Source: https://patents.google.com/patent/WO2001059402A2/en
Timestamp: 2019-11-17 16:04:04
Document Index: 379108468

Matched Legal Cases: ['Application No. 09', 'art 210', 'art 210', 'art 210', 'art 210', 'art 210', 'art 210', 'art 450', 'art 450', 'art 550', 'art 550', 'art 550', 'art 550', 'art/2']

WO2001059402A2 - Optical systems for measuring form and geometric dimensions of precision engineered parts - Google Patents
WO2001059402A2
WO2001059402A2 PCT/US2001/002411 US0102411W WO0159402A2 WO 2001059402 A2 WO2001059402 A2 WO 2001059402A2 US 0102411 W US0102411 W US 0102411W WO 0159402 A2 WO0159402 A2 WO 0159402A2
PCT/US2001/002411
WO2001059402A3 (en
2001-01-25 Application filed by Zygo Corporation filed Critical Zygo Corporation
2001-08-16 Publication of WO2001059402A2 publication Critical patent/WO2001059402A2/en
2002-01-17 Publication of WO2001059402A3 publication Critical patent/WO2001059402A3/en
230000003287 optical Effects 0 claims description title 179
238000005305 interferometry Methods 0 claims description 34
The invention features a method for determining a geometric property of a test object, the method including: interferometrically profiling a first surface of the test object in a first coordinate system; interferometrically profiling a second surface of the test object in a second coordinate system different from the first coordinate system; providing a relationship between the first and second coordinate system; and calculating the geometric property based on the interferometrically profiled surfaces and the relationship between the first and second coordinate system. In some embodiments, the relationship may be determined by using calibrated gage blocks or by using a displacement measuring interferometer. Corresonding systems are also described.
The invention includes an optical system having one or more optical profilers adapted to view a test part from different perspectives. Each profiler is capable of measuring absolute positions of surface points in three dimensions with respect to a coordinate system local to each profiler. The invention further includes initialization and calibration procedures to relate the coordinate systems of each profiler to the other, so as to relate each measured surface position to all others. Such procedures can employ, for example, mechanical standard artifacts or a distance measuring laser interferometer, to provide information regarding the separation and relative orientation of the two corresponding optical profiler coordinate systems. Suitable optical profilers include triangulation systems, time of flight systems, and optical interferometers, such as height-scanning interferometers, which employ mechanical or equivalent scans perpendicular to the surface to obtain a localized (e.g. coherence-limited) interference pattern for each image pixel. As described in greater detail below, height- scanning interferometers that employ infrared sources can be particularly advantageous when working with test parts having relatively rough surfaces. In general, in one aspect, the invention features a method for determining a geometric property of a test object. The method includes: interferometrically profiling a first surface of the test object with respect to a first datum surface; interferometrically profiling a second surface of the test object in a second coordinate system with respect a second datum surface different from the first datum surface; providing a spatial relationship between the first and second datum surfaces; and calculating the geometric property based on the interferometrically profiled surfaces and the spatial relationship between the first and second datum surfaces.
The interferometric profiling of the first surface can include directing electromagnetic radiation to the first surface along a first direction and the interferometric profiling of the second surface includes directing electromagnetic radiation to the second surface along a second direction different from the first direction. The interferometric profiling of the first surface can include positioning the test object relative to an interferometry system and the interferometric profiling of the
9 - second surface includes repositioning the test object relative to at least one component of the interferometry system. For example, the repositioning of the test object relative to the interferometry system can include moving the test object or moving the at least one component of the interferometry system. In the latter case, the method can further include measuring the movement of the at least one component of the interferometry system to determine the spatial relationship between the first and second datum surfaces.
For example, determining the relationship between the first and second coordinate system can include: interferometrically profiling a first surface of a reference object with respect to the first datum surface; interferometrically profiling a second surface of the reference object with respect to the second coordinate system; providing at least one calibrated dimension for the reference object: and calculating the spatial relationship between the first and second datum surfaces based on the profiled surfaces and the at least one calibrated dimension. The reference object can be selected according to approximate dimensions of the test object.
The spatial relationship can also be determined by: interferometrically profiling a first surface of a initialization artifact with respect to the first datum surface; interferometrically profiling a second surface of the initialization artifact with respect to the second datum surface; calculating an initial spatial relationship between the first and second datum surfaces based on at least the profiled surfaces of the initialization artifact; adjusting the first and second datum surfaces to accommodate the first and second surfaces of the test object; and interferometrically measuring at least one displacement corresponding to the adjustment of the first and second datum surfaces. For example, the first and second surfaces of the initialization artifact can be the front and back of a common interface. Furthermore, the method can provide at least one calibrated dimension for the initialization artifact, and the calculation of the initial relationship can be based on the profiled surfaces of the initialization artifact and the at least one calibrated dimension.
The interferometric profiling of at least one of the first and second surfaces can include any of: performing scanning, white light interferometry; performing infrared, scanning interferometry; performing scanning MESA interferometry; performing scanning, grazing-incidence interferometry; and performing multiple wavelength interferometry.
The test object can also be partially transparent and the geometric property can relate to the positions of points on opposite sides of the partially transparent test object. The first and second surfaces of the test object can be interferometrically profiled from a common side and the first and second datum surfaces can be spaced from one another by a distance greater than a profiling range η of an interferometry system used for the interferometric profiling steps. Furthermore, the interferometry system used for the interferometric profiling steps can include a reference object having a partially reflective, first surface and a reflective, second surface, the first surface defining the first datum surface and the second surface defining the second datum surface. The spatial relationship can be defined by the spatial separation between the first and second surfaces of the reference object. In general, in another aspect, the invention features an apparatus for determining a geometric property of a test object. The apparatus includes: means for interferometrically profiling a first surface of the test object with respect to a first datum surface; means for interferometrically profiling a second surface of the test object with respect to a second datum surface different from the first datum system; and means for calculating the geometric property based on the interferometrically profiled surfaces and a spatial relationship between the first and second datum surfaces. The apparatus can further include means for determining the spatial relationship between the first and second datum surfaces. In general, in another aspect, the invention features an apparatus for determining a geometric property of a test object. The method includes: an interferometric profiling system which during operation interferometrically profiles a first surface of the test object with respect to a first datum surface and interferometrically profiles a second surface of the test object with respect to a second datum surface different from the first datum surface; and an electronic processor coupled to the interferometric profiling system, wherein during operation the electronic processor calculates the geometric property based on the interferometrically profiled surfaces and a spatial relationship between the first and second datum surfaces.
The interferometric profiling system can include a mount for supporting the test object, wherein the mount is adjustable between a first position for exposing the first surface of the test object and defining the datum surface and a second position fui exposing the second surface of the test object and defining the second datum surface. The interferometric profiling system can includes an interferometric optical profiler having a first viewing port for viewing the first surface of the test object and a second viewing port for viewing the second surface of the test object. For example, the optical profiler can include a first camera positioned to record a field of view for the first viewing port and a second camera positioned to record a field of view for the second viewing port. Alternatively, the optical profiler can include a camera positioned to record a split field of view for the first and second viewing ports. The optical profiler can include at least one source of EM radiation. The optical profiler can further include a first optic positioned to direct a first portion of the EM radiation towards the first viewing port and a second portion of the EM radiation towards the second viewing ports. For example, the first optic can be a beam splitting optic positioned to reflect the first portion of the EM radiation towards the first viewing port, reflect the second portion of the EM radiation towards the second viewing port, and transmit at least one additional portion of the incident EM radiation through the beam splitting optic. The optical profiler can further include a reflective reference surface positioned to receive the at least one additional portion of the incident EM radiation transmitted through the beam splitting optic. Furthermore, the optical profiler can include a transducer coupled to the reflective reference surface for scanning the position of the reflective reference surface.
The apparatus can further include a displacement measuring interferometer positioned to measure the spatial relationship between the first and second datum surfaces. The electronic processor can use at least one value indicative of PCOR dispersion in the interferometric profiling system and the test object to calculate the geometric property.
In general, in another aspect, the invention features an apparatus for determining a geometric property of a test object. The apparatus includes: an interferometric profiling system which during operation interferometrically profiles a first surface of the test object with respect to a first datum surface and interferometrically profiles a second surface of the test object with respect to a second datum surface, wherein the interferometric profiling system includes at least one movable stage for adjusting the position of the first datum surface and the second datum surface: a displacement measuring interferometer positioned to measure a change in a relative position of the first and second datum surface caused by an adjustment to the at least one movable stage; and an electronic processor coupled to the interferometric profiling system and the displacement measuring interferometer. wherein during operation the electronic processor calculates the geometric property based on the interferometrically profiled surfaces and the relative position of the first and second datum surfaces.
Embodiments of this aspect can include any of the following features. The interferometric profiling system can includes a second moveable stage, and during operation the first-mentioned movable stage adjusts the position of the first datum surface and the second movable stage adjusts the position of the second datum surface. Alternatively, the at least one movable stage can include a first movable stage adjustable from a first position defining the first datum surface to a second position defining the second datum surface.
In general, in another aspect, the invention features a method for determining a geometric property of a test object. The method includes: interferometrically profiling a first surface of the test object with respect to a first datum surface; interferometrically profiling a second surface of the test object with respect to a second datum surface different from the first datum surface; determining a spatial relationship between the interferometrically profiled surfaces which accounts for PCOR dispersion; and calculating the geometric property based on the interferometrically profiled surfaces and the spatial relationship. In general, in another aspect, the invention features an optical profiling system including: a broadband source; a scanning interferometer which during operation directs a first wavefront along a reference path including a partially reflective first surface and a reflective second surface and a second wavefront along a measurement path contacting a measurement object, and, after the second wavefront contacts the measurement object, combines the wavefronts to produce an optical interference pattern; a detector producing interference data in response to the optical interference pattern; an electronic processor coupled to the detector for analyzing the interference data; and a scanning controller coupled to the scanning interferometer and the electronic processor, wherein during operation the scanning controller causes the scanning interferometer to adjust the position of the first and second surfaces. In some embodiments, the partially reflective first surface of the scanning interferometer defines a first datum surface and the reflective second surface defines a second datum surface, and during operation the electronic processor calculates a geometric property of the test object based on the interference data and a relationship between the first and second datum surfaces.
Figure 1 is a drawing illustrating common definitions for flatness and parallelism.
Figure 2 is a drawing illustrating a part thickness measurement.
Figure 3 is a drawing illustrating another part third thickness measurement. Figure 4 is a drawing illustrating a step-height measurement.
Figure 5 is a schematic drawing of a two-sided all-optical FTP system.
Figure 6 is a schematic drawing of a single-sided optical FTP using a surface plate to simulate the part datum.
Figure 7 is a schematic drawing of a calibration using a gage block. Figure 8 is a schematic drawing of a simultaneous part measurement and system calibration using a gage block.
Figure 9 is a schematic drawing of a calibration using a displacement measuring interferometer. Figure 10 is a schema tic drawing of a structured optical profiler datum for use in measuring a step height.
Figure 11 is a schematic drawing of a structured optical profiler datum for use in calibration. Figure 12 is a schematic drawing of a structured optical profiler datum for measuring the relationship between curved surfaces.
Figure 13 is a schematic drawing of a optical profiling system from measuring step-height.
Figure 14 is a schematic drawing of a optical profiling system from measuring step-height and thickness.
Figure 15 is a schematic drawing of an optical profiling system measuring flatness and perpendicularity.
Figure 16 is a schematic drawing of a calibration of the optical profiling system of Figure 15. Figure 17 is a schematic drawing of an optical profiling geometry measuring flatness, thickness, perpendicularity, and orthogonality (FTPO).
Figure 18 is a schematic drawing of the camera image for the geometry of Figure 15.
Figure 19 is a schematic drawing of a profiling system measuring orthogonality. Figure 20 is a schematic drawing of an FTPO profiling system.
Figure 21 is a schematic diagram of an infrared scanning height measuring interferometer.
Figure 22 is a schematic diagram of an FTP optical profiling system for measuring a partially transparent test part. Figure 23 is a perspective diagram of an infrared scanning FTP system using a gage block for calibration.
Figure 24 is a schematic diagram of an FTP system using structured profiler datums.
Figure 25 is a schematic diagram of an IR scanning FTP system using a DMI for calibration.
Figure 26 is a flow chart describing operation of the IR scanning FTP system of Figure 25.
Figure 27 is a schematic drawing of a two-beam Michelson interferometer. Figure 28 is a graph illustrating interferometric coherence profiling data and the effects of PCOR and PCOR dispersion.
Figure 29 is a graph of interferometric phase as a function of wave number to illustrate to the effects of PCOR and PCOR dispersion.
Often one wants to verify that machined parts conform to GD&T specifications in accordance with national and international standards for engineering drawings. The ASME document Y14.5M-1994 (the "ASME Standards") defines GD&T practice in the US. The definitions contained in the ASME Standards relate closely to the way a skilled machinist would manufacture, verify and assemble parts. For example, for a part having opposing plane parallel surfaces, specifications of interest include flatness. thickness, and parallelism (FTP).
A parallelism tolerance often specifies a zone within which a surface lies, defined by two planes both parallel to a datum plane. Figure 1 summarizes flatness (F) and parallelism (P) for an example part having two opposing surfaces X and ∑i . The datum plane O is a theoretically exact plane in contact with the lower surface or a designated feature ∑i of the part. Parallelism is the minimum separation of two planes parallel to the datum Q that contain the entire upper surface Σ2 of the part. Evidently, the parallelism tolerance is greater than or equal to the flatness tolerance.
There are several relevant interpretations of thickness consistent with GD&T: Thickness 1 = Profile with respect to a datum: One approach is to tolerance a profile with respect to the part datum Q in Figure 1. This datum-referenced profile tolerance incorporates the basic dimension from surface ∑ι to surface Σ2. For the purpose of sorting the part according to thickness, the measured thickness may be considered the average distances from the datum Q of the two planes used to verify the parallelism of surface Σ2 with respect to the designated surface ∑i. Thickness 2 = Actual local size: A second possibility associates thickness with actual local size, which is the value of any individual distance at any cross section of a feature, as shown in Figure 2, e.g., local size values 7\2. N- Actual local size does not involve a reference to a datum. We propose to take the average of the maximum and minimum actual local size and call this measured thickness. In this case, and only in this case, it is possible to have the thickness tolerance be smaller than the parallelism tolerance.
Thickness 3 = Size: Yet a third interpretation of thickness is to consider it a synonym for part size. Once again, part size does not involve a reference to a datum. Rather, the definitions of MMC (maximum material condition) and LMC (minimum material condition) control part size. The MMC corresponds to the largest allowable separation of two parallel planes entirely containing the part. It is therefore the analog of flatness applied to the entire part. The LMC corresponds to the smallest allowable separation of any two opposing points on surfaces ∑i and Σ . The average of the LMC and the MMC and is a third possible definition of thickness (Figure 3).
Table 1 As illustrated in Table 1. to accommodate all of these potential GD&T definitions into an optical FTP measurement system, one distinguishes between relative surface topography measurements, which may have an arbitrary constant offset, and absolute measurements, which do not have this ambiguity. Evidently, the thickness definition 3 drives the requirements. If we collect all of the data necessary to calculate part size, then we have all of the information necessary for all of the other GD&T characteristics. We also have all of the necessary data to satisfy virtually any other meaningful definitions of FTP. Therefore, it is advantageous to have a metrology tool that provides high data density, absolute surface topography maps of both sides of a test part with respect to a common coordinate system. Similarly, for other applications, it is advantageous to have a metrology tool that provides high data density, absolute surface topography maps of disconnected surfaces Σ 4,ΣB of a test part with respect to a common coordinate system. For example, the disconnected surfaces may separated from one another
a step height, and the measurements of interest for the part may include flatness, parallelism, and the step- height (FP-H) of the disconnected surfaces, as illustrated in Figure 4. For example, one of the surfaces, e.g., Σ/( . could be fit to a plane to define the datum surface, and the step height could be defined as the average of the highest and lowest point on the recessed surface ∑β with respect to this datum.
Embodiments of the present invention make use of optical profilers to measure a height hHΣ within a restricted range η for any given point x,y on a surface Σ with respect to an optical profiler datum H. For example, such height measurements are characteristic of scanning height-measurement interferometers, e.g., the NewView 5000 from Zygo Corp. (Middletown, CT), for which η is the PowFoc scan range of 100 microns. The position and orientation of the NewView optical profiler datum are related to the starting point of the PowFoc scan as well as the locations of all optical components that influence the peak fringe contrast position. Using two such optical profilers to profile two part surfaces and relating the two corresponding optical profiler datums H . H2 for the profiling, provides information sufficient for FTP, FPH, and other such geometric part properties.
Figure 5 illustrates an all-optical FTP measurement involving two surface height profiles hH Σ ,hπ Σ taken either by independent optical profilers or by one profiler having two opposing viewing ports. The two planes labeled (H are parallel to Hi. Knowing the relationship between the two optical profiler datum planes Hi, H2 by means of a prior calibration, we can reference both surface profiles to a common plane, e.g. H :
h Hχ∑2 (x,y) = DHχH2 + h ll2∑2 (x,y) + x tan(aH]H2 ) + ytan(βMiH2 ) . (1 )
Here DH Hη is the distance from Hi to H2 at x=0, _y=0, and aH H , βH Ul are the tip and tilt angles between these two planes. Knowing b//,∑ and hH ∑9 for all x,y is sufficient to satisfy the needs of the FTP measurements in Table 1. An alternative to viewing the part from both sides for FTP measurements is to view it from one side only, using a mechanical datum simulator such as a surface plate (Figure 6). This satisfies the flatness, parallelism and thickness- 1 requirements outlined in Table 1 , provided that the contact with the surface plate is repeatable and reliable. Fixturing would be straightforward, and the object would be turned over to measure both sides for flatness. Furthermore, FPH measurements can be made using a single optical profiler by translating the optical profiler with respect to the part to sequentially view the disconnected surfaces. Moreover, embodiments can include a single optical profiler system in which the part is supported by an adjustable mount, which provides calibrated repositioning of the part with respect to the optical profiler so that two or more surfaces can be sequentially viewed by the profiler. Also, embodiments can include single optical profiler systems in which the optical profiler provides a split field of view for simultaneously viewing different part surfaces.
The optical profiling systems are calibrated to determine the relative orientation and distance between the datums Hi. H? corresponding to the two part surface measurements. Such calibration may be necessary when, for example, the datum positions are adjusted to accommodate varying part thickness by bringing them within the profiling range η.
One type of calibration involves standard artifacts such as certified gage blocks. The objective of the calibration is to establish the distance DH / and orientation angles a π ^ , βH //? that relate the two optical profiler datum planes H, H2. When using a mechanical standard artifact for calibration as shown in Figure 7, the first step is to use the profilers to measure the lower and upper surfaces G\. G . The next step is to rms fit planes G , G 2 to the profiler data, and reduce this information to distances DH] Gi ' DH2C and to orientation angles α^q , βH}G> , a HlG2 , βHlΑ . Knowing in advance how G relates to a G 2 (i.e., by NIST traceable certification), we calculate
aH\H1 = a/l}Gi ~ aH2G2 + aG{G2 βHxIl2 = βn G{ ~ βH2G2' + βG[G > (2) DH\H2 = DH\G\ ~ DH2G2 + DG{G2
Once this is accomplished, measuring the part proceeds according to Eq. (1). As shown in Figure 7, translation stages (e.g., z stages) can be used to position planes G , G within profiling range η of the optical profilers. The foregoing calibration using a mechanical standard artifact remains valid for a length of time characteristic of the overall mechanical and thermal stability of the measurement system. For many industrial parts, the metrology tolerances for thickness are tight (6σ< 1 μm) and it proves necessary to calibrate very frequently. An alternative is to place the artifact next to the test part for simultaneous calibration and part characterization in one measurement, as shown in Figure 8. In other words, the profiling system compares a gage block directly with the test part.
A convenient data analysis procedure is to measure the step height between the gage block and the test part on each side to obtain
■■ a G2∑7 • β(n∑-'> X*G2∑'2 ■ Parallelism comes from the angles, and the thickness is the difference of the DG>Σ> , DG^∑2 values plus the known or assumed characteristics of the artifact:
a∑\∑2 = aG\Σ\ - aG2 2 + aG{G2
DΣ Σ' = DG[Σ ~ DG2Σ2 + DG[G2
Calibration using a wavelength scale As has been noted above, adjusting the optical profiling system for varying part thickness involves adjusting one or both of the datums H, H2 to bring the object surfaces within the measurement η. Calibration determines the new relative positions and orientation of the datums Hi, H2 after this adjustment. An alternative to using a mechanical standard artifact to recalibrate for every thickness would be to monitor any z-stage displacements and compensate for any resulting changes in tip and tilt. For example, one could use a laser-based displacement measuring interferometer (DMI) to measure stage motion as well as any other parameter related to calibration. This wavelength scale eliminates the need for maintaining multiple artifacts and should be more flexible. The DMI measurement is initialized to establish the relationship between the
DMI measurement and the profiler readings. Initialization involves an initialization artifact, preferably thin, fully characterized and thermally stable, inserted temporarily into the path of the optical profilers. As the name implies, part of the function of the initialization artifact is to establish a point of origin for all thickness measurements. Figure 9 illustrates a full calibration sequence involving an initialization (a) in which the optical profilers translate to a position from which they may measure the initialization artifact, shown here as a thin block having a known relationship between the two surfaces Z\, Z2. The result of the initial zeroing sequence is four angles aXχ z{ /fz; ' «z /2°z< ∞cl two heights D^, , E z, resulting from the
rms plane fits Z ,Z2 to height data with respect to the optical profiler datums
H, . H . Based on this information and knowing in advance the relationship between
Z{ and ZT . the relationship between the two optical profiler datums Hf'. H, is given by aXX2 - aHx°z[ a H Z2 + a Z[Z2
At the same time, the DMI provides the angles or W 0 M 1 0 ■> β W o M , o and heights D W 0 M o resulting from a measurement of the initial relative position and orientation of the DMI mirror M° attached to profiler 2 with respect to the DMI internal reference datum W° . This completes the initialization process.
Now we can translate the optical profiler to any other position and thanks to the DMI, know precisely how far we have moved (see Figure 9, step (b)). The following equations calibrate the instrument for new positions:
aU] H1 = aH°H^ + a^ ~ aiV°M° βll, II2 = βH*H + βwM ~ βW°M» (5) D H H2 = DH*ll ~ D wM ~ DW°M°
where W ! , β WM ,DWM are DMI angles and heights measured for the new stage positions. An underlying assumption in this calculation is that the relationship between the
DMI internal reference datum H and the optical profiler datum H, is always the same. Further, the relationship between the DMI mirror M and the optical profiler datum H2 is also assumed to be constant. Mechanical and thermal drift may compromise this assumption over time, necessitating re-initialization. These calculations assume that the coordinate system for both the DMI and the optical profilers are the same, in particular, the x,y=0,0 lateral origin along which all of the distance measurements "E> " are taken. Thus minimizing Abbe offset errors would entail positioning the DMI beams so that the angles WM . β WM have the smallest possible impact on calculating DWM . There are several embodiments for wavelength scale initialization. For example, the initialization artifact could be transparent, with one surface partially reflective. In this case, the two surfaces Z\, Z would be opposite sides of the same surface, and the angles a z\z^ β z{z' and distance Dz^ would be very nearly equal to zero. A partially transparent zero-pane artifact could conceivably remain in the field of view at all times, and be a permanent fixture in the system. An additional calibration task can include subtraction of wavefront system errors that can degrade the flatness metrology. For example, a reference flat of very high quality can be inserted into the instrument to determine wavefront system errors, which are stored and used to correct the error in subsequent measurements. Measurement of system errors can take place simultaneously with initialization, e.g. if this reference flat is identical to the initialization artifact.
In one embodiment, a laser-based interferometer working in parallel with the optical profiler can be used, such as a 3.39 μm Jodon HeNe integrated into an IR Scanning system operating at 3.5-5.0 μm. The HeNe laser in the IR is naturally stable wavelength and mode stable, and all of the optics are shared by the wavelength scale and the optical profiler. IR cameras operating in this wavelength band may require low-MTBF Stirling cycle coolers. Alternatively, sources in the range of 8-12 μm can be used in the IR Scanning system because of the high reliability of commercial microbolometers. Such a source includes a \ 0.6-μm C02 laser. Alternatively, a multiple wavelength C02 laser interferometry can be used as the wavelength scale. Such an instrument would measure absolute height over a much larger range η, potentially covering the entire anticipated range of part thickness (e.g. 0-75mm). Another appropriate wavelength scale is a commercial 0.63- m HeNe heterodyne DMI, such as a ZMI 510 from Zygo Corp. (Middletown. CT). Complex features and structured datums
Some part types have somewhat more complex features than two opposing surfaces. For example, Figure 10 shows a part having three parallel surfaces, one upper surface and two offset lower surfaces. In addition to the thickness measurement, which relates to opposing surfaces, there is therefore a step height measurement. If the step height exceeds the measurement range η of the optical profiler, this presents a problem. As described above, this provides motivation for FPH-type measurements where each of the two offset lower surfaces are profiled in respective coordinate systems, and the coordinate systems are related to one another to determine the step height.
Alternatively, one can provide a structured optical profiler datum for the optical profiler. For example, this can be accomplished in interferometric optical profiler by positioning an object having a structured lateral profile in the reference arm of the optical profiler, e.g., the profiler could have a structured reference mirror. For the case illustrated in Figure 10. the structured optical profiler datum comprises two parallel planes having a nominal offset equivalent to that of the step height. The offset between the parallel planes in the structured profiler datum may be calibrated by a procedure similar to that described above, or may be a stable, known internal characteristic of the optical profiler. An optical profiler of this kind is capable of flatness, step height and parallelism measurement from one side, and flatness, step height, thickness and parallelism from two sides.
Another potential use of a structured profiler datum is to simplify calibration. Figure 1 1 shows how a small gage block may be employed to calibrate the system for measuring a larger test part, assuming that the structured profiler datum has a known offset. This type of calibration essentially transfers the calibration burden to the optical profiler itself. This could be advantageous if, for example, the optical profiler were configured to provide a variety of calibrated structured profiler datums without requiring the additional calibration steps described above.
Another example illustrates how a structured datum extends the underlying concepts of FTP measurement to non-planar surface, e.g.. the form, diameter. roundness, and/or straightness of spherical or cylindrical objects. Figure 12 illustrates conceptually how measurements from a curved optical profiler datum provide straightness. diameter and roundness of a cylinder. Preferably, in this case, a turntable would rotate and perhaps translate the part so as to complete the measurement over the entire surface.
FPH Optical Profiling System Figure 13 is schematic drawing for directly measuring step height. The system is a single-sided step-height-measuring tool (e.g, an FPH tool) employing a DMI as a wavelength scale. An IR Scanning optical profiler (discussed in more detail further below) measures a height hHΣ for any given point x,y on a surface Σ with respect to an optical profiler datum H. A translation of the optical profiler (i.e., a z-stage translation) provides an "extended scan" to capture both surfaces Σ 4 , ΣB when the step height exceeds the range η, the orientation and position of the optical profiler datum H changes between the two positions A and B. If we know the relationship between the two corresponding optical profiler datums HA, Hj, then we have a means of measuring step height. The role of the ZMI, therefore, is to relate HR to HA- Knowing the relationship between the optical profiler datum planes HA, HB for the two positions A and B, we can reference both surface profiles to a common plane, e.g. HA:
h llA∑B (x> y) = h HB∑B {x, y) + DH/tHB + x tan (aH lllB ) + y tan (βHA„B ) . (6)
Here DH ,, is the distance from HA to HB at x=0, y=0. and a,, ,, , βu ,, are the tip and tilt angles between these two planes. Knowing hπ Σ and hn Σ for all x,y provides all the information necessary for FP-H measurements. In the system of Figure 10, the test part is attached to DMI mirror M. either directly or by mechanical fixturing. to thereby maintain a rigid relationship between the part and the mirror. Thus in this embodiment, the DMI directly monitors the position of the optical profiler with respect to the part. The DMI data for beams a and b condenses to distances D and angles a,β according to the following formulas: aWM = arctan (WWM ■ w WM IA β M = const • (7) *WM - \ W WM
where WWM refer t0 me distances measured by the two ZMI beams a,b as shown in Figure 13, and L is the lateral separation of these beams. Note that because there are only two DMI beams, the ?or "tip" angle is assumed constant and is not tracked. The relative orientation and separation for the two optical datum plane positions A and B is then
aHAHB = WBMB - a WAMA
DH 4HB = DWBMB - DWAMA
In practice, it makes sense to set to zero both w M and v>wAMA as a standard procedure, in which case ocw M = 0 and Dw M - 0 , thus further simplifying Eq.
Figure 14 is a schematic diagram of an optical profiling system capable of both FTP and FPH measurements. In this embodiment, the DMI mirror is a virtual construct, resulting from reflections from several fold mirrors in the system (those attached to IR Scanning Profiler 2), none of which are actually attached to the part or the part fixture. Therefore, the DMI readings in this embodiment are only sensitive to the apparent or effective separation between the two optical profilers, as is required for thickness measurement, and do not report the actual part position.
Although the system of Figure 14 has a different geometry than that of Figure 13, it is still possible to measure step height according to an alternative extended-scan procedure. Here, the system performs two successive FTP measurements with a z stage motion in between. The part in this case, shown in Figure 14 has a back surface Σ9 nominally parallel to the surface regions Σ A , Σ B , or a mounting fixture having a mirror that serves as a substitute back surface. The step-height measurement proceeds as follows. First, we obtain a height profile h∑> ∑ of surface region Σl A with respect to an rms plane fit Σ2 to the back surface Σ2 . using FTP functions. Then we repeat the procedure for Σ]5 with respect to Σ2 . The two surface regions Σ] A, ΣlB are now related to a common reference plane Σ2 , as required for step height analysis.
The FTP optical metrology concepts readily translate to other types of relational measurements between surfaces, including those that are not nominally parallel. Figure 15 illustrates a measurement of flatness and perpendicularity of two surfaces. For this type of measurement, thickness is not a relevant parameter; however the calibration procedures are similar to what has been discussed above. Figure 16 shows calibration by a standard artifact and a DMI monitoring system, either of which can be used for the calibration. Furthermore, the artifact could be a partially-transparent element, in which case, it could be permanently in the field of view. Additional embodiments can combine FTP and angle measurements, e.g., flatness, thickness, parallelism, and orthogonality (FTPO). For example. Figure 17 illustrates a potential geometry for simultaneously measuring four surfaces, labeled (1) through (4). of an object having a rectangular cross section. The basic FTP instrument illuminates the object from two directions, labeled (A) and (B). The objective is to measure the flatness of all surfaces, the thickness and parallelism of surface ( 1 ) with respect to (3 ) as well as surface (2) with respect to (4), and the orthogonality of all adjacent surfaces.
In Figure 17. the two mirrors (orthogonality-test mirrors) are fixtured to be plane parallel and have a known separation, thus, the measurement geometry converts all 90-degree reflections into 180-degree reversals. This conversion transforms all of the angle measurements into simple parallelism checks. Thus if surface ( 1) is orthogonal to surface (4). they will appear to be parallel in the instrument. This is true even if either the object or the orthogonality-test mirror pair is rotated about an axis perpendicular to Figure 17. Figure 18 illustrates the appearance of the part as viewed by a camera imaging the system of Figure 17. The symbols x, ®, •, and θ, mark corresponding surface points on opposite sides of the object. For example, an LMC calculation of minimum thickness between surfaces (1) and (3) would involve the distance from the points marked with an x on each of these surfaces. Also, the origin or zero-thickness position is shifted by an amount L in the negative direction, equal in magnitude to the separation of the two orthogonality-test mirrors. Furthermore, A thickness D between any two surfaces is magnified in the geometry by V2 , because of the double-pass reflection at a 45° angle of incidence.
Another arrangement is shown in Figure 19, which tests the orthogonality of adjacent surfaces. This arrangement includes an additional orthogonality artifact to reference an initialization position. Like the system in Figure 17, the mirrors convert the orthogonality measurement into a parallelism measurement.
Yet another arrangement is shown in Figure 20, which tests all of FTPO. Here each of two perpendicular mirrors split the field of view from one of two optical profilers to accommodate profiling of four sides of a rectangular test part. The FTPO system of Figure 20 also includes a structured reference or employs a z-stage motion to accommodate for the fact that the distances to surfaces (1 ) and (3) are not the same as those to surfaces (2) and (4), respectively.
For relational measurements such as FTP, FTPO, and FPH, the optical profiler measures absolute surface height with respect to an optical profiler datum plane over at least a restricted measurement range η. Suitable optical profilers include triangulation systems, which involve geometric interpretation of position using trigonometry and assuming linear light propagation, time of flight systems, which utilize light pulse or amplitude modulation to associate time delay with distance, multiple wavelength interferometers, which use a sequence of discrete wavelengths followed by fractional fringe or synthetic wavelength analysis, phase-shifting interferometers, and height scanning interferometers. For many applications, the optical profilers are preferably height scanning interferometers, which include scanning white light interferometers (SWLI). scanning MESA interferometers, scanning grazing incidence interferometers, and IR scanning interferometers.
SWLI is described, for example, in commonly owed U.S. Patent Nos. 5,398,1 13 and 5,402,234. the contents of which are incorporated herein by reference. The NewView 5000 from Zygo Corp. (Middlefield CT) is a commercially available, SWLI instrument, which is capable of absolute height measurement. When a SWLI instrument is used on a part with a surface rough compared to the visible wavelength of the SWLI source, speckle phenomena degrade the meaningfulness of conventional interferometric fringe patterns. The white light coherence peak, however, can still provide distance information. See, e.g., T. Dresel, G. Haeusler, and H. Venzke in "Three-dimensional sensing of rough surfaces by coherance radar," Appl. Opt. 31 7). 919-925 (1992).
Scanning MESA interferometers are described in commonly owed U.S. Patent No. 5,598,265, the contents of which are incorporated herein by reference. Scanning grazing incidence interferometers are described in commonly owed, U.S. Patent
Application No. 09/325.175 entitled "Grazing Incidence Interferometer and Method" filed June 3, 1999, the contents of which are incorporated herein by reference.
IR scanning interferometers are like SWLI instruments except that broadband infrared light is used rather than white light. Surfaces that appear rough and generate speckle at visible wavelengths take on an entirely different appearance at longer wavelengths, e.g. in the IR. Thus, the IR scanning interferometer utilizes IR wavelengths sufficiently large so as to eliminate the troublesome speckle phenomena that are characteristic of rough-surface white light interferometry. The image and the interference fringes are therefore free of speckle and of all of the attending limitations and difficulties. By means of a broadband source to localize fringes, a suitable scanning mechanism and computer control, we achieve unambiguous measurement of technical surface profiles as well as relationships between surfaces and points over large areas, with high accuracy and rapid measurement speed. IR scanning interferometry systems are described in commonly owed U.S. utility patent application 09/514.215. filed February 25, 2000.
As shown in Figure 21 , an IR scanning interferometer typically includes: i) a broadband source providing a range of IR wavelengths for which the technical surfaces of the object appear specular, i.e., the reflected light at normal incidence is free of speckle; ii) an interferometric optical system, including at least one measurement beam reflecting from at least one object surface or surface point; iii) means for scanning the optical path difference of the interferometer (e.g., PZT-actuated reference mirror) while collecting interference data with an IR camera; and iii) computer control and processing for interpreting the interference data, so as to profile selected technical surfaces, and/or to determine parallelism, thic ness and/o height separation of multiple surfaces without fringe ambiguity.
Figure 21 illustrates a embodiment of the invention based on a Michelson-type interferometer 100 but operating entirely in the IR, at a wavelength sufficiently long such that the object technical surfaces within the field of view appear specular, e.g. 1 to 20 μm. The IR source 1 10 is sufficiently broadband to provide a limited coherence range, e.g. a few tens of μm. A diffuser 1 12 and a collimating lens 114 are positioned between the source and a beam splitter 120. The beam splitter directs a first portion of the broadband radiation along a reference leg to a reference mirror 130, and a second portion along a measurement leg to a measurement object 140. Imaging optics 180 direct the radiation recombined by the beam splitter to an IR camera 160. A computer 150 collects interference data from IR camera 160 while varying the optical path difference between the measurement and reference legs by means of a piezoelectric transducer (PZT) 170 attached to reference mirror 130. The effect of the PZT scan is to scan the measurement plane horizontally (e.g., with reference to measurement plane 195). The resulting interference data produces a localization of fringe data around the zero optical-path difference (OPD) position, which is characteristic of interferometry with a broadband source. The fringe localization provides a means of determining the precise moment when the measurement plane intersects the object point corresponding to the image pixel. The PZT motion is precisely controlled, so that knowledge of when a given object point is at zero OPD can be directly translated into a local surface height that is free of the ambiguity normally associated with interferometry. A compensator plate 175 compensates for dispersion caused by the beam splitter.
Because technical surfaces appear smooth in the IR scanning interferometer, it is meaningful to interpolate the interference phase for high accuracy, in a way that is not possible with prior-art, rough-surface white-light interferometry. Thus once the basic dimensions have been determined using fringe contrast, one may obtain a higher precision by means of the interference phase free of fringe ambiguity. Alternatively, one may process the data entirely in terms of broadband interference phases, using the frequency-domain analysis procedure disclosed in commonly owned U.S. Patent No. 5,398,1 13.
Many other embodiments of the IR scanning interferometer are possible. For example, the interferometer may be a Twyman-Green capable of profiling lenses, non- flat surfaces and optical components in the grinding phase of fabrication. Another variant is a Fizeau-type interferometer, with a comb-spectrum source providing periodic coherence peaks. Another variant uses a Mirau-type interference microscope objective. The source can be any broadband source operating in the infrared, e.g., a source operating in the range of about 1 micron to 20 microns, or more particularly, for example, 3 to 10 microns. The coherence length of the broadband IR source can be, e.g., in the range of about 10 to 50 microns. Suitable sources include a naked filament, a halogen bulb, a chemical source, a multimode C02 laser, other lasers such as diode lasers operating in the infrared, infrared LEDs, etc.. The detector can be any detector suitable for measuring the IR radiation, e.g., a pixellated microbolometer such as an InSb array.
An optical profiling system 200 for measuring a geometric property (e.g.. FTP) of a partially transparent test part 210 is shown in Fig. 22. Because test part 210 is partially transparent, surface profile measurements of both its front and back surfaces (212 and 214. respectively) can be made by using a scanning interferometer that includes a partially transparent reference mirror 220. Reference mirror 220 includes a partially reflective, first surface 222, which defines a first optical datum plane H near front surface 212 of test part 210, and a second surface 224. which defines a second optical datum plane H? near back surface 214 of test part 210.
The other components of system 200 are similar to those in Fig. 21. except that the system can operate at any wavelength (e.g.. the ultraviolet (LTV), visible, near- infrared (NIR). and infrared (IR)). Source 230 provides broadband radiation that passes through a diffuser 232 and a collimator 234. The collimated radiation is split by a beam splitter 240 to define a reference leg where a reference portion of the radiation is directed to reference mirror 220, and a measurement leg where a measurement portion of the radiation is directed to test part 210. Beam splitter 240 then recombines radiation reflected by reference mirror 220 and test part 210 to produce an interferogram, which is focused by imaging optics 245 onto a camera 250. Camera 250 records the interferometric data and sends it to computer 260 for analysis. Reference mirror 220 is mounted on a scanning mechanism 225 (such as a piezoelectric transducer or motorized stage) coupled to computer 260. During operation computer 260 causes the scanning mechanism to adjust the position of the reference mirror and store the interferometric data as a function of the scan position. Also, a compensator plate 283 is positioned in the reference leg to compensate for dispersion caused by the beam splitter.
The optical datum planes H and H> are specified for an initial starting position for reference mirror 220. As scanning mechanism 225 (e.g., a PZT) adjusts the position of reference mirror 220 over a scanning range η, the zero OPD (optical path length difference) planes corresponding to surfaces 221 and 222 of the reference mirror are scanned from the position of datum planes H and H>. When either zero-OPD plane intersects a surface feature of the test part during the scan, the interference from the broadband radiation is optimized (i.e., we have a coherence peak in the interferometric data). In practice, the interference data corresponding to the front and back surfaces of the test part can be distinguished from one another when the separation between the surfaces of the test object differs from the separation between the surfaces of the reference mirror by greater than the coherence length of the broadband source. Accordingly, the system may include multiple partially reflective reference mirrors, each of which can be attached to, and detached from, the scanning mechanism to accommodate different test part thickness. Thus, front surface 21 1 of the test part is profiled relative to datum plane H and back surface 212 of the test part is profiled relative to datum plane Hi. The relationship between the two datum surfaces is defined by the optical separation of surfaces 221 and 222 of the reference mirror. By calibrating the reference mirror, computer 260 can store the relationship between the datum planes and calculate FTP and other geometric properties for transparent test object 210 based on the profiled surfaces and the relationship. Such calculations are similar to those described above for other embodiments, however, one needs to account for optical path length within the transparent reference mirror and test object, which will be optically more dense than the surrounding air or gas.
Because each surface of the reference mirror defines an optical datum plane, optical profiling system 200 can be thought of as having two optical profilers that monitor substantially parallel surfaces of a test object from the same side. Accordingly it is clear that optical profiling system 200 can also be used for FPH measurements (e.g., step-height measurements) of a non-transparent test object, with the surfaces of the reference mirror providing datum surfaces for profiling the surfaces of the test part that define the step-height. To calibrate the separation between the surfaces of the reference mirror and determine the relationship between optical datum planes H and H?, one can replace test object 210 with a partially transparent calibration object having a predetermined thickness. The calibration follows analogously to that described earlier involving gage blocks. Moreover, as with previously described embodiments, the partially transparent calibration object can remain in the field of view during measurements of the test part to provide online data for the calibration. Alternatively, the thickness of the reference mirror can be precalibrated prior to its incorporation into optical profiling system 200. For example, the reference mirror may be a "master" to which the other test objects are being compared. The thickness of the master may be measured, e.g., by a careful physical thickness measurement, which is then multiplied by its refractive index to obtain its optical thickness. Alternatively, the master may be qualified by its functional properties only, and the quantity of interest is absolute FTP measurements with respect to the master, without concern for the precise actual thickness of the master itself.
We note that the measurements here presume that the nominal thickness of the test part (or the step height) is greater than the scanning range ;/. If this were not the case, a conventional scanning interferometer (i.e., one having only one reflective surface in the reference leg) could directly measure the front and back surfaces (or step- height surfaces) with respect to a single datum plane.
Furthermore, in additional embodiments, the reference mirror may be replaced with a partially reflective beam splitter (to define a surface equivalent to surface 221) and a separate reflective ele ent (to define a surface equivalent to surface 222). In such embodiments, one or bo h of the beam splitter and the separate reflective element can be positioned on a translation stage (e.g., a z-stage) to adjust their separation, and thereby adjust the positions of datum planes H/ and H?to accommodate the test part. Calibration and monitoring of the relationship between the datum planes can accomplished by DMI measurements to a DMI mirror on the z-stage in a manner similar to that described above.
Moreover, in other embodiments, the Michelson-type scanning interferometer shown in Fig. 22, can be replaced with any other interferometer arrangement suitable for scanning interferometric measurements (e.g., Twyman Green, Mirau. etc.).
Additional Examples of FTP and FPΗ Systems
Figure 23 shows an embodiment of an FTP system 300 based on IR scanning technology, although a similar configuration could be used with broadband radiation at other wavelengths (e.g.. ultraviolet, visible, near-infrared, etc.). A beam splitter 320 splits the field of view (FOV) to provide, in effect, two optical profilers sharing a common source 310, common camera 350, and common optics (e.g., camera lens 312, beam splitter 315, beam splitter 320, reference mirror 330 mounted on scanning stage 340, and reference gage block 350). The instrument may be thought of as two Twyman Green interferometers sharing a common optics.
There are two fold mirrors 360 and 370 mounted on translations stages (e.g.. z stages) 362 and 372, respectively. Beam splitter 320 includes two angled, beam- splitting surfaces. The first surface reflects a first portion of the broadband radiation towards fold mirror 360, the second surface reflects a second portion of the broadband radiation towards fold mirror 370, and both surfaces transmit the remaining broadband radiation to common reference mirror 330. Fold mirrors 360 and 370 direct their respective portions of the broadband radiation to opposite faces of a test object 380 and a hollow cylindrical gauge block 390. Gauge block 390 surrounds test object 380, and provides front and back surfaces in the split field of view (FOV) for calibration. During operation translation stages 362 and 372 adjust the optical path length of the measurement legs, effectively adjusting the nominal optical profiler datums Hi H2 with respect to the test part surfaces. The reference mirror scans over the range η to generate the height maps. Figure 24 shows another embodiment of a scanning FTP system 400. FTP system 400 includes a structured reference object 430, to provide structured profiler datums. The system includes two independent Twyman-Green interferometers 410 and 460 linked by structured reference object 430, which replaces the more usual reference mirror. Interferometer 410 includes broadband source 412, camera 414, beam splitter 416, and fold mirror 418. Similarly, interferometer 460 includes broadband source 462, camera 464. beam splitter 466. and fold mirror 468. Notably, in this embodiment, structured reference object 430 provides master datum surfaces for initialization artifact 445 and test part 450 at the same time, thus translation or z-stages are not necessary. In other words, the structured reference makes it possible to profile initialization artifact 445 and test part 450 at the same time. The scanning function for this geometry may be fulfilled by displacement of the reference object, the test part or any other appropriate optical component.
Figure 25 is a diagram of a dual-sided optical FTP system 500 based on IR scanning profiler technology and a 2-axis HeNe-based heterodyne DMI for the wavelength scale (e.g.. the ZMI 510 from Zygo Corporation). As in the embodiment of Figure 23, a similar arrangement can be used of other embodiments providing broadband radiation at other wavelengths (e.g.. visible. UV. NIR. etc.) for the surface profiling.
Referring to Figure 25, the broadband IR radiation is shown as solid lines and lies in the plane of the page along with the corresponding surface profiling optics, whereas the HeNe radiation is shown as dotted lines and lies above and below (not shown) the plane of the page, along with the DMI components, to provide the two axes of DMI metrology.
The scanning optical profiling system in system 500 includes a source 510 providing broadband IR radiation, which is collimated by lens 512 and incident on an IR beam splitter 514. IR beam splitter 514 splits the field of view by reflecting a first portion of the IR radiation to mirrors 521 on a first z stage 520, reflecting a second portion of the IR radiation to mirrors 531 on a second z-stage 530. and transmitting the remaining IR radiation to a reference mirror 540. Reference mirror 540 is modulated by a PZT-actuated flexure stage 542 with capacitive feedback, providing a 200- m scanning range η. The scan is repeatable and takes less than 3 sec to complete, a relatively short time compared to the drift rate of any of the optical components. Z stage 520 directs the first portion of IR radiation to fold mirror 522, which directs it to a first surface of a test part 550, to define a first viewing port. Similarly, Z stage 530 directs the second portion of IR radiation to fold mirror 532, which directs it to a second surface of a test part 550, to define a second viewing port. Each of the two z- stages can be translated to adjust the nominal positions of the optical profiler datums H, 2 to accommodate the first and second surfaces of the test part. IR beam splitter
514 recombines the broadband radiation reflected from the reference mirror and the two surfaces of the test object, and directs it to beam splitter 516, which in turn directs it to an IR imaging camera (e.g., a 10-micron microbolometer).
A ZnSe window with an antireflection (AR) coating one side and a -5% partially reflective surface on the other side is positioned as an initialization artifact 544 between fold mirror 522 and test part 550, with the partially reflective surfaces nearest the test part. To initialize the instrument, the z stages are moved so that the scanning range η for each of the two viewing ports overlaps the partially reflective surface. A window 546 positioned between test part 550 and fold mirror 532 has all of its surfaces AR-coated.
The geometry of the DMI system differs somewhat from that in the embodiment of Figure 9. In particular, reference mirror 540 in Figure 25 plays essentially the same role as the DMI mirror M in Figure 9.
Referring to Figure 25, a vertical beam doubler 562 splits the beam from a DMI source 560 (e.g., a Ηelium-Neon laser) to provide two axis of DMI vertically displaced above and below the plane of the page. As described above, only beam displaced above the plane is shown (as a dotted line) in the Figure. The two axes monitor a difference in the optical path difference (OPD) between the two viewing ports as well as any component rotatations about an axis parallel to the plane of the figure. The return beams from polarizing beam splitters (PBSs) positioned above and below IR beam splitter 514 (PBS) goes to a fiber-optic pick-up (FOP) 595 for signal detection. Only two measurements or "axes" are needed to monitor the unconstrained degrees of freedom in the optical system, as may be understood from the following discussion of the effects of various rigid body rotations of the optical components.
The mirror pairs 521 and 531 on the z stages 520 and 530, respectively, each form a rigid roof mirror. The same is true of the two fold mirrors 522 and 532 near the part. The two folds are mechanically constrained to have a highly stable orthogonal relationship (e.g. <5 rad drift in relative angle). A rotation of any of the roof mirror structures about a vertical axis has no effect on measured FTP of the part. A rotation of the reference mirror or the beamsplitter about a vertical axis modifies only the apparent longitudinal position of the test part, assuming that the DMI measurement of OPD intersects the line of symmetry for the two reference paths (e.g. there is no Abbe error). We can assume that one of the orientation angles will always be the same, e.g. aWM - o u „ = 0 and therefore we need not monitor this angle. A rotation of any of the components about a horizontal axis, however, couples directly into the apparent parallelism of the part; thus this rotation must be monitored. Two DMI beams projected symmetrically to upper and lower sides of the plane of the figure account for both rotations about the horizontal axis and the overall OPD of the system.
The DMI optics include two high-stability plane mirror interferometers (HSPMTs) 580 and 582 positioned above and below IR beam splitter 514. as shown in inset 579. For each DMI axis, there are two orthogonally polarized beams circulating in the measurement path in the same direction. HSPMI 580 includes a PBS 570. a corner cube reflector 572, a quarter-wave plate 574, and a half-sized half-wave plate 576. HSPMI 582 includes an identical set of optics below the plane of the page. The HSPMIs uses the half-sized half- wave plate instead of the usual full-sized quarter- wave plate to rotate the polarization of the measurement beam, so that all of the measurement beams are linearly polarized when reflecting from the various fold mirrors. In other embodiments, conventional HSPMIs can be used in which a full-sized quarter-wave plate replaces the half-sized half-wave plate.
Other embodiments of the instrument in Figure 25 can accommodates the structured profiler datum concepts described above by e.g., either (1) providing a structured reference mirror or (2) a structured mirror, window or other combination of optical components in the measurement path.
Figure 26 is a flowchart of the measurement procedure for the system of Figure 25. The first column desc ϊbes the initialization procedure. First, the z-stages are moved to bring the zero plant initialization surfaces Zx ,Z2 (i.e., the internal and external reflections from the parti a ily-re fleeting surface of the zero plane artifact) within the scanning range η of both of the optical profiler ports. Then the profilers do a fine scan over the range η to acquire surface height profiles h 0 x,y) , h 0 (x,y)
"\ Z\ H\ Z\ of initialization surfaces Z ,Z2 with respect to the optical profiler datums Hj° ,H2 . Based on this data, an electronic processor (not shown) coupled to the system calculates a least squares fit of artifact planes Z ,Z2 to the surface profile data z , hH Q z , and extracts a ^ . β ^ , a ^ , β π z, and D /{ , D ^ from height
profiler data Z\ , Z2 .
Next, DMI data is acquired for DMI mirror M with respect to the DMI internal reference datum W for z-stage positions corresponding to the initialization. From this data, the electronic processor extracts initial orientation and separation of ° with respect to W and uses it to calculate the relationship between the two optical profiler datums H] ). H2 using Eq. 4. Accordingly, the initialization provides the electronic processor with the following information a 0 0. β /0 0 , D 0 0 and
The second column of Figure 26 describes the part set-up. First, the test part is positioned in a mount or support fixture (not shown), and then the Z-stages are moved to bring the object surfaces within the scanning range η of the respective optical profilers. If desired, the part position can then be adjusted with respect to the system FOV.
The third column of Figure 26 describes DMI calibration. DMI data is collected for DMI mirror M with respect to the DMI internal reference datum W according to the z-stage positions for the test part. Then electronic processor extracts α/(/Λ/ , β M and
DWM from the DMI data, and calculates the relationship between the two optical
profiler datums H ,H7 using Eq. (5) to produce outputs or ., ,β. , D
1 2 1 ^~> ^\ ^7 The fourth column of Figure 26 describes data acquisition for the test part. The optical profilers scan over their scanning range η and determines surface height profiles hH Σ {χ ^y) < ^ 2∑? ix> y) °f Part surfaces ∑1 ,Σ2 with respect to the optical profiler
datums H\ ,H2 . Electronic processor then calculates b//.∑_, (x.y) from the surface height and calibration data using Eq. (1) .
The last column of Figure 26 describes FTP calculations based on the acquired data. For example, the electronic processor can calculate flatness from the results of
Chebychev fits to Λu ∑ (x,y) hH (x,y) ■ Local part size can be calculated
according to h∑ ∑ (x,y) = n Hx∑ (x' 7) _ ^//1 ∑] {x>y) ■ MMC can be calculated from the
results of a Chebychev fit to total part h∑ Σ (*, ■) . and LMC is given by the minimum
value of h∑ ∑ (x,y) ■ Furthermore, by defining a datum O to be the outermost plane resulting from the Chebychev flatness fit to the surface ∑i : parallelism can be calculated as the high point minus the low point on surface Σ2 with respect to datum Q thickness 1 can be calculated as the average of the high and low points on Σ2 with respect to O thickness 2 can be calculated as the mean value (max - min) of h∑ ∑ (x ^y) ; and thickness 3 can be calculated as the average value of MMC and LMC.
The optical profiling systems described herein optically profile two or more surfaces of a test object to determine one or more geometric properties of the object. The surfaces are each profiled with respect to a fixed datum surface or coordinate system, and the respective coordinate systems are then related to one another. As a result, the surface profiling provides absolute positions in a common coordinate system for a plurality of points on each surface. This is in contrast to relative surface profile measurements where the heights of some points on the surface are determined relative to other points on the surface to thereby measure surface texture. Thus, for the optical profiling described herein, the measurements provide the overall position (piston), tip and tilt of the object part with respect to the datum surface (i.e.. a reference surface independent from the test part), in addition to providing the form and texture of the surface.
Interferometric contributions of PCOR and PCOR dispersion are explained with reference to a two-beam scanning Michelson interferometer 600 (Figure 27). Scanning interferometer 600 operates similarly to those described above to measure the height profile of test surface 670. Interferometer 600 includes broadband source 610. beam splitter 620, scanning reference mirror 630, camera 640, and dispersion compensator 650. The interferometer is arranged to measure a height h in the z coordinate direction at each point x,y on an object part surface using interference phase information. The virtual surface H is the optical profiler datum to which all height and interference phase measurements are referenced. To first order in the angular wavenumber k = 2π/λ, the interference phase φ with respect to H is
φ (k) = 2nk (h - ζ) + (γpan + γsys ) + [τpart + τsys ) (k - k0 ) , (9)
where k0 is the nominal wavenumber, <^is the reference mirror scan position, γ t is
the part surface phase change on reflection (PCOR), and γsvs is the system phase offset
with respect to H attributable to the interferometer system. The value γsvs includes
PCOR contributions from the interferometer optics and any constant offsets resulting. e.g. from the starting position of the scan ζ. The linear dispersions coefficients τ part
and τsvs correspond to the phase offsets γ part and γsvs . respectively. The phase offsets 7 part ' Ysys are evaluated at the nominal wavenumber k0 . The index of refraction n for air and is assumed to be independent of wavenumber. Those skilled in the art will appreciate that the teachings of the invention can be extended to denser transparent media than air by taking into account the wavenumber dependence of material index. All of the terms in Eq. 9, are potentially a function of field position x,y. although for the subsequent description, the variables n. ζ, k0 are assumed to be constant over the field of view.
In scanning interferometric measurements, the light source provides broadband radiation so that interference fringes are only produced when the optical path difference (OPD) between the reference and measurement legs are within the coherence length of the broadband radiation. Thus, scanning interferometric measurements can be considered a "coherence profiling" mode in that it uses the broadband nature of the interference effect, e.g. the localization of fringe contrast or equivalently. the measurement of the rate of change of interference phase with wavenumber. Figure 28 shows an example of a coherence profiling intensity signal as the reference mirror position ζ is scanned. According to Eq. 9, the overlapping interference fringes for the various emissions of the broadband source result in a normalized intensity / given by
I = ] + V h + (τsvs + τpart )J2n - "] cos [2nk0 {h - ζ) + γ part + γsvs ] ( 10)
where V is the fringe contrast envelope. The envelope V is proportional to the F ourier Transform of the spectral distribution of the light as detected by the camera, including the spectral sensitivity of the camera itself. In Figure 28, it is assumed that the light source has a symmetric, approximately gaussian, spectral emission.
For a symmetric contrast envelope, the peak value of the fringe contrast envelope is given by the scan position for which dφ/dk = 0 . This is the stationary phase position, where the interference phase is the same independent of wavenumber, and all of the interference patterns add up constructively. More generally, it can be shown that the stationary phase condition dφ/dk = 0 corresponds approximately to the centroid of the square of the fiinge contrast envelope V. The phase gap G between the stationary phase position and lie nearest zero phase point φ = 0 position is given by
G = ( ϊpart + ϊsys ) ~ k0 ( τ'sys + τ part ) • ( )
This is a constant phase offset, independent of wavenumber k, but dependent on the system and part parameters. The phase φo is the phase at the nominal wavenumber k0 (with respect to a ζ = 0 scan position), e.g., from Eq. (9) we have
φQ = 2nk0h + ( γ par, + γsys ) . (12)
From Eq. 10 and Figure 28, it can be seen that the maximum or peak fringe contrast occurs at the scan position ζ = h + (τsvs + τpart )/2n . Thus, in one data processing embodiment, the system determines the fringe-contrast envelope V as a function of ζ, e.g., by electronic or digital conversion, for every camera pixel. It then determines the scan position ζmax for which the envelope breaches a specific value, e.g., its maximum or peak value. The corresponding height h is this scan position minus the dispersion offset:
In another signal processing method, the coherence profiling intensity signal is Fourier transformed with respect to the scan position ζ into the frequency domain (i.e.. with respect to frequency wave number k). The phase of the transformed data corresponds directly to the phase φ[[k) in Eq. 9. From this phase, the signal processor calculates the phase derivative dφ/dk , and determines height h for each camera pixel according to:
2n dk K ' " ;/ where the derivative dφ/dk is calculated for ζ = 0. Eq. 14 follows directly from Eq. 9.
From Eqs. (13) and (14), one sees that surface height measurements based on coherence profiling data can be more accurately calculated by accounting, e.g., by calibration, for PCOR dispersion for the interferometry system and the test part (e.g.. r^. and τ pan , respectively).
In addition to coherence profiling, surface profile measurements can also be based on interferometric phase profiling data where the interferometric phase φ(k) is measured directly for one or more wavenumbers k. For example, phase shifting interferometry (PSI) techniques can be used for such measurements. From Eq. 9, it is clear that if direct interferometric phase measurements are used to determine height h. accounting for PCOR γ part and γsvs (and PCOR dispersion r ., and τsrs for wave numbers other than the nominal wave number ko) improves the accuracy of the height measurement. Generally, the sensitivities to particular noise sources for coherence profiling measurements differ from those for phase profiling measurements, thus a particular technique may be preferable for a particular application, or they may be used to complement one another. One drawback of many phase profiling measurements, however, is the measured phase φ{k) includes 2π fringe ambiguity. For relatively smooth surfaces, relative fringe ambiguity over the surface may be interpolated from the data of multiple camera pixels using standard fringe unwrapping procedures. More generally, however, it is preferable to have an independent measurement, such as coherence profiling data, to remove such fringe ambiguity. Thus, to obtain absolute surface profile measurements, the coherence profiling height measurement can be used alone, or it can be used to remove the absolute fringe ambiguity from the phase profiling measurement, which may be more accurate than the coherence measurement in some cases.
In one such embodiment, the height h determined from a coherence profiling measurement is used to calculate an absolute phase profiling height measurement /?' based on phase profiling data for the phase φ0 = φ(k0 ) according to:
where Int [ ] returns the nearest integer to its argument. Eq. 15 can be applied independently to every point x,y on the part surface. Again, as is apparent from Eq. 15, accounting for PCOR χ t and γsys improves the accuracy of the absolute phase profiling measurement. Moreover, Eq. 15 implicitly depends on PCOR dispersion values τ pan and r^ through the coherence profiling determination of h.
Figure 29 shows graphically how the frequency transformed coherence profiling data φ(k) removes fringe ambiguity from a phase profiling measurement. The line dφ/dk showing the rate of change of phase is evaluated by taking a few phase data points about φ0 . The line removes the fringe-order ambiguity, provided we know the phase-axis intercept point G for the line according to Eq. 1 1. The evaluation is for a reference scan position ζ = 0 , although the raw data for determining phase and phase derivative data require a scan such as that shown in Figure 28. Note that in this graph, the gap G is the phase-axis intercept point, i.e.. the phase at zero wavenumber. To make use of the expressions above for calculating absolute height measurements, values for PCOR and PCOR dispersion are determined for the system and the part. The procedure that establishes γsvs, τsys is a system characterization. System characterization also establishes implicitly the location and shape of the optical profiler datum H System characterization involves a characterization artifact having known optical properties γart , τarl and surface form harl . The artifact is inserted temporarily in the field of view and a measurement of the x^-dependent phase profile φ0 provides the necessary information for determining the system phase offset γsvs :
γSλ , = φ0 - fan ~ 2nkQhart ■ ( 16)
where it is understood that all values potentially have an x,y field dependence. Note that the phase profile φ0 must be unwrapped, meaning that 2 π fringe jumps must be removed under the assumption that the artifact is a continuous surface. The procedure defined by Eq. (16) effectively locates the optical profiler datum H to the surface of origin of the pre-determined surface profile map hart . Thus, for example, if the artifact is known to be perfectly flat, we can set hart = 0 for all x,y and the optical profiler datum His defined as a plane coincident with the surface of the characterization artifact. Any tip/tilt or unaccounted-for surface profile information would in this case be incorporated into the system phase offset γ .
Once the γSVi is known, the value of τiVi can be determined as
*"svs = (ϊart + » s ~ Gex )/k Q ~ an ( ] 7)
where Ge is the experimentally-observed phase gap (see Figure 29):
G„ dφ \
= Φo ~k (18) dk <r=o
Here again, all of the values with the exception of n and k are expected to have an x,y field dependence related to optical distortions such as chromatic and spherical aberrations. There may also be a dependence on the tip and tilt of the part, which if it is substantial, will have to be recorded and used in the remaining calculations in much the same way as the x,y field dependence. It is not necessary to preserve the overall tip. tilt and piston of the system parameters
Ysvsi τ svs> which are partly a function of the location and orientation of the characterization artifact itself. Thus it is permitted to subtract common tip, tilt and piston terms from the field-dependent χn s, τsvs data, as long as it is done in exactly the same mamier for both , , τsv , so as to preserve the relationship between these terms. This is effected by first removing tip/tilt from yiVi, then recalculating τs, using Eq. (17). Adjusting the tip. tilt and piston of the system parameters is equivalent to adjusting the tip, tilt and piston of the optical profiler datum H. Alternatively, if we pi eserve the overall tip, tilt and piston of the system parameters ϊsys, χ ys, and if the initialization artifact is identical to the characterization artifact, it is possible to set one or more of the initial geometric parameters, e.g. a 0 , , ? 0 , , D 0
H, Z\ , Z] H, Z] to zero; realizing that these tip, tilt and piston parameters are already incorporated in
Ysysi τsys-
We have several options for a characterization artifact. The simplest is an uncoated glass part or other pure dielectric. In this case, we know with great certainty that γart = 0 and (apart from tip and tilt) τart = 0 for all x,y. Then assuming that the artifact has the exact same shape as the optical profiler datum we wish to establish, we have simply γsvs = φ0 (flat dielectric artifact) and τsvs = Ge (dielectric artifact). Note that the former expression defines the location and shape of the optical datum Hto be identical to the location and surface shape of the dielectric artifact itself.
Part PCOR values γ , can be calculated from well-established physics principles governing reflection from an interface (e.g., the Fresnal equations) and tabulated values for the complex refractive index n + ik of the part material. The part PCOR dispersion value τpart can be determined in a manner similar to the system characterization using the experimentally observed phase gap Gex and known values for
Ypart nd τsys-
' part ( Part - Gex
- sys (19) For most pure materials, we expect the height offset τparl j2n to be of the same order of magnitude as γpart/2nk0 and to have the same sign. An alternative method for determining τpart is to calculate the dispersion of calculated PCOR values using tabulated values of n + ik as a function of wavelength.
For any of the embodiments described above, a one or more controllers or computers can be used to control different components (e.g., scanning mirrors and z- stages), acquire data (e.g., from an IR camera and DMI detector), and/or make calculations (e.g, FTP, FTPO, and FPH) based on the acquired data. The analysis steps described above can be implemented in computer programs using standard programming techniques. Such programs are designed to execute on programmable computers each comprising an electronic processor, a data storage system (including memory and/or storage elements), at least one input device, and least one output device, such as a display or printer. The program code is applied to input data (e.g., images from the camera) to perform the functions described herein and generate output information (e.g., geometric properties of the test object), which is applied to one or more output devices. Each such computer program can be implemented in a high-level procedural or object-oriented programming language, or an assembly or machine language. Furthermore, the language can be a compiled or inteφreted language. Each such computer program can be stored on a computer readable storage medium (e.g., CD ROM or magnetic diskette) that when read by a computer can cause the processor in the computer to perform the analysis described herein.
1. A method for determining a geometric property of a test object, the method comprising: interferometrically profiling a first surface of the test object with respect to a first datum surface; interferometrically profiling a second surface of the test object in a second coordinate system with respect a second datum surface different from the first datum surface; providing a spatial relationship between the first and second datum surfaces; and calculating the geometric property based on the interferometrically profiled surfaces and the spatial relationship between the first and second datum surfaces.
3. The method of claim 2, wherein the interferometric profiling of the second surface provides a distance to each of a plurality points on the first surface from a corresponding point on the first datum surface.
4. The method of claim 1 , wherein the first datum surface is a portion of a plane.
8. The method of clai n 1, wherein the first and second surfaces correspond to opposite faces of the test obje;t.
9. The method of claim 1 , wherein the first and second surfaces correspond to adjacent faces of the test object.
10. The method of claim 1 , wherein the first and second surfaces are adjacent faces separated by a step height.
1 1. The method of claim 1 , wherein the first and second surfaces are displaced from one another by a distance greater than a range of the interferometric profiling of the first surface and greater than a range of the interferometric profiling of the second surface.
13. The method of claim 1 , wherein the interferometric profiling of the first surface comprises positioning the test object relative to an interferometry system and the interferometric profiling of the second surface comprises repositioning the test object relative to at least one component of the interferometry system.
14. The method of claim 13, wherein the repositioning of the test object relative to the interferometry system comprises moving the test object.
15. The method of claim 13. wherein the repositioning of the test object relative to the interferometry system comprises moving the at least one component of the interferometry system.
16. The method of claim 1, wherein the relationship between the first and second datum surfaces is defined by a distance between corresponding reference points on the first and second datum surfaces and two angles defining a relative orientation of the first and second datum surfaces.
17. The method of claim 1, further comprising determining the spatial relationship between the first and second datum surfaces.
18. The method of claim 17, wherein determining the relationship between the first and second coordinate system comprises: interferometrically profiling a first surface of a reference object with respect to the first datum surface; interferometrically profiling a second surface of the reference object with respect to the second coordinate system; providing at least one calibrated dimension for the reference object; and calculating the spatial relationship between the first and second datum surfaces based on the profiled surfaces and the at least one calibrated dimension.
19. The method of claim 18, further comprising selecting the reference object according to approximate dimensions of the test object.
20. The method of claim 1, further comprising determining the spatial relationship between the first and second datum surfaces based on at least one interferometric displacement measurement.
21. The method of claim 20, further comprising determining the spatial relationship based on at least one interferometric distance measurement and an initial calibration.
22. The method of claim 20, further comprising adjusting at least one of the first and second datum surfaces to accommodate the interferometric profiling of the first and second surfaces of the test object and interferometrically measuring the adjustment of the at least one of the first and second datum surfaces to determine the spatial relationship between the first and second datum surfaces.
23. The method of claim 15, further comprising interferometrically measuring the movement of the at least one component of the interferometry system to determine the spatial relationship between the first and second datum surfaces.
24. The method of claim 17, wherein the determining of the spatial relationship comprises: interferometrically profiling a first surface of a initialization artifact with respect to the first datum surface; interferometrically profiling a second surface of the initialization artifact with respect to the second datum surface; calculating an initial spatial relationship between the first and second datum surfaces based on at least the profiled surfaces of the initialization artifact; adjusting the first and second datum surfaces to accommodate the first and second surfaces of the test object; and interferometrically measuring at least one displacement corresponding to the adjustment of the first and second datum surfaces.
25. The method of claim 24, wherein the first and second surfaces of the initialization artifact are the front and back of a common interface.
26. The method of claim 24, further comprising providing at least one calibrated dimension for the initialization artifact, and wherein the calculation of the initial relationship is based on the profiled surfaces of the initialization artifact and the at least one calibrated dimension.
27. The method of claim 1, wherein the geometric property is flatness of the test object.
28. The method of claim 1 , wherein the geometric property is thickness of the test object.
29. The method of claim 1, wherein the geometric property is parallelism of the test object.
30. The method of claim 1, wherein the geometric property is a step height.
31. The method of claim 1 , wherein the geometric property is angular orientation of the first surface relative to the second surfaces.
32. The method of claim 31 , wherein the geometric property is perpendicularity of the first and second surfaces.
33. The method of claim 1, wherein the geometric property is roundness of the test object.
34. The method of claim 1, wherein the geometric property is defined by positions in a common coordinate system of a plurality of points on the first surface and a plurality of points on the second surface.
35. The method of claim 1, wherein the interferometric profiling of at least one of the first and second surfaces comprises performing scanning, white light interferometry.
36. The method of claim 1, wherein the interferometric profiling of at least one of the first and second surfaces comprises performing infrared, scanning interferometry.
37. The method of claim 1 , wherein the interferometric profiling of at least one of the first and second surfaces comprises performing scanning MESA interferometry.
38. The method of claim 1 , wherein the interferometric profiling of at least one of the first and second surfaces comprises performing scanning, grazing-incidence interferometry.
39. The method of c im 1 , wherein the interferometric profiling of at least one of the first and second surfaces comprises performing multiple wavelength interferometry.
40. An apparatus for determining a geometric property of a test object, the apparatus comprising: means for interferometrically profiling a first surface of the test object with respect to a first datum surface; means for interferometrically profiling a second surface of the test object with respect to a second datum surface different from the first datum system; and means for calculating the geometric property based on the interferometrically profiled surfaces and a spatial relationship between the first and second datum surfaces.
41. The apparatus of claim 40, further comprising: means for determining the spatial relationship between the first and second datum surfaces.
42. An apparatus for determining a geometric property of a test object, the method comprising: an interferometric profiling system which during operation interferometrically profiles a first surface of the test object with respect to a first datum surface and interferometrically profiles a second surface of the test object with respect to a second datum surface different from the first datum surface; and an electronic processor coupled to the interferometric profiling system, wherein during operation the electronic processor calculates the geometric property based on the interferometrically profiled surfaces and a spatial relationship between the first and second datum surfaces.
43. The apparatus of claim 42, wherein the interferometric profiling system includes a mount for supporting the test object, wherein the mount is adjustable between a first position for exposing the first surface of the test object and defining the datum surface and a second position for exposing the second surface of the test object and defining the second datum surface.
44. The apparatus of claim 42, wherein the interferometric profiling system comprises an interferometric optical profiler having a first viewing port for viewing the first surface of the test object and a second viewing port for viewing the second surface of the test object.
45. The apparatus of claim 44, wherein the optical profiler comprises a first camera positioned to record a field of view for the first viewing port and a second camera positioned to record a field of view for the second viewing port.
46. The apparatus of claim 44, wherein the optical profiler comprises a camera positioned to record a split field of view for the first and second viewing ports.
47. The apparatus of claim 44, wherein the optical profiler comprises at least one source of EM radiation.
48. The apparatus of claim 47, wherein the optical profiler further comprises a first optic positioned to direct a first portion of the EM radiation towards the first viewing port and a second portion of the EM radiation towards the second viewing ports.
49. The apparatus of claim 48. wherein the first optic is a beam splitting optic positioned to reflect the first portion of the EM radiation towards the first viewing port, reflect the second portion of the EM radiation towards the second viewing port, and transmit at least one additional portion of the incident EM radiation through the beam splitting optic.
50. The apparatus of claim 49, wherein the optical profiler further includes a reflective reference surface positioned to receive the at least one additional portion of the incident EM radiation transmitted through the beam splitting optic.
51. The apparatus of claim 50, wherein the optical profiler further includes a transducer coupled to the reflective reference surface for scanning the position of the reflective reference surface.
52. The apparatus of claim 49. wherein the optical profiler further comprises a first viewing port optic supported by a first movable stage, the first viewing port optic positioned to direct at least one part of the first portion of the EM radiation towards the first surface of the test object and the first movable stage adjustable to accommodate the interferometric profiling of the first surface of the test object.
53. The apparatus of claim 52, wherein the optical profiler further comprises a second viewing port optic supported by a second movable stage, the second viewing port optic positioned to direct at least one part of the second portion of the EM radiation towards the second surface of the test object and the second movable stage adjustable to accommodate the interferometric profiling of the second surface of the test object.
54. The apparatus of claim 52, wherein the first reflective optic is a roof mirror.
55. The apparatus of claim 52, wherein the optical profiler further includes a first fold mirror for further directing the at least one part of the first portion of the EM radiation towards the first surface of the test object.
56. The apparatus of claim 53 further comprising a displacement measuring interferometer positioned to measure changes in the spatial relationship between the first and second datum surfaces caused by at least one of an adjustment to the first movable stage and an adjustment to the second movable stage.
57. The apparatus of claim 42, wherein the interferometric profiling system comprises a first interferometric optical profiler for viewing the first surface of the test object and a second interferometric optical profiler for viewing the second surface of the test object.
58. The apparatus of claim 57, wherein the first optical profiler is movable relative to the second optical profiler to adjust the spatial relationship between the first and second datum surfaces.
59. The apparatus of claim 58, further comprising a displacement measuring interferometer positioned to measure changes in the spatial relationship between the first and second datum surfaces caused by relative movement of the first and second optical profilers.
60. The apparatus of claim 42, wherein the interferometric profiling system comprises a moveable stage adjustable from a first position defining the first datum surface to a second position defining the second datum surface.
61. The apparatus of claim 42, further comprising a gauge object having first and second surfaces, the first surface being positioned to be profiled by the interferometric profiling system with respect to the first datum surface and the second surface being positioned to be profiled by the interferometric profiling system with respect to the second datum surface.
62. The apparatus of claim 61 , wherein the electronic processor determines the spatial relationship between the first and second datum surfaces based on interferometric profiling measurements of the first and second surfaces of the gauge object provided by the first and second optical profilers.
63. The apparatus of claim 61. wherein the gauge object has at least one calibrated dimension and wherein the electronic processor determines the spatial relationship between the first and second datum surfaces based on interferometric profiling measurements of the first and second surfaces of the gauge object provided by the first and second optical profilers and the at least one calibrated dimension.
64. The apparatus of claim 61. wherein the gauge object is positioned to be in a field of view of the interferometric profiling system during interferometric profiling of the test object.
65. An apparatus of c aim 42, further comprising a displacement measuring interferometer positioned to measure the spatial relationship between the first and second datum surfaces.
66. The apparatus of claim 42, wherein the electronic processor uses at least one value indicative of PCOR dispersion in the interferometric profiling system and the test object to calculate the geometric property.
67. An apparatus for determining a geometric property of a test object, the apparatus comprising: an interferometric profiling system which during operation interferometrically profiles a first surface of the test object with respect to a first datum surface and interferometrically profiles a second surface of the test object with respect to a second datum surface, wherein the interferometric profiling system comprises at least one movable stage for adjusting the position 'of the first datum surface and the second datum surface; a displacement measuring interferometer positioned to measure a change in a relative position of the first and second datum surface caused by an adjustment to the at least one movable stage; and an electronic processor coupled to the interferometric profiling system and the displacement measuring interferometer, wherein during operation the electronic processor calculates the geometric property based on the interferometrically profiled surfaces and the relative position of the first and second datum surfaces.
68. The apparatus of claim 67, wherein the interferometric profiling system comprises a second moveable stage, and wherein during operation the first-mentioned movable stage adjusts the position of the first datum surface and the second movable stage adjusts the position of the second datum surface.
69. The apparatus of claim 67, wherein the at least one movable stage comprises a first movable stage adjustable from a first position defining the first datum surface to a second position defining the second datum surface.
70. The apparatus of claim 67, wherein the displacement measuring interferometer provides multiple axes of measurement.
71. The apparatus of claim 67, wherein the interferometric profiling system is a scanning interferometric profiling system using infrared wavelengths.
72. A method for determining a geometric property of a test object, the method comprising: profiling a first surface of the test object in a first coordinate system; profiling a second surface of the test object in a second coordinate system different from the first coordinate system; determining a spatial relationship between the first and second coordinate system based on at least one interferometric distance measurement; and calculating the geometric property based on the profiled surfaces and the relationship between the first and second coordinate system.
73. A method for determining a geometric property of a test object, the method comprising: interferometrically profiling a first surface of the test object with respect to a first datum surface; interferometrically profiling a second surface of the test object with respect to a second datum surface different from the first datum surface; determining a spatial relationship between the interferometrically profiled surfaces which accounts for PCOR dispersion; and calculating the geometric property based on the interferometrically profiled surfaces and the spatial relationship.
74. The method of claim 1, wherein the test object is partially transparent.
75. The method of claim 74, wherein the geometric property is determined by positions of a plurality of point on a front surface of the test object relative to positions of a plurality of points on a back surface of the test object
76. The method of claim 1 , wherein the first and second surfaces of the test object are interferometrically profiled from a common side and the first and second datum surfaces are spaced from one another by a distance greater than a profiling range η of an interferometry system used for the interferometric profiling steps.
77. The method of claim 76, wherein the interferometry system used for the interferometric profiling steps comprises a reference object having a partially reflective, first surface and a reflective, second surface, the first surface defining the first datum surface and the second surface defining the second datum surface.
78. The method of claim 77, wherein the relationship is defined by the spatial separation between the first and second surfaces of the reference object.
79. An optical profiling system comprising: a broadband source; a scanning interferometer which during operation directs a first wavefront along a reference path including a partially reflective first surface and a reflective second surface and a second wavefront along a measurement path contacting a measurement object, and. after the second wavefront contacts the measurement object, combines the wavefronts to produce an optical interference pattern; a detector producing interference data in response to the optical interference pattern; an electronic processor coupled to the detector for analyzing the interference data a scanning controller coupled to the scanning interferometer and the electronic processor, wherein during operation the scanning controller causes the scanning interferometer to adjust the position of the first and second surfaces.
80. The interferometry system of claim 79, wherein the partially reflective first surface of the scanning interferometer defines a first datum surface and the reflective second surface defines a second datum surface, and wherein during operation the electronic processor calculates a geometric property of the test object based on the interference data and a relationship between the first and second datum surfaces.
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JP2001558688A JP5112588B2 (en) 2000-01-25 2001-01-25 Method and apparatus for measuring the shape and geometric dimensions of precision industrial parts
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