in accordance with an aspect of the invention , a precision printing system employing a scanner and multiple scan beams includes an array of dove prisms . an acousto - optic modulator or deflector in the printing system controls the intensities of the scan beams . as the acousto - optic modulator turns a beam on or off , successive portions of a scan beam cross - section brighten or darken along the direction of propagation of acoustic waves in the acousto - optic modulator . each dove prism in the array independently rotates the direction of brightening of an associated scan beam so that in the image plane of the printing system , the scan beams brighten in a direction along or opposite the scan direction . to create a dove prism array with suitable accuracy for precision printing , a rigid or crystalline substrate , such as silicon , is etched with a series of parallel grooves for mounting of the dove prisms . placing dove prisms formed from fiber - optic material or fine silica rods in the grooves precisely aligns the prisms in the array . fig2 shows a precision printing system 200 that employs scanning in accordance with an embodiment of the invention . a prescan portion of system 200 includes a beam source 210 , an acousto - optic modulator ( aom ) 220 , and prescan optics 230 . beam source 210 forms multiple input beams 219 having intensities which aom 220 modulates . prescan optics 230 direct modulated input beams 229 onto a scanning element 240 . in accordance with an aspect of the invention , an optical array 222 and brush rotation optics 228 between aom 220 and scanning element 240 change the direction in which portions of modulated beams 229 successively brighten or darken as aom 220 turns on or shuts off the beams . array 222 is an array of prisms or other optical elements that change the brightening directions for individual beams while preserving the orientation of a brush formed by the beams . brush rotation optics 228 , which can be a k mirror or a single dove prism , rotates the brush to the appropriate orientation for scanning and can also change the brightening directions of the individual beams . scanning element 240 directs multiple scan beams 249 into post - scan optics 250 . scanning element 240 is preferably a rotating polygon mirror but alternatively an oscillating mirror or a rotating holographic element could be employed . post - scan optics 250 focuses scan beams 249 as scan beams 249 sweep along scan lines on a surface of a workpiece . post - scan optics 250 include a scan lens 252 and a reduction lens 258 . in an exemplary embodiment of system 200 , scan lens 252 is an f - θ lens because such lenses are known to provide a uniform scanning rates . scan lens 252 can alternatively be another type of lens such as a f - sin θ lens , which reduces scan line bow for extended scan brushes but causes the scan rate to be non - uniform . reduction lens 258 reduces the scan line and resulting image size as required for the image to be formed on the workpiece . for the exemplary embodiment , the workpiece is a mask , a reticule , an unprocessed wafer , or a partially processed wafer that is coated with a layer of photoresist . a precision stage system 260 which is connected to an interferometer 262 and an alignment system 264 positions and moves the workpiece as required for alignment and indexing of scan lines . alignment system 264 identifies the positions of alignment marks on the workpiece as viewed through reduction lens 258 and accordingly determines the position of the alignment relative to the scan lines . interferometer 262 monitors the movement of the workpiece for indexing . beam source 210 includes a light source 211 , beam - shaping elements 212 and 214 , a beam steering system 213 , a beam splitter 215 , and brush optics ( or telescope ) 216 . light source 211 is preferably a laser that generates a coherent beam of suitable power and wavelength for the printing performed . in the exemplary embodiment of the invention , light source 211 is a laser that produces a monochromatic beam of deep ultraviolet light having power greater than about 0 . 1 w . for example , a “ sabre fred ” system available from coherent , inc . delivers 0 . 5 w beam at 244 nm or 257 nm . such deep uv lasers have a resonant cavity free of oxygen and moisture to prevent formation of ozone and degradation of the bbo crystal . these lasers with appropriate components in the rest of system 200 can achieve a minimum feature size of 360 nm with a uniformity of ± 20 nm and a placement accuracy of less than 20 nm at exposure doses up to 200 mj / cm 2 using multiple pass printing . the environment for the optical system and workpiece is a clean environment that is kept at a temperature controlled to ± 0 . 05 ° c . high purity nitrogen is a suitable purge gas where required . beam preparation optics 212 and beam steering system 213 direct the beam from light source 211 to beam splitter 215 which splits the beam into multiple input beams 219 for aom 220 . beams 219 form a “ brush ” for simultaneous illumination of multiple scan lines . in the exemplary embodiment , beam splitter 215 and telescope 216 form thirty - two input beams 219 which are along a line with a 404 . 8 - μm on center spacing . the center two beams are separated by an extra 202 . 4 μm ( one half the normal spacing ) for a total of 607 . 2 μm . the separation provides gaps between input beams 219 sufficient for aom 220 to modulate the intensity of each beam independently . rotation optics 228 rotates the brush so that , in the image plane of system 200 , the projections of beams 219 along the scan direction overlap so that the scan brush illuminates a continuous strip with some overlap of the separate scan lines . additionally , after scan across a set of 32 scan lines , the entire brush is indexed ( moved in the image perpendicular to the scan direction ) by half the width of the brush . the larger spacing between the center beams of the brush causes beams in the top half of the brush in a subsequent scan to be interleaved with beams the lower half of the brush in the previous scan . this provides a more uniform illumination for smoother imaging . aom 220 is a block of material such as fused silica having a patterned layer of lithium niobate bonded to one surface . electric signals applied to the contacts lithographically defined in a conductive layer over the lithium niobate layer create multiple acoustic waves . each acoustic wave propagates through the path of an associated input beam in the block , deflects the associated input beam , and controls the intensity reaching an aperture that selects only the diffracted beam . a rasterizer 224 generates the signals that create the acoustic waves and as a result controls the intensity of modulated beams 229 . in particular , rasterizer 224 divides each scan line into pixels and generates the signals as required for each pixel to have a desired intensity . a timing generator 226 generates a pixel clock signal that is synchronized with the movement of the scan beams . a facet detection system 242 detects the orientation of scanning element 240 to identify the beginnings of scan lines . while a scan beam sweeps across a scan line , timing generator 226 generates the pixel clock for the scan line . if the motion of scanning element 240 and the characteristics of post - scan optics 250 cause the scan beams to scan at a uniform rate , the pixel clock signal is uniform . otherwise , the pixel clock period can vary according to variations in the scan rate . co - filed patent app . ser . no . unknown describes a timing generator suitable for systems having a non - uniform scan rate . to provide the maximum space for separate acoustic waves that separately control individual beam intensities , the acoustic wave propagate along a direction perpendicular to the line of input beams 229 . fig3 a illustrates input beams 219 that are in a line 310 with the direction 312 of propagation of the acoustic waves perpendicular to line 310 . direction 312 is the direction in which successive portions of beam 229 become illuminated as aom 220 turns on the beam and is sometimes referred to herein as a brightening direction . if array 222 were not present , a brush rotation optics 228 , which rotates line 310 to a line 320 relative to scan direction 330 , would rotate brightening direction 312 by the same amount . accordingly , a direction 322 in which beam cross - sections brighten would be perpendicular to line 320 and at angle to scan direction 330 as shown in fig3 a . this would blur edges , skew rectangles , and create a 45 °/ 135 ° bias in the scanned image as described above . in system 200 , array 222 separately rotates the brightening direction 312 of each modulated beam 229 . for example , as illustrated in fig3 b , array 222 rotates the brightening direction 312 of modulated beams 229 in line 310 to a brightening direction 314 while keeping modulated beams 229 in line 310 . direction 314 is such that when brush rotation optics 228 rotate line 310 to line 320 , the beam cross - sections brighten along a direction 324 that is opposite scan direction 330 . array 222 should be positioned in the paths of modulated beams 229 where beams 229 are tightly collimated or focused . as shown in fig2 array 222 is immediately adjacent or part of aom 220 . alternatively , array 222 can be at or near a focus in prescan optics 230 . fig4 shows a possible orientation of aom 220 and array 222 . as shown , each modulated beam 229 from aom 220 has in array 222 an associated dove prism 410 that rotates the brightening direction for that beam . in the exemplary embodiment , beams 229 and dove prisms 410 are 404 . 8 μm apart on center to match the separation of beams in the brush . each prism 410 is formed as described below from a cylindrical rod approximately 400 μm in diameter . beams 229 have a cross - section preferably less than about 150 μm in diameter . fig5 illustrates the operation of a dove prism 500 on a beam 229 . prism 500 has a three flat facets 510 , 520 , and 530 that affect the transmission of modulated beam 229 . base facet 520 is parallel to an x - z plane where the z axis is parallel to the incident direction of beam 229 . front and back facets 510 and 520 are an angle φ with the x - z plane and at an angle ( 90 °- φ ) with an x - y plane . beam 229 has a brightening direction at an angle θ with the base facet 520 , and in the cross - section of beam 229 , brightening illuminates a ray b before a central ray a and ray a before a ray c . as shown in fig5 rays a , b , and c are refracted at facet 510 , experience total internal reflection at facet 520 , and are refracted at surface 530 . because of the total internal reflection , an exit beam 529 has a brightening direction with a y component that is the negative of the y component of the brightening direction of beam 229 . thus , dove prism 500 effectively rotates the brightening direction of beam 229 by an angle of 2θ . ideally , exit beam 529 is otherwise the same as incident beam 229 , i . e ., exit beam 529 propagates along the same line as incident beam 229 . however , if the angle ( nominally φ ) facet 510 makes with base facet 520 differs from the angle ( also nominally φ ) facet 530 makes with base facet 520 , beams 229 and 559 propagate in slightly different directions . additionally , dove prism 500 shifts exit beam 529 in the y direction unless the incident position of beam 229 and the length of dove prism 500 cause reflection of central ray a from the exact mid - point of prism 500 . changes in position and direction of beams 229 in array 222 are not critical if each beam experiences the same change . to achieve only uniform changes , dove prisms 410 of fig4 are identical , as nearly as possible , and have common alignment with beams 229 . fig6 , 8 , and 9 illustrate a method for making a dove prism array that provides only uniform changes in beam position and direction across a multi - beam scanning brush . fig6 illustrates an initial step for forming multiple dove prisms having uniform geometry . the initial step bonds rods 610 to a precision optical flat 620 using an adhesive or optical pitch . rods 610 may be fiber optic material , glass , fused silica , quartz , or any sufficiently transparent material capable of withstanding the required power and wavelength of light in beams 229 . rods 610 are in contact with each other to keeps rods 610 parallel to each other . the rods have a diameter that is controlled to submicron accuracy and on the order of 300 μm to 400 μm . a second step of the process grinds or polishes the combined assembly of rods 610 and flat 620 to create flat surfaces 710 , 720 , and 730 as shown in fig7 . surface 720 is on the top of rods 610 and parallel to flat 620 . surfaces 710 and 730 are at the ends of rods 610 and at an angel with surface 720 sufficient to refract an incident beam to surface 720 for total internal reflection . after grinding , rods 610 are removed from optical flat 620 to provide multiple matched dove prisms such as dove prism 800 of fig8 . dove prism 800 has facets 810 , 820 , and 830 that correspond to the facets 510 , 520 , and 530 of fig5 described above . dove prism 800 also has a rounded ( portion of a cylinder ) surface 840 that is not involved in the optical operation of a dove prism . the dove prisms formed in a batch as described here are nearly identical with any geometric errors likely to be common to all of the prisms . fig9 shows a cross - section of a completed dove prism array 900 . to complete the array , photolithography techniques known from integrated circuit manufacturing processes mask a polished silicon wafer 920 for etching of precisely spaced grooves 922 of uniform size . in an exemplary , embodiment grooves 922 are v grooves formed by etching with potassium hydroxide ( koh ). each previously formed rod 800 has its rounded surface 840 in one of grooves 922 . rods 800 are rotated so that the normals to flat surfaces 820 are at an angle θ with the brightening directions of associated beams 229 . the resulting rotation of the brightening directions is 2θ . grooves 922 precisely fix the locations of the central axes of rods 800 so that the direction and position of the central axes are well controlled . the rotations and placement along the length of grooves 922 can vary from rod to rod . the effects of such variations are not critical . in particular , placement error along the channel only has a second order effect on the positions of the beams that is dependent on angular error in the orientation of the front and back facets . variation in the rotations of facets 820 affect how close the brightening directions will be to opposite the scanning direction , but an error of a degree or less is a relatively small effect when compared to uncorrected case where the brightening direction can be nearly 90 ° from the scanning direction . although the invention has been described with reference to particular embodiments , the description is only an example of the invention &# 39 ; s application and should not be taken as a limitation . various adaptations and combinations of features of the embodiments disclosed are within the scope of the invention as defined by the following claims .