JP7629252B2 - Scanning Optical System - Google Patents

Description

The present invention relates to a scanning optical system.

The imaging optical systems used in printers and multifunction machines are required to have the function of scanning a scanning spot on the scanning surface at a constant speed (constant-speed scanning function) in addition to the function of converging a light beam on the scanning surface (convergence function). However, it is difficult to miniaturize a scanning optical system that achieves the convergence function and the constant-speed scanning function. Therefore, scanning optical systems have been proposed that achieve miniaturization by sacrificing the convergence function and the constant-speed scanning function to some extent (for example, Patent Document 1).

In such a scanning optical system, the function of scanning the scanning spot at a constant speed can be realized by electrically controlling the light emission timing of the light source, even if it cannot be realized by the scanning optical system itself. On the other hand, there is a problem with the convergence function of such an optical system in that the diameter of the scanning spot of the light beam increases, especially at the periphery of the scanning area.

Therefore, there is a need for a scanning optical system that achieves compactness by sacrificing some of the convergence function and constant speed scanning function, and that suppresses an increase in the scanning spot diameter of the light beam at the periphery of the scanning area.

JP 2015-31824 A

The object of the present invention is to provide a scanning optical system that achieves compactness by sacrificing some of the convergence function and constant speed scanning function, and that suppresses an increase in the scanning spot diameter of the light beam at the periphery of the scanning area.

The scanning optical system of the present invention includes a deflector that deflects a light beam from a light source, and an imaging optical system that includes a first scanning lens closer to the deflector and a second scanning lens farther from the deflector, and that guides the polarized light beam to a scanning surface. The scanning direction is perpendicular to the rotation axis of the deflector and the optical axis of the imaging optical system, the angle formed by a straight line that is a projection of the principal ray of the deflected light beam onto a plane perpendicular to the rotation axis of the deflector and a straight line that is a projection of the optical axis onto the plane is defined as a deflection angle θ, a value obtained by dividing half the scanning width W by the maximum value of the deflection angle θ is defined as a system focal length f, the distance from the deflection surface of the deflector to the scanning surface on the optical axis is defined as L, and the distance from the deflection surface to the surface of the second scanning lens farther from the deflector is defined as d,
0.88≦f/L
d/L≦0.3
satisfies the above condition, the scanning direction is the y-axis direction, the y-coordinate of the optical axis is 0, and the y-coordinate of the position of the principal ray of the light beam on the scanning surface is expressed as a function of the deflection angle θ. When this function's differential function dy/dθ increases in absolute value according to the absolute value of the deflection angle θ, and the ratio of the deflection angle to the maximum absolute value of the deflection angle θ is r, the differential function dy/dθ is
-1 ≦ r ≦ -0.4 and
0.4 ≦ r ≦ 1
Each of these has multiple inflection points in the range.

The scanning optical system of the present invention comprises:
0.88≦f/L
Since the above relation is satisfied, f is relatively large and the length of the second scanning lens in the y-axis direction is relatively small.
d/L≦0.3
Since the second scanning lens is disposed relatively close to the deflector, the scanning optical system becomes compact.

In the scanning optical system of the present invention, when the y coordinate of the position on the scanning surface of the principal ray of the light beam is expressed as a function of the deflection angle θ, the shape of the curve of the differential function dy/dθ of the function can be appropriately determined, thereby suppressing an increase in the scanning spot diameter of the light beam at the periphery of the scanning area.

In the scanning optical system of the first embodiment of the present invention, the direction of the optical axis is the z-axis direction, and the refractive power of the first scanning lens in the yz cross section is positive for light rays passing near the optical axis, decreases according to the absolute value of the y coordinate of the position where the light rays pass, and is negative for light rays passing through the peripheral portion in the y-axis direction, and the refractive power of the second scanning lens in the yz cross section is negative for light rays passing near the optical axis, increases according to the absolute value of the y coordinate of the position where the light rays pass, and is positive for light rays passing through the peripheral portion in the y-axis direction.

In the scanning optical system of this embodiment, the relationship between the absolute value of the y coordinate of the position through which the light ray passes and the refractive powers of the first and second scanning lenses with respect to that light ray is adjusted, and the shape of the curve of the differential function dy/dθ is appropriately specified, thereby suppressing an increase in the scanning spot diameter of the light beam at the periphery of the scanning area.

In the scanning optical system of the second embodiment of the present invention, the value of (|dy/dθ| - f)/f is -3% or less when the deflection angle θ is 0, and is 5% or more when the absolute value of the deflection angle θ is at its maximum value.

The present invention is particularly effective when the value of (|dy/dθ| - f)/f satisfies the above conditions.

1 is a perspective view showing an example of an optical system including a scanning optical system of the present invention. FIG. 1 is a plan view showing an example of an optical system including a scanning optical system of the present invention. 1 is a diagram showing an embodiment of a scanning optical system of the present invention, which will be described later. 4 is a diagram for explaining a deflection angle of a scanning optical system. FIG. 1 is a diagram showing the relationship between the deflection angle and the image height of a scanning optical system that satisfies the relationship of formula (1) for various values of B. FIG. 10 is a diagram showing the difference between the image height of a scanning optical system that satisfies the relationship of formula (1) for various values of B and the image height of a scanning optical system in which B is 0. FIG. 1 is a diagram showing the relationship between the deflection angle of a scanning optical system that satisfies the relationship of formula (1) for various values of B and the partial magnification of a light beam at that deflection angle. 1 is a diagram showing the deflection angle of a scanning optical system that satisfies the relationship of formula (1) for various values of B, and the diameter in the main scanning direction of a light beam spot on a scanning surface of a light beam at that deflection angle. FIG. 2 is a diagram showing a scanning optical system according to a comparative example of the present invention. FIG. 4 is a diagram showing the partial magnification of a scanning optical system of a comparative example. 11 is a diagram showing a diameter in the main scanning direction of a light beam spot on a scanning surface of a scanning optical system of a comparative example. 4 is a diagram for explaining the refractive power of a scanning lens in a yz cross section; FIG. 13 is a diagram showing the refractive power of the first scanning lens of the comparative example in the yz cross section. FIG. 13 is a diagram showing the refractive power of the second scanning lens of the comparative example in the yz cross section. FIG. FIG. 4 is a diagram showing the refractive power of the first scanning lens in the yz cross section of the example. FIG. 11 is a diagram showing the refractive power of the second scanning lens in the yz cross section of the example. 3A and 3B are diagrams for explaining functions of a first scanning lens 301 and a second scanning lens 302 in the embodiment. FIG. 4 is a diagram showing the partial magnification of the scanning optical system of the embodiment. FIG. 13 is a diagram showing differential values of partial magnification with respect to the deflection angle of the scanning optical system of the embodiment. 4 is a diagram showing a diameter in the main scanning direction of a light beam spot on a scanning surface of a scanning optical system of an embodiment.

Figure 1 is a perspective view showing an example of an optical system including a scanning optical system of the present invention.

Figure 2 is a plan view showing an example of an optical system including a scanning optical system of the present invention.

In the example shown in Figures 1 and 2, multiple light beams are incident on a deflector that is a polygon mirror to perform scanning on multiple scanning surfaces. In the example shown in Figures 1 and 2, four light beams are incident on one polygon mirror by four light sources. The first scanning optical system includes a first light source 1, a first lens 1 of the incident optical system, a polygon mirror, a first scanning lens 1, and a third scanning lens 3. The second scanning optical system includes a second light source 2, a second lens 2 of the incident optical system, a polygon mirror, a second scanning lens 2, and a fourth scanning lens 4. The third scanning optical system includes a third light source 3, a third lens 3 of the incident optical system, a polygon mirror, a first scanning lens 1, and a third scanning lens 3. The fourth scanning optical system includes a fourth light source 4, a fourth lens 4 of the incident optical system, a polygon mirror, a second scanning lens 2, and a fourth scanning lens 4. That is, the polygon mirror is shared by the first to fourth scanning optical systems, the first scanning lens 1 and the third scanning lens 3 are shared by the first and third scanning optical systems, and the second scanning lens 2 and the fourth scanning lens 4 are shared by the second and fourth scanning optical systems.

Figure 3 is a diagram showing an embodiment of the scanning optical system of the present invention, which will be described later. The light beam emitted from the light source 101 passes through the aperture and lens 103, is deflected by the deflector 200, which is a polygon mirror, and is then focused on the scanning surface 400 by the imaging optical system including the first scanning lens 301 and the second scanning lens 303. The x-axis is defined as the direction of the rotation axis of the deflector, the z-axis is defined as the direction of the optical axis of the imaging optical system, and the y-axis is defined as being perpendicular to the x-axis and z-axis. The scanning direction is the direction of the y-axis. The y-axis direction is also called the main scanning direction, and the x-axis direction is also called the sub-scanning direction.

Figure 4 is a diagram for explaining the deflection angle of the scanning optical system. The deflection angle θ is the angle between a straight line which is a projection of the principal ray of the light beam deflected by the deflector 200 onto the yz plane and a straight line which is a projection of the optical axis of the imaging optical system onto the yz plane. In Figure 4, P represents the reflection point of the principal ray on the deflection surface of the deflector 200. In Figure 4, the path of the principal ray of the first scanning optical system, which has a relatively small maximum value of the deflection angle θ, is shown by a solid line, and the path of the principal ray of the second scanning optical system, which has a relatively large maximum value of the deflection angle θ, is shown by a solid line. If the effective scanning width of both scanning optical systems is W, the passing range of the light beam of the first scanning lens 301 and the second scanning lens 303 of the first scanning optical system is smaller than the passing range of the light beam of the first scanning lens 301 and the second scanning lens 303 of the second scanning optical system.

の関係が求められる。この関係をｆθ特性と呼称する。ここで、ｙは光軸の座標を0とした場合の走査面４００上の主光線の位置、すなわち結像位置のｙ座標であり像高とも呼称する。上記の関係が成立する場合に偏向器が一定速度で回転すると走査面上の走査スポットは一定速度で移動する。走査光学系の有効走査幅をＷとして、ｆは有効走査幅の半値Ｗ／２を偏向角θの絶対値の最大値で除した値でありシステム焦点距離と呼称する。 On the other hand, in the scanning optical system, a function of uniform speed scanning of the scanning spot on the scanning surface 400 is realized.

The following relationship can be obtained. This relationship is called the fθ characteristic. Here, y is the position of the principal ray on the scanning surface 400 when the coordinate of the optical axis is 0, that is, the y coordinate of the imaging position, and is also called the image height. When the above relationship is established, if the deflector rotates at a constant speed, the scanning spot on the scanning surface moves at a constant speed. Assuming that the effective scanning width of the scanning optical system is W, f is the value obtained by dividing half the effective scanning width W/2 by the maximum absolute value of the deflection angle θ, and is called the system focal length.

In order to achieve the converging and constant speed scanning functions of the scanning optical system, the scanning lens needs to be positioned sufficiently far away from the deflector, and as a result, the scanning lens and scanning optical system cannot be made sufficiently compact.

Ｂは０から１の範囲の値のパラメータでありＫは定数である。Ｂが０の場合に

であり、Ｂが１の場合に

である。 In order to realize a compact scanning optical system, Japanese Patent Application Laid-Open No. 2003-233696 proposes a scanning optical system in which the y coordinate of the scanning spot and the deflection angle θ have the following relationship:

B is a parameter whose value ranges from 0 to 1, and K is a constant. When B is 0,

and when B is 1,

It is.

Next, consider the properties of the scanning optical system that satisfy the relationship of formula (1) for various values of B. As an example, if the scanning width W is 220 millimeters and the maximum absolute value of the deflection angle is 45 degrees, the various values of B and the corresponding values of K are as shown in Table 1 below. The unit of K is millimeters.

Figure 5A shows the relationship between deflection angle and image height for a scanning optical system that satisfies the relationship of equation (1) for various values of B. The horizontal axis of Figure 5A shows the ratio of the deflection angle to the maximum absolute value of the deflection angle. The vertical axis of Figure 5A shows the y coordinate on the scanning plane of the light ray of the deflection angle on the horizontal axis, i.e., the image height. The vertical axis is in millimeters.

Figure 5B shows the difference between the image height of a scanning optical system that satisfies the relationship of equation (1) for various values of B and the image height of a scanning optical system in which B is 0. The horizontal axis of Figure 5B shows the ratio of the deflection angle to the maximum absolute value of the deflection angle. The vertical axis of Figure 5B shows the difference between the y coordinate on the scanning plane of the light beam with the deflection angle on the horizontal axis of the scanning optical system and the y coordinate on the scanning plane of the light beam with the same deflection angle of a scanning optical system in which B is 0. The vertical axis is in millimeters.

ここで、式（２）中のｙｒは式（１）の関係を有しＢが０ではない走査光学系による偏向角θの光線の走査面上のｙ座標を表し、式（２）中のｙはy = fθの関係を有する走査光学系による偏向角θの光線の走査面上のｙ座標を表す。 Fig. 6 is a diagram showing the relationship between the deflection angle of a scanning optical system that satisfies the relationship of formula (1) for various values of B and the partial magnification of a light beam at that deflection angle. The horizontal axis of Fig. 6 indicates the ratio of the deflection angle to the maximum absolute value of the deflection angle. The vertical axis of Fig. 6 indicates the partial magnification. The unit of the vertical axis is percent. The partial magnification is defined by the following formula.

Here, yr in equation (2) represents the y coordinate on the scanning surface of the light ray at a deflection angle θ by the scanning optical system having the relationship of equation (1) and where B is not 0, and y in equation (2) represents the y coordinate on the scanning surface of the light ray at a deflection angle θ by the scanning optical system having the relationship of y = fθ.

The partial magnification shown in Figure 6 indicates the deviation of the scanning spot of the scanning optical system from the constant velocity characteristic. When the partial magnification is 0, the scanning spot has a constant velocity. As the absolute value of the partial magnification increases, the deviation of the scanning spot from the constant velocity characteristic increases.

Figure 7 shows the deflection angle of a scanning optical system that satisfies the relationship of formula (1) for various values of B, and the diameter of the light beam spot on the scanning surface in the main scanning direction of the light beam at that deflection angle. The horizontal axis of Figure 7 shows the ratio of the deflection angle to the maximum absolute value of the deflection angle. The unit of the horizontal axis is millimeters. The vertical axis of Figure 7 shows the diameter of the light beam spot in the main scanning direction. In Figure 7, the diameter of the light beam spot in the main scanning direction is referred to as the main spot diameter. The unit of the vertical axis is micrometers. The main spot diameter when the deflection angle is 0 is 60 micrometers.

The diameter of the light beam spot shown in Figure 7 indicates the convergence function of the scanning optical system.

Ultimately, if B is brought closer to 1, the imaging optical system can be made compact, but the partial magnification and the diameter of the light beam spot on the scanning surface in the main scanning direction increase according to the absolute value of the deflection angle θ, and reach a maximum at the maximum absolute value of the deflection angle θ. Here, even if the uniform speed scanning function of the scanning spot cannot be realized by the scanning optical system, it is possible to realize it by electrically controlling the light emission timing of the light source. Therefore, a scanning optical system in which B is not 0, and in which the diameter of the light beam spot in the main scanning direction is relatively small, especially near the maximum absolute value of the deflection angle θ, is required.

Next, comparative examples and examples of the present invention will be described.

ただし、

y：主走査方向座標
x：副走査方向座標
z：サグ
k：コーニック係数
Ry：主走査方向断面曲率半径
rx(y)：副走査方向断面の主走査方向座標yにおける曲率半径
rx(0)：副走査方向断面の光軸上の曲率半径
Ai：主走査方向断面の非球面係数（i = １、２、３、４・・・）
Bi：副走査方向断面曲率半径を決定する係数（i = １、２、３、４・・・） The shapes of the entrance surface and exit surface of the first scanning lens in the comparative example and the example can be expressed by the following formula A. In the following description, the main scanning direction cross section means a yz cross section perpendicular to the x axis, and the sub-scanning direction cross section means an xz cross section perpendicular to the y axis.

however,

y: Main scanning direction coordinate
x: Sub-scanning direction coordinate
z: sag
k: Conic coefficient
Ry: Radius of curvature in the main scanning direction
rx(y): Radius of curvature at the main scanning coordinate y of the cross section in the sub-scanning direction
rx(0): Radius of curvature on the optical axis in the cross section in the sub-scanning direction
Ai: Aspheric coefficient of the cross section in the main scanning direction (i = 1, 2, 3, 4, ...)
Bi: Coefficient that determines the cross-sectional curvature radius in the sub-scanning direction (i = 1, 2, 3, 4, ...)

ただし、

ただし、

y：主走査方向座標
x：副走査方向座標
z：サグ
zs：主走査方向サグ
zm：副走査方向サグ
ky：主走査方向コーニック係数
Ry：主走査方向断面曲率半径
h：母線湾曲関数
rx(y)：副走査方向断面の主走査方向座標yにおける曲率半径
rx(0)：副走査方向断面の光軸上の曲率半径
Ai：主走査方向断面の非球面係数（i = １、２、３、４・・・）
Bi：副走査方向断面曲率半径を決定する係数（i = １、２、３、４・・・）
Ci：母線湾曲係数（i = １、２、３、４・・・）
Di：副走査方向断面の非球面係数（i = １、２、３、４・・・）
ただし、係数Ai、Biは主走査方向座標符号+/-によって個別の値をとる。+y領域ではApi、Bpi、-y領域ではAmi、Bmiをとる。 The shapes of the entrance surface and the exit surface of the second scanning lens in the comparative example and the embodiment can be expressed by the following formula B.

however,

however,

y: Main scanning direction coordinate
x: Sub-scanning direction coordinate
z: sag
zs: Sag in the main scanning direction
zm: Sub-scanning direction sag
ky: Conic coefficient in the main scanning direction
Ry: Radius of curvature in the main scanning direction
h: Generatrix curvature function
rx(y): Radius of curvature at the main scanning coordinate y of the cross section in the sub-scanning direction
rx(0): Radius of curvature on the optical axis in the cross section in the sub-scanning direction
Ai: Aspheric coefficient of the cross section in the main scanning direction (i = 1, 2, 3, 4, ...)
Bi: Coefficient that determines the cross-sectional curvature radius in the sub-scanning direction (i = 1, 2, 3, 4, ...)
Ci: Generatrix curvature coefficient (i = 1, 2, 3, 4...)
Di: Aspheric coefficient of the cross section in the sub-scanning direction (i = 1, 2, 3, 4, ...)
However, the coefficients Ai and Bi take different values depending on the +/- coordinate sign in the main scanning direction. In the +y area, they take Api and Bpi, and in the -y area, they take Ami and Bmi.

8 is a diagram showing a scanning optical system of a comparative example of the present invention. A light beam emitted from a light source 101 passes through an aperture and a lens 103', is deflected by a deflector 200 which is a polygon mirror, and is then focused on a scanning surface 400 by an imaging optical system including a first scanning lens 301' and a second scanning lens 303'.

The scanning optical system of the comparative example was designed so that the relationship in equation (1) was satisfied for the light rays at each deflection angle, the aberrations were appropriately corrected, and the spot diameter of the light beam was usable.

のＢは0.62であり、有効走査幅が216ミリメータであり、偏向角θの絶対値の最大値は44度である。 In the scanning optical system of the comparative example, the formula (1)

is 0.62, the effective scanning width is 216 millimeters, and the maximum absolute value of the deflection angle θ is 44 degrees.

Table 2 shows the numerical data of the scanning optical system of the comparative example. In Table 2 and the following tables, the first scanning lens is referred to as Lens A, and the second scanning lens is referred to as Lens B. The "deflection reference point" is the reflection point of the principal ray of the deflected light beam on the surface of the deflector when the straight line obtained by projecting the principal ray of the deflected light beam onto the yz plane is in the z-axis direction. The "principal angle of incidence" and "secondary angle of incidence" are the angles of incidence on the yz plane and xz plane, respectively.

On the optical axis of the imaging optical system, the distance from the deflection surface of the deflector to the scanning surface is L, and the distance from the deflection surface to the surface of the second scanning lens that is farther away from the deflector is d. The following relationship holds:

f/L = 139.4/158.32 = 0.88
d/L= (38.4+4.5)/158.32=0.270

Tables 3A and 3B are tables showing coefficients of the equations expressing the surface shapes of the first and second scanning lenses of the comparative example.

Figure 9 is a diagram showing the partial magnification of a scanning optical system of a comparative example. The horizontal axis of Figure 9 shows the ratio of the deflection angle to the maximum absolute value of the deflection angle. The vertical axis of Figure 9 shows the partial magnification of the scanning optical system for the light beam with the deflection angle shown on the horizontal axis. The curve showing the partial magnification in Figure 9 is approximate to the curve showing the partial magnification when B in Figure 6 is 0.6.

Figure 10 is a diagram showing the diameter in the main scanning direction of the light beam spot on the scanning surface of the scanning optical system of the comparative example. The horizontal axis of Figure 10 shows the coordinates of the actual imaging position of the light beam. The unit of the horizontal axis is millimeters. The vertical axis of Figure 10 shows the diameter in the main scanning direction of the light beam spot on the scanning surface of the light beam at the coordinates of the actual imaging position shown on the horizontal axis. The curve showing the diameter in the main scanning direction of the light beam spot in Figure 10 is approximated to the curve showing the diameter in the main scanning direction of the light beam spot when B in Figure 7 is 0.6.

FIG. 11 is a diagram for explaining the refractive power of the scanning lens in the yz section. FIG. 11 shows the yz section including the points where the principal ray of each deflection angle intersects with the optical surface. The radius of curvature at the incident position Ym1 of the light incident surface is Rm1, and the radius of curvature at the light incident surface position Ym2 of the exit surface is Rm2. The angle between the principal ray of the light beam incident on the incident surface and the normal to the incident surface is θo1, and the angle between the principal ray of the light beam passing through the incident surface and the normal to the incident surface is θi1. The angle between the principal ray of the light beam arriving at the exit position of the exit surface and the normal to the exit surface is θo2, the angle between the principal ray of the light beam passing through the exit surface and the normal to the exit surface is θi2, and the optical path length from the entrance surface to the exit surface is dm. The refractive index of the scanning lens material is N. The refractive power φm of the scanning lens in the yz section at this time is defined by the following formula.

Figure 12 is a diagram showing the refractive power in the yz cross section of the first scanning lens 301' of the comparative example. The horizontal axis of Figure 12 shows the coordinates of the actual imaging position of the light beam. The unit of the horizontal axis is millimeters. The vertical axis of Figure 12 shows the refractive power in the yz cross section of the first scanning lens 301' of the comparative example for a light ray that reaches the coordinates of the actual imaging position shown on the horizontal axis.

Figure 13 is a diagram showing the refractive power in the yz cross section of the second scanning lens 302' of the comparative example. The horizontal axis of Figure 13 shows the coordinates of the actual imaging position of the light beam. The unit of the horizontal axis is millimeters. The vertical axis of Figure 13 shows the refractive power in the yz cross section of the second scanning lens 302' of the comparative example for a light ray that reaches the coordinates of the actual imaging position shown on the horizontal axis.

EXAMPLES The scanning optical system of the examples was designed by adjusting the surface shapes of the first and second scanning lenses according to a procedure to be described later, using the scanning optical system of the comparative example as a reference.

In the scanning optical system of the embodiment, the effective scanning width is 216 millimeters, and the maximum absolute value of the deflection angle θ is 42 degrees.

Table 4 shows the numerical data of the scanning optical system of the embodiment.

On the optical axis of the imaging optical system, the distance from the deflection surface of the deflector to the scanning surface is L, and the distance from the deflection surface to the surface of the second scanning lens that is farther away from the deflector is d. The following relationship holds:

0.88≦f/L=147.3/158.07=0.93
d/L=(37.93+4.5)/158.07=0.268≦0.3

Since f/L in the scanning optical system of the embodiment is larger than f/L in the scanning optical system of the comparative example, the length in the y-axis direction of the second scanning lens of the embodiment can be made shorter than that of the comparative example. Also, since d/L in the scanning optical system of the embodiment is smaller than d/L in the scanning optical system of the comparative example, the scanning optical system of the embodiment is more compact than the scanning optical system of the comparative example.

Tables 5A and 5B are tables showing coefficients of the equations expressing the surface shapes of the first and second scanning lenses of the embodiment.

Figure 14 is a diagram showing the refractive power in the yz cross section of the first scanning lens 301 of the embodiment. The horizontal axis of Figure 14 indicates the coordinates of the actual imaging position of the light beam. The unit of the horizontal axis is millimeters. The vertical axis of Figure 14 indicates the refractive power in the yz cross section of the first scanning lens 301 of the embodiment for a light ray that reaches the coordinates of the actual imaging position shown on the horizontal axis. In Figure 14, the solid line indicates the refractive power in the yz cross section of the first scanning lens 301 of the embodiment, and the dashed line indicates the refractive power in the yz cross section of the first scanning lens 301' of the comparative example shown in Figure 12. According to Figure 14, the refractive power in the y-z cross section of the first scanning lens 301' in the comparative example is a substantially constant positive value regardless of the coordinate of the actual imaging position, whereas the refractive power in the y-z cross section of the first scanning lens 301 in the embodiment is positive in areas where the absolute value of the coordinate of the actual imaging position is relatively small, decreases as the absolute value of the coordinate of the actual imaging position increases, and is negative in areas where the absolute value of the coordinate of the actual imaging position is relatively large.

In other words, the refractive power of the first scanning lens 301 in the yz cross section is positive for light rays passing near the optical axis, decreases according to the absolute value of the y coordinate of the position where the light rays pass, and is negative for light rays passing through the peripheral portion in the y-axis direction.

Figure 15 is a diagram showing the refractive power in the yz section of the second scanning lens 302 of the embodiment. The horizontal axis of Figure 15 indicates the coordinates of the actual imaging position of the light beam. The unit of the horizontal axis is millimeters. The vertical axis of Figure 15 indicates the refractive power in the yz section of the second scanning lens 302 of the embodiment for the light beam that reaches the coordinates of the actual imaging position shown on the horizontal axis. In Figure 15, the solid line indicates the refractive power in the yz section of the second scanning lens 302 of the embodiment, and the dashed line indicates the refractive power in the yz section of the second scanning lens 302' of the comparative example shown in Figure 13. According to Figure 15, the refractive power in the yz section of the second scanning lens of the comparative example and the embodiment both increases with an increase in the absolute value of the coordinate of the actual imaging position. The refractive power in the yz section of the second scanning lens 302' of the comparative example is positive in the entire range of the coordinates of the actual imaging position. The refractive power in the yz section of the second scanning lens 302 of the embodiment is negative in areas where the absolute value of the coordinate of the actual imaging position is relatively small, increases as the absolute value of the coordinate of the actual imaging position increases, is positive in areas where the absolute value of the coordinate of the actual imaging position is relatively large, and is greater than the refractive power in the yz section of the second scanning lens 302' of the comparative example at the periphery of the scanning area.

In other words, the refractive power in the yz cross section of the second scanning lens 302 is negative for light rays passing near the optical axis, increases according to the absolute value of the y coordinate of the position through which the light rays pass, and is positive for light rays passing through the peripheral portion in the y-axis direction.

Figure 16 is a diagram for explaining the functions of the first scanning lens 301 and the second scanning lens 302 of the embodiment. In an area where the absolute value of the y coordinate of the first scanning lens 301 is relatively small, the refractive power in the yz cross section is positive, so the light beam is focused. In an area where the absolute value of the y coordinate of the first scanning lens 301 is relatively large, the refractive power in the yz cross section is negative, so the light beam is diverged. In an area where the absolute value of the y coordinate of the second scanning lens 302 is relatively small, the refractive power in the yz cross section is negative, so the light beam is diverged. In an area where the absolute value of the y coordinate of the second scanning lens 302 is relatively large, the refractive power in the yz cross section is positive, so the light beam is focused.

Figure 17 is a diagram showing the partial magnification of the scanning optical system of the embodiment. The horizontal axis of Figure 17 shows the ratio of the deflection angle to the maximum absolute value of the deflection angle. The vertical axis of Figure 17 shows the partial magnification of the scanning optical system for the light beam of the deflection angle shown on the horizontal axis. The vertical axis is in percent. In Figure 17, the solid line shows the partial magnification of the embodiment, and the dashed line shows the partial magnification of the comparative example shown in Figure 9. The partial magnification of the embodiment and the comparative example is negative and minimum when the deflection angle is 0, increases according to the absolute value of the deflection angle, and is maximum at the maximum absolute value of the deflection angle. The partial magnification of the scanning optical system of the embodiment is smaller than the partial magnification of the comparative example, especially near the maximum absolute value of the deflection angle, i.e., near 1 and -1, when the ratio of the deflection angle to the maximum absolute value of the deflection angle.

In the embodiment, the partial magnification is approximately -8% when the deflection angle is 0, and the partial magnification is approximately 10% when the absolute value of the deflection angle is at its maximum value.

Fig. 18 is a diagram showing the differential value with respect to the deflection angle of the partial magnification of the scanning optical system of the embodiment. The horizontal axis of Fig. 18 indicates the ratio of the deflection angle to the maximum absolute value of the deflection angle. The vertical axis of Fig. 18 indicates the differential value with respect to the deflection angle of the partial magnification of the scanning optical system for the light beam of the deflection angle shown on the horizontal axis. The unit of the vertical axis is percentage. In Fig. 18, the solid line indicates the differential value with respect to the deflection angle of the partial magnification of the embodiment, and the dashed line indicates the differential value with respect to the deflection angle of the partial magnification of the comparative example shown in Fig. 9. According to Fig. 18, the differential value with respect to the deflection angle of the partial magnification of the scanning optical system of the embodiment is expressed as r, where r is the ratio of the deflection angle to the maximum absolute value of the deflection angle.
-1 ≦ r ≦ -0.4 and
0.4 ≦ r ≦ 1
Therefore, the partial magnification of the scanning optical system of the embodiment as a function of the deflection angle is
-1 ≦ r ≦ -0.4 and
0.4 ≦ r ≦ 1
In the range of

が偏向角θの絶対値にしたがって増加し、偏向角θの絶対値の最大値に対する偏向角の比率をｒとして該関数の偏向角θに関する微分

は
-1 ≦ r ≦ -0.4 及び
0.4 ≦ r ≦ 1
の範囲でそれぞれ３個の変曲点を有する。 From equation (2), when the y coordinate of the position of the principal ray of the light beam on the scanning surface is expressed as a function of the deflection angle θ, the absolute value of the derivative of the function with respect to the deflection angle θ is

increases according to the absolute value of the deflection angle θ, and the ratio of the deflection angle to the maximum absolute value of the deflection angle θ is r, and the derivative of the function with respect to the deflection angle θ is

teeth
-1 ≦ r ≦ -0.4 and
0.4 ≦ r ≦ 1
Each of the three inflection points is in the range of

By adjusting the relationship between the coordinates of the actual imaging position of the light beam and the refractive powers of the first and second scanning lenses with respect to the light rays that reach those coordinates using the scanning optical system of the comparative example as a reference, the shape of the partial magnification curve shown in Figure 17 for the scanning optical system of the embodiment can be adjusted.

Figure 19 is a diagram showing the diameter in the main scanning direction of the light beam spot on the scanning surface of the scanning optical system of the embodiment. The horizontal axis of Figure 19 indicates the y coordinate of the actual imaging position of the light beam. The unit of the horizontal axis is millimeters. The vertical axis of Figure 19 indicates the diameter in the main scanning direction of the light beam spot on the scanning surface of the light beam having the chief ray passing through the coordinate of the actual imaging position shown on the horizontal axis. In Figure 19, the solid line indicates the diameter in the main scanning direction of the light beam spot on the scanning surface of the scanning optical system of the embodiment, and the dashed line indicates the diameter in the main scanning direction of the light beam spot on the scanning surface of the scanning optical system of the comparative example shown in Figure 10. In Figure 19, the maximum value of the diameter in the main scanning direction of the light beam spot on the scanning surface of the scanning optical system of the embodiment is smaller than the maximum value of the diameter in the main scanning direction of the light beam spot on the scanning surface of the scanning optical system of the comparative example, and the difference is greater than 3 micrometers.

Claims (3)

A deflector that deflects a light beam from a light source;
a scanning optical system including a first scanning lens closer to the deflector and a second scanning lens farther from the deflector, and an imaging optical system that guides a polarized light beam to a scanning surface, wherein the scanning direction is perpendicular to the rotation axis of the deflector and the optical axis of the imaging optical system, the angle formed by a straight line which is a projection of a principal ray of the deflected light beam onto a plane perpendicular to the rotation axis of the deflector and a straight line which is a projection of the optical axis onto the plane is defined as a deflection angle θ, a value obtained by dividing half-value W/2 of a scanning width W by the maximum value of the deflection angle θ is defined as a system focal length f, a distance on the optical axis from a deflection surface of the deflector to the scanning surface is defined as L, and a distance from the deflection surface to a surface of the second scanning lens farther from the deflector is defined as d,
0.88≦f/L
d/L≦0.3
satisfies the above condition, the scanning direction is the y-axis direction, the y-coordinate of the optical axis is 0, and the y-coordinate of the position of the principal ray of the light beam on the scanning surface is expressed as a function of the deflection angle θ. When this function's differential function dy/dθ increases in absolute value according to the absolute value of the deflection angle θ, and the ratio of the deflection angle to the maximum absolute value of the deflection angle θ is r, the differential function dy/dθ is
-1 ≦ r ≦ -0.4 and
0.4 ≦ r ≦ 1
A scanning optical system having a plurality of inflection points in each range. The scanning optical system of claim 1, wherein the direction of the optical axis is the z-axis direction, the refractive power of the first scanning lens in the y-z cross section is positive for light rays passing near the optical axis, decreases according to the absolute value of the y coordinate of the position where the light rays pass, and is negative for light rays passing through the peripheral portion in the y-axis direction, and the refractive power of the second scanning lens in the y-z cross section is negative for light rays passing near the optical axis, increases according to the absolute value of the y coordinate of the position where the light rays pass, and is positive for light rays passing through the peripheral portion in the y-axis direction. A scanning optical system as described in claim 1, wherein the value of (|dy/dθ| - f)/f is -3% or less when the deflection angle θ is 0, and 5% or more when the absolute value of the deflection angle θ is at its maximum value.

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