Abstract:
An opto-electronic image magnifying system. The magnifiying system includes: a light source ( 38, 39 ) which illuminates an object to be viewed; a miniaturized opto-electronic magnifier module (MOM), made of a lens ( 31 ) and a photodetector array ( 32 ), which receives the light from the illuminated object; an electronic circuit ( 34 ) which receives the signal from the MOM; a video-monitor ( 35 ) which receives the magnified signal from the electronic circuit and displays the image. The opto-electronic image magnifying system allows for small objects or features of small objects to be observed in which historically compound microscopes or specialized optical viewing systems were required to observe the small objects.

Description:
RELATED CASES 
   Applicant hereby claims the benefit of their copending provisional application Ser. No. 60/112,172, filed Dec. 14, 1998. 

   FIELD OF THE INVENTION 
   This invention relates to the ever-increasing need in industry, commerce, and education to observe small objects or very small features of objects and to characterize those objects and or features. Historically, such observations have been made on compound microscopes or specialized optical viewing systems. 
   BACKGROUND OF THE INVENTION 
   Leeuwenhoek founded the science of microbiology in about 1700 using a single-lens microscope. His bead of glass had a magnification of 266 times. Fifty years earlier the compound microscope had been discovered. Although Leeuwenhoek&#39;s single-lens microscope produced higher resolution and better image quality than the compound microscope, it did not withstand the test of time. The compound microscope, with objective and eyepiece lens systems, became the standard for all modern light microscopes. The principle reason for success of the compound microscope was its ease-of-use. To use the Leeuwenhoek microscope, the sample and microscope had to be placed very close to the eye. This made Leeuwenhoek&#39;s simple microscope difficult, and many times nearly impossible, to use. Over the centuries, the compound microscope has been improved and enhanced, but it has largely maintained its use of an objective lens with a relatively long (at least 160 mm) distance to the image formation plane, and an eyepiece to perform second stage magnification and presentation to the human eye. 
   Lenses are used to create real images in cameras and projectors of many kinds, including video cameras, the part of a television transmitting apparatus that receives the primary image formed by a lens on a light-sensitive material and transforms it into electrical impulses. In its standard use, a video camera transmits images of large objects onto a monitor screen. The image produced by the lens on the light-sensitive material is reduced in size, or demagnified. As objects are brought closer to the lens they appear larger on the monitor screen, but the lens does not create an image larger than the object. Even in a macro mode, the image formed by the lens on the light-sensitive material is not magnified. 
   A lens creates a magnified image either as a virtual image or as a real image. If an object is placed at a distance closer to the lens than its focal length, then a magnified virtual image is seen when the eye is placed close to the lens. This is the Leeuwenhoek microscope. 
   If an illuminated object is placed at a distance greater than the focal length of the lens, but less than twice the focal length of the lens, then a magnified real image is projected. The objective lens of the compound light microscope projects a magnified real image. Viewing this real image requires an eyepiece lens or screen. The eyepiece lens magnifies the real image and transforms it into a magnified virtual image seen with the eye. This combination of objective and eyepiece lenses is the compound microscope. 
   Compound microscopes have been the standard configuration for a light microscope for over two hundred years. They continue to be a primary tool for science and technology. The height of compound microscopes usually exceeds 16 inches and is often much larger. A sample must be positioned on a stage and mechanical devices are required so each person using the microscope can adjust the focus for his/her eyes. People requiring corrective eyeglasses often have difficulty using eyepiece lenses. Special “high eyepoint” eyepieces might be required. 
   Light microscopes have magnifications that range from 5 to 2,000 times. Most of this magnification is produced by the objective lens that typically has a magnifying power range from 0.5 up to 160 times. The objective lens projects an image 160 mm or more (infinity corrected systems use 180 mm telan lenses to form the primary image) from the objective lens. This projection distance (or tube length) combined with the eyepiece lens is a major factor which establishes the physical size of the microscope. Eyepiece magnifications range from 5 to 20 times, and since the eye must be placed closer to the lens of a high magnification eyepiece, higher magnification eyepieces are difficult to use. A 10 times eyepiece is common, while the majority of light microscopy applications use magnifications between 10 and 500 times. 
   Video microscopy has been a useful technology for several decades to extend the capability of the compound light microscope. The early uses are documented by Inoue&#39; in  Video Microscopy , Plenum Press, New York, 1986. The most common implementation of video microscopy is to attach a video camera to the accessory port on a trinocular viewer. While several types of video cameras were used for video microscopy, the current state-of-art is to use solid-state charge coupled devices (CCD). For low light levels, cooled CCD video cameras are used because of their increased sensitivity. These cameras are very expensive, but have demonstrated unique sensitivity for certain biological applications. The most common uses of video microscopy are to supplement visual observations, record images and provide digital images for image analysis using a digital computer. 
   When using a compound microscope for photography or video microscopy, a camera apparatus replaces the eye. These cameras contain an additional lens to project a real image onto the film or electronic video-imaging device. Video camera accessories require a special eyepiece lens to reduce the effects of the electronic scaling. In all cases, adding photographic or video cameras increases the size, complexity and cost of the compound light microscope. The addition of a video camera to a compound light microscope can add six to ten inches. 
   Video cameras have been incorporated into microspectrometer systems for electronic imaging. The system disclosed in U.S. Pat. No. 5,581,085 (Reffner and Wihlborg) used a built-in video camera to generate an electronic image for sample viewing and image recording. Several micro-Raman spectrometer systems use video imaging to protect the viewer from exposure to the laser radiation that is used to generate the Raman spectra. All of these systems use the principles of the compound light microscope with an objective lens, one or more intermediate lenses and a video camera. These video microscope systems use conventional microscope optics with long tube-lengths and add-on video cameras. The standard tube-length is 160 mm (6.3 inch) and the addition of a video imaging system can more than double this length. 
   Combining microscopes with spectroscopes, spectrometers or spectrographs to provide spectrochemical analysis of small objects or small features of objects has a history of over 125 years (Ford,  Single Lens, The Story of the Simple Microscope , Harper &amp; Row, New York, 1985). The early microspectrometers were combinations of visible light microscopes and dispersive spectrometers used for color analysis. In 1949, the first uses of infrared radiant energy in microspectroscopy were reported by Gore, R. C.,  Science,  110, 70 (1949) and Barer et al,  Nature,  163, 198 (1949). In 1953, the first commercial, infrared microspectrometer accessory was produced (Coats et al,  J. Opt. Soc. Am,  43, 984, (1953). It was not until the development of Fourier transform infrared (FT-IR) spectrometers that infrared microspectroscopy became a practical technology. The first microscope accessories for FT-IR were introduced in 1983. The design of these accessory microscopes followed the general teachings and design of the compound light microscopy for imaging and spectral measurements. 
   The wavelength (lambda) of radiation and objective lens aperture limits the spatial resolution of all microscopes. This diffraction limited spatial resolution (d) for a microscope with a limiting numerical aperture (N.A.) is d=(0.62 lambda/N.A.). As the diffraction limited spatial resolution value becomes smaller, the resolving power of the microscope becomes higher. In video microscopy, the resolution element of the photo detector array is an additional factor that can limit resolution. To meet the Nyquest limit, two picture elements are required for a specified resolution to be recorded. 
   Radiant energy in the mid-infrared range (2.5 to 25 micrometers) is the most useful for the analysis of molecular compounds like organic substances, certain ionic salts and silicate minerals. In this spectral range, the conventional diffraction limited spatial resolution is generally considered to be about 10 micrometers. 
   To improve spatial definition of the sample area in infrared microspectrometry, Messerschmidt and Sting (U.S. Pat. No. 4,877,960) applied the principles of confocal microscopy. In this development, a pair of image plane masks was used to achieve the confocal geometry as introduced by Minsky (U.S. Pat. No. 3,013,467). Using masks, however, adds complexity and cost to microscopes that are used for infrared microscopical analysis. 
   Internal reflection microanalysis is achieved by reducing the area of the sample contacting the internal reflection element (IRE) as revealed by Sting and Reffner (U.S. Pat. No. 5,172,182). The teachings of Sting (U.S. Pat. No. 5,093,580) reveals a reflecting ATR microscope objective and a mechanical slider containing aperture masks to select different optical paths through an attached IRE. The ATR objective requires shifting aperture masks between viewing a sample through the IRE and recording its ATR spectrum. By selecting different optical paths, it is possible to collect ATR spectra, observe sample contact or see the sample. While microanalysis with the ATR objective was made easier by these three modes, they added significant cost and complexity. 
   SUMMARY OF THE INVENTION 
   The invention relates to a miniaturized opto-electronic image magnifying system, i.e. a system for producing enlarged images of objects in which part of the magnification is provided by one or more lenses or other optical elements and the balance is provided by an electronic scaling system. This miniaturized opto-electronic system is comprised of a lens or lens system such as a variable focal length zoom lens (as used herein, the term “lens” is intended to encompass both single lenses and systems with multiple lenses, such a compound lenses and zoom lenses), an array of solid-state photo-detectors, and electronic circuits that provide input to electronic display apparatus such as a television, video monitor or computer monitor screen. The lens or lens system projects a magnified real image of an illuminated or luminous object, or some portion thereof, directly onto the small solid-state photo-detectors, which produce an electronic signal that is representative of the magnified real image projected on the photo-detectors. This optical image is then further enlarged electronically when it is displayed on the display screen. The image focus on the detector is the same for all individuals viewing the screen. Seeing the image on a screen is convenient and viewers can wear their corrective glasses as needed. 
   The core of this invention is the combination of a lens or lens system with a small solid-state photo-detector. This combination is referred to in this application as a miniaturized opto-electronic magnifier (MOM) module. The. miniaturized opto-electronic image magnifying system of this invention eliminates the need for conventional microscope objectives and eyepieces by using the MOM module in combination with a video display monitor. It thereby regains the benefits of the Leeuwenhoek microscope, such as compact size and simple optics, while eliminating its major problem of forcing the observer to be near both the eyepiece lens and the object under observation. Using our invention, the eye is moved from near the lens of the Leeuwenhoek microscope to a location of comfortable viewing of a computer monitor or television screen. While neither the idea of viewing a projected magnified image on a screen nor the adaptation of a video camera to a microscope is new, our invention&#39;s novelty make it possible to magnify images of objects in a uniquely simple and unexpected way that provides “visual access” not previously available at affordable prices. 
   The MOM module is substantially smaller than standard compound light microscopes, which typically have a tube-length of 160 mm. The size of our MOM modules is reduced by selecting the appropriate focal length lens combined with a small photo-detector array to achieve the desired magnification. The small MOM module, which may have an overall height of about 25 to about 100 mm, can be placed within devices to produce magnified images that can be observed remotely on a separate video-monitor screen. 
   The total magnification of this opto-electronic image magnifying system is the product of the optical magnification and the electronic scaling. For most systems, the electronic scaling will be from about 20 to about 100 times, whereas the optical magnification by the lens or lens system will be about 2 to 20 times. The optical magnification will more typically be about 2 to about 10 times, and even more typically about 2 to 5 times. Thus, the majority, but not all, of the magnification typically results from the electronic scaling. In preferred combinations, the electronic scaling be the major component to the overall magnification, and the optical magnification will be the minor component. The ratio of the magnification provided by electronic scaling and the magnification provided by optical magnification will generally be between about 1.5 to 1 and 30 to 1, and will more typically be between about 4 to 1 and about 10 to 1. 
   The miniaturized opto-electronic magnifying system of this invention eliminates the need to look through a microscope eyepiece and objective lens system or to incur the significant cost of a video camera coupled to a compound microscope system. Instead, the magnified electronic image is seen solely on the monitor screen without using an associated compound microscope. The system alone provides significant benefits in the form of very small, low cost magnifying systems such as inverted microscopes and the like, for viewing insects, soil, plants and minerals. When coupled with other sensing technologies such as FT-IR or Raman spectroscopy, even more dramatic benefits result from seeing samples that are being analyzed, such as defects in packaging materials or analyzing trace forensic evidence. 
   A preferred embodiment of this invention allows continuous viewing of a magnified image of the sample and simultaneous collection of ATR spectra by internal reflection spectroscopy. This makes the internal reflection apparatus more stable and easier-to-use while lowering cost. Viewing the sample through the IRE has special value in microanalysis, providing visual confirmation of what object or feature is being analyzed. Internal reflection is very useful for spectral analysis of polymers and other organic objects and is particularly useful for analyzing surfaces of thick, opaque materials. Locating areas for spectral analysis on thick opaque samples requires looking through the IRE. 
   Another preferred embodiment of this miniaturized opto-electronic magnifying system is for use with commercial FT-IR spectrometers for internal reflection spectral analysis. The MOM module fits within an internal reflection accessory providing magnified images of the sample (object) while it is being analyzed by infrared spectroscopy. The internal reflection accessory is mounted in the sample compartment of a general purpose FT-IR spectrometer. The space limitations of the spectrometer&#39;s sample compartment restrict access for normal viewing of the sample through the internal reflection element (IRE). A MOM module placed within the internal reflection accessory makes it possible to look through the IRE and see material contacting the IRE. While the viewing light path and the internal reflection radiant energy path are separate in the internal reflection element, their paths converge on the same point on the sample. Because these optical paths are separate, the sample can be visually observed simultaneously with the recording of its infrared spectrum. 
   In another form, the MOM module of this invention is incorporated in a spectrometer system dedicated to internal reflection microanalysis. Either the internal reflection imaging accessory or the dedicated system is able to use a plurality of single or multiple reflection IRE&#39;s. This unique combination of magnified video observation and internal reflection FT-IR microspectroscopy results in a simple, inexpensive apparatus which can be used to analyze a wide range of materials including organic compounds, drugs, plastics, paint, and most minerals. 

   
     DRAWINGS 
     The invention will be described now by way of example only, with particular reference to the accompanying drawings, wherein: 
       FIG. 1  is a schematic drawing of the current state of art of the conventional compound light microscope used for direct viewing of a magnified image showing the principal elements; 
       FIG. 2  is a schematic drawing of the current state of art in video microscope technology showing the principal elements; 
       FIG. 3  is a schematic drawing of the miniaturized opto-electronic magnifying system of the present invention showing the principal elements; 
       FIG. 4  is a block diagram of the miniaturized opto-electronic magnifying system outlining the component parts used in implementing a system in accordance with the present invention; 
       FIG. 5  is a schematic drawing showing the miniaturized opto-electronic magnifying system of the present invention placed in an internal reflection accessory used for infrared spectral analysis. A magnified image of the sample, placed on the internal reflecting element, is displayed on a video-monitor screen; 
       FIG. 6  is a schematic drawing showing the miniaturized opto-electronic magnifying system of the present invention in an inverted microscope, which produces magnified images of small objects on a TV monitor; 
       FIG. 7  is a schematic drawing showing the miniaturized opto-electronic magnifying system of the present invention placed in a sample compartment of an FT-Raman spectrometer to produce magnified images of the sample being analyzed; 
       FIG. 8   a  is a schematic drawing showing the miniaturized opto-electronic magnifying system of the present invention placed in an ATR probe apparatus for viewing an area of an internal reflection element with controlled infrared illumination of the analyte area for ATR spectral measurement; and 
       FIG. 8   b  is an expanded view of the probe tip in  FIG. 8   a , provided by the miniaturized opto-electronic magnifying system in the ATR probe apparatus of that Figure. 
   

   DETAILED DESCRIPTION 
     FIG. 1  shows the principal elements of a conventional compound light microscope used for direct viewing of an optically magnified image. The conventional compound light microscope consists of an illumination source  1 , a mirror  2  directing the light into the condenser lens  3  that directs the light to illuminate an object  4 . Objective lens  5  projects a real image  6  of the illuminated object into an eyepiece lens  7 , eye  8  views a virtual image  9  and an eye lens  10  forms a real image  11  of the object on the retina  17 . 
   The present art for converting a compound light microscope into a system for electronic imaging, shown in  FIG. 2 , is to replace the eye  8 , of  FIG. 1 , with a video camera  12  consisting of a lens  13  and an electronic imaging element  14 . The video camera is usually mounted in a separate port to retain normal direct viewing through conventional eyepiece lenses. The electronic image is displayed on a video-display screen  15 . 
   While compound light microscopes have been built in many shapes and sizes, the microscope of today is a large, complex, versatile scientific instrument. The mechanical distance from the objective lens mount to the seat of the eyepiece lens it called the mechanical tube length  16 . The standard light microscope has a tube-length of 160 mm or longer. The addition of a video accessory to a conventional compound light microscope adds size and complexity. 
   Electronic imaging has had a major impact on conventional microscopy, especially in the field of electronic image analysis and increased sensitivity to detection of small contrast differences. Those skilled in the art will appreciate the manor in which such a microscope operates and a full explanation of this operation is not required for purpose of understanding the present invention. 
   This invention reduces the size and complexities of a microscope so it can be used to observe objects that are inaccessible or too costly to inspect with a conventional microscope. As noted above, the core of this invention is the miniaturized opto-electronic image magnifier module, i.e. the combination of a lens with one or more arrays of small solid-state photo-detectors. The photo-detectors may be a component of a charge-coupled (CCD) camera. They may also be part of a simple board camera, i.e. a printed circuit or other board on which the photo-detectors are mounted, with circuitry that produces a signal that is representative of the image on said photo-detectors. A ¼ inch CCD camera and a 12 mm focal length lens is an example of a MOM module. 
   With reference to  FIG. 3 , the lens  31  forms a real image of a luminous or illuminated object  32  onto a solid-state photo-detection array  33 . Since the object may be either transparent or opaque, two visible light illumination sources  38  and  39  are provided. Lens  31  and photo-detector array  32  form the MOM module. Each element of the array detector contains a pixel of the magnified image. The electronically generated signal from the MOM module is processed by an electronic circuit  34  and a magnified image is displayed on a video-monitor  35 . In many systems, photodetector array  32  and electronic circuit  34  will be combined in a system such the CCD camera mentioned above. However, for certain applications, e.g. when a MOM module is placed within compact apparatus such as Fourier transform spectrometers, thermal analysis systems and miniaturized probes for visual inspection, the photo-detector arrays  32  may be combined with lens  31  to form the MOM module, and electronic circuit  34  may be located at another, convenient location, as illustrated in FIG.  3 . In applications of this sort, board cameras may be particularly advantageous. 
   Miniaturized solid-state charge coupled device (CCD) video cameras are used in this invention to produce a miniature scale alternative to a microscope. Commercial CCD video cameras (such as CHUGAI BOYEKI (America) Commack, N.Y. 11725, Model CEC100) are compact and have ¼ inch CCD elements. This camera has a small size, 1.25 inches square (3 boards) by 1.0 inch height. The CCD has 512 horizontal (H)×492 vertical (V) elements and its scanning size is 3.69(H)×2.76(V) mm. This camera has a TV line resolution of 330(H)×330(V). 
   This CCD camera illustrates the principle of electronic scaling. An image formed on the CCD solid-state array is displayed on a monitor screen. If the monitor&#39;s screen horizontal (H) size is 10 inches (254 mm), then 254/3.69=68.8 is the electronic scaling factor for this system. If a lens or lens system formed an image magnified 3 times on the CCD element, then the image seen on the monitor would be magnified 3×68.8 or 206.4 times. As may be readily appreciated, electronic scaling is a major element of this invention. 
   It is possible to use other miniature video cameras with different geometry, size of CCD solid-state array and other video monitors. In order to match commercially available lenses that are well suited for this invention, the camera, or other solid-state photo-detector array, should be less than 1 inch wide (measured along the diagonal), have a density of pixel elements equal to the monitor screen resolution and detect a minimum luminance of less than 50 lux. 
   A lens is used in combination with a CCD solid-state array to form a miniature opto-electronic magnifier (MOM) module of the miniaturized opto-electronic magnifying system of this invention. The lens produces an image of specific size and resolution to achieve a desired magnification in the final electronic image. The magnifying power of the lens is calculated as the ratio of the image to object size. The image size equals the size of the CCD solid-state array. Using the CCD solid-state array and monitor described above, the lens magnification and resolution are calculated for a final magnification of 3×68.8=206.4 times. The total magnification equals the product of the optical magnification and electronic scaling factors, so in this example the optical magnifying power is 3 times. For this CCD solid-state array, the horizontal dimension is 3.69 mm. The maximum object size for a three times magnification is 3.69/3=1.23 mm. This 1.23 mm object is imaged onto 512 elements, therefore each CCD array element has an image element size equaling 1.23/512=0.0024 mm (2.4 microns). For the optical resolution to equal the electronic resolution, the lens must produce an image with a resolution of 2.4 micrometers. This means that the numerical aperture (NA) of the lens must satisfy the Abbe resolution criteria that d=wavelength/NA, wherein d is the minimum distance of separation that can be detected. For visible light this relation is NA=(0.5 E-3)/d, which in this example d=2.4 E-3 and NA=0.208. 
   The total magnification of this opto-electronic system is the product of the optical magnification and the electronic scaling. The optical magnification is the ratio of the object distance  36  to the image distance  37 . The electronic scaling is the ratio of the size of the video-monitor screen  35  to the size of the photo-detector element  33 . The majority, but not all, of the magnification typically results from the electronic scaling. 
   Table 1 lists properties of exemplar commercial lenses that are readily available that can be used to achieve the desired magnification, resolution and small total MOM module length. In order to match commercially available solid-state photoelectric array detectors, and achieve the advantages provided by this invention, the lens should be a single lens or lens system, with fixed or variable focal lengths (zoom lens system) and capable of producing an optical magnification of up to 20 times. The lens focal lengths should be in the range between 2 and 50 mm. 
   
     
       
             
           
             
             
             
             
             
             
             
           
         
             
               TABLE 1 
             
           
           
             
                 
             
             
               Commercial Lenses for MOMs 
             
           
        
         
             
               Optical 
                 
                 
               Lens 
               Object 
                 
                 
             
             
               Magnifi- 
               Focal 
               Resolu- 
               Aperture 
               Dis- 
               Image 
               Total 
             
             
               cation 
               Length 
               tion* 
               (NA) 
               tance 
               Distance 
               Length 
             
             
                 
             
             
               2 
                8 
               0.0048 
               0.1138 
               12.00 
               24.00 
               36.00 
             
             
               2 
               12 
               0.0048 
               0.1138 
               18.00 
               38.00 
               54.00 
             
             
               2 
               25 
               0.0048 
               0.1138 
               37.50 
               75.00 
               112.50  
             
             
               3 
                8 
               0.0024 
               0.2275 
               10.67 
               32.00 
               42.67 
             
             
               3 
               12 
               0.0024 
               0.2275 
               16.00 
               48.00 
               64.00 
             
             
               3 
               25 
               0.0024 
               0.2275 
               33.33 
               100.00  
               133.33  
             
             
               4 
                8 
               0.0012 
               0.4550 
               10.00 
               40.00 
               50.00 
             
             
               4 
               12 
               0.0012 
               0.4550 
               15.00 
               60.00 
               75.00 
             
             
               4 
               25 
               0.0012 
               0.4550 
               31.25 
               125.00  
               156.25  
             
             
                 
             
             
               Distances for focal length, object distance, image distance and total length are in millimeters.  
             
             
               *Resolution is calculated for a CCD with 512 elements on a 3.69 mm (H) width.  
             
           
        
       
     
   
   As noted above, in most preferred combinations the electronic scaling will be the major component of the overall magnification, and the optical magnification will be the minor component. For a system using a 20-inch monitor and with a 0.25-inch solid-state array in the MOM module that produces a total magnification of 400 times, the electronic scaling component is 80 times and the optical magnification component is 5 times. In this example, the electronic scaling is 16 times greater that the optical magnification. This is in direct contrast to the conventional compound light microscope where all magnification is optical and the objective lens generally produces the bulk of the magnification. Since the optical magnification in the MOM module is typically less that 20 times, the lenses are less costly and require fewer lens elements to correct for aberrations. 
   Small element solid-state photo-detectors, such as CCD board cameras, were developed for commercial use in hand-held camcorders and security surveillance cameras. The elements are available in nominal sizes from, ¼ to ½ inches. Conventional ¼ inch cameras have arrays measuring about 3.96 mm horizontal (H) by about 2.79 mm vertical (V). The screen size of video monitors range from 5 to 20 inches and home video screens are available up to 48 inches wide. The electronic scaling can be very high. Presently, much of this electronic scaling is “empty magnification” in that the resolution is limited by pixel size and monitor screen resolution. Empty magnification is enlargement that exceeds the resolution of details; the image is larger but it does not reveal new details. Current video technology limits resolution, and hence the real total magnification of the miniature opto-electronic magnifying apparatus of this invention to 500 or less. However, the development of high definition TV, and future advances in video technology will raise the magnifying value to the optical diffraction limits for light microscopes and magnifications of 1,000 or more will be achievable. 
   In addition to providing electronic scaling, the solid-state photo-detectors are very sensitive and low levels of light intensity produce high quality images. In this invention, the increased sensitivity is used to simplify and reduce the cost of illuminators. Ambient lighting is sufficient for many applications. In other cases, low wattage lamps provide sufficient light. 
   In its generalized form, the MOM module unit of this invention is one component of the miniaturized opto-electronic magnifying system. Referring to the block diagram of the system,  FIG. 4 , the MOM module  41  is positioned to view an object  42  which is illuminated by sources  43  or  44 , the electronically signal from the MOM module  41  is transmitted to a video monitor  45  or computer  46 . In addition a video recorder  47  and, or a printer  48  are examples of additional components which may be added to document magnified images. 
   The currently available miniature board cameras generate NTSC, PAL or S-video output. It is expected that these commercial video standards will change to improve TV quality, which will extend the applications of this invention. 
   This invention provides miniaturized opto-electronic magnifying systems that are suitable accessories for internal reflection, infrared spectroscopic analysis. The internal reflection apparatus by ASI SensIR Technologies manufactured and sold as the DuraSamplIR™ is used as an example, however this invention is not limited to this.  FIG. 5  is a schematic drawing of a miniaturized opto-electronic image magnifier module of this invention mounted within the body of the DuraSamplIR. 
   Referring to  FIG. 5 , infrared radiant energy  51  from a spectrometer  50  is directed by mirror  52  onto a zinc selenide (ZnSe) element  53  that transmits the infrared radiation through the diamond window  54  mounted in a fixture  55 . At the diamond surface  56  the radiant energy is internally reflected so that it returns through the diamond window  54  and ZnSe element  53  and is directed towards mirror  57  which then directs it to a detector  58 . A visible light source  500  illuminates surface  56  and this light is transmitted through the diamond window  54  and ZnSe element  53  where it is collected by lens  501  and the image of surface  56  is formed on the solid-state photo-detector  502 . In  FIG. 5 , items  501 ,  502  and  504  are the MOM module  503 . The electronic signal produced by the photo-detector is processed by the camera electronics  504  and the electronic signal is sent to a video-monitor  505  for viewing the magnified image of surface  56 . The image on the video-monitor screen is magnified. The image may have the same geometrical orientation as the sample and movements left-to-right and up-and-down are the same for sample and image. The electrical power for the camera is provided by the power supply  506 . For opaque samples, a visible light illuminator  507  is positioned below the ZnSe element  53 . Because of the high sensitivity of the CCD photo-detector, low wattage illumination is all that is required. 
   In this form, a CCD element ¼ inch is preferred with a 12 mm focal length lens. With this combination in a DuraSamplIR, the IRE measuring 1.5 mm will be magnified to fill the monitor&#39;s vertical screen size. 
   Internal reflection spectroscopy is a very important method because it produces ATR infrared spectra to analyze liquid or solid samples without the need for extensive sample preparation. Optical contact between the internal reflection element (IRE) and the sample is the only requirement. The use of small IRE&#39;s was a major advance in internal reflection spectroscopy. Small contact surface makes analysis of solids more reproducible and quantitative. In transmission measurements in the mid-infrared spectral range, samples must be thin (0.03 mm or less) and uniform. This requires special care in preparing a sample for analysis. In internal reflection, the sample thickness is established by the wavelength of the radiation, the angle of incidence and the difference in refractive index between sample and IRE. Large IRE elements are useful for quantitative analysis of liquids, but not for solids. Only when small IRE&#39;s are used can reproducible contact be made with solid samples. This invention makes it possible to see the contact of solid sample on small IRE surfaces. Seeing this contact improves the reproducibility of analyses while assuring the analyst that the correct sample is analyzed. 
   This invention also provides a simple video imaging system for inspection of objects at magnification. In this implementation, a fixed focus miniature opto-electronic magnifying apparatus is produced such that any object placed on its viewing port appears magnified on a monitor, computer terminal or TV.  FIG. 6  is a schematic drawing showing the incorporation of the miniaturized opto-electronic magnifying system in a fixture for examination of or opaque objects. In  FIG. 6 , fixture  60  is a mechanical enclosure with a viewing port  61  supported by the enclosure. Viewing port  61  is a transparent, scratch resistant material with flat polished surfaces. While glass and some plastics may be used for the viewing port, quartz and sapphire are preferred scratch resistant transparent materials. Lens  62  forms a real image of the outer surface of viewing port  61  onto the photo-detector element  63 . Lens  62  is selected to have the focal length and numerical aperture to produce the desired magnification and resolution. Multiple lenses on rotating disks or sliders could be used as well as zoom lens systems for variable magnifications. The photo-detector  63  is a CCD or other solid-state video camera electronics  64  that produces an electronic signal to a video monitor  65 . The electrical power for the camera is supplied by power supply  68 . The sample is placed on the viewing port surface  61  for inspection. The sample is lighted up by illuminators  66  and, or  67 . For general use, a total magnification from 5 to 200 times is most practical, but a total magnification up to 1,500 is possible. 
   In this embodiment, the miniaturized opto-electronic magnifying system would have no moving parts other that possible changing magnifications. The sample would be placed on the viewing port and examined on the monitor. The magnified image could be recorded on standard video recorders or imported to a computer through a video port. In this form, this invention is expected to have applications in teaching and industrial inspection. 
   FT-Raman spectrometers provides another example where inserting the miniaturized opto-electronic magnifying system of this invention into a spectrometer sample compartment has unique advantages. In FT-Raman, intense lasers with invisible near-infrared wavelengths (i.e. 1064 nm) are used to excite Raman spectra. If viewed directly these beams can cause serious damage to eye tissue. Since the laser beam is small, viewing the sample is important so that the laser beam can be positioned on the desired area. With inhomogeneous solids, it is critically important to see what the laser is focused on. 
     FIG. 7  is a schematic drawing showing the miniaturized opto-electronic magnifying system of the present invention placed in a sample compartment of an FT-Raman spectrometer to produce magnified images of the sample being analyzed. Referring to  FIG. 7 , a laser beam  70  passes through a small opening in an aspherical mirror element  71  and is incident on a sample  72  contained in a glass tube  73 . The laser radiation  70  is Raman scattered and the scattered radiation  74  is collected by the aspherical mirror  71 . This mirror directs the Raman scattered radiation into the Fourier-transform spectrometer  75 . Lens  76 , solid-state photo-detector array  77  and camera electronics  78  comprise the MOM module  79 . The sample may be lighted up by illuminator  700 . The electronic image is sent to the video-monitor  701  to display a magnified image of the sample. The electrical power for the camera is provided by power supply  702 . The mirror  71 , sample  73 , sample container  72 , MOM module  79  are all contained inside the sample compartment ( 703 ) of the FT-Raman spectrometer. 
   Sample compartments of Raman spectrometers are small but the MOM module can be fitted inside to view the sample positioning in the laser beam. The small size is an important factor. The sample can be view at magnifications between 10 and 200 times and the near-infrared laser beam is weakly detected by the solid-state photo-detector array. In this embodiment, it is necessary to modify the sensing element. The standard configuration of silicon based CCD camera used for normal visible light imaging is to have a near-infrared blocking filter positioned over the devise. For the Raman application, it is necessary to remove this filter from the CCD camera. 
   Another objective of this invention, the MOM module is incorporated into an ATR probe to provided a magnified image of the contacting surface between the internal reflection element and the sample. In this embodiment an image plane mask restricts the area of the interface irradiated with infrared radiation. This system also has coaxial visible illumination to provide a means to see the area of the sample being analyzed using the MOM module.  FIGS. 8   a  and  8   b  are schematic drawings of an ATR probe accessory apparatus that illustrates this application. Infrared radiant energy  80  from a spectrometer  79  is reflected from mirror  81  to mirror  82 . The infrared radiation is focused by mirror  82  on to a variable mask  83  and then continues on to mirror  84 . Mirror  94  redirects this beam on to the composite ZnSe-diamond IRE  85  mounted in a fixture  101 . At the surface  86  of the diamond  100 , the radiant energy is internally reflected. After reflection from the IRE-sample interface  86 , the IRE element directs the infrared radiation back to mirror  84 . On reflection from mirror  84 , the infrared radiation is again focused on to variable mask  83  and continues to mirror  82 . From mirror  82  the beam is directed to mirror  87  and then to an infrared radiant energy detector  88 . The sample is lighted up with visible light from illuminator  89  when mirror  90  is positioned in the infrared beam path with a mechanical means  91 . The visible light is coaxial with the infrared, passing through the variable mask  83 , and is then redirected to the IRE-sample interface  86  by mirror  84 . From mirror  84  the visible light is directed on to the transparent internal reflection element  85  to illuminate the sample area defined by the variable mask  83 . A magnified image of the illuminated sample-IRE interface is produced by reflecting the light from mirror  92  in to a MOM  95  comprised of lens  93 , photo-detector array  94  and electronic interface  97 . The electrical signals are displayed on the video-display screen  96 . The electrical power for the camera is provided by power supply  98 . This probe apparatus has uses in extending the analysis by ATR into containers, analysis of biological growths on surfaces or materials on production lines. 
   Thus, the novel miniaturized opto-electronic magnifying system presented in this invention has achieved the above stated objectives and eliminates difficulties encountered in the use of prior devices and system, solves problems, reduces cost and obtains the desirable results described herein. 
   In the forgoing description, certain terms have been used for brevity, clarity and understanding, however, no unnecessary limitations are to e implied therefrom because such terms are for descriptive purposes only and are intended to be broadly construed. Moreover, the descriptions and illustrations are by way of examples and the invention, which is defined by the following claims, is not limited to the details shown and described.