CA1066932A - Flying spot scanner - Google Patents
Flying spot scannerInfo
- Publication number
- CA1066932A CA1066932A CA306,001A CA306001A CA1066932A CA 1066932 A CA1066932 A CA 1066932A CA 306001 A CA306001 A CA 306001A CA 1066932 A CA1066932 A CA 1066932A
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- cylindrical lens
- scan
- spot
- light
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Abstract
FLYING SPOT SCANNER
ABSTRACT OF THE DISCLOSURE
A flying spot scanning system is provided by utilizing reflected light from a multifaceted rotating polygon which is then directed to the scanned medium.
A light source illuminates at least two contiguous facets of the polygon during each scanning cycle, to provide the desired sequence of spot scanning. To assure a uniform spot size at the scanned medium, an optical convolution of elements is selected in combination with the light source such that an adequate depth of focus at the medium is assured. In each scanning cycle, information is transmitted to the scanned medium by modulating the light from the light source in accordance with a video signal.
ABSTRACT OF THE DISCLOSURE
A flying spot scanning system is provided by utilizing reflected light from a multifaceted rotating polygon which is then directed to the scanned medium.
A light source illuminates at least two contiguous facets of the polygon during each scanning cycle, to provide the desired sequence of spot scanning. To assure a uniform spot size at the scanned medium, an optical convolution of elements is selected in combination with the light source such that an adequate depth of focus at the medium is assured. In each scanning cycle, information is transmitted to the scanned medium by modulating the light from the light source in accordance with a video signal.
Description
' ` 10669~Z
BACKGROUND OF THE IN~7ENTION
This invention relates to a flying spot scanning system for communicating video information to a scanned medium, and more particularly to a scanning system which utilizes a multifaceted rotating polygon for controlling the scanning cycles.
Much attention has been given to a various optical approaches in flying spot scanning for the purpose of imparting the information content of a modulated lig~t beam to a scanned medium. Galvanometer arrangements have been used to scan the light across a document for recording its information content thereon.
Such arrangements have included planar reflecting mirrors which are driven in an oscillatory fashion. Other approaches have made use of multifaceted mirrors which are driven continuously. Various efforts have been made to define the spot size in order to provide for an optimum utilization of the scanning system.
~ ne such effort is that described in United States Patent No. 3,675,016. The approach used was to make the spot size invariant and as small as possible by defining the dimensions of the focused beam so that only part, preferably half, of a mirror facet is illuminated during ~canning. This teaching alludes to generalized techniques for assuring the constancy of the size of the aperture of a rotating mirror scanning system. ~y either illuminating several facets of the mirror or by directing light in a beam that is sufficiently narrow to assure that less than a full facet is the most that can ever be illuminated by the beam and limiting scanning to that portion of the rotary travel of the facet when such facet i~ illuminated by all of such light beam. However, such system apertures are dimensionally invariant because the dimensions of the rotating facets have no influence on such apertures.
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. '~'' ~066932 While the system as described in U.S. Patent No.
3,675,016 may have advantages over the prior art, nevertheless, various constraints must be imposed upon the spot size and other relationships of optical elements within the system which are not always desirable.
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~ ' 1066932 SUMMARY OF THE INVENTION
In accordance with an aspect of this invention there is provided apparatus for recording information from an electrical signal onto a scanned medium comprising: means for providing a beam of high intensity light, means for modulating the light beam in accordance with the information content of an electrical signal, means for focusing said modulated beam to a spot upon the surface of a light sensitive medium at a predetermined distance from said focusing means, scanning means positioned in the optical path of said modulated beam for scanning the spot across said medium to impart the :
information content of said spot to said medium, a first cylindrical lens so positioned in the optical path of the focused beam between said scanning means and said medium that runout errors are substantially corrected at said medium, the plane of no power of said cylindrical lens being oriented in the direction of scan, means for deflecting a portion of the scanned spot to provide a second beam directed at a predetermined start of scan position located spatially from said medium, means for detecting the start of the scan located at said start of scan position at a distance from said focus-ing means approximately equal to said predetermined distance, and a second cylindrical lens so positioned in the path of said second beam between said detecting means and said deflecting means that runout errors are substantially corrected at said detecting means, the plane of no power of said second cylindrical lens being oriented in the direction of scan.
In accordance with another aspect of this invention there is provided apparatus for recording information from an electrical signal onto a scanned medium comprising: means for providing a beam of high intensity light, means for modulating the light beam in accordance with the information content of an electrical signal, first optical means for ~ _ 4 _ - ~066932 expanding said modulated beam, second optical means in convolu-tion with said first optical means for imaging said expanded beam to a spot in a focal plane at a predetermined distance from said second optical means, scanning means positioned between said second means and the focal plane for scanning the spot across a light sensitive medium in said focal plane to impart the information content of said spot to said medium, means for detecting the start of the scan located spatially from said medium at said predetermined distance from said ;~
second optical means, means for deflecting a portion of the scanned spot at a predetermined start of scan position to form a second beam directed away from said medium to illuminate said detecting means, a first cylindrical lens so positioned in the optical path of the imaged beam between said second optical means and said medium that runout errors are substan-tially corrected at said medium, the plane of no power of said cylindrical lens being oriented in the direction of scan, and a second cylindrical lens so positioned in the second beam path between said deflecting means and said detecting means that runout errors are substantially corrected at said detect-ing means, the plane of no power of said second cylindrical lens being oriented in the direction of scan.
A feature of an embodiment of the invention is that the beam of light incident upon the multifaceted polygon illuminates at least two contiguous facets of the polygon during each scanning cycle to provide the desired sequence of spot scanning. Such feature provides a flying spot scan-ning system which has an extremely high duty cycle.
Another feature of an embodiment of the invention is that a very large depth of focus is provided for the spot at the contact loci at the surface of the scanned medium.
This feature is provided by utilizing a finite conjugate ~ - 4a -- ~66932 imaging system in convolution with the light beam and the rotating polygon. A doublet lens, in series with a convex imaging lens between the light source and the medium provides such an arrangement. The doublet lens enables the original light beam to be sufficiently expanded for illuminating multiple contiguous facets of the polygon, - 4b --` 106693Z
whereas the imaging lens converges the expanded beam to focus at the contact loci on the surface of the scanned . . .
medium. Employing such an optical system assures a uniform spot size at the scanned medium even though a substantial scan width is traversed by the spot.
Still another feature of an embodiment of the invention is the modulation of the original light beam by means of a video signal. The information content within the video signal is thereby imparted to the light beam itself. The medium to be scanned is one which is responsive to the modulated beam and records its information content as contained within the scanning spot in a usable form on its ! surface across the scan width.
Also, another feature of an embodiment of the invention is that a start/stop of scan detection apparatus is in combination with and substantially matches the con-volution of imaging elements which focus the flying spot at the surface of the scanned medium, although such detection apparatus is spacially distant from the scanned medium.
Yet another feature of an embodiment of the invention includes an embodiment of the flying spot scanning system for utilization in high speed xerography. The scanned medium in such an embodiment would consist of a xerographic drum which rotates consecutively through a charging station, an exposure station where the spot traverses che scan width of the drum, through a developing station, and a transfer station where a web of copy paper is passed in contact with the drum and receives an electrostatic discharge to induce the transfer of the developed image from the drum to the 30 copy paper. A fusing device then fixes the images to the copy paper as it passes to an output station.
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DESCRIPTION OF THE DRAWINGS
Figure 1 is an isometric illustration of a flying spot scanning system in accordance with the invention.
Figure 2(a) is a partial perspective view illus-trating the-use of the scanning beam generated by the system of Figure 1.
Figure 2(b) is a top perspective view of the optical system shown in Figure 2(a). ~ -Figure 3 is an isometric illustration of a first alternate to the flying spot scanner of Figure 1 and with the same numbers indicating the same or similarly operating parts.
Figure 4 is a perspective view of the utiliza-tion of the scanning beam according to the first alternate embodiment.
Figure 5 is an isometric illustration of a second alternative to the flying spot scanning system of Fisure 1 and wherein the same number indicates same or similar parts.
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~06693Z
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Figure 6(a) is a side perspective view of the utilization of the cylindrical correction lens of Figure 6.
Figure 6(b) is a top perspective view of the utilization of the cylindrical lens.
Figure 7 is an isometric illustration third alternative to that of Figure 1 of a flying spot scanning system with the same numerals indicating the same or similar parts.
DESCRIPTION OF THR PREFERRED EMBODIMENT
In Figure 1, an embodiment of a flying spot scanning system in accordance with the invention is shown. A light ; source 1 provides the original light beam for utilization by the scanning s~stem. The light source 1 is preferably a laser which generates a collimated beam of monochromatic light which may easily be modulated by modulator 4 in conformance with the information contained in a video signal.
Modulator 4 may be any suitable electro-optical modulator for recording the video information in the form of a modulated light beam 6 at the output of the modulator 4.
The modulator 4 may be, for example, a Pockel's cell comprising a potassium dihydrogen phosphate crystal, whose index of re-fraction is periodically varied by the application of the vary-ing voltage which represents the video signal. The video signal may contain information either by means of binary pulse code modulation or wide-band frequency code modulation. In any event, by means of the modulator 4 the information within the video signal is represented by the modulated light beam 6.
The light beam 6 is reflected from mirror 8 in convolution with a doublet lens 10. The lens 10 may be any lens, preferably of two elements, which elements are in spaced relation to each other such that the external curved suxfaces are provided in symmetry with the internal surfaces. Preferably the internal surfaces of lens 10 are cemented together to form a common contact zone. Of course, as is often the case in the embodiment of such a lens as a microscope objective, the elements may be fluid spaced.
The lens 10 is required to image the axial point of beam 6 through a focal point on the opposite side of lens 10.
At the focal point, beam 6 diverges or expands to form beam 12 which impinges upon at least two contiguous facets of a scanning polygon 16.
In this embodiment, the rotational axis of polygon 16 is orthogonal to the plane in which light beams 6 travels.
The facets of the polygon 16 are mirrored surfaces for the reflection of any illuminating light impinging upon them.
With the rotation of the polygon 16, a pair of light beams are reflected from the respective illuminated facets and turned through a scan angle for flying spot scanning.
Alternatively, flying spot scanning could be provided by any other suitable device, such as mirrored piezoelectric crystals or planar reflecting mirrors which are driven in an oscillatory fashion.
In all of these arrangements, however, the reflecting surfaces would be at a distance S from the originating focal point of light beam 12 and in orthogonal relation to the plane bounded by the beam 6 such that the reflected beams would be in substantially the same plane as beam 6.
At a distance a from the leading illuminated facet :
of polygon 16 is positioned an imaging lens 20. Lens 20 is -of a diameter D to cooperate with the respective reflected light beams throughout an angle of 2 ~ to render convergent beams 22 which define a focal plane 24 at a distance f from the imag- :
ing lens 20. In this preferred embodiment, imaging lens 20 is ; a five element compound lens as disclosed in United States Patent 3,741,521 issued January 10, 1973 and assigned to the assignee of the present invention. The focal plane 24 is proximate a recording medium 25 whose surface 26 is brought in contact with the respective focal spots of the convergent light beams throughout a scan width x.
A uniform spot size is assured throughout the scan width x even though a curved focal plane 24 is defined through-out the scanning cycle. The lens 10 in convolution with the imaging lens 20 provides a finite conjugate imaging system which allows a large depth of focus d which is coextensive with the contact loci of a spot throughout the scan width x on the :
surface 26 of the medium 25.
The beam of light from the light source 1, through the optical elements and reflected from the scanning polygon to the scanning medium 25 defines a light path.
As shown in figure 2(a), medium 25 may be a xero-graphic drum which rotates consecutively through a charging station depicted by corona discharge device 27, exposure surface 26 where the beam from the rotating polygon 16 traverses the scan width x on the drum 25, through developing station 28 depicted by a cascade development enclosure, transfer station 30 where a web of copy paper is passed in contact with the drum 25 and receives an electrostatic discharge to induce a transfer of the developed image from the drum 25 to the copy paper.
The copy paper is supplied from the supply reel 31, passes around guide rollers 32 and through drive rollers 33 into rec~iving bin 35. A fusing device 34 fixes the images to ~e copy paper as it passes to bin 35.
Usable images are provided in that the information c~ntent of the scanning spot is represented by the modulated or variant intensity of light respective to its postion within the scan width x. As the spot traverses the charged surface 26 th~ough a given scan angle c7~, the spot dissipates t~e electrostatic charge in accordance with its light intensity. The electrostatic charge pattern thus produced i~ developed in the developing station 28 and then transferred to the final copy paper. The xerographic drum 25 is cleaned by some cleaning device such as a rotating brush 36 bef~re being recharged by charging device 27. In this manner, the information content of the scanned spot i8 recorded on a more permanent and useful medium. Of course, alternative prior art techniques may be employed to cooperate with a scanned spot in order to utilize the information contained therein.
m e polygon 16 is continuously driven by a motor 40 and synchronized in rotation to a synchronization signal representative of the scan rate used to obtain the original video signal. The rotation rate of the xerographic drum 25 determines the spacing of the scan lines. It also may be peferable to synchronize the drum 25 in some manner to the signal source to maintain image linearity. The source image is reproduced in accordance with the signal and is transferred to prlntout paper for use or storage.
4~ _ 9_ ` ~066932 The number of facets has been found to be optimum if at least 20 to 30 facets are employed. The scan angle o~
traversed would be equal to the number of facets chosen in relation to one complete revolution of the polygon 16. An extremely useful arrangement would have the polygon 16 with 24 facets and a scan anglec~ of 15 degrees. Since the depth of focus d of the converging beam 22 is related to the scan angle in that as the scan angle c~ increases the radius of curvature of the focal plane 24 increases, it is important to define a scan angle in relation to the desired scan width x. For a scan width x of approximately ll inches it has been found that the scan angle o~ of 12 to 18 degrees, with 20 to 30 facets on the polygon 16, is optimum. Figure 2(b) is a top perspective view of the optical system shown in Figure 2(a).
The optical system of the present invention provides a virtually lO0~ duty cycle scan for the entire scan angle c~ by virtue of the illumination of at least two contiguous facets. The illumination of two contiguous facets is preferred. ~With such illumination, another scanning spot is provided at a distance equal to the scan width x behind the leading scanning spot with virtually no wait between successive scans. With the continuous rotation of the polygon 16 additional contiguous facets are subsequently illuminated, thereby providing successive convergent beams following the leading convergent beam 22 by no more than the scan angle, if so desired. Thus, a flying spot scanning system which has an extremely high duty cycle is provided.
The optical system of the present invention projects the highest energv portion of the laser beam onto the rotating - 9a -1()66932 polygon and to the photoreceptor surface. The energy output of the laser beam has a Gaussian distribution with the highest intensity distribution being concentrated near the axis of projection. In the Gaussian distribution the highest inten-sity energy is located at the centre of the beam. By spreading the beam out over a plurality of facets, the beam centre portion having the highest intensity radiation energy fills all the polygon facets reflecting the beam onto the photoconductive surface. The fringes of the beam having the lowest Gaussian energy intensities are spread out beyond those polygon facets and are excluded from the information signal scanned across the photoreceptor surface. Shaping the beam to spread it across a plurality of facets thereby filters the lower energy radiation within the beam and excludes it, permitting the utilization of the maximum energy content of the beam.
In the first alternate embodiment as shown in Figure 3, the light beam 6 is reflected from mirror 8 in convolution with a doublet lens 10. The lens 10 may be any lens, preferably of two elements, which elements are in spaced relation to each other such that external curved surfaces are provided in symmetry with the internal surfaces.
Preferably the internal surfaces of lens 10 are cemented together to form a common contact plane. Of course, as is often the case in the embodiment of such a lens as a micro-scope objective, the elements may be fluid spaced. The lens 10 is required to image either a virtual or real axial point of beam 6 through a focal point, for example, on the opposite side of lens 10 for a real image. At the focal point, beam 6 diverges or expands to form beam 12 which would be more than sufficient to impinge upon a given facet of a scanning polygon 16.
At a distance S2 from the leading illuminated facet of polygon 16 is positioned an imaging lens 18. Lens 18 is ~
of a diameter D to cooperate with the expanded light beam 12 ;
to render a convergent beam 2 which illuminates the desired facets to reflect respective light beams 22 to focus to focal plane 24 at a distance d from the polygon 16. In this first alternate embodiment, imaging lens 18 is a l-n element lens.
The focal length f of lens 18 is related to Sl, S2 and d by the following thin lens equation: 1 +
Sl S2 +d f The rotational axis of polygon 16 is orthogonal to the plane in which light beam 6 travels. The facets of the polygon 16 are mirrored surfaces for the reflection of any illuminating light impinging upon them. With the rotation of the polygon 16, assuming two contiguous facets are illuminated at a given time, a pair of light beams 22 are reflected from the respective illuminated facets and turned through a scan angle ~ for flying spot scanning. Alternatively, flying spot scanning could be provided by any other suitable device, such as mirrored piezo-electric crystals or planar reflecting mirrors which are driven ( in oscillatory fashion.
In all of these arrangements, however, the reflectingsurfaces would be at a distance Sl from the originating focal point of light beam 12 and in orthogonal relation to the plane bounded by the beam 6 such that the reflected beams would be in substantially the same plane as beam 6.
The focal plane 24 is proximate a recording medium 25 whose surface 26 is brought in contact with the respective focal spots of the convergent light beams throughout a scan width x.
- -A uniform spot size is assured throughout the scan width x even though a curved focal plane 24 is defined through-out the scanning cycle. The lens 10 in convolution with the imaging lens 18 provides a finite conjugate imaging system which allows a large depth of focus of which is coextensive with the contact loci of a spot throughout the scan width x on the surface 26 of the medium 25.
As shown in Figure 4, medium 25 may be a xerographic drum and in all respects is similar to the arrangement of Figure 2 except for the position of the imaging lens as shown in Figure 3.
The second alternative embodiment is as shown in Figure 5. At a distance a from the leading illuminated facet of polygon 16 is positioned an imaging lens 20. As shown, the lens 20 is located between the polygon 16 and the medium 25.
Alternatively, the lens 20 may be located between the polygon 16 and the lens 10 as shown in Figure 3. In this embodiment, lens 20 is of a diameter Dl to cooperate with the respective reflected light beams throughout each scan of 2 d~ to render convergent beams 22 which define a focal plane 24 at a distance f, from the imaging lens 20. In the first embodiment, imaging lens 20 is a five element compound lens as disclosed in United States Patent 3,741,621 to G.L. McCrobie issued June 26, 1973 and assigned to the assignee of the present invention. The focal plane 24 is proximate a recording medium 25 whose surface 26 is brought in contact with the respective focal spots of :~
the convergent light beams throughout a scan width x. .
Since runout errors and polygon facet errors may cause poor results in terms of the quality of image transfer to the scanned medium, a cylindrical lens 36 is positioned in the optical path between the polygon and the scanned medium with its ` 106693Z
aperture aligned with the aperture of the polygon 16. The lens 23 may be either bi-convex, plano-convex, or meniscus.
The light beam 22 impinges on the convex surface of the lens 36 to focus at plane 24 at a predetermined position in an ordinate perpendicular to the direction of scan on the surface 26 of the medium 25.
- As shown in Figure 6, the polygon 16 is continuously driven by a motor 40 and may be synchronized in rotation to a synchronization signal representative of the scan rate used to obtain the original video signal. In the case of the utilization of a xerographic drum, the rotation rate of the drum determines the spacing of the scan lines. The rotation of the polygon 16 off-axis from that desired causes runout errors or, in this case, a deflection of the beam 22 in the vertical direction away from the desired scan line. Assuming an angular deviation of ~ from the desired axis of rotation for the polygon 16, a runout angle of ~ defines the deflection from the intended direction of scan. Other misalignments of optical elements within the system, such as facet misalignment, also may cause the same runout effects.
The disposition of the cylindrical lens 36 in Figures 6(a), 6(b), the optical path, though, compensates for such effects. The lens 36 is located at a distance b from the origin of the angular deflection ~ and a distance u from the imaging lens 20. The compensation is effected in that the off-axis beam passes through the convex surfaces of lens 36. Then, the lens 36 focuses the beam 22 to a spot at a predetermined line -~
of scan in the focal plane 24 at a distance b' from the lens 36.
To insure that lens 36 is sufficiently wide a length L is pro-vided approximately equal to or greater than the scan width s. The runout dimensions at lenses 20 and 36 are Dl' and D2', 10~6932 respectively.
In this embodiment, in order to determine the optimum relationship between the imaging elements 20 and 36, the aperture Dl of the imaging lens 20 shall be equal to approximately 2ax/fl, with an (f/number)l equal to approximately s/2a tan2 ~
Furthermore, the focal length of lens 36 is f2, which is defined as l/b + l/b = l/f2. From this we may define the optimum focal length f2 for determining the distance of the focused spot from the lens 36.
Since it is also necessary to define the aperture D2 of the lens 36 to practice the invention, the following relationship is preferred:
D2 ~ 2b tan ~
Having defined f2 and D2, it is helpful to determine the necessary (f/number)2 for the lens 36:
(f/number)2 = f2/D2 = b'/2 tan ~ (b' + b) An optimum relationship is that the cylindrical lens 36 be located at a distance from the surface 26 of the medium 25 approximately equal to the focal length f2 of the lens 36.
A third alternative embodiment shown in Figure 7, wherein the same numerals correspond to the same or similar parts as in Figure 3.
The light beam 6 is reflected from mirror 8 in con-volution with a doublet lens 10. The lens 10 may be any lens, preferably of two elements, which elements are in spaced -~
relation to each other such that the external curved surfaces are provided in symmetry with the planar internal surfaces.
Preferably the internal surfaces of lens 10 are cemented together to form a common contact zone. Of course, as is often the case in the embodiment of such a lens as a microscope objective, the elements may be fluid spaced. The lens 10 is required to image either a virtual or real axial point of beam 6 through a focal point, for example, on the opposite side of lens 10 for a real image. At the focal point, beam 6 diverges or expands to form beam 12 which would be more than sufficient to impinge upon a given facet of a scanning polygon 16.
At a distance S2 from the leading illuminated facet of polygon 16 is positioned an imaging lens 18. Lens 18 is of a diameter D to cooperate with the expanded light beam 12 to render a convergent beam 20 which illuminates the desired facets to reflect respective light beams 22 through a positive cylindrical lens 23 to focus to the focal plane 24 at a distance S3 from the polygon 16. In this preferred embodiment, imaging lens 18 is a five element compound lens as disclosed in afore-mentioned U.S. Patent 3,741,521.
The rotational axis of polygon 16 is orthogonal to the plane in which light beam 6 travels. The facets of the polygon 16 are mirrored surfaces parallel to the axis of rotation for the reflection of any illuminating light imping-ing upon them. With the rotation of the polygon 16, assumingtwo contiguous facets are illuminated at a given time, a pair of light beams 22 are reflected from the respective illuminated facets and turned through an angle 2 dL for flying spot scanning~
Alternatively, flying spot scanning could be provided by any other suitable device, such as mirrored piezoelectric crystals of planar reflecting mirrors which are driven in an oscillatory fashion.
In all of these arrangements, however, the reflecting surfaces would be at a distance Sl from the originating focal point of light beam 12 and in orthogonal relation to the plane bounded by the beam 6 such that the reflected beams would be in ~ - 15 -substantially the same plane as beam 6.
The cylindrical lens 23 is positioned in the optical path between the polygon 16 and the desired line of scan in the focal plane 24 with its aperture aligned with the aperture of the polygon 16.
- The function of the lens 23 is to compensate for runout errors in the scanning system. The lens 23 may be either bi-convex, plano-convex or meniscus and further relates to the scanning system as described with respect to Figure 6.
The focal plane 24 is proximate a recording medium 25 whose surface 26 is brought in contact with the respective focal spots of the convergent light beams throughout a scan width x.
A substantially uniform spot size is assured through-out the scan width x even though a curved focal plane 24 is defined throughout the scanning cycle. The lens 10 in con-volution with the imaging lens 18 provides a finite conjugate imaging system which allows a large depth of focus d which is coextensive with the contact loci of a spot throughout the scan width x on the surface 26 of the medium 25.
- 15a -~ As is further shown in figure 7, a mirror 42 is positioned proximate the start of scan location to deflect at least a portion of the beam 22 to direct a beam 44 through a positive cylindrical lens 46 to focus at a detector 48. The detector 48 includes a photodiode (not shown), or other optically sensitive element, which produces an eled~rical pulse to indicate the start of scan upon illumination by the beam 44. The detector 48 further includes a timing element (not shown) in combination with the optically sensitive element which is responsive to the start of scan pulse. The timing element through well known techniques times out the predetermined duration of a scanning cycle to produce a stop of scan pulse. An example of such a technique would be a capacitive element charged at the start of scan pulse which charge decays in relation to a predetermined time constant to trigger a one-shot multivibrator at the stop of scan. The start/stop of scan signa~s are then used to slave the video signal to the scan rate of the scanning system.
The detection elements 46 and 48 are substantially matched with the convolution of imaging elements which focus ( the flying spot at the surface of the scanned medium. The cylindrical lens 46 i5 distanced along it9 respective optical path from the lens 18 precisely at the same length as the cylindrical lens 23 is distanced along its respective optical path from the lens 18. Furthermore, the aperture, focal lèngth, and focal number of the lens 46 is substantially identical to that required for lens 23. Therefore, the focused spot of the beam 44 is in a focal plane at a distance _ -~6 _ ...
- - .
~ ` 1066932 S3 along the optical path from the polygon 16, where the detector 48 is located. Thereby, an effective detection system is provided which contributes to a high degree of synchronization accuracy and constancy, with no interference with the spot scanning elements within the system.
_ 17 -
BACKGROUND OF THE IN~7ENTION
This invention relates to a flying spot scanning system for communicating video information to a scanned medium, and more particularly to a scanning system which utilizes a multifaceted rotating polygon for controlling the scanning cycles.
Much attention has been given to a various optical approaches in flying spot scanning for the purpose of imparting the information content of a modulated lig~t beam to a scanned medium. Galvanometer arrangements have been used to scan the light across a document for recording its information content thereon.
Such arrangements have included planar reflecting mirrors which are driven in an oscillatory fashion. Other approaches have made use of multifaceted mirrors which are driven continuously. Various efforts have been made to define the spot size in order to provide for an optimum utilization of the scanning system.
~ ne such effort is that described in United States Patent No. 3,675,016. The approach used was to make the spot size invariant and as small as possible by defining the dimensions of the focused beam so that only part, preferably half, of a mirror facet is illuminated during ~canning. This teaching alludes to generalized techniques for assuring the constancy of the size of the aperture of a rotating mirror scanning system. ~y either illuminating several facets of the mirror or by directing light in a beam that is sufficiently narrow to assure that less than a full facet is the most that can ever be illuminated by the beam and limiting scanning to that portion of the rotary travel of the facet when such facet i~ illuminated by all of such light beam. However, such system apertures are dimensionally invariant because the dimensions of the rotating facets have no influence on such apertures.
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. '~'' ~066932 While the system as described in U.S. Patent No.
3,675,016 may have advantages over the prior art, nevertheless, various constraints must be imposed upon the spot size and other relationships of optical elements within the system which are not always desirable.
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~ ' 1066932 SUMMARY OF THE INVENTION
In accordance with an aspect of this invention there is provided apparatus for recording information from an electrical signal onto a scanned medium comprising: means for providing a beam of high intensity light, means for modulating the light beam in accordance with the information content of an electrical signal, means for focusing said modulated beam to a spot upon the surface of a light sensitive medium at a predetermined distance from said focusing means, scanning means positioned in the optical path of said modulated beam for scanning the spot across said medium to impart the :
information content of said spot to said medium, a first cylindrical lens so positioned in the optical path of the focused beam between said scanning means and said medium that runout errors are substantially corrected at said medium, the plane of no power of said cylindrical lens being oriented in the direction of scan, means for deflecting a portion of the scanned spot to provide a second beam directed at a predetermined start of scan position located spatially from said medium, means for detecting the start of the scan located at said start of scan position at a distance from said focus-ing means approximately equal to said predetermined distance, and a second cylindrical lens so positioned in the path of said second beam between said detecting means and said deflecting means that runout errors are substantially corrected at said detecting means, the plane of no power of said second cylindrical lens being oriented in the direction of scan.
In accordance with another aspect of this invention there is provided apparatus for recording information from an electrical signal onto a scanned medium comprising: means for providing a beam of high intensity light, means for modulating the light beam in accordance with the information content of an electrical signal, first optical means for ~ _ 4 _ - ~066932 expanding said modulated beam, second optical means in convolu-tion with said first optical means for imaging said expanded beam to a spot in a focal plane at a predetermined distance from said second optical means, scanning means positioned between said second means and the focal plane for scanning the spot across a light sensitive medium in said focal plane to impart the information content of said spot to said medium, means for detecting the start of the scan located spatially from said medium at said predetermined distance from said ;~
second optical means, means for deflecting a portion of the scanned spot at a predetermined start of scan position to form a second beam directed away from said medium to illuminate said detecting means, a first cylindrical lens so positioned in the optical path of the imaged beam between said second optical means and said medium that runout errors are substan-tially corrected at said medium, the plane of no power of said cylindrical lens being oriented in the direction of scan, and a second cylindrical lens so positioned in the second beam path between said deflecting means and said detecting means that runout errors are substantially corrected at said detect-ing means, the plane of no power of said second cylindrical lens being oriented in the direction of scan.
A feature of an embodiment of the invention is that the beam of light incident upon the multifaceted polygon illuminates at least two contiguous facets of the polygon during each scanning cycle to provide the desired sequence of spot scanning. Such feature provides a flying spot scan-ning system which has an extremely high duty cycle.
Another feature of an embodiment of the invention is that a very large depth of focus is provided for the spot at the contact loci at the surface of the scanned medium.
This feature is provided by utilizing a finite conjugate ~ - 4a -- ~66932 imaging system in convolution with the light beam and the rotating polygon. A doublet lens, in series with a convex imaging lens between the light source and the medium provides such an arrangement. The doublet lens enables the original light beam to be sufficiently expanded for illuminating multiple contiguous facets of the polygon, - 4b --` 106693Z
whereas the imaging lens converges the expanded beam to focus at the contact loci on the surface of the scanned . . .
medium. Employing such an optical system assures a uniform spot size at the scanned medium even though a substantial scan width is traversed by the spot.
Still another feature of an embodiment of the invention is the modulation of the original light beam by means of a video signal. The information content within the video signal is thereby imparted to the light beam itself. The medium to be scanned is one which is responsive to the modulated beam and records its information content as contained within the scanning spot in a usable form on its ! surface across the scan width.
Also, another feature of an embodiment of the invention is that a start/stop of scan detection apparatus is in combination with and substantially matches the con-volution of imaging elements which focus the flying spot at the surface of the scanned medium, although such detection apparatus is spacially distant from the scanned medium.
Yet another feature of an embodiment of the invention includes an embodiment of the flying spot scanning system for utilization in high speed xerography. The scanned medium in such an embodiment would consist of a xerographic drum which rotates consecutively through a charging station, an exposure station where the spot traverses che scan width of the drum, through a developing station, and a transfer station where a web of copy paper is passed in contact with the drum and receives an electrostatic discharge to induce the transfer of the developed image from the drum to the 30 copy paper. A fusing device then fixes the images to the copy paper as it passes to an output station.
_ 5 _ .~ - : , . , : ~ ~ . - ,:
DESCRIPTION OF THE DRAWINGS
Figure 1 is an isometric illustration of a flying spot scanning system in accordance with the invention.
Figure 2(a) is a partial perspective view illus-trating the-use of the scanning beam generated by the system of Figure 1.
Figure 2(b) is a top perspective view of the optical system shown in Figure 2(a). ~ -Figure 3 is an isometric illustration of a first alternate to the flying spot scanner of Figure 1 and with the same numbers indicating the same or similarly operating parts.
Figure 4 is a perspective view of the utiliza-tion of the scanning beam according to the first alternate embodiment.
Figure 5 is an isometric illustration of a second alternative to the flying spot scanning system of Fisure 1 and wherein the same number indicates same or similar parts.
- 5a -., ~
~06693Z
. .
Figure 6(a) is a side perspective view of the utilization of the cylindrical correction lens of Figure 6.
Figure 6(b) is a top perspective view of the utilization of the cylindrical lens.
Figure 7 is an isometric illustration third alternative to that of Figure 1 of a flying spot scanning system with the same numerals indicating the same or similar parts.
DESCRIPTION OF THR PREFERRED EMBODIMENT
In Figure 1, an embodiment of a flying spot scanning system in accordance with the invention is shown. A light ; source 1 provides the original light beam for utilization by the scanning s~stem. The light source 1 is preferably a laser which generates a collimated beam of monochromatic light which may easily be modulated by modulator 4 in conformance with the information contained in a video signal.
Modulator 4 may be any suitable electro-optical modulator for recording the video information in the form of a modulated light beam 6 at the output of the modulator 4.
The modulator 4 may be, for example, a Pockel's cell comprising a potassium dihydrogen phosphate crystal, whose index of re-fraction is periodically varied by the application of the vary-ing voltage which represents the video signal. The video signal may contain information either by means of binary pulse code modulation or wide-band frequency code modulation. In any event, by means of the modulator 4 the information within the video signal is represented by the modulated light beam 6.
The light beam 6 is reflected from mirror 8 in convolution with a doublet lens 10. The lens 10 may be any lens, preferably of two elements, which elements are in spaced relation to each other such that the external curved suxfaces are provided in symmetry with the internal surfaces. Preferably the internal surfaces of lens 10 are cemented together to form a common contact zone. Of course, as is often the case in the embodiment of such a lens as a microscope objective, the elements may be fluid spaced.
The lens 10 is required to image the axial point of beam 6 through a focal point on the opposite side of lens 10.
At the focal point, beam 6 diverges or expands to form beam 12 which impinges upon at least two contiguous facets of a scanning polygon 16.
In this embodiment, the rotational axis of polygon 16 is orthogonal to the plane in which light beams 6 travels.
The facets of the polygon 16 are mirrored surfaces for the reflection of any illuminating light impinging upon them.
With the rotation of the polygon 16, a pair of light beams are reflected from the respective illuminated facets and turned through a scan angle for flying spot scanning.
Alternatively, flying spot scanning could be provided by any other suitable device, such as mirrored piezoelectric crystals or planar reflecting mirrors which are driven in an oscillatory fashion.
In all of these arrangements, however, the reflecting surfaces would be at a distance S from the originating focal point of light beam 12 and in orthogonal relation to the plane bounded by the beam 6 such that the reflected beams would be in substantially the same plane as beam 6.
At a distance a from the leading illuminated facet :
of polygon 16 is positioned an imaging lens 20. Lens 20 is -of a diameter D to cooperate with the respective reflected light beams throughout an angle of 2 ~ to render convergent beams 22 which define a focal plane 24 at a distance f from the imag- :
ing lens 20. In this preferred embodiment, imaging lens 20 is ; a five element compound lens as disclosed in United States Patent 3,741,521 issued January 10, 1973 and assigned to the assignee of the present invention. The focal plane 24 is proximate a recording medium 25 whose surface 26 is brought in contact with the respective focal spots of the convergent light beams throughout a scan width x.
A uniform spot size is assured throughout the scan width x even though a curved focal plane 24 is defined through-out the scanning cycle. The lens 10 in convolution with the imaging lens 20 provides a finite conjugate imaging system which allows a large depth of focus d which is coextensive with the contact loci of a spot throughout the scan width x on the :
surface 26 of the medium 25.
The beam of light from the light source 1, through the optical elements and reflected from the scanning polygon to the scanning medium 25 defines a light path.
As shown in figure 2(a), medium 25 may be a xero-graphic drum which rotates consecutively through a charging station depicted by corona discharge device 27, exposure surface 26 where the beam from the rotating polygon 16 traverses the scan width x on the drum 25, through developing station 28 depicted by a cascade development enclosure, transfer station 30 where a web of copy paper is passed in contact with the drum 25 and receives an electrostatic discharge to induce a transfer of the developed image from the drum 25 to the copy paper.
The copy paper is supplied from the supply reel 31, passes around guide rollers 32 and through drive rollers 33 into rec~iving bin 35. A fusing device 34 fixes the images to ~e copy paper as it passes to bin 35.
Usable images are provided in that the information c~ntent of the scanning spot is represented by the modulated or variant intensity of light respective to its postion within the scan width x. As the spot traverses the charged surface 26 th~ough a given scan angle c7~, the spot dissipates t~e electrostatic charge in accordance with its light intensity. The electrostatic charge pattern thus produced i~ developed in the developing station 28 and then transferred to the final copy paper. The xerographic drum 25 is cleaned by some cleaning device such as a rotating brush 36 bef~re being recharged by charging device 27. In this manner, the information content of the scanned spot i8 recorded on a more permanent and useful medium. Of course, alternative prior art techniques may be employed to cooperate with a scanned spot in order to utilize the information contained therein.
m e polygon 16 is continuously driven by a motor 40 and synchronized in rotation to a synchronization signal representative of the scan rate used to obtain the original video signal. The rotation rate of the xerographic drum 25 determines the spacing of the scan lines. It also may be peferable to synchronize the drum 25 in some manner to the signal source to maintain image linearity. The source image is reproduced in accordance with the signal and is transferred to prlntout paper for use or storage.
4~ _ 9_ ` ~066932 The number of facets has been found to be optimum if at least 20 to 30 facets are employed. The scan angle o~
traversed would be equal to the number of facets chosen in relation to one complete revolution of the polygon 16. An extremely useful arrangement would have the polygon 16 with 24 facets and a scan anglec~ of 15 degrees. Since the depth of focus d of the converging beam 22 is related to the scan angle in that as the scan angle c~ increases the radius of curvature of the focal plane 24 increases, it is important to define a scan angle in relation to the desired scan width x. For a scan width x of approximately ll inches it has been found that the scan angle o~ of 12 to 18 degrees, with 20 to 30 facets on the polygon 16, is optimum. Figure 2(b) is a top perspective view of the optical system shown in Figure 2(a).
The optical system of the present invention provides a virtually lO0~ duty cycle scan for the entire scan angle c~ by virtue of the illumination of at least two contiguous facets. The illumination of two contiguous facets is preferred. ~With such illumination, another scanning spot is provided at a distance equal to the scan width x behind the leading scanning spot with virtually no wait between successive scans. With the continuous rotation of the polygon 16 additional contiguous facets are subsequently illuminated, thereby providing successive convergent beams following the leading convergent beam 22 by no more than the scan angle, if so desired. Thus, a flying spot scanning system which has an extremely high duty cycle is provided.
The optical system of the present invention projects the highest energv portion of the laser beam onto the rotating - 9a -1()66932 polygon and to the photoreceptor surface. The energy output of the laser beam has a Gaussian distribution with the highest intensity distribution being concentrated near the axis of projection. In the Gaussian distribution the highest inten-sity energy is located at the centre of the beam. By spreading the beam out over a plurality of facets, the beam centre portion having the highest intensity radiation energy fills all the polygon facets reflecting the beam onto the photoconductive surface. The fringes of the beam having the lowest Gaussian energy intensities are spread out beyond those polygon facets and are excluded from the information signal scanned across the photoreceptor surface. Shaping the beam to spread it across a plurality of facets thereby filters the lower energy radiation within the beam and excludes it, permitting the utilization of the maximum energy content of the beam.
In the first alternate embodiment as shown in Figure 3, the light beam 6 is reflected from mirror 8 in convolution with a doublet lens 10. The lens 10 may be any lens, preferably of two elements, which elements are in spaced relation to each other such that external curved surfaces are provided in symmetry with the internal surfaces.
Preferably the internal surfaces of lens 10 are cemented together to form a common contact plane. Of course, as is often the case in the embodiment of such a lens as a micro-scope objective, the elements may be fluid spaced. The lens 10 is required to image either a virtual or real axial point of beam 6 through a focal point, for example, on the opposite side of lens 10 for a real image. At the focal point, beam 6 diverges or expands to form beam 12 which would be more than sufficient to impinge upon a given facet of a scanning polygon 16.
At a distance S2 from the leading illuminated facet of polygon 16 is positioned an imaging lens 18. Lens 18 is ~
of a diameter D to cooperate with the expanded light beam 12 ;
to render a convergent beam 2 which illuminates the desired facets to reflect respective light beams 22 to focus to focal plane 24 at a distance d from the polygon 16. In this first alternate embodiment, imaging lens 18 is a l-n element lens.
The focal length f of lens 18 is related to Sl, S2 and d by the following thin lens equation: 1 +
Sl S2 +d f The rotational axis of polygon 16 is orthogonal to the plane in which light beam 6 travels. The facets of the polygon 16 are mirrored surfaces for the reflection of any illuminating light impinging upon them. With the rotation of the polygon 16, assuming two contiguous facets are illuminated at a given time, a pair of light beams 22 are reflected from the respective illuminated facets and turned through a scan angle ~ for flying spot scanning. Alternatively, flying spot scanning could be provided by any other suitable device, such as mirrored piezo-electric crystals or planar reflecting mirrors which are driven ( in oscillatory fashion.
In all of these arrangements, however, the reflectingsurfaces would be at a distance Sl from the originating focal point of light beam 12 and in orthogonal relation to the plane bounded by the beam 6 such that the reflected beams would be in substantially the same plane as beam 6.
The focal plane 24 is proximate a recording medium 25 whose surface 26 is brought in contact with the respective focal spots of the convergent light beams throughout a scan width x.
- -A uniform spot size is assured throughout the scan width x even though a curved focal plane 24 is defined through-out the scanning cycle. The lens 10 in convolution with the imaging lens 18 provides a finite conjugate imaging system which allows a large depth of focus of which is coextensive with the contact loci of a spot throughout the scan width x on the surface 26 of the medium 25.
As shown in Figure 4, medium 25 may be a xerographic drum and in all respects is similar to the arrangement of Figure 2 except for the position of the imaging lens as shown in Figure 3.
The second alternative embodiment is as shown in Figure 5. At a distance a from the leading illuminated facet of polygon 16 is positioned an imaging lens 20. As shown, the lens 20 is located between the polygon 16 and the medium 25.
Alternatively, the lens 20 may be located between the polygon 16 and the lens 10 as shown in Figure 3. In this embodiment, lens 20 is of a diameter Dl to cooperate with the respective reflected light beams throughout each scan of 2 d~ to render convergent beams 22 which define a focal plane 24 at a distance f, from the imaging lens 20. In the first embodiment, imaging lens 20 is a five element compound lens as disclosed in United States Patent 3,741,621 to G.L. McCrobie issued June 26, 1973 and assigned to the assignee of the present invention. The focal plane 24 is proximate a recording medium 25 whose surface 26 is brought in contact with the respective focal spots of :~
the convergent light beams throughout a scan width x. .
Since runout errors and polygon facet errors may cause poor results in terms of the quality of image transfer to the scanned medium, a cylindrical lens 36 is positioned in the optical path between the polygon and the scanned medium with its ` 106693Z
aperture aligned with the aperture of the polygon 16. The lens 23 may be either bi-convex, plano-convex, or meniscus.
The light beam 22 impinges on the convex surface of the lens 36 to focus at plane 24 at a predetermined position in an ordinate perpendicular to the direction of scan on the surface 26 of the medium 25.
- As shown in Figure 6, the polygon 16 is continuously driven by a motor 40 and may be synchronized in rotation to a synchronization signal representative of the scan rate used to obtain the original video signal. In the case of the utilization of a xerographic drum, the rotation rate of the drum determines the spacing of the scan lines. The rotation of the polygon 16 off-axis from that desired causes runout errors or, in this case, a deflection of the beam 22 in the vertical direction away from the desired scan line. Assuming an angular deviation of ~ from the desired axis of rotation for the polygon 16, a runout angle of ~ defines the deflection from the intended direction of scan. Other misalignments of optical elements within the system, such as facet misalignment, also may cause the same runout effects.
The disposition of the cylindrical lens 36 in Figures 6(a), 6(b), the optical path, though, compensates for such effects. The lens 36 is located at a distance b from the origin of the angular deflection ~ and a distance u from the imaging lens 20. The compensation is effected in that the off-axis beam passes through the convex surfaces of lens 36. Then, the lens 36 focuses the beam 22 to a spot at a predetermined line -~
of scan in the focal plane 24 at a distance b' from the lens 36.
To insure that lens 36 is sufficiently wide a length L is pro-vided approximately equal to or greater than the scan width s. The runout dimensions at lenses 20 and 36 are Dl' and D2', 10~6932 respectively.
In this embodiment, in order to determine the optimum relationship between the imaging elements 20 and 36, the aperture Dl of the imaging lens 20 shall be equal to approximately 2ax/fl, with an (f/number)l equal to approximately s/2a tan2 ~
Furthermore, the focal length of lens 36 is f2, which is defined as l/b + l/b = l/f2. From this we may define the optimum focal length f2 for determining the distance of the focused spot from the lens 36.
Since it is also necessary to define the aperture D2 of the lens 36 to practice the invention, the following relationship is preferred:
D2 ~ 2b tan ~
Having defined f2 and D2, it is helpful to determine the necessary (f/number)2 for the lens 36:
(f/number)2 = f2/D2 = b'/2 tan ~ (b' + b) An optimum relationship is that the cylindrical lens 36 be located at a distance from the surface 26 of the medium 25 approximately equal to the focal length f2 of the lens 36.
A third alternative embodiment shown in Figure 7, wherein the same numerals correspond to the same or similar parts as in Figure 3.
The light beam 6 is reflected from mirror 8 in con-volution with a doublet lens 10. The lens 10 may be any lens, preferably of two elements, which elements are in spaced -~
relation to each other such that the external curved surfaces are provided in symmetry with the planar internal surfaces.
Preferably the internal surfaces of lens 10 are cemented together to form a common contact zone. Of course, as is often the case in the embodiment of such a lens as a microscope objective, the elements may be fluid spaced. The lens 10 is required to image either a virtual or real axial point of beam 6 through a focal point, for example, on the opposite side of lens 10 for a real image. At the focal point, beam 6 diverges or expands to form beam 12 which would be more than sufficient to impinge upon a given facet of a scanning polygon 16.
At a distance S2 from the leading illuminated facet of polygon 16 is positioned an imaging lens 18. Lens 18 is of a diameter D to cooperate with the expanded light beam 12 to render a convergent beam 20 which illuminates the desired facets to reflect respective light beams 22 through a positive cylindrical lens 23 to focus to the focal plane 24 at a distance S3 from the polygon 16. In this preferred embodiment, imaging lens 18 is a five element compound lens as disclosed in afore-mentioned U.S. Patent 3,741,521.
The rotational axis of polygon 16 is orthogonal to the plane in which light beam 6 travels. The facets of the polygon 16 are mirrored surfaces parallel to the axis of rotation for the reflection of any illuminating light imping-ing upon them. With the rotation of the polygon 16, assumingtwo contiguous facets are illuminated at a given time, a pair of light beams 22 are reflected from the respective illuminated facets and turned through an angle 2 dL for flying spot scanning~
Alternatively, flying spot scanning could be provided by any other suitable device, such as mirrored piezoelectric crystals of planar reflecting mirrors which are driven in an oscillatory fashion.
In all of these arrangements, however, the reflecting surfaces would be at a distance Sl from the originating focal point of light beam 12 and in orthogonal relation to the plane bounded by the beam 6 such that the reflected beams would be in ~ - 15 -substantially the same plane as beam 6.
The cylindrical lens 23 is positioned in the optical path between the polygon 16 and the desired line of scan in the focal plane 24 with its aperture aligned with the aperture of the polygon 16.
- The function of the lens 23 is to compensate for runout errors in the scanning system. The lens 23 may be either bi-convex, plano-convex or meniscus and further relates to the scanning system as described with respect to Figure 6.
The focal plane 24 is proximate a recording medium 25 whose surface 26 is brought in contact with the respective focal spots of the convergent light beams throughout a scan width x.
A substantially uniform spot size is assured through-out the scan width x even though a curved focal plane 24 is defined throughout the scanning cycle. The lens 10 in con-volution with the imaging lens 18 provides a finite conjugate imaging system which allows a large depth of focus d which is coextensive with the contact loci of a spot throughout the scan width x on the surface 26 of the medium 25.
- 15a -~ As is further shown in figure 7, a mirror 42 is positioned proximate the start of scan location to deflect at least a portion of the beam 22 to direct a beam 44 through a positive cylindrical lens 46 to focus at a detector 48. The detector 48 includes a photodiode (not shown), or other optically sensitive element, which produces an eled~rical pulse to indicate the start of scan upon illumination by the beam 44. The detector 48 further includes a timing element (not shown) in combination with the optically sensitive element which is responsive to the start of scan pulse. The timing element through well known techniques times out the predetermined duration of a scanning cycle to produce a stop of scan pulse. An example of such a technique would be a capacitive element charged at the start of scan pulse which charge decays in relation to a predetermined time constant to trigger a one-shot multivibrator at the stop of scan. The start/stop of scan signa~s are then used to slave the video signal to the scan rate of the scanning system.
The detection elements 46 and 48 are substantially matched with the convolution of imaging elements which focus ( the flying spot at the surface of the scanned medium. The cylindrical lens 46 i5 distanced along it9 respective optical path from the lens 18 precisely at the same length as the cylindrical lens 23 is distanced along its respective optical path from the lens 18. Furthermore, the aperture, focal lèngth, and focal number of the lens 46 is substantially identical to that required for lens 23. Therefore, the focused spot of the beam 44 is in a focal plane at a distance _ -~6 _ ...
- - .
~ ` 1066932 S3 along the optical path from the polygon 16, where the detector 48 is located. Thereby, an effective detection system is provided which contributes to a high degree of synchronization accuracy and constancy, with no interference with the spot scanning elements within the system.
_ 17 -
Claims (10)
PROPERTY OR PRIVILEGE IS CLAIMED ARE DEFINED AS FOLLOWS:
1. Apparatus for recording information from an electrical signal onto a scanned medium comprising: means for providing a beam of high intensity light, means for modulating the light beam in accordance with the information content of an electrical signal, means for focusing said modulated beam to a spot upon the surface of a light sensitive medium at a predetermined distance from said focusing means, scanning means positioned in the optical path of said modulated beam for scanning the spot across said medium to impart the information content of said spot to said medium, a first cylindrical lens so position-ed in the optical path of the focused beam between said scan-ning means and said medium that runout errors are substantially corrected at said medium, the plane of no power of said cylindrical lens being oriented in the direction of scan, means for deflecting a portion of the scanned spot to provide a second beam directed at a predetermined start of scan position located spatially from said medium, means for detecting the start of the scan located at said start of scan position at a distance from said focusing means approximately equal to said predetermined distance, and a second cylindrical lens so positioned in the path of said second beam between said detect-ing means and said deflecting means that runout errors are substantially corrected at said detecting means, the plane of no power of said second cylindrical lens being oriented in the direction of scan.
2. The apparatus as claimed in claim 1, wherein said second cylindrical lens is positioned from said detecting means at substantially the same distance said first cylindrical lens is positioned from said medium.
3. The apparatus as claimed in claim 2, wherein said second cylindrical lens is optically matched with said first cylindrical lens.
4. The apparatus as defined in claim 3, wherein said second cylindrical lens has substantially the same focal length and aperture as does said first cylindrical lens.
5. Apparatus for recording information from an electrical signal onto a scanned medium comprising: means for providing a beam of high intensity light, means for modulating the light beam in accordance with the information content of an electrical signal, first optical means for expanding said modulated beam, second optical means in convolution with said first optical means for imaging said expanded beam to a spot in a focal plane at a predetermined distance from said second optical means, scanning means positioned between said second means and the focal plane for scanning the spot across a light sensitive medium in said focal plane to impart the information content of said spot to said medium, means for detecting the start of the scan located spatially from said medium at said predetermined distance from said second optical means, means for deflecting a portion of the scanned spot at a predetermined start of scan position to form a second beam directed away from said medium to illuminate said detecting means, a first cylindrical lens so positioned in the optical path of the imaged beam between said second optical means and said medium that runout errors are substantially corrected at said medium, the plane of no power of said cylindrical lens being oriented in the direction of scan, and a second cylindrical lens so positioned in the second beam path between said deflecting means and said detecting means that runout errors are substantially corrected at said detecting means, the plane of no power of said second cylindrical lens being oriented in the direction of scan.
6. The apparatus as claimed in claim 5, wherein said second cylindrical lens is positioned from said detecting means at substantially the same distance said first cylindrical lens is positioned from said medium.
7. The apparatus as defined in claim 6, wherein said second cylindrical lens is optically matched with said first cylindrical lens.
8. The apparatus as defined in claim 7, wherein said second cylindrical lens has substantially the same focal length and aperture as does said first cylindrical lens.
9. The system as defined in claim 8, wherein the scanning means includes a multifaceted polygon having reflective sides for reflecting the light converging from said second optical means onto said medium and means for rotating said polygon such that the reflected light is scanned in successive traces across said medium.
10. The system as defined in claim 9, wherein said light source is a laser which emits a beam of collimated light of substantially uniform intensity.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CA306,001A CA1066932A (en) | 1972-11-27 | 1978-06-22 | Flying spot scanner |
Applications Claiming Priority (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US30987372A | 1972-11-27 | 1972-11-27 | |
| US30987472A | 1972-11-27 | 1972-11-27 | |
| US30985972A | 1972-11-27 | 1972-11-27 | |
| CA185,340A CA1041209A (en) | 1972-11-27 | 1973-11-08 | Flying spot scanner |
| CA306,001A CA1066932A (en) | 1972-11-27 | 1978-06-22 | Flying spot scanner |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA1066932A true CA1066932A (en) | 1979-11-27 |
Family
ID=27508020
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA306,001A Expired CA1066932A (en) | 1972-11-27 | 1978-06-22 | Flying spot scanner |
Country Status (1)
| Country | Link |
|---|---|
| CA (1) | CA1066932A (en) |
-
1978
- 1978-06-22 CA CA306,001A patent/CA1066932A/en not_active Expired
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