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US 8,797,659 B2Granted
Macro lens and imaging apparatus
AssigneeKonica Minolta Optics, Inc.
InventorYoshihito Souma
Life of this patent
Estimating the term…
Abstract
A macro lens and an imaging apparatus include, in the order from an object side to an image side, a first lens group, a second lens group, and a third lens group. Focusing is performed by fixing the first lens group and the third lens group, and by moving the second lens group having a positive refractive power as a whole on the optical axis in focusing from an infinite object to a close distance object. The first lens group has a plane S1 and a plane S2 of curvature radii of a same sign and satisfying a specified condition.
Claims13
A macro lens comprising, in the order from an object side to an image side:
- a first lens group;
- a second lens group having a positive refractive power as a whole;
- and
- a third lens group, wherein
- the first lens group includes a plane S1 and a plane S2 having curvature radii of a same sign and defined by the following conditional expressions (1) through (3), and
- focusing is performed by fixing the first lens group and the third lens group, and by moving the second lens group on an optical axis in focusing from an infinite object to a close distance object,
- 0.6<M2/f2<1 (1)
- (φinf−φnear)f2<−0.0002 (2)
- e0/f2<0.15 (3)
- where
- M2:
- a moving amount of the second lens group from an infinite distance to a closest distance,
- f2:
- a focal length of the second lens group,
- e0:
- an air equivalent distance between the plane S1 and the plane S2 on the optical axis,
- φinf:
- a combined optical power of the plane S1 and the plane S2 in a direction parallel to the optical axis, and an optical power to be defined by the following conditional expression (4A), assuming that Yinf is a height of a light ray of a light flux from the optical axis, the light ray passing a center of an aperture stop and intersecting the plane S1, the light flux forming an image having a maximum image height at a time of forming an infinite object,
- φinf=(φ1(Yinf)+φ2(Yinf)−φ1(Yinf)φ2(Yinf)e(Yinf))/n3 (4A)
- assuming that n1 is a refractive index of an object-side medium of the plane S1 for a d-line, n2 is a refractive index of a medium between the plane S1 and the plane S2 for the d-line, n3 is a refractive index of an image-side medium of the plane S2 for the d-line, C1(Y) is a curvature of the plane S1 at a height Y, C2(Y) is a curvature of the plane S2 at the height Y, and e(Y) is an air equivalent distance (air equivalent plane interval) between the plane S1 and the plane S2 in the direction parallel to the optical axis with respect to the height Y,
- φ1(Y) is an optical power of the plane S1 at the height Y from the optical axis, and is an optical power to be defined by the following conditional expression (5), and
- φ2(Y) is an optical power of the plane S2 at the height Y from the optical axis, and is an optical power to be defined by the following conditional expression (6),
- φ1(Y)=(n2−n1)C1(Y) (5)
- φ2(Y)=(n3−n2)C2(Y) (6)
- where
- φnear:
- a combined optical power of the plane S1 and the plane S2 in the direction parallel to the optical axis, and an optical power to be defined by the following conditional expression (4B), assuming that Ynear is a height of a light ray of a light flux from the optical axis, the light ray passing a center of an aperture stop and intersecting the plane S1, the light flux forming an image having a maximum image height at a time of forming a closest distance object,
- φnear=(φ1(Ynear)+φ2(Ynear)−φ1(Ynear)φ2(Ynear)e(Ynear))/n3 (4B).
25 more elements
Dependencies are inferred from the claim text.