BACKGROUND OF THE INVENTION Field of the Invention The present invention relates generally to the field of optical imaging and more particularly to catadioptric optical systems used for microscopic imaging, inspection, and lithography applications.

Description of the Related Art Many optical and electronic systems exist to inspect surface features for defects such as those on a partially fabricated integrated circuit or a photomask.

Defects may take the form of particles randomly localized on the surface, scratches, process variations, and so forth. Such techniques and devices are well known in the art and are embodied in various commercial products such as those available from KLA-Tencor Corporation of San Jose, California.

Specialized optical systems are required in inspection devices to enable imaging of defects found on semiconductor wafers and photomasks. Improved performance for such systems may be realized using specially designed components that facilitate beneficial inspection parameters, such as high numerical apertures. The numerical aperture of an objective represents the objective's ability to collect light and resolve fine specimen detail at a fixed object distance. Numerical aperture is measured as the sine of the vertex angle of the largest cone of meridional rays that can enter or leave the optical system or element, multiplied by the refractive index of the medium in which the vertex of

the cone is located. A large numerical aperture provides distinct advantages during inspection, not the least of which is an ability to resolve smaller features of the specimen. Also, high NAs collect a larger scattering angle, thereby tending to improve performance in darkfield environments over systems having relatively low NAs. Two patents that disclose high numerical aperture (NA) catadioptric systems are U. S. Patent 5,717, 518 to Shafer et al. and U. S. Patent 6, 4839638 to Shafer et al. A representative illustration of a catadioptric design 100 in accordance with the teachings of the'518 patent is presented in FIG. 1, which is similar to FIG. 1 of the'518 patent. A representative illustration of a catadioptric design 200 in accordance with the teachings of the'638 patent is presented in FIG. 2, which has similarities to FIG. 4 of the'638 patent.

U. S. Patent 5,717, 518 to Shafer et al. discloses an imaging design capable of high NA, ultra broadband UV imaging. The high NA (up to approximately 0.9) system can be used for broadband bright field and multiple wavelength dark- field imaging. Certain issues exist with designs similar to that presented in FIG.

1. First, the field lens group may need to be physically located within a central hole in the large curved catadioptric element, which can make manufacturing very difficult and extremely expensive. Second, the field lens elements in such a design may require at least one glued interface. In the presence of wavelengths less then 365nm, reliable glues that can withstand light intensity levels at an internal focus are generally unavailable. Third, the lens elements in such a design may be located very close to a field plane, thereby requiring a high degree of, or nearly perfect, surface quality and bulk material quality to prevent image degradation. Fourth, element diameters are typically larger than a standard microscope objective, especially for the catadioptric group. Large diameter elements frequently make integration into an inspection system difficult and can increase manufacturing costs.

The design of FIG. 2 is generally capable of high NA, ultra broadband W imaging. The design is a high NA (up to approximately 0. 9) imaging system that can be used for broadband bright field and multiple wavelength dark-field imaging and can use a varifocal tube lens to provide a large range of magnifications. The FIG. 2 design introduces very tight tolerances in the field lens group, due in part to increased on-axis spherical aberration produced by the catadioptric group. This on-axis spherical aberration must be corrected by the following refractive lens elements. The design of FIG. 2 is relatively large, thereby generally requiring complicated optomechanical mounting of elements, especially in the catadioptric group.

Other optical arrangements have been developed to perform specimen inspection, but each arrangement tends to have certain specific drawbacks and limitations. Generally, in a high precision inspection environment, an objective with a short central wavelength provides advantages over those with long central wavelengths. Shorter wavelengths can enable higher optical resolution and improved defect detection, and can facilitate improved defect isolation on upper layers of multi-layer specimens, such as semiconductor wafers. Shorter wavelengths can provide improved defect characterization. An objective that can cover as large a wavelength range as possible may also be desirable, particularly when using an arc lamp as an illumination source. An all refractive objective design is difficult in this wavelength range because few glass materials having high transmission are effective for chromatic correction. A small bandwidth may not be desirable for inspection applications due to limitation of available light power and increased interference from thin films on the surface being inspected.

A large field size can provide distinct advantages during inspection. One advantage is an ability to scan a larger area of the specimen in a given period of time, thereby increasing throughput, measured as the ability to scan a large area over a small period of time. A relatively large field size in a typical design in this

type of environment can be approximately or greater than 0.2 mm using an imaging magnification of 200x to support a sensor with an 40mm diagonal. Small objectives are also desirable, as small objectives can be used in combination with standard microscope objectives and fit in standard microscope turrets. The standard objective flange to object length is 45mm, while certain objectives employ lens diameters greater than 100mm having length of over 100 mm. Other smaller catadioptric objectives have been produced, but still typically have lens diameters in excess of 60 mm and length over 60mm. Certain of these smaller objectives have NAs limited to 0.75 and field sizes limited to 0. 12mm with a bandwidth less than 10nu. Such designs typically use a Schwartzchild approach with lenses added within the catadioptric group in an effort to improve performance. Working distances are typically greater than 8 mm. This design approach can somewhat reduce the objective diameter, at the cost of increasing central obscuration, significantly degrading objective performance.

An objective having low intrinsic aberrations is also desirable, as is an objective that is largely self-corrected for both monochromatic and chromatic aberrations. A self corrected objective will have looser alignment tolerances with other self corrected imaging optics. An objective with loose manufacturing tolerances, such as lens centering tolerances, may be particularly beneficial.

Further, reducing incidence angles on lens surfaces can have a large effect on optical coating performance and manufacturing. In general, lower angles of incidence on lens surfaces also produce looser manufacturing tolerances.

It would be beneficial to provide a system overcoming these drawbacks present in previously known systems and provide an optical inspection system design having improved functionality over devices exhibiting those negative aspects described herein.

SUMMARY OF THE INVENTION According to a first aspect of the present design, there is provided an objective employed for use with light energy having a wavelength in the range of approximately 285 to 320 nanometers. The objective comprises a focusing lens group comprising at least one focusing lens configured to receive the light energy, a field lens oriented to receive focused light energy from the focusing lens group and provide intermediate light energy, and a Mangin mirror arrangement positioned to receive the intermediate light energy from the field lens and form controlled light energy. A ratio of lens diameter for a largest element of all focusing lenses, the field lens, and the Mangin mirror arrangement to field size is less than 100 to 1.

According to a second aspect of the present design, there is provided an objective employed for use with light energy having a wavelength in the range of approximately 157 nanometers through the infrared light range. The objective comprises a focusing lens group configured to receive the light energy and comprising at least one focusing lens, at least one field lens oriented to receive focused light energy from the focusing lens group and provide intermediate light energy, and a Mangin minor arrangement positioned to receive the intermediate light energy from the field lens and form controlled light energy. The Mangin mirror arrangement imparts controlled light energy to a specimen with a numerical aperture in excess of 0.65, wherein each lens employed in the objective and each element in the Mangin mirror arrangement has diameter less than 100 millimeters.

According to a third aspect of the present design, there is provided an objective constructed of a single glass material for use with light energy having a wavelength in the range of approximately 157 nanometers through the infrared light range. The objective comprises at least one focusing lens having diameter less than approximately 100 millimeters receiving the light energy and

transmitting focused light energy, at least one field lens having diameter less than approximately 100 millimeters, receiving the focused light energy and transmitting intermediate light energy, and at least one Mangin mirror element having diameter less than 100 millimeters receiving the intermediate light energy and providing controlled light energy to a specimen.

According to a fourth aspect of the present design, there is provided a system for imaging a specimen using light energy in the range of 157 nanometers through the infrared light range. The system comprises a plurality of lenses having diameter of less than approximately 25 millimeters receiving the light energy and providing intermediate light energy, and a Mangin mirror arrangement receiving the intermediate light energy and providing controlled light energy to the specimen.

According to a fifth aspect of the present design, there is provided a catadioptric objective comprising a catadioptric group comprising at least one element configured to receive light energy from a specimen and providing reflected light energy forming reflected light energy, a field lens group comprising at least one field lens receiving the reflected light energy and transmitting resultant light energy, and a focusing lens group comprising at least one focusing lens receiving resultant light energy and transmitting focused resultant light energy, wherein an imaging numerical aperture for the objective is at least 0.65, the objective having a maximum lens diameter for all lenses employed and a field size, and wherein the ratio of maximum lens diameter to field size is less than 100 to 1.

According to a sixth aspect of the present design, there is provided a method of imaging a specimen. The method comprises focusing received light energy using a focusing lens group, receiving focused light energy and providing intermediate light energy using a field lens group, and receiving intermediate light energy and forming controlled light energy using a Mangin mirror arrangement.

A field size is formed using the focusing lens group, the field lens group, and the Mangin mirror arrangement, and a ratio of a largest element in the focusing lens group, field lens group, and Mangin mirror arrangement to field size is less than 100 to 1.

According to a seventh aspect of the present design, there is provided an objective comprising means for focusing received light energy using a focusing lens group, means for receiving focused light energy and providing intermediate light energy using a field lens group, and means for receiving intermediate light energy and forming controlled light energy using a Mangin mirror arrangement.

A field size is formed using the focusing lens group, the field lens group, and the Mangin mirror arrangement, and a ratio of a largest element in the focusing lens group, field lens group, and Mangin mirror arrangement to field size is less than 100 to 1.

According to an eighth aspect of the present design, there is provided an objective employed for use with light energy having a wavelength in the range of approximately 157 nanometers through the infrared light range. The objective comprises focusing means for receiving the light energy and providing focused light energy, field lensing means for receiving focused light energy from the focusing means and providing intermediate light energy, and mirror means for receiving the intermediate light energy from the field lensing means and forming controlled light energy, the mirror means imparting the controlled light energy to a specimen with a numerical aperture in excess of 0.65, wherein each lens employed in the objective and each element in the mirror means has diameter less than 100 millimeters.

These and other objects and advantages of the present invention will become apparent to those skilled in the art from the following detailed description of the invention and the accompanying drawings.

DESCRIPTION OF THE DRAWINGS FIG. 1 illustrates an aspect of the catadioptric objective design similar to that presented in FIG. 1 of U. S. Patent 5,717, 518; FIG. 2 is an aspect of the catadioptric objective design similar to that presented in FIG. 4 of U. S. Patent 6, 483, 638 ; FIG. 3 presents a reduced size catadioptric objective with a high NA in accordance with the present invention; FIG. 4 is a size comparison between the objective of the design presented in FIG. 2, the reduced size catadioptric objective of FIG. 3, and a standard microscope objective; FIG. 5A is a graph of decenter sensitivity for the objective design of FIG.

3; FIG. 5B presents a sensitivity comparison between the design of FIG. 3, a UV refractive objective corrected from 365-436nm, and a catadioptric objective based on the design of FIG. 2; FIG. 6 is an alternate aspect of the reduced size catadioptric objective in accordance with the present invention; FIG. 7A illustrates a tube lens arrangement in accordance with the present invention; FIG 7B illustrates an objective and tube lens corrected from 266-405nm with a 0. 4mm diameter field; FIG. 7C illustrates an objective design with a lmm field size and diameter of approximately 58mm ;

FIG. 8 is a design able to perform in the presence of wavelengths from approximately 311-315 nm, having approximately 26 mm diameter, a field size of approximately. 28 mm, and NA of approximately 0. 90 ; FIG. 9 is an approximately 0. 28 mm field design having approximately 26 mm diameter, a wavelength of between approximately 297 and 313 nm, and NA of approximately 0.90 ; FIG. 10 is an approximately 0.4 mm field design having approximately 26 mm diameter, a wavelength of between approximately 297 and 313 nm, and NA of approximately 0.90 ; FIG. 11 illustrates a broad band design having approximately 26 mm diameter, a wavelength of between approximately 266 and 313 nm, field size of approximately. 28 mm, and NA of approximately 0.90 ; and FIG. 12 is a graph comparing relative bandwidth versus the maximum lens element diameter of certain designs, including the current design; and FIG. 13 is a graph comparing field size versus the maximum lens element diameter of certain designs, including the present design.

DETAILED DESCRIPTION OF THE INVENTION According to the present invention9 there is provided a catadioptric objective corrected over a wavelength range from 285-320nm using a single glass material, or in certain circumstances, more than one glass material to improve performance. One aspect of the objective design is shown in FIG. 3. The catadioptric objective as shown in FIG. 3 is optimized for broad-band imaging in the UV spectral region, namely approximately 0.285 to 0.320 micron wavelengths. The objective provides relatively high numerical apertures and large object fields. The inventive design presented uses the Schupmann principle in combination with an Offner field lens to correct for axial color and first order lateral color. As shown in the aspect presented in FIG. 3, the field lens group 305 is slightly displaced from the intermediate image 306 to obtain enhanced performance.

From FIG. 3, the catadioptric group 301 or Mangin mirror arrangement includes a Mangin mirror element 302. Mangin mirror element 302 is a reflectively coated lens element. The catadioptric group 301 also includes and a concave spherical reflector 303, also a reflectively coated lens element. Both elements in the catadioptric group 301 have central optical apertures where reflective material is absent. This allows light to pass from the object or specimen 300 (not shown) through Mangin mirror element 302, reflect from the second or inner surface of concave spherical reflector 303, onto the reflective surface 320 of Mangin mirror element 302, and through concave spherical reflector 303 to form an intermediate image 306 between concave spherical reflector 303 and field lens group 304. The field lens group 304 may comprise one or more lenses, and in the aspect shown in FIG. 3, one field lens is employed in the field lens group 304.

The focusing lens group 307 uses multiple lens elements, in the aspect shown six lens elements 308, 309,310, 3119 312, and 313. All lenses in the

focusing lens group 307 may be formed from a single type of material to collect the light from the field lens group 304 and the intermediate image 306.

The lens prescription for the aspect of the invention illustrated in FIG. 3 is presented in Table 1.

Table 1. Prescription for lenses for the design of FIG. 3 Surface Number Radius Thickness Glass Diameter OBJ Infinity Infinity 0 1 Infinity 15.50165 9. 39467 STO Infinity-15. 50165 8 3 53. 51878 2 Fused Silica 9. 376161 4-18. 17343 0. 976177 9. 234857 5 10.48757 1.249953 Fused Silica 8. 151456 6 5. 891816 3. 328088 7. 199539 7 -5. 254784 5. 105439 Fused Silica 7. 084075 8-8. 860388 0. 5 9. 430437 9 12.82516 2 Fused Silica 9. 711337 10 61. 04848 0. 5 9. 468601 11 8.892555 1.75 Fused Silica 9. 125279 12 15. 75614 2. 126452 8. 563035 13 7.216376 2 Fused Silica 7. 4431 14 21. 90145 5. 382485 6. 702302 15 2. 321495 1. 3 Fused Silica 2. 530266 16 13. 47255 0. 669203 1. 651874 17 0. 498865 0. 7 18 17. 99728 3.170995 Fused Silica 25 19 13. 41607 6. 08537 21 20 94145. 220004Fused Silica20. 5 21-78-5. 220004MIRROR'205 22 972. 9414-6. 08537 20. 5 23 13. 41607-3. 170995 Fused Silica 21 '2417. 997283. 170995MIRROR'25 25 13. 41607 6. 08537 21 26 972. 9414 5. 220004 Fused Silica 20. 5 27-78 0. 3 20. 5 IMA Infinity 0. 410191

As may be appreciated by one skilled in the art, the numbers in the leftmost column of Table 1 represent the surface number counting surfaces from the left of FIG. 3. For example, the left surface of lens 308 in the orientation presented in FIG. 3 (surface 3 in Table 1) has a radius of curvature of 53.51878 mm, a thickness of 2 mm, and the rightmost surface (surface 4) has a radius of curvature of-18. 17343 mm, and is 0.976177 mm from the next surface. The material used is fused silica, and the diameter of the left surface is 9.376161 mm and of the right surface is 9.234857 mm.

In the design presented in FIG. 3, the numerical aperture may approach or even exceed approximately 0.90. The design presented herein, including the aspect illustrated in FIG. 3, provides a maximum numerical aperture in all cases in excess of 0.65.

From FIG. 3, the focusing lens group 307 has the ability to receive light energy and transmit focused light energy. The field lens group 304 has the ability to receive the focused light energy and provide intermediate light energy, and form intermediate image 306. The catadioptric group or Mangin mirror

arrangement 301 receives the intermediate energy and provides controlled light energy to the specimen. Alternately, the reflected path originates at the specimen, and light reflected from the specimen is received by the catadioptric group or Mangin mirror arrangement 301 and forms and transmits reflected light energy.

The field lens group 304 receives the reflected light energy and transmitting resultant light energy, and the focusing lens group receives resultant light energy and transmits focused resultant light energy.

The design presented in FIG. 3 and Table 1 thus uses a single glass material, fused silica. Other materials may be employed, but it is noted that fused silica or any material used within the design may require low absorption over a wide range of wavelengths from 190 nm through the infrared wavelength. Use of fused silica can enable the design to be re-optimized for any center wavelength in this wavelength range. For example, the design can be optimized for use with lasers at 193,198. 5,213, 244,248, 257,266, 308,325, 351,355, or 364nm. The design can also be optimally employed to cover lamp spectral bands from 192- 194,210-216, 230-254, 285-320, and 365-546mon. In addition, if calcium fluoride is employed as the glass or lens material, the design can be employed with an excimer laser at 157 nm or excimer lamps at 157 or 177nm. Re-optimization requires tuning or altering components within the abilities of those skilled in the art. Calcium fluoride lenses may also be employed in the field lens group to increase the bandwidth of the objective, a modification discussed generally in U. S. Patent 5,717, 518.

As noted in FIG. 3, the objective has a diameter of 26 millimeters, which is significantly smaller than objectives previously employed in this wavelength range. The small size of this objective is particularly beneficial in view of the performance characteristics of the objective. The objective can be mounted in a standard microscope turret with a 45mm flange-to-object separation. The objective supports a numerical aperture of approximately 0.90, a field size of

approximately 0. 4mm, has a corrected bandwidth from approximately 285- 313nan, and a polychromatic wavefront error of less than approximately 0. 038 waves. A size comparison between the objective of the design presented in FIG.

2, the design of FIG. 3, and a standard microscope objective is shown in FIG. 4..

As is true with any optical design, certain tradeoffs may be made to improve performance characteristics depending on the desired application of the objective or optical design. It is possible, for example, to sacrifice bandwidth, field size, numerical aperture, and/or objective size to enhance one of the aforementioned performance characteristics, depending on the application. For example, optimizing for lower or higher NAs is possible. Reducing the NA can reduce the manufacturing tolerance and the outer diameter of the objective.

Lower NA designs can provide larger field sizes and larger bandwidths. Lower NA designs with the same performance and less optical elements are also possible. Optimizing for higher NAs is also possible. Optimizing the design for higher NAs would generally limit the field size or bandwidth and may require slightly increased diameter objective elements.

The design of FIG. 3 has a field size of 0.4mm in diameter. Such a relatively large field size can support a large high speed sensor. For example, using an imaging magnification of 200x, a sensor having an 80mm diagonal can be supported. The design of FIG. 3 can also be extended to larger field sizes by allowing larger lens diameters and re-optimizing the elements, again a task within the range of those skilled in the art.

The design of FIG. 3 has a relatively low intrinsic polychromatic wavefront aberration over the design bandwidth from approximately 285-320nm.

The low wavefront aberration provides increased manufacturing headroom, or ease of manufacture, while enabling relatively high performance of the manufactured objective. The design of FIG. 3 provides good performance over narrow bands from approximately 266 to 365nm if the objective is focused,

again a task that may be readily performed by one of ordinary skill in the art. Use of the objective of FIG. 3 in this narrow band range allows use of lasers or narrow lamp spectra, such as the 365run line of lasers. The design is also self corrected.

Self corrected in this context means that the objective does not require any additional optical components to correct aberrations in order to achieve the design specifications. The ability to self-correct tends to simplify optical testing metrology and optical alignment to other self corrected imaging optics. Further correction of residual aberrations using additional imaging optics is also possible.

Further aberration correction can increase optical specifications such as bandwidth or field size.

One advantage of the present design is relatively loose manufacturing tolerances. Specifically, the decenter tolerances of individual lenses are relatively loose. Having loose decenter tolerances for individual lens elements tends to simplify the manufacturing requirements of the system. Any lens decenters encounterd during manufacturing may cause on-axis coma, a phenomenon that can be difficult to compensate without introducing other residual aberrations.

Using the present design, it is possible to reduce the decenter sensitivity of the lens and mirror elements by carefully balancing the aberrations within the catadioptric group 301 and focusing lens group 307. Total aberrations of the catadioptric group may be optimized using the design of FIG. 3 to balance the compensation required by the field lens group 304 and focusing lens group 307.

FIG. 5A shows the decenter sensitivity for the objective. A 10 micron decenter, without using any compensators, introduces less than approximately 0.2 waves of aberration in all elements except lens 302. A 10 micron decenter without compensators introduces approximately 0.29 waves of aberration. In the design presented in FIG. 3, average tolerance is approximately 0.13 waves of error at approximately 313nm. Further balancing the tolerances on the elements in the catadioptric group 301 is also possible.

The decenter tolerances also scale with the wavelength being used. This is because the optical path errors introduced for small decenters are not a strong function of wavelength. For example, if a 10 micron decenter introduces 0. 2 waves of aberration at a 266nm wavelength, this is equivalent to a 0.0532 micron optical path error. The system operating at 365nm would only introduce 0.15 waves of aberration for the same decenter. This would have the same 0.0532 micron optical path error.

These tolerances tend to be looser than other catadioptric designs in similar environments, and tend to be looser than most standard refractive objective designs. FIG. 5B presents a sensitivity comparison between the design of FIG. 3, a UV refractive objective corrected from 365-436nm, and a catadioptric objective based on the design shown in FIG. 2. Generally, in the plots of FIG.

5B, a value lower on the vertical scale indicates a more desirable design.

Wavefront error is plotted for a 10 micron decenter for each element without compensation. Average sensitivity is less than the refractive objective and much less than the sensitivity of the catadioptric objective design similar to that from the design of FIG. 2.

This design also has very loose tolerances on the index of the glass material. This is largely because the design is of a single material and does not rely on the index difference of two different glass materials to compensate for chromatic aberrations. This also makes the design very insensitive to temperature changes. Standard designs use multiple glass materials with different index profiles for color correction. The index profile for each material changes differently with temperature. This changes the chromatic correction for temperatures other than the design temperature and reduces the performance.

The objective design presented herein can support various modes of illumination and imaging. Modes supported can include bright field and a variety of dark field illumination and imaging modes. Other modes such as confocal,

differential interference contrast, polarization contrast may also be supported using the present design.

Bright field mode is commonly used in microscope systems. The advantage of bright field illumination is the clarity of the image produced. Using bright field illumination with an objective such as that presented herein provides a relatively accurate representation of object feature size multiplied by the magnification of the optical system. The objective and optical components presented herein can be readily used with image comparison and processing algorithms for computerized object detection and classification. Brightfield mode typically uses a broad band incoherent light source, but it may be possible to use laser illumination sources using slightly modified illumination system components employing the design presented herein.

The confocal mode has been used for optical sectioning to resolve height differences of object features. Most imaging modes have difficulty detecting changes in the height of features. The confocal mode forms separate images of object features at each height of interest. Comparison of the images then shows the relative heights of different features. Confocal mode may be employed using the design presented herein.

Dark field mode has been used to detect features on objects. The advantage of the dark field mode is that flat specular areas scatter very little light toward the detector, resulting in a dark image. Surface features or objects protruding above the object tend to scatter light toward the detector. Thus, in inspecting objects like semiconductor wafers, dark field imaging produces an image of features, particles, or other irregularities on a dark background. The present design may be employed with dark field mode illumination. Dark field mode provides a large resultant signal upon striking small features that scatter light. This large resultant signal allows larger pixels to be employed for a given feature size, permitting faster object

inspections. Fourier filtering can also be used to minimize the repeating pattern signal and enhance the defect signal to noise ratio during dark field inspection.

Many different dark field modes exist, each including a specific illumination and collection scheme. Illumination and collection schemes can be chosen such that the scattered and diffracted light collected from the object provides an acceptable signal-to-noise ratio. Certain optical systems use different dark field imaging modes including ring dark field, laser directional dark field, double dark field, and central dark ground. Each of these dark field imaging modes may be employed in the present design.

An alternate aspect of the present design presents an objective with increased bandwidth. This aspect of the design is presented in FIG. 6. The main difference between the design of FIG. 6 and that of FIG. 3 is the tradeoff between bandwidth and field size. The objective of the design of FIG. 6 is corrected over a broader bandwidth from 266 to 320nm but has a relatively smaller field, approximately 0. 28mm, as compared with the 0.4mm of the design of FIG. 3.

The design of FIG. 6 maintains the high approximately 0.90 numerical aperture.

The worst case polychromatic wavefront error for the FIG. 6 design is approximately 0.036 waves.

From FIG. 6, the catadioptric group 601 includes a Mangin mirror element 602, which is a reflectively coated lens element, and a concave spherical reflector 603, which is also a reflectively coated lens element. Both Mangin mirror element 602 and concave spherical reflector 603 have central optical apertures where reflective material is absent. The absence of reflective material, in the center of the components shown, allows light to pass from the object or specimen 600 (not shown) through Mangin mirror element 602, reflect from the second surface of concave spherical reflector 603 onto the Mangin mirror element 602, and transmit through concave spherical reflector 603 to form an intermediate

image 620 between concave spherical reflector 603 and field lens group 604, comprising a single field lens 615 in this aspect of the design.

The focusing lens group 605 employs multiple lens elements, in this aspect the six lens elements 606,607, 608, 609, 610, and 611, which may all be formed from a single type of material. The focusing lens group 605 collects light from the field lens group 604, including the intermediate image 620.

The design presented in FIG. 6 has the advantages and flexibility described with respect to the design of FIG. 3. The lens prescription for this embodiment is shown in Table 2.

Table 2. Prescription for lenses for the design of FIG. 6 Surf Radius Thickness Glass Diameter OBJ Infinity Infinity 0 1 Infinity 16. 20723 9. 020484 STO Infinity -16.20723 3 64. 63011 2 FUSED SILICA 9. 010584 4-19. 00905 1.675169 8.894847 5 10. 3536 1. 249991 FUSED SILICA 7. 776084 6 5. 91317 3. 249904 6. 942948 7-5. 240171 5. 243182 FUSED SILICA 6. 855225 8-9. 11876 0.5 9.288367 9 16. 20784 2 FUSED SILICA 9. 638653 10 Infinity 0.5 9. 499901 11 8. 951438 3. 573584 FUSED SILICA 9. 210718 12 12. 83071 0. 5 7. 808034 13 7. 107306 2 FUSED SILICA 7. 502914 14 29. 37779 5.583862 6.837774 15 252897T3FUSED SILICA2. 391106 16 86360. 6681641. 486574 17 Infinity 0. 499742 0. 548495 18 17. 95894 3. 09472 FUSED SILICA 25 19 13. 41421 6. 156826 21 20 1134 5. 204856 FUSED SILICA 20. 5 21-78-5. 204856 MIRROR 20.5 22 1134-6. 156826 20. 5 23 13. 41421-3. 09472 FUSED SILICA 21 24 17. 95894 3. 09472 MIRROR 25 25 13. 41421 6. 156826 21 26 1134 5. 204856 FUSED SILICA 20. 5 27-78 0. 3 20. 5 IMA Infinity 0. 289101

A further aspect of the present design uses a tube lens to correct for residual aberrations in the objective. Residual aberrations are primarily the chromatic variation of distortion and higher order lateral color. These residual aberrations are related to use of the Offner field lens in the objective. One method to correct these residual aberrations is to employ a second glass material in the Offner field lens. Use of a second material can lead to an optical design with large elements and relatively tight tolerances. The alternative approach presented in this design is to use additional imaging optics to correct for residual aberrations. Such a design can produce a system having high NA, large field size, small lens diameter, as well as relatively loose tolerances.

Correcting these residual aberrations can further increase the field size or increase the bandwidth while maintaining the field size. The design of FIG. 7A

maintains the same approximately 0. 4mm field size as in the design of FIG. 3 and extends the bandwidth to cover 266 to 365nm without need for refocusing. The worst case polychromatic wavefront error for the design of FIG. 7A is approximately 0.036 waves.

The design includes two air spaced doublets 701, 702, 703, and 704, the doublets 701-704 fashioned from fused silica and calcium fluoride. The doublets 701-704 focus light through three fused silica lens elements, namely lens elements 705,706, and 707. These lens elements 705-707 are in proximity to an internal field. Light is then collimated by an air spaced triplet 708,709, and 710. Light then forms an external pupil at 711. The external pupil 711 can be used for placing dark field apertures, Fourier filters, and beamsplitters.

The lens prescription for the aspect of the invention illustrated in FIG. 7A is shown in Table 3.

Table 3. Prescription for lenses for the design of FIG. 7A Surf Radius Thickness Glass Diameter OBJ Infinity 0. 3 0. 4 1 78 5. 155765 FUSED SILICA 21 2 -1031.094 6.132752 21 3-13. 38766 3. 334036 FUSED SILICA 21. 5 4-18. 2281-3. 334036 MIRROR 25. 5 5-13. 38766-6. 132752 21. 5 -1031. 094-5. 155765 FUSED SILICA 21 7 78 5. 155765 MIRROR 21 8-1031. 094 6. 132752 21 9-13. 38766 3. 334036 FUSED SILICA 21. 5 10-18. 2281 0.598511 25.5 11 Infinity 0.595647 0. 87265 12-22. 2 -22.67364 1.496994 FUSED SILICA 1.716759 13-2. 487035 5. 332021 2. 721696 14-24. 12325 1.749722 FUSED SILICA 6. 761726 15-8. 563906 1. 647307 7. 426322 16 Infinity 1.017137 8. 707626 17-23. 20559 1.75 FUSED SILICA 9.034138 18-10. 09888 0.499806 9. 544791 19 459. 357 2 FUSED SILICA 10. 00487 20-12. 90167 0. 499731 10. 16545 21 9. 888518 5. 284916 FUSED SILICA 9. 738469 22 5. 468369 3. 606566 7. 299015 23-6. 158311 1. 499744 FUSED SILICA 7. 434168 24-10. 89758 0.499623 8. 474502 25 18.52911 2 FUSED SILICA 9. 287792 26-68. 1321-15. 25736 9. 417208 STO Infinity 15. 25736 8. 09706 28 Infinity 34. 89506 9. 431455 29 0- 30 Infinity 6 FUSED SILICA 18. 46143 31 Infinity 0 25. 39024 32 33 Infinity 30 17. 16851 34 - 0 - 35 Infinity 6 FUSED SILICA 26. 81778 36 Infinity 0 20. 63295 37 - 0 - 38 Infinity 81 15. 2277 39-159.7003 4 FUSED SILICA 22. 27788 40 37.47386 0.999856 22.92295 41 33.36497 9 CAF2 23.58799 42-80. 14523 3.436442 24. 07579 43 38.4464 8 CAF2 23. 97432 44 -53.0633 1.5 22.95647 45-39. 45511 3 FUSED SILICA 22. 35342 46 1094. 058 43. 27621 21. 67501 47 10. 8487 3. 18507 FUSED SILICA 12. 40192 48 8. 96916 4. 999989 10. 71199 49-24. 58978 2. 5 FUSED SILICA 10. 26452 50 117. 1346 47. 95638 10. 34545 51 175. 9777 5 FUSED SILICA 16. 71625 52 -37.37344 74.18151 17.10185 53-1113. 4 5 CAF2 11. 5593 54-14. 94822 0. 99955 11. 38304 55-13. 4032 2 FUSED SILICA 10. 93698 56 18. 26209 0. 99969 10. 92178 57 17.51017 6 CAF2 11. 25199 58-33. 75194 38. 51994 11. 218 59-100 4. 910667 IMA Infinity 16. 34334

The tube lens design of FIG. 7A uses only fused silica and calcium fluoride. Both of these materials have transmissions from approximately 190 nm through the infrared. Thus a tube lens can be designed to operate with an objective that can be re-optimized for different center wavelengths. Other tube lens magnifications may be achieved using this design. The design of FIG. 7A can be re-optimized for different afocal magnifications depending on the desired

overall magnification. Using the design presented herein, a focusing tube lens that directly forms an image that can expose a high speed sensor may be realized.

An additional aspect of the present design uses a tube lens to correct for residual aberrations in the objective. Correcting these residual aberrations can increase the field size or increase the bandwidth while maintaining the field size.

Residual aberrations are primarily the chromatic variation of distortion and higher order lateral color. The design of FIG. 7B maintains the same approximately 0.4mm field size as in the design of FIG. 3 and extends the bandwidth to cover 266 to 405run without need for refocusing. The worst case polychromatic wavefront error for the design of FIG. 7B is approximately 0.041 waves.

The design in FIG. 7B is composed of an objective 751 that collects the light and a tube lens 753 that corrects residual aberations. A set of lenses 752 may be provided to enhance performance. To achieve additional bandwidth beyond the design of FIG. 7A, the objective and tube lens of FIG. 7B are partially optimized together. Partial combined optimization of the objective and tube lens allows for further correction of the limiting off axis lateral color and chromatic variation of distortion. The tube lens forms an external pupil 754 that can be used in the same fashion as the design of FIG. 7A. The design presented in FIG. 7B also shows optional beamsplitter elements 754 that can be used to fold in illumination and autofocus light. The lens prescription for the aspect of the invention illustrated in FIG. 7B is shown in Table 4.

Table 4. Prescription for lenses for the design of FIG. 7B Surf Radius Thickness Glass Diameter OBJ Infinity 0. 300 0. 4 1 78. 000 5. 168 Fused silica 21 2-850. 121 6. 031 21 3-13. 361 3. 505 Fused silica 21. 5 4-180352-3. 505 MIRROR25. 5 5-13. 361-6. 031 21. 5 6-850. 121-5. 168 Fused silica 21 7 78.000 5.168 MIRROR 21 8-850. 121 6. 031 21 -13.361 3. 505 Fused silica 21. 5 10-18. 352 0. 599 25. 5 11 Infinity 0. 598 0. 8876633 12-22. 089 498 Fused silica 1. 735372 13-2. 492 5. 525 2. 742536 14-25. 242 1. 750 Fused silica 6.958087 15-8. 752 1. 574 7. 613493 STO Infinity 1. 011 8. 782304 17-26. 420 1. 750 Fused silica 9.130406 18-10. 453 0. 500 9. 615398 19 214. 479 2. 000 Fused silica 10.09149 20-12. 858 0. 500 10. 245 21 10.710 5. 074 Fused silica 9.775169 22 5.5729 3.622 7.468521 23-6. 365 1. 499 Fused silica 7.601525 24-11. 721 0. 499 8. 660195 25 20. 390 2. 000 Fused silica 9.505927 26-47.176-15. 391 9. 654623 27 Infinity 15.391 8. 373404 28 Infinity 40.197 9. 675574 29 0. 000 30 Infinity 6. 000 Fused silica 19.30992 31 Infinity 0.000 26. 25127 32-0. 000 33 Infinity 30. 000 17. 76485 34-0. 000 - 35 Infinity 6. 000 Fused silica 27.58405 36 Infinity 0.000 21. 36646 37 0. 000 38 Infinity 81.000 15. 75755 39-140. 860 4. 000 Fused silica 22.67915 40 35. 044 1. 068 23. 39086 41 31. 623 9. 000 CAF2 24. 17115 42 -71.279 1.000 24. 64826 43 34. 991 8. 000 CAF2 24. 5185 44-50. 752 1. 500 23. 4315 45 -37.766 3. 000 Fused silica 22. 75917 46 331. 53739. 13821. 89289 4711. 7293. 402 Fused silica 12. 61895 489. 2756. 25410. 82904 49-22. 713 2. 500 Fused silica 10.19172 50 149. 521 45. 554 10. 31249 51-142. 117 5. 000 Fused silica 16. 06325 52-25. 943 76.816 16. 73351 53-369. 224 5. 000 CAF2 11. 62667 54-14. 234 1. 000 11. 50051 55-12. 790 2. 000 Fused silica 11.04605 56 20. 324 1. 000 11. 08561 57 18. 583 5. 500 CAF2 11. 41199 58-32. 851 38. 519 11. 39769 59 100. 000 5. 11369 IMA Infinity 16. 29315

The design spectrum can be limited to 266-365nm and reoptimized for a 0.5 mm field size. The tube lens design of FIG. 7B also uses only fused silica and calcium fluoride and has all the flexibility for reoptimizing presented for the design in FIG. 7A.

The maximum numerical apertures of the current designs approaches or exceeds 0.9. The numerical aperture of a design may be reduced by placing a variable aperture at the aperture stop of the objective, effectively limiting the illumination and imaging light angles. It is also possible to control illumination and imaging angles independently by placing apertures at an external pupil plane using imaging optics such as the tube lens designs in FIG. 7A or FIG 7B. The numerical aperture of the illumination may be reduced by underfilling the objective aperture with the illumination light. Such a design enables the full imaging NA to be used.

An alternate aspect of the current design is an objective with increased field size. This aspect of the design is presented in FIG. 7C. The main difference between the design of FIG. 7C and that of FIG. 3 is the increase field size from 0. 4 mm to 1. 0mm and an increase in lens diameter from 25mm to 58mm. In

contrast, this field diameter is the same as in the design of FIG. 2. Maximum lens diameter of this design is much smaller than the design of FIG. 2. The objective of the design of FIG. 7C is corrected over a bandwidth from 285 to 320nm, maintains the high 0.90 numerical aperture, and the worst case polychromatic wavefront error for the FIG. 7C design is approximately 0.033 waves.

From FIG. 7C, the catadioptric group 771 includes a Mangin mirror element 772, which is a reflectively coated lens element, and a concave spherical reflector 773, which is also a reflectively coated lens element. Both Mangin mirror element 772 and concave spherical reflector 773 have central optical apertures where reflective material is absent. The absence of reflective material, in the center of the components shown, allows light to pass from the object or specimen 770 (not shown) through Mangin mirror element 772, reflect from the second surface of concave spherical reflector 773 onto the Mangin mirror element 772, and transmit through concave spherical reflector 773 to form an intermediate image 790 between concave spherical reflector 773 and field lens group 774, comprising three field lens elements 783,784, and 785 in this aspect of the design.

The focusing lens group 775 employs multiple lens elements, in this aspect the seven lens elements 776,777, 778, 779,780, 781, and 782, which may all be formed from a single type of material. The focusing lens group 775 collects light from the field lens group 774, including the intermediate image 790.

The design presented in FIG. 6 has the advantages and flexibility described with respect to the design of FIG. 3. The lens prescription for this design is shown in Table 5.

Table 5. Prescription for lenses for the design of FIG. 7C Surf Radius Thickness Glass Diameter OBJ Infinity Infinity 0.000 1 Infinity 43.913 STO Infinity-43. 913 20. 000 3 349. 851 4. 500 Fused silica 23.928 4-43. 383 0. 500 23. 709 5 30. 361 3. 650 Fused silica 21. 950 6 16. 181 7. 177 19. 386 7-17. 138 7. 305 Fused silica 19. 277 8 32.672 0.872 23. 722 9 47. 511 7. 000 Fused silica 23. 916 10-30. 308 0. 500 25. 201 11 37. 466 5. 500 Fused silica 26. 737 12-147. 458 27. 319 26. 555 13 14. 910 4. 500 Fused silica 21. 011 14 22. 738 0. 500 19. 515 15 20. 121 5. 000 Fused silica 19. 161 16-127. 415 7. 984 17. 640 17 12. 578 2. 500 Fused silica 7. 187 18-46. 4140. 5005333 19-12. 279 3. 131 Fused silica 4. 668 20-15. 865 2. 594 1. 955 21-576. 001 2. 250 Fused silica 4. 516 22-20. 181 0. 250 6. 277 23 40. 385 6. 603 Fused silica 60. 000 24 29. 574 15. 917 50. 000 25 -777.423 10. 056 Fused silica 50. 000 26-202.605-10. 056 MIRROR 50. 000 27-777. 423-15. 917 50. 000 28 29. 574-6.603 Fused silica 50. 000 29 40. 385 6. 603 MIRROR 60. 000 30 29. 574 15. 917 50. 000 31 -777.423 10. 056 Fused silica 50. 000 32-202. 605 0. 750 50. 000 IMA Infinity 1. 005

Further aspects of the design are presented in FIGs. 8-11, where FIG. 8 is a design able to perform in the presence of wavelengths from approximately 311-

315 nm, having approximately 26 mm diameter, a field size of approximately. 28 mm, and NA of approximately 0. 90. The lens prescription for this design is shown in Table 6.

Table 6. Prescription for lenses for the design of FIG. 8 Surf Radius Thiclçness Glass Diameter OBJ Infinity Infinity 0. 000 1 Infinity 18.849 8. 538 STO Infinity-18. 849 7. 220 3 6. 048 4. 786 Fused silica 8. 419 4 4. 149 1. 727 5. 777 5 19. 860 2. 000 Fused silica 5. 724 6-17. 207 1. 449 5. 502 7-3. 955 1. 200 Fused silica 5.247 8-12. 991 0. 100 5. 861 9 10. 518 5. 617 Fused silica6. 098 10-15. 147 0. 100 5. 985 11 4.995 2. 249 Fused silica 5. 701 12-159. 821 0. 999 5. 037 13-5. 316 4. 092 Fused silica 4. 659 14-4. 477 0.904 4. 116 15 2. 448 1. 906 Fused silica 2. 619 16 4. 138 0. 248 1. 101 17 Infinity1-. 5010. 801 18 16.697 2. 750 Fused silica 25. 240 19 13. 901 7. 871 22. 000 20-78. 318 2. 000 Fused silica 22. 000 21-100.000-2. 000 MIRROR 22. 000 22-78. 318-7. 871 22. 000 23 13. 901-2.750 Fused silica 22. 000 24 16. 697 2. 750 MIRROR 25. 240 25 13. 901 7. 871 22. 000 26-78. 318 2. 000 Fused silica 21. 000 27-100. 000 0. 200 22. 000 IMA Infinity 0. 291 FIG. 9 is an approximately 0.28 mm field design having approximately 26 mm diameter, a wavelength of between approximately 297 and 313 nm, and NA of approximately 0. 90. The lens prescription for this design is shown in Table 7.

Table 7. Prescription for lenses for the design of FIG. 9

Surf Radius Thielmess Glass Diameter OBJ Infinity Infinity 0. 000 1 Infinity 20.163 8. 585 STO Infinity-20. 163 7. 170 3-115. 896 1. 750 Fused silica 8. 591 4-16. 723 5. 036 8. 562 5-8. 430 2. 000 Fused silica 7. 122 6-9. 664 0. 100 7. 349 7 11.608 1. 200 Fused silica 7. 019 8 4.779 1.598 6. 337 9 10. 332 1. 750 Fused silica 6. 622 10 135. 162 1. 719 6. 592 11-6. 281 2. 555 Fused silica 6. 583 12-9. 052 0.100 7. 587 13 5.854 3. 250 Fused silica 7. 900 14-17. 400 1. 125 7. 264 15-7. 026 1. 499 Fused silica 6. 559 16-8. 971 5. 055 6. 242 17 2. 951 1. 906 Fused silica 2. 442 18-21. 084 0. 500 1. 255 19 Infinity 1.580 0. 314 20 17. 135 4. 713 Fused silica 26.000 21 12. 147 6. 064 20. 000 22-164. 287 2. 500 Fused silica 20.000 23-100.000-2. 500 MIRROR 20. 000 24-164.287-6. 064 20. 000 25 12. 147-4. 713 Fused silica 20.000 26 17. 135 4. 713 MIRROR 26. 000 27 12. 147 6. 064 20. 000 28-164. 287 2. 500 Fused silica 20.000 29-100. 000 0. 200 20. 000 IMA Infinity 0. 280 FIG. 10 is an approximately 0.4 mm field design having approximately 26 mm diameter, a wavelength of between approximately 297 and 313 nm, and NA of approximately 0. 90. The lens prescription for this design is shown in Table 8.

Table 8. Prescription for lenses for the design of FIG. 10 Surf Radius Thickness Glass Diameter OBJ Infinity Infinity 0.000 1.000 Infinity 17.977 8.974 STO Infinitv -17.977 7. 171 3. 000-73. 415 1. 750 Fused silica 8. 988 4.000-16. 484 3. 889 8. 954 5.000-7. 914 3. 077 Fused silica 7. 822 6.000-8. 792 0. 103 8. 317 7. 000 10. 984 1. 200 Fused silica 7. 777 8. 000 4. 966 1. 460 6. 942 9. 000 9. 494 1. 500 Fused silica 7. 137 10. 000 23. 256 2. 020 7. 037 11.000-6. 669 1. 871 Fused silica 7. 044 12.000-10. 034 0. 100 7. 866 13. 000 6. 034 2. 500 Fused silica 8. 344 14. 000 66. 970 0. 100 7. 904 15. 000 12.304 1. 750 Fused silica 7. 531 16. 000-60. 162 1. 300 6. 846 17.000-6. 852 1. 499 Fused silica 6. 139 18. 000-8. 993 4. 511 5. 804 19. 000 3. 141 1. 750 Fused silica 2. 466 20.000-15. 561 0. 499 1. 420 21.000 Infinity 1. 841 0. 794 22. 000 17.138 4.708 Fused silica 26. 000 23. 000 12. 005 6. 070 20. 000 24.000-177. 009 2. 500 Fused silica 20. 000 25.000-100. 000-2.500 MIRROR 20. 000 26.000-177. 009-6. 070 20. 000 27. 000 12. 005-4. 708 Fused silica 20. 000 28. 000 17. 138 4. 708 MIRROR 26. 000 29. 000 12. 005 6. 070 20. 000 30.000-177. 009 2. 500 Fused silica 20. 000 31. 000-100. 000 0. 200 20. 000 IL Infinity 0. 401

FIG. 11 illustrates a broad band design having approximately 26 mm diameter, a wavelength of between approximately 266 and 313 nm, field size of approximately. .28 mm, and NA of approximately 0.90. The lens prescription for this design is shown in Table 9.

Table 9. Prescription for lenses for the design of FIG. 11 Surf Radius Thickness Glass Diameter OBJ Infinity Infinity 0. 000 1.000 Infinity19. 1098. 783 STO Infinity-19. 109 7. 500 3. 000 59. 725 1.500 F_SILICA 8. 772 4.000-337. 579 1. 500 8. 650 5.000-9. 464 1. 500 F SILICA 8. 574 6.000-9. 415 4.925 8. 900 7. 000 8. 637 1. 200 F SILICA 7. 651 8. 000 4. 897 2. 128 6. 903 9. 000 214. 349 1. 750 F_SILICA 7. 117 10.000-12. 598 1. 147 7. 334 11.000-7. 560 1. 000 F SILICA 7. 320 12.000-772. 023 0. 100 7. 974 13. 000 9.411 2. 000 F_SILICA 8. 548 14.000-56. 012 0. 099 8. 529 15. 000 7. 107 2. 750 F_SILICA 8.352 16.000-22. 495 1. 159 7. 805 17.000-7. 960 1. 499 F SILICA 7. 103 18. 000-10. 073 5.482 6. 716 19. 000 3. 034 1. 748 F SILICA 2. 380 20.000-20. 121 0. 245 1. 276 21.000 Infinity 1. 041 0. 955 22. 000 16. 855 4. 806 F_SILICA 26. 000 23. 000 11. 392 6. 422 20. 000 24.000-133. 502 2. 000 F SILICA 20. 000 25.000-100. 000-2.000 MIRROR 20. 000 26.000-133. 502-6. 422 20. 000 27. 000 11. 392-4.. 806 F_SILICA 20. 000 28. 000 16. 855 4. 806 MIRROR26. 000 29. 000 11.392 6.422 20. 000 30.000-133. 502 2. 000 F_SILICA 20. 000 31. 000 -100.000 0.200 20.000

Infinity l l l 0. 283 l The current invention is capable of similar or better performance over previously known catadioptric objectives with smaller maximum lens diameters.

The lens having the largest diameter in these designs is typically the highly curved Mangin mirror element, the second optical element from the object or specimen.

Designs similar to the objective shown in FIG. 2 have 0.9 NA, large corrected bandwidths using large optical elements, and relatively tight manufacturing tolerances. The current designs presented above display large corrected bandwidths but use relatively small optical elements, and the designs have loose manufacturing tolerances. FIG. 12 is a graph contrasting previous systems against the current design in terms of relative bandwidth and maximum lens diameter. Relative bandwidth is defined as the bandwidth of the objective divided by the center wavelength. Previous systems are well corrected for relative bandwidths of at least 0.5 using lenses with maximum diameters greater than 100mm. Current objective designs as presented herein use a single glass material and are self corrected up to approximately 0.16 using lenses with maximum diameters from around 20mm up to 100mm. Further correction of these objectives over relative bandwidths up to 0.5 are possible using tube lenses to correct residual chromatic aberrations as in the designs of FIGs. 7A and 7B.

Similar correction is also possible for the objective alone by restricting NA or field size requirements.

FIG. 13 is a graph contrasting previous designs and the present design in terms of field size and maximum lens diameter. Previous systems tend to be well corrected for field sizes of 1 mm using lenses with maximum diameters greater than 100mm. Current objectives using the designs presented herein are corrected for field sizes of 0. 4 mm using lenses with maximum diameters from around

25mm, and 1. 0mm field sizes using lens diameters of 58mm. From this and the graph of FIG. 12, the ratio between field size and diameter of the largest element (including the Mangin mirror arrangement, field lens (es), and focusing lens (es), is generally less than 100 to 1, and may be less than 60 to 1. For example, the 58 mm lens diameter versus the 1.0 mm field size produces a ratio of 58 to 1. Larger field sizes are also possible with increasing lens diameter. Further correction of these objectives over larger field sizes are possible using tube lenses to correct residual chromatic aberrations as in the designs of FIGs. 7A and 7B. Similar correction is also possible for the objective alone by restricting NA or bandwidth requirements.

The present design may be employed in various environments, including but not limited to lithography, microscopy, biological inspection, medical research, and the like.

The design presented herein and the specific aspects illustrated are meant not to be limiting, but may include alternate components while still incorporating the teachings and benefits of the invention, namely the small design having a high NA able to be employed in various wavelengths using different illumination modes. While the invention has thus been described in connection with specific embodiments thereof, it will be understood that the invention is capable of further modifications. This application is intended to cover any variations, uses or adaptations of the invention following, in general, the principles of the invention, and including such departures from the present disclosure as come within known and customary practice within the art to which the invention pertains.