Abstract:
Apparatus for dynamic surface annealing of a semiconductor wafer includes a source of laser radiation emitting at a laser wavelength and comprising an array of lasers arranged in rows and columns, the optical power of each the laser being individual adjustable and optics for focusing the radiation from the array of lasers into a narrow line beam in a workpiece plane corresponding to a workpiece surface, whereby the optics images respective columns of the laser array onto respective sections of the narrow line beam. A pyrometer sensor is provided that is sensitive to a pyrometer wavelength. An optical element in an optical path of the optics is tuned to divert radiation emanating from the workpiece plane to the pyrometry sensor. As a result, the optics images each of the respective section of the narrow line beam onto a corresponding portion of the pyrometer sensor. The apparatus further includes a controller responsive to the pyrometry sensor and coupled to adjust individual optical outputs of respective columns of the laser array in accordance with outputs of corresponding portions of the pyrometry sensor.

Description:
CROSS-REFERENCE TO RELATED APPLICATIONS 
       [0001]    This application claims the benefit of U.S. Provisional Application Ser. No. 60/817,131, filed Jun. 27, 2006. 
     
    
     FIELD OF THE INVENTION 
       [0002]    The invention relates generally to thermal processing of semiconductor substrates. In particular, the invention relates to laser thermal processing of semiconductor substrates. 
       BACKGROUND OF THE INVENTION 
       [0003]    Thermal processing is required in the fabrication of silicon and other semiconductor integrated circuits formed in silicon wafers or other substrates such as glass panels for displays. The required temperatures may range from relatively low temperatures of less than 250° C. to greater than 100° C. or 1300° C., for example, and may be used for a variety of processes such as dopant implant annealing, crystallization, oxidation, nitridation, silicidation, and chemical vapor deposition as well as others. 
         [0004]    For the very shallow circuit features required for advanced integrated circuits, it is greatly desired to reduce the total thermal budget in achieving the required thermal processing. The thermal budget may be considered as the total time at high temperatures necessary to achieve the desired processing temperature. The time that the wafer needs to stay at the highest temperature can be very short. 
         [0005]    Rapid thermal processing (RTP) uses radiant lamps. Such lamps have an on/off switching time of at least a half second and therefore cannot avoid heating the entire bulk of the wafer. As a result, the anneal time must be limited to avoid exceeding the thermal budget. Pulsed laser annealing using very short (about 20 ns) laser pulses is effective at heating only the surface layer and not the underlying wafer, thus allowing very short ramp up and ramp down rates. 
         [0006]    A more recently developed approach in various forms, sometimes called thermal flux laser annealing or dynamic surface annealing (DSA), is described by Jennings et al. in PCT/2003/00196966 based upon U.S. patent application Ser. No. 10/325,497, filed Dec. 18, 2002 and incorporated herein by reference in its entirety. This DSA apparatus uses CW diode lasers to produce very intense beams of light that strike the wafer as a thin long line of radiation. The line is then scanned over the surface of the wafer in a direction perpendicular to the long dimension of the line beam. 
         [0007]    In DSA processing, temperature measurement is desirable because the amount of light coupled into the wafer strongly depends upon the surface structure already formed in the wafer. Furthermore, light source conditions may vary somewhat. Wide-angle pyrometers are generally used in RTP apparatus to monitor large portions of the wafer. Such pyrometers are generally inappropriate for the focused laser beams of DSA apparatus the irradiate only a small area of the wafer at any time, leaving the bulk of the wafer near ambient temperature. 
         [0008]    In DSA processing, there is a need to compensate for absorption and reflectivity variations across the semiconductor substrate surface and variation in output of the laser array across the thin line of radiation. For example, variation in reflectivity and absorption of thermal energy at the semiconductor device level for devices which are comprised of features that have varying absorption and reflectivity of said thermal radiation. Such features are many micrometers to submicrometers in dimension. 
       SUMMARY OF THE INVENTION 
       [0009]    Apparatus for dynamic surface annealing of a semiconductor wafer includes a source of laser radiation emitting at a laser wavelength and comprising an array of lasers arranged in rows and columns, the optical power of each the laser being individual adjustable and optics for focusing the radiation from the array of lasers into a narrow line beam in a workpiece plane corresponding to a workpiece surface, whereby the optics images respective columns of the laser array onto respective sections of the narrow line beam. A pyrometer sensor is provided that is sensitive to a pyrometer wavelength. An optical element in an optical path of the optics is tuned to divert radiation emanating from the workpiece plane to the pyrometry sensor. As a result, the optics images each of the respective section of the narrow line beam onto a corresponding portion of the pyrometer sensor. The apparatus further includes a controller responsive to the pyrometry sensor and coupled to adjust individual optical outputs of respective columns of the laser array in accordance with outputs of corresponding portions of the pyrometry sensor. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0010]      FIG. 1  is an orthographic representation of a thermal flux laser annealing apparatus employed in the present invention. 
           [0011]      FIGS. 2 and 3  are orthographic views from different perspectives of optical components of the apparatus of  FIG. 1 . 
           [0012]      FIG. 4  is an end plan view of a portion of a semiconductor laser array in the apparatus of  FIG. 1 . 
           [0013]      FIG. 5A  is a view back side of the laser array of  FIG. 4  and depicts row and column addressing of the laser array. 
           [0014]      FIG. 5B  depicts the individual image elements along the line beam  26  of  FIG. 1  corresponding to individual columns of emitter in the laser stack of  FIGS. 4 and 5A . 
           [0015]      FIG. 6  is a schematic diagram of a system including the features of  FIGS. 2-4  in accordance with a preferred embodiment. 
           [0016]      FIG. 7  depicts the row and column addressing of a typical individual emitter logic associated with an individual laser emitter of the addressable array of laser emitters of  FIG. 5A . 
           [0017]      FIG. 8  depicts a process performed by the controller of the DSA apparatus of  FIGS. 3 and 6  for producing a more uniform wafer surface temperature distribution across wafer surface zone illuminated by the scanning laser line beam of  FIG. 1 . 
           [0018]      FIG. 9A  is a graph depicting an example of an uncorrected temperature distribution. 
           [0019]      FIG. 9B  is a graph of the supply current distribution across the columns of the laser array corresponding to the temperature distribution of  FIG. 9A . 
           [0020]      FIG. 9C  is a graph of the supply current distribution across the columns of the laser array that has been corrected in accordance with deviations in the temperature distribution of  FIG. 9A . 
           [0021]      FIG. 9D  is a graph depicting the compensated temperature distribution produced by the corrected supply current distribution of  FIG. 9C . 
           [0022]      FIG. 10  depicts a row-column addressable laser array that can be employed in carrying out the invention. 
           [0023]      FIG. 11  is a schematic diagram of a dynamic surface anneal system in one aspect of the invention employing the laser array of  FIG. 10 . 
           [0024]      FIG. 12  is a schematic diagram of a system for controlling the apparatus of  FIG. 11 . 
           [0025]      FIG. 13  illustrates an alternative mode of the laser array of  FIG. 10  in which successive rows of laser emitters are offset from one another. 
           [0026]      FIG. 14  is a graph depicting the spatial distribution of optical radiation from the laser stack of  FIG. 13  in a first operational mode. 
           [0027]      FIG. 15  is a graph depicting the spatial distribution of optical radiation from the laser stack of  FIG. 13  in a second operational mode. 
       
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     Introduction: 
       [0028]    A DSA processing apparatus employs an imaging pyrometer, an imaging emissometer, and computer addressable laser diode array to compensate for absorption and reflectivity variations across the water. The addressable laser diode array energy is focused onto the semiconductor substrate surface for the purposes of DSA thermal processing. As the substrate is heated, the imaging emissometer and pyrometer measure the emmissivity and determine the temperature variation across the line beam image zone on semiconductor substrate surface produced by the addressable laser diode array through the focusing optics. The addressable laser diode array is intensity corrected by a programmed controller to compensate for variations detected by the emissometer and pyrometer. Essentially, a line of laser light is focused onto the semiconductor surface and individual zones or image elements along the laser line are temperature controlled by controlling the electrical current to like zones (e.g., columns of laser emitters) within the addressable laser diode array. In this manner the invention is able to compensate for variations in reflectivity and emmissivity on the semiconductor substrate surface and for variations in radiance of the laser array. 
       Dynamic Surface Annealing: 
       [0029]    One embodiment of the DSA apparatus described in the above-referenced application by Jennings et al. is illustrated in the schematic orthographic representation of  FIG. 1 . A gantry structure  10  for two-dimensional scanning includes a pair of fixed parallel rails  12 ,  14 . Two parallel gantry beams  16 ,  18  are fixed together a set distance apart and supported on the fixed rails  12 ,  14  and are controlled by an unillustrated motor and drive mechanism to slide on rollers or ball bearings together along the fixed rails  12 ,  14 . A light beam source  20  is slidably supported on the gantry beams  16 ,  18 , and may be suspended below the beams  16 ,  18  which are controlled by unillustrated motors and drive mechanisms to slide along them. A silicon wafer  22  or other substrate is stationarily supported below the gantry structure  10 . The beam source  20  includes a laser light source and optics to produce a downwardly directed fan-shaped beam  24  that strikes the wafer  22  as a line beam  26  extending generally parallel to the fixed rails  12 ,  14 , in what is conveniently called the slow direction. Although not illustrated here, the gantry structure further includes a Z-axis stage for moving the laser light source and optics in a direction generally parallel to the fan-shaped beam  24  to thereby controllably vary the distance between the beam source  20  and the wafer  22  and thus control the focusing of the line beam  26  on the wafer  22 . Exemplary dimensions of the line beam  26  include a length of 1 cm and a width of 66 microns with an exemplary power density of 220 kW/cm 2 . Alternatively, the beam source and associated optics may be stationary while the wafer is supported on a stage which scans it in two dimensions. 
         [0030]    In typical operation, the gantry beams  16 ,  18  are set at a particular position along the fixed rails  12 ,  14  and the beam source  20  is moved at a uniform speed along the gantry beams  16 ,  18  to scan the line beam  26  perpendicularly to its long dimension in a direction conveniently called the fast direction. The line beam  26  is thereby scanned from one side of the wafer  22  to the other to irradiate a 1 cm swath of the wafer  22 . The line beam  26  is narrow enough and the scanning speed in the fast direction fast enough that a particular area of the wafer is only momentarily exposed to the optical radiation of the line beam  26  but the intensity at the peak of the line beam is enough to heat the surface region to very high temperatures. However, the deeper portions of the wafer  22  are not significantly heated and further act as a heat sink to quickly cool the surface region. Once the fast scan has been completed, the gantry beams  16 ,  18  are moved along the fixed rails  12 ,  14  to a new position such that the line beam  26  is moved along its long dimension extending along the slow axis. The fast scanning is then performed to irradiate a neighboring swath of the wafer  22 . The alternating fast and slow scanning are repeated, perhaps in a serpentine path of the beam source  20 , until the entire wafer  22  has been thermally processed. 
         [0031]    The optics beam source  20  includes an array of lasers. An example is orthographically illustrated in  FIGS. 2 and 3 , in which laser radiation at about 810 nm is produced in an optical system  30  from two laser bar stacks  32 , one of which is illustrated in end plan view in  FIG. 4 . Each laser bar stack  32  includes 14 parallel bars  34 , generally corresponding to a vertical p-n junction in a GaAs semiconductor structure, extending laterally about 1 cm and separated by about 0.9 mm. Typically, water cooling layers are disposed between the bars  34 . In each bar  34  are formed  49  emitters  36 , each constituting a separate GaAs laser emitting respective beams having different divergence angles in orthogonal directions. The illustrated bars  34  are positioned with their long dimension extending over multiple emitters  36  and aligned along the slow axis and their short dimension corresponding to the less than 1-micron p-n depletion layer aligned along the fast axis. The small source size along the fast axis allows effective collimation of the fast axis. The divergence angle is large for the fast axis and relatively small for the slow axis. 
         [0032]    Referring to  FIGS. 2 ,  3  and  4 , two arrays of cylindrical lenslets  40  are positioned along the laser bars  34  to collimate the laser light in a narrow beam along the fast axis. They may be bonded with adhesive on the laser stacks  32  and aligned with the bars  34  to extend over the emitting areas  36 . 
         [0033]    The optics beam source  20  can further include conventional optical elements to collect and focus the light from all the laser bars  32  into a single thin line beam on the wafer surface. Such conventional optical elements can include an interleaver and a polarization multiplexer, although the selection by the skilled worker of such elements is not limited to such an example. In the example of  FIGS. 2 and 3 , the two sets of beams from the two bar stacks  32  are input to an interleaver  42 , which has a multiple beam splitter type of structure and having specified coatings on two internal diagonal faces, e.g., reflective parallel bands, to selectively reflect and transmit light. Such interleavers are commercially available from Research Electro Optics (REO). In the interleaver  42 , patterned metallic reflector bands are formed in angled surfaces for each set of beams from the two bar stacks  32  such that beams from bars  34  on one side of the stack  32  are alternatively reflected or transmitted and thereby interleaved with beams from bars  34  on the other side of the stack  32  which undergo corresponding selective transmission/reflection, thereby filling in the otherwise spaced radiation profile from the separated emitters  36 . 
         [0034]    A first set of interleaved beams is passed through a quarter-wave plate  48  to rotate its polarization relative to that of the second set of interleaved beams. Both sets of interleaved beams are input to a polarization multiplexer (PMUX)  52  having a structure of a double polarization beam splitter. Such a PMUX is commercially available from Research Electro Optics. First and second diagonal interface layers  54 ,  56  cause the two sets of interleaved beams to be reflected along a common axis from their front faces. The first interface  54  is typically implemented as a dielectric interference filter designed as a hard reflector (HR) while the second interface  56  is implemented as a dielectric interference filter designed as a polarization beam splitter (PBS) at the laser wavelength. As a result, the first set of interleaved beams reflected from the first interface layer  54  strikes the back of the second interface layer  56 . Because of the polarization rotation introduced by the quarter-wave plate  48 , the first set of interleaved beams passes through the second interface layer  56 . The intensity of a source beam  58  output by the PMUX  52  is doubled from that of the either of the two sets of interleaved beams. 
         [0035]    Although shown as being separated in the drawings, the interleaver  42 , the quarter-wave plate  48 , and the PMUX  52  and its interfaces  54 ,  56 , as well as additional filters that may be attached to input and output faces are typically joined together by a plastic encapsulant, such as a UV curable epoxy, to provide a rigid optical system. The lenslets  40  are bonded by plastic bonding to the laser stacks  32 , on which they are aligned to the bars  34 . The source beam  58  is passed through a set of cylindrical lenses  62 ,  64 ,  66  to focus the source beam  58  along the slow axis. 
         [0036]    As further illustrated in the schematic view of  FIG. 6 , further anamorphic lens set or optics  80 ,  82  expands the output beam in the slow axis and includes a generally spherical lens to project the desired line beam  26  on the wafer  22 . The anamorphic optics  80 ,  82  shape the source beam in two dimensions to produce a narrow line beam of limited length. 
       Pyrometery: 
       [0037]    One aspect of the invention uses the same optics used to focus the laser source light on the wafer to direct thermal radiation emitted from the neighborhood of the line beam  26  on the wafer  22  in the reverse direction to a pyrometer  60 , schematically illustrated in  FIG. 6 , including an optical detector  61 , such as a photodiode, and an optical filter  63  blocking the wavelength, e.g., 810 nm, of the laser radiation. The pyrometer filter  63  preferably is a narrow passband filter covering a region of the thermal radiation curve which is quickly changing at the temperatures of interest. A preferred pyrometer passband is centered at 1550 nm (in which case the detector  61  may be an InGaAs photodiode). As one of many alternatives, the pyrometer passband may be centered at 950 nm (in which case the detector  61  may be a Si photodiode). The passband may extend over a few tens of nm for the shorter wavelength and perhaps 100 nm at the longer wavelength. The optics are generally reciprocal and thus in the reverse direction detect only a small area of the wafer  22  on or very near to the line beam  26  and optically expands that image to an area generally having a size of the emission face of the bar stacks. Typically narrow band interference filters  63  are used having a passband near 1550 nm or 950 nm which block the laser wavelength at 810 nm by several orders of magnitude and substantially block the laser spontaneous emission not coincident with the pyrometer wavelength. The two PMUX interfaces  54 ,  56  are designed to pass the pyrometer wavelength irrespective of its polarization. Such a function can be implemented with interference mirrors tuned to the 810 nm source radiation and not the pyrometer wavelength. The more conventional interfaces  54 ,  56  are designed such that the first interface  54  is a hard-reflector (HR) interference filter but the second interface  56  is a polarization beam splitter (PBS) tuned to 810 nm or other laser wavelength. The interference filter at the PBS interface  56  may be detuned to the extent that it passes a substantial portion (e.g. 72%) of a first polarization at the pyrometer wavelength while reflecting the first polarization of the laser light (or at least most of it). Likewise, the interference filter in the HR interface  54  is redesigned such that it passes a large fraction (e.g., 90%) of the first polarization at the pyrometer wavelength while reflecting most of the other polarization of both wavelengths. As a result of the filtering of both the PMUX interfaces  54 ,  56  and the narrow band pyrometer filter  63 , the photodetector  61  receives only the narrow-band optical signal in a portion of the thermal (blackbody radiation) spectrum. Thus, an optical filter or path that blocks or admits a particular wavelength is sufficient even though it does not completely block or completely admit all of the light at that wavelength. 
         [0038]    The output of the photodetector  61  is supplied to a source controller  65 , which converts the detected photocurrent to a wafer temperature and compares it to a desired temperature and thereby adjusts the power supplied to the laser bars  32  to increase or decrease their optical output in the direction of the desired wafer temperature. 
         [0039]    A difficulty with this approach is that the GaAs or other semiconductor lasers either emit or induce a fairly wide spectrum of low-level pit-of-band emission that typically overlaps the pyrometer wavelength. As a result of the out-of-band emission, which the pyrometer filter  63  does not block at the pyrometer wavelength, the photodetector  61  would detect both: (a) the wafer thermal radiation at the pyrometer wavelength and (b) the portion of the out-of-band emission at the pyrometer wavelength, in the absence of additional filtering. This difficulty is avoided in large part by filtering out the out-of-band emission at the pyrometer wavelength with a notch filter  67  placed between the lens array  40  and the interleaver  42  or a notch filter  68  placed between the interleaver  42  and the PMUX  52 . The notch filter  67  or  68  blocks the out-of-band radiation at the pyrometer wavelength, specifically whatever wavelengths are passed by the pyrometer filter  63 , e.g. 1550 nm or 950 nm, and pass at least the laser radiation at 810 nm. The ratio of the transmission coefficient of the laser wavelength to that of pyrometer wavelength should be several orders of magnitude. A minimum requirement of the notch filters  67 ,  68  is that they block wavelengths longer than the laser wavelength, e.g., 810 nm, although radiation at shorter wavelengths do not inherently degrade the pyrometer. The notch filters  67 ,  68  may be easily implemented as interference filters coated on either the interleaver  42  or the PMUX  52 , although they may be implemented as stand alone filters. Examples are described in U.S. patent application Ser. No. 11/195,380, filed Aug. 2, 2005 entitled MULTIPLE BAND PASS FILTERING FOR PYROMETRY IN LASER BASED ANNEALING SYSTEMS by Bruce Adams, et al. and assigned to the present assignee, and particularly at  FIGS. 7-9  of the cited patent application. 
         [0040]    The anamorphic optics between the optical source and the water typically include anti-reflection coatings. With the invention, the anti-reflection and other coatings need to be designed not only for the laser wavelength but also for the pyrometer wavelength. 
         [0041]    As an alternative, the wavelength filtering performed by the PMUX interfaces can be replaced by selective transmission at the laser wavelength and selective reflection at the pyrometer wavelength. It may be possible to carry out the invention without either the interleaver  42  or the polarization multiplexer  52  or without both of them. As one possible example, an optical element similar to the reflective surfaces  54 ,  56  (or similar to one of them) may be employed to carry out the invention, that element not being part of a polarization multiplexer. 
       Compensation for Non-Uniformities in Wafer Surface Temperature Using an Addressable Laser Array: 
       [0042]      FIG. 3  indicates that the controller  65  interfaces with the lasers stacks  32  through a row-column address decoder  33 . This feature enables the controller to govern the output levels of individual laser emitter  36  independently.  FIG. 5A  depicts an embodiment of the back side of the laser stack or array  32  of  FIG. 4 , in which each laser emitter  36  depicted in  FIG. 4  controlled by an individual emitter logic circuit  37 . The laser emitters  36  of the laser stack of the array  32  are arranged in rows (bars  34 ) and columns.  FIG. 5A  shows that the row-column address decoder  33  consists of a column address decoder  33 - 1  and a row address decoder  33 - 2 , which together enable the controller  65  to access an individual emitter  36  through its emitter logic circuit  37  based upon its row and column position within the array  32 . 
         [0043]    Referring to  FIG. 7 , in one implementation the emitter logic circuit  37  has a programmable resistor  37 - 1  through which supply current flows to the individual laser diode (emitter  36 ). The emitter logic circuit also has a dual gate switch  37 - 2  through which a resistance-changing command is gated from the controller  65  to the programmable resistor  37 - 1 . The two gates of the switch  37 - 2  are coupled to corresponding column and row outputs of the address decoders  33 - 1 ,  33 - 2 . The switch  37 - 2  permits a resistance-changing signal from the controller  65  to reach the programmable resistor  37 - 1  whenever both the column and row address decoders  33 - 1 ,  33 - 2  enable the corresponding row and column. The programmable resistor  37 - 1  may be a field effect transistor with a floating gate device, in which case the resistance-changing signal from the controller  65  is one which either charges or discharges the floating gate depending upon whether the resistance is to be increased or decreased. Other implementations may be employed. By thus changing the resistance of the programmable resistor  37 - 1 , the controller  65  separately controls the supply current to each individual diode laser, and thus independently controls the optical power output of each emitter  36 . 
         [0044]    Each column of emitters  36  in the array  32  is focused by the optics on an individual one of sections or image elements  26 - 1  through  26 - n  of the line beam  26  depicted in  FIG. 5R . The width of each of the n beam sections or image elements corresponds approximately to the minimum resolvable spot size of the focused line beam. The controller  65  can vary the beam intensity at a particular one of the line beam sections or image elements  26 - 1  through  26 - n  by varying the supply current to the laser diodes in the corresponding column. For example, the controller  65  could increase or decrease the supply current to some or all of the laser diodes in the selected column. 
         [0045]    The detector  61  is preferably a CCD camera that captures the image of the entire line beam  26  with each image sample and has sufficient resolution to sense the irradiance at each individual image element  26 - 1  through  26 - n . The output of the camera  61  is used in the manner of pyrometry to compute the temperature at each of the n image elements  26 - 1  through  26 - n  on the wafer surface. From this, the wafer surface temperature distribution along the line beam  26  is constructed by the controller  65 . The controller  65  deduces from this distribution how to change the distribution of laser diode supply currents to different columns of lasers so as to minimize or eliminate deviations in the temperature distribution. 
         [0046]    The process is depicted in  FIG. 8 . In order to employ pyrometry computations to compute the wafer surface temperature at each image element, emissivity is measured first. This is accomplished by flashing an emissometry light source  21  ( FIG. 1 ) of a measured irradiance onto the zone of the wafer surface currently illuminated by the laser line beam  26  (block  86  of  FIG. 8 ). The CCD camera  61  samples and stores the image of the ambient background radiation from the wafer prior to the flashing of the emissometry light source. Then, during the instant in which the emissometry light source is flashed, the CCD camera  61  subtracts the previously sampled background radiation from the current image, so that the output of the CCD camera  61  is an accurate measurement of the emissometry source light reflected from each image element  26 - 1  through  26 - n  on the wafer surface. During that instant, the controller  65  captures the reflected light intensity for each individual image element  26 - 1  through  26 - n  (block  88  of  FIG. 8 ) and computes n corresponding emissivities given the brightness of the emissometry light source (block  90  of  FIG. 8 ). After the emissivity light source  21  has flashed and is not radiating, the controller  65  samples the thermal radiation from each image element  26 - 1  through  26 - n  measured by the camera  61  (block  92  of  FIG. 8 ). The controller  65  combines the computed emissivity of each individual image element  26 - 1  through  26 - n  on the wafer surface with the thermal radiance sensed from that image element by the camera  61  to compute the wafer surface temperature at the corresponding image element (block  94  of  FIG. 8 ). This computation produces n wafer surface temperatures corresponding to the n image elements illuminated by the line beam  26 . The controller  65  then constructs the distribution of the n temperature measurements and determines which image elements are either above or below the desired wafer surface temperature value or limited range (block  96  of  FIG. 8 ). The controller changes the distribution of supply currents among the different columns of emitters  36  so as to reduce the deviation in the temperature distribution (block  98  of  FIG. 8 ). For example, the controller  65  reduces the supply current to those columns of emitters  36  corresponding to an image element associated with a surface temperature above the desired value or range. Likewise the controller increases the supply current to those columns of emitters  36  corresponding to an image element associated with a surface temperature below the desired value or range. 
         [0047]    A simplified example of this process is depicted in  FIGS. 9A through 9D . In  FIG. 9A , an initial temperature distribution reveals several zones along the line beam  26  that are above a uniform level. This distribution was produced by an uncorrected distribution of supply currents to all the laser columns, which was therefore uniform as indicated in  FIG. 9B . The supply current distribution among the columns of laser emitters is then corrected so as to compensate for the non uniformities in the temperature distribution of  FIG. 9A , the corrected supply current distribution being depicted in  FIG. 9C  and appearing to have variations similar to an inverse of the initial temperature distribution of FIG.  9 A. The resulting “corrected” temperature distribution is depicted in  FIG. 9D , in which the non-uniformities apparent in  FIG. 9A  have been nearly eliminated. 
         [0048]      FIG. 10  illustrates a row/column addressable laser diode stack  101  constructed in accordance with U.S. Pat. No. 6,728,275. The row of the stack  101  consists of an individual laser diode bar comprised of individual emitters  102 . The emitters  102  of the stack  101  are aligned in columns. The columns may vary in number and this number is dependent upon the number of emitters  102  within each laser diode bar. The number of rows is determined by the number of laser diode bars in the laser diode stack  101 . The laser output radiation or beam  104  is made substantially plane wave in propagation with the use of attached microlenses  103 . One or more emitters  102  are electrically connected in parallel within a laser diode bar and in parallel with emitters of adjacent laser diode bars. There are many possible electrical wiring configurations. One example is for the emitters  102  located in each particular column (e.g., column  0 ) to be electrically common so that they operate in unison and emit laser beams  104  simultaneously. This approach is taught in U.S. Pat. No. 6,728,275. 
         [0049]    An alternative mode of U.S. Pat. No. 6,728,275 is to offset adjacent rows of the emitters  102  so that neighboring rows of emitters  102  are displaced by a distance “n” in the manner depicted in  FIG. 13 , where n may be a fraction of or equivalent to the distance between emitters  102  in the column direction. In this case, if only the emitters  102  of alternate rows (for example, the even numbered rows) are electrically powered, the spatial distribution of the optical radiation of the laser diode stack  101  may appear as shown in  FIG. 14  after passing through a lens system that superimposes all rows with a magnification such that the laser beams  104  from individual emitters will overlap at the full width half maximums of each emitter beam distribution. Now, if the remaining rows (the odd numbered rows) are electrically powered, the more uniform radiation distribution shown in  FIG. 15  can be realized by properly adjusting the individual supply current levels delivered to the individual columns of emitters  102 . Such a uniform and flat distribution of radiation or energy may be useful to compensate for variations in light output within the laser diode stack  101 , system optics, or variations in reflectivity or absorption on the substrate. Further, modifications to the radiation distribution of the laser stack  101  can be made to have non-uniformities that perfectly compensate for non-uniformities of reflectivity and absorption on the surface of the substrate. Such modifications to the laser stack output radiation distribution may be accomplished with a computer controlled system utilizing appropriate sensors to measure reflectivity and absorption variations and to electrically vary the output of individual columns of lasers in the stack  101 , so that these variations are compensated for in nearly real time. 
         [0050]    An implementation of a DSA system employing the laser diode stack  101  is shown in  FIG. 11 . The linearly polarized laser output radiation or beam  104  of the laser diode stack  101  enters a polarizing beam splitting cube  105  in which the hypotenuse  105   a  is coated to efficiently transmit the laser light. The linearly polarized laser light then enters a one quarter wave phase retardation plate  106  and becomes circularly polarized. The laser light next enters a beam splitting cube  107  where it is transmitted to reduction optics  108 . The reduction optics  108  forces the beams of all rows of emitters to be superimposed at a focus position located slightly above, at, or slightly below the surface of the substrate  109 . A portion of the laser light is reflected by the substrate  109  and as a result of reflection becomes circularly polarized in the opposite direction. This oppositely circularly polarized light enters the reduction optics  108 , the beam splitting cube  107 , and then the one quarter wave phase retardation plate  106  where it becomes linearly polarized again but with the e-field of the laser light rotated ninety degrees from the first pass. The 90 degree rotated linearly polarized light then impinges upon the hypotenuse  105   a  of the polarizing beam splitting cube  105  where it is mostly reflected and finally mostly absorbed by an absorbing surface  111  which may be fluid cooled. In this manner the laser diode stack  101  is protected from energy which is reflected from the substrate  109  which may otherwise cause undesirable thermal heating and or damage to the laser diode stack  101  or its components, or undesirable optical performance such as laser feedback to the laser cavities within the emitters  102 . 
         [0051]    Thermal radiation is emitted by the substrate  109  as a result of heat created by the impinging laser light. A portion of the thermal radiation is collected by the reduction optics  108  and reflected by the beam splitting cube  107  where it enters pyrometry and emissometry imaging optics  112 . A camera  113  produces an image of the thermal radiation at the substrate  109  at each image element corresponding to a zone of the substrate surface illuminated by a particular column of emitters  104  of the stack  101 . For accurate calculation of the temperature of the substrate  109 , the emissivity of the substrate  109  is first obtained. Emissometry light source  114  is flashed to illuminate the substrate  109 , and this flashed radiation is partially reflected into the reduction optics  108 , beam splitting cube  107 , and imaged by the pyrometry and emissometry imaging optics  112  on to the camera  113 . When the emissometry light source  114  is flashed or powered, the output of the camera  113  will be essentially only comprised of the emittance of the substrate  109 , because the CCD camera  113  subtracts out the background radiation in the same manner as described above with reference to the CCD camera  61  in the process of  FIG. 8 . In this way, the system is able to measure the emittance of the substrate  109  and calculate the temperature at discrete points (i.e., the image elements on the wafer surface illuminated by discrete columns of the emitters  104  of the stack  101 ) based upon the emittance at those discrete points. The computation of emittance and hence temperature from the radiation sensed by the CCD camera  113  is carried out in accordance with well-understood principles. The system of measuring discrete points for emittance and thermal radiation is referred to in this embodiment as “imaging emissometry and pyrometry.” 
         [0052]    There is benefit in performing this thermal process at elevated temperatures prior to illumination with the laser energy. A heated electrostatic chuck (ESC)  110  heats the substrate  109  to a user-selected temperature to reduce the amount of laser energy required for processing and reduce thermal strain gradients within the substrate  109 . 
         [0053]      FIG. 12  illustrates a block diagram of a DSA system controlling the DSA apparatus of  FIG. 11 . In  FIG. 12 , a system control computer  120  communicates with laser array, pyrometry, emissometry, camera, stage motion, electrostatic chuck temperature and beam diagnostics controllers  122 ,  124 ,  126 ,  128 ,  130 ,  132 ,  134 , respectively, over a data buss  136 . Alternately, the system control computer may communicate directly with the controllers  122 ,  124 ,  126 ,  128 ,  130 ,  132 ,  134 . During operation, the wafer or substrate  109  is loaded onto the heated ESC  110 . An alignment system (not shown) may be used to find fiducials on the substrate  109  and align the patterns (if any) with locations expected to be encountered based on information stored in memory of the system control computer  120 . The information may be useful for passively or dynamically controlling the output of the laser diode array  101 . The system control computer  120  confirms that the substrate ESC temperature controller  132  senses that the ESC  110  has reached the correct temperature and then commands the stage motion controller  130  to move the ESC  110 /substrate  109  to the starting position. The X Y Z stage ( FIG. 1 ) is set into motion and the output power level of the laser array  101  is increased, while a focus sensor  138  not illustrated in  FIG. 11  simultaneously provides feedback to the stage motion controller  130  to enable the stage motion controller  130  to z-position the substrate  109  to the user-selected focus position. Additionally, and simultaneously, the emissometer light source  114  is flashed to allow the emmissometry controller  126  to begin calculating the emmittance from each image element of the substrate  109 . The pyrometry controller  124  calculates the temperature distribution along the laser-illuminated zone of the surface of the substrate  109 . The output of the pyrometry and emissometry controllers  124 ,  126  may be read by the system control computer  120  to create a map of the wafer and or to command the laser array controller  122  to send different electrical current level to appropriate columns within the laser diode stack  101  to produce the desired (or user selectable) temperature uniformity in the illuminated zone of the substrate surface. Alternatively, the emissometry and pyrometry controllers  126 ,  124  can provide direct feedback to the laser array controller  122  to control the temperature distribution across the laser-illuminated zone of the substrate surface. Beam profiler and power detector sensors  140 ,  142  not illustrated in  FIG. 11  provide the beam diagnostics controller  134  with inputs for determining power as a function of current and voltage, spot size, spot profile, depth of focus, field curvature, and power level for each column of the laser diode stack  101 . 
         [0054]    The substrate  109  may be moved in a plane, in the x-y directions, to process smaller sections of the substrate  109  until the entire substrate  109  has been processed. Alternatively, the substrate  109  may be moved in one direction (for example the x direction) and the laser and optical system shown in  FIG. 11  moved in the orthogonal direction (y direction). Additionally, the substrate  109  may be fixed and the laser and optical system shown in  FIG. 11  may be moved in the x-y-z directions to sweep across the Substrate ( 9 ) and thermally process it. 
         [0055]    While the invention has been described in detail by specific reference to preferred embodiments, it is understood that variations and modifications thereof may be made without departing from the true spirit and scope of the invention.