CA1175095A - Unitary, modular demountable optical system for laser 1 diode printing copying apparatus - Google Patents
Unitary, modular demountable optical system for laser 1 diode printing copying apparatusInfo
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- CA1175095A CA1175095A CA000423657A CA423657A CA1175095A CA 1175095 A CA1175095 A CA 1175095A CA 000423657 A CA000423657 A CA 000423657A CA 423657 A CA423657 A CA 423657A CA 1175095 A CA1175095 A CA 1175095A
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- laser
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Abstract
ABSTRACT OF THE DISCLOSURE
An Optical scanning and imaging system util-izing laser diode light generation comprising;
a solid state laser light generating device producing a divergent electromagnetic visible emission, means for collecting and collimating said divergent emission into a beam of light;
means for optically shaping said beam to effectively expand the verticle dimension thereof; and for reducing the horizontal dimension of said beam;
a rotatable polygon mirror assembly in the path of said light beam and having a plurality of flat mirror facets disposed around the periphery thereof;
means for bringing said beam into sharp focus on a single facet of said rotatable ploygon mirror assembly;
angularly, adjustably positionable, reflective means disposed adjacent to said polygon mirror assembly;
a photoconductive drum rotatably disposed adjacent to said adjustably positionable reflective means, and focusing means interposed between said polygon mirror assembly and said adjustably positionable reflective means for bringing said beam into focus on said drum as said beam is moved by said polygon mirror assembly across the surface of said rotatable drum effectively causing said beam to scan said drum from side to side.
An Optical scanning and imaging system util-izing laser diode light generation comprising;
a solid state laser light generating device producing a divergent electromagnetic visible emission, means for collecting and collimating said divergent emission into a beam of light;
means for optically shaping said beam to effectively expand the verticle dimension thereof; and for reducing the horizontal dimension of said beam;
a rotatable polygon mirror assembly in the path of said light beam and having a plurality of flat mirror facets disposed around the periphery thereof;
means for bringing said beam into sharp focus on a single facet of said rotatable ploygon mirror assembly;
angularly, adjustably positionable, reflective means disposed adjacent to said polygon mirror assembly;
a photoconductive drum rotatably disposed adjacent to said adjustably positionable reflective means, and focusing means interposed between said polygon mirror assembly and said adjustably positionable reflective means for bringing said beam into focus on said drum as said beam is moved by said polygon mirror assembly across the surface of said rotatable drum effectively causing said beam to scan said drum from side to side.
Description
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UNITARY, MODULAR, DEMOUNTABLE
OPTICAL SYSTEM FOR LASER DIODE/
BACKGROUND OF THE INVENTION
1. Field of the Invention This invention relates to photo-optical scanning apparatus utilizing a laser ~iode light generating device and a polygonal mirror assembly in conjunction with suitable light beam collimating and focusing apparatus. More specifically, the invention relates to a system for precisely shapin~ the laser generating light beam into an efficient spot scanning size for electrophotographic printing and/or copying.
UNITARY, MODULAR, DEMOUNTABLE
OPTICAL SYSTEM FOR LASER DIODE/
BACKGROUND OF THE INVENTION
1. Field of the Invention This invention relates to photo-optical scanning apparatus utilizing a laser ~iode light generating device and a polygonal mirror assembly in conjunction with suitable light beam collimating and focusing apparatus. More specifically, the invention relates to a system for precisely shapin~ the laser generating light beam into an efficient spot scanning size for electrophotographic printing and/or copying.
2. Descriptlon of the Prior Art Many problems are associated with scanning systems wherein a modulated/or unmodulated light beam is caused to scan by means of a rotatable polygonal mirror. For example, the position of each scanning line becomes dificult to control. This problem is a result of the angular relationship between adjacent facets of the polygon as well as between the facet planes and the rotational axis of the polygon.
Another problem is associated with the location of the laser light generating apparatus and its angular relationship to the operably associated . .
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hardware. A further problem is that as the polygon mirror asse~bly is rotated at a constant rotational rate the speed of the generated spot will be constant along an arc but will not be constant with respect to a straight line scan. ~n fact, the laser beam or spot speeds up at the periphery of the scan line which in - turn has the effect of changing the dimension of the output data being developed. These and other ~imilarly associated problems have caused many of the prior art devices to be less than commercially satisfactory.
2. Description of the Prior Art A number of techniques and apparatus have been suggested for use in laser printing copying. Each has certain characteristics which recommend it for a specific application. Obviously, the goal is to provide a type of printing/copyiny device which accommodates a variety of purposes and performs these functions effectively and efficiently.
The following patents are considered to be pertinent to the present invention which iq considered to be an improvement thereover, as well as an improvement over the earlier filed application `USSN
27~,2~0, as will be described later on herein.
~ Fleischer, 3,750,189 shows and describes a helium-neon laser scanner whose light output is coupled through a lens system to a rotating polygon mirror from which the light is reflected through a lens system to a rotating drum. In the Fleischer structure a cylindrical lens is employed to focus the collimated beam of light to a line on a flat facet of the polygon mirror while a second cylindrical or toric lens after the polygon is used to recollimate the light reflected from the ~t75 polygon. A spherical lens then focuses the recollimated light beam to a small spot on the scan line of the photocopy drum.
For appreciable scan an~les it is necessary to use a toroid in order to maintain the spot size over the scan line. However, toroidal lenses are relatively difficult to manufacture and are therefore usually not economically or commercially feasible due to their high cost.
Grafton, 3,946,150 employs a cylindrical lens near the photoreceptor. This proximity requires the use of a long cylindrical lens. Also, since this lens is located close to the developer unit it tends to become coated with toner which degrades the light and resulting photocopy.
Rabedeau, 4,123,135 is stated to be an improve-ment over the apparatus described in Fleischer,
Another problem is associated with the location of the laser light generating apparatus and its angular relationship to the operably associated . .
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hardware. A further problem is that as the polygon mirror asse~bly is rotated at a constant rotational rate the speed of the generated spot will be constant along an arc but will not be constant with respect to a straight line scan. ~n fact, the laser beam or spot speeds up at the periphery of the scan line which in - turn has the effect of changing the dimension of the output data being developed. These and other ~imilarly associated problems have caused many of the prior art devices to be less than commercially satisfactory.
2. Description of the Prior Art A number of techniques and apparatus have been suggested for use in laser printing copying. Each has certain characteristics which recommend it for a specific application. Obviously, the goal is to provide a type of printing/copyiny device which accommodates a variety of purposes and performs these functions effectively and efficiently.
The following patents are considered to be pertinent to the present invention which iq considered to be an improvement thereover, as well as an improvement over the earlier filed application `USSN
27~,2~0, as will be described later on herein.
~ Fleischer, 3,750,189 shows and describes a helium-neon laser scanner whose light output is coupled through a lens system to a rotating polygon mirror from which the light is reflected through a lens system to a rotating drum. In the Fleischer structure a cylindrical lens is employed to focus the collimated beam of light to a line on a flat facet of the polygon mirror while a second cylindrical or toric lens after the polygon is used to recollimate the light reflected from the ~t75 polygon. A spherical lens then focuses the recollimated light beam to a small spot on the scan line of the photocopy drum.
For appreciable scan an~les it is necessary to use a toroid in order to maintain the spot size over the scan line. However, toroidal lenses are relatively difficult to manufacture and are therefore usually not economically or commercially feasible due to their high cost.
Grafton, 3,946,150 employs a cylindrical lens near the photoreceptor. This proximity requires the use of a long cylindrical lens. Also, since this lens is located close to the developer unit it tends to become coated with toner which degrades the light and resulting photocopy.
Rabedeau, 4,123,135 is stated to be an improve-ment over the apparatus described in Fleischer,
3,750,189. Rabedeau notes that the beam entering the spherical lens need not be collimated. Rabedeau makes use of this by employing a negative cylindrical lens with power in the scan direction following the polygon to produce the same beam divergence in both azimuths for the beam that enters the spherical focusing lenses.
The method and structure permits the use of less expensive cylindrical lenses but also tends to ~latten the field. However, it remains a very dif ficult problem to flatten the fie]d over wide angles when relatively high resolution is required.
SUMMARY OF THE INVENTION
The present invention overcomes the above difficulties first, by providing a cylindrical meniscus lens with power in the horizontal scan direction to focus the beam to a small spot in the scan direction.
~ ~75~9~i Second, by providing a pair of cylindrical-spherical lenses to provide cross-scan or vertical focus. The cylindrical-spherical lenses provide a function similar to a pair o~ toric lenses but at a more reasonable cost.
For the laser diode scanning system of the present invention it is also an advantage to have the horizontal - and vertical focus independent.
The optical system of the present invention is structured and fabricated as demountable, unitary, modular assembly independent of the remainder of the apparatus with which it is or may be operably associ-ated. The lens assemblies of the optical system, once adjusted for focus, are fixed in position with.in the module although each lens is in fact demountable for replacement without the need for realign~ent upon re-insertion in the assembly. The module is sealed against du t and dirt contaminatior. and is provided with its own source of pressurize~ air to prevent dust and dirt from accumulating within the assembly from one source or another. Additionally the module is angularly adjust-ably positionable relative to the photoreceptor drum and includes means for preventing accidental ingress of toner into the optical module. Precisely located pivot pins enable accurate adjustment of the optics relative to the photoreceptor drum which, once fixed in position, need no further adjustment or alteration.
It is, ~herefore, an object for the present invention to overcome ~ach of these problems in a new, novel and heretofore unobvious manner and to provide a photo-optical solid state laser diode scanning system wherein a solid state laser is caused to produce a divergent beam of visible electromagnetic radiation which is collected and collimated and thereafter - ~.1L7~
optically shaped to reduce the vertical dimension while expanding the horizontal dimension for subsequent impingement upon a rotatable polygonal mirror assembly.
The collimated laser beam is then focused onto a photo-conductor, for example, a rotatable drum, through acylindrical lens and a light folding mirror, passing through a spherical lens to the photoconductor itself.
A novel aspect of the invention is the pro-vision for the apparatus to be modularly related and to be mounted to a rigid, fixed base mel~ber. Each element of the novel combination is adjustably, positionable relative to the base as well as to the axis of the laser beam, the lenses, mirrors and polygonal mirror facets thereby insuring an ~ccurate, clear and highly defined, latent image on the photoconductor,i.e. drum.
Another novel aspect of the present invention is the yrovision ~f a novel photoconductor drum charging, exposing, toning and cleaning apparatus for a laser diode and printing and/or copying apparatus utilizing a novel folded laser scanning light path in combination with a corna charging, discharging apparatus not heretofore available in electrophotographic processing apparatus.
Other objects, features and advantages of the invention will be readily apparent from the following description of two different embodiments thereof, taken in conjunction with the ~ccompanying drawings, although variations and modifications may be efected without departing from the spirit and scope of the novel concepts of the disclosuxe.
BRIEF DESCRIPTION OF THE DRAWINGS
Figure 1 is a schematic side elevational view, not to scale, of apparatus embodying the present invention;
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Figure 2 is a detailed side elevational view o the apparatus of Figure l;
Figure 3 is a schematic top end view not to scale, of the apparatus of Figures 1 and 2;
` Figure 4 is a detailed top plan view of the apparatus of Figure 3;
Figure 5 is a schematic illustration, not to scale, of the electrophotographic process sta~ion of the present invention;
10Figure 6 is a detailed view of the apparatus illustrated in Fisure 5;
Figure 7 is a schematic representation, not to scale, o the light beam path for the apparatus incorporating the dified invention;
1~Figure 8 is an unfolded schematic representa-tion of the light beam formation as it passes through diferent lens assemblies in the apparatus of the invention;
Figure 9 is a perspective view, not to scale, of the apparatus o the invention;
Figure 10 is a partial top plan view of apparatus incorporating the invention;
Figure 11 i~ a plan of the organization of the views of Figure llA and llBi and 25Figures llA and llB are side elevational views of the modular structure of the invention.
~ESCRIPTIO~ OF ONE EMBODIMENT OF THE INVENTIO~
In one of its broadest aspects the apparatus of the present invention is typified by the arrangements set forth schematically in Figure 1. The laser diode printer apparatus 10 is seen to comprise a laser diode 12, energized in a known manner to produce a beam of electromagnetic radiation, arrow 14, which is adapted to sc~
be passed through a lens system 16 which acts to collimate the light beam 14 and direct the collimated liyh-t beam 18 into and through a pair of optical prisms 20 and 22, respectively, ~hich act to change the beam from an elliptical cross section to a circular cross section.
The now collimated, altered, beam 24 of light is next directed through a focusing lens 26 to a rotatable polygonal mirror assembly 28. The focused light beam 30 is reflected off the faces or facets of the polyyon 28 as the latter is rotated by drive motor 32 in the direction of arrow 3~. The rays 36 of the reflected beam are focused onto the photoconductive drum surface 38 of rotatable drum 40 via a tiltable mirror assembly 42 and a second focusing lens system 44, Figure 1.
The focusad laser beam 46 is adapted to scan the cylindrical photGconductor surface 38 from edge to edye or side to side to means of the rotating polygon mirror 28 and drive motor 28. Modulation (by means not shown) of the laser diode 12 produces a latent electro-static image upon the surface 38 of photoconductor 40.
Copying and/or printing media 48, Figures 5 and 6, ls adapted to receive the image o~ the intelligence carried by the latent electrostatic ima~e by means o~ and ln a manner to be described 1.ater on herein.
A physical embodiment of the apparatus 1~
schematically` illustrated in Figure 1 is seen most clearly in the side elevational view of Figure 2, to comprise a rigid base member 50 on which the entire assembly is mounted and adapted to be slideably moveable back and forth or right to left as the case may be. A~
earlier mentioned, mirror 42 is adapted to be tllted 75¢D~315 .
about its horizontal axis mounting pivot 52 so as to fold the laser beam 36 upwardly toward the cylindxical lens 44, Figure l. Tilting adjustment of the mirror 42 is provided by means of the threaded horizontal cross shaft 54 adjustably moveable by means of thumb wheel 56 against the vertical mirror support column 58 disposed - in vertical mounting pillar 60 secured to base 50.
Vertical, erectable movement of mirror 42 is provided by means of slo~ 62 and pin 64, as seen most clearly in Figure 2.
The laser diode 12 (light generatiny element) is surrounded by a thermo-electric cooling member 66 and is gimbally mounted, as at 68 to support 70. A heat sink 72 of copper or similar material capable of rapidly and efficiently dissipating large quantities of heat abuts the laser diode assembly 12. The gimble pivoting arrangement 68 supports the heat sink 72 and cooling member 66 enabling the laser diode 12 to be pivoted about two orthogonal axes that pass directly through the diode chip. The laser diode temperature is regulated so as to be constant at approximately 20-21 degreees C by a feedback controller with a thermistor sensor (not shown). It is necessary that the heat sink temperature, which is close to ambient, be somewhat above the c~ntrol temperature since the thermoelectric device can only cool and cannot heat.
The laser light 14 emitted by the diode 12 is ; collected by the objective lens 16 which in one embodiment comprises a microscope objective having a maynification of 20 times. This is necessary since the output area ~of the diode is about two tenths micron by about five micronsj from which light is being emitted and is extremely small. The objective lens 16 has the ~ ~ ~75~
laser light at its focu~. The light enters the lens as a diverging set of light rays 14 from the laser diode 12. The objective lens 16 ~ollimates the light, as seen most clearly in ~igure 2. Since the light from the diode 12 is diverging on the entering side of lens 16 and is collimated on the exiting side thereof, the bea~
is not generally circular but rather oblong or ellipti-cal in cross section.
In order to correct ~his9 two separate but optically complimentary photo-optical elements are employed. The collimated light is first passed through prism 20 which is configured so as to compress the beam in the vertical plane or direction down to approximately one tenth inch. Therea~ter, the beam is redirected into and through prism 22 which is constructed such that the li~ht bealn is expanded slightly in the horizontal direction. Exiting from the second ~rism 22 the light beam now has a ciroul2r cross section and is collimated before entering focusing lens 26.
Except for the tiltable mirror 42, which is provided with its own separate, individual adju table mounting ~eans previously described, each of the lenses and prisms heretofore mentioned are provided with separate means ~or orthogonally positioning these eLements relative to each other as well as with respect to the axis of the laser liyht beam.
A rigid elevating platform 74 is secured to the base 50 to which is mounted, as by bolts (not shown) a second rigid mount 76. ~ember 76 provides oppositely disposed parallel guidin~ tracks (not shown) for slide-ably moviny support member 78. To one end of the me~ber 78 is secured a rockably, pivoted support member 80 accurately moveable about pivot 82 on the leftward ~'7~
projecting end of the member 78. Member 80 provides a tiltable support for the laser diode 12 including its heat sink 72 as well as for the objective lens assembly 16 and its adjus~ing means. Vertical, slideable, adjust-ment for diode 12 is controlled and actuated by means ofmicrometer slides and the knurled thumb wheel 84. The horizontal adjustment is by means of thumb wheel 8~, Figure 4. Rockins movement for platforln 8~ to axially align the laser beam 14 is provided by means of the threaded adjusting wheel 88 which is adapted to rockably pivot the member 80 about pivot 82 by means of threaded shaft 90 against the right end of member 80. Sliding, focus.i}lg adjustment for objective lens assembly 16 is provided by thumb wheel and shaft assembly 92 at the rightward end of member 80.
Laser beam light rays 18 pass, as before mentioned, through a compression prism 20 which is angularly, adjusta~]y mounted on a horizontal pivot 94 and tiltable about this pivot by means of thumb wheel 96, cam 9~ and L-shaped follower link 100. Adjustrnent movement of prism 72 is accomplished by means o~ thumb wheel 102, Figures 2 and 4, cylindrical cam 104 and L-shaped cam follower 10~ secured to prism 22. Focusing lens 26 is threadedly, adjustable backwards and forward 2~ for accurate focus ing by rotation within the lens support 108.
The focused laser light beam 30 after passing throuyh the focusing lens 26 is reflectively scanned across the surface 38 of photoconducting drum member 40 3 in a manner such that the data or intelligence contained in the modulated beam is placed upon the drum for copying/printing purposes, as will be hereinaftar described.
S~.5 Polygon mirror 28, rotating in the direction of arrow 34 by drive motor 32 carries 20 mirror facets and rotates at the rate of 12,558 RPM. The laser light is passed from the ocusing lens 26 to the face of each mirror facet so as to scan through an angle of 3~
degrees (as the polygon rotates) which is precisely twice the angle that the facet moves through during the period of time for one scan line. With the focusi~g lens 26 positioned in front of or before the polygon 28, the focal point tends to be on the arc of a sphere.
Rather than in a plane this marks for correction problems since the beam 24 passes throuyh the same point of this lens all the time. Additionally, as the polygon scanner 28 rotates, the deflected beam is rotatiny at a constant rotational rate so the speed will be constant on an arc but will not be constant on the straight scan line. The beam or spot speeds up at the periphery, which produces a small effect in changing the dimension of the characters.
In the preferred embodiment as seen in Figure 3 a focusing lens 110 is positioned after the polygon 28.
This lens characterized as a F-theta lens (fe) and avoids the variation of lineal scan velocity with the scan angle. Normally, the spot displacement d of a simple lens varies as the focal length times the tangent of theta. (d = f tan- e). It is possible to make an F-theta (fe) lens so that the lineal displacement varies as the focal length times theta (fe) itself. This allows a linear relationship between polygon rotation and spot position. Plus, it produces a flatter field so that th~ focus is in a plane (including the scan line).
The (fe) lens is triplet lens.
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As the polyyon 28 turns, the focused light is reflected off tilt mirror 42 and angularly, upwardly into and through the elongated, focusing cylindrical lens 44 to be raster scanned across the photoconductor 40. Only about 25 degrees of the total scan is used for the printed scan line. Located on the right hand side of the scan line facing the drum 40 is a start of scan detector (not shown) which is used to time the initia-tion-of printing.
Lens 44 has a 1at surface on one side and convex surface Oll the other side and is utilized to reduce the vertical or facet apex angle error, an error in the position of the beam due to wobbling of the facets from one facet to the other, i.e., the so-called change in the apex angle. (The angle between the axis of rotation of the pvlygon and the facet, varies from one facet to the other and this variation causes the beam to deflect sll~htly in the vertical direction).
Utilization of cylindrical lens 44 reduces the effect of the wobble. The rotating polygon causes the light to scan a full raster scan length i.e. the width of the dru,n or the width of the lins that is to be printed on the page one scan length for each facet on the polygon.
Obviously, the more facets there are on the polygon the easier it is to reduce the RPM's required of this rotating device. For example, with only eight facets the device would have to be rotated at a high RPM to get the same number of scans per seconds. Scans per second is determined by the speed at whlch it is desired to 3 print. At ninety pages per minute this is approxi~
mately 6,000 lines per minute. This is a lineal surface velocity on the drum of 17.42 inches per second. The raster line spacing is determined by the resolution ~L~'7~
~13-desired for 240 dots per inch. Each raster line is spaced by 1 over 240. Thus, the raster scan lines ars spaced l/240th of an inch or .00417 inches apart.
Dividing the raster line spacing by the velocity of the drum gives the time permitted for each scan line. The reciprocal of the scan line time gives the scan rate.
In other words, the scan rate would be just equal to 17.44 inches per second by .00417 inches. However, since .00417 is equivalent to 1 over 24~, the result can be expressed as 17.44 times 240 dots per inch. This gives a repetition rate for the scan in scans per second. Each scan occurs in approximately 239 micro-seconds. Obviously, the more facets on the polygon the more the total RPM can be reduced. The present polygon has 20 facets. The number of facets is tied in with the resolution that is desired to be achieved.
To derive the desired resolution, the beam must be expanded to a pre~etermined size as it is passed into the final focusi~g lens. The larger the beam goiny into the focusing lens~ the smaller the spot size. A
reciprocal relationshlp exists between the spot size and beam size entering the focusing lens. The larger the beam going into the focus lens, the smaller the spot size. In other words, when the aperture is smal]. at the focusing lens, the di*fraction is greater so the d~E~action limited spot is larger. Thus, the collimated beam size (aperture) should be larger to obtain a small spot.
PRINTING/COPYING STATION
_ Referring now to Figures 5 and 6, with emphasis first to Figure 5, there is shown a highly schematic or diagrammatic ~ide elevational view o~ the electrophoto-graphic process station of the present invention. The - ~t~5~5 bloc'~ identified in Figure 5 as "optical scanning assembly" is ~eant, for purposes of illustration, to include the complete optical structural arrangement shown in Figure 2 including the cylindrical ~ocusing lens 44 through which the modulated laser beam 46 passes to impinge upon the rotatable drum 40. The cylindrical lens corrects for any beam motion introduced by the rotating polygon and its associated vertically disposed mirrors.
Drum 40 is provided with a relatively hard, long wearing, photoconductive coatiny 38 having a high infrared response, Figure 1 and is adapted to be rotated in the direction of arrow 112. The size of the drum is calculated to accept 11 inch or 14 inch length sheets o plain paper for copying/printing in serial fashion, one after the other, so as to increase the general "through put" of the apparatus.
Initially the drum 40 has no surface charge on it and no toner. The charge coratron 114, which consists of six wires stretched across, parallel to but out of contact with the drwn surface, is electrically energized p~acing a uniform electrical char~e across the photoconductive surface 38. The drum 40 rotates clock-wise, so that the light from the laser diode 12 strikes the areas on the drurn surface where no printing is desired which discharges the background. The laser diode beam is swept across the length of the drum and selectively modulated with the intelligence necessary to produce the printed matter desired. Each scan line at a resolution of 240 dots per inch will have 240 scan lines per inch of printing. The dots will be generated by turning the laser diode 12 on and of to get the intelligence information on the dru.n. The drum now has ~ ~7S~
~elective regions of electrical charge and regions that are discharged or have no electrical char~e thus forming a latent electrostatic image thereon.
The drun next passes to the toner station 11~.
; Toner station 116 has an electrical charge bias supply to the toner 118 with a polarity and magnitude such that the toner is attracted to the drum surfaces 38 in the regions corresponding to where the print will be. At this point in the process, the apparatus has produced a developed image. As the drum 40 continues to rotate fur~her, it comes into the transfer area 120 where the image is to be transferred from the photoconductive drum to the copy material, e.g. paper 48. Paper 48 is moved from left to r ght axrow 122. Two implementations are employed for toner transfer. Both of them use electro-static means. Nonconductive toner 118 is used. The paper 48 is charged by means of a transfer coratron 124.
The coratron wires develop an electrostatic charge field which essentially causes the toner to have a greater attraction towards the paper 48 and the downstream (rightward) detac coratron 126 than it does towards the photoconductive drum 40. The toner effectively lifts off th~e drum and is applied to the paper. The detac coratron 126 separates the paper 48 from the drum to which is electrostatically attracted. Detac coratron 126 applies a DC pulse at the front or leadin~ edge of the paper to li~t the leading edge up. As the paper continues to move under member 126 and as soon as the leading edge is picked up off the drum, an AC electrical potential is applied to member 126. This di~char~es the paper, the paper 48 thus is lifted off the drum with the toner intact.
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The paper carrying the toner image next passes into the fuser 128 which is a combination of pressure and heat produced by means of two opposing roller mernbers 130 and 132, respectively. Thereafter, the papar is passed into the next station of the machine at - which time the paper bears an image o~ the intelligence copied or printed thereon. Although greater than 98 per cent of the toner is transferred to the paper 48, in order to offset the problems with residual toner on the photoconductive druln, if any, a preclean coratron 134 and preclean lamp member 136 are used. An AC coratron wire is used at this point with the AC switchiny polarity between positive and negative, discharges the surface of the drum 40 and also discharges the toner 118. Since light also discharges the surface of the druln a low wattage (8 watt)fluorescent bar li~ht is used to make sure tha~ all of the charge is removed in addition to the toner. A vacuum cleanin~ station 138 provided with a rotating bristle brush 140 of soft bristles, with a vacuum applied from a source (not shown~ sucks off residual toner which may be on the drum. ~t this point the drum is considered to be clean as far as toner is concerned. However, since toner was covering some suraces of the photoconductor that the light from the drum is rotated past a inal discharge lamp 142. Light from lamp 142 shines onto a completely cleared drurn removes all residual charge very effectively. The apparatus is now ready to start the copy process again at the charge coratron 114.
If however, the paper for some reason, does not detach or lift up o~f the drum 40, oppositely disposed stripper finger members 144, which protrude slightly into the drw~ and into recessed areas at the edyes i.e.
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opposite sides of the paper, catch the paper and tend to lift the paper away from the drum.
DESCRIPTION OF ANOTHER EMBODIMEL~T OF THE PRESE~T I~EL~TION
_ Briefly, as seen in the highly schematic, views g of Figures 7 and 8 a laser diode lOA mounted behind a sapphire window 12A is pulsed by a driver circuit (not shown) which is fed from the imaging electronics operably coupled ~o the present apparatus and also not shown herein. The logic i5 set up such that ~he laser diode is "off" when intelligible characters or other information is to be prin~ed. Solid state laser diodes of the double heterostructure variety produce a diverging ~eam of light when pulsed by the driver circuit and therefore, requires collimated optics.
15Light rays 14A emitted from the laser diode lOA
are first collected and collimated by a four element objective lens assembly the elements of which are designated 16A, 18A, ~OA and 22A respectively, provided with spherical elements. The first two lenses act as converging or positive elements and collect the light with minimum aberration while the third objective element 20A is a diverging lens that compensates the residual aberration from the other three elements.
Collimated light 24A erneryes from fourth element 22A
when the facet of the laser diode chip lOA is located at the focal point of the objective lens assernbly. The collimated beam 24A now has an elliptical shape corresponding to the differing divergence angles of the beam from the laser diode lOA in planes parallel and 3o perpendicular to the junction of the diode. It is noted that a three element objec~ive lens could be employed in place of the present four element lens assembly with suitable choice of glasses.
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The collimated laser beam 24A is then scanned and focused onto a rotatable photoreceptor drum 26A, Figs. 8 and 9 by means of a polygon scanner assembly 28A
and a set of four lens elements designated hereinafter.
An additional function of the four lens set i5 to correct for the pyramidal angle variation or the varia-- tion in the angle be~een the facets of the polygon and the axis of rotation. Without this correction the laser scan lines on the drum 26A would not overlap uniformly from one scan line to the next. Since the light from the la'ser diode lOA discharges the surface potential or white space between the latent images of characters and or intelliyible information, the variable overlap of scan lines would cause a variation in the discharga of the potential therefore and cause lines to appear in the "white" space of the toned image.
The above variation in scan line overlap is reduced in the following manner. First, the collimated beam 24A is focused in the cross scan direction by a first cylindrical lens 30A to form a line image on the facet of the polygon 28A. Lenses that follow tha poly-gon 28A focus the beam to a small spot on the photo-receptor 26A.
I the line of focus is strictly in the plane of the facet, then rotation of the facet about that focus line would produce no movement of the subsequently focused spot on the photoreceptor 26A. In practice, however, the correction for pyramidal angle error is not absolute and the focus~d spot will move slightly in the cross scan direction as a line cannot be perfectly focused on the facet for all positions. Following the polygon 28A a cylindrical meniscus lens 32A serves to focus the beam to a small dimension in the scanning or ~ ~75~
horizontal direction. By appropriately curving or bendiny ~his lens the field of the horizontal ocus can be ~lattened and the aberration can be minimized. This lens interacts very weakly with the ver~ical or cross scan focus since the power is negligible in that direc~ion. The cross scan or vertical focus~ng is achieved by a pair of cylindrical-spherical lenses 3~A
and 36A with the corresponding centers of the cylindrical and spherical surfaces located near the facet and with power mainly in the vertical or cross scan direction. Thus, aberrations in the vertical direction are reduced and the field is flattened in the scan direction first by using a pair of lenses and second by bending or curving the lenses slightly in the horizontal direction. It can be shown from thin lens theory that the index of refraction of the glass in the pair should be greater than 1.62 to have a finite separa-tion between the pair. Plint glasses such as SF6 have a high index of refraction and allow a comfortable space between the pair. One novel aspect of thls optical combination is that the pair approximates a pair of toroidal lenses which have been used in the prior art but which are expensive to manufacture. Another novel aspect is that the horizontal and vertical spot size can be focused independently. Finally, a mirror 38A, Figure 9 bends the light at a suitable angle to cause the light to impinge upon the surface of drum 26A.
Referring to the detailed drawings Fiyure lO
and llA and llB the laser diode lOA is moun~ed on a copper block 42A, as seen from above. The copper block in turn is mounted on a thermo-electric cooler 44A that cools the laser diode lOA to approximately l9 degrees centigrade. The diode lOA is positioned accurately by ~S~D~
means of a setup fixture (not shown) rel~tive to a microscope objective 46A 50 that it is on the center line of the microscope objective optics. The position of the laser diode lOA is thus preset relative to the optical axis before installing it in the laser diode assembly. The diode ase~bly lOA including cooler 44~ is - positioned on locating pins (not shown) that locate it so as to avoid any adjustments while in place on the copy machine. From the laser diode l~A the light diverges, more in the hori7ontal direction than in the vertical direction. The horizontal direction is characterized herein as "the scan direction" and the vertical direction is characterized herein as the "cross scan direction". The light in the scan direction diverges by 30 degrees to the half intensity points on the beam and by 10 degrees to the half intensity points on the beam i~ the cross scan direction. After the light passes through the microscope ohjective 46A, the beam is collimated assumin~ that the microscope objective is positioned properly. This divergence of the beam produces a different beam si7e in the scan direction as opposed to the cross scan direction. The beam produces a diferent beam size in the scan direction as opposed to the cross scan dir~ction. The beam will have a larger dimension in the cross scan direction than in the scan direction with about a three to one ratio.
~ he collimated beam is next passad through a cylindrical lens 48A. The ~irst cylindrical lens (similar to lens 30A) has power in the cross scan direction and will cause the beam to focus down to a line image on the rotatable polygon 50A. It does not have any power in the scan direction. The baam is still 1~7$~D~
collimated in the scan or horizontal direc-tion. The light is then focused by a horizontal meniscus lens 52A
(similar to lens 32A~ which is the first lens following the polygon 50A. Lens 52A has power in the scan 5 direction only so it focuses the wide horizontal dimension of the beam down to a narrow spot on the photo-receptor drum 54A after passing throuyh the third and fourth lenses 58A and 60A, respectively, ~identical to lenses 34A and 36A) which individually have no power in 10 the horizontal direction and, after reflecting off of folding mirror 56A (identical to mirror 38A) is in focus both horizontally and vertically on the drum 54A. For the cross scan direction, the bealn is focused by the third ana fourth lenses 58A and 60A which have a 15 cylindrical surface on the first surface 62A and 64A, respectively, and a spherical surface 6~A and 68A on the second su~face, respectively. T~is pair of lenses (following each other in succession) have power in the 20 cross scan direction and essentially focus the line which is imaged on the polygon 50A to a point in the cross scan dirçction. The focusing in the other direction is performed by the horizontal meniscus lens 52A which is, as before mentioned, the first lens 25 following the polygon.
The lenses are curved 50 as to flatten the field. The horiæonta} meniscus lens 52A is generally curved concave toward the facet of the polygon 50A, almost producing a spherical surface with its center at 30 the facet. The curving or bending of t~e lenses permits the field of focus at the drum 54A to be flat and also improves the scan linearity at the drum.
~t751~5 -~ ach one of the four lenses 43A, 52A, 62A and 64A is demountably removable relative to each respective frame of ref rence. This permits cleaning, polishiny, replacement, e;c. Fixed locating pins 60A are arranged to provide ixed reference for each lens and 5 enables these individual elements to be removed at wlll and replaced without fear of mislocation.
As can be seen in Figures 10, llA and llB the complete optical assembly is mounted within a rectangu-- lar casting 70~ which includes a cover 72A that encloses the top of the casting. The top 72A itself is provided with an air inlet 74A and a flange 76A that comes down close over the polygon 50A. Rotation of the polygon 50 by motor 78A creates a vacuum which causes air to be pulled in through a filter 80A that is centered over the l; top of the polyson 50A. The filtered air is forced out inside of the optical castiny 70A to create a positive air pressure therein. The air flow is through the casting 70A, through an elongated opening 82A (the beam scanning aperture) up through a wedge shaped shroud 84A
20 that is mounted to the top cover 72A. The air pressure is maintained such that the positive air flow prevents toner from getting .into casting 70A. The shroud 84A is angled in such a way as to overhang the as~embly, thus the optics is protected ~rom dust, dirt or falliny 25 objects from falling directly into the optics.
As can be seen in Figures 9 and 10 the beam is folded off of folding mirror 56A Figure 10 and directed up through the shroud 84~ to the photoreceptor drum 54A.
Beam scanning begins with each facet rotation starting 3 from the left side of thne drum 26A Figure 9. The beam crosses a start of scan detector 88A that is mounted up near the photoreceptor 54A. This member provides the 51~ 5 timiny for the printing that is to be performed. The start of scan pulse provided by detector 88A is used to initiate the print cycle on a scan line and so many counts after that pulse, the electronics (not shown) initiates the unloading of the dot line buffers (not shown) that provides the information for each character - in bit form.
The polyyon 50A which is six inches in diameter is provided with 1-3 facets 90A. Obviously the smaller the number of facets the higher the speed must be. The size of the present polygon was chosen for a thirty page per minute copier so as to keep the RPM of the motor down to a speed around 4900 RPM. At this speed the polygon is expected to last for the life o the machine.
The size of the facets 90A were selected to provide uniform illumination across the full scan width. The beam as it falls on facet 90A is about two tenths of an inch in diameter bet~een half intensity points. This is the so-called underilled case,i.e. a facet 90A is under-filled. The intensity of the scanning beam or scanningspot must remain constant across the full scan width.
If part of the beam is cut of toward the edge of the facets, this results in a decrease of intensity. The width of the facets is designed so as to keep the intensity of the beam constant across a nine and a half inch scan within five percent variation. The nine and a half inch dimension is slightly wider than the width of the drum. The start of the scan detector 88A is included within this dimension.
3 The complete optical assembly of the present invention is set into the printer/copier machine on a pair of pivots 92A. One on each opposite side of castin-~ 70A to the left in Figure llA. The center of ~'7~
these pivot points passes through the center 94A of folding mirror 56A. The whole assembly is horizontally angularly adjusted by means of screw 96A and slot 98A on the underslde of casting 70A located at the opposite end 5 of the casting removed fro~ the pivot points. After the box like assembly 7~A is placed into the machine, the adjusting screw 96A tilts the whole assembly until the beam falls onto the start to scan detector 88A. By having the pivot points pass through the center of folding mirror 56A the plane of focus remains sub-stantially constant or unchanged on the photoreceptor as the assembly is tilted to make the beam fall on the start of scan detector.
There has thus been described a new, novel and heretofore unobvious photo-optical laser diode printing/
copying apparatus which provides a very high speed, very efficient and very cost effective combination of oper-ational apparatus tG provide clean, clear, crisp copies without the attendant problems associated with much of the prior art devices.
The method and structure permits the use of less expensive cylindrical lenses but also tends to ~latten the field. However, it remains a very dif ficult problem to flatten the fie]d over wide angles when relatively high resolution is required.
SUMMARY OF THE INVENTION
The present invention overcomes the above difficulties first, by providing a cylindrical meniscus lens with power in the horizontal scan direction to focus the beam to a small spot in the scan direction.
~ ~75~9~i Second, by providing a pair of cylindrical-spherical lenses to provide cross-scan or vertical focus. The cylindrical-spherical lenses provide a function similar to a pair o~ toric lenses but at a more reasonable cost.
For the laser diode scanning system of the present invention it is also an advantage to have the horizontal - and vertical focus independent.
The optical system of the present invention is structured and fabricated as demountable, unitary, modular assembly independent of the remainder of the apparatus with which it is or may be operably associ-ated. The lens assemblies of the optical system, once adjusted for focus, are fixed in position with.in the module although each lens is in fact demountable for replacement without the need for realign~ent upon re-insertion in the assembly. The module is sealed against du t and dirt contaminatior. and is provided with its own source of pressurize~ air to prevent dust and dirt from accumulating within the assembly from one source or another. Additionally the module is angularly adjust-ably positionable relative to the photoreceptor drum and includes means for preventing accidental ingress of toner into the optical module. Precisely located pivot pins enable accurate adjustment of the optics relative to the photoreceptor drum which, once fixed in position, need no further adjustment or alteration.
It is, ~herefore, an object for the present invention to overcome ~ach of these problems in a new, novel and heretofore unobvious manner and to provide a photo-optical solid state laser diode scanning system wherein a solid state laser is caused to produce a divergent beam of visible electromagnetic radiation which is collected and collimated and thereafter - ~.1L7~
optically shaped to reduce the vertical dimension while expanding the horizontal dimension for subsequent impingement upon a rotatable polygonal mirror assembly.
The collimated laser beam is then focused onto a photo-conductor, for example, a rotatable drum, through acylindrical lens and a light folding mirror, passing through a spherical lens to the photoconductor itself.
A novel aspect of the invention is the pro-vision for the apparatus to be modularly related and to be mounted to a rigid, fixed base mel~ber. Each element of the novel combination is adjustably, positionable relative to the base as well as to the axis of the laser beam, the lenses, mirrors and polygonal mirror facets thereby insuring an ~ccurate, clear and highly defined, latent image on the photoconductor,i.e. drum.
Another novel aspect of the present invention is the yrovision ~f a novel photoconductor drum charging, exposing, toning and cleaning apparatus for a laser diode and printing and/or copying apparatus utilizing a novel folded laser scanning light path in combination with a corna charging, discharging apparatus not heretofore available in electrophotographic processing apparatus.
Other objects, features and advantages of the invention will be readily apparent from the following description of two different embodiments thereof, taken in conjunction with the ~ccompanying drawings, although variations and modifications may be efected without departing from the spirit and scope of the novel concepts of the disclosuxe.
BRIEF DESCRIPTION OF THE DRAWINGS
Figure 1 is a schematic side elevational view, not to scale, of apparatus embodying the present invention;
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Figure 2 is a detailed side elevational view o the apparatus of Figure l;
Figure 3 is a schematic top end view not to scale, of the apparatus of Figures 1 and 2;
` Figure 4 is a detailed top plan view of the apparatus of Figure 3;
Figure 5 is a schematic illustration, not to scale, of the electrophotographic process sta~ion of the present invention;
10Figure 6 is a detailed view of the apparatus illustrated in Fisure 5;
Figure 7 is a schematic representation, not to scale, o the light beam path for the apparatus incorporating the dified invention;
1~Figure 8 is an unfolded schematic representa-tion of the light beam formation as it passes through diferent lens assemblies in the apparatus of the invention;
Figure 9 is a perspective view, not to scale, of the apparatus o the invention;
Figure 10 is a partial top plan view of apparatus incorporating the invention;
Figure 11 i~ a plan of the organization of the views of Figure llA and llBi and 25Figures llA and llB are side elevational views of the modular structure of the invention.
~ESCRIPTIO~ OF ONE EMBODIMENT OF THE INVENTIO~
In one of its broadest aspects the apparatus of the present invention is typified by the arrangements set forth schematically in Figure 1. The laser diode printer apparatus 10 is seen to comprise a laser diode 12, energized in a known manner to produce a beam of electromagnetic radiation, arrow 14, which is adapted to sc~
be passed through a lens system 16 which acts to collimate the light beam 14 and direct the collimated liyh-t beam 18 into and through a pair of optical prisms 20 and 22, respectively, ~hich act to change the beam from an elliptical cross section to a circular cross section.
The now collimated, altered, beam 24 of light is next directed through a focusing lens 26 to a rotatable polygonal mirror assembly 28. The focused light beam 30 is reflected off the faces or facets of the polyyon 28 as the latter is rotated by drive motor 32 in the direction of arrow 3~. The rays 36 of the reflected beam are focused onto the photoconductive drum surface 38 of rotatable drum 40 via a tiltable mirror assembly 42 and a second focusing lens system 44, Figure 1.
The focusad laser beam 46 is adapted to scan the cylindrical photGconductor surface 38 from edge to edye or side to side to means of the rotating polygon mirror 28 and drive motor 28. Modulation (by means not shown) of the laser diode 12 produces a latent electro-static image upon the surface 38 of photoconductor 40.
Copying and/or printing media 48, Figures 5 and 6, ls adapted to receive the image o~ the intelligence carried by the latent electrostatic ima~e by means o~ and ln a manner to be described 1.ater on herein.
A physical embodiment of the apparatus 1~
schematically` illustrated in Figure 1 is seen most clearly in the side elevational view of Figure 2, to comprise a rigid base member 50 on which the entire assembly is mounted and adapted to be slideably moveable back and forth or right to left as the case may be. A~
earlier mentioned, mirror 42 is adapted to be tllted 75¢D~315 .
about its horizontal axis mounting pivot 52 so as to fold the laser beam 36 upwardly toward the cylindxical lens 44, Figure l. Tilting adjustment of the mirror 42 is provided by means of the threaded horizontal cross shaft 54 adjustably moveable by means of thumb wheel 56 against the vertical mirror support column 58 disposed - in vertical mounting pillar 60 secured to base 50.
Vertical, erectable movement of mirror 42 is provided by means of slo~ 62 and pin 64, as seen most clearly in Figure 2.
The laser diode 12 (light generatiny element) is surrounded by a thermo-electric cooling member 66 and is gimbally mounted, as at 68 to support 70. A heat sink 72 of copper or similar material capable of rapidly and efficiently dissipating large quantities of heat abuts the laser diode assembly 12. The gimble pivoting arrangement 68 supports the heat sink 72 and cooling member 66 enabling the laser diode 12 to be pivoted about two orthogonal axes that pass directly through the diode chip. The laser diode temperature is regulated so as to be constant at approximately 20-21 degreees C by a feedback controller with a thermistor sensor (not shown). It is necessary that the heat sink temperature, which is close to ambient, be somewhat above the c~ntrol temperature since the thermoelectric device can only cool and cannot heat.
The laser light 14 emitted by the diode 12 is ; collected by the objective lens 16 which in one embodiment comprises a microscope objective having a maynification of 20 times. This is necessary since the output area ~of the diode is about two tenths micron by about five micronsj from which light is being emitted and is extremely small. The objective lens 16 has the ~ ~ ~75~
laser light at its focu~. The light enters the lens as a diverging set of light rays 14 from the laser diode 12. The objective lens 16 ~ollimates the light, as seen most clearly in ~igure 2. Since the light from the diode 12 is diverging on the entering side of lens 16 and is collimated on the exiting side thereof, the bea~
is not generally circular but rather oblong or ellipti-cal in cross section.
In order to correct ~his9 two separate but optically complimentary photo-optical elements are employed. The collimated light is first passed through prism 20 which is configured so as to compress the beam in the vertical plane or direction down to approximately one tenth inch. Therea~ter, the beam is redirected into and through prism 22 which is constructed such that the li~ht bealn is expanded slightly in the horizontal direction. Exiting from the second ~rism 22 the light beam now has a ciroul2r cross section and is collimated before entering focusing lens 26.
Except for the tiltable mirror 42, which is provided with its own separate, individual adju table mounting ~eans previously described, each of the lenses and prisms heretofore mentioned are provided with separate means ~or orthogonally positioning these eLements relative to each other as well as with respect to the axis of the laser liyht beam.
A rigid elevating platform 74 is secured to the base 50 to which is mounted, as by bolts (not shown) a second rigid mount 76. ~ember 76 provides oppositely disposed parallel guidin~ tracks (not shown) for slide-ably moviny support member 78. To one end of the me~ber 78 is secured a rockably, pivoted support member 80 accurately moveable about pivot 82 on the leftward ~'7~
projecting end of the member 78. Member 80 provides a tiltable support for the laser diode 12 including its heat sink 72 as well as for the objective lens assembly 16 and its adjus~ing means. Vertical, slideable, adjust-ment for diode 12 is controlled and actuated by means ofmicrometer slides and the knurled thumb wheel 84. The horizontal adjustment is by means of thumb wheel 8~, Figure 4. Rockins movement for platforln 8~ to axially align the laser beam 14 is provided by means of the threaded adjusting wheel 88 which is adapted to rockably pivot the member 80 about pivot 82 by means of threaded shaft 90 against the right end of member 80. Sliding, focus.i}lg adjustment for objective lens assembly 16 is provided by thumb wheel and shaft assembly 92 at the rightward end of member 80.
Laser beam light rays 18 pass, as before mentioned, through a compression prism 20 which is angularly, adjusta~]y mounted on a horizontal pivot 94 and tiltable about this pivot by means of thumb wheel 96, cam 9~ and L-shaped follower link 100. Adjustrnent movement of prism 72 is accomplished by means o~ thumb wheel 102, Figures 2 and 4, cylindrical cam 104 and L-shaped cam follower 10~ secured to prism 22. Focusing lens 26 is threadedly, adjustable backwards and forward 2~ for accurate focus ing by rotation within the lens support 108.
The focused laser light beam 30 after passing throuyh the focusing lens 26 is reflectively scanned across the surface 38 of photoconducting drum member 40 3 in a manner such that the data or intelligence contained in the modulated beam is placed upon the drum for copying/printing purposes, as will be hereinaftar described.
S~.5 Polygon mirror 28, rotating in the direction of arrow 34 by drive motor 32 carries 20 mirror facets and rotates at the rate of 12,558 RPM. The laser light is passed from the ocusing lens 26 to the face of each mirror facet so as to scan through an angle of 3~
degrees (as the polygon rotates) which is precisely twice the angle that the facet moves through during the period of time for one scan line. With the focusi~g lens 26 positioned in front of or before the polygon 28, the focal point tends to be on the arc of a sphere.
Rather than in a plane this marks for correction problems since the beam 24 passes throuyh the same point of this lens all the time. Additionally, as the polygon scanner 28 rotates, the deflected beam is rotatiny at a constant rotational rate so the speed will be constant on an arc but will not be constant on the straight scan line. The beam or spot speeds up at the periphery, which produces a small effect in changing the dimension of the characters.
In the preferred embodiment as seen in Figure 3 a focusing lens 110 is positioned after the polygon 28.
This lens characterized as a F-theta lens (fe) and avoids the variation of lineal scan velocity with the scan angle. Normally, the spot displacement d of a simple lens varies as the focal length times the tangent of theta. (d = f tan- e). It is possible to make an F-theta (fe) lens so that the lineal displacement varies as the focal length times theta (fe) itself. This allows a linear relationship between polygon rotation and spot position. Plus, it produces a flatter field so that th~ focus is in a plane (including the scan line).
The (fe) lens is triplet lens.
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As the polyyon 28 turns, the focused light is reflected off tilt mirror 42 and angularly, upwardly into and through the elongated, focusing cylindrical lens 44 to be raster scanned across the photoconductor 40. Only about 25 degrees of the total scan is used for the printed scan line. Located on the right hand side of the scan line facing the drum 40 is a start of scan detector (not shown) which is used to time the initia-tion-of printing.
Lens 44 has a 1at surface on one side and convex surface Oll the other side and is utilized to reduce the vertical or facet apex angle error, an error in the position of the beam due to wobbling of the facets from one facet to the other, i.e., the so-called change in the apex angle. (The angle between the axis of rotation of the pvlygon and the facet, varies from one facet to the other and this variation causes the beam to deflect sll~htly in the vertical direction).
Utilization of cylindrical lens 44 reduces the effect of the wobble. The rotating polygon causes the light to scan a full raster scan length i.e. the width of the dru,n or the width of the lins that is to be printed on the page one scan length for each facet on the polygon.
Obviously, the more facets there are on the polygon the easier it is to reduce the RPM's required of this rotating device. For example, with only eight facets the device would have to be rotated at a high RPM to get the same number of scans per seconds. Scans per second is determined by the speed at whlch it is desired to 3 print. At ninety pages per minute this is approxi~
mately 6,000 lines per minute. This is a lineal surface velocity on the drum of 17.42 inches per second. The raster line spacing is determined by the resolution ~L~'7~
~13-desired for 240 dots per inch. Each raster line is spaced by 1 over 240. Thus, the raster scan lines ars spaced l/240th of an inch or .00417 inches apart.
Dividing the raster line spacing by the velocity of the drum gives the time permitted for each scan line. The reciprocal of the scan line time gives the scan rate.
In other words, the scan rate would be just equal to 17.44 inches per second by .00417 inches. However, since .00417 is equivalent to 1 over 24~, the result can be expressed as 17.44 times 240 dots per inch. This gives a repetition rate for the scan in scans per second. Each scan occurs in approximately 239 micro-seconds. Obviously, the more facets on the polygon the more the total RPM can be reduced. The present polygon has 20 facets. The number of facets is tied in with the resolution that is desired to be achieved.
To derive the desired resolution, the beam must be expanded to a pre~etermined size as it is passed into the final focusi~g lens. The larger the beam goiny into the focusing lens~ the smaller the spot size. A
reciprocal relationshlp exists between the spot size and beam size entering the focusing lens. The larger the beam going into the focus lens, the smaller the spot size. In other words, when the aperture is smal]. at the focusing lens, the di*fraction is greater so the d~E~action limited spot is larger. Thus, the collimated beam size (aperture) should be larger to obtain a small spot.
PRINTING/COPYING STATION
_ Referring now to Figures 5 and 6, with emphasis first to Figure 5, there is shown a highly schematic or diagrammatic ~ide elevational view o~ the electrophoto-graphic process station of the present invention. The - ~t~5~5 bloc'~ identified in Figure 5 as "optical scanning assembly" is ~eant, for purposes of illustration, to include the complete optical structural arrangement shown in Figure 2 including the cylindrical ~ocusing lens 44 through which the modulated laser beam 46 passes to impinge upon the rotatable drum 40. The cylindrical lens corrects for any beam motion introduced by the rotating polygon and its associated vertically disposed mirrors.
Drum 40 is provided with a relatively hard, long wearing, photoconductive coatiny 38 having a high infrared response, Figure 1 and is adapted to be rotated in the direction of arrow 112. The size of the drum is calculated to accept 11 inch or 14 inch length sheets o plain paper for copying/printing in serial fashion, one after the other, so as to increase the general "through put" of the apparatus.
Initially the drum 40 has no surface charge on it and no toner. The charge coratron 114, which consists of six wires stretched across, parallel to but out of contact with the drwn surface, is electrically energized p~acing a uniform electrical char~e across the photoconductive surface 38. The drum 40 rotates clock-wise, so that the light from the laser diode 12 strikes the areas on the drurn surface where no printing is desired which discharges the background. The laser diode beam is swept across the length of the drum and selectively modulated with the intelligence necessary to produce the printed matter desired. Each scan line at a resolution of 240 dots per inch will have 240 scan lines per inch of printing. The dots will be generated by turning the laser diode 12 on and of to get the intelligence information on the dru.n. The drum now has ~ ~7S~
~elective regions of electrical charge and regions that are discharged or have no electrical char~e thus forming a latent electrostatic image thereon.
The drun next passes to the toner station 11~.
; Toner station 116 has an electrical charge bias supply to the toner 118 with a polarity and magnitude such that the toner is attracted to the drum surfaces 38 in the regions corresponding to where the print will be. At this point in the process, the apparatus has produced a developed image. As the drum 40 continues to rotate fur~her, it comes into the transfer area 120 where the image is to be transferred from the photoconductive drum to the copy material, e.g. paper 48. Paper 48 is moved from left to r ght axrow 122. Two implementations are employed for toner transfer. Both of them use electro-static means. Nonconductive toner 118 is used. The paper 48 is charged by means of a transfer coratron 124.
The coratron wires develop an electrostatic charge field which essentially causes the toner to have a greater attraction towards the paper 48 and the downstream (rightward) detac coratron 126 than it does towards the photoconductive drum 40. The toner effectively lifts off th~e drum and is applied to the paper. The detac coratron 126 separates the paper 48 from the drum to which is electrostatically attracted. Detac coratron 126 applies a DC pulse at the front or leadin~ edge of the paper to li~t the leading edge up. As the paper continues to move under member 126 and as soon as the leading edge is picked up off the drum, an AC electrical potential is applied to member 126. This di~char~es the paper, the paper 48 thus is lifted off the drum with the toner intact.
~ 7~
The paper carrying the toner image next passes into the fuser 128 which is a combination of pressure and heat produced by means of two opposing roller mernbers 130 and 132, respectively. Thereafter, the papar is passed into the next station of the machine at - which time the paper bears an image o~ the intelligence copied or printed thereon. Although greater than 98 per cent of the toner is transferred to the paper 48, in order to offset the problems with residual toner on the photoconductive druln, if any, a preclean coratron 134 and preclean lamp member 136 are used. An AC coratron wire is used at this point with the AC switchiny polarity between positive and negative, discharges the surface of the drum 40 and also discharges the toner 118. Since light also discharges the surface of the druln a low wattage (8 watt)fluorescent bar li~ht is used to make sure tha~ all of the charge is removed in addition to the toner. A vacuum cleanin~ station 138 provided with a rotating bristle brush 140 of soft bristles, with a vacuum applied from a source (not shown~ sucks off residual toner which may be on the drum. ~t this point the drum is considered to be clean as far as toner is concerned. However, since toner was covering some suraces of the photoconductor that the light from the drum is rotated past a inal discharge lamp 142. Light from lamp 142 shines onto a completely cleared drurn removes all residual charge very effectively. The apparatus is now ready to start the copy process again at the charge coratron 114.
If however, the paper for some reason, does not detach or lift up o~f the drum 40, oppositely disposed stripper finger members 144, which protrude slightly into the drw~ and into recessed areas at the edyes i.e.
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opposite sides of the paper, catch the paper and tend to lift the paper away from the drum.
DESCRIPTION OF ANOTHER EMBODIMEL~T OF THE PRESE~T I~EL~TION
_ Briefly, as seen in the highly schematic, views g of Figures 7 and 8 a laser diode lOA mounted behind a sapphire window 12A is pulsed by a driver circuit (not shown) which is fed from the imaging electronics operably coupled ~o the present apparatus and also not shown herein. The logic i5 set up such that ~he laser diode is "off" when intelligible characters or other information is to be prin~ed. Solid state laser diodes of the double heterostructure variety produce a diverging ~eam of light when pulsed by the driver circuit and therefore, requires collimated optics.
15Light rays 14A emitted from the laser diode lOA
are first collected and collimated by a four element objective lens assembly the elements of which are designated 16A, 18A, ~OA and 22A respectively, provided with spherical elements. The first two lenses act as converging or positive elements and collect the light with minimum aberration while the third objective element 20A is a diverging lens that compensates the residual aberration from the other three elements.
Collimated light 24A erneryes from fourth element 22A
when the facet of the laser diode chip lOA is located at the focal point of the objective lens assernbly. The collimated beam 24A now has an elliptical shape corresponding to the differing divergence angles of the beam from the laser diode lOA in planes parallel and 3o perpendicular to the junction of the diode. It is noted that a three element objec~ive lens could be employed in place of the present four element lens assembly with suitable choice of glasses.
.
~L7~
The collimated laser beam 24A is then scanned and focused onto a rotatable photoreceptor drum 26A, Figs. 8 and 9 by means of a polygon scanner assembly 28A
and a set of four lens elements designated hereinafter.
An additional function of the four lens set i5 to correct for the pyramidal angle variation or the varia-- tion in the angle be~een the facets of the polygon and the axis of rotation. Without this correction the laser scan lines on the drum 26A would not overlap uniformly from one scan line to the next. Since the light from the la'ser diode lOA discharges the surface potential or white space between the latent images of characters and or intelliyible information, the variable overlap of scan lines would cause a variation in the discharga of the potential therefore and cause lines to appear in the "white" space of the toned image.
The above variation in scan line overlap is reduced in the following manner. First, the collimated beam 24A is focused in the cross scan direction by a first cylindrical lens 30A to form a line image on the facet of the polygon 28A. Lenses that follow tha poly-gon 28A focus the beam to a small spot on the photo-receptor 26A.
I the line of focus is strictly in the plane of the facet, then rotation of the facet about that focus line would produce no movement of the subsequently focused spot on the photoreceptor 26A. In practice, however, the correction for pyramidal angle error is not absolute and the focus~d spot will move slightly in the cross scan direction as a line cannot be perfectly focused on the facet for all positions. Following the polygon 28A a cylindrical meniscus lens 32A serves to focus the beam to a small dimension in the scanning or ~ ~75~
horizontal direction. By appropriately curving or bendiny ~his lens the field of the horizontal ocus can be ~lattened and the aberration can be minimized. This lens interacts very weakly with the ver~ical or cross scan focus since the power is negligible in that direc~ion. The cross scan or vertical focus~ng is achieved by a pair of cylindrical-spherical lenses 3~A
and 36A with the corresponding centers of the cylindrical and spherical surfaces located near the facet and with power mainly in the vertical or cross scan direction. Thus, aberrations in the vertical direction are reduced and the field is flattened in the scan direction first by using a pair of lenses and second by bending or curving the lenses slightly in the horizontal direction. It can be shown from thin lens theory that the index of refraction of the glass in the pair should be greater than 1.62 to have a finite separa-tion between the pair. Plint glasses such as SF6 have a high index of refraction and allow a comfortable space between the pair. One novel aspect of thls optical combination is that the pair approximates a pair of toroidal lenses which have been used in the prior art but which are expensive to manufacture. Another novel aspect is that the horizontal and vertical spot size can be focused independently. Finally, a mirror 38A, Figure 9 bends the light at a suitable angle to cause the light to impinge upon the surface of drum 26A.
Referring to the detailed drawings Fiyure lO
and llA and llB the laser diode lOA is moun~ed on a copper block 42A, as seen from above. The copper block in turn is mounted on a thermo-electric cooler 44A that cools the laser diode lOA to approximately l9 degrees centigrade. The diode lOA is positioned accurately by ~S~D~
means of a setup fixture (not shown) rel~tive to a microscope objective 46A 50 that it is on the center line of the microscope objective optics. The position of the laser diode lOA is thus preset relative to the optical axis before installing it in the laser diode assembly. The diode ase~bly lOA including cooler 44~ is - positioned on locating pins (not shown) that locate it so as to avoid any adjustments while in place on the copy machine. From the laser diode l~A the light diverges, more in the hori7ontal direction than in the vertical direction. The horizontal direction is characterized herein as "the scan direction" and the vertical direction is characterized herein as the "cross scan direction". The light in the scan direction diverges by 30 degrees to the half intensity points on the beam and by 10 degrees to the half intensity points on the beam i~ the cross scan direction. After the light passes through the microscope ohjective 46A, the beam is collimated assumin~ that the microscope objective is positioned properly. This divergence of the beam produces a different beam si7e in the scan direction as opposed to the cross scan direction. The beam produces a diferent beam size in the scan direction as opposed to the cross scan dir~ction. The beam will have a larger dimension in the cross scan direction than in the scan direction with about a three to one ratio.
~ he collimated beam is next passad through a cylindrical lens 48A. The ~irst cylindrical lens (similar to lens 30A) has power in the cross scan direction and will cause the beam to focus down to a line image on the rotatable polygon 50A. It does not have any power in the scan direction. The baam is still 1~7$~D~
collimated in the scan or horizontal direc-tion. The light is then focused by a horizontal meniscus lens 52A
(similar to lens 32A~ which is the first lens following the polygon 50A. Lens 52A has power in the scan 5 direction only so it focuses the wide horizontal dimension of the beam down to a narrow spot on the photo-receptor drum 54A after passing throuyh the third and fourth lenses 58A and 60A, respectively, ~identical to lenses 34A and 36A) which individually have no power in 10 the horizontal direction and, after reflecting off of folding mirror 56A (identical to mirror 38A) is in focus both horizontally and vertically on the drum 54A. For the cross scan direction, the bealn is focused by the third ana fourth lenses 58A and 60A which have a 15 cylindrical surface on the first surface 62A and 64A, respectively, and a spherical surface 6~A and 68A on the second su~face, respectively. T~is pair of lenses (following each other in succession) have power in the 20 cross scan direction and essentially focus the line which is imaged on the polygon 50A to a point in the cross scan dirçction. The focusing in the other direction is performed by the horizontal meniscus lens 52A which is, as before mentioned, the first lens 25 following the polygon.
The lenses are curved 50 as to flatten the field. The horiæonta} meniscus lens 52A is generally curved concave toward the facet of the polygon 50A, almost producing a spherical surface with its center at 30 the facet. The curving or bending of t~e lenses permits the field of focus at the drum 54A to be flat and also improves the scan linearity at the drum.
~t751~5 -~ ach one of the four lenses 43A, 52A, 62A and 64A is demountably removable relative to each respective frame of ref rence. This permits cleaning, polishiny, replacement, e;c. Fixed locating pins 60A are arranged to provide ixed reference for each lens and 5 enables these individual elements to be removed at wlll and replaced without fear of mislocation.
As can be seen in Figures 10, llA and llB the complete optical assembly is mounted within a rectangu-- lar casting 70~ which includes a cover 72A that encloses the top of the casting. The top 72A itself is provided with an air inlet 74A and a flange 76A that comes down close over the polygon 50A. Rotation of the polygon 50 by motor 78A creates a vacuum which causes air to be pulled in through a filter 80A that is centered over the l; top of the polyson 50A. The filtered air is forced out inside of the optical castiny 70A to create a positive air pressure therein. The air flow is through the casting 70A, through an elongated opening 82A (the beam scanning aperture) up through a wedge shaped shroud 84A
20 that is mounted to the top cover 72A. The air pressure is maintained such that the positive air flow prevents toner from getting .into casting 70A. The shroud 84A is angled in such a way as to overhang the as~embly, thus the optics is protected ~rom dust, dirt or falliny 25 objects from falling directly into the optics.
As can be seen in Figures 9 and 10 the beam is folded off of folding mirror 56A Figure 10 and directed up through the shroud 84~ to the photoreceptor drum 54A.
Beam scanning begins with each facet rotation starting 3 from the left side of thne drum 26A Figure 9. The beam crosses a start of scan detector 88A that is mounted up near the photoreceptor 54A. This member provides the 51~ 5 timiny for the printing that is to be performed. The start of scan pulse provided by detector 88A is used to initiate the print cycle on a scan line and so many counts after that pulse, the electronics (not shown) initiates the unloading of the dot line buffers (not shown) that provides the information for each character - in bit form.
The polyyon 50A which is six inches in diameter is provided with 1-3 facets 90A. Obviously the smaller the number of facets the higher the speed must be. The size of the present polygon was chosen for a thirty page per minute copier so as to keep the RPM of the motor down to a speed around 4900 RPM. At this speed the polygon is expected to last for the life o the machine.
The size of the facets 90A were selected to provide uniform illumination across the full scan width. The beam as it falls on facet 90A is about two tenths of an inch in diameter bet~een half intensity points. This is the so-called underilled case,i.e. a facet 90A is under-filled. The intensity of the scanning beam or scanningspot must remain constant across the full scan width.
If part of the beam is cut of toward the edge of the facets, this results in a decrease of intensity. The width of the facets is designed so as to keep the intensity of the beam constant across a nine and a half inch scan within five percent variation. The nine and a half inch dimension is slightly wider than the width of the drum. The start of the scan detector 88A is included within this dimension.
3 The complete optical assembly of the present invention is set into the printer/copier machine on a pair of pivots 92A. One on each opposite side of castin-~ 70A to the left in Figure llA. The center of ~'7~
these pivot points passes through the center 94A of folding mirror 56A. The whole assembly is horizontally angularly adjusted by means of screw 96A and slot 98A on the underslde of casting 70A located at the opposite end 5 of the casting removed fro~ the pivot points. After the box like assembly 7~A is placed into the machine, the adjusting screw 96A tilts the whole assembly until the beam falls onto the start to scan detector 88A. By having the pivot points pass through the center of folding mirror 56A the plane of focus remains sub-stantially constant or unchanged on the photoreceptor as the assembly is tilted to make the beam fall on the start of scan detector.
There has thus been described a new, novel and heretofore unobvious photo-optical laser diode printing/
copying apparatus which provides a very high speed, very efficient and very cost effective combination of oper-ational apparatus tG provide clean, clear, crisp copies without the attendant problems associated with much of the prior art devices.
Claims (21)
1. An Optical scanning and imaging system util-izing laser diode light generation comprising;
a solide state laser light generating device producing a divergent electromagnetic visible emission;
means for collecting and collimating said divergent emission into a beam of light;
means for optically shaping said beam to effectively expand the verticle dimension thereof; and for reducing the horizontal dimension of said beam;
a rotatable polygon mirror assembly in the path of said light beam and having a plurality of flat mirror facets disposed around the periphery thereof;
means for bringing said beam into sharp focus on a single facet of said rotatable ploygon mirror assembly;
angularly, adjustably positionable, reflective means disposed adjacent to said polygon mirror assembly;
a photoconductive drum rotatably disposed adjacent to said adjustably positionable reflective means, and focusing means interposed between said polygon mirror assembly and said adjustably positionable reflective means for bringing said beam into focus on said drum as said beam is moved by said polygon mirror assembly across the surface of said rotatable drum effectively causing said beam to scan said drum from side to side.
a solide state laser light generating device producing a divergent electromagnetic visible emission;
means for collecting and collimating said divergent emission into a beam of light;
means for optically shaping said beam to effectively expand the verticle dimension thereof; and for reducing the horizontal dimension of said beam;
a rotatable polygon mirror assembly in the path of said light beam and having a plurality of flat mirror facets disposed around the periphery thereof;
means for bringing said beam into sharp focus on a single facet of said rotatable ploygon mirror assembly;
angularly, adjustably positionable, reflective means disposed adjacent to said polygon mirror assembly;
a photoconductive drum rotatably disposed adjacent to said adjustably positionable reflective means, and focusing means interposed between said polygon mirror assembly and said adjustably positionable reflective means for bringing said beam into focus on said drum as said beam is moved by said polygon mirror assembly across the surface of said rotatable drum effectively causing said beam to scan said drum from side to side.
2. The invention in accordance with Claim wherein said optical scanning system is adjustably mounted to a rigid base assembly for linear movement along fixed guide rails.
3. The invention in accordance with Claim 1 wherein said solid state laser and collimating means are gimbal mounted and disposed on a rigid support pivotally mounted to said rigid base assembly and including a conductive dissipating element for removing heat from said laser.
4. The invention in accordance with Claim 1 further including means for slidably positioning said collimating means relative to said laser light generating device and further including vernier adjusting means for tilting said laser and said collimating means about a fixed axis.
5. The invention in accordance with Claim 1 wherein said light collecting-collimating means comprises a microscope objective which collects the diverging light from the laser and collimates the light into a beam of substantially elliptical cross section.
6. The invention in accordance with Claim 1 wherein said means to reduce the vertical dimension of said beam and the horizontal dimension of the beam to produce exiting beam of a circular cross section prior to entering said optical focusing means comprise optical prisms.
7. The invention in accordance with Claim 1 wherein said adjustable mirror assembly further includes both a vertical as well as a horizontal tilt adjusting means for accurately positioning said beam at the surface of said photoconductive drum.
8. The invention in accordance with Claim 1 wherein said elongated focusing lens comprises a cylindrical optical assembly.
9. The invention in accordance with Claim 1 wherein said optical focusing means is positioned in the beam path subsequent to the beam reflecting off the selected facet of said polygon.
10. The invention in accordance with Claim 1 wherein said laser is mounted to a thermoelectric cooling member and wherein said cooling member and said laser are gimbal mounted to said rigid support including vertical and horizontal adjustment means for said laser.
11. The invention in accordance with Claim 1 wherein said means for optically shaping said beam is replaced by multiple optical means in the focus of said beam providing cross scan focusing in the vertical direction so as to produce the same function as toroidal lenses but wherein the surface characteristics of said optical means is relatively simple and easier to fabricate.
12. Optical scanning system for laser diode printing apparatus utilizing a folded light beam path comprising;
a rotatable photoreceptor drum capable of receiving a latent photo-optical image of intelligible indicia thereon;
solid state laser light beam generating means;
a rotatable polygon multi-facet mirror assembly for causing said light beam to scan the drum in a horizontal dir-ection;
optical light collimating means for collimating the beam from said laser light generating means;
means focussing the light beam from said collimating means into a line image on a facet of said polygon mirror ass-embly;
means focussing the scanned light beam to a small di-mension in the horizontal direction on the photoreceptor drum;
multiple optical means in the focus of said scanned light beam providing cross-scan focussing in the vertical direction producing the same function as toroidal lenses but having sur-face characteristics which are simple and easier to fabricate;
and reflecting means adjustably disposed in the path of said scanned light beam for folding said light beam back upon itself for impingement on said photoreceptor drum.
a rotatable photoreceptor drum capable of receiving a latent photo-optical image of intelligible indicia thereon;
solid state laser light beam generating means;
a rotatable polygon multi-facet mirror assembly for causing said light beam to scan the drum in a horizontal dir-ection;
optical light collimating means for collimating the beam from said laser light generating means;
means focussing the light beam from said collimating means into a line image on a facet of said polygon mirror ass-embly;
means focussing the scanned light beam to a small di-mension in the horizontal direction on the photoreceptor drum;
multiple optical means in the focus of said scanned light beam providing cross-scan focussing in the vertical direction producing the same function as toroidal lenses but having sur-face characteristics which are simple and easier to fabricate;
and reflecting means adjustably disposed in the path of said scanned light beam for folding said light beam back upon itself for impingement on said photoreceptor drum.
13. The invention in accordance with claim 12 wherein said laser diode is provided with a heat sink and wherein cooling means is provided to maintain said diode at a fixed temperature relative to ambient during operation.
14. The invention in accordance with claim 12 wherein said collimating means comprises a compound optical lens assem-bly including first and second light converging elements, a third spherical light diverging means, fourth light converging means and light generating means located at the focal point of said objection lens assembly producing an elliptically shaped beam corresponding to the differing divergence angles of the beam from the laser diode in planes parallel and perpendicular to the junction of the diode.
15. The invention in accordance with claim 12 wherein said means focussing said light beam into a line image comprises a cylindrical lens with its curved surface oriented toward the compound collimating lens assembly.
16. The invention in accordance with claim 12 wherein said means focussing said light being scanned to a small dimen-sion in the horizontal direction comprises a cylindrical menis-cus lens.
17. The invention in accordance with claim 16 wherein said cylindrical meniscus lens is bent or bowed effectively flattening the field of the horizontal focus thereby minimizing any aberrations that might occur.
18. The invention in accordance with claim 12 wherein said multiple optical means providing cross-scan focussing in the vertical direction comprises cylindrical-spherical lenses with the centers of the spherical surfaces located near the facet of the polygon and with power mainly in the vertical or cross-scan direction.
19. The invention in accordance with claim 18 wherein said cylindrical-spherical lenses are bent or curved in the horizontal direction effectively reducing aberrations in the vertical direction while the field is flattened in the scan direction.
20. The invention in accordance with claim 19 wherein said cylindrical-spherical lenses are each provided with a cylindrically curved surface on the first surface portion there-of and with a spherically curved surface on the second curved surface, thereby essentially focussing the line which is imaged on the polygon assembly to a point in the cross-scan direction.
21. The invention in accordance with claim 12 wherein said means focussing said light being scanned to a small dimension comprises a horizontal cylindrical meniscus lens generally curved concave toward the facet of the polygon assembly.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CA000423657A CA1175095A (en) | 1983-03-15 | 1983-03-15 | Unitary, modular demountable optical system for laser 1 diode printing copying apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CA000423657A CA1175095A (en) | 1983-03-15 | 1983-03-15 | Unitary, modular demountable optical system for laser 1 diode printing copying apparatus |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA1175095A true CA1175095A (en) | 1984-09-25 |
Family
ID=4124789
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA000423657A Expired CA1175095A (en) | 1983-03-15 | 1983-03-15 | Unitary, modular demountable optical system for laser 1 diode printing copying apparatus |
Country Status (1)
| Country | Link |
|---|---|
| CA (1) | CA1175095A (en) |
-
1983
- 1983-03-15 CA CA000423657A patent/CA1175095A/en not_active Expired
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