Scanning optical system

Abstract

A scanning optical system has an object side lens unit for condensing light from an object, a mirror for performing a main scan to read the image of the object by deflecting the light transmitted through the object side lens and an image side lens unit for forming an image on the image sensing surface using both the extra-axial light and axial light in a subscan direction deflected by the mirror. The scanning optical system satisfies the predetermined condition defined by lenses of Abbe number.

Description

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is based on Patent Application No. 11-72910 filed in Japan, the content of which is hereby incorporated by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a scanning optical system, for example a scanning optical system used in a film scanner or the like capable of high-speed image retrieval.

2. Description of the Related Art

Various scanning optical systems have been proposed for use in film scanners and the like. Among the proposed systems for high-speed, high-precision image retrieval is a scanning optical system for forming a film image on a unidimensional linear image sensing element (e.g., a line CCD) having an array of photoreceptor elements arranged in a subscan direction via a mirror rotated in a main scan direction to read an object. scanning optical systems suitable for this type of mirror scanning optical system have been disclosed in Japanese Laid-Open Patent Application Nos. 9-236741, 9-236747, 9-236766, and 9-236767.

The scanning optical systems disclosed in these patents use a color separation prism to accomplish so-called 3-panel color separation of color images, and therefore are disadvantageously expensive. Conventionally, in order to reduce cost while maintaining high resolution, it has been thought most effective to eliminate the color separation prism while using a tri-linear image sensing element having the aforesaid unidimensional line image sensing element arrayed in three lines in the main scan direction.

When the aforesaid tri-linear image sensing element is used, however, it becomes necessary not only to correct magnification chromatic aberration, but also axial chromatic aberration which is not a problem in optical systems using the color separation prism. That is, identical focusing is required on the three line image sensing elements on the same surface. When scanning via a mirror, severe disadvantages arise in the scanning optical system from the perspective of the various types of aberration generated, e.g., chromatic aberration, coma and the like.

SUMMARY OF THE INVENTION

In view of the previously mentioned disadvantages, an object of the present invention is to provide a high performance scanning optical system at low cost which specifically corrects magnification chromatic aberration and axial chromatic aberration without using a color separation prism, and is not susceptible to performance deterioration when scanning via a mirror.

These objects are attained by a scanning optical system having, an object side lens unit for condensing light from an object, a mirror for performing a main scan to read the image of the object by deflecting the light transmitted through the object side lens; and an image side lens unit for forming an image on the image sensing surface using both the axial light and extra-axial light in a subscan direction deflected by the mirror; and wherein the following condition is satisfied.

0.1<|(Σν fp−Σνfm )/ Lf |<20.0

Where Σνfp represents the sum of the Abbe numbers of the positive optical power lenses within the object side lens unit, Σνfm represents the sum of the Abbe numbers of the negative optical power lenses within the object side lens unit, and Lf represents the number of lenses in the object side lens unit.

BRIEF DESCRIPTION OF THE DRAWINGS

These and other objects and features of this invention will become clear from the following description, taken in conjunction with the preferred embodiments with reference to the accompanying drawings, in which:

FIG. 1 is a construction of the scanning optical systems of the first embodiment (the angle θ=45°);

FIG. 2 is a construction of the scanning optical systems of the first embodiment (the angle θ=45°−6.1°);

FIG. 3 is a construction of the scanning optical systems of the second embodiment (the angle θ=45°);

FIG. 4 is a construction of the scanning optical systems of the second embodiment (the angle θ=45°−6.1°);

FIG. 5 is a construction of the scanning optical systems of the third embodiment (the angle θ=45°);

FIG. 6 is a construction of the scanning optical systems of the third embodiment (the angle θ=45°−6.1°);

FIG. 7 is a construction of the scanning optical systems of the fourth embodiment (the angle θ=45°);

FIG. 8 is a construction of the scanning optical systems of the fourth embodiment (the angle θ=45°−6.1°);

FIG. 9 is a construction of the scanning optical systems of the fifth embodiment (the angle θ=45°);

FIG. 10 is a construction of the scanning optical systems of the fifth embodiment (the angle θ 32 45°−6.1°);

FIG. 11 is an aberration diagram of the first embodiment, FIG. 11A shows spherical aberration diagram, FIG. 11B shows astigmatism and FIG. 11C shows distortion;

FIG. 12 is an aberration diagram of the second embodiment, FIG. 12A shows spherical aberration diagram. FIG. 12B shows astigmatism and FIG. 12C shows distortion;

FIG. 13 is an aberration diagram of the third embodiment, FIG. 13A shows spherical aberration diagram, FIG. 13B shows astigmatism and FIG. 13C shows distortion;

FIG. 14 is an aberration diagram of the fourth embodiment, FIG. 14A shows spherical aberration diagram, FIG. 14B shows astigmatism and FIG. 14C shows distortion; and

FIG. 15 is an aberration diagram of the fifth embodiment, FIG. 15A shows spherical aberration diagram, FIG. 15B shows astigmatism and FIG. 15C shows distortion.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

The preferred embodiments of the present invention are described hereinafter with reference to the accompanying drawings. FIGS. 1 and 2 , FIGS. 3 and 4 , FIGS. 5 and 6 , FIGS. 7 and 8 , FIGS. 9 and 10 respectively show the constructions of the scanning optical systems of the first through fifth embodiments. In the drawings, the x-axis, y-axis, and z-axis are shown mutually perpendicular one to another: the drawing surface is designated the x-y plane, and the z-axis is perpendicular to the drawing surface toward the foot of the drawing. These scanning optical systems are of a mirror scanning type comprising sequentially from the image side an image side lens unit Gr 1 , stop S, mirror M, and object side lens unit Gr 2 .

A film screen not shown in the drawing is arranged as an object at a stationary position within the image sensing range on the object side of the scanning optical system, (i.e., the left side of lens unit Gr 2 in each drawing), and a tri-linear image sensing element 1 is arranged as an image sensing surface on the image side of the scanning optical system, (i.e., the bottom side of the lens unit Gr 1 in each drawing). The tri-linear image sensing element 1 is disposed with the z-axis direction (subscan direction) designated as the lengthwise direction, and the unidimensional line image sensing elements are arranged in three lines in the x-axis direction (main scan direction) (details not shown in the drawings).

The light from the film screen condensed by the object side lens unit Gr 2 is deflected by the mirror M, and the axial light and extra-axial light in the subscan direction both form an image on the tri-linear image forming element 1 via the image side lens unit Gr 1 . The image side lens unit Gr 1 and the object side lens unit Gr 2 comprise rotationally symmetrical spherical surface lenses, and have a symmetrical type construction advantageous in aberration correction via the mirror M.

FIGS. 1 , 3 , 5 , 7 , and 9 show the optical path L at a rotational angle relative to the Y-axis of the mirror M, i.e., the mirror oscillation angle, of θ=45°. The angle range of θ=45°±6.1° centered on the mirror oscillation angle of θ=45° becomes the main scanning range. FIGS. 2 , 4 , 6 , 8 , and 10 show the optical path La at a mirror oscillation angle of θ=45°−6.1°. The angle range of θ=45°±6.1° centered on the mirror oscillation angle of θ=45° becomes the main scanning range. Although the optical path has been omitted at θ=45°+6.1°, the optical path through the object side lens unit Gr 2 at this time is approximately symmetrical to the optical axis X in FIGS. 1 , 3 , 5 , 7 , 9 relative to the optical path shown in FIGS. 2 , 4 , 6 , 8 , 10 .

In the first embodiment shown in FIGS. 1 and 2 , the object side lens unit Gr 2 comprises sequentially from the object side ten lens elements G 1 ˜G 10 along the optical axis X, and the image side lens unit Gr 1 comprises sequentially from the object side six lens elements G 11 ˜G 16 along the optical axis Y. The object side lens unit Gr 2 can be understood as comprising sequentially from the object side an object side front lens unit Gr 2 - 1 and an object side back lens unit Gr 2 - 2 arranged with a relatively large spacing therebetween. The object side front lens unit Gr 2 - 1 is a cemented lens comprising two lens elements G 1 and G 2 , and the object side back lens unit Gr 2 - 2 comprises eight lens elements G 3 ˜G 10 .

In the second embodiment shown in FIGS. 3 and 4 , the object side lens unit Gr 2 comprises sequentially from the object side nine lens elements G 1 ˜G 9 along the optical axis X, and the image side lens unit Gr 1 comprises sequentially from the object side six lens elements G 10 ˜G 15 along the optical axis Y. The object side lens unit Gr 2 can be understood as comprising sequentially from the object side an object side front lens unit Gr 2 - 1 and an object side back lens unit Gr 2 - 2 arranged with a relatively large spacing therebetween. The object side front lens unit Gr 2 - 1 is a cemented lens comprising two lens elements G 1 and G 2 , and the object side back lens unit Gr 2 - 2 comprises seven lens elements G 3 ˜G 9 .

In the third embodiment shown in FIGS. 5 and 6 , the object side lens unit Gr 2 comprises sequentially from the object side nine lens elements G 1 ˜G 9 along the optical axis X, and the image side lens unit Gr 1 comprises sequentially from the object side six lens elements G 10 ˜G 15 along the optical axis Y. The object side lens unit Gr 2 can be understood as comprising sequentially from the object side an object side front lens unit Gr 2 - 1 and an object side back lens unit Gr 2 - 2 arranged with a relatively large spacing therebetween. The object side front lens unit Gr 2 - 1 is a cemented lens comprising two lens elements G 1 and G 2 , and the object side back lens unit Gr 2 - 2 comprises seven lens elements G 3 ˜G 9 .

In the fourth embodiment shown in FIGS. 7 and 8 , the object side lens unit Gr 2 comprises sequentially from the object side eight lens elements G 1 ˜G 8 along the optical axis X, and the image side lens unit Gr 1 comprises sequentially from the object side six lens elements G 9 ˜G 14 along the optical axis Y. The object side lens unit Gr 2 can be understood as comprising sequentially from the object side an object side front lens unit Gr 2 - 1 and an object side back lens unit Gr 2 - 2 arranged with a relatively large spacing therebetween. The object side front lens unit Gr 2 - 1 is a cemented lens comprising two lens elements G 1 and G 2 , and the object side back lens unit Gr 2 - 2 comprises six lens elements G 3 ˜G 8 .

In the fifth embodiment shown in FIGS. 9 and 10 , the object side lens unit Gr 2 comprises sequentially from the object side seven lens elements G 1 ˜G 7 along the optical axis X, and the image side lens unit Gr 1 comprises sequentially from the object side five lens elements G 8 ˜G 2 along the optical axis Y. The object side lens unit Gr 2 can be understood as comprising sequentially from the object side an object side front lens unit Gr 2 - 1 and an object side back lens unit Gr 2 - 2 arranged with a relatively large spacing therebetween. The object side front lens unit Gr 2 - 1 is a cemented lens comprising two lens elements G 1 and G 2 , and the object side back lens unit Gr 2 - 2 comprises five lens elements G 3 ˜G 7 .

Desirable conditions for the scanning optical system are described below. In scanning optical systems comprising an object side lens unit for condensing light from an object, a mirror for performing a main scan to read the image of the object by deflecting the light transmitted through the object side lens, and an image side lens unit for forming an image on the image sensing surface using both the extra-axial light and axial light in a subscan direction deflected by the mirror, such as in the previously described embodiments, magnification chromatic aberration is generated by mirror scanning. In order to reduce this chromatic aberration, the chromatic aberration of each lens unit must be preset at a desirable state. Furthermore, it is desirable to accomplish aberration correction by negating each aberration via the respective lens units by correcting the aberration generated by the object side lens unit via the image side lens unit.

In the scanning optical systems of the above mentioned embodiments, it is desirable that the object side lens unit satisfies condition (1) below. When the following condition is satisfied, excellent chromatic aberration correction can be achieved, and a high-performance optical system can be realized:

0.1<|(Σν fp−Σνfm )/ Lf |<20.0  (1)

where Σvfp represents the sum of the Abbe numbers of the positive optical power lenses within the object side lens unit, Σvfm represents the sum of the Abbe numbers of the negative optical power lenses within the object side lens unit, and Lf represents the number of lenses in the object side lens unit.

Chromatic aberration generated within the object side lens unit can be reduced, and particularly a reduction of axial chromatic aberration is achieved in the complete optical system by satisfying the above conditions. When the upper limit of condition (1) is exceeded, chromatic aberration generated by the positive optical power lens elements within the object side lens unit is particularly increased, so as to make it difficult to correct the chromatic aberration generated by the object side lens unit via the image side lens unit. Conversely, when the lower limit of condition (1) is exceeded, chromatic aberration generated by the negative optical power lens elements within the object side lens unit is particularly increased, so as to make it difficult to correct the chromatic aberration generated by the object side lens unit via the image side lens unit.

In the scanning optical systems of each of the previously mentioned embodiments, it is desirable that the image side lens unit satisfies condition (2) below:

10.0<|(Σν rp−Σνrm )/ Lr |<50.0  (2)

where Σvrp represents the sum of the Abbe numbers of the positive optical power lenses within the image side lens unit, Σvrm represents the sum of the Abbe numbers of the negative optical power lenses within the image side lens unit, and Lr represents the number of lenses in the image side lens unit.

Chromatic aberration generated by the object side lens unit can be corrected by the image side lens unit, and a high-performance optical system can be realized by satisfying the above condition. When the upper limit of condition (2) is exceeded, chromatic aberration generated by the positive optical power lens elements within the image side lens unit is particularly increased, so as to make it difficult to correct the chromatic aberration generated by the object side lens unit via the image side lens unit. Conversely, when the lower limit of condition (2) is exceeded, chromatic aberration generated by the negative optical power lens elements within the image side lens unit is particularly increased, so as to make it difficult to correct the chromatic aberration generated by the object side lens unit via the image side lens unit.

Although it is desirable to correct the chromatic aberration of the total optical system by correcting the chromatic aberration generated by the object side lens unit via the image side lens unit, if the chromatic aberration of each lens unit is becomes too large, an undesirable effect is that magnification chromatic aberration becomes particularly large when scanning via a mirror. In correspondence therewith, the previously mentioned conditions aim not only to reduce axial chromatic aberration, but also to reduce magnification chromatic aberration generated during mirror scanning.

In the scanning optical systems of each of the previously mentioned embodiments, it is desirable that the cemented lens comprises a negative lens element and a positive lens element on the outermost object side. In this way, it is possible to achieve excellent correction of magnification chromatic aberration, particularly extra-axial magnification chromatic aberration. It is further desirable that the cemented lens on the outermost object side within the object side lens unit satisfies condition (3) below:

|(φ f− 1)/φ f|< 1.0  (3)

where φf−1 represents the optical power of the cemented lens on the outermost object side within the object side lens unit, and φf represents the optical power of the object side lens unit.

Condition (3) is a condition for correcting chromatic aberration, and particularly extra-axial aberration, via the cemented lens on the outermost object side within the object side lens unit. When the upper limit of condition (3) is exceeded, it becomes difficult to correct the various types of aberration such as magnification chromatic aberration and extra-axial aberration generated by the lens elements.

In the scanning optical systems of each of the aforementioned embodiments, it is desirable that the object side lens unit comprises sequentially from the object side an object side front lens unit and an object side back lens unit disposed with a relatively large space therebetween. In this way, a difference is created in the ray height of the paraxial marginal ray between the outermost image side lens element of the object side front lens unit and the outermost object side lens element of the object side back lens unit, which is greatly effective in correcting the extra-axial aberration in particular.

It is desirable that the outermost image side lens element within the object side front lens unit and the outermost object side lens element within the object side back lens unit satisfy condition (4) below:

0.4<( Rf− 1 r )/( Rf− 2 f )<5.0  (4)

where Rf−1r represents the radius of curvature of the image side surface of the outermost image side lens element within the object side front lens unit, and Rf−2f represents the radius of curvature of the object side surface of the outermost object side lens element within the object side back lens unit.

Condition (4) is a condition for correcting various types of aberration, most importantly spherical aberration and extra-axial coma generated within the lens unit of the object side lens unit, and is a condition particularly for balancing the aberration generated by over-correction by the object side front lens unit by means of the image side lens element. When this condition is eliminated, the balance of aberration correction is adversely affected within the object side lens element, resulting in insufficient correction or over-correction of aberration, and undesirably generating high order aberration in particular.

It is desirable that the object side lens unit satisfies condition (5) below:

0.05<( Tf− 12)×φ f< 0.4  (5)

where Tf−12 represents the distance between the object side front lens unit and the object side back lens unit, and φf represents the optical power of the object side lens unit.

Condition (5) relates to the spacing between the object side front lens unit and the object side back lens unit, and from aberration theory is greatly effective in correcting the extra-axial aberration in particular by creating a difference in the ray height of the paraxial marginal ray between the object side front lens unit and the object side back lens unit. When the lower limit of condition (5) is exceeded, sufficient difference in ray height of the paraxial marginal ray cannot be obtained. Conversely, when the upper limit is exceeded, the total length of the object side lens unit is increased, so as to undesirably increase the space required by the optical system.

In the scanning optical system of the previously mentioned embodiments, it is desirable that the exit pupil of the object side lens unit approximately matches the entrance pupil of the image side lens unit. For this reason, it is desirable to provide a common stop for both the object side lens unit and the image side lens unit near the mirror used for scanning.

The object side lens unit desirably possesses at least one negative lens element for chromatic aberration correction, spherical aberration correction, and Petzval sum correction. In this way, the height of the pass-through ray is increased so as to effectively correct spherical aberration. Furthermore, the height of the extra-axial light passing through the lens is also increased, which is advantageous in correcting extra-axial aberration.

It is desirable that the extra-axial luminous flux heightened at the lens passage position nearly matches the passage position near the stop position, and to achieve this end, it is desirable that the outermost image side lens element within the object side lens unit has a concave surface on the image side, and it is particularly desirable that this lens element having a concave meniscus shape on the image side. In this way, extra-axial aperture efficiency is maintained, and mirror used for the main scan can be made more compact.

It is desirable that the negative lens of the image side lens unit satisfies condition (6) below:

νrm<35.0  (6)

where νrm represents the Abbe number of the negative lens in the image side lens unit. Condition (6) is a condition for obtaining a desired chromatic aberration generated within the image side lens unit. When the range of condition (6) is omitted, it becomes difficult to correct the aberration generated by the positive lens element within the image side lens unit via the negative lens element.

When considering aberration correction of the entire optical system, it is necessary to balance the respective aberrations generated by the object side lens unit and the image side lens unit. Although it is desirable that the negative lens element in the object side lens unit have a relatively large optical power to correct chromatic aberration, spherical aberration, and extra-axial aberration, the large optical power generates negative aberration. In order to correct this aberration in the negative direction, it is desirable that the surface of the outermost object side lens element within the image side lens unit is a positive lens element having a convex shape on the object side. In this way, the pass-through position of the extra-axial luminous flux from the object side lens unit can be reduced in the lens element following the image side lens unit, so as to have a more compact lens diameter.

It is further desirable that the surface of the lens element on the outermost image side in the image side lens unit is a concave surface on the image side. In this way, extra-axial aberration, and particularly distortion, can be corrected in a desired direction.

The construction of the photographic optical system of the present invention is described below by way of specific examples of construction data and aberration diagrams. The optical systems of examples 1˜5 respectively correspond to the optical systems of the first through fifth embodiments. The structural diagrams ( FIGS. 1 and 2 , FIGS. 3 and 4 , FIGS. 5 and 6 , FIGS. 7 and 8 , FIGS. 9 and 10 ) representing the scanning optical systems of the first through fifth embodiments respectively show the construction of the corresponding optical systems of examples 1˜5.

In each example, ri (i=1, 2, 3 . . . ) represents the No. i surface and the radius of curvature of the No. i surface counting from the object side, di (i=1, 2, 3 . . . ) represents the axial distance of the No. i surface counting from the object side, Gi (i=1, 2, 3 . . . ) represents the No. i lens element counting from the object side, Ni (i=1, 2, 3) and vi (i=1, 2, 3 . . . ) respectively represent the d-line refractive index and Abbe number of the No. i lens element counting from the object side.

EXAMPLE 1

Object distance:	60 mm
Effective F. No.:	5.0
Mirror oscillation angle:	±6.1 degrees
[Radius of Curvature]	[Axial Distance]	[Lens]	[Refractive Index]	[Abbe Number]
r1 = 91.255	d1 = 9.00	G1	N1 = 1.75450	ν1 = 51.57
r2 = −197.911	d2 = 2.50	G2	N2 = 1.67339	ν2 = 29.25
r3 = 49.624	d3 = 22.89
r4 = 73.094	d4 = 12.00	G3	N3 = 1.61800	ν3 = 63.39
r5 = −56.042	d5 = 1.50
r6 = −53.916	d6 = 4.00	G4	N4 = 1.67339	ν4 = 29.25
r7 = 43.252	d7 = 2.00
r8 = 52.205	d8 = 10.49	G5	N5 = 1.83350	ν5 = 21.00
r9 = −59.216	d9 = 1.00
r10 = −59.339	d10 = 2.50	G6	N6 = 1.67339	ν6 = 29.25
r11 = 295.777	d11 = 1.00
r12 = 33.245	d12 = 9.85	G7	N7 = 1.61800	ν7 = 63.39
r13 = −131.394	d13 = 2.00
r14 = −116.242	d14 = 2.50	G8	N8 = 1.74000	ν8 = 31.72
r15 = 28.824	d15 = 2.00
r16 = 27.762	d16 = 4.76	G9	N9 = 1.78831	ν9 = 47.32
r17 = 110.880	d17 = 1.00
r18 = 24.041	d18 = 2.00	G10	N10 = 1.74000	ν10 = 31.72
r19 = 16.756	d19 = 30.00
r20 = ∞ (Mirror M)	d20 = 13.00
r21 = ∞ (Stop S)	d21 = 4.50
r22 = 21.064	d22 = 2.50	G11	N11 = 1.83350	ν11 = 21.00
r23 = 30.406	d23 = 5.68
r24 = 103.496	d24 = 3.00	G12	N12 = 1.61800	ν12 = 63.39
r25 = −21.355	d25 = 1.50
r26 = −17.416	d26 = 4.00	G13	N13 = 1.67339	ν13 = 29.25
r27 = 23.035	d27 = 2.00
r28 = 17.575	d28 = 6.00	G14	N14 = 1.48749	ν14 = 70.44
r29 = 17.480	d29 = 1.91
r30 = 38.082	d30 = 6.00	G15	N15 = 1.61800	ν15 = 63.39
r31 = −42.455	d31 = 14.74
r32 = 18.131	d32 = 6.00	G16	N16 = 1.83350	ν16 = 21.00
r33 = 15.603

EXAMPLE 2

Object distance:	60 mm
Effective F. No.:	5.0
Mirror oscillation angle:	±6.1 degrees
[Radius of Curvature]	[Axial Distance]	[Lens]	[Refractive Index]	[Abbe Number]
r1 = −240.881	d1 = 5.00	G1	N1 = 1.67339	ν1 = 29.25
r2 = 48.112	d2 = 10.98	G2	N2 = 1.61800	ν2 = 63.39
r3 = −51.267	d3 = 18.72
r4 = −34.071	d4 = 5.00	G3	N3 = 1.67339	ν3 = 29.25
r5 = 49.737	d5 = 1.71
r6 = 69.807	d6 = 8.86	G4	N4 = 1.83350	ν4 = 21.00
r7 = −42.348	d7 = 0.50
r8 = −52.992	d8 = 2.00	G5	N5 = 1.67339	ν5 = 29.25
r9 = −97.001	d9 = 0.50
r10 = 43.391	d10 = 9.07	G6	N6 = 1.61800	ν6 = 63.39
r11 = −57.547	d11 = 0.50
r12 = −69.091	d12 = 2.00	G7	N7 = 1.74000	ν7 = 31.72
r13 = 175.888	d13 = 0.50
r14 = 32.474	d14 = 5.27	G8	N8 = 1.78831	ν8 = 47.32
r15 = −340.116	d15 = 2.00	G9	N9 = 1.74000	ν9 = 31.72
r16 = 22.354	d16 = 30.00
r17 = ∞ (Mirror M)	d17 = 13.00
r18 = ∞ (Stop S)	d18 = 4.50
r19 = 13.417	d19 = 4.00	G10	N10 = 1.83350	ν10 = 21.00
r20 = 12.250	d20 = 5.88
r21 = 15.255	d21 = 3.00	G11	N11 = 1.61800	ν11 = 63.39
r22 = −103.932	d22 = 1.50
r23 = −27.710	d23 = 4.00	G12	N12 = 1.67339	ν12 = 29.25
r24 = 13.714	d24 = 2.00
r25 = 16.057	d25 = 6.00	G13	N13 = 1.48749	ν13 = 70.44
r26 = 21.020	d26 = 1.00
r27 = 100.722	d27 = 4.00	G14	N14 = 1.61800	ν14 = 63.39
r28 = −45.399	d28 = 8.06
r29 = 26.041	d29 = 6.00	G15	N15 = 1.83350	ν15 = 21.00
r30 = 36.220

EXAMPLE 3

Object distance:	60 mm
Effective F. No.:	5.0
Mirror oscillation angle:	±6.1 degrees
[Radius of Curvature]	[Axial Distance]	[Lens]	[Refractive Index]	[Abbe Number]
r1 = −202.859	d1 = 5.00	G1	N1 = 1.67339	ν1 = 29.25
r2 = 68.971	d2 = 15.00	G2	N2 = 1.61800	ν2 = 63.39
r3 = −50.708	d3 = 18.90
r4 = −38.535	d4 = 5.00	G3	N3 = 1.67339	ν3 = 29.25
r5 = 43.944	d5 = 16.65	G4	N4 = 1.83350	ν4 = 21.00
r6 = −67.607	d6 = 0.57
r7 = −87.488	d7 = 5.93	G5	N5 = 1.67339	ν5 = 29.25
r8 = −193.041	d8 = 0.50
r9 = 57.498	d9 = 10.80	G6	N6 = 1.61800	ν6 = 63.39
r10 = −43.765	d10 = 2.00	G7	N7 = 1.74000	ν7 = 31.72
r11 = −473.216	d11 = 0.50
r12 = 28.465	d12 = 7.06	G8	N8 = 1.78831	ν8 = 47.32
r13 = 2190.149	d13 = 2.13	G9	N9 = 1.74000	ν9 = 31.72
r14 = 19.784	d14 = 30.00
r15 = ∞ (Mirror M)	d15 = 13.00
r16 = ∞ (Stop S)	d16 = 4.50
r17 = 20.435	d17 = 4.00	G10	N10 = 1.83350	ν10 = 21.00
r18 = 28.301	d18 = 4.95
r19 = 23.548	d19 = 3.45	G11	N11 = 1.61800	ν11 = 63.39
r20 = −36.096	d20 = 1.50
r21 = −25.425	d21 = 2.00	G12	N12 = 1.67339	ν12 = 29.25
r22 = 13.784	d22 = 1.50
r23 = 14.186	d23 = 6.00	G13	N13 = 1.48749	ν13 = 70.44
r24 = 15.802	d24 = 10.90
r25 = 34.838	d25 = 5.00	G14	N14 = 1.61800	ν14 = 63.39
r26 = −128.323	d26 = 1.68
r27 = 23.872	d27 = 6.00	G15	N15 = 1.83350	ν15 = 21.00
r28 = 21.263

EXAMPLE 4

Object distance:	60 mm
Effective F. No.:	5.0
Mirror oscillation angle:	±6.1 degrees
[Radius of Curvature]	[Axial Distance]	[Lens]	[Refractive Index]	[Abbe Number]
r1 = −202.555	d1 = 5.00	G1	N1 = 1.67339	ν1 = 29.25
r2 = 80.484	d2 = 15.00	G2	N2 = 1.61800	ν2 = 63.39
r3 = −44.412	d3 = 10.70
r4 = −34.397	d4 = 5.00	G3	N3 = 1.74000	ν3 = 31.72
r5 = 47.267	d5 = 20.00	G4	N4 = 1.83350	ν4 = 21.00
r6 = −111.845	d6 = 0.95
r7 = 70.466	d7 = 11.00	G5	N5 = 1.61800	ν5 = 63.39
r8 = −43.286	d8 = 2.00	G6	N6 = 1.74000	ν6 = 31.72
r9 = −107.883	d9 = 0.50
r10 = 30.328	d10 = 9.00	G7	N7 = 1.78831	ν7 = 47.32
r11 = 759.423	d11 = 2.00	G8	N8 = 1.74000	ν8 = 31.72
r12 = 20.24	d12 = 30.00
r13 = ∞ (Mirror M)	d13 = 13.00
r14 = ∞ (Stop S)	d14 = 4.50
r15 = 19.553	d15 = 4.00	G9	N9 = 1.83350	ν9 = 21.00
r16 = 25.954	d16 = 3.49
r17 = 19.469	d17 = 3.00	G10	N10 = 1.61800	ν10 = 63.39
r18 = −56.217	d18 = 1.50
r19 = −35.333	d19 = 2.67	G11	N11 = 1.67339	ν11 = 29.25
r20 = 11.612	d20 = 1.50
r21 = 12.549	d21 = 6.00	G12	N12 = 1.48749	ν12 = 70.44
r22 = 14.527	d22 = 6.72
r23 = 39.772	d23 = 3.00	G13	N13 = 1.61800	ν13 = 63.39
r24 = −180.197	d24 = 6.47
r25 = 18.515	d25 = 3.00	G14	N14 = 1.83350	ν14 = 21.00
r26 = 19.184

EXAMPLE 5

Object distance:	60 mm
Effective F. No.:	5.0
Mirror oscillation angle:	±6.1 degrees
[Radius of Curvature]	[Axial Distance]	[Lens]	[Refractive Index]	[Abbe Number]
r1 = −4116.921	d1 = 2.00	G1	N1 = 1.83350	ν1 = 21.00
r2 = 30.233	d2 = 11.78	G2	N2 = 1.61800	ν2 = 63.39
r3 = −128.331	d3 = 7.00
r4 = −37.813	d4 = 5.00	G3	N3 = 1.74000	ν3 = 31.72
r5 = 90.115	d5 = 12.14	G4	N4 = 1.83350	ν4 = 21.00
r6 = −54.53	d6 = 0.50
r7 = 48.656	d7 = 15.00	G5	N5 = 1.61800	ν5 = 63.39
r8 = −64.370	d8 = 3.26	G6	N6 = 1.74000	ν6 = 31.72
r9 = −218.994	d9 = 0.88
r10 = 25.751	d10 = 8.00	G7	N7 = 1.83350	ν7 = 21.00
r11 = 18.652	d11 = 30.00
r12 = ∞ (Mirror M)	d12 = 13.00
r13 = ∞ (Stop S)	d13 = 4.50
r14 = 22.510	d14 = 8.00	G8	N8 = 1.61800	ν8 = 63.39
r15 = −44.563	d15 = 2.61
r16 = −29.747	d16 = 5.00	G9	N9 = 1.84666	ν9 = 23.82
r17 = 23.336	d17 = 12.33
r18 = 94.078	d18 = 4.00	G10	N10 = 1.83350	ν10 = 21.00
r19 = −36.841	d19 = 12.75
r20 = 26.392	d20 = 5.42	G11	N11 = 1.61800	ν11 = 63.39
r21 = −32.560	d21 = 0.60
r22 = −30.487	d22 = 6.00	G12	N12 = 1.75000	ν12 = 25.14
r23 = 23.340

FIGS. 11-15 are aberration diagrams corresponding to the optical systems of examples 1˜5, respectively. In the spherical aberration diagrams, the solid line represents spherical aberration on the C-line, the small dash line represents spherical aberration on the d-line, the dash-dot line represents spherical aberration on the f-line, and the large dash line represents spherical aberration on the g-line. In the astigmatism diagrams, the small dash line S and the large dash line M respectively represent astigmatism on the sagittal plane and meridional plane at the d-line. The distortion diagrams show distortion on the d-line. Conditions (1)˜(6) are satisfied in the optical systems of examples 1˜5. Numerical values of conditions (1)˜(6) in each example 1˜5 are given below.

	Ex. 1	Ex. 2	Ex. 3	Ex. 4	Ex. 5
	|(Σνfp − Σνfm)/Lf|	9.55	4.88	4.88	14.90	2.33
	|(Σνrp − Σνrm)/Lr|	35.00	35.00	35.00	35.00	16.47
	|φf − 1/φf|	0.347	0.711	0.721	0.880	0.188
	Rf − 1r/Rf − 2f	0.679	1.505	1.316	1.291	3.394
	Tf − 12 × φf	0.275	0.224	0.227	0.128	0.084
	νrm	29.25	29.25	29.25	29.25	23.82

Examples of public disclosure of the previously mentioned conventional art include values of conditions (1)˜(6) listed below in the optical systems of examples 1˜3 disclosed in Japanese Laid-Open Patent No. 9-236741. It will be understood that these values do not necessarily satisfy the conditional range.

	Ex. 1	Ex. 2	Ex. 3
	|(Σνfp − Σνfm)/Lf|	23.96	23.10	28.74
	|(Σνrp − Σνrm)/Lr|	17.56	17.38	24.48
	|φf − 1/φf|	0.583	0.988	1.320
	Rf − 1r/Rf − 2f	1.111	1.633	−1.340
	Tf − 12 × φf	−0.583	0.030	0.100
	νrm	57.07	57.07	27.51

As described above, the present invention provides a high-performance scanning optical system at low cost, which specifically corrects magnification chromatic aberration and axial chromatic aberration without using a color separation prism, and is not susceptible to performance deterioration when scanning via a mirror.

The present invention specifically reduces chromatic aberration generated within an object side lens unit, and reduces axial chromatic aberration of the total optical system.

Although the present invention has been fully described by way of examples with reference to the accompanying drawings, it is to be noted that various changes and modification will be apparent to those skilled in the art. Therefore, unless otherwise such changes and modifications depart from the scope of the present invention, they should be construed as being included therein.

Claims

1. A scanning optical system for imaging an object, comprising:an object side lens unit for receiving light having a plurality of color components from an object; a mirror for performing a main scan by deflecting the light transmitted through the object side lens unit, the mirror having a reflecting surface including a rotational axis on the reflecting surface; and an image side lens unit for forming an image on an image sensing surface, said image sensing surface for receiving an image having a plurality of color components, using both the extra-axial light and axial light in a subscan direction deflected by the mirror; wherein the following condition is satisfied: 0.1<|(Σνfp−Σνfm)/Lf|<15 where Σνfp represents the sum of the Abbe numbers of the positive optical power lenses within the object side lens unit, Σνfm represents the sum of the Abbe numbers of the negative optical power lenses within the object side lens unit, and Lf represents the number of lenses in the object side lens unit.

2. The scanning optical system according to claim 1, wherein the following condition is satisfied:10.0<|(Σνrp−Σνrm)/Lr|<50.0 where Σνrp represents the sum of the Abbe numbers of the positive optical power lenses within the image side lens unit, Σνrp represents the sum of the Abbe numbers of the negative optical power lenses within the image side lens unit, and Lr represents the number of lenses in the image side lens unit.

3. The scanning optical system according to claim 1, wherein the object side lens unit includes a cemented lens comprising a negative lens element and a positive lens element.

4. The scanning optical system according to claim 3, wherein the cemented lens satisfies the following condition:|(φf−1)/φf|<1.0 where φf−1 represents the optical power of the cemented lens within the object side lens unit, and φf represents the optical power of the object side lens unit.

5. The scanning optical system according to claim 1, wherein the object side lens unit comprises, sequentially from the object side, an object side front lens unit and an object side back lens unit arranged with a relatively large spacing therebetween.

6. The scanning optical system according to claim 5, wherein the outermost image side lens element within the object side front lens unit and the outermost object side lens element within the object side back lens unit satisfy the following condition:0.4<(Rf−1r)/(Rf−2f)<5.0 where Rf−1r represents the radius of curvature of the image side surface of the outermost image side lens element within the object side front lens unit, and Rf−2f represents the radius of curvature of the object side surface of the outermost object side lens element within the object side back lens unit.

7. The scanning optical system according to claim 5, wherein the object side front lens unit satisfies the following condition:0.05<(Tf−12)×φf<0.4 where Tf−12 represents the distance between the object side front lens unit and the object side back lens unit, and φf represents the optical power of the object side lens unit.

8. The scanning optical system according to claim 3, wherein the cemented lens is arranged at the outermost object side of the object side lens unit.

9. The scanning optical system according to claim 8, wherein the positive lens element of the cemented lens is arranged at the outermost object side of the object side lens unit.

10. The scanning optical system according to claim 1, wherein the following condition is satisfied:νrm<35.0 where νrm represents the Abbe number of a negative lens in the image side lens unit.