Imaging lens
An imaging lens ( 100 ) comprising, arranged sequentially from the object side, a positive-meniscus first lens ( 1 ) with its convex plane facing the object side, a negative-power-meniscus second lens ( 2 ), and a positive-power third lens ( 3 ), the second and third lenses ( 2, 3 ) functioning as correction lenses. The first lens ( 1 ) has a strong power, and both the second and third lenses ( 2, 3 ) are aspherical on opposite planes. When the synthetic focal distance of the imaging lens is f, the focal distance of the first lens f1, the distance from the incident surface on the object side to the imaging surface of the first lens ( 1 ) Σd, and the Abbe number of the second lens √d2, the following conditional expressions are satisfied. 0.50<f1/f<1.5 (1) 0.50<Σd/f<1.5 (2) 50>√d2 (3). Accordingly, a small, low-cost imaging lens capable of high-quality imaging can be realized.
1. An imaging lens comprising a first lens, a second lens, and a third lens arranged in sequence from an object side, wherein
the first lens is a meniscus lens having a positive power, whose convex surface faces the object side;
the second lens is a meniscus lens having a positive or negative power, whose concave surface faces the object side;
the third lens is a lens having a positive power; and
a shape of at least one of the lens surfaces of the first, second, and third lenses is determined by an aspherical shape in which an inflection point does not appear within an effective lens surface region thereof, and wherein
the following two conditions are satisfied when a curvature of the lens surface of the third lens on the object side is Ra, a radius of curvature of the lens surface thereof on the image side is Rb, a total focal distance of the imaging lens is f and a focal distance of the first lens is f1:
1.0<| Rb/Ra | and 0.5< f 1/ f< 1.5.
2. The imaging lens according to claim 1 , wherein the following condition is satisfied when a back focus of the imaging lens is BF:
0.25< BF/f< 1.0.
3. The imaging lens according to claim 2 , wherein a maximum exit angle of a principal ray is 30 degrees or less.