JP2016095541A - Wide-angle lens and imaging device - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a compact wide-angle lens of high resolution that is composed of four to six lenses.SOLUTION: A photographing lens 10 comprises, arranged in order from an object side to an image side: a first group lens 11 having negative power; a second group lens 12 having positive power; a third group lens 13 having negative power; and a fourth group lens 14 having positive power. When focal length of an entire lens system is denoted by f and focal length of the second group lens 12 is denoted ff2, 1.0≤ff2/f≤2.0 is satisfied, thereby overall length of the lens system can be shortened and curvature of an image face can be suppressed. Since respective lens surfaces on the object side of the second group lens 12, third group lens 13, and fourth group lens 14 and respective lens surfaces on the image side have an aspherical shape, the photographing lens 10 is configured to be a high brightness lens.SELECTED DRAWING: Figure 1

Description

  The present invention relates to a small, high-resolution wide-angle lens composed of four to six lenses and an image pickup apparatus equipped with the wide-angle lens.

  A wide-angle lens mounted on an in-vehicle camera or a surveillance camera is described in Patent Document 1. The wide-angle lens of this document includes a first lens with negative power, a second lens with positive power, a third lens with negative power, and a positive power, which are arranged in order from the object side to the image side. It consists of a 4th lens provided with. The wide-angle lens of this document has a diagonal field angle of about 65 °.

JP 2009-14947 A

  A wide-angle lens mounted on an imaging device such as an in-vehicle camera or a surveillance camera is required to be downsized, and with the increase in the number of pixels of the image sensor mounted on these imaging devices, higher resolution is achieved. Is required. Here, in order to improve the resolution of the wide-angle lens, it is necessary to suppress aberrations such as curvature of field as compared with the related art.

  In view of such a point, an object of the present invention is to provide a wide-angle lens having a small size and higher resolution. Another object of the present invention is to provide an imaging apparatus equipped with such a wide-angle lens.

In order to solve the above problems, the wide-angle lens of the present invention is
A first lens unit having a negative power, a second lens unit having a positive power, a third lens unit having a negative power, and a positive power, which are arranged in order from the object side to the image side. Consists of a fourth lens group
The first group lens is composed of one lens having negative power, or two lenses each having negative power,
The second group lens is composed of one lens having positive power, or two lenses each having positive power,
The third group lens is composed of one lens having negative power,
The fourth group lens is composed of one lens having positive power,
The lens constituting the first group lens has a concave shape on the image side lens surface,
The lens arranged adjacent to the third group lens in the second group lens has a convex shape on the image side lens surface,
The third lens group has a concave shape on the object side lens surface, a convex shape on the image side lens surface,
At least one of the lenses constituting the second group lens, the third group lens, and the fourth group lens has at least one of the object-side lens surface and the image-side lens surface being non-surface. It has a spherical shape,
When the focal length of the entire lens system is f, the focal length of the second lens group is ff2, and the focal length of the third lens group is ff3, the following conditional expressions (1) and (2) are satisfied. And
1.0 ≦ ff2 / f ≦ 2.0 (1)
-1.9 ≦ ff2 / ff3 ≦ −1.3 (2)

Since the wide-angle lens of the present invention satisfies the conditional expression (1), the overall length of the lens system can be kept short, and field curvature can be suppressed. Further, by providing the lenses constituting the second group lens, the third group lens, and the fourth group lens with an aspherical shape, it becomes easy to increase the aperture. Here, if the upper limit value of conditional expression (1) is exceeded, the curvature of field increases to the positive side, and correction thereof becomes difficult. If the lower limit of conditional expression (1) is exceeded, the curvature of field increases on the negative side, making correction difficult. If the upper limit of conditional expression (1) is exceeded, the positive power of the second lens group becomes relatively weak, making it difficult to keep the overall length of the lens system short. The wide-angle lens is an imaging lens having a diagonal field angle of 60 ° or more.
In addition, since the wide-angle lens of the present invention satisfies the conditional expression (2), as described below, chromatic aberration and curvature of field can be suppressed in a well-balanced manner, and the overall length of the lens system can be suppressed.

In the present invention, it is desirable that the following conditional expression (2) is satisfied when the focal length of the third lens group is ff3.
−2.0 ≦ ff2 / ff3 ≦ −1.0 (2)

  The upper limit value of conditional expression (2) is for suppressing chromatic aberration. When the upper limit value of conditional expression (2) is exceeded, the negative power of the third lens having a concave shape becomes too weak compared to the positive power of the second lens unit having a convex shape, so that chromatic aberration increases. The correction becomes difficult. Accordingly, the upper limit is set to −1.0 or less in order to suppress chromatic aberration. The lower limit value of the conditional expression (2) is for suppressing the curvature of field and the total length of the lens system. When the lower limit value of conditional expression (2) is exceeded, the negative power of the third lens having a concave shape becomes too strong with respect to the positive power of the second lens unit having a convex shape. Invite. Therefore, the lower limit is set to −2.0 or more in order to suppress the curvature of field. If the lower limit of conditional expression (2) is exceeded, the positive power of the second lens group becomes weaker than the negative power of the third lens group, so it is difficult to keep the entire length of the lens system short. . Here, by setting the range of conditional expression (2) to be −1.9 to −1.3, it is possible to balance chromatic aberration and curvature of field.

In the present invention, it is desirable that the following conditional expression (3) is satisfied when the focal length of the fourth lens group is ff4.
0.5 ≦ ff4 / f ≦ 2.0 (3)

  Conditional expression (3) is for suppressing curvature of field. That is, when the upper limit value of conditional expression (3) is exceeded, the curvature of field increases on the positive side, and correction thereof becomes difficult. If the lower and lower limit values of conditional expression (3) are exceeded, the curvature of field increases on the negative side, making correction difficult. Therefore, in order to further suppress the curvature of field, the range is set to 0.5 or more and 2.0 or less. Here, with respect to the conditional expression (3), the range of 0.7 or more and 1.7 or less can balance the image plane.

  In the present invention, in order to satisfactorily correct chromatic aberration, the second group lens includes a lens having an Abbe number of 40 or more, and the third group lens includes a lens having an Abbe number of 35 or less. It is desirable.

  In the present invention, a configuration with a diagonal angle of view of 100 ° or more can be employed. That is, field curvature can be suppressed even in such a wide-angle lens having a large angle of view.

  Next, an image pickup apparatus according to the present invention includes the above wide-angle lens and an image pickup element disposed at a focal position of the wide-angle lens.

  According to the present invention, since the wide-angle lens has a high resolution, the image pickup apparatus can have a high resolution by adopting an image pickup element having a large number of pixels as the image pickup element. In addition, since the overall length of the wide-angle lens can be shortened, the imaging device can be downsized.

  According to the wide-angle lens of the present invention, the entire length of the lens system can be suppressed to be short, and the occurrence of field curvature can be suppressed. Moreover, it is easy to increase the number of apertures.

It is a block diagram of the imaging lens of Example 1 to which the present invention is applied. FIG. 2 is an axial chromatic aberration diagram, lateral aberration diagram, field curvature diagram, and distortion diagram of the imaging lens of FIG. 1. It is a block diagram of the imaging lens of Example 2 to which the present invention is applied. FIG. 4 is a longitudinal chromatic aberration diagram, lateral aberration diagram, field curvature diagram, and distortion diagram of the imaging lens of FIG. 3. It is a block diagram of the imaging lens of Example 3 to which the present invention is applied. FIG. 6 is an on-axis chromatic aberration diagram, lateral aberration diagram, field curvature diagram, and distortion diagram of the imaging lens of FIG. 5. It is a block diagram of the imaging lens of Example 4 to which the present invention is applied. FIG. 8 is an on-axis chromatic aberration diagram, lateral aberration diagram, field curvature diagram, and distortion diagram of the imaging lens of FIG. 7. It is a block diagram of the imaging lens of Example 5 to which the present invention is applied. FIG. 9 is an on-axis chromatic aberration diagram, lateral aberration diagram, field curvature diagram, and distortion diagram of the imaging lens of FIG. 8. It is explanatory drawing of the imaging device carrying an imaging lens.

  An imaging lens to which the present invention is applied will be described below with reference to the drawings.

Example 1
FIG. 1 is a configuration diagram of the imaging lens of the first embodiment. As shown in FIG. 1, the imaging lens 10 includes a first group lens 11 having a negative power, a second group lens 12 having a positive power, and a negative power, which are arranged in order from the object side to the image side. And a fourth group lens 14 having positive power. The imaging lens 10 of this example is composed of four lenses, the first group lens 11 is composed of one first lens 111, and the second group lens 12 is composed of one second lens 121. The third group lens 13 is composed of one third lens 131, and the fourth group lens 14 is composed of one fourth lens 141. A diaphragm 17 is disposed between the first group lens 11 and the second group lens 12, that is, between the first lens 111 and the second lens 121, and a cover glass 18 is disposed on the image side of the fourth lens 141. Has been placed. The image plane 19 is at a position spaced from the cover glass 18.

  In the first lens 111, the object side lens surface 111a has a planar shape, and the image side lens surface 111b has a concave shape. In the second lens 121, the object side lens surface 121a and the image side lens surface 121b each have a convex shape. In the third lens 131, the object side lens surface 131a has a concave shape, and the image side lens surface 131b has a convex shape. In the fourth lens 141, the object side lens surface 141a and the image side lens surface 141b each have a convex shape.

The numerical aperture of the imaging lens 10 is set to Fno. Assuming that the half angle of view is ω and the total length of the lens diameter is L, these values are as follows.
Fno. = 2
ω = 57.5 °
L = 12.303mm

The focal length of the entire lens system is f, the focal length of the first group lens 11 (first lens 111) is ff1, the focal length of the second group lens 12 (second lens 121) is ff2, and the third group lens 13 is used. Assuming that the focal length of the (third lens 131) is ff3 and the focal length of the fourth group lens 14 (fourth lens 141) is ff4, these values are as follows.
f = 1.9748
ff1 = −7.394
ff2 = 2.019
ff3 = −1.089
ff4 = 1.545

Here, the imaging lens 10 of this example satisfies the following conditional expressions (1) to (3).
1.0 ≦ ff2 / f ≦ 2.0 (1)
−2.0 ≦ ff2 / ff3 ≦ −1.0 (2)
0.5 ≦ ff4 / f ≦ 2.0 (3)

  That is, ff2 / f = 1.02, ff2 / ff3 = −1.85, and ff4 / f = 0.78.

  Since the imaging lens 10 of this example satisfies the conditional expression (1), it is possible to suppress the entire length of the lens system and to suppress curvature of field. That is, when the upper limit value of conditional expression (1) is exceeded, the curvature of field increases to the positive side, making correction difficult. If the lower limit of conditional expression (1) is exceeded, the curvature of field increases on the negative side, making correction difficult. If the upper limit of conditional expression (1) is exceeded, the positive power of the second lens group 12 becomes relatively weak, making it difficult to keep the entire length of the lens system short.

  In addition, since the imaging lens 10 satisfies the conditional expression (2), it is possible to suppress the entire length of the lens system and suppress curvature of field while suppressing chromatic aberration. That is, when the upper limit value of conditional expression (2) is exceeded, the negative power of the third lens 131 having a concave shape becomes too weak with respect to the positive power of the second lens group 12 having a convex shape. Increases, making it difficult to correct. Accordingly, the upper limit is set to −1.0 or less in order to suppress chromatic aberration. The lower limit value of the conditional expression (2) is for suppressing the curvature of field and the total length of the lens system. When the lower limit value of conditional expression (2) is exceeded, the negative power of the third lens 131 having a concave shape becomes too strong with respect to the positive power of the second group lens 12 having a convex shape. Incurs an increase. Therefore, the lower limit is set to −2.0 or more in order to suppress the curvature of field. If the lower limit of conditional expression (2) is exceeded, the positive power of the second group lens 12 becomes weaker than the negative power of the third group lens 13, so it is difficult to keep the total length of the lens system short. become. Here, by setting the range of conditional expression (2) to be −1.9 to −1.3, it is possible to balance chromatic aberration and curvature of field.

  Furthermore, since the imaging lens 10 satisfies the conditional expression (3), the field curvature can be further suppressed. That is, when the upper limit value of conditional expression (3) is exceeded, the curvature of field increases on the positive side, and correction thereof becomes difficult. If the conditional expression (3) is equal to or greater than the lower limit value, the curvature of field increases on the negative side, and correction thereof becomes difficult. Therefore, in order to further suppress the curvature of field, the range is set to 0.5 or more and 2.0 or less. Here, with respect to the conditional expression (3), the range of 0.7 or more and 1.7 or less can balance the image plane.

In this example, when the Abbe number of the second group lens 12 (second lens 121) is νd2, and νd3 of the third group lens 13 (third lens 131), the following conditional expression (4) and condition Formula (5) is satisfy | filled.
νd2 ≧ 40 (4)
νd3 ≦ 35 (5)

  In this example, νd2 = 52 and νd3 = 23.4. As a result, in the imaging lens 10, the second lens 121 made of a low-dispersion material and the third lens 131 made of a high-dispersion material are arranged adjacent to each other, so that chromatic aberration can be corrected well.

  Next, Table 1A shows lens data of each lens surface of the imaging lens 10. In Table 1A, each lens surface is specified in the order counted from the object side. The lens surface marked with an asterisk is aspheric. In this example, the object side lens surfaces 121a and 131a of the second lens 121 (second group lens 12), the third lens 131 (third group lens 13), and the fourth lens 141 (fourth group lens 14), respectively. 141a and the image side lens surfaces 121b, 131b, and 141b have aspherical shapes. S indicates the diaphragm 17. The 9th and 10th surfaces are the glass surfaces of the cover glass 18. The unit of curvature radius and spacing is millimeters.

  Next, Table 1B shows aspherical coefficients for defining the aspherical shape of the aspherical lens surface. Also in Table 1B, each lens surface is specified in the order counted from the object side.

  The aspherical shape adopted for the lens surface is such that Y is the sag amount, c is the reciprocal of the radius of curvature, K is the cone coefficient, h is the ray height, 4th order, 6th order, 8th order, 10th order, 12th order, If the 14th and 16th aspherical coefficients are A4, A6, A8, A10, A12, A14, and A16, respectively, they are expressed by the following equations.

(Function and effect)
2A to 2D are an axial chromatic aberration diagram, a lateral aberration diagram, a field curvature diagram, and a distortion aberration diagram of the imaging lens 10. In the longitudinal chromatic aberration diagram of FIG. 2 (a), focal shift is shown, and the vertical axis shows wavelength. In the lateral aberration diagram of FIG. 2B, the horizontal axis indicates the entrance pupil coordinates, and the vertical axis indicates the amount of aberration. FIG. 2B shows simulation results for a plurality of light beams having different wavelengths. In the field curvature diagram of FIG. 2C, the horizontal axis indicates the distance in the optical axis direction, and the vertical axis indicates the height of the image. In FIG. 2C, S represents the field curvature aberration on the sagittal surface, and T represents the field curvature aberration on the tangential surface. In the distortion diagram of FIG. 2D, the horizontal axis indicates the amount of image distortion, and the vertical axis indicates the height of the image. As shown in FIG. 2A, according to the imaging lens 10 of this example, the axial chromatic aberration is corrected well. Further, as shown in FIG. 2B, color bleeding is suppressed. Further, as shown in FIGS. 2C and 2D, the field curvature is corrected well. Therefore, the imaging lens 10 has a high resolution.

  In this example, the object side lens surfaces 121a of the second lens 121 (second group lens 12), the third lens 131 (third group lens 13), and the fourth lens 141 (fourth group lens 14), Since the 131a and 141a and the image side lens surfaces 121b, 131b, and 141b have aspherical shapes, the imaging lens 10 is brightly configured. Furthermore, in this example, the total length L of the lens system can be kept as short as 12.303 mm.

(Example 2)
FIG. 3 is a configuration diagram of the imaging lens 20 of the second embodiment. As shown in FIG. 3, the imaging lens 20 includes a first group lens 21 having a negative power, a second group lens 22 having a positive power, and a negative power, which are arranged in order from the object side to the image side. And a fourth group lens 24 having positive power. The imaging lens 20 of this example is composed of five lenses, the first group lens 21 is composed of one first lens 211, and the second group lens 22 is composed of the second lens 221 and the third lens 222. The third lens group 23 is composed of one fourth lens 231, and the fourth lens group 24 is composed of one fifth lens 241. In the second group lens 22, a diaphragm 27 is disposed between the second lens 221 and the third lens 222, and a cover glass 28 is disposed on the image side of the fifth lens 241. The image plane 29 is at a position spaced from the cover glass 28.

  In the first lens 211, the object side lens surface 211a has a planar shape, and the image side lens surface 211b has a concave shape. In the second lens 221, the object side lens surface 221a and the image side lens surface 221b each have a convex shape. In the third lens 222, the object side lens surface 222a and the image side lens surface 222b each have a convex shape. In the fourth lens 231, the object side lens surface 231a has a concave shape, and the image side lens surface 231b has a convex shape. In the fifth lens 241, the object-side lens surface 241a and the image-side lens surface 241b each have a convex shape.

The numerical aperture of the imaging lens 20 is set to Fno. Assuming that the half angle of view is ω and the total length of the lens diameter is L, these values are as follows.
Fno. = 2
ω = 69.0 °
L = 12.300mm

In addition, the focal length of the entire lens system is f, the focal length of the first group lens 21 (first lens 221) is ff1, and the focal length of the second group lens 22 (second lens 221 and third lens 222) is ff2. When the focal length of the third lens group 23 (fourth lens 231) is ff3 and the focal length of the fourth lens group 24 (fifth lens 241) is ff4, these values are as follows.
f = 1.9055
ff1 = −3.430
ff2 = 2.059
ff3 = −1.481
ff4 = 2.451

If the focal length of the second lens 221 constituting the second group lens 22 is ff21 and the focal length of the third lens 222 is ff22, these values are as follows.
ff21 = 4.080
ff22 = 2.855

Here, the imaging lens 20 of this example satisfies the conditional expressions (1) to (3) as follows.
1.0 ≦ ff2 / f = 1.08 ≦ 2.0 (1)
−2.0 ≦ ff2 / ff3 = −1.39 ≦ −1.0 (2)
0.5 ≦ ff4 / f = 1.29 ≦ 2.0 (3)

Further, in this example, the Abbe number of the third lens 222 having a large Abbe number among the second lens 221 and the third lens 222 constituting the second group lens 22 is νd2, and the third group lens 23 (fourth lens 231). When the Abbe number of νd3 is νd3, the following conditional expressions (4) and (5) are satisfied.
νd2 = 56 ≧ 40 (4)
νd3 = 23.4 ≦ 35 (5)

  Next, Table 2A shows lens data of each lens surface of the imaging lens 20. In Table 2A, each lens surface is specified in the order counted from the object side. The lens surface with an asterisk is an aspherical surface. In this example, each of the third lens 222, the fourth lens 231 (third group lens 23), and the fifth lens 241 (fourth group lens 24). The object side lens surfaces 222a, 231a, and 241a and the image side lens surfaces 222b, 231b, and 241b have aspherical shapes. S indicates the diaphragm 27. The 12th and 13th surfaces are the glass surfaces of the cover glass 28. The unit of curvature radius and spacing is millimeters.

  Next, Table 2B shows aspherical coefficients for defining the aspherical shape of the aspherical lens surface. Also in Table 2B, each lens surface is specified in the order counted from the object side.

(Function and effect)
Since the imaging lens 20 of the present example satisfies the conditional expressions (1) to (3), it is possible to suppress the entire length of the lens system and to suppress curvature of field and chromatic aberration. Further, in this example, since the third lens 222 made of a low dispersion material and the fourth lens 231 made of a high dispersion material are disposed adjacent to each other, chromatic aberration can be corrected well.

  Further, in this example, the third lens 222, the fourth lens 231 (third group lens 23), and the fifth lens 241 (fourth group lens 24) of the second group lens 22 are respectively connected to the object side lens surface 222a, 231a and 241a and the image side lens surfaces 222b, 231b and 241b are provided with aspherical shapes. As a result, the numerical aperture: Fno. = 2, and the imaging lens 20 is brightly configured. In this example, the total length L of the lens system can be kept as short as 12.300 mm.

  4A to 4D are an axial chromatic aberration diagram, a lateral aberration diagram, a field curvature diagram, and a distortion diagram of the imaging lens 20. As shown in FIG. 4A, according to the imaging lens 20 of this example, the axial chromatic aberration is corrected well. Further, as shown in FIG. 4B, color bleeding is suppressed. Further, as shown in FIGS. 4C and 4D, the field curvature is corrected well. Therefore, the imaging lens 20 has a high resolution.

(Example 3)
FIG. 5 is a configuration diagram of the imaging lens 30 of the third embodiment. As shown in FIG. 5, the imaging lens 30 includes a first group lens 31 having a negative power, a second group lens 32 having a positive power, and a negative power, which are arranged in order from the object side to the image side. And a fourth lens group 34 having a positive power. The imaging lens 30 of this example is composed of five lenses, the first group lens 31 is composed of one first lens 311, and the second group lens 32 is composed of the second lens 321 and the third lens 322. The third lens group 33 is composed of one fourth lens 331, and the fourth lens group 34 is composed of one fifth lens 341. In the second group lens 32, a diaphragm 37 is disposed between the second lens 321 and the third lens 322, and a cover glass 38 is disposed on the image side of the fifth lens 341. The imaging plane 39 is at a position spaced from the cover glass 38.

  In the first lens 311, the object side lens surface 311 a has a planar shape, and the image side lens surface 311 b has a concave shape. In the second lens 321, the object side lens surface 321 a and the image side lens surface 321 b have convex shapes. In the third lens 322, the object-side lens surface 322a and the image-side lens surface 322b each have a convex shape. In the fourth lens 331, the object side lens surface 331a has a concave shape, and the image side lens surface 331b has a convex shape. In the fifth lens 341, the object side lens surface 341a and the image side lens surface 341b each have a convex shape.

The numerical aperture of the imaging lens 30 is set to Fno. Assuming that the half angle of view is ω and the total length of the lens diameter is L, these values are as follows.
Fno. = 2
ω = 56.5 °
L = 12.303mm

The focal length of the entire lens system is f, the focal length of the first group lens 31 (first lens 311) is ff1, and the focal length of the second group lens 32 (second lens 321 and third lens 322) is ff2. When the focal length of the third group lens 33 (fourth lens 331) is ff3 and the focal length of the fourth group lens 34 (fifth lens 341) is ff4, these values are as follows.
f = 1.986
ff1 = −6.278
ff2 = 2.321
ff3 = −1.602
ff4 = 2.206

If the focal length of the second lens 321 constituting the second lens group 32 is ff21 and the focal length of the third lens 322 is ff22, these values are as follows.
ff21 = 5.442
ff22 = 2.766

Here, the imaging lens 30 of this example satisfies the conditional expressions (1) to (3) as follows.
1.0 ≦ ff2 / f = 1.17 ≦ 2 (1)
−2.0 ≦ ff2 / ff3 = −1.38 ≦ −1.0 (2)
0.5 ≦ ff4 / f = 1.11 ≦ 2.0 (3)

Further, in this example, the Abbe number of the third lens 322 having the larger Abbe number among the second lens 321 and the third lens 322 constituting the second group lens 32 is νd2, and the third group lens 33 (fourth lens 331). When the Abbe number of νd3 is νd3, the following conditional expressions (4) and (5) are satisfied.
νd2 = 56 ≧ 40 (4)
νd3 = 23.4 ≦ 35 (5)

  Next, Table 3A shows lens data of each lens surface of the imaging lens 30. In Table 3A, each lens surface is specified in the order counted from the object side. The lens surface to which the star mark is attached is an aspherical surface, and in this example, the third lens 322, the fourth lens 331 (third group lens 33), and the fifth lens 341 (fourth group lens 34) respectively. The object side lens surfaces 322a, 331a, and 341a and the image side lens surfaces 322b, 331b, and 341b have aspherical shapes. S indicates the diaphragm 37. The 12th and 13th surfaces are the glass surfaces of the cover glass 38. The unit of curvature radius and spacing is millimeters.

  Next, Table 3B shows aspherical coefficients for defining the aspherical shape of the aspherical lens surface. Also in Table 3B, each lens surface is specified in the order counted from the object side.

(Function and effect)
Since the imaging lens 30 of this example satisfies the conditional expressions (1) to (3), it is possible to suppress the entire length of the lens system and to suppress field curvature and chromatic aberration. In this example, since the third lens 322 made of a low dispersion material and the fourth lens 331 made of a high dispersion material are disposed adjacent to each other, chromatic aberration can be corrected well.

  Furthermore, in this example, the third lens 322, the fourth lens 331 (third group lens 33), and the fifth lens 341 (fourth group lens 34) of the second group lens 32 are respectively connected to the object side lens surface 322a, 331a, 341a and image side lens surfaces 322b, 331b, 341b are provided with aspherical shapes. As a result, the numerical aperture: Fno. = 2, and the imaging lens 30 is brightly configured. In this example, the total length L of the lens system can be kept as short as 12.303 mm.

  6A to 6D are an axial chromatic aberration diagram, a lateral aberration diagram, a field curvature diagram, and a distortion diagram of the imaging lens 30. FIG. As shown in FIG. 6A, according to the imaging lens 30 of this example, the axial chromatic aberration is corrected well. Further, as shown in FIG. 6B, color bleeding is suppressed. Further, as shown in FIGS. 6C and 6D, the field curvature is corrected well. Therefore, the imaging lens 30 has a high resolution.

Example 4
FIG. 7 is a configuration diagram of the imaging lens 40 of the fourth embodiment. As shown in FIG. 7, the imaging lens 40 includes a first group lens 41 having a negative power, a second group lens 42 having a positive power, and a negative power, which are arranged in order from the object side to the image side. And a fourth lens group 44 having a positive power. The imaging lens 40 of this example is composed of five lenses, the first group lens 41 is composed of two lenses, a first lens 411 and a second lens 412, and the second group lens 42 is composed of one lens. The third lens 421 is composed of one fourth lens 431, and the fourth lens group 44 is composed of one fifth lens 441. A diaphragm 47 is disposed between the first group lens 41 and the second group lens 42, that is, between the second lens 412 and the third lens 421, and a cover glass 48 is disposed on the image side of the fifth lens 441. Has been placed. The imaging surface 49 is at a position spaced from the cover glass 48.

  In the first lens 411, the object side lens surface 411a has a convex shape, and the image side lens surface 411b has a concave shape. In the second lens 412, the object side lens surface 412a has a convex shape, and the image side lens surface 412b has a concave shape. In the third lens 421, the object side lens surface 421a and the image side lens surface 421b each have a convex shape. In the fourth lens 431, the object side lens surface 431a has a concave shape, and the image side lens surface 431b has a convex shape. In the fifth lens 441, the object side lens surface 441a and the image side lens surface 441b each have a convex shape.

The numerical aperture of the imaging lens 40 is set to Fno. Assuming that the half angle of view is ω and the total length of the lens diameter is L, these values are as follows.
Fno. = 2.4
ω = 95 °
L = 11.16 mm

The focal length of the entire lens system is f, the focal length of the first group lens 41 (first lens 411 and second lens 412) is ff1, and the focal length of the second group lens 42 (third lens 421) is ff2. If the focal length of the third lens group 43 (fourth lens 431) is ff3 and the focal length of the fourth lens group 44 (fifth lens 441) is ff4, these values are as follows.
f = 1.376
ff1 = -4.394
ff2 = 1.754
ff3 = −1.114
ff4 = 1.446

When the focal length of the first lens 411 constituting the first group lens 41 is ff11 and the focal length of the second lens 412 is ff12, these values are as follows.
ff11 = -11.304
ff12 = −8.279

Here, the imaging lens 40 of this example satisfies the conditional expressions (1) to (3) as follows.
1.0 ≦ ff2 / f = 1.27 ≦ 2.0 (1)
−2.0 ≦ ff2 / ff3 = −1.57 ≦ −1.0 (2)
0.5 ≦ ff4 / f = 1.05 ≦ 2.0 (3)

In this example, when the Abbe number of the second group lens 42 (third lens 421) is νd2, and the Abbe number of the third group lens 43 (fourth lens 431) is νd3, the following conditional expression (4 ) And conditional expression (5) are satisfied.
νd2 = 56 ≧ 40 (4)
νd3 = 23.4 ≦ 35 (5)

  Next, Table 4A shows lens data of each lens surface of the imaging lens 40. In Table 4A, each lens surface is specified in the order counted from the object side. The lens surface marked with an asterisk is an aspherical surface, and in this example, the second lens 412, the third lens 421 (third group lens 43), the fourth lens 431 (third group lens 43), and the fifth lens. Each of the object side lens surfaces 412a, 421a, 431a, 441a and the image side lens surfaces 412b, 421b, 431b, 441b of the lens 441 (fourth group lens 44) has an aspherical shape. S indicates the diaphragm 47. The 12th and 13th surfaces are the glass surfaces of the cover glass 48. The unit of curvature radius and spacing is millimeters.

  Next, Table 4B shows aspheric coefficients of the lens surfaces of the second lens 412, and Table 4C shows aspheric coefficients of the lens surfaces of the third lens 421, the fourth lens 431, and the fifth lens 441. In Tables 4B and 4C, the lens surfaces are specified in the order counted from the object side.

(Function and effect)
Since the imaging lens 40 of the present example satisfies the conditional expressions (1) to (3), it is possible to suppress the entire length of the lens system and to suppress field curvature and chromatic aberration. In this example, since the third lens 421 made of a low dispersion material and the fourth lens 431 made of a high dispersion material are arranged adjacent to each other, chromatic aberration can be corrected well.

  Furthermore, in this example, the second lens 412, the third lens 421 (second group lens 42), the fourth lens 431 (third group lens 43), and the fifth lens 441 (fourth group lens 44) are respectively The object side lens surfaces 412a, 421a, 431a, 441a and the image side lens surfaces 412b, 421b, 431b, 441b are provided with aspherical shapes. As a result, the numerical aperture: Fno. = 2.4, and the imaging lens 40 is brightly configured. In this example, the total length L of the lens system can be kept as short as 11.16 mm.

  8A to 8D are an axial chromatic aberration diagram, a lateral aberration diagram, a field curvature diagram, and a distortion diagram of the imaging lens 40. FIG. As shown in FIG. 8A, according to the imaging lens 40 of this example, the axial chromatic aberration is corrected well. Further, as shown in FIG. 8B, color bleeding is suppressed. Further, as shown in FIGS. 8C and 8D, the field curvature is corrected well. Therefore, the imaging lens 40 has a high resolution.

(Example 5)
FIG. 9 is a configuration diagram of the imaging lens 50 of the fifth embodiment. As shown in FIG. 7, the imaging lens 50 includes a first group lens 51 having a negative power, a second group lens 52 having a positive power, and a negative power, which are arranged in order from the object side to the image side. And a fourth group lens 54 having positive power. The imaging lens 50 of this example is composed of six lenses, the first group lens 51 is composed of two lenses, a first lens 511 and a second lens 512, and the second group lens 52 is a third lens. It is composed of two lenses, 521 and a fourth lens 522. The third group lens 53 includes one fifth lens 531, and the fourth group lens 54 includes one sixth lens 541. A diaphragm 57 is disposed between the third lens 521 and the fourth lens 522 constituting the second group lens 52, and a cover glass 58 is disposed on the image side of the sixth lens 541. The imaging plane 59 is at a position spaced from the cover glass 58.

  In the first lens 511, the object side lens surface 511a has a convex shape, and the image side lens surface 511b has a concave shape. In the second lens 512, the object side lens surface 512a and the image side lens surface 512b each have a concave shape. In the third lens 521, the object side lens surface 521a and the image side lens surface 521b each have a convex shape. In the fourth lens 522, the object-side lens surface 522a and the image-side lens surface 522b each have a convex shape. In the fifth lens 531, the object side lens surface 531a has a concave shape, and the image side lens surface 531b has a convex shape. In the sixth lens 541, the object side lens surface 541a and the image side lens surface 541b each have a convex shape.

The numerical aperture of the imaging lens 50 is set to Fno. Assuming that the half angle of view is ω and the total length of the lens diameter is L, these values are as follows.
Fno. = 2.2
ω = 72.8 °
L = 15.57mm

The focal length of the entire lens system is f, the focal length of the first lens group 51 (first lens 511 and second lens 512) is ff1, and the second lens group 52 (third lens 521 and fourth lens 522). Assuming that the focal length is ff2, the focal length of the third lens group 53 (fifth lens 531) is ff3, and the focal length of the fourth lens group 54 (sixth lens 541) is ff4, these values are as follows. .
f = 1.356
ff1 = −3.279
ff2 = 2.459
ff3 = −1.602
ff4 = 2.183

The focal length of the first lens 511 constituting the first group lens 51 is ff11, the focal length of the second lens 512 is ff12, and the focal length of the third lens 521 constituting the second group lens 52. Where ff21 and the focal length of the fourth lens 522 are ff22, these values are as follows.
ff11 = -14.13
ff12 = -4.958
ff21 = 3.649
ff22 = 2.793

Here, the imaging lens 50 of this example satisfies the conditional expressions (1) to (3) as follows.
1.0 ≦ ff2 / f = 1.81 ≦ 2.0 (1)
−2.0 ≦ ff2 / ff3 = −1.53 ≦ −1.0 (2)
0.5 ≦ ff4 / f = 1.61 ≦ 2.0 (3)

In this example, among the second group lenses 52 (the third lens 521 and the fourth lens 522), the Abbe number of the fourth lens 522 having a large Abbe number is νd2, and the third group lens 53 (the fifth lens 531) has the same Abbe number. When the Abbe number is νd3, the following conditional expressions (4) and (5) are satisfied.
νd2 = 56 ≧ 40 (4)
νd3 = 23.4 ≦ 35 (5)

  Next, Table 5A shows lens data of each lens surface of the imaging lens 50. In Table 5A, each lens surface is specified in the order counted from the object side. The lens surface marked with an asterisk is an aspheric surface. In this example, the second lens 512, the fourth lens 522 of the third group lens 53, the fifth lens 531 (third group lens 53), and the The object side lens surfaces 512a, 522a, 531a, 541a and the image side lens surfaces 512b, 522b, 531b, 541b of the six lenses 541 (fourth group lens 54) have aspherical shapes. S indicates the aperture 57. The 14th and 15th surfaces are the glass surfaces of the cover glass 58. The unit of curvature radius and spacing is millimeters.

  Next, Table 5B shows aspheric coefficients of the lens surfaces of the second lens 512, and Table 5C shows aspheric coefficients of the lens surfaces of the fourth lens 522, the fifth lens 531 and the sixth lens 541. In Tables 5B and 5C, the lens surfaces are specified in the order counted from the object side.

(Function and effect)
Since the imaging lens 50 of this example satisfies the conditional expressions (1) to (3), it is possible to suppress the entire length of the lens system and to suppress field curvature and chromatic aberration. In this example, since the fourth lens 522 made of a low dispersion material and the fifth lens 531 made of a high dispersion material are arranged adjacent to each other, chromatic aberration can be corrected well.

  Further, in this example, each of the second lens 512, the fourth lens 522 of the second group lens 52, the fifth lens 531 (third group lens 53), and the sixth lens 541 (fourth group lens 54) is an object. The side lens surfaces 512a, 522a, 531a and 541a and the image side lens surfaces 512b, 522b, 531b and 541b are provided with aspherical shapes. As a result, the numerical aperture: Fno. = 2.2, and the imaging lens 50 is brightly configured. In this example, the total length L of the lens system can be kept as short as 15.57 mm.

  10A to 10D are an axial chromatic aberration diagram, a lateral aberration diagram, a field curvature diagram, and a distortion diagram of the imaging lens 50. FIG. As shown in FIG. 10A, according to the imaging lens 50 of this example, the axial chromatic aberration is corrected well. Further, as shown in FIG. 10B, color bleeding is suppressed. Further, as shown in FIGS. 10C and 10D, the curvature of field is corrected well. Therefore, the imaging lens 50 has a high resolution.

(Imaging device)
FIG. 11 is an explanatory diagram of an image pickup apparatus 60 equipped with the image pickup lens 10 of the present invention. As shown in FIG. 11, the imaging device 60 includes an imaging element 61 in which a sensor surface 61 a is arranged on the imaging surface 19 (focal position) of the imaging lens 10. The image sensor 61 is a CCD sensor or a CMOS sensor.

  According to this example, since the resolution of the imaging lens 10 is high, the imaging device 60 can have a high resolution by adopting the imaging device 61 having a large number of pixels as the imaging device 61. In addition, since the total length of the lens system of the imaging lens 10 is short, the imaging device 60 can be downsized. The imaging device 60 can be equipped with the imaging lenses 20, 30, 40, and 50 in the same manner as the imaging lens 10. In this case, the same effect can be obtained.

10, 20, 30, 40, 50 ... Imaging lens Examples 11, 21, 31, 41, 51 ... First lens group 12, 22, 32, 42, 52 ... Second lens group 13, 23, 33, 43, 53 ... Third lens group 14, 24, 34, 44, 54 ... Fourth lens group 17, 27, 37, 47, 57 ... Aperture 18, 28, 38, 48 58 ... Cover glass 19, 29, 39, 49, 59 ... Imaging surface 60 ... Imaging device 61 ... Imaging element 61a ... Sensor surface

Claims (5)

A first lens unit having a negative power, a second lens unit having a positive power, a third lens unit having a negative power, and a positive power, which are arranged in order from the object side to the image side. Consists of a fourth lens group
The first group lens is composed of one lens having negative power, or two lenses each having negative power,
The second group lens is composed of one lens having positive power, or two lenses each having positive power,
The third group lens is composed of one lens having negative power,
The fourth group lens is composed of one lens having positive power,
The lens constituting the first group lens has a concave shape on the image side lens surface,
The lens arranged adjacent to the third group lens in the second group lens has a convex shape on the image side lens surface,
The third lens group has a concave shape on the object side lens surface, a convex shape on the image side lens surface,
At least one of the lenses constituting the second group lens, the third group lens, and the fourth group lens has at least one of the object-side lens surface and the image-side lens surface being non-surface. It has a spherical shape,
When the focal length of the entire lens system is f, the focal length of the second lens group is ff2, and the focal length of the third lens group is ff3, the following conditional expressions (1) and (2) are satisfied. A wide-angle lens.
1.0 ≦ ff2 / f ≦ 2.0 (1)
-1.9 ≦ ff2 / ff3 ≦ −1.3 (2) 2. The wide angle lens according to claim 1, wherein the following conditional expression (3) is satisfied when a focal length of the fourth lens group is ff4.
0.5 ≦ ff4 / f ≦ 2.0 (3) 2. The wide angle lens according to claim 1, wherein the second group lens includes a lens having an Abbe number of 40 or more, and the third group lens includes a lens having an Abbe number of 35 or less. 2. The wide-angle lens according to claim 1, wherein the diagonal angle of view is 100 degrees or more. An imaging apparatus comprising: the wide-angle lens according to claim 1; and an imaging element disposed at a focal position of the wide-angle lens.

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