The present invention relates to an imaging optical system which can be provided in an imaging apparatus such as, e.g., an in-vehicle camera, a surveillance camera, and a portable terminal (including a mobile phone, a smart phone or other smart devices).
An imaging optical system is known in the related art that can achieve both a wide angle-of-view and a higher definition of a telescopic image in a central area of a picture frame. Patent Literature 1 discloses an imaging optical system which achieves a wide angle-of-view by causing a large amount of negative distortion, and achieves an enlarged (and distorted) image in the central area of the picture frame.
Patent Literature 1: Japanese Unexamined Patent Publication No. 2005-010521.
However, in the imaging optical system of Patent Literature 1, the overall length of the imaging optical system becomes long when set to a large aperture; and if the overall length of the imaging optical system is shortened, there is the disadvantage of not being able to provide a large aperture ratio. For example, the fourth embodiment in Patent Literature 1 discloses an imaging optical system having a relatively large aperture having an f-number of about 1.8. However, the value of the overall length of the imaging optical system divided by the maximum image height is 9.8; hence, the overall length of the imaging optical system is long relative to the maximum image height. Whereas, in the first embodiment of Patent Literature 1, the value of the overall length of the imaging optical system divided by the maximum image height is 5.1, so that the overall length of the imaging optical system is short relative to the maximum image height; however, the f-number is 2.8, i.e., the aperture ratio is not very large.
The present invention has been devised in view of the above-described problems, and provides an imaging optical system which can achieve a wide angle-of-view while enlarging the object image at the central area of the picture screen, has a short overall length, has a large aperture, and various aberrations can be favorably corrected.
According to an aspect of the present invention, an imaging optical system is provided, including a positive or negative first lens group, an aperture diaphragm, and a positive second lens group, in that order from the object side. The first lens group includes a negative lens element provided closest to the object side within the first lens group. The negative lens element that is closest to the object side includes an aspherical surface on the object side thereof, the aspherical surface including a paraxial convex surface convexing toward the object side, a paraxial curvature (curvature of the central portion) that is the greatest within the effective aperture, and a portion within the effective aperture that has a curvature that is less than ½ of the paraxial curvature (curvature of the central portion). The following conditions (1), (2), (3) and (4) are satisfied:
R1/f<1.35 (1),
D1/f>0.4 (2),
−2.5<f1/f<−1.3 (3), and
V>56 (4),
wherein f designates the focal length of the imaging optical system, f1 designates the focal length of the negative lens element provided closest to the object side within the first lens group, R1 designates a paraxial radius of curvature of a surface on the object side (the radius of curvature of the paraxial convex surface) of the negative lens element provided closest to the object side within the first lens group, D1 designates a thickness, along the optical axis, of the negative lens element provided closest to the object side within the first lens group, and V designates the Abbe number with respect to the d-line of a lens element, within the second lens group, that is provided closest to the aperture diaphragm.
It is desirable for the following condition (4′) to be satisfied within the scope of condition (4):
V>63 (4′).
In the present specification, in addition to the case where an aperture diaphragm is positioned between a surface closest to the image side on the first lens group and a surface closest to the object side on the second lens group, “a first lens group, an aperture diaphragm and a second lens group, in that order from the object side (in other words, an aperture diaphragm is provided between the first lens group and the second lens group)” also refers to the case where the aperture diaphragm is positioned on a plane that is orthogonal to the optical axis and is tangent to surface closest to the image side on the first lens group, or at a position that is slightly toward the object side from such a plane so that the aperture diaphragm and the first lens group overlap with respect to the optical axis direction; and also refers to the case where the aperture diaphragm is positioned on a plane that is orthogonal to the optical axis and is tangent to surface closest to the object side on the second lens group, or at a position that is slightly toward the image side from such a plane so that the aperture diaphragm and the second lens group overlap with respect to the optical axis direction.
In the present specification, “effective aperture of a lens element” refers to the maximum area of a light-ray passage of the lens element determined by light rays that pass through the lens element at a maximum position (distance) from the optical axis out of the light rays from the center (on the optical axis) of an image, formed by an optical system that includes the lens element, to the maximum image height.
It is desirable for the following condition (5) to be satisfied:
−0.45<f1/fg1<1 (5),
wherein f1 designates the focal length of the negative lens element provided closest to the object side within the first lens group, and fg1 designates the focal length of the first lens group.
It is desirable for the following condition (6) to be satisfied:
0.3<(R1−R2)/(R1+R2)<0.55 (6),
wherein R1 designates the paraxial radius of curvature of the surface on the object side (the radius of curvature of the paraxial convex surface) of the negative lens element provided closest to the object side within the first lens group, and R2 designates the paraxial radius of curvature of the surface on the image side of the negative lens element provided closest to the object side within the first lens group.
It is desirable for the first lens group to include a positive lens element behind the negative lens element provided closest to the object side within the first lens group.
It is desirable for the positive lens element that is provided behind the negative lens element provided closest to the object side, within the first lens group, to be a positive meniscus lens element having a convex surface on the image side.
It is desirable for the positive lens element that is provided behind the negative lens element provided closest to the object side, within the first lens group, to have an Abbe number of at least 35 with respect to the d-line.
It is desirable for the second lens group to include at least one positive lens element that has an Abbe number of at least 70 with respect to the d-line.
It is desirable for the second lens group to include at least one negative lens element that has an Abbe number of 20 or less with respect to the d-line.
According to the present invention, an imaging optical system is obtained, which can achieve a wide angle-of-view while enlarging the object image at the central area of the picture screen, has a short overall length, has a large aperture, and various aberrations can be favorably corrected.
The present disclosure relates to subject matter contained in Japanese Patent Application No. 2016-052422 (filed on Mar. 16, 2016) which is expressly incorporated herein in its entirety.
The present invention will be discussed below in detail with reference to the accompanying drawings, in which:
The imaging optical system of the present invention is configured of a positive or negative first lens group G1, an aperture diaphragm S, and a positive second lens group G2, in that order from the object side. In each of the first and fifth numerical embodiments, the first lens group G1 has a positive refractive power. In each of the second through fourth and sixth through thirteenth numerical embodiments, the first lens group G1 has a negative refractive power. In each of the first, second, fourth, fifth and seventh through thirteenth numerical embodiments, a cover glass CG is provided between the second lens group G2 and an imaging surface IM. In each of the third and sixth numerical embodiments, an optical filter OP and a cover glass CG are provided between the second lens group G2 and the imaging surface IM.
In the first numerical embodiment, the first lens group G1 is configured of a negative lens element 11 formed from aspherical glass molded lens element (having an aspherical surface on each side thereof), and a positive lens element 12 formed from a spherical glass lens element, in that order from the object side. The aspherical surface on the object side of the negative lens element 11 includes a paraxial convex surface convexing toward the object side, a paraxial curvature (curvature of the central portion) that is the greatest within the effective aperture, and a portion within the effective aperture (at a peripheral portion other than the paraxial portion) that has a curvature that is less than ½ of the paraxial curvature (curvature of the central portion). The positive lens element 12 is a biconvex positive lens element.
In each of the second through fourth and sixth through thirteenth numerical embodiments, the first lens group G1 is configured of a negative lens element 11 formed from an aspherical glass molded lens element (having an aspherical surface on each side thereof), and a positive lens element 12 formed from aspherical glass molded lens element (having an aspherical surface on each side thereof), in that order from the object side. The aspherical surface on the object side of the negative lens element 11 includes a paraxial convex surface convexing toward the object side, a paraxial curvature (curvature of the central portion) that is the greatest within the effective aperture, and a portion within the effective aperture (at a peripheral portion other than the paraxial portion) that has a curvature that is less than ½ of the paraxial curvature (curvature of the central portion). The positive lens element 12 is a positive meniscus lens element having a convex surface on the image side.
In the fifth numerical embodiment, the first lens group G1 is configured of a negative lens element 11′ formed from an aspherical glass molded lens element (having an aspherical surface on each side thereof), a positive lens element 12′ formed from a spherical glass lens element, a negative lens element 13′ formed from a spherical glass lens element, and a positive lens element 14′ formed from a spherical glass lens element, in that order from the object side. The aspherical surface on the object side of the negative lens element 11′ includes a paraxial convex surface convexing toward the object side, a paraxial curvature (curvature of the central portion) that is the greatest within the effective aperture, and a portion within the effective aperture (at a peripheral portion other than the paraxial portion) that has a curvature that is less than ½ of the paraxial curvature (curvature of the central portion). The positive lens element 12′ is a positive meniscus lens element having a convex surface on the image side. The negative lens element 13′ is a negative meniscus lens element having a convex surface on the image side. The positive lens element 14′ is a biconvex positive lens element.
By providing the positive lens element 12 or 12′ subsequently (immediately) behind the negative lens element 11 or 11′, which is closest to the object side within the first lens group G1, the height of light rays of an abaxial light bundle incident on the negative lens element 11 or 11′ can be reduced, and the diameter of the negative lens element 11 or 11′ can also be reduced. Furthermore, by forming the positive lens element 12 or 12′ as a positive meniscus lens element having a convex surface on the image side, a negative refractive power can be provided on the surface on the object side of the positive lens element 12 or 12′, so that astigmatism and distortion can be favorably corrected. Furthermore, by setting the Abbe number with respect to the d-line of the positive lens element 12 or 12′ to 35 or more, lateral chromatic aberration can be favorably corrected.
As shown in the first through thirteenth numerical embodiments that are described hereinafter, there is a certain degree of freedom in the configuration of the second lens group G2 in which a number of variations are possible.
Among such variations, it is desirable for the second lens group G2 to include at least one positive lens element having an Abbe number of at least 70 with respect to the d-line and/or at least one negative lens element having an Abbe number of 20 or less with respect to the d-line. By including a positive lens element using a low-dispersion glass having an Abbe number of at least 70, with respect to the d-line, within the second lens group G2, axial chromatic aberration can be favorably corrected. By including a negative lens element using a high-dispersion glass having an Abbe number of 20 or less, with respect to the d-line, within the second lens group G2, due to a synergistic effect of the positive lens element using a low-dispersion glass and the negative lens element using a high-dispersion glass, axial chromatic aberration can be more favorably corrected. Furthermore, since the refractive index of such a negative lens increases, the radius of curvature also increases, so that light-ray angle of incident on the image sensor can be made smaller.
A positive lens element or a negative lens element may be provided closest to the aperture diaphragm (S) side within the second lens group G2. For example, in the first numerical embodiment (described in detail later), a negative lens element (21) is provided closest to the aperture diaphragm (S) side within the second lens group G2, and in the second through thirteenth numerical embodiments (described in detail later), a positive lens element (21′, 21″, 21A, 21B, 21C or 21D) is provided closest to the aperture diaphragm (S) side within the second lens group G2.
In the imaging optical system of the illustrated embodiments, by reducing the effective aperture of the negative lens element 11 or 11′ that is provided closest to the object side within the first lens group G1 and reducing the number of lens elements, the overall length of the imaging optical system can be shortened, and miniaturization of the imaging optical system, and consequently the imaging apparatus in which the imaging optical system is provided, can be achieved. Furthermore, the imaging optical system of the illustrated embodiments achieves an f-number (lens speed) of 1.6.
In the imaging optical system of the illustrated embodiments, in order to achieve a wide angle-of-view while enlarging the object image at the central area of the picture screen, the focal length, which determines the magnification of the central area of the lens, is increased and a wider angle-of-view is provided at the lens peripheral portion.
More specifically, the aspherical surface on the object side of the negative lens element 11 or 11′, provided closest to the object side within the first lens group G1, has a profile that includes a paraxial convex surface convexing toward the object side, a paraxial curvature (curvature of the central portion) that is the greatest within the effective aperture, and a portion within the effective aperture (at a peripheral portion other than the paraxial portion) that has a curvature that is less than ½ of the paraxial curvature (curvature of the central portion). Accordingly, it is possible to generate negative distortion to thereby achieve a wide angle-of-view. The smaller the curvature of the above-mentioned “portion” of the negative lens element 11 or 11′, provided closest to the object side within the first lens group G1 (in the case where the curvature is a negative value, the greater the absolute value of the negative curvature), the more advantageous the negative lens element 11 or 11′ is for widening the angle-of-view. For example, the aspherical surface on the object side of the negative lens element 11 or 11′ can have the greatest paraxial curvature (curvature of the central portion) within the effective aperture, and the curvature from a central portion toward the peripheral portion can be decreased and thereafter increased at an outermost peripheral portion.
Condition (1) specifies the ratio of the focal length of the entire lens system (imaging optical system) to the paraxial radius of curvature of the surface on the object side (the radius of curvature of the paraxial convex surface) of the negative lens element 11 or 11′ that is provided closest to the object side within the first lens group G1. By satisfying condition (1), since the position of the principle point becomes distant from the imaging surface (imaging plane) IM (since the lateral magnification in regard to the optical system after the surface on the object side of the negative lens element 11 or 11′ increases), the paraxial focal length of the entire optical system increases, so that the object image at a central portion (of the picture frame) can be enlarged.
If the upper limit of condition (1) is exceeded, it becomes difficult to form an enlarged object image at a central portion of the picture frame.
Condition (2) specifies the ratio of the focal length of the entire lens system (imaging optical system) to the thickness of the negative lens element 11 or 11′, provided closest to the object side within the first lens group G1, along the optical axis. By satisfying condition (2), since the position of the principle point becomes distant from the imaging surface (imaging plane) IM (since the lateral magnification in regard to the optical system after the surface on the object side of the negative lens element 11 or 11′ increases), the paraxial focal length of the entire optical system increases, so that the object image at a central portion (of the picture frame) can be enlarged.
If the lower limit of condition (2) is exceeded, it becomes difficult to form an enlarged object image at a central portion of the picture frame.
By satisfying conditions (1) and (2), the focal length, normalized by the image-sensor size, of the imaging optical system of the illustrated embodiments can be increased to 1.6 mm through 1.7 mm, so that the object image at a central portion (of the picture frame) can be enlarged.
Condition (3) specifies the ratio of the focal length of the entire lens system (imaging optical system) to the focal length of the negative lens element 11 or 11′, provided closest to the object side within the first lens group G1. By satisfying condition (3), the overall length of the entire lens system (imaging optical system) can be shortened and the object image at a central portion (of the picture frame) can be enlarged.
If the upper limit of condition (3) is exceeded, the focal length of the negative lens element 11 or 11′ becomes too short, so that the lateral magnification of the optical system thereafter (the remaining lens elements within the first lens group G1 and the second lens group G2) must be increased, thereby increasing the overall length of the entire lens system (imaging optical system).
If the lower limit of condition (3) is exceeded, it becomes difficult to form an enlarged object image at a central portion of the picture frame.
Conditions (4) and (4′) specify the Abbe number with respect to the d-line of the lens element (21, 21′, 21″, 21A, 21B, 21C and 21D) provided closest to the aperture diaphragm S and within the second lens group G2. By satisfying condition (4), even if the refractive power of the lens element that bears most of the positive refractive power burden (within the second lens group G2) is increased, occurrence of axial chromatic aberration can be suppressed; therefore, an imaging optical system can be achieved which has an increased positive refractive power, thereby shortening the overall length of the lens system while achieving a large aperture and favorably correcting aberrations. The f-number of the imaging optical system of the illustrated embodiments is approximately 1.6, the value of the overall length of the imaging optical system divided by the maximum image height is approximately 6.3 through 9.9, and achieves a shortened overall length of the imaging optical system while having a larger aperture than that disclosed in the aforementioned Patent Literature 1. These functional effects are more prominent when condition (4′) is satisfied.
If the lower limit of condition (4) is exceeded, it becomes difficult to achieve an imaging optical system which can have a large aperture and favorably correct various aberrations.
Condition (5) specifies the ratio of the focal length of the negative lens element 11 or 11′ that is provided closest to the object side within the first lens group G1 to the focal length of the first lens group G1. By satisfying condition (5), the object image at a central portion (of the picture frame) can be enlarged, astigmatism can be favorably corrected, and the overall length of the lens system (imaging optical system) can be shortened.
If the specified range of condition (5) is exceeded, since the refractive power of the negative lens element 11 or 11′ becomes small (weak), the focal length of the overall lens system (imaging optical system) becomes short, so that it becomes difficult to form an enlarged object image at a central portion of the picture frame.
Condition (6) specifies the shape (shaping factor) of the negative lens element 11 or 11′ that is provided closest to the object side within the first lens group G1. By satisfying condition (6), the lens diameter of the negative lens element 11 or 11′ can be reduced, the overall length of the lens system (imaging optical system) can be reduced, and an enlarged object image at a central portion can be formed over a wide range within the picture frame.
If the upper limit of condition (6) is exceeded, the lens diameter of the negative lens element 11 or 11′ increases and the overall length of the lens system (imaging optical system) increases, so that it becomes difficult to form an enlarged object image at a central portion of the picture frame.
If the lower limit of condition (6) is exceeded, it becomes difficult to correct various aberrations.
Specific numerical first through thirteenth embodiments will be herein discussed. In the aberration diagrams and the tables, the d-line, g-line and C-line show aberrations at their respective wave-lengths; S designates the sagittal image, M designates the meridional image, f designates the focal length of the entire optical system, Fno. designates the f-number, W designates the half angle of view (°), Y designates the image height (maximum image height), r designates the (paraxial) radius of curvature, d designates the lens thickness or distance between lenses, N(d) designates the refractive index at the d-line, and νd designates the Abbe number with respect to the d-line. The unit used for the various lengths is defined in millimeters (mm). The “Effective Aperture” in the lens data indicates a radius (a distance from the optical axis).
An aspherical surface which is rotationally symmetrical about the optical axis is defined as:
x=cy
2/(1+[1−{1+K}c2y2]1/2)+A4y4+A6y6+A8y8+A10y10+A12y12 . . .
wherein ‘c’ designates the curvature (1/r) of the aspherical vertex, ‘y’ designates the distance from the optical axis, ‘K’ designates the conic coefficient, A4 designates a fourth-order aspherical coefficient, A6 designates a sixth-order aspherical coefficient, A8 designates an eighth-order aspherical coefficient, A10 designates a tenth-order aspherical coefficient, A12 designates a twelfth-order aspherical coefficient, and ‘x’ designates the amount of sag.
The imaging optical system of the first numerical embodiment is configured of a positive first lens group G1, an aperture diaphragm S, and a positive second lens group G2, in that order from the object side. A cover glass CG is provided between the second lens group G2 and an imaging surface IM.
The first lens group G1 is configured of a negative lens element 11 formed from an aspherical glass molded lens element (having an aspherical surface on each side thereof), and a positive lens element 12 formed from a spherical glass lens element, in that order from the object side. The aspherical surface on the object side of the negative lens element 11 includes a paraxial convex surface convexing toward the object side, a paraxial curvature (curvature of the central portion) that is the greatest within the effective aperture, and a portion within the effective aperture (at a peripheral portion other than the paraxial portion) that has a curvature that is less than ½ of the paraxial curvature (curvature of the central portion). The positive lens element 12 is a biconvex positive lens element.
The second lens group G2 is configured of a negative lens element 21 formed from a spherical glass lens element, a positive lens element 22 formed from a spherical glass lens element, and a positive lens element 23 formed from an aspherical glass molded lens element (having an aspherical surface on each side thereof), in that order from the object side. The negative lens element 21 is a negative meniscus lens element having a convex surface on the object side, the positive lens element 22 is a biconvex positive lens element, and the negative lens element (negative meniscus lens element) 21 and the positive lens element (biconvex positive lens element) 22 are cemented to each other. The positive lens element 23 is a positive meniscus lens element having a convex surface on the object side.
The second numerical embodiment has the same lens arrangement as that of the first numerical embodiment except for the following features:
(1) The first lens group G1 has a negative refractive power instead of a positive refractive power.
(2) The positive lens element 12 of the first lens group G1 is a positive meniscus lens element, having a convex surface on the image side, that is formed from an aspherical glass molded lens element (having an aspherical surface on each side thereof).
(3) The second lens group G2 is configured of a positive lens element 21′ formed from a spherical glass lens element, a negative lens element 22′ formed from a spherical glass lens element, a positive lens element 23′ formed from a spherical glass lens element, and a positive lens element 24′ formed from an aspherical glass molded lens element (having an aspherical surface on each side thereof), in that order from the object side. The positive lens element 21′ is a biconvex positive lens element. The negative lens element 22′ is a negative meniscus lens element having a convex surface on the object side, and the positive lens element 23′ is a biconvex positive lens element. The negative lens element (negative meniscus lens element) 22′ and the positive lens element (biconvex positive lens element) 23′ are cemented to each other. The positive lens element 24′ is a positive meniscus lens element having a convex surface on the object side.
The third numerical embodiment has the same lens arrangement as that of the second numerical embodiment except for the following feature:
(1) An optical filter OP is provided between the second lens group G2 and the cover glass CG.
The fourth numerical embodiment has the same lens arrangement as that of the first numerical embodiment except for the following features:
(1) The first lens group G1 has a negative refractive power instead of a positive refractive power.
(2) The positive lens element 12 of the first lens group G1 is a positive meniscus lens element, having a convex surface on the image side, that is formed from an aspherical glass molded lens element (having an aspherical surface on each side thereof).
(3) The second lens group G2 is configured of a positive lens element 21″ formed from a spherical glass lens element, a positive lens element 22″ formed from a spherical glass lens element, a negative lens element 23″ formed from a spherical glass lens element, a positive lens element 24″ formed from a spherical glass lens element, and a positive lens element 25″ formed from a spherical glass lens element, in that order from the object side. The positive lens element 21″ is a positive meniscus lens element having a convex surface on the image side. The positive lens element 22″ is a biconvex positive lens element. The negative lens element 23″ is a biconcave negative lens element and the positive lens element 24″ is a positive meniscus lens element having a convex surface on the object side; the negative lens element (biconcave negative lens element) 23″ and the positive lens element (positive meniscus lens element) 24″ are cemented to each other. The positive lens element 25″ is a positive meniscus lens element having a convex surface on the object side.
The fifth numerical embodiment has the same lens arrangement as that of the first numerical embodiment except for the following features:
(1) The first lens group G1 is configured of a negative lens element 11′ formed from an aspherical glass molded lens element (having an aspherical surface on each side thereof), a positive lens element 12′ formed from a spherical glass lens element, a negative lens element 13′ formed from a spherical glass lens element, and a positive lens element 14′ formed from a spherical glass lens element, in that order from the object side. The aspherical surface on the object side of the negative lens element 11′ includes a paraxial convex surface convexing toward the object side, a paraxial curvature (curvature of the central portion) that is the greatest within the effective aperture, and a portion within the effective aperture (at a peripheral portion other than the paraxial portion) that has a curvature that is less than ½ of the paraxial curvature (curvature of the central portion). The positive lens element 12′ is a positive meniscus lens element having a convex surface on the image side. The negative lens element 13′ is a negative meniscus lens element having a convex surface on the image side. The positive lens element 14′ is a biconvex positive lens element.
(2) The second lens group G2 is configured of a positive lens element 21A formed from a spherical glass lens element, a negative lens element 22A formed from a spherical glass lens element, a positive lens element 23A formed from spherical glass lens element and a positive lens element 24A formed from spherical glass lens element, in that order from the object side. The positive lens element 21A is a biconvex positive lens element. The negative lens element 22A is a biconcave negative lens element, and the positive lens element 23A is a biconvex positive lens element; the negative lens element (biconcave negative lens element) 22A and the positive lens element (biconvex positive lens element) 23A are cemented to each other. The positive lens element 24A is a positive meniscus lens element having a convex surface on the object side.
The sixth numerical embodiment has the same lens arrangement as that of the first numerical embodiment except for the following features:
(1) The first lens group G1 has a negative refractive power instead of a positive refractive power.
(2) The positive lens element 12 of the first lens group G1 is a positive meniscus lens element, having a convex surface on the image side, that is formed from an aspherical glass molded lens element (having an aspherical surface on each side thereof).
(3) The second lens group G2 is configured of a positive lens element 21B formed from a spherical glass lens element, a negative lens element 22B formed from a spherical glass lens element, a positive lens element 23B formed from a spherical glass lens element, and a positive lens element 24B formed from spherical glass lens element, in that order from the object side. The positive lens element 21B is a biconvex positive lens element. The negative lens element 22B is a negative meniscus lens element having a convex surface on the object side, and the positive lens element 23B is a positive meniscus lens element having a convex surface on the object side; the negative lens element (negative meniscus lens element) 22B and the positive lens element (positive meniscus lens element) 23B are cemented to each other. The positive lens element 24B is a positive meniscus lens element having a convex surface on the object side.
(4) An optical filter OP is provided between the second lens group G2 and the cover glass CG.
The seventh numerical embodiment has the same lens arrangement as that of the first numerical embodiment except for the following features:
(1) The first lens group G1 has a negative refractive power instead of a positive refractive power.
(2) The positive lens element 12 of the first lens group G1 is a positive meniscus lens element, having a convex surface on the image side, that is formed from an aspherical glass molded lens element (having an aspherical surface on each side thereof).
(3) The second lens group G2 is configured of a positive lens element 21C formed from a spherical glass lens element, a positive lens element 22C formed from a spherical glass lens element, a negative lens element 23C formed from a spherical glass lens element, and a positive lens element 24C formed from a spherical glass lens element, in that order from the object side. The positive lens element 21C is a biconvex positive lens element. The positive lens element 22C is a biconvex positive lens element and the negative lens element 23C is a biconcave negative lens element; the positive lens element (biconvex positive lens element) 22C and the negative lens element (biconcave negative lens element) 23C are cemented to each other. The positive lens element 24C is a positive meniscus lens element having a convex surface on the object side.
The eighth numerical embodiment has the same lens arrangement as that of the first numerical embodiment except for the following features:
(1) The first lens group G1 has a negative refractive power instead of a positive refractive power.
(2) The positive lens element 12 of the first lens group G1 is a positive meniscus lens element, having a convex surface on the image side, that is formed from an aspherical glass molded lens element (having an aspherical surface on each side thereof).
(3) The second lens group G2 is configured of a positive lens element 21D formed from a spherical glass lens element, a positive lens element 22D formed from a spherical glass lens element, a negative lens element 23D formed from a spherical glass lens element, and a positive lens element 24D formed from an aspherical glass molded lens element (having an aspherical surface on each side thereof), in that order from the object side. The positive lens element 21D is a biconvex positive lens element. The positive lens element 22D is a biconvex positive lens element, and the negative lens element 23D is a biconcave negative lens element; the positive lens element (biconvex positive lens element) 22D and the negative lens element (biconcave negative lens element) 23D are cemented to each other. The positive lens element 24D is a biconvex positive lens element.
The ninth numerical embodiment has the same lens arrangement as that of the eighth numerical embodiment except for the following feature:
(1) The positive lens element 24D of the second lens group G2 is a positive meniscus lens element having a convex surface on the object side.
The tenth numerical embodiment has the same lens arrangement as that of the eighth numerical embodiment.
The eleventh numerical embodiment has the same lens arrangement as that of the eighth numerical embodiment except for the following feature:
(1) The biconvex positive lens element 21D of the second lens group G2 is formed from an aspherical glass molded lens element (having an aspherical surface on each side thereof).
The twelfth numerical embodiment has the same lens arrangement as that of the ninth numerical embodiment.
The thirteenth numerical embodiment has the same lens arrangement as that of the ninth numerical embodiment except for the following feature:
(1) The negative lens element 23D of the second lens group G2 is a negative meniscus lens element having a convex surface on the image side.
The numerical values of each condition for each embodiment are shown in Table 53.
As can be understood from Table 53, the first through thirteenth numerical embodiments satisfy conditions (1) through (6). Furthermore, as can be understood from the aberration diagrams, the various aberrations are suitably corrected.
Obvious changes may be made in the specific embodiments of the present invention described herein, such modifications being within the spirit and scope of the invention claimed. It is indicated that all matter contained herein is illustrative and does not limit the scope of the present invention.
Number | Date | Country | Kind |
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2016-052422 | Mar 2016 | JP | national |
This is a continuation application of U.S. patent application Ser. No. 15/450,456, filed Mar. 6, 2017, which claims the benefit of Japanese Patent Application No. 2016-052422, filed on Mar. 16, 2016. The entire disclosure of each of the above-identified applications, including the specification, drawings, and claims, is incorporated herein by reference in its entirety.
Number | Date | Country | |
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Parent | 15450456 | Mar 2017 | US |
Child | 16108825 | US |