Abstract:
A sample investigation system (ES) in functional combination with an alignment system (AS), and methodology of enabling very fast, (eg. seconds), sample height, angle-of-incidence and plane-of-incidence adjustments, with application in mapping ellipsometer or the like systems.

Description:
RELATION TO EXISTING APPLICATIONS AND PATENTS 
     This Application directly Claims Benefit of Provisional Application Ser. No. 61/127,062 Filed May 9, 2008. This Application is a CIP of 11/890,391 filed Aug. 5, 2007 now U.S. Pat. No. 7,746,471 and therefrom Claims benefit of Provisional 60/836,232 Filed Aug. 9, 2006, and threvia is a CIP of patent application Ser. No. 11/105,852 filed Apr. 14, 2005, now U.S. Pat. No. 7,277,171 and therevia this Application Claims benefit of Provisional Applications 60/564,747 Filed Apr. 23, 2004, and 60/580,314 Filed Jun. 17, 2004. This Application is further a Continuation-In-Part of Utility application Ser. No. 10/829,620 Filed Apr. 22, 2004 now U.S. Pat. No. 7,193,710; and of application Ser. No. 10/925,333 Filed Aug. 24, 2004 now U.S. Pat. No. 7,265,838, and therevia of 10/050,802 Filed Jan. 15, 2002, (now U.S. Pat. No. 6,859,278). Via the above Applications this Application is further a Continuation-In-Part of Utility application Ser. No. 10/925,333 Filed Aug. 24, 2004, and of Ser. No. 10/829,620 Filed Apr. 22, 2004, and is a Divisional of application Ser. No. 10/050,802 Filed Jan. 15, 2002; and via the above Applications Claims Benefit of Provisional Application Ser. No. 60/261,243 Filed Jan. 16, 2001, 60/263,874 Filed Jan. 25, 2001, 60/287,784 Filed May 2, 2001. This Application is further a CIP of Utility application Ser. No. 10/699,540 Filed Nov. 1, 2003, now U.S. Pat. No. 7,158,231 and application Ser. No. 10/857,774 Filed May 28, 2004, now U.S. Pat. No. 7,274,450 and therevia Claims benefit of Provisional Applications 60/424,589 Filed Nov. 7, 2002, 60/427,043 Filed Nov. 18, 2002, and 60/480,851 Filed Jun. 24, 2003. This Application is further directly a CIP of application Ser. No. 11/704,545 Filed Feb. 10, 2007 now U.S. Pat. No. 7,426,030 and therevia Claims Benefit of Provisional Application Ser. No. 60/772,926 Filed Feb. 13, 2006; and is a CIP of application Ser. No. 11/145,470 Filed Jun. 6, 2005, now U.S. Pat. No. 7,327,456 and therevia of Ser. No. 10/376,677 Filed Feb. 28, 2003 now U.S. Pat. No. 6,982,792 and from Ser. No. 09/531,877 Filed Mar. 21, 2000; now U.S. Pat. No. 6,535,286 and from application Ser. No. 10/178,723 filed Jun. 24, 2002 now U.S. Pat. No. 6,950,182; and Ser. No. 09/583,229 filed May 30, 2000 now U.S. Pat. No. 6,804,004; and from Ser. No. 09/864,840 filed May 24, 2001 now U.S. Pat. No. 6,456,376; and Ser. No. 09/845,548 filed Apr. 30, 2001 now U.S. Pat. No. 6,585,128; and Claims benefit of Provisional Application Ser. Nos. 60/300,714 filed Jun. 26, 2001, and 60/424,589 filed Nov. 7, 2002, and 60/427,043 filed Nov. 18, 2002 and 60/431,489 filed Dec. 6, 2002. This Application also is a CIP of application Ser. No. 10/849,740 Filed May 20, 2004 now U.S. Pat. No. 7,385,697. This Application is also a CIP of application Ser. No. 11/105,852 Filed Apr. 14, 2005 also therevia Claims benefit of Provisional Applications 60/564,747 Filed Apr. 23, 2004, and 60/580,314 Filed Jun. 17, 2004. This Application is further a Continuation-In-Part of Utility application Ser. No. 10/829,620 Filed Apr. 22, 2004; and of Ser. No. 10/925,333 Filed Aug. 24, 2004, and therevia of Ser. No. 10/050,802 Filed Jan. 15, 2002, (now U.S. Pat. No. 6,859,278). This Application is further a Continuation-In-Part of Utility application Ser. No. 10/925,333 Filed Aug. 24, 2004, and of Ser. No. 10/829,620 Filed Apr. 22, 2004, and is a Divisional of Ser. No. 10/050,802 Filed Jan. 15, 2002; and via the above Applications Claims Benefit of Provisional Application Ser. No. 60/261,243 Filed Jan. 16, 2001, 60/263,874 Filed Jan. 25, 2001, 60/287,784 Filed May 2, 2001. 
     This Application also is a CIP from application Ser. No. 11/784,750 Filed Apr. 10, 2007, and therevia from Provisional Application 60/878,799 Filed Jan. 5, 2007. 
    
    
     TECHNICAL AREA 
     The present invention relates to the practice of ellipsometry, polarimetry, reflectometry and spectrophotometry; and more particularly to a sample investigation system and method of enabling very fast sample height, angle-of-incidence and plane-of-incidence adjustments, with application in a sample mapping or the like systems. 
     BACKGROUND 
     Ellipsometry is a well known approach to determining physical and optical properties of samples. To obtain accurate results, however, requires that values for certain adjustable parameters, including the distance between the ellipsometer and the sample under investigation, (eg. the “height” of the sample), and the angle-of-incidence and plane-of-incidence of the ellipsometer beam with respect to the sample, be known. Where single point on a sample is to be investigated, alignment procedures are well established which provide the required values within acceptable time constraints, (eg. many seconds to a minute or so). However, in situations wherein many points on a large sample, (eg. a mapping of the sample is to be performed), the time required to do conventional alignments at each of the many point investigated can introduce unacceptable, (eg. 5 seconds each), time delays in achieving desired results. The present invention provides an alignment system, and method of its use, which enables very fast, (eg. on the order a second or two), setting of sample height, and angle, and plane-of-incidence, at each spot on the sample to be investigated. The present invention also discloses a relevant sample mapping system which applies the alignment system. 
     As further insight, it is noted that Pending patent application Ser. No. 11/890,391 Filed Aug. 5, 2007 provides priority back to application Ser. No. 11/105,852, Filed Apr. 14, 2005, with Priority back to Apr. 23, 2004 via Provisional Application Ser. No. 60/564,747, and describes a substantially self contained flying ellipsometer, polarimeter, reflectometer or spectrophotometer system that provides for moving a combined source and detector of electromagnetic radiation over the a surface of a sample in two, (eg. “X” and “Y”), orthogonal dimensions to enable positioning it at desired locations on, and offset distance from sample in a “Z” dimension corresponding to a distance between said combined source and detector and said sample, and which enables easy sequential setting of different Angles-of-Incidence of a beam of electromagnetic radiation to a surface of said sample. 
     As related in the 391 Pending Application, Ellipsometer Systems generally include a source of a beam of electromagnetic radiation, a Polarizer, which serves to impose a known, (typically linear), state of polarization on a beam of electromagnetic radiation, a Stage for supporting a sample, and an Analyzer which serves to select a polarization state in a beam of electromagnetic radiation after it has interacted with a material system, and pass it to a Detector System for analysis therein. As well, one or more Compensator(s) can be present and serve to affect a phase retardance between orthogonal components of a polarized beam of electromagnetic radiation. A number of types of ellipsometer systems exist, such as those which include rotating elements and those which include modulation elements. Those including rotating elements include Rotating Polarizer (RP), Rotating Analyzer (RA) and Rotating Compensator (RC). A preferred embodiment is a Rotating Compensator Ellipsometer System because they do not demonstrate “Dead-Spots” where obtaining ellipsometric data is difficult. They can read PSI and DELTA of a Material System over a full Range of Degrees with the only limitation being that if PSI becomes essentially zero (0.0), one can&#39;t then determine DELTA as there is not sufficient PSI Polar Vector Length to form the angle between the PSI Vector and an “X” axis. In comparison, Rotating Analyzer and Rotating Polarizer Ellipsometers have “Dead Spots” at DELTA&#39;s near 0.0 or 180 Degrees and Modulation Element Ellipsometers also have a “Dead Spot” at PSI near 45 Degrees). The utility of Rotating Compensator Ellipsometer Systems should then be apparent. Another benefit provided by Rotating Compensator Ellipsometer Systems is that the Polarizer (P) and Analyzer (A) positions are fixed, and that provides benefit in that polarization state sensitivity to input and output optics&#39; during data acquisition is essentially non-existent. This enables relatively easy use of optic fibers, mirrors, lenses etc. for input/output. 
     Typical construction of spectrophotometer, reflectometer, polarimeter, ellipsometer and the like systems, (eg. Rotating Analyzer, Rotating Polarizer, Rotating Compensator, Modulator Element Ellipsometer), provides a Sample Supporting Stage which is substantially fixed in location. Functionally oriented with respect thereto are a Substantially Fixed Position Source Means (S) for providing a beam of electromagnetic radiation at an oblique angle to said Sample Supporting Stage, and a Substantially Fixed Position Data Detector Means (D) for intercepting Electromagnetic Radiation which Reflects (or Transmits through), a Sample placed on said Sample Supporting Stage. Typical procedure is to place a Sample onto the Sample Supporting Stage, cause a beam of Electromagnetic Radiation to impinge thereonto, and record data produced by the Data Detector Means in response to electromagnetic radiation which enters thereinto, which data is analyzed to provide insight into Sample Optical and Physical properties. Said procedure can include adjustment of the Sample Supporting Stage, or the source and detector of electromagnetic radiation in an “X”-“Y” Plane, and along a “Z” direction perpendicular to its surface, (ie. a vertical position adjustment where the Electromagnetic Radiation approaches the Sample at an oblique angle from a laterally located Source). This purpose of said “Z” adjustment is, for instance, to enable the directing of a beam of Electromagnetic Radiation Reflected from a Sample placed on said Sample Supporting Stage into the Data Detector without moving the Data Detector so it intercepts a beam exiting said Sample. It should be appreciated then that conventional Reflectometer, Ellipsometer and Polarimeter Systems which include provision for such Sample positioning adjustment and orientation with respect to an impinging Electromagnetic beam, typically do so by allowing the Sample Supporting Stage position to be adjusted, rather than by effecting simultaneous change in location of the Source and Data Detector with respect to the Sample Supporting Stage, because it is far simpler to implement Sample Supporting Stage location change. However, an alternative is mount a Reflectometer, Spectrophotometer, Ellipsometer, Polarimeter or the like System to a means for moving it in an “X”-“Y” Plane, and along a “Z” direction perpendicular to its surface of the Sample with respect to a substantially fixed position Stage for supporting a Sample. In either case, however, a relative motion occurs between the Reflectometer, Ellipsometer, Polarimeter or the like System and a sample. 
     The present invention then breaks with conventional practice by, while typically providing a substantially fixed position Stage for supporting a Sample, providing a Reflectometer, Spectrophotometer, Ellipsometer, Polarimeter or the like System which is mounted to a positioning system which allows adjustment its location in an “X”-“Y” Plane, and along a “Z” direction perpendicular to its surface of the Sample. The present invention then, allows investigation of a large Sample at many locations thereof. 
     Continuing, while present invention systems can be applied in any material system investigation system such as Polarimeter, Reflectometer, Spectrophotometer and the like Systems, an important application is in Ellipsometer Systems, whether monochromatic or spectroscopic. It should therefore be understood that Ellipsometry involves acquisition of sample system characterizing data at single or multiple Wavelengths, and at one or more Angle(s)-of-Incidence (AOI) of a Beam of Electromagnetic Radiation to a surface of the sample system. 
     A typical goal in ellipsometry is to obtain, for each wavelength in, and angle of incidence of said beam of electromagnetic radiation caused to interact with a sample system, sample system characterizing PSI and DELTA values, (where PSI is related to a change in a ratio of magnitudes of orthogonal components r p /r s  in said beam of electromagnetic radiation, and wherein DELTA is related to a phase shift entered between said orthogonal components r p  and r s , caused by interaction with said sample system:
 
TAN(ψ) e   (iΔ)   =r   p   /r   s  
 
While Data taken at one (AOI) and one or multiple wavelengths is often sufficient to allow ellipsometric characterization of a sample system, the results of Ellipsometric Investigation can be greatly enhanced by using multiple (AOI&#39;s) to obtain additional data sets. However, while it is relatively easy to provide Wavelength change without extensive difficult physical Ellipsometer System Orientation change, it is typically difficult to change the Angle-of-Incidence (AOI) that a Beam of Electromagnetic Radiation makes to a surface of a sample system. An (AOI) change requires that both the Source of the Electromagnetic Beam and the Detector must be re-positioned and aligned, and such is tedious and time consuming. The present invention therefore can provide means to easily effect (AOI) change. It is also noted that ellipsometric data is typically analyzed by proposing a mathematical model for the sample and regressing it on to said ellipsometric data to arrive at values for parameters in the mathematical model which meet, for instance, a best fit based on a least square error criteria. Further, it is known to obtain data from multiple similar samples and simultaneously regress the similar models onto the different ellipsometric data sets. This technique can break correlation between thickness and refractive index, where the samples have different thicknesses. A similar approach can be applied to data acquired from multiple spots on a single sample.
 
     A patent to Finarov, U.S. Pat. No. 5,764,365 is disclosed as it describes a system for moving an ellipsometer beam over a large two-dimensional area on the surface of a sample system, which system utilizes beam deflectors. 
     A patent to Berger et al., U.S. Pat. No. 5,343,293 describes an Ellipsometer which comprises prisms to direct an electromagnetic beam onto a sample system. 
     A patent to Canino, U.S. Pat. No. 4,672,196 describes a system which allows rotating a sample system to control the angle of incidence of a beam of electromagnetic radiation thereonto. Multiple detectors are present to receive the resulting reflected beams. 
     A patent to Bjork et al., U.S. Pat. No. 4,647,207 describes an ellipsometer system in which reflecting elements are moved into the path of a beam of electromagnetic radiation. 
     U.S. Pat. No. 6,081,334 to Grimbergen et al. describes a system for detecting semiconductor end point etching including a means for scanning a beam across the surface of a substrate. 
     A patent to Ray, U.S. Pat. No. 5,410,409 describes a system for scanning a laser beam across a sample surface. 
     U.S. Pat. No. 3,874,797 to Kasai describes means for directing a beam of electromagnetic radiation onto the surface of a sample using totally internally reflecting prisms. 
     U.S. Pat. No. 5,412,473 to Rosencwaig et al., describes a ellipsometer system which simultaneously provides an electromagnetic beam at a sample surface at numerous angles of incidence thereto. 
     A patent to Chen et al., U.S. Pat. No. 5,581,350 is identified as it describes the application of regression in calibration of ellipsometer systems. 
     A Search of Patents which contain both “ellipsometer” and “Mapping” provided patents Nos.:
         U.S. Pat. No. RE40,225 to Finarov;   U.S. Pat. No. RE38,153 to Finarov;   U.S. Pat. No. 6,678,043 to Vurens;   U.S. Pat. No. 7,099,010 to Schulz;   U.S. Pat. No. 7,295,330 to Chow;   U.S. Pat. No. 7,327,444 to Naka et al.       

     An article by Johs, titled “Regression Calibration Method For Rotating Element Ellipsometers”, which appeared in Thin Film Solids, Vol. 234 in 1993 is also identified as it predates the Chen et al. patent and describes an essentially similar approach to ellipsometer calibration. 
     Even in view of the prior art, need remains for:
         an ellipsometer system which enables very fast, (eg. on the order a second or two), setting of sample height, and angle, and plane-of-incidence, at each spot on the sample to be investigated and a sample mapping system which applies the alignment system; and   an ellipsometer system which is functionally mounted in a three dimension location means for positioning said selected system at points in a three dimensional setting, including rotational capability.       

     DISCLOSURE OF THE INVENTION 
     The present invention comprises a method of aligning a sample in an ellipsometer system. Said ellipsometer system can be described as comprising:
         a source of a beam of electromagnetic radiation;   a polarizer;   a stage for supporting a sample;   an analyzer;   a data detector;   means for adjusting the relative “height” positioning between said stage for supporting a sample and, as a unit, said source of a beam of electromagnetic radiation and data detector; as well as means for translating relative positioning of said sample with respect to said source of an ellipsometer beam of electromagnetic radiation and said data detector, along two orthogonal axes, and optionally means for adjusting the relative orientation of the ellipsometer systems with respect to said sample to set the angle and plane of incidence of said ellipsometer beam with respect to a surface of said sample.       

     Said ellipsometer system can comprise at least one compensator and/or focusing means between said source of a beam of electromagnetic radiation and said data detector. 
     In use a beam of electromagnetic radiation from said source thereof approaches said sample at an oblique angle-of-incidence and reflects therefrom into said data detector. 
     Said method of aligning a sample further comprises the steps of:
         a) functionally mounting a sample alignment system to said ellipsometer system, which sample alignment system comprises:
           an alignment source of an alignment beam of electromagnetic radiation;   a first alignment beam focusing means for focusing an alignment beam of electromagnetic radiation provided from said source thereof onto a sample on said ellipsometer system stage for supporting a sample;   a second alignment focusing means for focusing alignment beam electromagnetic radiation which reflects from said sample onto a two dimensional detector array; and   said two dimensional detector array;
 
such that in use an alignment beam of electromagnetic radiation from said source thereof is focused onto said sample at an oblique angle-of-incidence and reflects therefrom and is focused onto said two dimensional detector array.
 
Said sample alignment system can optionally further comprise:
   
           between said second alignment focusing means and said two dimensional detector array a beam splitter which diverts a portion of the alignment beam electromagnetic radiation which reflects from said sample to a secondary two dimensional detector array, and said secondary two dimensional detector array.
 
Said ellipsometer and alignment system are mounted with respect to one another such that the ellipsometer beam of electromagnetic radiation and said alignment beam of electromagnetic radiation impinge on said sample at substantially the same location.
 
Said method further can also comprise:
 
prior to step e, performing steps b and c at least once, said steps b and c being:
   b) while:
           monitoring output intensity from said data detector causing a beam of electromagnetic radiation from said source thereof to approach said sample at an oblique angle-of-incidence and reflect therefrom into said data detector,   
           adjusting the means for adjusting the relative “height” positioning between said stage for supporting a sample, and, as a unit, said source of a beam of electromagnetic radiation and data detector, until output from said data detector is of a desirable intensity; and   c) causing the source of an alignment beam of electromagnetic radiation from said source thereof to approach said sample at an oblique angle-of-incidence and reflect therefrom onto said two dimensional detector array and identifying the location on said two dimensional detector array as an aligned position.
 
Said method can then further comprise performing steps d, e and f a plurality of times, said steps d, e and f being:
   d) using said means for translating relative positioning of said sample with respect to, as a unit, said source of an ellipsometer beam of electromagnetic radiation and said data detector, along two orthogonal axes, causing relative translation of said sample along at least one of said orthogonal axes so that a new spot on said sample is investigated by said ellipsometer beam, and such that the location at which the alignment beam reflected from said sample surface in step c appears on the two dimensional detector array, possibly at a different location than said aligned position;   e) if necessary, adjusting the means for adjusting the relative “height” positioning between said stage for supporting a sample and, as a unit, said source of a beam of electromagnetic radiation and data detector, until said alignment beam reflected from said sample surface in step c appears on the two dimensional detector array at said aligned position;   f) with the above adjustment set, acquiring ellipsometric data from said data detector.
 
Said method can further comprise definitely providing:
   between said second alignment focusing means and said two dimensional detector array, a beam splitter which diverts a portion of the alignment beam electromagnetic radiation which reflects from said sample to a secondary two dimensional detector array and said secondary two dimensional detector array; and   means for adjusting the relative orientation of the ellipsometer with respect to said sample to set the angle and plane of incidence of said ellipsometer beam with respect to a surface of said sample.
 
Said method can then further comprise, prior to step e:
   while causing a beam of electromagnetic radiation from said source thereof to approach said sample at an oblique angle-of-incidence and reflect therefrom into said data detector, monitoring the output from the data detector and adjusting the means for adjusting the relative orientation of the ellipsometer with respect to said sample to set the angle and plane of incidence of said ellipsometer beam with respect to a surface of said sample until the intensity of the data detector output is maximized, and so that electromagnetic radiation from said alignment source thereof reflects from said sample and, via said beam splitter, appears on said secondary two dimensional detector array, and identifying the location on said secondary two dimensional detector array as an aligned position;
 
and in which said method, after practice of the step d causing of relative translation of said sample along at least one of said orthogonal axes so that a new spot on said sample is investigated by said ellipsometer beam, practice of step e, which step e further comprises:
   e) adjusting the means for adjusting the relative orientation of the ellipsometer with respect to said sample to set the angle and plane of incidence of said ellipsometric beam with respect to a surface of said sample until said alignment beam reflected from said sample surface in step c appears on the two dimensional detector array at said aligned position;
 
followed by practice of step f.
       

     A more comprehensive recitation of the method of aligning a sample in an ellipsometer system comprises, providing an ellipsometer system which comprises:
         a source of a beam of electromagnetic radiation;   a polarizer;   a stage for supporting a sample;   an analyzer;   a data detector;   means for adjusting the relative “height” positioning between said stage for supporting a sample and, as a unit, said source of a beam of electromagnetic radiation and data detector; as well as means for translating relative positioning of said sample with respect to said source of an ellipsometer beam of electromagnetic radiation and said data detector, along two orthogonal axes, and means for adjusting the relative orientation of the ellipsometer with respect to said sample to set the angle and plane of incidence of said ellipsometer beam with respect to a surface of said sample.       

     Said system optionally can comprise at least one polarizer, analyzer, compensator or focusing means between said source of a sample investigation beam of electromagnetic radiation and said data detector. 
     In use a beam of electromagnetic radiation from said source thereof approaches said sample at an oblique angle-of-incidence and reflects therefrom into said data detector. 
     Said method also comprises the steps of: 
     
         
         
           
             a) functionally mounting a sample alignment system to said ellipsometer system, which sample alignment system comprises:
           an alignment source of an alignment beam of electromagnetic radiation;   a first alignment beam focusing means for focusing an alignment beam of electromagnetic radiation provided from said source thereof onto a sample on said ellipsometer system stage for supporting a sample;   a second alignment focusing means for focusing alignment beam electromagnetic radiation which reflects from said sample onto a two dimensional detector array; and   said two dimensional detector array,
 
such that in use an alignment beam of electromagnetic radiation from said source thereof is focused onto said sample at an oblique angle-of-incidence and reflects therefrom and is focused onto said two dimensional detector array.
 
Said sample alignment system further comprises:
   
         
             between said second alignment focusing means and said two dimensional detector array, a beam splitter which diverts a portion of the alignment beam electromagnetic radiation which reflects from said sample to a secondary two dimensional detector array, and said secondary two dimensional detector array;
 
said ellipsometer and alignment system being mounted with respect to one another such that the ellipsometer beam of electromagnetic radiation and said alignment beam of electromagnetic radiation impinge on said sample at substantially the same location.
 
Said method then further comprises, prior to step e, performing steps b and c at least once, said steps b an c being:
 
             b) while causing a beam of electromagnetic radiation from said source thereof to approach said sample at an oblique angle-of-incidence and reflect therefrom into said data detector, monitoring the output from the data detector and adjusting the means for adjusting the relative orientation of the ellipsometer with respect to said sample to set the angle and plane of incidence of said ellipsometer beam with respect to a surface of said sample until the intensity of the data detector output is maximized, and so that electromagnetic radiation from said alignment source thereof reflects from said sample and, via said beam splitter, appears on said secondary two dimensional detector array, and identifying the location on said secondary two dimensional detector array as an aligned position; and 
             c) while monitoring output intensity from said data detector causing a beam of electromagnetic radiation from said source thereof to approach said sample at an oblique angle-of-incidence and reflect therefrom into said data detector adjusting the means for adjusting the relative “height” positioning between said stage for supporting a sample, and, as a unit, said source of a beam of electromagnetic radiation and data detector until output from said data detector is of a desirable intensity and identifying the location on said two dimensional detector array as an aligned position.
 
Said method then further comprises performing steps d, e and f a plurality of times, said steps d, e and f being:
 
             d) using said means for translating relative positioning of said sample with respect to, as a unit, said source of an ellipsometer beam of electromagnetic radiation and said data detector, along two orthogonal axes, causing relative translation of said sample along at least one of said orthogonal axes so that a new spot on said sample is investigated by said ellipsometer beam, and such that the location at which the alignment beam reflected from said sample surface in step c appears on the two dimensional detector array, possibly at a different location than said aligned position; 
             e) if necessary, adjusting the means for adjusting the relative “height” positioning between said stage for supporting a sample and, as a unit, said source of a beam of electromagnetic radiation and data detector, until said alignment beam reflected from said sample surface in step c appears on the two dimensional detector array at said aligned position and adjusting the means for adjusting the relative orientation of the ellipsometer with respect to said sample to set the angle and plane of incidence of said ellipsometric beam with respect to a surface of said sample until said alignment beam reflected from said sample surface in step c appears on the secondary two dimensional detector array at said aligned position; 
             f) with the above adjustment set, acquiring ellipsometric data from said data detector. 
           
         
       
    
     In the foregoing it is noted that steps b and c are practiced “at least once”, while steps d, e and f are practiced “a plurality of times”. This language is used to indicate that while step c, and optionally step b, could be practiced every time steps d, e and f are practiced at a location on a sample, it is often sufficient to practice steps c, (and optionally b), only once each followed by practice of steps d, e and f many times. This is because the sample can be sufficiently planar so that setting height, angle and plane of incidence once, for many locations thereupon, can be sufficient. Hence, while the methodology can involve practicing step c, and optionally step b, each time steps d, e and f are practiced, typically this will not be the case. 
     Present invention methodology of investigating a sample can further comprise analyzing ellipsometric data acquired from said data detector in step f, and that analysis can involve the acquiring of ellipsometric data involves repeating steps b-f at least twice to obtain ellipsometric data from at least two spots on said sample, and in which the analysis comprises simultaneous regression onto data obtained from said at least two spots on said sample. 
     It is also noted that steps wherein relative “height” positioning between said stage for supporting a sample and, as a unit, is involved, the data detector output is set to be of a “desirable intensity”. This is to indicate that it need not be “maximized”. However, where relative orientation of the ellipsometer with respect to said sample to set the angle and plane of incidence of said ellipsometer beam with respect to a surface of said sample is involved, maximizing the data detector output is practiced. This is because if said angle and/or plane of incidence is not set to direct a beam into the data detector no data detector output is obtained and the range over which a signal is detected is small. That is, the adjustment for the angle and plane of incidence is critical within tight limits in order to obtain data at all, whereas the height adjustment does not have such tight limits. Practice might include “maximizing” the data detector output while adjusting for height, but said maximization need not in the present invention. 
     The foregoing methods can then involve performing at least one selection from the group consisting of:
         storing at least some data provided by said data detector in machine readable media;   analyzing at least some of the data provided by said data detector and storing at least some of the results of said analysis in machine readable media;   displaying at least some data provided by said data detector by electronic and/or non-electronic means;   analyzing at least some of the data provided by said data detector and displaying at least some of the results of said analysis by electronic and/or non-electronic means;   causing at least some data provided by said data detector to produce a signal which is applied to provide a concrete and tangible result;   analyzing at least some of the data provided by said data detector and causing at least some thereof to produce a signal which is applied to provide a concrete and tangible result.       

     While the foregoing discussed the very relevant application of an exemplary ellipsometer system, the Claims should be broadly considered to involve any material system investigation system, such as:
         an ellipsometer;   a polarimeter;   a reflectometer;   a spectrophotometer; and   a Mueller Matrix measuring system.
 
In that light, the present invention can be recited as also comprising a combination sample investigation system and alignment system comprising a selection from the group consisting of:
   an ellipsometer;   a polarimeter;   a reflectometer;   a spectrophotometer; and   a Mueller Matrix measuring system;
 
which comprises:
   a source of a sample investigation beam of electromagnetic radiation;   a stage for supporting a sample;   a data detector;   means for adjusting the relative “height” positioning between said stage for supporting a sample and, as a unit, said source of a sample investigation beam of electromagnetic radiation and data detector; as well as, optionally, means for translating relative positioning of said sample with respect to said source of a sample Investigation beam of electromagnetic radiation and said data detector, along two orthogonal axes, and optionally means for adjusting the relative orientation of the sample investigation system with respect to said sample to set the angle and plane of incidence of said sample investigation beam of electromagnetic radiation with respect to a surface of said sample.       

     Said system optionally can comprise at least one polarizer, analyzer, compensator or focusing means between said source of a sample investigation beam of electromagnetic radiation and said data detector. 
     In use a sample investigation beam of electromagnetic radiation from said source thereof approaches said sample at an oblique angle-of-incidence and reflects therefrom into said data detector. 
     Said sample investigation system optionally comprises an alignment system which comprises:
         an alignment source of an alignment beam of electromagnetic radiation;   a first alignment beam focusing means for focusing an alignment beam of electromagnetic radiation provided from said source thereof onto a sample on said ellipsometer system stage for supporting a sample;   a second alignment focusing means for focusing alignment beam electromagnetic radiation which reflects from said sample onto a two dimensional detector array; and   said two dimensional detector array;
 
such that in use an alignment beam of electromagnetic radiation from said source thereof is focused onto said sample at an oblique angle-of-incidence and reflects therefrom and is focused onto said two dimensional detector array.
       

     Said sample alignment system optionally further comprises:
         between said second alignment focusing means and said two dimensional detector array a beam splitter which diverts a portion of the alignment beam electromagnetic radiation which reflects from said sample to a secondary two dimensional detector array, and said secondary two dimensional detector array;
 
said sample investigation system and alignment system being mounted with respect to one another such that the sample investigation beam of electromagnetic radiation and said alignment beam of electromagnetic radiation impinge on said sample at substantially the same location.
       

     Said combination sample investigation system and alignment system can further comprise:
         a mounting frame which supports said combination sample investigation system, and alignment system, said mounting frame projecting vertically upward from a horizontally oriented support as viewed in elevation, and having affixed thereto said means for adjusting the relative “height” positioning between said stage for supporting a sample and, as a unit, said source of a beam of electromagnetic radiation and data detector, as well as said means for translating relative positioning of said sample with respect to said source of a beam of electromagnetic radiation and said data detector, along two orthogonal axes, and said optional means for adjusting the relative orientation of the ellipsometer with respect to said sample to set the angle and plane of incidence of said beam with respect to a surface of said sample; and in which said stage for supporting a sample is oriented to secure a sample in a plane slightly offset from said vertically upward projected plane of said mounting frame so that a sample entered thereinto does not tend to fall back out thereof, said stage being of a construction to contact the edges of the sample only.       

     Further, said combination sample investigation system and alignment system can further comprise:
         a plurality of clamp means at the edges of said stage whereat the sample contacts said stage and which secure the sample to the stage at said edges thereof to better secure said sample, and to decrease non-planar warping therein.       

     Finally, it is noted that the Claims, in part, recite in some steps provide for setting data detector output of a “desirable intensity”. This terminology is to be interpreted as including the possibility of causing a maximum possible intensity, but where not stated otherwise, not requiring such. For instance, this can be the case where prevention of detector saturation occurs when a maximum detector output occurs. Within about 20% maximum is “desirable”. 
     The disclosed invention will be better understood by reference to the Detailed Description Section of this Disclosure, in combination with the Drawings. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG. 1  shows a combination ellipsometer (ES) and alignment (AS) system. 
         FIG. 2   a  shows that a basic alignment system (AS). 
         FIG. 2   b  is included to show that beam components reflected from the front (F), and back (B), respectively, sides of the sample (SAM) can form two spots on the two dimensional detector array (SCRN 1 ). 
         FIG. 3   a  shows a preferred sample alignment system (AS) which includes a beam splitter (BS) and a second two dimensional detector array (SCRN 2 ). 
         FIG. 3   b  demonstrates that the (AOI) and (POI) of an ellipsometric beam (EB) can be adjusted with respect to a surface of said sample (SAM/STG) by rotation. 
         FIG. 3   c  shows that adjusting the height (H) between the sample (SAM) and the alignment system (AS), causes a movement of a spot (HA) on two dimensional detector array (SCRN 1  ). 
         FIG. 3   d  shows that a relative tip/tilt between the sample (SAM) and the alignment system (AS) causes a spot (TTA) on the secondary two dimensional detector array (SCRN 2 ) to move vertically with (AOI) and horizontally with (POI). 
         FIGS. 4   a - 4   c  functionally show that the combination ellipsometer (ES) and alignment (AS) system just described can be commonly mounted to a mounting frame (MF) to form a sample mapping system. 
         FIGS. 4   d - 4   f  show actual embodiment mounting frame (MF), stage (STG) and sample (SAM). 
     
    
    
     DETAILED DESCRIPTION 
     Turning now to the Drawings,  FIG. 1  shows a combination ellipsometer (ES) and alignment (AS) system. The ellipsometer system (ES) is demonstrated as comprising:
         a source of a beam of electromagnetic radiation (ELS);   a polarizer (P);   a stage for supporting a sample (SAM/STG);   an analyzer (A);   a data detector (DDET); and   means for adjusting the relative “height” (H) positioning between said stage for supporting a sample (SAM/STG) and, as a unit, said source (ELS) of an ellipsometer beam (EB) of electromagnetic radiation and data detector (DDET); as well as means for translating relative positioning of said sample (SAM/STG) with respect to, as a unit, said source (ELS) of an ellipsometer beam (EB) of electromagnetic radiation and said data detector, along two orthogonal axes; and optionally means for adjusting the relative orientation of the ellipsometer with respect to said sample (SAM/STG) to set the angle (AOI) and plane (POI) of incidence, (see  FIG. 3   b ), of said ellipsometer beam (EB) with respect to a surface of said sample (SAM/STG).
 
Said ellipsometer system is shown to optionally comprise at least one compensator ((RC) and/or focusing means (CL 1 ) (CL 2 ) CL 3 ) CL 4 ) between said source (ELS) of a beam (EB) of electromagnetic radiation and said data detector (DDET). In use an ellipsometer beam (EB) of electromagnetic radiation from said source (WLS) thereof approaches said sample (SAM/STG) at an oblique angle-of-incidence and reflects therefrom into said data detector (DDET) which produces analyzable data.
       

       FIG. 2   a  shows that a basic alignment system (AS) comprises:
         an alignment source (ALS) of an alignment beam (AB) of electromagnetic radiation;   a first alignment beam (AB) focusing means (CLAL) for focusing an alignment beam (AB) of electromagnetic radiation provided from said source thereof onto the sample (SAM/STG) on said ellipsometer system stage (STG) for supporting a sample (SAM);   a second alignment focusing means (CLA 2 ) for focusing alignment beam electromagnetic radiation which reflects from said sample (SAM) onto a two dimensional detector array (SCRN 1  ); and   said two dimensional detector array (SCRN 1  ).
 
In use an alignment beam (AB) of electromagnetic radiation from said alignment source (ALS) thereof is focused onto said sample (SAM) at an oblique angle-of-incidence and reflects therefrom and is focused onto said two dimensional detector array (SCRN 1  ).
       
       FIG. 2   b  is included to show that beam components reflected from the front (F), and back (B), respectively, sides of the sample (SAM) can form two spots on the two dimensional detector array (SCRN 1  ). The distance between said spots is related to the thickness of the sample (SAM). 
       FIG. 3   a  shows that said sample alignment system (AS) preferably further comprises:
         between said second alignment focusing means (CLA 2 ) and said two dimensional detector array (SCRN 1  ) a beam splitter (BS) which diverts a portion of the alignment beam (AB) electromagnetic radiation which reflects from said sample (SAM) to a secondary two dimensional detector array (SCRN 2 ).
 
Said ellipsometer (ES) and alignment (AS) systems are mounted with respect to one another such that the ellipsometer beam (EB) of electromagnetic radiation and said alignment beam (AB) of electromagnetic radiation impinge on said sample (SAM) at substantially the same location thereupon.  FIG. 3   b  serves to show that the sample (SAM) and stage (STG) might be rotated about orthogonal axes to set (AOI) and POI) of the alignment beam (AB). This should be interpreted to indicate that a functionally equivalent rotational capability can, perhaps alternatively, be provided to the alignment system (AS) and that is relative rotations between the sample (SAM) and alignment system (AL) which is important in the present invention.
       
       FIG. 3   c  shows that adjusting the height (H) between the sample (SAM) and the alignment system (AS), causes a movement of a spot (HA) on two dimensional detector array (SCRN 1  ).  FIG. 3   d  shows that a relative tip/tilt between the sample (SAM) and the alignment system (AS) causes a spot (TTA) on the secondary two dimensional detector array (SCRN 2 ) to move vertically with (AOI) and horizontally with (POI). Said  FIGS. 3   c  and  3   d  actually provide specific insight to how the present invention is able to adjust height (H) and (AOI) and (POI) very quickly. Relative height (H) translation and relative (AOI) and (POI) rotations between the stage (STG), (note the stage (STG) is fixed in the  FIGS. 4   a - 4   c ), and the alignment system (AS) can be performed to position the spots (HA) and (TTA) on two dimensional detector arrays (SCRN 1  ) and (SCRN 2 ) at positions thereon identified as “ideal” (I) therein. The methodology for accomplishing this is described in the Disclosure of the Invention Section of the Disclosure. 
     Continuing,  FIGS. 4   a - 4   c  functionally show that the combination ellipsometer (ES) and alignment (AS) system just described can further comprise:
         a mounting frame (MF) which supports said combination ellipsometer (ES) and alignment (AL) system, said mounting frame (MF) projecting vertically upward from a horizontally oriented support as viewed in elevation.  FIG. 4   c  indicates the presence of means for adjusting the relative “height” (H) positioning between said stage (STG) for supporting a sample (SAM) and, as a unit, said source of a beam of electromagnetic radiation and data detector (collectively indicated by (ES)). A well, said means for translating (HR) (DR) relative positioning of said sample with respect to said source of a beam of electromagnetic radiation and said data detector, along two orthogonal axes. Said optional means for adjusting the relative orientation of the ellipsometer, (indicated by circular arrows), with respect to said sample to set the angle and plane of incidence of said ellipsometric beam with respect to a surface of said sample (SAM).       

     Further,  FIG. 4   c  shows that said stage (STG) for supporting a sample (SAM) is oriented to secure a sample (SAM) in a plane slightly offset from said vertically upward projected plane of said mounting frame (MF) so that a sample (SAM) entered thereinto does not tend to fall back out thereof, said stage (STG) being of a construction to contact the edges of the sample only, (see  FIG. 4   a ). Also note that a plurality of “clamp means” (LTCH) at the edges of said stage (STG) in  FIGS. 4   a  and  4   c , whereat the sample (SAM) contacts said stage (STG). Said clamp means secure the sample (SAM) to the stage (STG) at said edges thereof to better secure said sample (SAM), and to decrease non-planar warping therein. It is noted that sample (SAM) investigated in the present invention can be on the order of a meter or so long along a side and as such can be expected to demonstrate a non-planar surface. 
     In view of  FIGS. 4   a - 4   c , it is disclosed that the present invention can be recast as a sample (SAM) mapping system comprising a mounting frame (MF) which supports a combination ellipsometer (ES) and alignment (AS) system, said mounting frame (MF) projecting substantially vertically upward from a substantially horizontally oriented support, as viewed in elevation, and where said combination ellipsometer (ES) and alignment (AS) system are described above. Also note that  FIG. 4   b  shows the ellipsometer system (ES) can be moved horizontally via a sliding action in guides (HR) or vertically by a sliding action in guides (VR).  FIG. 4   c  indicates guides (DR) allow forward and backward motion which can be applied to adjust (H), (eg. the “height” between the sample (SAM) and the combination (ES).  FIG. 4   c  allows shows that the sample (SAM) is not oriented vertically, but rather is mounted in a fixed position at a slight off-vertical orientation. This is to better secure the sample (SAM). However, achieving that benefit requires that the combination (ES) be rotatable to provide (AOI) and (POI) adjustment capability as shown. 
     It is noted that  FIG. 4   b  also shows Standard Samples (SSMP) mounted at a location whereat the Ellipsometer system (ES) can cause an incident beam to impinge thereupon. In use, the Ellipsometer system (E) can be positioned to “investigate” a Standard Sample (SSMP) which has known physical and/or optical properties, and the data obtained from the Data Detector (DDET) while the Ellipsometer system (ES) is so positioned can be used to calibrate the Ellipsometer system (ES) via a regression procedure. This callibration approach is described in patent to Johs et al. U.S. Pat. No. 5,872,630 and basically evaluates parameters in a mathematical model which describe Ellipsometer system (ES) components, in the same way Sample (SAM) parameters are evaluated. 
       FIGS. 4   d - 4   f  show an actual embodiment mounting frame (MF), stage (STG) and sample (SAM), also showing guides (HR) and (VR) and the location at which the combination ellipsometer (ES) and alignment (AS) system is mounted in the mounting frame (MF), as were functionally indicated in  FIGS. 4   a - 4   c.    
     It is also noted that the alignment and secondary alignment screens (SCRN 1  ) (SCRN 2 ) can double as means to provide an image of the sample, when an illumination source is added to the alignment system (AS), (not shown). When that is done, as described in Pending application Ser. No. 11/784,750, a relatively large area of the sample surface can be viewed in focus if the relative tilt between the sample (SAM) and the alignment system (AS) is seet to meet the Scheimpflug condition. The 750 application is included by reference herein. 
     While the foregoing discussed the very relevant application of an ellipsometer system, the Claims should be broadly considered to include any material system investigation systems such as:
         ellipsometer;   polarimeter;   reflectometer;   spectrophotometer; and   Mueller Matrix measuring system;
 
which operate at least one wavelength in at least one wavelength range, such as:
   VUV;   UV;   Visible;   Infrared;   Far Infrared;   Radio Wave.
 
The major difference between an ellipsometer, polarimeter and Mueller Matrix measuring system as compared to a reflectometer or spectrophotometer is that the reflectometer or spectrophotometer does not comprise polarization related elements such as a polarizer (P) and analyzer (A)
       

     Finally, it is noted that the two dimensional detector array (SCRN 1  ) and secondary two dimensional detector array (SCRN 2 ) can be CDD or CMOS Camera etc. 
     Having hereby disclosed the subject matter of the present invention, it should be obvious that many modifications, substitutions, and variations of the present invention are possible in view of the teachings. It is therefore to be understood that the invention may be practiced other than as specifically described, and should be limited in its breadth and scope only by the Claims.