CN201293872Y - Two-slice type fTheta lens for micro-electromechanical laser scanning apparatus - Google Patents

Abstract

The utility model relates to a dual type f theta lens of a micro-electromechanical laser scanning device. A first lens is a crescentiform lens with positive dioptre and the second lens is also a crescentiform lens with positive dioptre, wherein the convex surface of the first lens and the convex surface of the second lens are arranged on a micro electromechanical reflecting mirror side. The first lens is provided with two optical surfaces, at least one optical surface is formed by a non-spherical surface in a main scanning direction, the second lens is provided with two optical surfaces, and at least one optical surface is formed by a non-spherical surface in the main scanning direction. The dual type f theta lens is mainly characterized by transforming a scanning light spot with reflected angle and reflected time of a micro-electromechanical laser reflecting mirror in nonlinear relation into a scanning light spot with distance and time in linear relation and correcting condensed light on an object. In addition, both the first lens and the second lens meet specific optical conditions, and through disposing the first lens and the second lens, the purpose of linear scanning effect and high-resolution scanning can be achieved.

Description

The two-chip type f theta lens of MEMS laser scanning device

Technical field

The utility model relates to a kind of two-chip type f theta lens of MEMS laser scanning device, relate in particular to and a kind ofly be the mems mirror of simple harmonic characteristic motion and produce the angle variable quantity that becomes sine relation in time, to realize the two-chip type f theta lens of the desired linear sweep effect of laser scanning device in order to correction.

Background technology

The used laser scanning device (LSU:Laser Scanning Unit) of laser beam printer (LBP:Laser Beam Print) utilizes the polygonal mirror (polygon mirror) of high speed rotating at present, with the scanning motion (laser beam scanning) that is used to control laser beam, as U.S. Pat 7079171, US6377293, US6295116, or as described in the patent I198966 of Taiwan.Its principle is as follows: utilize semiconductor laser give off laser beam (laser beam), earlier via collimating mirror (collimator), form parallel beam again via aperture (aperture), and after parallel beam passes through cylindrical mirror (cylindrical lens) again, can can be along the parallel focusing of parallel direction of the X-axis of main scanning direction (main scanning direction) and form wire imaging (line image) at the width on the Y-axis of sub scanning direction (sub scanning direction), be projected to again on the polygonal mirror of high speed rotating, and evenly being provided with polygonal mirror on the polygonal mirror continuously, it just in time is positioned at or approaches the focal position of above-mentioned wire imaging (line image).Projecting direction by polygonal mirror control laser beam, when continuous a plurality of catoptron high speed rotating, can be incident upon on the catoptron laser beam along the parallel direction of main scanning direction (X-axis) with identical tarnsition velocity (angular velocity) deflective reflector to f θ linear sweep eyeglass, and f θ linear sweep eyeglass is arranged at the polygonal mirror side, can be single-piece lens structure (single-element scanning lens) or is two formula lens structures.The function of this f θ linear sweep eyeglass is to make the laser beam of injecting the f Theta lens via the mirror reflects on the polygonal mirror can be focused into the ellipse luminous point and be incident upon light receiving surface (photoreceptor drum, be imaging surface) on, and the requirement of realization linear sweep (scanning linearity).Yet existing laser scanning device (LSU) has following point in the use:

(1) the manufacture difficulty height of rotary multi mirror and price are not low, increase the cost of manufacture of LSU relatively.

(2) polygonal mirror must possess the function of high speed rotating (as 40000 rev/mins), and precision requirement height, the minute surface Y-axis width that causes reflecting surface on the general polygonal mirror as thin as a wafer, thereby all need set up cylindrical mirror (cylindrical lens) in (LSU) of prior art, so that laser beam can be focused into line (on the Y-axis become a bit) through cylindrical mirror and be projeced on the catoptron of polygonal mirror again, thereby cause the increase of assembly cost and the increase of assembling operation.

(3) because existing polygonal mirror must high speed rotating (as 40000 rev/mins), cause Rotation Noise to improve relatively, and polygonal mirror must expend the long period from starting to working speed, increase the stand-by period after the start.

(4) in the package assembly of existing LSU, the laser beam central shaft that is projected to the polygonal mirror catoptron is not over against the central rotating shaft of polygonal mirror, so that when the f Theta lens that design matches, need consider simultaneously polygonal mirror from axle deviation (off axis deviation) problem, increase the design of f Theta lens relatively and make to go up difficulty.

In recent years since,, developed the mems mirror (MEMS mirror) of a kind of swing type (oscillatory) at present on the market, control laser beam flying in order to replace existing polygonal mirror in order to improve the problem of existing LSU package assembly.Mems mirror is torque oscillation device (torsionoscillators), has reflector layer on its top layer, can be by vibration swing reflector layer, the light reflection is scanned, can be applicable to the laser scanning device (LSU:laser scanning unit) of imaging system (imaging system), scanner (scanner) or laser printer (laser printer) future, its scan efficiency (Scanning efficiency) can be higher than traditional polygonal rotating mirror.As U.S. Pat 6,844,951, US6,956,597, produce at least one drive signal, the resonant frequency of the approaching a plurality of mems mirrors of its driving frequency, and with the drive mems mirror, to produce scanning pattern, similarly also have U.S. Pat 7,064,876, US7,184,187, US7,190,499, US2006/0113393; Or as Taiwan patent TW M253133, it utilizes mems mirror to replace existing rotary multi mirror and is arranged between the collimating mirror and f Theta lens in the LSU modular structure, controls the projecting direction of laser beam thus; Or as Jap.P. JP 2006-201350 etc.Described mems mirror has that assembly is little, and velocity of rotation is fast, advantage of low manufacturing cost.Yet because mems mirror is after receiving driven, to do simple harmonic motion, and the mode of this simple harmonic motion (harmonic motion) is that time and angular velocity are sine relation, the light that therefore is projeced into mems mirror after the mems mirror reflection reflection angle θ and the pass of time t be:

θ(t)＝θ _s·sin(2π·f·t) (1)

Wherein: f is the sweep frequency of mems mirror; θ _sFor laser beam behind mems mirror, the scanning angle of monolateral maximum.

Therefore, Δ t under the identical time interval, pairing reflection angle become sine function (Sinusoidal) to change with the time, and promptly at identical time interval Δ t, reflection angle is changed to: Δ θ (t)=θ _s(sin (2 π ft ₁)-sin (2 π ft ₂)), thereby be nonlinear relationship with the time, promptly when the light of this reflection is incident upon object with different angles, the spot distance that is produced in the identical time interval is at interval and inequality and increasing or decreasing in time.

For example, when the pendulum angle of mems mirror is positioned at sinusoidal wave crest and trough, angle variable quantity is increasing or decreasing in time, the mode of motion that forms the constant angular velocity rotation with existing polygonal mirror is different, if existing f Theta lens is applied to have on the laser scanning device (LSU) of mems mirror, can't revise the angle variable quantity that mems mirror produces, cause the laser light velocity that is incident upon on the imaging surface will produce speed scanning phenomenons such as non-, cause producing the imaging deviation that is positioned on the imaging surface.Therefore, for laser scanning device by mems mirror constituted, abbreviate MEMS laser scanning device (MEMS LSU) as, its characteristic is after laser beam scans via mems mirror, form the not equal angular scanning ray of constant duration, therefore press for the f Theta lens that development can be used in MEMS laser scanning device, with the correction scanning ray, thus can correct imaging on object.

The utility model content

In order to address the above problem, the purpose of this utility model is to provide a kind of two-chip type f theta lens of MEMS laser scanning device, this two-chip type f theta lens comprise the crescent and convex surface of the positive diopter that sets gradually from mems mirror first eyeglass of mems mirror side and positive diopter is crescent and convex surface at second eyeglass of mems mirror side, scanning ray correct imaging on object that mems mirror is reflected, thus realize the desired linear sweep effect of laser scanning device.

Another purpose of the present utility model is to provide a kind of two-chip type f theta lens of MEMS laser scanning device, in order to dwindling the area that is incident upon luminous point on the object (spot), thereby realizes improving the effect of resolution.

Another purpose of the present utility model is to provide a kind of two-chip type f theta lens of MEMS laser scanning device, the modifying factor that can distort scanning ray departs from optical axis, and cause skew to increase at main scanning direction and sub scanning direction, make the problem of the luminous point distortion ovalize that is imaged on photosensitive drums, and make each imaging luminous point size be able to homogenising, thereby realize promoting the effect of separating picture element amount (resolution quality).

Therefore, the two-chip type f theta lens of the MEMS laser scanning device that the utility model provides, be applicable to that the light source that comprises at least emission of lasering beam swings with resonance, make the laser beam of light emitted reflect the mems mirror that becomes scanning ray thus, with imaging on object; For laser printer, described object is photosensitive drums (drum) normally, the luminous point of promptly treating imaging gives off laser beam via light source, via scanning about mems mirror, the mems mirror reflection lasering beam forms scanning ray, scanning ray via two-chip type f theta lens angle correction of the present utility model and position after, on photosensitive drums, form luminous point (spot), because photosensitive drums scribbles photosensitizer, can respond to carbon dust it is gathered on the paper, so printablely go out data.

Two-chip type f theta lens of the present utility model comprises first eyeglass and second eyeglass that sets gradually from mems mirror, wherein first eyeglass has first optical surface and second optical surface, first optical surface and second optical surface, have at least an optical surface to be constituted at main scanning direction by aspheric surface, the speed scanning phenomenon such as non-that the luminous point spacing of mems mirror on imaging surface that mainly will be simple harmonic motion successively decreased by increasing in time originally or increased progressively, speed scanning such as be modified to, thereby make speed such as the projection work scanning of laser beam at imaging surface.Second eyeglass has the 3rd optical surface and the 4th optical surface, the 3rd optical surface and the 4th optical surface have at least an optical surface to be made of aspheric surface at main scanning direction, it is poor mainly on photosensitive drums to be formed into kine bias at main scanning direction and sub scanning direction because of the skew optical axis causes in order to the homogenising scanning ray, and the scanning ray correction of first eyeglass is concentrated on the object.

The utlity model has following effect:

Setting according to two-chip type f theta lens of the present utility model, the speed scanning phenomenon such as non-that the mems mirror that is simple harmonic motion can be successively decreased by increasing in time originally or increases progressively at imaging surface glazing dot spacing, speed scanning such as be modified to, make laser beam in the scanning of the speed such as projection work of imaging surface, make to image in the two adjacent luminous point spacings that form on the object and equate.

(1) according to the setting of two-chip type f theta lens of the present utility model, can distort and revise main scanning direction and sub scanning direction scanning ray, the luminous point on the object that focuses on imaging is dwindled.

(2) according to the setting of two-chip type f theta lens of the present utility model, can distort and revise main scanning direction and sub scanning direction scanning ray, make the luminous point size homogenising that is imaged on the object.

Description of drawings

The synoptic diagram of the optical path of the two-chip type f theta lens that Fig. 1 provides for the utility model;

Fig. 2 is the graph of a relation of mems mirror scanning angle θ and time t;

Fig. 3 is optical path figure and the symbol description figure by the scanning ray of first eyeglass and second eyeglass;

Fig. 4 is for after scanning ray is incident upon on the photosensitive drums, the synoptic diagram that spot areas changes with the difference of launching position;

Fig. 5 is the graph of a relation of the Gaussian distribution and the light intensity of light beam;

Fig. 6 is the optical path figure of the embodiment of the scanning ray that passes through first eyeglass and second eyeglass of the present utility model;

Fig. 7 is the luminous point synoptic diagram of first embodiment;

Fig. 8 is the luminous point synoptic diagram of second embodiment;

Fig. 9 is the luminous point synoptic diagram of the 3rd embodiment;

Figure 10 is the luminous point synoptic diagram of the 4th embodiment; And

Figure 11 is the luminous point synoptic diagram of the 5th embodiment.

Main symbol description: 10 is mems mirror; 11 is LASER Light Source; 111 is light beam; 113a, 113b, 113c, 114a, 114b, 115a, 115b are scanning ray; 131 is first eyeglass; 132 is second eyeglass; 14a, 14b are photoelectric sensor; 15 is photosensitive drums; 16 is cylindrical mirror; 2,2a, 2b, 2c are luminous point; And 3 be the effective scanning window.

Embodiment

With reference to Fig. 1, it is the synoptic diagram of optical path of the two-chip type f theta lens of MEMS laser scanning device of the present utility model.The two-chip type f theta lens of the MEMS laser scanning device that the utility model provides comprises first eyeglass 131 with the first optical surface 131a and second optical surface 131b, second eyeglass 132 with the 3rd optical surface 132a and the 4th optical surface 132b, is applicable to MEMS laser scanning device.Among the figure, MEMS laser scanning device mainly comprises LASER Light Source 11, mems mirror 10, cylindrical mirror 16, two photoelectric sensor 14a, 14b, and in order to the object of sensitization.In the drawings, object is a photosensitive drums (drum) 15.The light beam 111 that LASER Light Source 11 is produced projects on the mems mirror 10 by behind the cylindrical mirror 16.And the mode that mems mirror 10 swings with resonance is reflected into scanning ray 113a, 113b, 113c, 114a, 114b, 115a, 115b with light beam 111. Wherein scanning ray 113a, 113b, 113c, 114a, 114b, 115a, 115b are called sub scanning direction (sub scanning direction) in the projection of directions X, projection in the Y direction is called main scanning direction (mainscanning direction), and mems mirror 10 scanning angles are θ c.

With reference to Fig. 1 and Fig. 2, wherein Fig. 2 is the graph of a relation of mems mirror scanning angle θ and time t.Because mems mirror 10 is simple harmonic motion, its movement angle is sinusoidal variations in time, so the ejaculation angle of scanning ray and time are nonlinear relationship.Crest a-a ' as shown and trough b-b ', its pendulum angle are significantly less than wave band a-b and a '-b ', and the unequal phenomenon of this angular velocity causes scanning ray to produce the imaging deviation easily on photosensitive drums 15.Therefore, photoelectric sensor 14a, 14b are arranged within mems mirror 10 maximum scans angle ± θ c, and its angle is ± θ p that laser beam is begun to be reflected by mems mirror 10 by the crest place of Fig. 2, is equivalent to the scanning ray 115a of Fig. 1 this moment; When photoelectric sensor 14a detected scanning light beam, expression mems mirror 10 swung to+θ p angle, was equivalent to the scanning ray 114a of Fig. 1 this moment; When mems mirror 10 scanning angles change as during a point of Fig. 2, are equivalent to scanning ray 113b position at this moment; LASER Light Source 11 will be driven and give off laser beam 111 this moment, and when being scanned up to the b point of Fig. 2, be equivalent to scanning ray 113c position this moment till (quite ± θ n angle is interior to give off laser beam 111 by LASER Light Source 11); When mems mirror 10 produced reversals of vibrations, as when the wave band a '-b ', LASER Light Source 11 was driven and begins to give off laser beam 111; So finish one-period.

With reference to Fig. 1 and Fig. 3, wherein Fig. 3 is the optical path figure by the scanning ray of first eyeglass and second eyeglass.Wherein, ± θ n is the effective scanning angle, when the rotational angle of mems mirror 10 enter ± during θ n, LASER Light Source 11 begins to give off laser beam 111, be reflected into scanning ray via mems mirror 10, when scanning ray is reflected by the first optical surface 131a of first eyeglass 131 and the second optical surface 131b during by first eyeglass 131, it is the scanning ray of linear relationship with the time with the time that the distance that mems mirror 10 is reflected becomes the scanning ray of nonlinear relationship to convert distance to.After scanning ray is by first eyeglass 131 and second eyeglass 132, optical property according to the first optical surface 131a, the second optical surface 131b, the 3rd optical surface 132a, the 4th optical surface 132b, scanning ray is focused on the photosensitive drums 15, thereby on photosensitive drums 15, form a luminous point (Spot) 2 that is listed as.On photosensitive drums 15, two farthest the spacing of luminous point 2 be called effective scanning window 3.Wherein, d ₁Spacing, d for mems mirror 10 to first optical surface 131a ₂Be spacing, the d of first optical surface 131a to the second optical surface 131b ₃Be spacing, the d of the second optical surface 131b to the, three optical surface 132a ₄Be spacing, the d of the 3rd optical surface 132a to the four optical surface 132b ₅Be spacing, the R of the 4th optical surface 132b to photosensitive drums 15 ₁Be radius-of-curvature (Curvature), the R of the first optical surface 131a ₂Be radius-of-curvature, the R of the second optical surface 131b ₃Be radius-of-curvature and the R of the 3rd optical surface 132a ₄It is the radius-of-curvature of the 4th optical surface 132b.

With reference to Fig. 4, it is for after scanning ray is incident upon on the photosensitive drums, the synoptic diagram that spot areas (spot area) changes with the difference of launching position.When scanning ray 113a is incident upon photosensitive drums 15 after optical axis direction sees through first eyeglass 131 and second eyeglass 132, because of the angle that is incident in first eyeglass 131 and second eyeglass 132 is zero, in the deviation ratio that main scanning direction produced is zero, and the luminous point 2a that therefore images on the photosensitive drums 15 is circle.When scanning ray 113b and 113c see through first eyeglass 131 and second eyeglass, 132 backs and when being incident upon photosensitive drums 15, non-vanishing because of being incident in first eyeglass 131 and second eyeglass 132 and the formed angle of optical axis, non-vanishing in the deviation ratio that main scanning direction produced, thus the formed luminous point of projected length relative scanning light 113a that causes at main scanning direction is bigger; This situation is also identical at sub scanning direction, departs from the formed luminous point of scanning ray of scanning ray 113a, also will be bigger; So the luminous point 2b, the 2c that image on the photosensitive drums 15 are ellipse, and the area of 2b, 2c is greater than 2a.Wherein, S _A0With S _B0Be the luminous point of scanning ray on mems mirror 10 reflectings surface length at main scanning direction (Y direction) and sub scanning direction (directions X).As shown in Figure 5, G _aWith G _bFor the Gaussian beam (Gaussian Beams) of scanning ray is the Y direction at 13.5% place and the beam radius of directions X in light intensity, only show the beam radius of Y direction among Fig. 5.

In sum, two-chip type f theta lens of the present utility model the scanning ray of the scanning ray of mems mirror 10 reflection and Gaussian beam can be distorted (distortion) revise, and the relation of time-angular velocity is changed into the relation of time-distance.Scanning ray is exaggerated through the f Theta lens at the light beam of main scanning direction (Y direction) with sub scanning direction (directions X), produces luminous point on imaging surface, so that the resolution that meets demand to be provided.

For realizing above-mentioned effect, the two-chip type f theta lens that the utility model provides is at the first optical surface 131a of first eyeglass 131 or the 3rd optical surface 132a or the 4th optical surface 132b of the second optical surface 132a and second eyeglass 132, at main scanning direction or sub scanning direction, can use the design of sphere curved surface or non-spherical surface, if use the non-spherical surface design, its non-spherical surface satisfies following surface equation formula:

1: horizontal picture surface equation formula (Anamorphic equation)

$Z=\frac{\left(\mathrm{Cx}\right)X^2+\left(\mathrm{Cy}\right){\mathrm{<figure-callout\; id="2"\; label="Y"\; filenames="Y20082020788600261.png"\; state="\{\{state\}\}">Y</figure-callout>}}^2}{1+\sqrt{1-(1+\mathrm{Kx}){\left(\mathrm{Cx}\right)}^2{X}^2-(1+\mathrm{Ky}){\left(\mathrm{Cy}\right)}^2{\mathrm{<figure-callout\; id="2"\; label="Y"\; filenames="Y20082020788600261.png"\; state="\{\{state\}\}">Y</figure-callout>}}^2}}+A_R{[(1-A_P)X^2+(1+A_P)Y^2]}^2+$

$B_R{[(1-B_P)X^2+(1+B_P)Y^2]}^3+C_R{[(1-C_P)X^2+(1+C_P)Y^2]}^4+$

$D_R{[(1-D_P)X^2+(1+D_P)Y^2]}^5---\left(2\right)$

Wherein, Z be on the eyeglass any point with the distance (SAG) of optical axis direction to the initial point section; C _xWith C _yBe respectively the curvature (curvature) of directions X and Y direction; K _xWith K _yBe respectively the circular cone coefficient (Conic coefficient) of directions X and Y direction; A _R, B _R, C _RWith D _RBe respectively the circular cone deformation coefficient (deformation from the conic) with ten powers four times, six times, for eight times of rotation symmetry (rotationally symmetric portion); A _P, B _P, C _PWith D _PThe circular cone deformation coefficient that is respectively four times, six times, eight times, ten times powers (deformation from the conic) of the non-rotating symmetry of difference (non-rotationally symmetric components); Work as C _x=C _y, K _x=K _yAnd A _P=B _p=C _p=D _p=0, then be reduced to single aspheric surface.

2: ring is as surface equation formula (Toric equation)

$Z=\mathrm{Zy}+\frac{\left(\mathrm{Cxy}\right){\mathrm{<figure-callout\; id="2"\; label="X"\; filenames="Y20082020788600261.png"\; state="\{\{state\}\}">X</figure-callout>}}^2}{1+\sqrt{1-{\left(\mathrm{Cxy}\right)}^2{\mathrm{<figure-callout\; id="2"\; label="X"\; filenames="Y20082020788600261.png"\; state="\{\{state\}\}">X</figure-callout>}}^2}}$

$\mathrm{Cxy}=\frac{1}{(1/\mathrm{Cx})-\mathrm{Zy}}$

$\mathrm{Zy}=\frac{\left(\mathrm{Cy}\right){\mathrm{<figure-callout\; id="2"\; label="Y"\; filenames="Y20082020788600261.png"\; state="\{\{state\}\}">Y</figure-callout>}}^2}{1+\sqrt{1-(1+\mathrm{Ky}){\left(\mathrm{Cy}\right)}^2{\mathrm{<figure-callout\; id="2"\; label="Y"\; filenames="Y20082020788600261.png"\; state="\{\{state\}\}">Y</figure-callout>}}^2}}+B_4{\mathrm{<figure-callout\; id="4"\; label="Y"\; filenames="Y20082020788600261.png"\; state="\{\{state\}\}">Y</figure-callout>}}^4+B_6{Y}^6+B_8{\mathrm{<figure-callout\; id="8"\; label="Y"\; filenames="Y20082020788600321.png"\; state="\{\{state\}\}">Y</figure-callout>}}^8+B_{10}{Y}^{10}---\left(3\right)$

Wherein, Z be on the eyeglass any point with the distance (SAG) of optical axis direction to the initial point section; C _yWith C _xThe curvature (curvature) of difference Y direction and directions X; K _yCircular cone coefficient (Coniccoefficient) for the Y direction; B ₄, B ₆, B ₈With B ₁₀It is the coefficient (4th-10thorder coefficients deformation from the conic) of four times, six times, eight times, ten times powers; Work as C _x=C _yAnd K _y=A _P=B _p=C _p=D _p=0, then be reduced to single sphere.

For making scanning ray keep impartial sweep velocity on the imaging surface on the object, for example, in two identical time intervals, the spacing of keeping two luminous points equates; Two-chip type f theta lens of the present utility model can be with scanning ray 113a to the light between the scanning ray 113b, carry out the correction of scanning ray emergence angle by first eyeglass 131 and second eyeglass 132, make two identical scanning rays of the time interval, after the shooting angle correction, the distance of two luminous points that form on photosensitive drums 15 equates.Further, after laser beam 111 is via mems mirror 10 reflections, its Gaussian beam radius G _aWith G _bBigger, if this scanning ray is through the distance between mems mirror 10 and the photosensitive drums 15, then Gaussian beam radius G _aWith G _bIt is bigger to become, and causes not meeting practical resolution requirement; The scanning ray 113a that two-chip type f theta lens of the present utility model further can reflect mems mirror 10 is to the formation of the light between scanning ray 113b G _aWith G _bLess Gaussian beam makes on the photosensitive drums 15 of the image formation by rays after the focusing and produces less luminous point; Especially, two-chip type f theta lens of the present utility model more can be with the luminous point size homogenising (being limited in the scope that meets resolution requirement) that is imaged on the photosensitive drums 15, to obtain best parsing effect.

Two-chip type f theta lens of the present utility model comprises first eyeglass 131 and second eyeglass 132 that sets gradually from mems mirror 10, crescent and convex surface is constituted at the eyeglass of mems mirror 10 sides described first eyeglass 131 by positive diopter, crescent and convex surface is constituted at the eyeglass of mems mirror side described second eyeglass 132 by positive diopter, wherein first eyeglass 131 has the first optical surface 131a and the second optical surface 131b, be used for scanning ray luminous point with the angle of mems mirror 10 reflection and time nonlinear relationship convert to apart from the time be the scanning ray luminous point of linear relationship; Wherein second eyeglass 132 has the 3rd optical surface 132a and the 4th optical surface 132b, to be used for that the scanning ray correction of first eyeglass 131 is concentrated on object; According to of scanning ray on photosensitive drums 15 imaging of this two-chip type f theta lens with mems mirror 10 reflections; Wherein, the first optical surface 131a, the second optical surface 131b, the 3rd optical surface 132a and the 4th optical surface 132b have at least one can have one at least by optical surface that aspheric surface constituted or the optical surface that all uses sphere and constituted at sub scanning direction by optical surface, the first optical surface 131a, the second optical surface 131b, the 3rd optical surface 132a and the 4th optical surface 132b that aspheric surface constituted at sub scanning direction at main scanning direction.Further, at first eyeglass 131 and second eyeglass 132 constitutes and on optical effect, two-chip type f theta lens of the present utility model, further satisfy formula (4)-Shi (5) condition at main scanning direction:

$0.1<\frac{{\mathrm{<figure-callout\; id="3"\; label="d"\; filenames="Y20082020788600261.png"\; state="\{\{state\}\}">d</figure-callout>}}_3+{\mathrm{<figure-callout\; id="4"\; label="d"\; filenames="Y20082020788600261.png"\; state="\{\{state\}\}">d</figure-callout>}}_4+d_5}{f_{\left(1\right)Y}}<0.8---\left(4\right)$

$0.2<\frac{d_5}{f_{\left(2\right)Y}}<0.8---\left(5\right)$

Or, satisfy formula (6) at main scanning direction

$0.1<|f_{\mathrm{sY}}\&CenterDot;(\frac{(n_{d1}-1)}{f_{\left(1\right)y}}+\frac{(n_{d2}-1)}{f_{\left(2\right)y}})|<0.6---\left(6\right)$

And satisfy formula (7) at sub scanning direction

$0.3<|(\frac{1}{R_{1x}}-\frac{1}{R_{2x}})+(\frac{1}{R_{3x}}-\frac{1}{R_{4x}})f_{\mathrm{sX}}|<0.8---\left(7\right)$

Wherein, f _{(1) Y}Be focal length, the f of first eyeglass 131 at main scanning direction _{(2) Y}Be focal length, the d of second eyeglass 132 at main scanning direction ₃Distance, d for θ=0 ° first eyeglass, 131 object side optical surface to the second eyeglasses, 132 mems mirrors, 10 side optical surfaces ₄Be θ=0 ° second eyeglass, 132 thickness, d ₅Be the distance of θ=0 ° second eyeglass, 132 object side optical surfaces to object, f _SxBe compound focal length (combination focal length), the f of two-chip type f theta lens at sub scanning direction _SYBe compound focal length, the R of two-chip type f theta lens at main scanning direction _IxBe the radius-of-curvature of i optical surface at sub scanning direction; R _IyBe the radius-of-curvature of i optical surface at main scanning direction; n _D1With n _D2It is the refractive index (refraction index) of first eyeglass 131 and second eyeglass 132.

And, the formed luminous point homogeneity of two-chip type f theta lens of the present utility model, the maximal value that can the beam size of scanning ray on photosensitive drums 15 and the ratio delta of minimum value are represented, promptly satisfy formula (8):

$0.8<\mathrm{\&delta;}=\frac{\min (S_b\&CenterDot;S_a)}{\max (S_b\&CenterDot;S_a)}---\left(8\right)$

Further, the formed resolution of two-chip type f theta lens of the present utility model can be used η _MaxFor the luminous point of scanning ray on mems mirror 10 reflectings surface through the scanning peaked ratio of luminous point and η on photosensitive drums 15 _MinFor the luminous point of scanning ray on mems mirror 10 reflectings surface is expression through the ratio of scanning luminous point minimum value on photosensitive drums 15, can satisfy formula (9) and (10),

${\mathrm{\&eta;}}_{\max }=\frac{\max (S_b\&CenterDot;S_a)}{({\mathrm{<figure-callout\; id="0"\; label="S\; b"\; filenames="Y20082020788600261.png,Y20082020788600311.png"\; state="\{\{state\}\}">S</figure-callout>}}_b\&CenterDot;S_{a0})}<0.10---\left(9\right)$

${\mathrm{\&eta;}}_{\min }=\frac{\min (S_b\&CenterDot;S_a)}{({\mathrm{<figure-callout\; id="0"\; label="S\; b"\; filenames="Y20082020788600261.png,Y20082020788600311.png"\; state="\{\{state\}\}">S</figure-callout>}}_b\&CenterDot;S_{a0})}<0.10---\left(10\right)$

Wherein, S _aWith S _bAny luminous point that forms for scanning ray on the photosensitive drums 15 is that ratio, the η of smallest spot and maximum luminous point is the ratio of luminous point on the luminous point of scanning ray on mems mirror 10 reflectings surface and the photosensitive drums 15 on the photosensitive drums 15 at length, the δ of Y direction and directions X; S _A0With S _B0Be the luminous point of scanning ray on mems mirror 10 reflectings surface length at main scanning direction and sub scanning direction.

Below, describe structure of the present utility model and technical characterictic more in detail in conjunction with preferred embodiment of the present utility model and accompanying drawing.

The utility model embodiment describes at the main composition assembly of the two-chip type f theta lens of the utility model MEMS laser scanning device, though therefore embodiment of the present utility model is applied to MEMS laser scanning device, but common MEMS laser scanning device is except the two-chip type f theta lens that the utility model provides, other structure belongs to known technology, so those skilled in the art should be understood that content of the present utility model.And, the constituent components of the two-chip type f theta lens of MEMS laser scanning device provided by the utility model is not restricted to the following examples, wherein, each constituent components of the two-chip type f theta lens of MEMS laser scanning device can carry out various changes, modification even equivalence change, and for example: the radius-of-curvature design of first eyeglass 131 and second eyeglass 132 or the design of face type, material are selected for use, spacing adjustment etc. is not restricted to embodiment of the present utility model.

＜the first embodiment 〉

With reference to figure 3 and Fig. 6, wherein Fig. 6 is the optical path figure of the embodiment of the scanning ray that passes through first eyeglass and second eyeglass of the present utility model.The two-chip type f theta lens of present embodiment comprises first eyeglass 131 and second eyeglass 132, wherein first eyeglass 131 is the eyeglass of the crescent and convex surface of positive diopter in mems mirror 10 sides, second eyeglass 132 is the eyeglass of the crescent and convex surface of positive diopter in mems mirror 10 sides, the first optical surface 131a of first eyeglass 131 is a sphere, the 3rd optical surface 132a and the 4th optical surface 132b of the second optical surface 131b, second eyeglass 132 are aspheric surface, utilize formula (2) to carry out the aspheric surface design.Its optical characteristics and aspheric surface parameter are shown in table one and table two.

The f θ optical characteristics of table one, first embodiment

^*The expression aspheric surface

The optical surface aspheric surface parameter of table two, first embodiment

The as above two-chip type f theta lens that is constituted, f _{(1) Y}=246.44, f _{(2) Y}=247.59, f _SX=21.735, f _SYIt is the scanning ray luminous point of linear relationship with the time that=128.30 (mm) can convert scanning ray to distance, and with luminous point S on the mems mirror 10 _A0=12.90 (μ m), S _B0=4618.85 (μ m) scanning becomes scanning ray, in photosensitive drums 15 enterprising line focusings, forms less luminous point 6, and satisfies the condition of formula (4)-Shi (10), as shown in Table 3; On the photosensitive drums 15 with central shaft Z axle as shown in Table 4 at the Gaussian beam diameter (μ m) of the luminous point of Y direction distance center axle Y distance (mm); And the luminous point distribution plan of present embodiment as shown in Figure 7.Among the figure, the unit circle diameter is 0.05mm.

Table three, first embodiment table that satisfies condition

The maximal value of luminous point Gaussian beam diameter on the photosensitive drums of table four, first embodiment

＜the second embodiment 〉

The two-chip type f theta lens of present embodiment comprises first eyeglass 131 and second eyeglass 132, wherein first eyeglass 131 is the eyeglass of the crescent and convex surface of positive diopter in mems mirror 10 sides, second eyeglass 132 is the eyeglass of the crescent and convex surface of positive diopter in mems mirror 10 sides, the 3rd optical surface 132a and the 4th optical surface 132b of the first optical surface 131a of described first eyeglass 131 and the second optical surface 131b, second eyeglass 132 are aspheric surface, utilize formula (2) to carry out the aspheric surface formulae design.Its optical characteristics and aspheric surface parameter are shown in table five and table six.

The f θ optical characteristics of table five, second embodiment

^*The expression aspheric surface

The optical surface aspheric surface parameter of table six, second embodiment

The as above two-chip type f theta lens of Gou Chenging, f _{(1) Y}=442.09, f _{(2) Y}=173.53, f _SX=40.302, f _SYIt is the scanning ray luminous point of linear relationship with the time that=-480 (mm) can convert scanning ray to distance, and with luminous point S on the mems mirror 10 _A0=12.902 (μ m), S _B0=4618.85 (μ m) scanning becomes scanning ray, in photosensitive drums 15 enterprising line focusings, forms less luminous point 8, and satisfies the condition of (4)-Shi (10), as shown in Table 7; On the photosensitive drums 15 with the Gaussian beam diameter (μ m) of central shaft Z axle, as shown in Table 8 at the luminous point of Y direction distance center axle Y distance (mm); And the luminous point distribution plan of present embodiment as shown in Figure 8.Among the figure, the unit circle diameter is 0.05mm.

Table seven, second embodiment table that satisfies condition

The maximal value of luminous point Gaussian beam diameter on the photosensitive drums of table eight, second embodiment

＜the three embodiment 〉

The two-chip type f theta lens of present embodiment comprises first eyeglass 131 and second eyeglass 132, wherein first eyeglass 131 is the eyeglass of the crescent and convex surface of positive diopter in the mems mirror side, second eyeglass 132 is the eyeglass of the crescent and convex surface of positive diopter in mems mirror 10 sides, the 3rd optical surface 132a and the 4th optical surface 132b of the first optical surface 131a of first eyeglass 131 and the second optical surface 131b, second eyeglass 132 are aspheric surface, utilize formula (2) to carry out the aspheric surface formulae design.Its optical characteristics and aspheric surface parameter are shown in table nine and table ten.

The f θ optical characteristics of table nine, the 3rd embodiment

^*The expression aspheric surface

The optical surface aspheric surface parameter of table ten, the 3rd embodiment

The as above two-chip type f theta lens of Gou Chenging, f _{(1) Y}=420.884, f _{(2) Y}=172.712, f _SX=22.667, f _SYIt is the scanning ray luminous point of linear relationship with the time that=129.254 (mm) can convert scanning ray to distance, and with luminous point S on the mems mirror 10 _A0=12.90 (μ m), S _B0=4618.85 (μ m) scanning becomes scanning ray, in photosensitive drums 15 enterprising line focusings, forms less luminous point 10, and satisfies the condition of (4)～formula (10), shown in table ten one; Photosensitive drums 15 central shaft Z axles are at the Gaussian beam diameter (μ m) of the luminous point of Y direction distance center axle Y distance (mm), shown in table ten two; The luminous point distribution plan of present embodiment as shown in Figure 9.Among the figure, the unit circle diameter is 0.05mm.

Table ten the one, the 3rd embodiment table that satisfies condition

The maximal value of luminous point Gaussian beam diameter on the photosensitive drums of table ten the two, the 3rd embodiment

＜the four embodiment 〉

The two-chip type f theta lens of present embodiment comprises first eyeglass 131 and second eyeglass 132, wherein first eyeglass 131 is the eyeglass of the crescent and convex surface of positive diopter in the mems mirror side, second eyeglass 132 is the eyeglass of the crescent and convex surface of positive diopter in mems mirror 10 sides, the 3rd optical surface 132a and the 4th optical surface 132b of the first optical surface 131a of first eyeglass 131 and the second optical surface 131b, second eyeglass 132 are aspheric surface, utilize formula (2) to carry out the aspheric surface formulae design.Its optical characteristics and aspheric surface parameter are shown in table ten three and table ten four.

The f θ optical characteristics of table ten the three, the 4th embodiment

^*The expression aspheric surface

The optical surface aspheric surface parameter of table ten the four, the 4th embodiment

The as above two-chip type f theta lens of Gou Chenging, f _{(1) Y}=241.788, f _{(2) Y}=251.443, f _SX=23.607, f _SYIt is the scanning ray luminous point of linear relationship with the time that=128.23 (mm) can convert scanning ray to distance, and with luminous point S on the mems mirror 10 _A0=12.902 (μ m), S _B0=4618.85 (μ m) scanning becomes scanning ray, in photosensitive drums 15 enterprising line focusings, forms less luminous point 12, and satisfies the condition of (4)～formula (10), shown in table ten five; Photosensitive drums 15 central shaft Z axles are at the Gaussian beam diameter (μ m) of the luminous point of Y direction distance center axle Y distance (mm), shown in table ten six; And the luminous point distribution plan of present embodiment as shown in figure 10.Among the figure, the unit circle diameter is 0.05mm.

Table ten the five, the 4th embodiment table that satisfies condition

The maximal value of luminous point Gaussian beam diameter on the photosensitive drums of table ten the six, the 4th embodiment

＜the five embodiment 〉

The two-chip type f theta lens of present embodiment comprises first eyeglass 131 and second eyeglass 132, wherein first eyeglass 131 is positive diopter and the convex surface eyeglass in mems mirror 10 sides, second eyeglass 132 is the eyeglass of the crescent and convex surface of positive diopter in mems mirror 10 sides, the first optical surface 131a at first eyeglass 131, utilize formula (3) to carry out the aspheric surface design, at the second optical surface 131b of first eyeglass 131, the 3rd optical surface 132a and the 4th optical surface 132b of second eyeglass 132 is aspheric surface, utilizes formula (2) to carry out the aspheric surface formulae design.Its optical characteristics and aspheric surface parameter are shown in table ten seven and table ten eight.

The f θ optical characteristics of table ten the seven, the 5th embodiment

^*The expression aspheric surface

The optical surface aspheric surface parameter of table ten the eight, the 5th embodiment

The as above two-chip type f theta lens of Gou Chenging, f _{(1) Y}=420.884, f _{(2) Y}=172.712, f _SX=22.667, f _SYIt is the scanning ray luminous point of linear relationship with the time that=129.254 (mm) can convert scanning ray to distance, and with luminous point S on the mems mirror 10 _A0=12.902 (μ m), S _B0=4618.848 (μ m) scanning becomes scanning ray, in photosensitive drums 15 enterprising line focusings, forms less luminous point 12, and satisfies the condition of (4)～formula (10), shown in table ten nine; On the photosensitive drums 15 with the Gaussian beam diameter (μ m) of central shaft Z axle, shown in table two ten at the luminous point of Y direction distance center axle Y distance (mm); And the luminous point distribution plan of present embodiment as shown in figure 11.Among the figure, the unit circle diameter is 0.05mm.

Table ten the nine, the 5th embodiment table that satisfies condition

The maximal value of luminous point Gaussian beam diameter on table two the ten, the 5th embodiment photosensitive drums

By the foregoing description explanation as can be known, the utlity model has following effect:

Setting according to two-chip type f theta lens of the present utility model, the speed scanning phenomenon such as non-that the mems mirror that is simple harmonic motion can be successively decreased by increasing in time originally or increases progressively at imaging surface glazing dot spacing, speed scanning such as be modified to, make laser beam in the scanning of the speed such as projection work of imaging surface, make to image in the two adjacent luminous point spacings that form on the object and equate.

(1) according to the setting of two-chip type f theta lens of the present utility model, can distort and revise main scanning direction and sub scanning direction scanning ray, the luminous point on the object that focuses on imaging is dwindled.

(2) according to the setting of two-chip type f theta lens of the present utility model, can distort and revise main scanning direction and sub scanning direction scanning ray, make the luminous point size homogenising that is imaged on the object.

The above is a preferred embodiment of the present utility model only, concerning the utility model, only is illustrative, and nonrestrictive; Those skilled in the art can change it in the spirit and scope that the utility model claim is limited, revises, even the equivalence change, but all belong in the protection domain of the present utility model.

Claims (5)

1, a kind of two-chip type f theta lens of MEMS laser scanning device, it is applicable to MEMS laser scanning device, described MEMS laser scanning device comprise at least in order to the light source of emission light beam, in order to resonance swing with the beam reflection of light emitted become the mems mirror of scanning ray, and in order to the object of sensitization; It is characterized in that described two-chip type f theta lens comprise the crescent and convex surface of the positive diopter that sets gradually from described mems mirror first eyeglass of described mems mirror side and positive diopter is crescent and convex surface at second eyeglass of described mems mirror side, wherein said first eyeglass has first optical surface and second optical surface, described first optical surface and described second optical surface have at least an optical surface to be made of aspheric surface at main scanning direction, be used for scanning ray luminous point with the angle of described mems mirror reflection and time nonlinear relationship convert to apart from the time be the scanning ray luminous point of linear relationship; Described second eyeglass has the 3rd optical surface and the 4th optical surface, described the 3rd optical surface and described the 4th optical surface have at least an optical surface to be made of aspheric surface at main scanning direction, to be used for that the scanning ray correction of described first eyeglass is concentrated on described object; Image on the described object according to the scanning ray of described two-chip type f theta lens described mems mirror reflection.

2, the two-chip type f theta lens of MEMS laser scanning device according to claim 1 is characterized in that further satisfying following condition at main scanning direction:

$0.1<\frac{d_3+d_4+d_5}{f_{\left(1\right)Y}}<0.8;$

$0.2<\frac{d_5}{f_{\left(2\right)Y}}<0.8;$

Wherein, f _{(1) Y}Be focal length, the f of described first eyeglass at main scanning direction _{(2) Y}Be focal length, the d of described second eyeglass at main scanning direction ₃Be distance, the d of the θ=0 ° described first eyeglass object side optical surface to the described second eyeglass mems mirror side optical surface ₄Thickness, d for θ=0 ° described second eyeglass ₅Be the distance of the θ=0 ° described second eyeglass object side optical surface to described object.

3, the two-chip type f theta lens of MEMS laser scanning device according to claim 1 is characterized in that further satisfying following condition:

Satisfy at main scanning direction

$0.1<|f_{\mathrm{sY}}\&CenterDot;(\frac{(n_{d1}-1)}{f_{\left(1\right)y}}+\frac{(n_{d2}-1)}{f_{\left(2\right)y}})|<0.6;$

Satisfy at sub scanning direction

$0.3<|(\frac{1}{R_{1x}}-\frac{1}{R_{2x}})+(\frac{1}{R_{3x}}-\frac{1}{R_{4x}})f_{\mathrm{sX}}|<0.8;$

Wherein, f _{(1) Y}With f _{(2) Y}Be described first eyeglass and described second eyeglass focal length, f at main scanning direction _SXBe compound focal length, the f of two-chip type f theta lens at sub scanning direction _SYBe compound focal length, the R of two-chip type f theta lens at main scanning direction _IxBe radius-of-curvature, the n of i optical surface at sub scanning direction _D1With n _D2Be respectively the refractive index of described first eyeglass and described second eyeglass.

4, the two-chip type f theta lens of MEMS laser scanning device according to claim 1 is characterized in that the ratio of maximum luminous point and smallest spot size on the described object satisfies:

$0.8<\mathrm{\&delta;}=\frac{\min (S_b\&CenterDot;S_a)}{\max (S_b\&CenterDot;S_a)};$

Wherein, S _aWith S _bAny luminous point that forms for scanning ray on the object is the ratio of smallest spot and maximum luminous point on the described object at length, the δ of main scanning direction and sub scanning direction.

5, the two-chip type f theta lens of MEMS laser scanning device according to claim 1 is characterized in that the ratio of maximum luminous point on the described object and the ratio of smallest spot on described object satisfy respectively

${\mathrm{\&eta;}}_{\max }=\frac{\max (S_b\&CenterDot;S_a)}{(S_{b0}\&CenterDot;S_{a0})}<0.10;$

${\mathrm{\&eta;}}_{\min }=\frac{\min (S_b\&CenterDot;S_a)}{(S_{b0}\&CenterDot;S_{a0})}<0.10;$

Wherein, S _A0With S _B0Be the luminous point of scanning ray on the described mems mirror reflecting surface length, S at main scanning direction and sub scanning direction _aWith S _bAny luminous point that forms for scanning ray on the object is at length, the η of main scanning direction and sub scanning direction _MaxBe the luminous point of scanning ray on the described mems mirror reflecting surface ratio, η through scanning maximum luminous point on described object _MinBe the luminous point of scanning ray on the described mems mirror reflecting surface ratio through scanning smallest spot on described object.

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