.750
5 -195.811665 49.974335 SIO2HL 1.56018811 92.870
6 -158.185918 9.821764 101.539
7 138.796255 49.218181 SIO2HL 1.56018811 90.394
8 301.060143 1.660319 80.597
9 161.646552 42.095627 SIO2HL 1.56018811 78.153
10 -406.812049 0.979493 70.852
11 100.020556 24.469422 SIO2HL 1.56018811 52.354
12 102.330592 10.088496 38.573
13 0.000000 10.406389 37.226
14 -157.109979 8.950512 SIO2HL 1.56018811 38.841
15 618.822068 8.847956 46.776
16 -561.300665 33.147649 SIO2HL 1.56018811 51.388
17 -73.150544 9.448760 56.377
18 -699.300574 8.926672 SIO2HL 1.56018811 57.781
19 -86.551998 8.003693 64.608
20 -78.306541 10.360105 SIO2HL 1.56018811 66.592
21 -117.142798 2.915635 75.827
22 -356.673528 46.693825 SIO2HL 1.56018811 86.465
23 -108.386760 266.538313 90.245
24 -177.092218 -236.552196 REFL 129.567
25 200.462621 288.213928 REFL 136.687
26 604.677438 50.022575 SIO2HL 1.56018811 82.440
27 125.234518 13.901039 73.274
28 257.421526 34.367199 SIO2HL 1.56018811 73.449
29 111.03495 29.307766 73.890
30 -848.480773 29.119950 SIO2HL 1.56018811 74.404
31 -194.073508 7.840952 80.032
32 -225.307336 46.053997 SIO2HL 1.56018811 81.668
33 -535.709449 0.941640 105.651
34 -1622.810467 46.410355 SIO2HL 1.56018811 108.373
35 -173.207717 0.932943 113.398
36 -236.921577 22.327373 SIO2HL 1.56018811 116.764
37 -261.220038 0.938270 124.709
38 364.988031 40.936258 SIO2HL 1.56018811 142.520
39 11406.698081 0.943482 142.679
40 379.203162 36.840265 SIO2HL 1.56018811 142.867
41 -33782.42006 0.921857 141.929
42 245.879991 49.886843 SIO2HL 1.56018811 134.831
43 -10061.581161 0.883850 132.020
44 145.995266 39.892414 SIO2HL 1.56018811 105.854
45 375.256079 0.817132 99.565
46 86.107554 37.429431 SIO2HL 1.56018811 73.276
47 215.234027 0.667291 63.094
48 52.718236 26.546970 SIO2HL 1.56018811 42.800
49 0.000000 16.594510 SAPHIR 1.92674849 42.800
50 0.000000 0.999826 H2O 1.43612686 42.800
51 0.000000 0.000000 Air 0.00000000 15.501
Table 2A
Aspheric constants
SRF 1 6 9 12 14
K 0 0 0 0 0
C1 -8.448852e-08 -4.108258e-09 -6.153759e-08 4.456016e-07 -6.305745e-07
C2 -4.761055e-12 -9.598657e-12 -1.480269e-11 1.857407e-11 -7.903687e-11
C3 -1.420861e-16 1.072661e-15 1.473191e-15 1.064538e-14 -2.534563e-14
C4 -8.023974e-20 -6.889975e-0 -3.255374e-19 -5.079476e-18 -3.735078e-18
C5 1.173437e-23 2.314066e-24 3.131675e-23 1.056992e-22 1.905659e-22
C6 -1.454073e-27 -3.793935e-29 -6.955428e-28 7.981996e-26 -3.500146e-26
C7 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00
SRF 20 24 25 26 29
K 0 0 0 0 0
C1 1.209336e-07 1.259532e-08 -4.077497e-09 1.111414e-07 -8.942189e-08
C2 1.869926e-11 3.424346e-13 -8.690596e-14 3.172584e-13 -1.116520e-13
C3 1.314270e-15 6.952906e-18 -1.505812e-18 3.429058e-19 4.168290e-16
C4 3.650689e-19 3.744203e-22 -8.583957e-23 -1.068048e-20 -2.231424e-19
C5 -5.603440e-23 -1.203108e-26 2.784182e-27 1.935865e-24 2.267328e-23
C6 9.844086e-27 6.714766e-31 -1.06660e-31 -5.318242e-29 -1.588914e-27
C7 0.000000e+00 0.00000e+00 0.000000e+00 0.000000e+00 0.000000e+00
SRF 32 34 39 45 47
K 0 0 0 0 0
C1 -9.549663e-08 -5.673614e-09 -1.220571e-08 -2.613273e-08 1.649072e-07
C2 -3.034519e-12 -5.774683e-14 4.574492e-13 4.882999e-12 -4.982295e-13
C3 1.985443e-16 -1.715933e-16 -3.026161e-17 -2.171852e-16 -2.462341e-16
C4 -1.403621e-20 5.949307e-21 8.480395e-22 8.220913e-21 6.329880e-19
C5 2.496197e-24 1.220843e-25 -5.629908e-27 2.183741e-25 -1.498580e-22
C6 -1.598958e-28 -2.178077e-29 -3.377722e-32 -2.816869e-29 1.552461e-26
C7 0.000000e+00 0.000000e+00 0.000000e+00 1.520501e-33 0.000000e+00
Table 3
Embodiment 3 (b037a): NA=1.45, β=-0.25, λ=193.4nm
The surface Radius Thickness Material Refractive index Semidiameter
0 0.000000 37.647680 62.000
1 178.098560 47.089109 SIO2HL 1.56018811 83.684
2 508.791874 0.982161 86.920
3 260.152118 29.610169 SIO2HL 1.56018811 89.203
4 -897.680969 14.988854 89.348
5 -224.555888 50.010854 SIO2HL 1.56018811 89.318
6 -167.290149 6.943751 94.603
7 185.350898 29.083481 SIO2HL 1.56018811 84.200
8 161.696842 4.567325 74.817
9 156.295087 29.687097 SIO2HL 1.56018811 74.801
10 -1628.579737 27.610587 72.999
11 116.709207 25.652669 SIO2HL 1.56018811 57.349
12 3359.816893 2.336800 52.702
13 0.000000 42.058143 50.890
14 -114.711496 34.899486 SIO2HL 1.56018811 53.065
15 -73.282662 4.817213 60.856
16 -72.166685 17.818288 SIO2HL 1.56018811 60.190
17 -80.823907 4.905081 66.269
18 -78.170209 34.642475 SIO2HL 1.56018811 65.802
19 -161.353349 3.907912 83.613
20 -250.115507 50.004289 SIO2HL 1.56018811 87.033
21 -130.504962 244.427626 94.956
22 -180.721067 -214.432541 REFL 135.011
23 179.125663 274.568868 REFL 126.490
24 337.886373 47.239794 SIO2HL 1.56018811 107.066
25 -899.516467 5.847365 104.221
26 -2346.009271 43.828445 SIO2HL 1.56018811 101.016
27 101.771490 35.484160 86.055
28 -4439.596410 23.703533 SIO2HL 1.56018811 86.263
29 -254.324560 5.801976 87.609
30 -445.540133 48.164461 SIO2HL 1.56018811 87.772
31 -735.213902 16.951226 100.097
32 -650.817086 49.961292 SIO2HL 1.56018811 102.416
33 -281.005458 31.479288 116.698
34 -649.019441 49.768062 SIO2HL 1.56018811 130.316
35 -215.856617 0.928162 134.641
36 312.849138 39.828764 SIO2HL 1.56018811 135.256
37 -1022.199791 0.857904 133.831
38 278.748013 42.635737 SIO2HL 1.56018811 128.369
39 -3295.326556 0.914469 126.650
40 128.656616 61.387113 SIO2HL 1.56018811 106.520
41 -2188.188515 0.730038 100.722
42 90.065507 18.596750 SIO2HL 1.56018811 69.706
43 93.775489 1.000000 60.097
44 73.203900 33.227474 SAPHIR 1.92674849 55.900
45 0.000000 11.657723 SIO2HL 1.56018811 55.900
46 0.000000 0.999913 HIINDEX 1.55600000 55.900
47 0.000000 0.000000 Air 0.00000000 15.520
Table 3A
Aspheric constants
SRF 1 6 8 12 14
K 0 0 0 0 0
C1 -3.797021e-08 4.091151e-08 9.284044e-09 1.793476e-07 -3.526789e-07
C2 -1.858357e-12 -7.880362e-12 2.927990e-11 -4.710051e-11 -5.029864e-11
C3 6.026920e-17 9.074630e-16 -2.187906e-15 2.197728e-15 -6.353989e-15
C4 -3.792813e-20 -7.153651e-20 3.131133e-19 -3.553387e-18 -2.243484e-18
C5 3.121506e-24 2.884237e-24 -3.422295e-23 -7.638265e-23 1.422334e-23
C6 -1.940311e-28 -4.358943e-29 2.472280e-27 2.576563e-26 -7.652798e-26
C7 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00
SRF 18 22 23 24 27
K 0 0 0 0 0
C1 4.805447e-08 1.366493e-08 -7.247654e-09 2.039086e-09 -2.335210e-07
C2 6.053101e-12 3.157722e-13 -1.844324e-13 4.079171e-12 -3.581428e-12
C3 1.864225e-16 4.418704e-18 -3.130608e-18 3.415807e-19 8.204976e-16
C4 1.774391e-19 3.842541e-22 -2.876782e-22 -3.143532e-21 -1.472132e-19
C5 -1.538124e-23 -1.422352e-26 1.047999e-26 -6.009771e-26 1.193755e-23
C6 1.486597e-27 5.625242e-31 -4.798652e-31 5.373759e-30 -5.012293e-28
C7 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00
SRF 30 32 37 41 43
K 0 0 0 0 0
C1 -9.015949e-08 -4.710517e-08 2.981775e-08 7.825942e-08 -1.254855e-07
C2 -5.963683e-12 1.502154e-12 -1.562632e-15 -5.678508e-12 4.044789e-11
C3 -2.709599e-17 -1.008729e-16 -1.924785e-17 9.897699e-16 5.935178e-15
C4 1.782520e-20 -2.037099e-20 1.470777e-21 -1.257950e-19 -7.518165e-19
C5 -1.313151e-25 1.244695e-24 -9.287054e-26 1.131690e-23 5.626054e-23
C6 1.114296e-28 -7.926554e-29 2.454712e-30 -6.106697e-28 5.101190e-26
C7 0.000000e+00 0.000000e+00 0.000000e+00 1.494562e-32 0.000000e+00
Table 4
Embodiment 4:NA=1.35, β=-0.25, λ=193.4nm
The surface Radius Thickness Material Refractive index Semidiameter
0 0.000000 37.647680 62.000
1 213.097095 21.139875 SIO2HL 1.56018811 81.073
2 980.962863 0.933467 81.638
3 312.309311 19.869666 SIO2HL 1.56018811 82.923
4 7050.227976 14.977212 82.853
5 -284.845054 46.899913 SIO2HL 1.56018811 82.842
6 -316.674517 31.820687 87.867
7 127.504953 32.199127 SIO2HL 1.56018811 90.842
8 177.687028 14.069304 84.748
9 233.816949 49.949045 SIO2HL 1.56018811 84.566
10 -272.601570 1.802731 81.010
11 92.974202 24.948435 SIO2HL 1.56018811 61.866
12 228.036841 31.795297 55.983
13 -128.436888 15.028089 SIO2HL 1.56018811 45.986
14 -208.039449 19.686225 50.292
15 -85.822730 9.039605 SIO2HL 1.56018811 51.590
16 -124.923386 5.248146 59.096
17 -134.255203 24.981296 SIO2HL 1.56018811 61.621
18 -866.028170 70.079618 66.114
19 -91.784845 49.926992 SIO2HL 1.56018811 78.125
20 -130.258172 3.354815 102.297
21 -819.889396 43.461173 SIO2HL 1.56018811 114.993
22 -193.549016 277.291798 117.690
23 -220.432400 -231.344649 REFL 147.536
24 175.171589 261.356424 REFL 120.087
25 222.618410 49.895981 SIO2HL 1.56018811 93.866
26 227.634130 10.722465 85.687
27 469.132386 43.799915 SIO2HL 1.56018811 85.491
28 112.693662 31.313114 76.622
29 12293.399547 31.702057 SIO2HL 1.56018811 77.313
30 -155.449641 4.962336 79.575
31 -219.506451 26.268152 SIO2HL 1.56018811 79.827
32 -1377.822971 32.354789 93.063
33 -519.892544 47.183977 SIO2HL 1.56018811 101.635
34 -163.140684 1.841108 110.786
35 -340.920966 26.977392 SIO2HL 1.56018811 116.967
36 -214.582539 2.006234 120.143
37 271.181444 53.143321 SIO2HL 1.56018811 127.047
38 -1118.441818 19.790952 125.887
39 0.000000 -14.609943 112.489
40 174.102740 52.205661 SIO2HL 1.56018811 107.954
41 -663.589997 3.836965 104.404
42 84.561977 46.625084 SIO2HL 1.56018811 71.481
43 95.046969 0.694913 51.033
44 64.492898 46.885676 SAPHIR 1.92674849 46.520
45 0.000000 1.000000 H2O 1.43612686 18.265
46 0.000000 0.000000 Air 0.00000000 15.515
Table 4A
Aspheric constants
SRF 1 6 8 12 15
K 0 0 0 0 0
C1 -7.766221e-09 3.921777e-08 -1.973978e-08 2.262385e-07 -2.849645e-07
C2 -1.414298e-12 -746692e-12 1.686856e-11 -3.111178e-11 -3.795087e-11
C3 2.026799e-16 9.877277e-16 -1.521195e-15 8.999889e-15 -4.195519e-15
C4 -9.311177e-21 -6.24165e-20 2.838141e-19 -4.631502e-18 -2.684695e-18
C5 8.98377e-26 3.68366e-24 -2.893390e-23 7.225241e-23 -2.249016e-23
C6 -5.139250e-30 -1.606542e-28 1.372152e-27 5.035383e-26 -5.606361e-26
C7 0.000000e+00 0.000000e+00 0.000000e+0 0.000000e+00 0.000000e+00
SRF 19 23 24 25 28
K 0 0 0 0 0
C1 2.306275e-08 9.197905e-09 -7.280789e-09 8.044076e-08 -1.035389e-08
C2 1.672430e-12 1.297990e-13 -2.062090e-13 6.845761e-13 5.752946e-14
C3 -3.451288e-18 1.447412e-18 -3.885785e-18 8.440855e-17 3.412577e-16
C4 3.656429e-20 4.002605e-23 -3.101616e-22 -8.233892e-21 -1.247784e-19
C5 -5.091821e-24 -7.044663e-28 1.113163e-26 1.115110e-24 5.556509e-24
C6 5.148418e-28 3.011922e-32 -6.186058e-31 -3.079026e-29 1.295943e-27
C7 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00
SRF 31 33 38 41 44
K 0 0 0 0 0
C1 -1.291718e-07 -4.530057e-08 -1.801990e-08 -2.682021e-08 -1.900216e-07
C2 -4.385607e-12 -2.081953e-13 6.277450e-13 7.361672e-12 -4.832504e-11
C3 -2.255698e-16 1.680387e-16 -5.256278e-17 -3.951877e-16 -1.233010e-14
C4 -2.117620e-21 -4.155797e-20 -4.688822e-21 1.434967e-20 7.440284e-19
C5 -1.322919e-24 3.040355e-24 4.497908e-25 -3.980440e-26 1.430823e-22
C6 1.074049e-28 -1.238033e-28 -9.348185e-30 -2.642973e-29 -3.924075e-25
C7 0.000000e+00 0.000000e+00 0.000000e+00 1.163864e-33 0.0000
Table 5
Embodiment 5:NA=1.6, β=-0.25, λ=193.4nm
The surface Radius Thickness Material Refractive index Semidiameter
0 0.000000 37.663108 62.000
1 192.084227 26.622297 SIO2V 1.56078570 87.833
2 1075.649716 0.946456 88.233
3 491.402040 19.101530 SIO2V 1.56078570 88.867
4 -934.209447 36.905290 88.935
5 125.340633 9.623977 SIO2V 1.56078570 90.013
6 122.019859 23.963817 87.312
7 252.185057 44.239148 SIO2V 1.56078570 87.669
8 -204.394078 0.923049 87.161
9 102.471834 52.8522020 SIO2V 1.56078570 67.768
10 254.533994 9.305878 48.073
11 0.000000 52.418616 46.820
12 -75.641562 68.872834 SIO2V 1.56078570 58.068
13 -124.953275 39.621161 93.864
14 -835.558655 54.318921 SIO2V 1.56078570 126.993
15 -178.850083 0.948020 130.230
16 2111.392648 22.857019 SIO2V 1.56078570 132.098
17 -901.583067 358.679202 132.071
18 -225.015829 -231.613549 REFL 160.876
19 168.185189 261.594819 REFL 120.144
20 -736.571530 23.114077 SIO2V 1.56078570 81.485
21 132.965130 36.406211 86.933
22 -512.908458 28.535664 SIO2V 1.56078570 87.621
23 -185.099986 6.615931 92.898
24 -544.628556 33.807132 SIO2V 1.56078570 99.839
25 -547.431224 19.995820 114.885
26 -359.224408 99.479683 SIO2V 1.56078570 119.014
27 -168.873687 12.916761 143.505
28 313.449462 92.758623 SIO2V 1.56078570 165.026
29 983.057723 1.167054 158.153
30 227.152511 48.817493 SIO2V 1.56078570 148.584
31 684.382976 0.981700 144.866
32 144.775480 60.829967 SIO2V 1.56078570 121.541
33 1285.387522 0.899534 116.276
34 99.002284 39.642869 SIO2V 1.56078570 84.155
35 243.117451 0.805490 74.674
36 65.952055 54.681070 SAPHIR 1.92674849 54.379
37 0.000000 0.000000 Air 0.00000000 15.530
Table 5A
Aspheric constants
SRF 4 5 10 14 18
K 0 0 0 0 0
C1 4.332466e-08 5.983847e-08 4.678448e-07 -5.502311e-09 9.581997e-09
C2 -4.251613e-12 -1.394334e-11 1.214772e-11 6.759433e-14 1.191548e-13
C3 8.548420e-16 1.246293e-15 1.462858e-14 -2.777895e-18 5.628084e-19
C4 -7.822847e-20 -2.065935e-19 -5.084805e-18 1.850960e-22 7.255139e-23
C5 3.463295e-24 1.861321e-23 4.192361e-22 -7.883399e-27 -1.691943e-27
C6 -7.495559e-29 -7.372680e-28 1.456331e-26 1.533878e-31 3.619858e-32
C7 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00
SRF 19 20 21 24 26
K 0 0 0 0 0
C1 -5.661490e-09 8.762490e-08 -3.207763e-08 -6.520443e-08 4.364974e-09
C2 -1.921628e-13 -1.093121e-11 -5.311243e-12 4.777722e-13 -1.522836e-12
C3 -7.055884e-19 1.359734e-15 6.816058e-16 -7.895875e-17 -6.656442e-18
C4 -6.935220e-22 -2.479964e-19 -2.253013e-19 1.733738e-20 -2.640069e-21
C5 3.152816e-26 2.421781e-23 2.354847e-23 -2.097861e-24 2.889539e-25
C6 -1.191863e-30 -1.346005e-27 -1.003551e-27 1.235456e-28 -1.101803e-29
C7 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00
SRF 29 33 35
K 0 0 0
C1 8.788855e-09 3.258556e-08 1.084860e-07
C2 -6.462954e-13 1.588293e-12 6.094001e-12
C3 -1.551858e-17 -1.752790e-16 1.646644e-16
C4 1.099566e-21 1.227022e-20 -9.287322e-20
C5 -1.930245e-26 -5.173475e-25 1.657126e-23
C6 1.160550e-31 1.295964e-29 -1.278529e-27
C7 0.000000e+00 -1.104258e-34 0.000000e+00

Claims (31)

1. one kind is used for the projection objective on the image surface that the projection objective that is suitable for the microlithographic projection exposure machine is provided at the pattern that provides on the object plane of projection objective is comprised:
For the radiation on the operation wavelength of projection objective is transparent a plurality of optical units;
Wherein at least one optical unit is the high index of refraction optical unit of being made by the high-index material with refractive index n 〉=1.6 on operation wavelength.
2. according to the projection objective of claim 1, wherein high-index material has refractive index n 〉=1.8 on operation wavelength.
3. according to the projection objective of claim 1 or 2, wherein high-index material is a sapphire.
4. according to the projection objective of claim 1 and 2, wherein high-index material is a germanium dioxide.
5. according to each projection objective of aforementioned claim, object side numerical aperture NA wherein ObjGreater than 0.3.
6. according to the projection objective of claim 5, wherein with | β | the object side numerical aperture NA that≤0.25 absolute minification combines Obj>0.36.
7. according to each projection objective of aforementioned claim, have the first high index of refraction optical unit and at least one second high index of refraction optical unit.
8. according to the projection objective of claim 7, wherein each of the first high index of refraction optical unit and the second high index of refraction optical unit is made by high-index material, this material presents the birefringence of the birefringent orientation of having stipulated each optical unit, wherein the first and second high index of refraction unit are differently installed with respect to birefringent orientation, so that birefringent effect to the small part that is caused by the high index of refraction optical unit is compensated.
9. according to each projection objective of aforementioned claim, wherein projection objective has a last optical unit that approaches image surface most, and wherein last optical unit to small part is made by the high-index material with refractive index n>1.6.
10. according to the projection objective of claim 9, wherein last optical unit is the monolithic plano-convex lens of being made by the high-index material with refractive index n>1.6.
11. projection objective according to claim 9, wherein last optical unit is by form along two optical units cutting apart the mutual optics contact of interface at least, and at least one optical unit that wherein forms last optical unit is made up of the high-index material with refractive index n>1.6.
12. according to the projection objective of claim 9, wherein last optical unit by the plano-convex lens unit of an entering surface of exit face with crooked entering surface and plane with form with the exit face planopaallel plate that this plano-convex lens unit optics contacts along the plane divisional plane.
13. according to the projection objective of claim 12, its convexity planar lens unit is made up of the high-index material with refractive index n>1.6, and wherein the exit face planopaallel plate is made up of fused quartz.
14. according to the projection objective of claim 12, wherein the plano-convex lens unit is made up of fused quartz and this exit face planopaallel plate is made up of the high-index material with refractive index n>1.6.
15. according to the projection objective of claim 11, wherein last optical unit is shaped as plano-convex lens, and divisional plane is bent so that two optical units that contact at the divisional plane place are the lens components with similar refracting power.
16. each projection objective according to aforementioned claim, wherein projection objective is designed to an immersion objective of revising with reference to aberration, so that filled greater than 1 submergence medium significantly by having refractive index at last optical unit and the image-side operating distance between the image surface.
17. according to the projection objective of claim 16, wherein projection objective adapts to immersion fluid, this immersion fluid has the refractive index greater than 1.4 when operation wavelength.
18. according to the projection objective of claim 17, wherein projection objective designed to be used the 193nm operation wavelength, and wherein immersion fluid is a cyclohexane.
19. each projection objective according to aforementioned claim 1 to 15, wherein projection objective is designed to have the solid immersion medium that are about or are lower than the limited image-side operating distance of operation wavelength, so that the evanescent field of going out from the image-side exit face of projection objective can be used in imaging.
20. according to each projection objective of aforementioned claim 1 to 15, wherein projection objective is designed to the solid immersion photoetching, wherein the image-side exit face of projection objective has Mechanical Contact with the coupling surface that the substrate that will be exposed is associated.
21. according to each projection objective of aforementioned claim, wherein image-side numerical aperture NA is greater than 1.3.
22., wherein approach most unthreaded hole face that image surface places and be placed between the zone of the zone of the beam diameter local maximum that approaches image surface most and the converging beam between the image surface according to each projection objective of aforementioned claim.
23. have image surface and a projection objective, and, has the converging beam of through this image surface, wherein unthreaded hole face or the system aperture image surface place distance of 10mm at least that is arranged at described lens from this projection objective from its lens farthest.
24. be used for the pattern that provides is imaged onto the on-chip microlithographic projection exposure method of the image surface that is arranged on projection objective on the mask of the object plane that is arranged in projection objective, wherein use according to each the microlithography projection objective at least in the aforementioned claim, and between the last lens of microlithography projection objective and the substrate that will be exposed, introduce immersion fluid.
25., wherein used the immersion fluid that on the operation wavelength of projection objective, has greater than 1.4 refractive index according to the method for claim 24.
26. according to the method for claim 25, wherein immersion fluid has the refractive index greater than 1.5 on operation wavelength.
27. be used for the pattern that provides is imaged onto the on-chip microlithographic projection exposure method of the image surface that is arranged on projection objective on the mask of the object plane that is arranged in projection objective, the last optical unit of wherein employed projection objective image-side is fitted or is pressed on the object that will be exposed, and comprises the step of following given sequence:
The substrate of placing projection objective relative to each other and will being exposed;
The exit face of projection objective and the coupling surface of substrate are contacted;
Come alignment mask with respect to projection objective, so that the area of the pattern of wanting in the mask is imaged at the target area of a substrate that contacts with the exit face of projection objective.
28., wherein a plurality of target areas arranged side by side on the substrate are repeated described each step according to the method for claim 27.
29., wherein thin transparent membrane is placed between the exit face of the substrate that will be exposed and projection objective according to the method for claim 27 or 28.
30., wherein use microlithography projection objective according to one of claim 1 to 23 according to each method of claim 24 to 29.
31. be used for the pattern that provides is imaged onto the on-chip microlithographic projection exposure method of the image surface that is arranged on projection objective on the mask of the object plane that is arranged in projection objective, wherein use microlithography projection objective, and between the last lens of microlithography projection objective and the substrate that will be exposed, introduce immersion fluid, and be immersion fluid wherein with cyclohexane give.
CN 200480037372 2003-12-15 2004-12-10 Projection objective having a high aperture and a planar end surface Pending CN1894632A (en)

Applications Claiming Priority (13)

Application Number Priority Date Filing Date Title
US10/734,623 US6995930B2 (en) 1999-12-29 2003-12-15 Catadioptric projection objective with geometric beam splitting
US10/734,623 2003-12-15
US60/530,623 2003-12-19
US60/530,978 2003-12-22
US60/536,248 2004-01-14
US60/544,967 2004-02-13
US60/568,006 2004-05-04
US60/587,504 2004-07-14
US60/591,775 2004-07-27
US60/592,208 2004-07-29
US60/612,823 2004-09-24
US60/617,674 2004-10-13
DE102004051730.4 2004-10-22

Publications (1)

Publication Number Publication Date
CN1894632A true CN1894632A (en) 2007-01-10

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ID=37598264

Family Applications (1)

Application Number Title Priority Date Filing Date
CN 200480037372 Pending CN1894632A (en) 2003-12-15 2004-12-10 Projection objective having a high aperture and a planar end surface

Country Status (1)

Country Link
CN (1) CN1894632A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103353669A (en) * 2013-07-30 2013-10-16 中国科学院光电技术研究所 High-numerical aperture immersion projection objective lens
CN103376539A (en) * 2012-04-26 2013-10-30 上海微电子装备有限公司 Refraction and reflection type projection objective

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103376539A (en) * 2012-04-26 2013-10-30 上海微电子装备有限公司 Refraction and reflection type projection objective
CN103376539B (en) * 2012-04-26 2016-02-03 上海微电子装备有限公司 A kind of refraction-reflection projection objective
CN103353669A (en) * 2013-07-30 2013-10-16 中国科学院光电技术研究所 High-numerical aperture immersion projection objective lens
CN103353669B (en) * 2013-07-30 2015-07-15 中国科学院光电技术研究所 High-numerical aperture immersion projection objective lens

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Application publication date: 20070110