Optical device having an electrically variable refractive index for scan line skew correction in electrostatographic printing machines

Abstract: An optical element (50), for selective scan line skew correction in a raster output scanner (ROS) of an electrophotographic printer, includes a chamber (54) containing a nematic material having a variable index of refraction as a function of voltage (58) applied thereacross. The chamber has a volume defined by surfaces having progressively decreasing widths in substantially perpendicular planes. The ROS includes a control and feedback system coupled to a variable voltage source for applying a biasing voltage across the optical element to control the variable index of refraction of the nematic material for selectively correcting scan line skew.

Description: This invention relates generally to a raster output scanning system for producing electrostatic latent images from electronically stored data in, for example, an electrostatographic printing machine and, more particularly, concerns a device and apparatus for providing controlled skew correction and alignment of a scan line on an imaging member in an electrostatographic printing machine. Electrostatographic printing machines have increasingly utilized digital electronics technology to produce output copies from input video data representing original image information. In this case, it is known to use a raster output scanner (ROS) for exposing the charged portions of the photoconductive member to record the electrostatic latent image thereon. Generally, the ROS has a laser for generating a collimated beam of monochromatic radiation. The laser beam is modulated in conformance with the image information and is directed toward the surface of the photoconductive member through an optics system to form the desired image on the photoconductive member. In the optics system, the modulated laser beam is transmitted through a lens onto a scanning element, typically a rotating polygon having mirrored facets, such that the light beam is reflected from a facet through a post-polygon scan lens and thereafter focused to a "spot" on the photoconductive member. The rotation of the polygon causes the spot to scan linearly across the photoconductive member in a fast scan (i.e., scan line) direction. Meanwhile, the photoconductive member is advanced in a process direction orthogonal to the scan line direction and relatively more slowly than the rate of the fast scan, the so-called slow scan direction. In this manner, the modulated laser beam is scanned across the recording medium as an array of scan lines in a raster scanning pattern. The light beam is intensity-modulated in accordance with an input image serial data stream at a rate such that individual picture elements ("pixels") of the image represented by the data stream are exposed on the photosensitive medium as a series of parallel lines to form the latent image. The photosensitive medium is a belt which should be aligned so that these parallel lines are formed perpendicular to the direction of belt travel. It is difficult to achieve this perpendicularity, resulting in a condition referred to as "scan line skew", wherein the image effectively takes the form of a parallelogram. This condition will affect the images which are subsequently developed and transferred to output prints, the output prints exhibiting degradation of quality due to the skew effects. In a single pass color xerographic system, a plurality of ROS stations are selectively energized to create successive image exposures, each corresponding to the three primary colors. A fourth ROS station may also be added if black images are to be created as well. Thus, each image area on the photoconductive member makes at least three passes relative to an image scan line formed by the modulated laser beam of the ROS system to create a color output copy. Alternatively, highlight color applications might use black plus one or two colors. Each image pass is eventually superimposed on one another in a manner such that each image must be measured to within a 0.1 mm circle or within a tolerance of ± 0.05 mm, and each color image must be registered in both the photoreceptor process direction (slow scan direction) and in the direction transverse to the process direction (fast scan direction). Thus, if a number of raster scan lines are superimposed on a document, as in a color copier, different scan line skews will cause a noticeable interference pattern on the document, resulting in unacceptable copy quality. In many printing machines, the sampling rate of the slow scan direction data equates to 300 lines per inch or more. It has been shown that errors in the slow scan direction of as small as 1% of the nominal line spacing may be perceived in a half tone or continuous tone image. This implies a need for a high degree of control in positioning the scan line in the slow scan direction on the image plane, especially in such applications as multiple beam and multiple ROS color printers where a plurality of scan lines are written onto a single photoreceptor. As described above, scan line skew errors occur when a scan line is not perpendicular to the direction of motion of the imaging member when positioned thereon or when relative variation in skew angle exists between one color and another. The resulting copy output will exhibit quality defects resulting from scan line skew. Errors of scan line skew arise from many sources, including polygon and/or photosensitive member motion flaws, facet and/or image plane (e.g., photoconductive member) surface defects, etc. Skew error correction is most commonly addressed in the prior art by passive or active in-line optics. Prior art disclosures include US-A-4,213,158; US-A-4,903,067; and US-A-4,958,914. US-A-4,213,158 discloses an optical data recording system in which an acousto-optic modulator is used to deflect a laser beam in order to write on a surface, the deflection of the laser beam being determined by the frequency of a voltage source applied to the modulator. US-A-4,958,914 discloses an electro-optic arrangement in which light intensity of a beam is converted to positional information. Liquid crystal materials are disclosed which vary in refractive index in accordance with applied voltage, the liquid crystal materials being mounted on a photoconductive material. In a transmissive mode of operation, light incident on photoconductor passes therethrough and into the liquid crystal materials where each ray is deflected in accordance with its intensity. The deflected rays are then focussed on a screen positioned at the focal plane of a convex lens. Low intensity rays are not deflected as much as high intensity rays and therefore the intensity of a particular ray is determined by its position from the optical axis of the arrangement. Each of these various prior art schemes has disadvantages and/or shortcomings. For example, the use of precision optics requires not only high quality optical elements, but also tight control in the positioning of those optics in order to obtain the requisite very precise mechanical control sufficient to adjust spot position as required in many cases. In order to achieve this level of spot position control with the acousto-optic modulators, an acoustic wave must be established and maintained with great precision. These acousto-optic modulators are relatively expensive and require a correspondingly accurate high frequency signal generator and related electronics to produce and maintain the acoustic waves. Further, such systems which incorporate feedback circuits to provide mechanical reorientation of rotating or translating mirrors generally operate too slowly to correct for motion quality errors because mirror components are relatively bulky and are difficult to move precisely and quickly. JP-A-3/107931 discloses an optical device in which the refractive index can be varied to deflect a beam of light passing therethrough. The optical device comprises a wedge prism of constant refractive index combined with a wedge liquid crystal prism, the refractive index of the liquid crystal prism being altered in accordance with an applied voltage. US-A-4,313,651 discloses an optical beam scanner which does not employ any moving parts. The scanner comprises a Stark cell in the shape of a prism which is mounted between parallel capacitor plates, the plate being connected to a variable power source. A beam incident on the prism is deflected in accordance with the applied voltage due to the Stark effect within the prism. By arranging two pairs of parallel capacitor plates in planes which are orthogonal to one another, the beam can be deflected in two orthogonal directions. EP-A-0,144,008 discloses several embodiments of optical scanning apparatus having dynamic scan path control. The apparatus utilises an error detector arrangement for ensuring that the beam which is scanned across a drum is in the desired position. A rotatable prism is positioned in the main scanning beam and is controlled by a motor in accordance with an error signal produced by the error detector arrangement. Various embodiments are described to provide main and auxiliary beams, the auxiliary beams being used in feedback circuits to control the main beams. According to one aspect of the present invention, there is provided an optical element comprising: a member having a pair of parallel external surfaces, said member including first and second optically transmissive plates defining a chamber interposed therebetween; and a material having a variable index of refraction substantially filling the chamber of said member; characterised in that said chamber has a volume defined by a first plane having a progressively decreasing width from one marginal region to another marginal region opposed therefrom in the first plane, and a second plane, substantially perpendicular to the first plane, having a progressively decreasing width from the one marginal region to another marginal region opposed therefrom in the second plane. According to another aspect of the present invention, there is provided a raster output scanner comprising: means for generating a light beam modulated in accordance with a video input data signal; means for scanning the light beam onto a movable imaging surface being transported in a process direction to provide successive scan lines thereon; an optical element as described above; and a voltage source for applying a biasing voltage across said optical element to generate electric fields therethrough to selectively deflect the light beam to correct scan line skew on the imaging surface as a function of voltage applied thereacross. A control and feedback system may also be provided for detecting skew alignment errors and applying an appropriate biasing voltage to the optical element for correcting scan line skew. According to yet another aspect of the present invention, there is provided an electrostatographic printing machine of the type in which a raster output scanner produces a modulated light beam wherein the modulated light beam is scanned across a movable photoconductive imaging surface being transported in a process direction for recording images thereon, comprising an optical element as described above for selectively deflecting the light beam to correct scan line skew on the imaging surface as a function of voltage applied thereacross and a voltage source for applying a biasing voltage across the optical element to generate electric fields therethrough. A control and feedback system is also provided for detecting skew alignment errors and applying an appropriate biasing voltage to the optical element for correcting scan line skew. By way of example only, embodiments of the invention will be described with reference to the accompanying drawings in which: FIG. 1 shows a plan view of the general optical configuration of a Raster Output Scanner (ROS) system, showing an optical element according to the present invention disposed at various locations along the scan path of the ROS; FIG. 2 shows a graphic representation of the relationship between the index of refraction and the voltage applied to a nematic material; FIG. 3 shows a schematic side view of an optical element in accordance with the present invention; FIG. 4 shows a perspective schematic view of the optical element of FIG. 3; FIG. 5 shows a perspective schematic view of another optical element in accordance with the present invention; FIG. 6 shows a simplified perspective view of the skew correction provided by an optical element of the present invention; and FIG. 7 shows a schematic perspective view of a prior art, single pass, multiple ROS system for forming a multicolor image in a xerographic machine. Referring initially to FIG. 7, there is shown a prior art, single pass, ROS multicolor printing system having four ROS systems, 10, 20, 30, and 40. The multicolor printing system includes a photoreceptor belt 2, driven in a process direction, indicated by the arrow 4. The length of the belt 2 is designed to accept an integral number of spaced image areas, I 1 - I n , represented by dashed line rectangles. Each image area has an associated charging station (not shown) which places a predetermined electrical charge on the surface of belt 2. Each image area I 1 - I n is exposed successively by ROS systems 10, 20, 30, 40, respectively. As each of the image areas I 1 - I n reaches a transverse line of scan, represented by lines 19, 29, 39, 49, the image area is progressively exposed on closely spaced transverse raster lines, shown generally with exaggerated longitudinal spacing as reference numerals 19a and 49a on the image areas I 1 and I 4 , respectively. Downstream from each exposure station, a development station (not shown) develops the latent image formed in the associated image area. A fully developed color image is then transferred to an output sheet. The charge, development, and transfer stations are conventional in the art. Details of charge and development xerographic stations in a multiple exposure single pass system are disclosed, for example, in U.S. Patent 4,660,059. Each ROS system 10, 20, 30, and 40 contains its own conventional scanning components, as variously described in the art. For purposes of simplicity, each ROS system 10, 20, 30, 40 is shown as having two components, namely, a laser light source 12, 22, 32, 42 and a rotating polygon 16, 26, 36, 46, respectively. It will be appreciated by those of skill in the art that multiple scan lines may also be generated with a single ROS. An exemplary ROS system 10, includes a gas, or preferably, diode laser light source 12, having an output which is modulated by signals from control circuit 8, which output is optically processed to impinge on the facets of rotating polygon 16. Each facet reflects the modulated incident laser beam as it is rotated to produce a scan line which is focused at the photoreceptor surface 2. Control circuit 8 contains the circuit and logic modules which respond to input video data signals and other control and timing signals to operate the photoreceptor drive in synchronism with the image exposure and to control the rotation of the polygon 8 by a motor (not shown). The other ROS systems 20, 30, 40, have their own associated laser diodes 22, 32, 42, and polygons 26, 36, 46, respectively. Moving now to a more detailed description of a ROS system used, for example, in an electrostatographic printing machine, FIG. 1 shows a general configuration of the optical system and the optical path of a ROS. For purposes of the present discussion, a single ROS system will be described in detail with reference to ROS system 10. It will be understood that each ROS system 20, 30, 40 may comprise similar components or may include other components, as the case may be. Initially, input video data is transmitted to the laser source 12 which embodies a self-modulating light source for producing a modulated diverging beam of coherent light. The beam may be collimated by a spherical or an aspherical collimating lens 14 and then refocused by a cylinder lens 15 that is part of a wobble correction system. The beam is next incident upon a rotating polygon 16 having at least one mirrored facet 16a for reflecting the beam through a post scan optics system. Other suitable devices for scanning are known in the art, including rotating hologons, rotating diffraction gratings, etc. The post scan optics system reconfigures the beam reflected by facet 16a to a circular or elliptical cross-section, refocuses the beam to the proper point on the surface of photoreceptor/drum 2, and corrects for scan nonlinearity (f-theta correction) as well as wobble defects. A recollimating lens 17and a toroidal or cylindrical lens 18 can be disposed between the scanning device 16 and the photoreceptor 2 to correct for wobble (scanner motion or facet errors) and other defects where appropriate. In the exemplary embodiment of FIG. 1, the rotation of the mirrored facets 16a causes the reflected beam to be deflected and thereby scanned across a photosensitive image member or the photoreceptor belt 2. Thus, if polygon 16 is rotated in a clockwise fashion, a beam reflected from one of its moving facets 16a will be caused to scan from left to right on the photoreceptor belt 2. Polygon 16 is preferably driven by a motor (not shown) through a shaft, with the angular velocity of the polygon 16 synchronized with the angular velocity of belt 2. The combination of the rotation of polygon 16 with movement of the photoreceptor belt 2 in the direction as shown by arrow 4, causes scanning to proceed in raster manner to form an array of scan lines. A typical ROS can illuminate the charged portion of drum 2 at a rate of about 600 pixels per inch (1 inch = 25.4 mm); e.g. at 600 spi resolution. The optical system so far as described hereinabove discloses the basic elements of a raster output scanning system as is well known in the art. In the system shown in FIG. 1, an additional optical element 50 is provided and disposed in the post-scan optics, subsequent to polygon 16, along the scan path of the optical system for deflecting the scan line such that the entire scan line will be manipulated and positioned on the imaging member. In FIG. 1, optical element 50 is shown at a position located between the magnification lens 18 and the imaging member 2. Alternatively, the optical element 50 may be disposed between the F-theta correction lens 17 and the magnification lens 18 or between the polygon 16 and the F-theta correction lens 17, as shown in phantom in FIG. 1. Placement of the optical element 50 in the post-scan optics is required for manipulating the entire scan line through the optical element 50 for proper alignment in the image receiver 2. Optical element 50 preferably includes a liquid crystal cell containing a parallel aligned nematic liquid crystal material as is generally known in the art. In utilizing such a cell, light polarization is parallel to the alignment direction of the liquid crystal material. It will be understood that other liquid crystal materials may be utilized, such as smectic phase crystal materials. The optical element 50 placed in the scan path of a ROS defines a chamber having a volume defined by a first plane having a progressively decreasing width and a second plane, substantially perpendicular to the first plane, also having a progressively decreasing width. This chamber is adapted to contain a volume of nematic material therein. When a biasing voltage is applied to the optical element 50, a combination of bias fields are formed across the chamber to produce a condition in which the molecules of the nematic material in the chamber are aligned by the bias fields in a generally uniform direction with respect to the magnitude of the voltage applied to the optical element 50. The manner in which the refractive index of the liquid crystal material varies in response to the biasing voltage is shown in FIG. 2. As shown in FIG. 2, by varying the magnitude of the biasing voltage, the refractive index n e of the nematic material can be freely controlled for light polarized parallel to the alignment direction of the nematic crystal material. That is, when the level of the biasing voltage exceeds the threshold value V Tth , the arrangement of the liquid crystal molecules in the nematic material will change from homogeneous toward homeotropic and the refractive index n e will also change with respect to the voltage. Thus, as the biasing voltage applied to the optical element 50 is varied, the refractive index of the liquid crystal material changes, thereby changing the angle at which the laser beam exits the optical element 50. This angle is continuously variable within the limits set by the available change in the refractive index. Typically, a liquid crystal cell is made up of parallel plates which form a liquid crystal layer of uniform thickness therebetween. Such liquid crystal cells are known in the art and have been described variously, as for example, in U.S. Patents 4,066,334 and 4,768,864 as well as the references cited therein. In standard practice, liquid crystal cells are used to achieve specific electro-optic effects by placing a small amount of nematic liquid crystal material between two glass plates. For a range of angles of incidence on the liquid crystal interface, light is either partially transmitted and refracted or totally reflected, depending on the electric field orientation of the optic axis in the nematic material. FIGS. 3 and 4 show, in schematic form, a preferred form of the optical element 50. The specific configuration of the optical element provides a chamber 54 interposed between two plates 52, 56 having substantially planar external surface 51, 55, respectively. The plates comprise glass or some other optically transmissive materials. One of the glass plates, in this case plate 56, is coated with a transparent dielectric material having an increasing thickness in two perpendicular planes, forming a dielectric region defining the shape of the chamber between the two glass plates for containing the nematic material, thereby forming the optical element 50. The dielectric region could be made, for example, by molding or casting a particular light transmissive material. Alternatively, grinding or other well known fabrication methods can be used. The optical element is then assembled by positioning the two plates 52, 56 such that the exterior surfaces 51, 55 remain parallel to one another, forming a triangularly shaped lateral side face and a triangularly shaped base face on a common axis such that the thickness of the chamber varies on two substantially perpendicular planes. It will be understood that the triangularly shaped faces of the chamber can be truncated as shown in FIG. 5 so that a chamber 54' can be formed, defined by a surface in a first plane having a progressively decreasing width from one marginal region to another marginal region opposed therefrom in the same plane, and a surface in a second plane, substantially perpendicular to the first plane, having a progressively decreasing width from one marginal region to another marginal region opposed therefrom in the second plane. The chamber 54 is then filled with the nematic material, as for example, a commercial nematic liquid crystal material produced by EM Industries of Hawthorne, New York, having a refractive index ranging from 1.33 to 1.79 depending on the voltage applied to the cell. The chamber configuration results in a structure that provides angular deviation of a scan line dependent on the position of the light beam along the length of the optical element. Since the cell contains a nematic material having a variable index of refraction with respect to voltage applied thereto, changing the voltage applied to the optical element 50 also results in a change in angular deviation along the length of the element 50. Conductive electrodes 53 and 57 are also provided for applying a biasing voltage across the chamber 54. In FIG. 3, transparent conductive electrodes 53 and 57 are placed directly on the exterior faces 51, 55 of the two glass substrates 52, 56, respectively. Alternatively, the transparent electrodes 53 and 57 may be embedded into the plates, as shown in FIGS. 4 and 5. It is an important feature that the electrodes are positioned parallel to one another in order to create uniform electric fields therebetween. That is, due to the biasing voltage applied to the electrodes 53, 57 by voltage source 58, electrodes 53 and 57 generate uniform electric fields across the chamber 54 to induce reorientation of the molecules in the chamber 54 and thereby control the refractive index thereof. While it may be possible to place the liquid crystal material between two glass plates that are angularly positioned with respect to one another, the parallel configuration of the electrodes provides the capability to maintain a uniform electric field between the electrodes 53, 57 when a biasing voltage is applied thereto. This uniform electric field provides means for creating a uniformly refractive index within the chamber 54. A typical liquid crystal cell of the type described herein should have a maximum thickness of less than 300 micrometers. A liquid crystal chamber having a maximum thickness of approximately 50 micrometers over a 1 mm aperture may be utilized to provide a wedge angle of 0.05 radians. The qualitative aspects of the electro-optic effect provided by the optical element can be explained by a simple application of Snell's Law: N l sin=N l sin i ' In the present analysis, Snell's Law must be applied four times at the air/glass interface along exterior face 51, at the glass/liquid crystal interface between plate 52 and chamber 54, at the liquid crystal/glass interface between chamber 54 and plate 56, and the glass/air interface along exterior face 55 in order to determine the aggregate angle of refraction for light rays passing through the optical element 50. For simplicity, it is assumed that the material making up the dielectric region has a refractive index similar to the glass substrate. However, it will be recognized by those of skill in the art that the dielectric region 56a may be composed of a material having a unique refractive index independent of that of the substrate making up the plates of the optical element 50. It will be appreciated that calculations based on Snell's Law will yield an output angle as a function of the input angle and the refractive index of the flat plate material as well as the variable refraction in the liquid crystal cell. In a typical application, the angular range covered by varying the voltage applied to the liquid crystal cell is in the range of 1 to 1.5 degrees. This angular range can be increased substantially for larger angles of incidence. Likewise, smaller angular ranges can be provided by reducing the wedge dimensions and/or by reducing the refractive index change attainable with the liquid crystal material. FIG. 6 illustrates the general principle by which optical element 50 can be used to rectify skew error. Optical element 50 has variable refractive properties by which a ROS scan line 19 can be rotated relative to the process direction of movement of an imaging member 2 in order to adjust the scan line skew. The configuration of the optical element 50 induces an angular displacement in the transmitted scan line relative to the position of the beam along the length of the optical element. As previously discussed, variation of the voltage applied to the optical element 50 changes the magnitude of angular displacement of the scan line. The skew adjustment provided by the angular deviation depends on various parameters but could be on the order of approximately 1.3°, as illustrated in FIG. 6. Thus, with no applied voltage, the scan line might be skewed on the imaging member 2 as shown in phantom in FIG. 6, while, with a properly applied biasing voltage, the scan line can be rotated to provide the desired perpendicular relationship between the scan line and the process direction of movement of the imaging plane. Typically, a coarse alignment can be made within an electronic tandem engine to within one half of a pixel width. The present invention provides for the critical adjustment of the optical system on the order of a pixel width of less in real time response to detected error. Various forms of an error detection and feedback control circuit 60, as shown in FIG. 1, are contemplated for determining the existence and extent of the skew alignment error of a scan line on the photoreceptive surface 2 and for controlling the biasing voltage applied to the optical element 50 for controlling the refractive index of the liquid crystal material necessary to correct the skew alignment error. Error detection and feedback control circuitry used for this purpose are known in the art. For example, an exemplary system is shown in EP-A-0,529,785, wherein a start of scan sensor emits signals at a frequency equal to the system slow scan resolution while timing marks are sensed by a light source/detector combination to provide the basic timing signals for the synchronization of the control system. The beam is initially aligned and adjusted with some relationship to the occurrences of the photoreceptor timing marks. A phase detector detects the phase difference between the signal from the start of scan detector and the timing marks on the photoreceptor and generates a phase error voltage that is fed to a biasing source which applies an appropriate biasing voltage across the electrodes 53, 57 of the optical element 50 to make the necessary scan line skew correction. In another arrangement, the first ROS of a multi-color engine as shown in FIG. 7 might have no skew correction device while the other ROS's each include one skew correction device as described above. In this case, the first ROS will lay down a reference scan line and the correction elements of each subsequent ROS will rotate the scan lines therethrough so that each scan line will be in alignment with the reference scan line. It will be understood that the optical element 50 may be placed in various locations in the post-scan optics along the scan path of the ROS, preferably in regions along the scan line path where the light beam has a limited divergence angle, or where complications regarding physical configurations do not exist. FIG. 1 shows three possible locations for the optical element 50. Since the size of the optical element and the concomitant quantity of nematic material will have significant impact on the cost of the optical element, it may be preferable to determine a location for the optical element in the scan line path at a position where the path length is minimal. The obvious advantageous positions would be directly in front of the polygon 16 or immediately after the F-theta lens 17. The optical element could also be incorporated in a double pass arrangement on a turning mirror, thus increasing the angular deviation while reducing cost by providing a multi-purpose component. In practice, the ROS is embodied in a modular device including a window from which the light beam is transmitted onto the imaging screen; replacement of this window by the optical element 50 may be desirable. In recapitulation, there has been shown a device and apparatus for skew correction control in an electrostatographic machine by means of an electro-optic device placed in the optical system of a raster output scanning system. The optical element has a variable refractive index in a configuration which facilitates rotation of the scan line to provide precise angular displacement of the scan line on the photoreceptor. A control system used in combination with the optical element may be adapted to monitor the skew of the each scan line and to apply a voltage to the optical element for changing the refractive index thereof to shift the position of a scan line. A configuration of the optical element having a liquid crystal chamber providing the desirable characteristics to provide the desired results is disclosed. Although the above description is with respect to a multi-color xerographic machine, the skew correction provided could also be incorporated into a black and white machine.

Claims: An optical element (50) comprising: a member having a pair of parallel external surfaces (51, 55), said member including first and second optically transmissive plates (52, 56) defining a chamber (54; 54') interposed therebetween and defining said external surfaces; and a material having a variable index of refraction substantially filling the chamber (54; 54') of said member; said material being a liquid crystal material; characterised in that said chamber (54; 54') has a volume defined by a first plane having a progressively decreasing width from one marginal region to another marginal region opposed therefrom in the first plane, and a second plane, substantially perpendicular to the first plane, having a progressively decreasing width from the one marginal region to another marginal region opposed therefrom in the second plane. An optical element as claimed in claim 1, further including a pair of electrodes (53, 57) disposed substantially parallel to one another with the chamber (54; 54') being interposed therebetween. An optical element as claimed in claim 2, wherein at least one of said pair of electrodes (53, 57) is disposed on one of said pair of external surfaces (51, 55). An optical element as claimed in any one of the preceding claims, wherein said material having a variable index of refraction includes a nematic liquid crystal material. An optical element as claimed in claim 4, wherein the index of refraction of said nematic material ranges between approximately 1.33 and 1.79 as a function of a biasing voltage applied thereto. An optical element as claimed in any one of the preceding claims, wherein said member has a maximum thickness of approximately 300 micrometers. A raster output scanner (10) comprising: means (12) for generating a light beam modulated in accordance with a video input data signal; means (16, 16a) for scanning the light beam onto a movable imaging surface (2) being transported in a process direction to provide successive scan lines thereon; an optical element (50) as claimed in any one of the preceding claims; and a voltage source (58) for applying a biasing voltage across said optical element (50) to generate electric fields therethrough to selectively deflect the light beam to correct scan line skew on the imaging surface (2) as a function of voltage applied thereacross. A raster output scanner as claimed in claim 7, further including: means for detecting scan line position on the imaging surface to generate an error signal in response thereto; and means (60) responsive to the error signal for controlling the biasing voltage applied to the optical element (50) for selectively varying the index of refraction thereof. An electrostatographic printing machine including at least one raster output scanner (10) as claimed in claim 7 or claim 8.

Inventors: ANDREWS JOHN R, ANDREWS, JOHN R.
Applicants: XEROX CORP, XEROX CORPORATION
Application year: 1993
Main classification: H04N1
IPC codes: G02F1, G02B26, H04N1