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Catoptric and catadioptric imaging system with pellicle and aperture-array beam-splitters and non-adaptive and adaptive catoptric surfaces

a technology of pellicle aperture and aperture array, applied in the direction of optical radiation measurement, instruments, interferometers, etc., can solve the problem of introducing the possibility of non-common path phase error

Inactive Publication Date: 2005-05-26
ZETETIC INST
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

AI Technical Summary

Benefits of technology

"The patent describes a new method for improving the image quality of an interferometric imaging system by using a thin beam-splitter to create an image with zero or minimal optical aberrations. The use of a thin beam-splitter reduces the need for optical elements in the system and increases the field of view. The patent also discusses the use of multi-element adaptive catoptric surfaces to compensate for optical aberrations introduced by a beam-splitter or other factors. Additionally, the patent describes the use of a thin fluorescent layer or interface to generate an optical interference signal and the impact of non-common path phase errors on the required performance specifications of the optical elements and detector. The patent also mentions the use of N-dimensional bi- and quad-homodyne detection methods to extend the advantages of these methods for measuring jointly N different properties of fields. Overall, the patent provides technical means for improving the performance of interferometric imaging systems."

Problems solved by technology

In the case where a beam-splitter is used for the beam combining function, the measurement beam component and the reference beam component of the combined beam may have subsequent to the beam-splitter different paths in the optical elements which introduces the possibility of non-common path phase errors.

Method used

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  • Catoptric and catadioptric imaging system with pellicle and aperture-array beam-splitters and non-adaptive and adaptive catoptric surfaces
  • Catoptric and catadioptric imaging system with pellicle and aperture-array beam-splitters and non-adaptive and adaptive catoptric surfaces
  • Catoptric and catadioptric imaging system with pellicle and aperture-array beam-splitters and non-adaptive and adaptive catoptric surfaces

Examples

Experimental program
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Effect test

first embodiment

[0102] Adaptive reflecting surfaces 42A-1, 42A-2, 42A-3, 42C-1, 42C-2, and 42C-3 and adaptive reflecting surfaces 46A-1, 46A-2, 46C-1, and 46C-2 shown in FIG. 1c may each be representative of annular rings or of sections of annular rings. The remaining description of the first embodiment will be based on the simple configuration wherein there are no additional reflecting surfaces beyond those described as a non-limiting example without departing from the scope and spirit of the present invention. The number of corresponding adaptive reflecting surfaces defines of the values of N that may be used in the N-dimensional bi- and quad-homodyne detection methods. In the non-limiting example of the simple configuration shown in FIG. 1c, the maximum value for N is 6.

[0103] Referring to FIG. 1d, the locations and orientations of adaptive reflecting surfaces are controlled by transducers according to servo control signal 98 from servo controller 96. For each of the adaptive reflective surfaces...

third embodiment

[0184] The location of the object plane of catadioptric imaging system 210A may also be on the plane surface of piano convex lens 258. In this case, the measurement beam can be arranged to probe substrate 60 as an evanescent field when h is of the order of λ / 4. The third embodiment can change rapidly from using the evanescent field as a probe beam to using the non-evanescent fields as a probe beam by use of the high speed vertical scan feature of the present invention.

[0185] The fourth embodiment of the present invention comprises interferometer 10 and catadioptric imaging system 210A of the third embodiment except that thin film fluorescent layer 12 is replaced by a pinhole array beam-splitter 12 the same as in the second embodiment shown schematically in FIG. 1f. Pinhole array beam-splitter 12 is used as the beam-splitter for generating the reference and measurement beams and for the function of combining the reference and measurement beam reflected / scattered by substrate 60. The ...

fifth embodiment

[0191] Referring to FIG. 3b, mirror system 354B redirects and displaces measurement beam 324A such that measurement beam 324C is propagating in a plane displaced out of the plane of FIG. 3b. Mirror system 354C displaces measurement beam 324C such that the transmitted measurement beam subsequently reflected by mirror 354D propagates in the plane of FIG. 3b. The remaining description of the present invention is the same as corresponding descriptions given for the first four embodiments of the present invention and corresponding descriptions given for embodiments given in cited U.S. Pat. No. 6,552,852 (ZI-38) and No. 10 / 366,651 (ZI-43); U.S. Provisional Patent Applications No. 60 / 447,254 (ZI-40), No. 60 / 448,360 (ZI-41), No. 60 / 448,250 (ZI-42), No. 60 / 442,982 (ZI-45), No. 60 / 459,425 (ZI-50), No. 60 / 485,255 (ZI-53), filed Jul. 7, 2003 (ZI-52) and entitled “Apparatus and Method for High Speed Scan for Subwavelength Defects in Semiconductor Metrology,” and filed Sep. 10, 2003 (ZI-54) entit...

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Abstract

An interferometric system including: an interferometer that directs a measurement beam at an object point to produce a return measurement beam, focuses the return measurement beam to an image point in an image plane, and mixes the return measurement beam with a reference beam at the image point to form a mixed beam; a beam combining layer located at the image plane which is responsive to the mixed beam and produces an optical beam therefrom, wherein the layer comprises a thin film with an array of transmissive openings formed therein and further comprises a fluorescent material associated with each of the openings of the array of openings; a detector that is responsive to the optical beam from the beam combining layer; and an imaging system that directs the optical beam from the beam combining layer onto the detector.

Description

[0001] This application claims the benefit of U.S. Provisional Application No. 60 / 506,715, filed Sep. 26, 2003.BACKGROUND OF THE INVENTION [0002] A number of different applications of catadioptric imaging systems for far-field and near-field interferometric confocal and non-confocal microscopy have been described such as in commonly owned U.S. Pat. No. 6,552,852 (ZI-38) entitled “Catoptric And Catadioptric Imaging Systems” and No. 6,717,736 (ZI-43) entitled “Catoptric And Catadioptric Imaging Systems;” U.S. Provisional Patent Applications No. 60 / 447,254, filed Feb. 13, 2003, entitled “Transverse Differential Interferometric Confocal Microscopy,” (ZI-40); No. 60 / 448,360, filed Feb. 19, 2003, entitled “Longitudinal Differential Interferometric Confocal Microscopy for Surface Profiling,” (ZI-41); No. 60 / 448,250, filed Feb. 19, 2003, entitled “Method and Apparatus for Dark Field Interferometric Confocal Microscopy,” (ZI-42); No. 60 / 442,982, filed Jan. 28, 2003, entitled “Interferometric...

Claims

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Application Information

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Patent Type & Authority Applications(United States)
IPC IPC(8): G01B9/02G01J1/58G02BG02B17/08G02B26/06
CPCG01J1/58G01B2290/70G01N21/9501G02B17/0808G02B17/086G02B26/06G03F1/84G03F7/7085G03F9/7088G01B9/02079G01B9/02007G01B9/02056G01B9/02014G01B9/02022G01B9/02068G01N21/8806
Inventor HILL, HENRY A.HAMANN, STEVENFISCHER, DAVID A.
Owner ZETETIC INST
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