MICROSCOPE

Abstract: A universal microscope for use with a commercial FT-IR spectrophotometer comprises a visible light source (224, 234) to permit a microscope to select and mask a target area on a sample image plane (200) that is then sampled with a beam of infrared radiant energy (1). The visible light microscope and the infrared microscope share a common optical path between objectives (217, 233) that form one or more remote image planes (202, 204) and the sample image plane (200). Both the visible light and the infrared radiant energy are masked twice to spatially define the target area at the sample image plane (200) using the infrared radiant energy. Radiant energy from outside the target area at the sample image plane is removed at first image plane (202). Energy diffracted outside the target area by the first mask or the focusing optics is removed at the second image plane mask (202, 204). The first remote image plane (202) is imaged onto the second remote image plane (202, 204) with the radiant energy gaining spectroscopic information and additional image information by passing through or reflecting off a sample located at the intervening sample image plane (200). Samples having a diameter of less than 8 microns can be spectroscopically isolated with 2-25 micron infrared radiant energy.

Description: MICROSCOPE The present invention relates to the general field of microscopy and particularly the field of Fourier- transform infrared (FT-IR) microspectrophotometry. The ready existence of commercial FT-IR spectrophotometers greatly facilitates infrared analysis of specimens. The utility of FT-IR microspectroscopy, however, is limited by the size of the microscopic sample that can be observed. If a sample is too small, radiant energy from surrounding areas reaches the detector and produces a spectrum containing the combined features of all materials in the field of view of the microscope. This phenomenon is termed spectroscopic mixing and is a problem which is particularly acute for an infrared microscope because the longer wavelength of the infrared radiation results in lower inherent resolution as compared to, for example, a visible light microscope. Spectroscopic mixing may be eliminated by electronically subtracting the spectrum of a known material from a mixed spectrum. Electronic subtraction does not work, however, without first knowing both the spectral features and the relative intensity of the features for the area immediately surrounding the object of interest. As a practical matter, electronic subtraction often does not work because the spectrum of the surrounding material cannot be isolated. The resolution of any microscope is limited by the effects of diffraction. Diffraction depends on the wavelength of the radiant energy, the numeric aperture of the optical system and the spatial coherence of the radiation. The smallest separation of objects that may be resolved is typically expressed in terms of Rayleigh's criterion which is mathematically defined as 0.61 times the wavelength of the radiant energy divided by the numerical aperture of the microscope. Diffraction, however, has long been recognized as a practical limit to resolution and not as a theoretical limit. Only the wavelength of the radiant energy ultimately need limit the resolution of a microscope. In U.S. Patent 3,013,476, Minsky discloses what has come to be known in the art as a confocal scanning microscope. The confocal microscope uses two pinhole apertures positioned at focal planes. One pinhole aperture is placed at a real image plane between a light source and an objective lens so that the lens focuses the light emerging from the pinhole aperture onto a sample. A second pinhole aperture is positioned between an objective lens and a detector at a real image plane so that light from the sample is focused onto the second pinhole aperture. A sample is placed at the sample image plane and moved in a scanning pattern s that the detector supplies an input signal corresponding to the raster scan of a television. Minsky discloses that the confocal scanning microscope reduces the depth of field for an optically thick transmissive sample because the detector receives very little light from outside the plane of the sample image plane. Others have noted that a confocal microscope increases the image contrast by reducing the amount of stray light that reaches the detector from outside the image plane. This superior depth of field resolution in a confocal microscope produces an apparent increase in resolution. Sheppard and Wilson of the University of Oxford have noted that a scanning confocal microscope may obtain an actual increase in the resolution above that anticipated for using the same optics without a confocal arrangement. This actual improvement in resolution, however, iε only as great as a factor of 2.4 and is accompanied by a reduction in image contrast and, hence, a reduction in apparent resolution. Experimental research in the field of confocal microscopy apparently has been directed to producing a scanning microscope for forming an image of a sample. The resolution of a scanning microscope is limited by the motion of the sample relative to the radiant energy. No known experiment has attempted to determine the actual point to point resolution of a confocal microscope. Present mathematical models of image formation in a confocal microscope provide an inadequate explanation of image formation in the field of microspectrophotometry. The transform function for a confocal microscope involves a complicated convolution of the transform functions of the condensing and collecting optics as well as the focal plane apertures. The only exact mathematical solutions that have been published involve the special cases of point to point imaging of a point source that emits radiant energy that is either perfectly coherent or perfectly incoherent. Microspectrophotometry, however, necessarily involves the use of partially coherent radiant energy. The source of the radiant energy has effective spatial dimensions that are determined by the size and shape of the sample. The wavelength range of the radiant energy is determined by the wavelength range of the spectroscopic characteristics of the sample which are to be observed. The optical properties of a confocal microscope that uses partially coherent radiant energy is therefore important for microspectrophotometry and must be determined experimentally. Practical concerns relating to throughput efficiency mitigate against using a confocal microscope in microspectroscopy. Conventional confocal microscopes have used a laser as an intense light source to supply monochromatic light to the source side pinhole aperture. However, conventional spectrometers, especially FT-IR spectrophotometers, do not have an intense source of constant amplitude radiant energy over a broad frequency range. Further, confocal microscopes have only attempted to image samples and not to distinguish between regions on a sample having different compositions. Thus, the theory of confocal microscopy and conventional confocal scanning microscopes have held no practical utility for microspectroscopy in general or for FT-IR microspectrophotometry in particular. The present invention relates, first, to the discovery that a microscope can obtain an order of magnitude improvement in spatial definition of an observation area on a sample by masking the imaging energy at least two remote image planes and, second, to a microscope for performing microscopy, particularly microspectrophotometry, in accordance with the discovery. Specifically, a universal microscope for use in combination with a commercial FT-IR spectrophotometer comprises a visible light microscope for selecting and masking an area of a sample and an infrared microscope for sampling the masked area. The visible light microscope and the infrared microscope share a common optical path between one or more remote image plane masks and a sample image plane such that both the visible light and the infrared radiant energy are masked twice, once when the radiant energy is incident to the surface of the sample and once when the radiant energy exits the sample, so as to spatially define the same area at the sample image plane. The first image plane mask removes energy from outside the target area at the sample image plane. The second image plane mask removes energy from outside the target area that is diffracted by the first mask or the condensing and collecting optics. The first remote image plane is effectively imaged onto the second remote image plane with the radiant energy gaining spectroscopic information and additional image information by passing through or reflecting off a sample located at an intervening sample image plane. The preferred embodiment of the present invention comprises a universal visible light and infrared microscope that easily switches between transmittance and reflectance modes in either upright or inverted configurations. A visual observation means permits a microscopist to observe a sample in reflectance mode simultaneously in both upright and inverted modes to as to properly mask a sample that is opaque to visible light but transparent to infrared radiant energy. A spectroscopist may thus select an observation area before directing the infrared energy beam of the FT-IR spectrophotometer at the selected area. Experiments have shown that the spatial extent of the area at the sample image plane defined by the mask in visible light is substantially the same area resolved by the infrared radiation even though the wavelength of the infrared radiation is approximately ten times greater than the wavelength of the visible light. The improvement in resolution obtained with partially coherent radiant energy exceeds anything predicted from theoretical investigations exceeds anything predicted from theoretical investigations of the special cases of confocal imagery for point sources of perfectly coherent and perfectly incoherent radiation. Samples having a diameter of less than 8 microns have been spectroscopically isolated with 2-25 micron infrared radiant energy. The present invention can be understood with the aid of the following drawings, in which: Figure 1 is a schematic layout of a universal microscope that places a sample image plane between masked remote image planes according to the present invention; Figure 2 is useful for understanding the phenomenon of spectroscopic mixing and how the present invention overcomes the problem; Figure 3 illustrates the diffraction pattern of masked microscope objectives using incoherent radiant energy; and Figure 4 is a spectrum obtained in accord with the teachings of the present invention. For purposes of the present invention, the phrase "radiant energy" describes electromagnetic radiation used to observe a microscopic sample with an electronic detector. In contrast, the phrase "visible light" refers to electromagnetic radiation that in some way makes the sample visible to a microscopist. It is preferred that the visible light have a shorter wavelength than the radiant energy. Figure 1 shows a universal microscope for use with the present invention. To simplify the drawing and aid in understanding the invention, condensing lenses are represented by outwardly pointing arrows and remote image planes are represented by dashed lines in a style that is generally known to those skilled in the art. A beam of radiant energy 1 is incident on mode selecting mirror 211. In a reflectance mode of operation, mirror 211 reflects radiant energy to mirrors 213 and 215. Mirror 215 directs the radiant energy to sample image plane 200 through first focusing objective 217 which is preferably a Cassegrainian mirror lens. Before being focused on the sample image plane, however, the microscope of the present invention focuses the radiant energy at a first remote image plane 202 that is physically remote from sample image plane 200. A first variable aperture diaphragm, not shown in Figure 1, spatially defines an arbitrary, adjustable geometric shape onto remote image plane 202. First focusing objective 217 reimages the first remote image plane at the sample image plane 200 to permit selecting the area on the sample image plane 200 to permit selecting the area on the sample image plane that is illuminated by the incident radiant energy. First focusing optics 217 reimages the remote image plane onto sample image plane 200 so that the first variable aperture diaphragm spatially defines both the incident and reflected radiant energy. In an inverse transmittance mode, mode mirror 211 permits the radiant energy to travel directly from the source of radiant energy to mirror 231. The incident radiant energy forms a focus at second remote image plane 204. A second variable aperture diaphragm at the second remote image plane, not shown in Figure 1, spatially defines an arbitrary geometric shape. Second focusing objective 233, preferably a Cassegrainian mirror lens, reimages the second remote image plane onto the sample image plane to permit selecting the area on the sample image plane that is illuminated by the radiant energy. First focusing objective 217 focuses the radiant energy transmitted through sample image plane 200 at first remote image plane 202. The first variable aperture diaphragm at first remote image plane 202 spatially defines the shape of the illuminated area at the first remote image plane to correspond to the image of the second variable aperture diaphragm at the second remote image plane. Mirrors 215, 213 and 211 direct the transmitted radiant energy to the detector. The microscope shown in Figure 1 permits the sample image plane 200 to be viewed in a variety of different modes. The microscope is operated in reflectance mode by positioning mirror 211 so that the beam of incident radiant energy is directed by mirror 231 through remote image plane 204. An appropriate beam splitter must be used to separate the incident and reflected radiant energy. Likewise, the microscope may operate in a trans issive mode by using first focusing objective 217 to direct the radiant energy from the source to the sample image plane. Second focusing objective 233 collects the transmitted radiant energy and directs it to the detector using mirror 231. The microscope is operated in an inverse transmissive/reflectance mode by directing the incident radiant energy to second focusing objective 233 and using first focusing objective 217 to collect radiant energy that is transmitted through the sample and second focusing objective 233 to collect radiant energy that is reflected from the sample. The microscope may be operated in a transmissive/reflectance mode by directing the incident radiant energy to first focusing objective 217 using second focusing objective 233 to collect radiant energy that is transmitted through the sample and first focusing objective 217 to collect radiant energy that is reflected from the sample. It is believed that the majority of the modes of operation using the radiant energy need not normally be used. Therefore, a microscope having only transmissive and reflectance modes of operation is preferred for reasons of mechanical simplicity and economy. The remaining modes, however, have utility in particular instances such as for easing sample handling and for checking the reliability of observations. The shape of the transmissive area at first remote image plane 202 may be determined using a reflectance observation beam with eyepiece 219 which, in combination with flipper mirror 221 and flat mirror 229, provides means for visually observing the combined images of both image sample plane 200 and first remote image plane 202. flipper mirror 221 preferably blocks out the radiant energy so that image planes 200 and 202 are observed only with visible light emanating from filament 224 of lamp 225 by way of a partially transmissive flipper mirror 227. The sample image plane may be viewed using a transmissive observation beam of visible light from filament 234 of lamp 235. Second focusing objective 233 preferably images the visible light reaching first remote image plane 204 by way of partially transmissive mirror 237. First focusing objective 217 directs the visible light to eyepiece 219 by way of mirrors 221 and 229. The microscope shown in Figure 1 can produce numerous additional observation beams of visible light. The microscope may receive an inverse reflectance observation beam from filament 234 of lamp 235. Partially transmissive mirror 237 reflects part of the beam of visible light to sample image plane 200. Mirror 239 directs the reflected light to mirror 241. Transfer optics 245 and 247 direct the light to eyepiece 219 by way of mirror 243. Further, eyepiece 219 may be constructed with appropriate transfer optics so that the microscope may receive dual reflectance observation beams from lamps 225 and 235 which permit simultaneously observing the masking of remote image planes 202 and 204 with reflected light. The dual reflectance beam permits masking each remote image plane to the same shape when the sample is opaque to visible light but transmissive to the radiant energy. Additionally, lamp 225 can produce an inverse transmissive observation beam using mirrors 227 and 239. The optical path of the microscope is symmetric with respect to the optical path taken by the radiant energy or the visible light with respect to the image sample plane. Thus, the microscope of the present invention easily converts from a conventional upright microscope into an inverted microscope as needed to make a particular measurement. The preferred embodiment of the present invention uses entirely mirror optics at any place where the visible light and radiant energy share a common optical path. For example, most visible light transmissive materials used in microscopes are opaque to infrared light and, in any event, no refracting lens is known that can focus infrared radiant energy and visible light at the same image plane. Exact concurrences of the image planes formed with the radiant energy and visible light is necessary to mask a sample with visible light and then observe it with the radiant energy. Adjustments to the focusing objective may be necessitated by optical distortions introduced by the sample. For example, it is known in the art that a sample may introduce spherical aberration into the observed image. This spherical aberration may be corrected by reducing the separation of the primary and secondary mirrors of focusing objectives 217 and 233 according to the formula: Kt (n ± 2 - 1) / n ± 3 ; where t = thickness of the sample; n. = index of refraction of the specimen, and K = a constant unique to the microscope objective. The derivation and use of this formula is understood by a person skilled in the art and, therefore, not a subject of the present invention. Figure 2 illustrates the phenomenon of spectroscopic mixing that limits the resolution of a microspectrophotometer. Figure 2a is a schematic representation of three sample materials, A, B and C. Figure 2b shows profile 401 which represents the intensity of the radiant energy from region B. Part 401a of profile 401 represents the radiant energy diffracted into region A. Likewise, Figure 2c shows profile 402 corresponds to the radiant energy from material C. Profile 402b represents the radiant energy from material C diffracted into the area of material A. Finally, Figure 2d shows profile 403 corresponding to the profile of the radiant energy from material A. Profiles 403a and 403b represent radiant energy that is diffracted from the region of material A into the regions containing materials B and C, respectively. The present of extraneous energy from materials B and C in the field of view of material A causes the spectrum of material A to be mixed with the spectra of all three materials. This spectroscopic mixing may be corrected in several ways. The microscope of the present invention minimizes spectroscopic mixing through the spatial definition of a target region at the sample image plane to correspond in shape to the shape of material A. Spatial definition means first removing radiant energy from outside the shape of a target at a real image plane corresponding to the sample image plane and then removing radiant energy that is diffracted from within said shape into regions outside said shape at a real image plane corresponding to said sample image plane. Defining the spatial extent of the incident radiation causes materials B and C to receive only energy from fringes 403a and 403b. Masking the sample a second time removes what energy has reached materials B and C and causes a substantial reduction in the spectroscopic mixing of the samples. Masking the radiant energy at remote image planes is preferred to "near field" masking at the surface of the sample because near field masking may destroy the sample. Remote image plane masking is also physically more convenient and produces superior optical performance for viewing inside an optically thick sample. The spatial definition of a microscope using multiple real image plane masks is not determined in the same way as is resolution in a conventional microscope. The improvement in spatial definition as a percentage of illuminated target area is substantially independent of the wavelength of the radiant energy formed by the remote image plane mask so long as: i) the masks define the same geometric target area at the sample image plane, and ii) the smallest dimension of the target area is greater than the wavelength of the radiant energy. If these conditions are met, the geometric shape of the target region may be established using radiation having a short wavelength and then observed with radiant energy having a longer wavelength without significantly enlarging the target area. Spatial definition may be limited by the contrast of the sample in the target area. A high contrast target sample diffracts more energy into adjacent regions than does a low contrast target since the amount of diffraction is proportional to the difference in the refractive indices between the adjoining materials. Masking more than two remote image planes does not appear to increase spatial definition although experimental evidence is not conclusive. Figure 3 illustrates the principles of diffraction that govern the present invention. Figure 3a shows a diffraction edge 500. Profile 502 of Figure 3b represents the distribution of diffracted energy in a microscope objective after it is masked once by edge 500 at a remote image plane using radiant energy from a perfectly incoherent point source. Profile 504 represents a corresponding profile for radiant energy from the first remote image plane that is masked at a second remote image plane. The energy in the main diffraction lobe is pulled closer to the edge of the mask so that twice masking the radiant energy from a remote image plane effectively reduces the relative amount of energy present in the diffraction fringes. If mask edge 500 is treated as a circular aperture, ninety five percent of the power contained in the radiant energy is typically included within the fourth or fifth diffraction minimum. For a microscope objective that is twice masked, however, the ninety five percent power threshold is within the first diffraction minimum. It is known in the art that the location of the first diffraction minimum is nearer a diffraction edge for coherent radiant than for incoherent radiant. Therefore, coherent radiation is preferred. Nevertheless, spatial definition at remote image planes also improves the resolution of a microscope objective using incoherent radiation. The resolution obtained using partially coherent radiation also increases. Another method for decreasing the spread of the main diffraction lobe is to apodize the microscope objective, especially the condenser. Apodization, however, transfers power into the diffraction fringes and greatly reduces throughput efficiency by blocking most of the aperture. The preferred embodiment of the present invention uses apodized objectives in the form of Cassegrainian mirror lenses that block only a small percentage of the incident radiation. Resolution might be improved by apodizing the objective to an even greater extent at the expense of a decrease in signal to noise. However, the signal to noise ratio produced by the present invention already requires using more sensitive infrared detectors than presently found on some commercial FT-IR spectrophotometers. Any increase in the resolution of the microscope that might be gained by apodizing the aperture is not considered to be worth the loss in throughput efficiency. EXAMPLE Figure 4 shows an infrared transmission spectrum of a human hair obtained by twice masking the radiant energy at remote image planes, once for the incident radiant energy and once for transmitted radiant energy. The hair was placed at an image sample plane and the infrared radiant energy transmitted through the hair was directed to a detector connected to the computer of an FT-IR spectrophotometer. The hair represents a high contrast sample that produces significant diffraction at the sample image plane. An absorption band 601 corresponds to a region in which human hair is known to exhibit total absorption of infrared radiant energy. Profile 611 corresponds to the spectrum obtained after adjusting, under visible light, a four-shutter, variable aperture diaphragm at a remote image plane positioned between the sample and the detector to define a rectangular cross section area on the sample image plane corresponding to the shape of the hair. The radiant energy between approximately 2950 and 3500 wave numbers corresponds to stray diffracted radiant energy from regions surrounding the hair. Next,- profile 613 was obtained by masking, in the same manner, a remote image - - plane between the source and the [detector] sample. The amount of stray radiant energy in the absorption band reaching the detector was reduced. Nevertheless, " approximately 3% of the radiant energy in this band reaching the detector was from areas located outside the sample area on the sample image plane. Finally, profile 615 corresponds to the spectrum obtained by masking the transmitted infrared radiant energy at both remote image planes so that both masks define substantially the same area on the sample image plane. Profile 615 exhibits the total absorption anticipated in the absorption band. The principles, preferred embodiments and modes of operation of the present invention have been described in the foregoing specification. The invention, which is intended to be protected herein should not, however, be construed as limited to the particular forms described herein as these are to be regarded as illustrative rather than restrictive. Variations and changes may be made by those skilled in the art without departing from the spirit of the invention. Accordingly, the foregoing detailed description should be considered exemplary in nature and not as limiting to the scope and spirit of the invention set forth in the appended claims.

Claims: WHAT IS CLAIMED IS: 1. A microscope, comprising: a first focusing objective positioned to focus radiant energy between a first remote image plane and a sample image plane; a first variable diaphragm positioned at said first remote image plane for spatially defining an arbitrary, readily changeable shape at said first remote image plane; a second focusing objective positioned to focus radiant energy between the sample image plane and a second remote image plane; and a second variable diaphragm positioned at said second remote image plane for spatially defining an arbitrary, readily changeable shape at said second remote image plane. 2. The microscope as claimed in Claim 1, further comprising: means for receiving a beam of radiant energy into said microscope, said beam of " radiant energy being selected from the group consisting of: (1) a transmittance mode beam in which said second and said first focusing objectives direct said beam of radiant energy from said second remote image plane to said sample image plane and from said sample image plane to said first remote image plane, -respectively; (2) a reflectance mode beam in which said first focusing objective directs said beam of radiant energy from said first remote image plane to said sample image plane and from said sample image plane back to said first remote image plane; (3) a transmittance/reflectance mode beam in which said second focusing objective directs said beam of radiant energy from said second remote image plane to said sample image plane and directs part of said beam of radiant energy from said sample image plane back to said second remote image plane, and said first focusing objective directs part of said beam of radiant energy from said sample image plane to said first remote image plane; (4) an inverse transmittance mode beam in which said first and said second focusing objectives direct said beam of radiant energy from said first remote image plane to said sample image plane and from said sample image plane to said second remote image plane, respectively; (5) an inverse reflectance mode beam in which said second focusing objective directs said beam of radiant energy from said second remote image plane to said sample image plane and from said sample image plane back to said second remote image plane; and (6) an inverse transmittance/reflectance mode beam in which said first focusing objective directs said beam of radiant energy from said first remote image plane to said sample image plane and directs part of said beam of radiant energy from said sample image plane back to said first remote image plane, and said second focusing objective directs part of said beam of radiant energy from said sample image plane to said second remote image plane. 3. The microscope as claimed in Claim 2, further comprising means for selecting a mode of operation for the microscope from among said group of receiving means. 4. The microscope as claimed in Claim 2, further comprising means for selecting a mode of operation for the microscope, said mode being selected from among the group consisting of said reflectance mode and said transmittance mode. 5. The microscope as claimed in Claim 2, further comprising: means for receiving a beam of visible light into said microscope, said beam of visible light being selected from the group consisting of: (1) a transmittance observation beam in which said second and said first focusing objectives direct said beam of visible light from said second remote image plane to said sample image plane and from said sample image plane to said first remote image plane, respectively; (2) a reflectance observation beam in which said first focusing objective directs said beam of visible light from said first remote image plane to said sample image plane and from said sample image plane back to said first remote image plane; (3) an inverse transmittance observation beam in which said first and said second focusing objectives direct said beam of visible light from said first remote image plane to said sample image plane and from said sample image plane to said second remote image plane, respectivel ; (4) an inverse reflectance observation beam in which said second focusing objective directs said beam of visible light from said second remote image plane to said sample image plane and from said sample image plane back to said second remote image plane; and (5) a dual reflectance observation beam in which said first focusing objective directs a first beam of visible light from said first remote image plane to said sample image plane and from said sample image plane back to said first remote image plane, and a second beam of visible light that said second focusing objective directs from said second remote image plane to said sample image plane and from said sample image plane back to said second remote image plane. 6. The microscope as claimed in Claim 5, further comprising means for visually observing said visible light so as to adjust the openings of said first or second variable diaphragms. 7. The microscope as claimed in Claim 6, further comprising means for selecting among said observation beams. 8. A microscope as claimed in Claim 6, further comprising means for selecting either said beam of radiant energy or said beam of visible light to be directed into said microscope. 9. A microscope, comprising: means for receiving radiation energy from a source of radiant energy along a common optical path; means for forming a sample image at a sample image plane along said common optical path, said sample image having an arbitrary shape; means for spatially defining said sample image at said sample image plane, including: i) means for removing radiant energy from outside said arbitrary shape at a real image plane corresponding to said sample image plane, and ii) means for removing radiant energy that is diffracted from within said arbitrary shape into regions outside said arbitrary shape at a real image plane corresponding to said sample image plane; and means for directing the radiant energy from said sample image plane to a detector. 10. The microscope as claimed in Claim 9, wherein said means for removing radiant energy from outside said arbitrary shape comprises: means for forming a first remote image plane at a location that is remote from said sample image plane along said common optical path; means for imaging said first remote image plane onto said sample image plane; and means for positioning a first adjustable mask at said first remote image plane so that said arbitrary shape formed by said mask corresponds to said arbitrary shape on said sample image plane. 11. The microscope as claimed in Claim 10, wherein said means for removing radiation diffracted from within said arbitrary shape into regions outside said arbitrary shape comprises means for imaging said sample image plane onto said first remote focus along said common optical path. 12. The microscope as claimed in Claim 11, further comprising: means for receiving visible light along said common optical path so as to illuminate said first adjustable mask at said first remote image plane and the image of said first adjustable mask at said sample, said visible light being spatially defined to the same arbitrary shape as the radiant energy; and means for observing said visible light so as to observe said arbitrary shape on said sample image plane. 13. The microscope as claimed in Claim 12, wherein: said means for imaging said first remote image plane onto said second remote image plane comprises at least a portion of a Cassegrainian mirror lens having primary and secondary mirror elements, said mirror lenses comprising means for adjusting the separation of said primary and secondary mirror elements, said mirror lens imaging both said radiant energy and said visible light; and said means for imaging said sample image plane onto said first remote image plane comprises at least a portion of said Cassegrainian mirror lens. 14. The microscope as claimed in Claim 10, wherein said means for removing radiation diffracted from within said arbitrary shape into region outside said arbitrary shape comprises: means for forming a second remote image plane at a location that is remote from said sample image plane along said common optical path; means for imaging sa d sample image plane onto said second remote image plane; and means for positioning a second adjustment mask at said first remote image plane so that said arbitrary shape formed by said mask corresponds to said arbitrary shape on said sample image plane. 15. The microscope as claimed in Claim 14 further comprising: means for receiving visible light along said common optical path so as to illuminate said first and second adjustable masks and the image of said first adjustable mask at said sample image plane, said visible light being spatially defined to the same arbitrary shape as the radiant energy; and means for observing said visible light so as to observe said arbitrary shape on said sample image plane. 16. The microscope as claimed in Claim 15, wherein; said means for imaging said first remote image plane onto said second remote image plane comprises at least a portion of a first Cassegrainian mirror lens having primary and secondary mirror elements, said first mirror lenses comprising means for adjusting the separation of said primary and secondary mirror elements, said first mirror lens imaging both said radiant energy and said visible light; and said means for imaging said sample image plane onto said second remote image plane comprises at least a portion of a second Cassegrainian mirror lens having primary and secondary mirror elements, said second mirror lenses comprising means for adjusting the separation of said primary and secondary mirror elements, second first mirror lens imaging both said radiant energy and said visible light. 17. The microscope as claimed in Claim 10, further comprising: means for forming one ur more additional remote image planes which are remote from said sample image plane; means for imaging said sample image plane onto said one or more additional remote image planes; and means for positioning one or more additional adjustable masks at said one or more additional remote image planes. 18. The microscope as claimed in Claim 11, wherein said first remote image plane is sequentially disposed along said common optical path without an intervening real image plane. 19. The microscope as claimed in Claim 14, wherein said first remote image plane and said second remote image planes are sequentially disposed along said common optical path without an intervening real image plane. 20. A method of illuminating a target in a microscope, comprising the steps of: receiving radiant energy from a source of radiant energy along a common optical path; forming a sample image at a sample image plane along said common optical path, said sample image having an arbitrary shape; spatially defining said sample image at said sample image plane, including the steps of: i) removing radiant energy from outside said arbitrary shape at a real image plane corresponding to said sample image plane, and ii) removing radiant energy that is diffracted from within said arbitrary shape into regions outside said arbitrary shape at a real image plane corresponding to said sample image plane; and directing the radiant energy from said sample image plane to a detector. 21. A method of illuminating a target in a microscope as claimed in Claim 20, wherein: said step of removing radiant energy from outside said arbitrary shape consists of masking the radiant energy at a first remote image plane that is remote from said sample image plane to correspond to said arbitrary shape and imaging said remote image plane onto said sample image plane; and said step of removing radiant energy that is diffracted from within said arbitrary shape consists of masking the radiant energy at said first remote image plane. 22. A method of illuminating a target in a microscope as claimed in Claim 21, wherein said first remote image plane is sequentially disposed along said common optical path without an intervening real image plane. 23. A method of illuminating a target in a microscope as claimed in Claim 20, wherein: said step of removing radiant energy from outside said arbitrary shape consists of masking the radiant energy at a first remote image plane that is remote from said sample image plane to correspond to said arbitrary shape and imaging said remote image plane onto said sample image plane; and said step of removing radiant energy that is diffracted from within said arbitrary shape consists of imaging said sample image plane at a second remote image plane that is remote from said sample image plane and masking said second remote image plane to correspond to said arbitrary shape. 24. A method of illuminating a target in a microscope as claimed in Claim 23, wherein said first and second remote image planes are sequentially disposed along said common optical path without an intervening real image plane.

Inventors: MESSERSCHMIDT ROBERT G, STING DONALD W, MESSERSCHMIDT, ROBERT, G., STING, DONALD, W.
Applicants: SPECTRA TECH INC, SPECTRA-TECH, INC.
Application year: 1988
Main classification: G02B21
IPC codes: G01J3, G01N21, G02B21