Image lens with high resolution, low chromatic aberration, and long flange back distance

Abstract

An image lens includes a first lens and a second lens. The first lens includes a first surface and a second surface. The second lens includes a third surface and a fourth surface. The image lens satisfies: FB/TTL>0.38; R11/F1>2.23; Z/Y>0.11; Z/T<0.42; R23/F2

Description

BACKGROUND

1. Technical Field

The present disclosure relates to lenses and, particularly, to an image lens with high resolution, low chromatic aberration, and long flange back distance.

2. Description of Related Art

Image sensors are used to capture an image. A size of an image sensor, such as a complementary metal oxide semiconductor device (CMOS), decreases with development of technology. To be well matched with such the image sensor, an image lens which is essentially comprised of a number of lenses should be able to meet requirements, such as, high resolution, low chromatic aberration, and long flange back distance (FBD). However, the existing image lenses cannot meet these requirements, thus, result in poor imaging effect.

Therefore, it is desirable to provide an image lens which can overcome the limitations described above.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a schematic view of an image lens in accordance with the present disclosure.

FIG. 2 is a graph showing characteristic curves of spherical aberration of the image lens of FIG. 1 in accordance with a first embodiment.

FIG. 3 is a graph showing characteristic curves of field curvature of the image lens of FIG. 1 in accordance with the first embodiment.

FIG. 4 is a graph showing characteristic curves of distortion of the image lens of FIG. 1 in accordance with the first embodiment.

FIG. 5 is a graph showing characteristic curves of modulation transfer function of the image lens of FIG. 1 in accordance with the first embodiment.

FIG. 6 is a graph showing chief ray angle of the image lens of FIG. 1, in accordance with the first embodiment.

FIG. 7 is a graph showing characteristic curves of spherical aberration of the image lens of FIG. 1 in accordance with a second embodiment.

FIG. 8 is a graph showing characteristic curves of field curvature of the image lens of FIG. 1 in accordance with the second embodiment.

FIG. 9 is a graph showing characteristic curves of distortion of the image lens of FIG. 1 in accordance with the second embodiment.

FIG. 10 is a graph showing characteristic curves of modulation transfer function of the image lens of FIG. 1 in accordance with the second embodiment.

FIG. 11 is a graph showing chief ray angle of the image lens of FIG. 1, in accordance with the second embodiment.

DETAILED DESCRIPTION

Embodiments of the disclosure will now be described in detail with reference to the accompanying drawings.

Referring to FIG. 1, an image lens 100, according to an exemplary embodiment, optically captures an image of an object at an object side and forms a corresponding image at an image side, particularly, at an image plane 60. The image lens 100 includes, in an order from the object side to the image side, a first lens G1 with positive refraction power and a second lens G2 with negative refraction power. The first lens G1 includes a convex first surface 11 facing the object side and a convex second surface 12 facing the image side. The second lens G2 includes a concave third surface 13 facing the object side and a convex fourth surface 14 facing the image side.

The image lens 100 further includes an aperture stop 20 and a filter glass 40. The aperture stop 20 is positioned in the object side of the first lens G1. The filter glass 40 is positioned between the second lens G2 and the image plane 60. The filter glass 40 includes a fifth surface 15 facing the object side and a sixth surface 16 facing the image side. Light rays enter the image lens 100, passing through the aperture stop 20, the first lens G1, the second lens G2, and the filter glass 40, finally forming optical images on the image plane 60. The filter glass 40 filters/removes infrared light from the light rays.

The image lens 100 further includes a cover glass 50. The cover glass 50 is positioned between the filter glass 40 and the image plane 60. The cover glass 50 includes a seventh surface 17 facing the object side and an eighth surface 18 facing the image side.

An image sensor, such as charge coupled device (CCD) or complementary metal-oxide-semiconductor transistor (CMOS), can be positioned on the image plane 60 thus, converting the optically images into electrical signals. The image lens 100 and the image sensor compose a camera module.

The image lens 100 satisfies the formulas:FB/TTL>0.38;  (1)R11/F1>2.23;  (2)Z/Y>0.11;  (3)Z/T<0.42;  (4)R23/F2<R12/F2<R24/F2;  (5)

wherein FB is a distance between the fourth surface 14 and the image plane 60 along an optical axis of the image lens 100, TTL is a total length of the image lens 100, Z is a distance from a central point of the fourth surface 14 to an outer edge of the fourth surface 14 along the optical axis, Y is a distance from the central point of the fourth surface 14 to the outer edge of the fourth surface 14 along a direction perpendicular to the optical axis, the central point is positioned at centre of a circle formed by the outer edge of the fourth surface 14, T is thickness of the second lens G2 along the optical axis, R23 is the curvature radius of the third surface 13, R24 is the curvature radius of the fourth surface 14, R11 is the curvature radius of the first surface 11, R12 is the curvature radius of the second surface 12, and F2 is focal length of the second lens G2.

Formula (1) is for maintaining a long flange back distance. Formula (2) is for decreasing the refraction power of the first lens G1, and then decreasing the core shift sensitivity of the image lens 100. Formulas (3) and (5) are for properly distributing the refraction power, while maintaining a relatively small spherical aberration. Formula (4) is convenient for injection molding of the second lens G2. If the image lens 100 does not satisfy the formulas (1) to (5), the flange back distance of the image lens 100 cannot be maintained and the images captured by the image lens 100 cannot be corrected.

The image lens 100 further satisfies the formula:R12/F2<0.36;  (6)R23/F2<0.27;  (7)R24/F2<0.46.  (8)

Formulas (6), (7), and (8) are for maintaining quality of images captured by the image lens 100. If the image lens 100 does not satisfy the formulas (6) to (8), the images captured by the image lens 100 cannot be corrected.

The image lens 100 further satisfies the formulas:Vd1>53;  (9)Vd2<33;  (10)Wherein Vd1 is the Abbe number of the first lens G1 and Vd2 is the Abbe number of the second lens G2. Formulas (9) and (10) are for correcting chromatic aberration of the image lens 100. If the image lens 100 does not satisfy the formulas (9) and (10), the images captured by the image lens 100 will have a greater chromatic aberration.

All of the first, second, third and fourth surfaces 11, 12, 13 and 14 are aspherical surfaces. Each aspherical surface is shaped according to the formula:

$Z=\frac{{\mathrm{ch}}^2}{1+\sqrt{1-\left(k+1\right)c^2{h}^2}}+\sum ^{}{A}_i{h}^i$

wherein Z is the length of a line drawn from a point on the aspherical surface to the tangential plane of the aspherical surface, h is the height from the optical axis to the point on the aspherical surface, c is a vertex curvature (=1/R, the radius of curvature), k is a conic constant, and Ai are the correction coefficients, to the order of “i” of the aspherical surface.

Detailed examples of the imaging lens 100 are given below in accompany with FIGS. 2-9, but it should be noted that the imaging lens 100 is not limited by these examples. Listed below are the symbols used in these detailed examples:

FNo: F number;

2ω: field angle;

ri: radius of curvature of the surface Si;

Di: distance between surfaces on the optical axis of the surface Si and the surface Si+1;

Ni: refractive index of the surface Si;

Vi: Abbe constant of the surface Si;

Ki: Secondary curvature of the surface Si.

EXAMPLE 1

Tables 1-3 show a first embodiment of the image lens 100.

TABLE 1
Surface	type	ri (mm)	Di (mm)	ni	vi	ki
aperture	standard	Infinity	0.04	—	—	—
stop 20
first	aspherical	1.26	0.56	1.53	56.0	0
surface 11
second	aspherical	−0.32	0.11	—	—	−1.88
surface 12
third	aspherical	−0.20	0.30	1.58	31.0	−0.81
surface 13
fourth	aspherical	−0.43	0.05	—	—	−2.75
surface 14
fifth	standard	Infinity	0.21	1.52	58.6	—
surface 15
sixth	standard	Infinity	0.25	—	—	—
surface 16
seventh	standard	Infinity	0.40	1.52	58.6	—
surface 17
eighth	standard	Infinity	0.05	—	—	—
surface 18
image	standard	—	—	—	—	—
plane 60

TABLE 2
aspherical	first surface	second surface	third surface	fourth surface
coefficient	11	12	13	14
A4	−2.0470	−1.6863	12.0693	0.1871
A6	41.7808	−3.0153	−24.2071	10.7301
A8	−1287.0617	−0.6344	82.5397	−35.3923
A10	9872.2407	29.3975	266.907	46.8491

TABLE 3
F(mm)	F/No	2ω
1.18	2.78	61°

In the embodiment, FB=0.96 mm; TTL=1.97 mm; Z=0.093 m; Y=0.43 mm; T=0.3 mm; F1=0.54 mm; F2=−1.21 mm.

As shown in FIG. 2, curves F, d, C, e, g, and h are respective spherical aberration characteristic curves of F light (wavelength: 486.1 nm), d light (wavelength: 587.6 nm), and C light (wavelength: 656.3 nm), e light (wavelength: 546.1 nm), and g light (wavelength: 435.8 nm), of the first embodiment. In this embodiment, spherical aberration of visible light (400-700 nm) of the image lens 100 is in a range of: −0.1 mm˜0.1 mm. As shown in FIG. 3, the curves T and S are the tangential field curvature curve and the sagittal field curvature curve, respectively. In this embodiment, field curvature of the image lens 100 is limited to a range of: −0.10 mm˜0.10 mm. In addition, as shown in FIG. 4, distortion of the image lens 100 is limited in a range of: 0%˜2.00%. Furthermore, as shown in FIG. 5, for half of the Nyquist frequency (about 1431 p/mm), the MTF of the central field is greater than 46% (see curve mc), the MTF of the 0.8 field is greater than 63% (see curve mp), the MTF between the central field and the 0.8 field is in a range of: 46%-63% (see curve mt, for example). As shown in FIG. 6, the chief ray angle of the image lens 100 of the first embodiment is limited in a range of: 0˜24.0 degrees. Overall, in this embodiment, the spherical aberration, the field curvature, the distortion, and the chief ray angle are limited in a small range.

EXAMPLE 2

Tables 4-6 show a second embodiment of the image lens 100.

TABLE 4
Surface	type	ri (mm)	Di (mm)	ni	vi	ki
aperture	standard	Infinity	0.04	—	—	—
stop 20
first	aspherical	1.31	0.55	1.53	56.0	−1.50
surface 11
second	aspherical	−0.31	0.12	—	—	−1.73
surface 12
third	aspherical	−0.19	0.30	1.58	31.0	−0.83
surface 13
fourth	aspherical	−0.42	0.05	—	—	−2.32
surface 14
fifth	standard	Infinity	0.21	1.52	58.6	—
surface 15
sixth	standard	Infinity	0.25	—	—	—
surface 16
seventh	standard	Infinity	0.40	1.52	58.6	—
surface 17
eighth	standard	Infinity	0.05	—	—	—
surface 18
image	standard	—	—	—	—	—
plane 60

TABLE 5
aspherical	first	second	third	fourth
coefficient	surface 11	surface 12	surface 13	surface 14
A4	−2.2994	−1.3780	12.4122	0.6127
A6	44.0334	−5.0957	−20.2905	8.1667
A8	−1387.1406	−21.2107	46.8574	−20.4456
A10	1.10E+04	302.6287	401.0828	12.4839
A12	−2.24E−06	−553.1794	12.4839	5.5424

TABLE 6
F(mm)	F/No	2ω
1.18	2.77	60. 85°

In the embodiment, FB=0.96 mm; TTL=1.97 mm; Z=0.097 mm; Y=0.43 mm; T=0.30 mm; F1=0.53 mm; F2=−1.19 mm.

As shown in FIG. 7, curves F, d, C, e, g, and h are respective spherical aberration characteristic curves of F light (wavelength: 486.1 nm), d light (wavelength: 587.6 nm), and C light (wavelength: 656.3 nm), e light (wavelength: 546.1 nm), and g light (wavelength: 435.8 nm), of the second embodiment. In this embodiment, spherical aberration of visible light (400-700 nm) of the image lens 100 is in a range of: −0.1 mm˜0.1 mm. As shown in FIG. 8, the curves T and S are the tangential field curvature curve and the sagittal field curvature curve, respectively. In this embodiment, field curvature of the image lens 100 is limited to a range of: −0.10 mm˜0.10 mm. In addition, as shown in FIG. 9, distortion of the image lens 100 is limited in a range of: 0%˜2.00%. Furthermore, as shown in FIG. 10, for half of the Nyquist frequency (about 1431 p/mm), the MTF of the central field is greater than 46% (see curve mc), the MTF of the 0.8 field is greater than 63% (see curve mp), the MTF between the central field and the 0.8 field is in a range of: 46%˜63% (see curve mt, for example). As shown in FIG. 11, the chief ray angle of the image lens 100 of the second embodiment is limited in a range of: 0˜24.0 degrees. Overall, in this embodiment, the spherical aberration, the field curvature, the distortion, and the chief ray angle are limited in a small range.

Particular embodiments are shown and described by way of illustration only. The principles and the features of the present disclosure may be employed in various and numerous embodiments thereof without departing from the scope of the disclosure as claimed. The above-described embodiments illustrate the scope of the disclosure but do not restrict the scope of the disclosure.

Claims

1. An image lens for imaging an object on an image plane, in the order from the object side to the image side thereof, comprising: a first lens having positive refraction power and comprising a first surface facing the object side and a second surface facing the image side; anda second lens having negative refraction power and comprising a third surface facing the object side and a fourth surface facing the image side;wherein the image lens satisfies the following formulas: FB/TTL>0.38;  (1)R11/F1>2.23;  (2)Z/Y>0.11;  (3)Z/T<0.42;  (4)R23/F2<R12/F2<R24/F2;  (5)wherein FB is a distance between the fourth surface and the image plane along an optical axis of the image lens, TTL is a total length of the image lens, Z is a distance from a central point of the fourth surface to an outer edge of the fourth surface along the optical axis of the image lens, Y is a distance from the central point of the fourth surface to the outer edge of the fourth surface along a direction perpendicular to the optical axis of the image lens, T is a thickness of the second lens on the optical axis, R23 is a curvature radius of the third surface, R24 is a curvature radius of the fourth surface, R11 is a curvature radius of the first surface; R12 is a curvature radius of the second surface, and F2 is a focal length of the second lens.

2. The image lens as claimed in claim 1, wherein the image lens further satisfies the formulas: R12/F2<0.36;  (6)R23/F2<0.27;  (7)R24/F2<0.46  (8).

3. The image lens as claimed in claim 1, wherein the image lens further satisfies the formulas: Vd1>53; and  (9)Vd2<33;  (10)wherein Vd1 is the Abbe number of the first lens, and Vd2 is the Abbe number of the second lens.

4. The image lens as claimed in claim 1, wherein the first lens and the second lens are aspherical lenses.

5. The image lens as claimed in claim 4, wherein the first surface is a convex surface facing the object side, the second surface is a convex surface facing the image side, the third surface is a concave surface facing the object side, and the fourth surface is a convex surface facing the image side.

6. The image lens as claimed in claim 1, wherein the image lens further comprises an aperture stop positioned at the objected side of the first lens.

7. The image lens as claimed in claim 1, further comprising a filter glass, wherein the filter glass is positioned between the second lens and the image plane.

8. The image lens as claimed in claim 7, further comprising a cover glass, wherein the cover glass is positioned between the filter glass and the image plane.

9. The image lens as claimed in claim 1, wherein the central point is positioned at a centre of a circle formed by the outer edge of the fourth surface.