DARK FIELD, PHOTON TUNNELING IMAGING SYSTEMS AND METHODS

Abstract: A dark-field imaging system and method is disclosed that employs photon tunneling to visualize and measure submicron features of reflecting or transmissive materials within the subnanometer-to-several-micron range. The system comprises an illumination section for providing an evanescent field, where the evanescent field is selectively scattered by the surface of the reflecting or transmissive material, and a collection section for transmitting the radiant energy produced by the evanescent field scattering to an imaging section, which may may be a vidicon, digital camera, or other photo detector device. Various embodiments are disclosed including the use of a bulk optic prismatic element, the forward aplantic element of a compound microscope objective, diffracting gratings, and optical waveguides. In each embodiment the collection section and illumination section may be completely optically, and thus physically, uncoupled.

Description: TITLE: DARK FIELD, PHOTON TUNNELING IMAGING SYSTEMS AND METHODS BACKGROUND OF THE INVENTION 1. Field Of The Invention This invention in general relates to the fields of imaging and metrology of surfaces and, more specifically, to systems and methods that use evanescent field illumination in real-time, whole-field imaging and measurement of surfaces at low magnification and at wide angle. 2. Description Of The Prior Art Photon tunneling microscopy for measuring and visualizing submicron surface topographic features is known. The prior art discloses whole-field reflected evanescent light microscopes where the sample is not transilluminated nor scanned, but rather is illuminated by an evanescent field from an unrestricted total reflection surface at the object plane of an epi, or reflected light, illuminator. Here, the sample can be opaque or transparent, thick or thin, and can be viewed in real-time with high energy throughput. Such microscopes are very sensitive to smooth surfaces because of their use of the exponentially- varying amplitude of the evanescent field in the vertical direction to sense very small surface height variation. On the other hand, rougher surfaces scatter light back into the microscope, which decreases contrast and sensitivity. Also, the deeper topography is rendered as bright, because these areas penetrate the evanescent field to a small degree so that the epi-illumination is nearly totally reflected. The difficulty in detecting and measuring small changes in bright scenes limits the observable topographic depths to about 3/4 of the illuminating wavelength (which is the wavelength in air divided by the index of refraction, «, and the sine of the angle of incidence, θ). Further, the illumination and imaging optics are coupled because the objective serves as the condenser as well. This limits in a practical sense the use of such instruments to the availability of suitable commercial objectives, magnifications, fields of view, and numerical aperture. In addition, it is difficult, because of the coupling of imaging and illumination optics, to affect the polarization, phase, incident angle, and direction of the illumination. This, in turn, restricts the ability to maximize the tunneling range, increase lateral resolution, or tunnel through less rare media such as water in biological applications. There are also disclosed in the prior art optical evanescent light field microscopes in which the light that enters the objective pupil is evanescent field light that has been scattered from a sample surface. However, in all of these microscopes, the sample is transilluminated, with the illumination incident at beyond the critical angle such that the evanescent field from the sample surface is received. It is then necessary that the sample be transparent at optical frequencies, or is made thin enough to be transparent. While the art describes a variety of devices that utilize evanescent field illumination for investigating surface characteristics, there remains a need for improvements that offer advantages and capabilities not found in presently available instruments, and it is a primary object of this invention to provide such improvements as will become apparent when reading the detailed description which follows. SUMMARY OF THE INVENTION This invention generally relates to the fields of surface imaging and fine detail measurement through the application of evanescent field illumination and, in particular, to methods and apparatus by which bound evanescent field illumination may be converted by scattering into propagating light that is collected and imaged for subsequent display and metrology purposes. Various embodiments of dark-field, photon tunneling imaging systems and methods of providing the necessary evanescent field illumination are disclosed. Using a dark field photon tunneling imaging system in accordance with the presnt invention, a sample is illuminated by the evanescent field and scatters the bound energy in accordance with its scattering properties. The scattered light is collected and imaged where the intensity variation of the image varies in accordance with the surface details. Image intensity is correlated with calibrated geometry to provide a means for encoding the intensity variations as variations in gray tones. The intensity of the image is mapped to a gray tone image in the form of a signal which bears tone density corresponding directly to surface feature dimensions. The gray tone signal thereafter may be used as an input to a number of display possibilities including digital monitors, 3-D oscilloscopes, or other forms of display. In a conventional photon tunneling microscope (PTM), the evanescent field is converted into propagating light by refraction into smooth surfaces and away from the entrance pupil of the microscope. Where there is no sample surface provided to the conventional PTM, the light is reflected totally into the microscope entrance pupil and presents a bright field. In contrast, when there is no sample surface provided to the dark field PTM, light is reflected totally outside of the entrance pupil of the imaging system and thus creates a dark field, from which the "dark-field" name is obtained. In addition, the dark field PTM differs from conventional dark-field microscopy in that the illumination is evanescent light, and not propagating light. Thus, as a surface feature increases in height, the feature appears more bright against the dark background. In a conventional dark field microscope, the brightness of a sample feature is a function of its size and slope, rather than of its height. In general, the inventive imaging systems are best used on samples that are scattering and rougher since very smooth surfaces scatter very little light energy into the pupil. On the other hand, these systems are less sensitive to the optical properties of the sample because the conversion of the evanescent field is largely by scattering, rather than by diffraction or refraction. Also, the imaging and illumination optics and optical paths are easily decoupled from one another so that the polarization, phase, incident angle, and wavelength of the illumination is easily controlled. And, because the imaging optics are separate and do not require a numerical aperture of one or greater, a much larger range of magnifications, fields of view, and numerical apertures are available. BRIEF DESCRIPTION OF THE DRAWINGS The structure and operation of the invention, together with other objects and advantages thereof, may best be understood by reading the detailed description in connection with the drawings in which unique reference numerals have been used throughout for each part and wherein: Fig. 1 is a diagrammatic partially elevational and partially perspective view of a dark- field, photon tunneling system of the invention; Fig. 2 is an enlarged, diagrammatic, elevational view of a portion of the system shown in Fig. 1 ; Fig. 3 is a flow chart illustrating the operation of various embodiments of the invention; Figs. 4a-4d are diagrammatic views illustrating how light may be scattered into the entrance pupil of the detection section of the embodiments of the invention depending on whether or not there is a scattering sample present and the corresponding images that may be observed on the display section; Fig. 5 is a diagrammatic view of an alternate embodiment of the invention in which a microscope is used to view through an aplanatic sphere to image scattered light; Fig. 6 is a diagrammatic, enlarged elevational view of a portion of the embodiment shown in Fig. 5; Figs. 7, 8, and 9 are diagrammatic illustrations in which a decoupled light source, objective, and detector camera are arranged for use in another embodiment of a dark field photon tunneling imaging system according to the invention; Figs. 10 through 24 are diagrammatic views illustrating variations of transmissive body geometries that can be used as the total internal reflection element for the invention; Figs. 25 through 30 are diagrammatic views of mounting arrangements in which the imaging section a dark field photon tunneling system comprises one pod in a three pod kinematic base for a portable surface profiler; Fig. 31 is a diagrammatic illustration of a viewing section of a dark field photon tunneling system that has been inverted to form yet another embodiment of the invention; Figs. 32a-32c are diagrammatic views showing a dark field photon tunneling microscope mounted as a spring-loaded piston in the center of a kinematic three point ring, in both an inverted as well as upright configuration; Fig. 33 is a diagrammatic illustration of a dark field photon tunneling microscope configured and used as a hand-held device that is placed in contact with the sample; Fig. 34 is a diagrammatic illustration of the dark field photon tunneling technique applied to measuring flying height of a magnetic data recording head in a typical drive arrangement for floppy or rigid disk magnetic media; Fig. 35 is a diagrammatic illustration of a dark field photon tunneling technique applied to high resolution writing and reading of optical data in an optical data drive; Fig. 36 is a diagrammatic view showing how the coupled imaging and illumination optics of a typical photon tunneling microscope can be modified for dark field photon tunneling microscopy; and Figs. 37 and 38 show representative displays of 3-D and gray scale images, profilometry, and roughness statistics such as are available from the dark field photon tunneling microscope. DETAILED DESCRIPTION Reference is now made to Fig. 1 which shows a dark field, photon tunneling imaging system designated generally at 10. As will be seen, system 10 is particularly suitable for visualizing and measuring at full field and in real time the microtopographic features of roughened or other surfaces that have small scattering features but which otherwise appear smooth. In particular, system 10 and other embodiments of the invention are suitable for use in measuring the surface characteristics of aircraft and space vehicle structures, paint, paper, and fabrics. Because of the lighting and detecting mechanisms employed in dark field imaging, it is possible to decouple the illumination and imaging paths so that probes remote from the imaging sections can be contrived. System 10 comprises an illumination and imaging section 12 and an image processing and display section 14. Section 14 may be any well-known general purpose computer or work station 16 having a CPU, RAM memory, hard and floppy drives, input devices such as a keyboard 18 and mouse 20, and color display monitor such as at 22. Preferably, computer 16 has at least sixteen megabytes of RAM and is otherwise equipped with high throughput data and video buses. The internal video card is preferably one selected with two or more megabytes of on-board memory and is capable of generating 32-bit or more colors for high tone resolution. Internal signal and image processing programs may be stored on the internal. hard drive of computer 16 and transferred to RAM in the usual way for any processing needs required. As best seen in Figs. 1 and 2, illumination and imaging section 12 comprises an optical head 24 for illuminating and contacting the surface of a sample to be visualized and measured, and a video camera 26 for collecting and imaging propagating radiation scattered from the surface of a sample. Video camera 26 may be any suitable conventionally available type of the desired spatial and tonal resolution and, preferably, is of a wide-angle type and has a magnifying or slightly minifying objective lens 28. Alternatively, objective lens 28 may be a zoom lens of appropriate tele- to wide-angle design. Located at the plane of best focus of objective lens 28 is a photo detector 30, which may be a conventional CCD or vidicon tube. Video signals generated from photo detector 30 may be processed on board camera 26 via a resident chip 32 for that purpose, or may be sent to an external device. Camera 26 and computer 16 are configured such that video signals are digitized to generate digital images for display on monitor 22 at real-time rates or at nearly real-time rates. Optical head 24 comprises a bulk optic, prismatic dielectric body 34 comprising a light entering facet 42, a sample contacting facet 44, and a light emitting facet 46. Optically coupled to facet 42 is an illumination section comprising a collimating optical section 36 consisting of a tube in which are resident suitable collimating optics in the form of spaced apart lenses 48 and 50. An illumination source 38 transmits radiation which is directed through facet 42 to facet 44. As best seen in Figs. 2 and 4a, light in transmissive dielectric body 34 is incident at an angle equal to or greater than the critical angle θ c so that the light totally reflects at the interface with a less dense medium such as air or water, i.e., at facet 44. It is understood that dielectric body 34 can be transmissive over all or any part of the electromagnetic spectrum, including but not limited to ultra-violet, infra-red, or even x-ray and millimeter wave extremes, depending on the application. Although the incident light is shown to be a collimated beam, it need not be, and in fact imaging resolution improves if the incident light is less coherent. As seen in Fig. 4a, an evanescent field 52 arises at the boundary between facet 44 and the lower index medium opposite it (usually air, but this medium may also be water or another low index medium). Evanescent field 52 has an amplitude that decays exponentially with distance from the surface of facet 44. The strength of evanescent field 52 is given by: E evanescent ~ where E 0 is the amplitude of the electric field associated with the photon in the medium comprising body 34 and, d is the penetration depth in the less dense £ medium at which E 0 decreases to — - and where: e and λ , is the wavelength in the denser medium, θ is the incidence angle, and n 2l is the ratio of denser to lower indices of refraction at the boundary of facet 44. The actual penetration depth, where E 0 falls to the limit of detectability, is dependent on these variables as well as both the photodetector sensitivity and the sample optical properties, and is typically approximately 0.75λ. However, the evanescent field, however small in intensity, can exist sensibly for tens of wavelengths, if the parameters on the last above equation are optimized. As is well-known, evanescent field 52 penetrates normal to the surface of facet 44 to the depth indicated above. Consequently, it extends beyond the physical boundary of facet to a predetermined depth and can be interrupted by a sample placed in close proximity to facet 44. In Fig. 4a, an incident beam of illumination 54 is shown illuminating facet 44 at the critical angle when no sample is in place. Normal to and above facet 44 is the entrance pupil 56 of video camera 26. Where no sample is present, the incident beam 54 is totally internally reflected from facet 44 and is directed as a beam 58 along the indicated path to emerge from facet 60. Since no light enters entrance pupil 56 under these conditions, the image displayed on monitor 22 is completely dark as shown in Fig. 4b at 62. Fig. 4c illustrates the changes which occur when a sample 64 is brought into contact with evanescent field 52. The scattering surface interrupts evanescent field 52 and scatters illumination 68 into entrance pupil 56 where it is used to form an image of the sample surface. The intensity of the scattered radiation, which is converted from bound energy at the surface of facet 44 to propagating radiation in dielectric body 34, depends on the local scattering properties and the local depth of penetration of the microtopographic features of sample 64. The resultant image displayed on monitor 22 is shown in Fig. 4d at 70 where it can be seen that an image area 72 is displayed against an otherwise dark field. In practice, a sample 74 is brought into contact with evanescent field 52 by means of a three-axis, micro manipulable translation stage 40 such as is shown in Fig. 2. It has been shown that the intensity of propagating radiation converted from the evanescent field can be high enough to visualize and measure surface details ranging from between less than a few angstroms to about 10 micrometers. Useful signal may also be generated with this illumination system to image both reflecting and transmissive materials. Fig. 3 is a general flow chart for the operation of imaging system 10 as well as for other embodiments described below. An evanescent field is formed at a suitable measuring interface, as indicated at block 80. Radiation from the bound evanescent field is converted by scattering and proximity into propagating radiation at block 82. The intensity of the propagating radiation depends on the local scattering properties and local depth of penetration of the sample surface into the evanescent field. At block 84, the propagating radiant energy is collected and imaged onto a photo detector as by the CCD of video camera 26. An image signal is then generated in block 86 and the intensity of the image signal varies in accordance with the microtopographic features of the sample under scrutiny. The image signal from block 86 is encoded as a gray tone map signal in which gray tones represent feature dimensions. This may be via a look-up table (LUT). The gray tone map signal is then formatted for two- and three-dimensional display via a computer or other suitable video signal processor at block 90. The formatted signal is then displayed at block 92 with monitor 22 or other suitable display as will be subsequently described. The dark field imaging system of the invention is seen to be complementary to the conventional PTM of the prior art in that scattering surfaces such as paper are difficult to view in the conventional PTM because the scatter competes with the gray scale tunneling image, while a smooth surface that is viewed easily with PTM will be largely invisible in dark field PTM because the image in the latter is formed by what is scattered out of the evanescent field, which is very little for such a smooth surface. Another important observation is that in Fig. 4a for the dark field PTM, the entrance pupil 56 is clear of the incident illumination in the dark field PTM, whereas the entrance pupil is the same as the exit pupil for the illumination in the photon tunneling microscope. This separation or decoupling of the illumination and imaging optics in the dark field PTM allows much more freedom in control of the illumination to maximize, for example, the vertical tunneling range that is the sensible amplitude of the exponentially decaying evanescent field, or to control polarization more easily so that non-dielectric samples may be viewed. Reference is now made to Figs. 5 and 6 which illustrate another embodiment for practicing the invention. Here, there is shown generally at 100 a dark field imaging system that comprises an illumination and imaging section 102 and display section 110. Section 102 comprises an optical head 106 which in turn comprises an aplanatic sphere 112 having a slightly curved contact surface 120. Illumination is provided at the critical angle via a fiber optic bundle 116 feed by a source such as a laser, LED, or other solid state device. Suitable radiation controlling filters may also be present in this optical path to control state of polarization or spectral content of illuminating radiation or both. Scattered radiation, as indicated at 124, propagates to the entrance pupil of an objective lens 122 of a microscope 104. Microscope 104 is focused through aplanatic lens 106 onto surface 120. Microscope 104 forms an enlarged image of a sample and aplanatic sphere 106 may be used to aide in the correction of spherical, coma, and astigmatism aberrations in the usual way. The image formed by microscope 104 is viewed by a photometric vidicon 108 of conventional design. Vidicon 108 converts the gray scale scattered image into a video signal that is restored by a three-axis oscilloscope 129 to a real-time 3-D image of the sample microtopography while controlling perspective. Other peripherals include a video image processor 122, a VCR 126, a 2D gray scale image display 124, and an XYZ screen video transfer section 128. An XYZ translation stage 118 is provided to bring a sample into proximity with the curved surface 120 of aplantic sphere 112. Curved surface 120 facilitates contact with the sample. Previously, the inventive dark field photon tunneling imaging system embodiments were intended to be used in stationary modes of operation with the sample moveable with respect to the optical heads. Because the dark field approach permits decoupling between the illumination and imaging optical paths, other optical head configurations are possible. In Fig. 7, an imaging device 140, such as a video camera, vidicon, or microscope, comprises an objective 142. Objective 142, which contains the entrance pupil 56 as shown in Fig. 4a, is made to image through a transmissive dielectric body 144 that corresponds to body 34 in previous figures. A light source 148 is incident on a prism 146 that is coupled optically to dielectric body 144 so that total internal reflection of the light occurs at least at the distal surface 145 of body 144 so that an evanescent field exists outside of distal surface 145. The sample to be imaged is brought proximal to distal surface 145 so that it is within the evanescent field as was illustrated in Fig. 4c. Although the light source 148 is shown as a unidirectional one, and in some cases this type of illumination is preferable, there are many possible illumination configurations as will be illustrated subsequently. In Fig. 8, there is shown another embodiment of a dark- field PTM instrument 150 comprising an imaging detector, such as a CCD camera 152, into which the real image from an objective 154 is projected. Alternately, a projection eyepiece can be included in this arrangement for increased magnification, and objective 154 can be of variable magnification. Illumination is provided via a totally internally reflecting slab block 156 where the evanescent field is formed at a distal end 158. A light source 159 is coupled to slab block 156 via a bent up tab section 157. In Fig. 9 a system 160 comprises a coherent imaging fiber optic bundle 162 to relay the image formed by an objective lens 164 to a remote camera and illumination source 166. This embodiment is particularly suitable for use in tight and otherwise inaccessible spaces. A number of additional illumination configurations are possible, as illustrated in Figs. 10 through 24, and each offers its own unique advantages. The common element in all of these variations is that total reflection of the illumination is made to occur at least at the distal surface of the body in order to cause the necessary evanescent field illumination outside of and adjacent to the distal surface. In Fig. 10, a transmissive body assembly 170 in the form of a figure of rotation provides the optical head functions of previous embodiments. Body assembly 170 comprises an angled incident entrance facet 172 that extends around its circumference. This allows for more than one discrete light source (e.g., 174, 176, and 178) to be placed at any azimuthal angle about the axis of rotation. It should be understood that "light source" or "lighting means" as used in this disclosure can be a laser diode, a light emitting diode (LED), a fiber bundle carrying light from a remote source, incandescent, halogen, or other light source. At plane 175 there may be placed a polarizing filter, wavelength filter, phase plate, or other light controlling device. In Fig. 11, the discrete light sources of Fig. 10 are replaced with an annular light bulb source 180 for lighting the angled circumferential edges 181 of an annular slab block 182 to illuminate the sample from all directions. In Figs. 12 and 13, light from a source is incident normal to the surface 192 of a flat plate 190 that is parallel to the distal surface 194 but is totally internally reflected by angled edge surface 196 so that it undergoes multiple total internal reflections 198. The light source can be discrete as at 200 or tubular as at 202. In Fig. 12, an optional truncated or "aplanatic" sphere 204 may made integral with the flat plate 190 in order to improve the image according to aplanatic principles. In Fig. 14, the light source is a monochromater 210 so that analytical dark field PTM can be done. An optional detector 212 is shown at angled edge surface 196 of flat plate 190 which is now inverted. In Fig. 15, the transmissive body is in the form of an aplanatic sphere 220 that is truncated at an optically prescribed center thickness 212 such that the image through aplanatic sphere 220 is improved over a parallel flat plate by being aplanatic. The illumination is incident to sphere 220 at angles equal to and greater than the critical angle θ c . The dotted lines 214 indicate an optional metallic coating, the purpose of which is to allow the incident light to enter the sphere at other angles. Surface 216 is the total reflection surface from which the evanescent field emanates. The dotted radius 218 indicates a preferred curved surface to facilitate proximity between the aplanatic sphere and the sample (which is not shown), and also to facilitate sliding of the aplanatic sphere along the sample in the XY plane. The slight curvature does not affect the optical quality of the image to any significant degree, and yet greatly simplifies the practical use of this aplanatic sphere. A complete sphere 230 is shown in Fig. 16. While the imaging quality of a completely spherical transmissive body is not as good as the aplanatic sphere or even the flat plate bodies, it is acceptable for certain applications where a rolling optical probe is needed. The spherical geometry allows for rolling contact with the sample, analogous to the tip of a ball point pen. This embodiment is beneficial where sliding contact between the transmissive body and the sample are undesirable. Fig. 17 shows a rotated solid Dove prism 240 with a curved distal surface indicated by the dotted radius line 244 in comparison to a flat distal surface, with curvature again to facilitate contact with the sample and aid in sliding over the sample in the XY plane. This curvature, the radius of which can be measured and known, also may serve to calibrate height to gray scale in the photon tunneling scattered image. Light enters the Dove prism as a beam 242 as shown. Fig. 18 shows another variation of a transmissive body that is a normal Dove prism 250 except that opposing the incident entrance plane 252 is a truncated plane 254 peφendicular to the distal surface 258, or as indicated by the dotted line 256, parallel to incident entrance plane 252. This geometry affords advantages in some analytical applications, such as spectroscopic. In Figs. 19 through 23, the transmissive body is a very thin plate which serves to guide the light that is launched into it at and beyond the critical angle with multiple total internal reflections. It should be understood that in all of these embodiments, the means of launching the light into the light guide can be a single unidirectional means as shown, or a multitude of discrete like means, or a continuous figure of rotation of the means shown for omnidirectional illumination, analogous to the illumination schemes discussed earlier. The advantage common to all of these embodiments is that an objective, such as that shown at 270 in Fig. 23, can now have a very small working distance and higher numerical aperture, thus affording higher lateral resolution and a wider range of magnifications and fields of view, as well as affording a much more compact device overall. As with the other embodiments, it is understood that these thin plate waveguides can substitute for the transmissive slab body assemblies. In Fig. 19, the means of launching light is a prism 282 optically coupled to a waveguide 280, so that light incident to prism 282 is at or beyond the critical angle and so undergoes multiple total internal reflections within waveguide 280, giving rise to evanescent field illumination at the distal surface 284. In Fig. 20, the means of launching light into a waveguide 290 is a set of micro prisms 292. This set of micro prisms 292 could also be in the form of periodic microstructure known as diffractive optics. Here, the periodic structures are provided with a spatial period smaller than the wavelength of the light from the lighting means such that the evanescent field is caused by diffraction of light by the periodic structure. In Fig. 21, the means of launching light into a waveguide 300 is a holographic optical element, or HOE 302. In Fig. 22, a waveguide 310 is flexible, and the means of launching light into the flexible waveguide 310 can be a prism 312, HOE, diffractive optics (kinoform), or microprisms. In Fig. 23a and 23b, a waveguide 320 has lower refractive index core 324 in which the total internal reflections occur. Core 324 is exposed on a distal surface 326 directly to the sample 328, while the cladding 330 above core 324 maintains total reflection when there is provided external contacting material. It will be appreciated that a thin transmissive parallel plate or flexible membrane may be used to contact to the distal surface of any of the above transmissive bodies and act as a disposable protective covering. If damaged during sliding contact with the sample, it is removed and replaced, so that expensive damage to the main distal surface is avoided. In addition, hard, diamond or other antiabrasion coatings may be applied to the distal end. Although not shown, all of the transmissive body embodiments discussed above and shown can have a metallized distal surface, with the thickness of the metallization chosen for the illumination wavelength and the incident angle such that a plasmon field is excited on the metal layer by the evanescent field. Therefore, all of the foregoing bodies can be used for surface plasmon microscopy, with all the benefits that brings to, for example, fluorescence microscopy. Similarly, all of the transmissive bodies discussed above can have multiple dielectric thin film coatings on their distal surfaces in order to cause optical resonance, such that the amplitude of the evanescent field is increased for better signal to noise, and better vertical resolution. The entrance and exit faces of the transmissive bodies can be coated and arranged geometrically so that the transmissive body becomes a cavity resonator. Additionally, all of the distal surfaces can be non-smooth surfaces, where the random or periodic surface structure has a spatial period smaller than the wavelength of the illuminating light in order to generate a diffraction-born evanescent field for even higher lateral resolution such as with the diffraction grating 331 formed in a transmissive body 332 shown in Fig. 24. In Figs 25 through 33, there are shown various methods of mounting and using the dark field PTM imaging system. The many embodiments of the illumination and transmissive bodies discussed above can be used and combined with these various mountings. In Fig. 25a, the transmissive body is shown at 340 as one of three pods, the other two pods shown at 342 and 344. All three pods are arranged in kinematic fashion on a baseplate 346 such that when baseplate 346 is placed on a reasonably flat sample surface, the distal surface of the transmissive body pod 340 is automatically in contact with the sample surface, in focus, and aligned. In this way, the dark field PTM functions ergonomically less like a traditional microscope and more as a computer "mouse", except that is a powerful surface profiler. This compact, portable device is easily placed on an airplane wing, or production web of paper, or painted hood of an automobile, for example. In Fig. 25b, the baseplate and pods are shown in profile with the rest of the dark field photon tunneling imaging system components mounted to the baseplate. These include an imaging and illumination section 348 and a control section 350. Imaging and illumination section 348 and control section 350 operate in a manner similar to system 160 of Fig. 9. Many mechanical and other features can be incorporated into the baseplate 346 to provide devices with different capabilities depending on the specific visualization or measurement tasks. Although they will described and shown individually in what follows, the features can in many cases be combined. In Fig. 26, two non-optical pods 360 are motor driven wheels or balls, with one means of drive indicated by motors 362 and 364. The baseplate 346 can then be translated about the sample surface. In Fig. 27, means for air bearing levitation 366 are incorporated into or around all three pods (340, 342, and 344). The air pressure can be used not only for frictionless movement about the sample, but can also control the separation between the distal surface of transmissive body pod 340 and the sample. With differential control over any two pods, alignment of the optical axis normal to the sample surface is achieved, even on non-planar sample surfaces. In Fig. 28, two of the pods (only one shown at 370) are mechanically adjustable in height with micrometers 368 or piezo drives to similarly adjust alignment on non- flat surfaces. In Fig. 29, a counterbalance weight 374 is added such that the two non- optical pods (only one shown at 372) are at the fulcrum point of the device. Sliding weight 374 toward or away from the fulcrum point adjusts the amount of gravity loading of the transmissive body pod 340 against the sample. In Fig. 30, a computer "mouse-like" feature is incorporated into the baseplate 346 so that the position and movement of baseplate 346 and the imaging and illumination sections may be indicated in a well-known manner on a computer screen. For this purpose a ball 376 and well-known positioning technology may be incorporated into baseplate 346. Also in Fig. 30, a marker 378 is added to baseplate 346 so that areas of interest, or defective areas, can be marked in industrial applications. Marker 378 may be any of well-known types such as an inking device. As seen in Fig. 31, the dark field photon tunneling imaging system is very convenient to use also in an inverted position, where a transmissive body distal surface 382 is facing upward. The operator can then hand-place a sample onto the distal surface 382 for immediate images of the sample topography and very rapid throughput of samples. In Fig. 31, an inverted system designated at 380 is accomplished by combination of the portable base 383 similar to the one discussed above nested in a receiver base 385 that has, for example, an optional port for a monochrometer 386 for spectral analysis in addition to topographic profilometry. An optional arm 390 is shown that serves to apply loading to the sample with a device 384 that is an air jet, spring loaded piston, or other mechanism for that purpose. Arm 390 may be raised and lowered into position via a column 392. Other useful, but optional features not shown, are means for heating or cooling the transducer pod and sample, or incorporation of patterning of the illumination for manipulation of microscopic particles. Another useful mounting for a dark field photon tunneling imaging system is seen in Figs. 32a-32c. Here, an imager 402 is mounted as a spring loaded piston 414 within a base 400 having three equally spaced pods or balls 404, as is found in an optical spherometer. The distal surface 406 of the transmissive body automatically contacts a flat or curved sample placed on the three pods 404. Piston 414 is mounted in a bored out block 410 in which there is placed a spring 412. In optical fabrication, this mounting configuration provides the optician with both the radius of curvature of the optical surface as well as the roughness statistics and topography, and the degree of optical polish. This configuration can also be used in a downward orientation, as in the center of the base described previously with pods 404 contacting the surface along with the piston 414. In Fig. 33, the dark field photon tunneling imaging and illumination sections are configured as a hand-held probe 420, with the distal surface of the transmissive body 422 placed against the sample 424. The dark field photon tunneling invention can be applied to measure flying height of magnetic read- write heads above floppy or rigid disks in the standard test drives, such as Guzik™, used in the industry. In Fig. 34, light 430 is launched into a glass or polycarbonate analog disk 432 so that it undergoes multiple total internal reflections 433 and therefore induces an evanescent field at both glass to air interfaces. Any of the launch methods previously discussed can be used for this application. Alternately, the edge of disk 432 can be chamfered to form an integral prism face, or can be molded with this prism face to begin with. Even a scattering surface on this edge will launch light into disk 432, though less efficiently and with less control over incident angle. An inside edge 437, nearest to a spindle hub 440, is shown and is the preferred light launch site, but even the outer edge of the disk 432 can serve as the launch site. As a real read/write head (434 or 436) approaches the disk surface 450, it is illuminated by the evanescent field, which is converted into propagating light via scatter by the head, rather than by refraction as in the optical proximity device or photon tunneling microscope. The scattered light enters the dark field PTM objective 438. The typical light-colored ceramic heads will scatter the best, but with a more sensitive detector other less scattering heads may be measured as well. The unadorned glass (or other material) disk will work. However, performance may be improved by blackening, metallization, anti-reflection, or high-low stack dielectric coatings that are selectively applied to strategic areas of the disc or head to improve image contrast and signal to noise, such as one or both of the disk surfaces, or the inside or outside rim of the disk. In addition, a magnetic coating may be added if optically transmissive enough to view through (the near infra-red wavelengths transmit best through such magnetic coatings). Also, a planar waveguide may be created in the disk surface facing the head by infusing chemicals to alter the refractive index. The advantages of using the dark field photon tunneling are all those of photon tunneling but, in addition, the viewing axis is normal to the disk and head surface, thereby eliminating the need for additional optics to view at the critical angle. In addition, it will be understood that it is preferable in the measurement of flying heights with head arrangements for double sided media, it is best to use one real head and one transparent head so the full aerodynamic environment of the read/write system is experienced. Referring now to Fig. 35, it can be seen that dark field photon tunneling, with its high resolution characteristics, can be applied with advantage to the field of optical data storage and retrieval. In Fig. 35, a rotating polycarbonate or other similar optical compact disc 460, or a similar optical card scanned in the XY plane, contains data bits in the form of optical scatter sites 138 on or very near the surface, or nanometer-high topographic bumps 470 on the surface, either of which the evanescent field is sensitive to. A flying total internal reflection head 464 and 468, that can be configured as previously described, serves to illuminate disc 460 in evanescent field light. The information bits convert the evanescent field to scattered light that an objective 466 receives. Alternately, the scatter sites or bumps can be internal to the disk. Into the surface of the disk may be formed a HOE, kinoform, or micro prisms such that, when illuminated normal to the disk surface, only the local area below each element of the micro prism or equivalent HOE is illuminated with evanescent light. As illustrated in Fig. 36, the benefits of dark field photon tunneling imaging or microscopy can be enjoyed in a normal photon tunneling microscope through the use of a conversion which restricts the useful NA of the objective to less than 1.0, and also by reducing the level of specular illumination. Both of these expediencies, while not completely necessary, enhance the performance for dark field puφoses. Here, a stop 480 is placed in the epi-illumination path to only allow illumination from numerical aperture 1 to the full extent of the objective, usually 1.25. A complementary annular mask 482 is placed in the imaging optical path to mask out light returning at a numerical aperture greater than one, thus assuring the collection of primarily scattered light from a sample. Reference is now made to Figs. 37 and 38 which show generally at 500 the viewable area of a monitor or other display device. Within the viewable area, it is possible using well-known techniques to provide different widows to display analytical data, such as statistical data, about the properties of a surface along with image of the surface. For example, box 502 could contain autocorrelation information, 504 could be the image, box 506 and enlargement of the image, and line 508 the surface profile. Similarly, boxes with this type of numerical and graphical or pictorial information can be displayed within boxes as box 512 is within box 510 in Fig. 38. The dark field photon tunneling imaging systems of present invention operate in a novel way because detected light has been scattered out of the evanescent light field by the sample surface. As a result, the advantages of this invention are: increased tunneling range, increased topographic sensing, ability to look at thick and opaque samples, ability to look at rougher surfaces, less sensitivity to optical inhomogeneity in the sample, decoupling of imaging and illumination optics for greater freedom to control illumination and imaging characteristics. Further advantages are real time high speed imaging, and high energy throughput that facilitates optical analytical techniques. It will be understood that the present invention is by no means limited to the particular constructions and methods herein disclosed and/or shown in the drawings, but also comprises any modifications or equivalents within the scope of the claims.

Claims: What is claimed is: 1. A dark field, photon tunneling imaging system, said system comprising: lighting means for illuminating a surface with an evanescent field of substantially an optical wavelength in extent so that radiation initially bound within said evanescent field is converted at least in part into propagating radiation through the process of back scattering from said surface and such that, in the absence of a surface or if a surface is distant, no evanescent radiant energy is converted into propagating radiation, said propagating radiation varying in correspondence with the scattering properties of said surface and the local distance of the surface's microtopographic features from said evanescent field; an imager having an optical axis positioned to collect said propagating radiation and form an image in which the microtopographic features of said surface are encoded as imagewise variations in image intensity; and photodetector means for generating an image signal having an amplitude that varies in accordance with said image intensity and position. 2. The system of claim 1 further comprising means for receiving said image signal and generating a tone mapping signal in which the size of a surface's microtopographic features are encoded imagewise variations in tone. 3. The system of claim 2 further comprising means for receiving said tone mapping signal and reformatting it into a three-dimensional display signal in which tone levels represent the size of the surface's microtopographic features. 4. The system of claim 3 further comprising display means for receiving said three-dimensional display signal and generating a three-dimensional representation of at least a part of a surface so that it can be seen by a human observer. 5. The system of claim 1 further comprising a base and a housing for providing a light tight enclosure over said base. 6. The system of claim 5 wherein said base includes a kinematic pod support comprising three pods arranged in a triangular pattern for positioning said system with respect to the surface of a sample to be measured. 7. The system of claim 6 wherein said base further includes as a fourth pod a spring loaded track ball for contacting a surface to be measured to facilitate tracking the position of said system on a sample surface. 8. The system of claim 1 further comprising: a light transmissive analog recording disk having a central axis; means for mounting said light transmissive analog recording disk for rotation about said central axis; and a read/write head positioned to fly above the surface of said light transmissive disk as said light transmissive analog disk rotates. 9. The system of claim 1 further comprising: a light transmissive recording media having a surface having formed therein a plurality of local optical scattering sites by which information has been encoded proximate said surface; and means for mounting said light transmissive recording media so that said scattering sites are brought into contact with said evanescent field so that light initially bound within said wavelength evanescent field is converted at least in part into propagating light through the process of back scattering from said scattering sites such that, in the absence of a scattering site or where a scattering site is distant, no evanescent light energy is converted into propagating light, said propagating light varying in correspondence with the scattering properties of said scattering sites and the local distance of said scattering sites from said evanescent field. 10. The system of claim 1 wherein said imager comprises a digital imaging camera having an objective lens focused on said evanescent field so that said surface image comprises the whole field of view of said camera objective lens. 1 1. The system of claim 1 wherein said lighting means comprises an optically transmissive body having an entrance facet for receiving illumination from which said evanescent field is formed, a distal facet at which said evanescent field is formed so that a sample surface can be brought proximate to it, and an exit facet from which propagating light emerges. 12. The system of claim 11 wherein said entrance facet, said exit facet, and said lighting means are structured and arranged with respect to one another so that said distal facet is a totally internally reflecting barrier where said evanescent field is caused by photons tunneling beyond said distal facet. 13. The system of claim 12 wherein said distal facet includes a periodic structure having a spatial period smaller than the wavelength of the optical radiation from said lighting means and where said evanescent field is caused by diffraction of said optical radiation from said lighting means by said periodic structure. 14. The system of claim 11 wherein the distal facet of said optically transmissive body has a predetermined radius of curvature to facilitate contact with the sample surface. 15. The system of claim 11 further comprising coupling means for introducing optical radiation from said lighting means into said optically transmissive body. 16. The system of claim 1 wherein said lighting means and said imager have optical paths that are optically uncoupled with respect to one another. 17. The system of claim 1 wherein said lighting means comprise at least two discrete optical radiation sources. 18. A dark field, photon tunneling method for imaging and measuring the microtopographic features of a surface, said method comprising the steps of: illuminating a surface with an evanescent field of substantially an optical wavelength so that light initially bound within said optical wavelength evanescent field is converted at least in part into propagating light through the process of back scattering from said surface and such that, in the absence of a surface or if a surface is distant, no evanescent light energy is converted into propagating light, said propagating light varying in correspondence with the scattering properties of said surface and the local distance of the surface's microtopographic features from said evanescent field; collecting said propagating light along an optical axis and forming an image with said collected light in which the microtopographic features of the surface are encoded as imagewise variations in image intensity; and detecting said image and generating an image signal having an amplitude that varies in accordance with said image intensity and image position. 19. The method of claim 18 further comprising the step of receiving said image signal and generating a tone mapping signal in which the size of a surface's microtopographic features are encoded imagewise variations in tone. 20. The method of claim 19 further comprising the step of receiving said tone mapping signal and reformatting it into a three-dimensional display signal in which tone levels represent the size of the surface's microtopographic features. 21. The system of claim 20 further comprising the step of receiving said three- dimensional display signal and generating a three-dimensional representation of at least a part of a surface so that said representation is observable by a human.

Inventors: GUERRA JOHN M, GUERRA, JOHN, M.
Applicants: POLAROID CORP, POLAROID CORPORATION
Application year: 1997
Main classification: G02B21
IPC codes: B62D57, B81B7, G01B11, G01N13, G01N21, G01N37, G11B5, G11B9, G11B33, G12B21