ZOOM LENS

Abstract

The present invention relates to the field of optical lenses and provides a zoom lens consisting of, from an object side to an image side in sequence, a first lens having negative refractive power, a second lens group having positive refractive power, a fifth lens having positive refractive power, and a sixth lens having negative refractive power. During zooming, a distance between adjacent lenses or between lens and adjacent lens group in a direction of an optic axis varies. The second lens group consists of a second lens having positive refractive power, a third lens having negative refractive power, and a fourth lens having negative refractive power, and following conditions are satisfied: f_Tele/f_Wide≥1.80; −1.75≤f3/f2≤−1.35; −1.75≤f4/f2≤−1.35. The present invention becomes compact when contracted, while during imaging, FNO is bright, and has good optical properties.

Claims

1. A zoom lens consists of, from an object side to an image side in sequence: a first lens having negative refractive power, a second lens group having positive refractive power, a fifth lens having positive refractive power, and a sixth lens having negative refractive power; wherein, among the first lens, the second lens group, the fifth lens, and the sixth lens, a distance between adjacent lenses or between lens and adjacent lens group in a direction of an optic axis varies during zooming; the second lens group consists of a second lens having positive refractive power, a third lens having negative refractive power, and a fourth lens having negative refractive power, and the zoom lens satisfies the following conditions:
f_Tele/f_Wide≥1.80;
−1.75≤f3/f2≤−1.35;
−1.75≤f4/f2≤−1.35; where, f_Wide denotes a total optical length of the zoom lens at a wide-angle end; f_Tele denotes a total optical length of the zoom lens at a telephoto end; f2 denotes a focal length of the second lens; f3 denotes a focal length of the third lens; and f4 denotes a focal length of the fourth lens.

2. The zoom lens according to claim 1, wherein the zoom lens further satisfies a following condition:
−1.30≤f1/fG2≤−1.00; where, f1 denotes a focal length of the first lens; and fG2 denotes a combined focal length of the second lens group.

3. The zoom lens according to claim 1, wherein the zoom lens further satisfies a following condition:
0.30≤f5/fG2≤0.40; where, f5 denotes a focal length of the fifth lens; and fG2 denotes a combined focal length of the second lens group.

4. The zoom lens according to claim 1, wherein the zoom lens further satisfies a following condition:
−1.50≤f6/fG2≤−1.00; where, f6 denotes a focal length of the sixth lens; and fG2 denotes the combined focal length of the second lens group.

5. The zoom lens according to claim 1, wherein the zoom lens further satisfies a following condition:
4.00≤LB_Tele/LB_Wide≤5.00; where, LB_Wide denotes an on-axis distance from an image side surface of the sixth lens to an image surface, at the wide-angle end; and LB_Tele denotes the on-axis distance from the image side surface of the sixth lens to the image surface, at the telephoto end.

6. The zoom lens according to claim 1, wherein the zoom lens further satisfies a following condition:
76.00≤v1≤82.00, where, v1 denotes an Abbe number of the first lens.

7. The zoom lens according to claim 1, wherein the first lens is a glass lens.

Description

BRIEF DESCRIPTION OF DRAWINGS

[0016] In order to more clearly illustrate the technical solutions in the embodiments of the present disclosure, the following will briefly describe the accompanying drawings used in the description of the embodiments. Obviously, the accompanying drawings in the following description are only some embodiments of the present disclosure. For a person of ordinary skill in the art, other drawings may be obtained from these drawings without creative work.

[0017] FIG. 1 is a schematic diagram of a general structure of a zoom lens LA according to Embodiment 1 of the present invention.

[0018] FIG. 2 is a schematic diagram of a longitudinal aberration, an astigmatism field curvature and a distortion of the zoom lens LA at a wide-angle end according to Embodiment 1 of the present invention.

[0019] FIG. 3 is a schematic diagram of a longitudinal aberration, an astigmatism field curvature and a distortion of the zoom lens LA at a telephoto end according to Embodiment 1 of the present invention.

[0020] FIG. 4 is a schematic diagram of a general structure of a zoom lens LA according to Embodiment 2 of the present invention.

[0021] FIG. 5 is a schematic diagram of a longitudinal aberration, an astigmatism field curvature and a distortion of the zoom lens LA at a wide-angle end according to Embodiment 2 of the present invention.

[0022] FIG. 6 is a schematic diagram of a longitudinal aberration, an astigmatism field curvature and a distortion of the zoom lens LA at a telephoto end according to Embodiment 2 of the present invention.

[0023] FIG. 7 is a schematic diagram of a general structure of a zoom lens LA according to Embodiment 3 of the present invention.

[0024] FIG. 8 is a schematic diagram of a longitudinal aberration, an astigmatism field curvature and a distortion of the zoom lens LA at a wide-angle end according to Embodiment 3 of the present invention.

[0025] FIG. 9 is a schematic diagram of a longitudinal aberration, an astigmatism field curvature and a distortion of the zoom lens LA at a telephoto end according to Embodiment 3 of the present invention.

[0026] FIG. 10 is a schematic diagram of a general structure of a zoom lens LA according to Embodiment 4 of the present invention.

[0027] FIG. 11 is a schematic diagram of a longitudinal aberration, an astigmatism field curvature and a distortion of the zoom lens LA at a wide-angle end according to Embodiment 4 of the present invention.

[0028] FIG. 12 is a schematic diagram of a longitudinal aberration, an astigmatism field curvature and a distortion of the zoom lens LA at a telephoto end according to Embodiment 4 of the present invention.

[0029] FIG. 13 is a schematic diagram of a general structure of a zoom lens LA according to Embodiment 5 of the present invention.

[0030] FIG. 14 is a schematic diagram of a longitudinal aberration, an astigmatism field curvature and a distortion of the zoom lens LA at a wide-angle end according to Embodiment 5 of the present invention.

[0031] FIG. 15 is a schematic diagram of a longitudinal aberration, an astigmatism field curvature and a distortion of the zoom lens LA at a telephoto end according to Embodiment 5 of the present invention.

DETAILED DESCRIPTION OF EMBODIMENTS

[0032] To make the objectives, technical solutions, and advantages of the present disclosure clearer, embodiments of the present disclosure are described in detail with reference to accompanying drawings in the following. A person of ordinary skill in the art can understand that, in the embodiments of the present disclosure, many technical details are provided to make readers better understand the present disclosure. However, even without these technical details and any changes and modifications based on the following embodiments, technical solutions required to be protected by the present disclosure can be implemented.

[0033] Embodiments of the zoom lens in the present invention are described below. The zoom lens LA has lens system of a lens structure having six pieces in four groups. The lens structure of six pieces in four groups, comprises from an object side to an image side in sequence, a first lens L1, a second lens group G2, a fifth lens L5, and a sixth lens L6. The second lens group G2 consists of a second lens L2, a third lens L3, and a fourth lens L4. A glass plate GF is provided between the sixth lens L6 and an image surface. The glass plate GF can be a glass cover plate or any optical filter. In the present invention, the glass plate GF can be provided at different positions, or can be omitted.

[0034] The first lens L1 has negative refractive power, the second lens group G2 has positive refractive power, the fifth lens L5 has positive refractive power, and the sixth lens L6 has negative refractive power. The second lens group G2 consists of the second lens L2, the third lens L3, and the fourth lens L4, the second lens L2 has positive refractive lens, the third lens L3 has negative refractive power, and the fourth lens L4 has negative refractive power. In order to correct various aberrations, it is desirable to design all surfaces of these six lenses as aspherical surfaces.

[0035] The zoom lens LA satisfies the following condition (1):

f_Tele/f_Wide≥1.80  (1)

[0036] The condition (1) specifies a zoom ratio of the zoom lens LA. When the condition (1) is satisfied, correction of each aberration is easily realized, and the zoom ratio becomes sufficient, which is an improvement.

[0037] The zoom lens LA satisfies the following condition (2):

−1.75≤f3/f2≤−1.35  (2).

[0038] The condition (2) specifies a ratio of a focal length f3 of the third lens L3 to a focal length f2 of the second lens L2. If it is within the range of condition (2), miniaturization in the contracted state and correction of each aberration at the wide-angle end with FNO≤2.0 and zoom ratio ≥1.80 are easily achieved, which is an improvement.

[0039] The zoom lens LA satisfies the following condition (3):

−1.75≤f4/f2≤−1.35  (3)

[0040] The condition (3) specifies a ratio of a focal length f4 of the fourth lens L4 to a focal length f2 of the second lens L2. If it is within the range of condition (3), miniaturization in the contracted state and correction of each aberration at the wide-angle end with FNO≤2.0 and zoom ratio ≥1.80 are easily achieved, which is an improvement.

[0041] The zoom lens LA satisfies the following condition (4).

−1.30≤f1/fG2≤−1.00  (4)

[0042] The condition (4) specifies a ratio of a focal length f1 of the first lens L1 to a combined focal length fG2 of the second lens group G2. If it is within the range of condition (4), miniaturization in the contracted state and correction of each aberration at the wide-angle end with FNO≤2.0 and zoom ratio ≥1.80 are easily achieved, which is an improvement.

[0043] The zoom lens LA satisfies the following condition (5).

0.30≤f5/fG2≤0.40  (5)

[0044] The condition (5) specifies a ratio of a focal length f5 of the fifth lens L5 to a combined focal length fG2 of the second lens group G2. If it is within the range of condition (5), miniaturization in the contracted state and correction of each aberration at the wide-angle end with FNO≤2.0 and zoom ratio ≥1.80 are easily achieved, which is an improvement.

[0045] The zoom lens LA satisfies the following condition (6).

−1.50≤f6/fG2≤−1.00  (6)

[0046] The condition (6) specifies a ratio of the focal length f6 of the sixth lens L6 to the combined focal length fG2 of the second lens group G2. If it is within the range of condition (6), miniaturization in the contracted state and correction of each aberration at the wide-angle end with FNO≤2.0 and zoom ratio ≥1.80 are easily achieved, which is an improvement.

[0047] The zoom lens LA satisfies the following condition (7).

4.00≤LB_Tele/LB_Wide≤5.00  (7)

[0048] The condition (7) specifies a ratio of an on-axis distance LB_Tele from the image side surface S12 of the sixth lens L6 to the image surface at the telephoto end to an on-axis distance LB_Wide from the image side surface S12 of the sixth lens L6 to the image surface at the wide-angle end. If it is within the range of condition (7), miniaturization in the contracted state and correction of each aberration at the wide-angle end with FNO≤2.0 and zoom ratio ≥1.80 are easily achieved, which is an improvement.

[0049] The zoom lens LA satisfies the following condition (8).

76.00≤v1≤82.00  (8)

[0050] The condition (8) specifies an Abbe number of the first lens L1. If it is within the range of the condition (8), miniaturization in the contracted state and correction of each aberration at the wide-angle end with FNO≤2.0 and zoom ratio ≥1.80 are easily achieved, which is an improvement.

[0051] The six lenses in four groups that form the zoom lens LA satisfy the above structure as well as the conditions, respectively, so that it is possible to obtain such a zoom lens as follows: the zoom lens becomes compact as TTL≤8.00 mm in the contracted state; while during imaging, the zoom lens becomes bright as FNO≤2.0 at a wide-angle end; and the zoom lens has good optical properties as well as a zoom ratio ≥1.80, and consists of six lenses in four groups.

EMBODIMENTS

[0052] The zoom lens LA the present invention will be described with reference to the embodiments below. The reference signs described in the embodiments are listed below. In addition, the distance, radius and center thickness are all in a unit of mm.

[0053] f denotes a focal length of the zoom lens LA.

[0054] f1 denotes a focal length of the first lens L1.

[0055] fG2 denotes a combined focal length of the second lens group G2.

[0056] f2 denotes a focal length of the second lens L2.

[0057] f3 denotes a focal length of the third lens L3.

[0058] f4 denotes a focal length of the fourth lens L4.

[0059] f5 denotes a focal length of the fifth lens L5.

[0060] f6 denotes a focal length of the sixth lens L6.

[0061] FNO denotes an aperture value (a ratio of an effective focal length of the zoom lens to a diameter of a pupil of entry), or F number.

[0062] 2ω denotes a full field of view.

[0063] STOP denotes an aperture.

[0064] R denotes a curvature radius of an optical surface, or a central curvature radius for a lens.

[0065] R1 denotes a curvature radius of an object side surface S1 of the first lens L1.

[0066] R2 denotes a curvature radius of an image side surface S2 of the first lens L1.

[0067] R3 denotes a curvature radius of an object side surface S3 of the second lens L2.

[0068] R4 denotes a curvature radius of an image side surface S4 of the second lens L2.

[0069] R5 denotes a curvature radius of an object side surface S5 of the third lens L3.

[0070] R6 denotes a curvature radius of an image side surface S6 of the third lens L3.

[0071] R7 denotes a curvature radius of an object side surface S7 of the fourth lens L4.

[0072] R8 denotes a curvature radius of an image side surface S8 of the fourth lens L4.

[0073] R9 denotes a curvature radius of an object side surface S9 of the fifth lens L5.

[0074] R10 denotes a curvature radius of the image side surface S10 of the fifth lens L5.

[0075] R11 denotes a curvature radius of the object side surface S11 of the sixth lens L6.

[0076] R12 denotes a curvature radius of an image side surface S12 of the sixth lens L6.

[0077] R13 denotes a curvature radius of an object side surface S13 of the glass plate GF.

[0078] R14 denotes a curvature radius of an image side surface S14 of the glass plate GF.

[0079] d denotes an on-axis thickness or an on-axis distance between lenses.

[0080] d1 denotes an on-axis thickness of the first lens L1.

[0081] D12 denotes an on-axis distance from the image side surface S2 of the first lens L1 to the object side surface S3 of the second lens L2.

[0082] d2 denotes an on-axis distance from the image side surface S2 of the first lens L1 to the aperture STOP.

[0083] d3 denotes an on-axis distance from the aperture STOP to the object side surface S3 of the second lens L2.

[0084] d4 denotes an on-axis thickness of the first lens L2.

[0085] d5 denotes an on-axis distance from the image side surface S4 of the second lens L2 to the object side surface S5 of the third lens L3.

[0086] d6 denotes an on-axis thickness of the third lens L3.

[0087] d7 denotes an on-axis distance from the image side surface S6 of the third lens L3 to the object side surface S7 of the fourth lens L4.

[0088] d8 denotes an on-axis thickness of the fourth lens L4.

[0089] d9 denotes an on-axis distance from the image side surface S8 of the fourth lens L4 to the object side surface S9 of the fifth lens L5.

[0090] d10 denotes an on-axis thickness of the fifth lens L5.

[0091] d11 denotes an on-axis distance from the image side surface S10 of the fifth lens L5 to the object side surface S11 of the sixth lens L6.

[0092] d12 denotes an on-axis thickness of the sixth lens L6.

[0093] d13 denotes an on-axis distance from the image side surface S12 of the sixth lens L6 to the object side surface S13 of the glass plate GF.

[0094] d14 denotes an on-axis thickness of the glass plate GF.

[0095] d15 denotes an on-axis distance from the image side surface S14 of the glass plate GF to an image plane.

[0096] nd denotes a refractive index of d line.

[0097] nd1 denotes a refractive index of d line of the first lens L1.

[0098] nd2 denotes a refractive index of d line of the second lens L2.

[0099] nd3 denotes a refractive index of d line of the third lens L3.

[0100] nd4 denotes a refractive index of d line of the fourth lens L4.

[0101] nd5 denotes a refractive index of d line of the fifth lens L5.

[0102] nd6 denotes a refractive index of d line of the sixth lens L6.

[0103] ndg denotes a refractive index of d line of the glass plate GF.

[0104] v denotes an abbe number.

[0105] v1 denotes an abbe number of the first lens L1.

[0106] v2 denotes an abbe number of the second lens L2.

[0107] v3 denotes an abbe number of the third lens L3.

[0108] v4 denotes an abbe number of the fourth lens L4.

[0109] v5 denotes an abbe number of the fifth lens L5.

[0110] v6 denotes an abbe number of the sixth lens L6.

[0111] vg denotes an abbe number of the glass plate GF.

[0112] TTL denotes a total optical length (on-axis distance from the object side surface S1 of the first lens L1 to the image surface) of the camera lens. and

[0113] LB denotes an on-axis distance from the image side surface S12 of the sixth lens L6 to the image surface.

[0114] IH denotes an image height.

Embodiment 1

[0115] FIG. 1 is a schematic diagram of a zoom lens LA according to Embodiment 1 of the present invention. The curvature radiuses R of the image side surfaces and object side surfaces of the first lens L1 to the sixth lens L6 of the camera lens LA according to the Embodiment 1, the on-axis thicknesses of the lenses, or on-axis distances d between the lenses, refractive indexes nd, abbe numbers vd are shown in Table 1. Values of A-D during imaging and in the contracted state are shown in Table 2; conic coefficients k and aspheric coefficients are shown in Table 3; and FNO, 2ω, f, TTL, LB, f1, fG2, f2, f3, f4,

TABLE-US-00001 TABLE 1 R d nd νd Effective radius (mm) S1 R1 7.67105 d1 0.719 nd1 1.5264 ν1 76.860 4.535 S2 R2 4.27375 D12 d2 A 3.923 Stop ∞ d3 −1.261  2.667 S3 R3 3.31060 d4 2.201 nd2 1.5438 ν2 56.029 2.670 S4 R4 −10.44730 d5 0.353 2.504 S5 R5 4.55214 d6 0.411 nd3 1.6153 ν3 25.936 2.154 S6 R6 2.35630 d7 0.583 1.890 S7 R7 −8.09266 d8 0.386 nd4 1.6700 ν4 19.392 1.878 S8 R8 11.80297 d9 B 1.845 S9 R9 7.55688  d10 0.783 nd5 1.6153 ν5 25.936 1.935 S10 R10 −7.66352  d11 C 1.906 S11 R11 10.46885  d12 0.400 nd6 1.5346 ν6 55.695 2.633 S12 R12 5.67503  d13 0.173 2.909 S13 R13 ∞  d14 0.210 ndg 1.5168 νg 64.167 2.974 S14 R14 ∞  d15 D 3.010 Reference wavelength = 587.6 nm

TABLE-US-00002 TABLE 2 Imaging Wide Tele Contracted A 9.953 1.478 1.461 B 0.225 0.633 0.200 C 4.122 1.591 0.360 D 1.040 6.661 0.890

TABLE-US-00003 TABLE 3 Cone coefficient Aspheric surface coefficient k A4 A6 A8 A10 S1 0.0000E+00 −5.7385E−03 3.6299E−04 −2.0970E−05 1.3349E−06 S2 0.0000E+00 −8.2258E−03 6.3034E−04 −9.4459E−05 1.2558E−05 S3 −3.0952E−01 7.4776E−04 5.9198E−04 −4.1787E−04 1.7321E−04 S4 0.0000E+00 1.2256E−02 −2.4500E−03 5.9863E−04 −1.3437E−04 S5 0.0000E+00 −3.8659E−02 3.8995E−03 1.7269E−03 −9.8686E−04 S6 −7.6118E+00 −3.3312E−03 −1.7005E−02 1.4689E−02 −6.6600E−03 S7 −5.0000E+01 7.0086E−03 3.1047E−03 −2.8514E−03 1.8458E−03 S8 0.0000E+00 3.9299E−02 −1.6687E−02 9.4272E−03 −3.0949E−03 S9 0.0000E+00 2.8733E−02 −2.7964E−02 1.9781E−02 −8.2089E−03 S10 0.0000E+00 2.9511E−02 −3.5157E−02 3.2777E−02 −1.7888E−02 S11 −1.0888E+01 −1.7153E−02 2.6433E−03 −3.2400E−04 4.3365E−05 S12 −3.0710E+01 −5.1779E−03 −1.6955E−03 7.6430E−04 −1.4174E−04 Cone coefficient Aspheric surface coefficient k A12 A14 A16 S1 0.0000E+00 −8.1503E−08 3.1114E−09 −4.9180E−11 S2 0.0000E+00 −1.1269E−06 5.4030E−08 −1.0782E−09 S3 −3.0952E−01 −3.7552E−05 4.1525E−06 −1.9096E−07 S4 0.0000E+00 1.6965E−05 −1.2495E−06 4.1593E−08 S5 0.0000E+00 2.3274E−04 −2.6947E−05 1.3007E−06 S6 −7.6118E+00 2.0674E−03 −3.7602E−04 3.0038E−05 S7 −5.0000E+01 −5.7675E−04 8.1320E−05 −4.3265E−06 S8 0.0000E+00 5.0214E−04 −3.6684E−05 6.1773E−07 S9 0.0000E+00 2.0668E−03 −2.9319E−04 1.9034E−05 S10 0.0000E+00 5.7863E−03 −1.0236E−03 7.7626E−05 S11 −1.0888E+01 −1.2835E−05 1.8482E−06 −9.0136E−08 S12 −3.0710E+01 9.1737E−06 1.6138E−07 −2.8105E−08 Herein, K is a conic coefficient, A4, A6, A8, A10, A12, A14, and A16 are aspheric surface coefficients.

y=(x.sup.2/R)/[1+{1−(k+1)(x.sup.2/R.sup.2)}.sup.1/2]+A4x.sup.4+A6x.sup.6+A8x.sup.8+A10x.sup.10+A12x.sup.12±A14x.sup.14+A16x.sup.16  (9)

[0116] Herein, x is a vertical distance between a point on an aspherical curve and the optic axis, and y is an aspherical depth (a vertical distance between a point on an aspherical surface, having a distance of x from the optic axis, and a surface tangent to a vertex of the aspherical surface on the optic axis).

[0117] For convenience, an aspheric surface of each lens surface adopts the aspheric surfaces shown in the condition (9). However, the present invention is not limited to the aspherical polynomials form shown in the condition (8).

TABLE-US-00004 TABLE 4 Wide Tele Fno  1.96 2.84 2ω (°) 46.29 24.00 f (mm)  7.110 14.536 Wide Tele Contracted TTL (mm) 20.298 15.323 7.870 LB (mm)  1.423  7.044 1.273 f1 (mm) −19.776 f2 (mm) 15.970 f2 (mm) 4.899 f3 (mm) −8.549 f4 (mm) −7.110 f5 (mm) 6.308 f6 (mm) −23.877 IH (mm) 3.074 Zoom ratio 2.044

[0118] The following Table 21 shows corresponding values of the parameters defined in the conditions (1) to (8) of Embodiments 1-5.

[0119] As shown in the Table 21, the embodiment 1 satisfies the conditions (1) to (8).

[0120] FIG. 2 illustrates an axial spherical aberration, an astigmatism field curvature, and a distortion of the zoom lens LA according to Embodiment 1 at the wide-angle end. FIG. 3 illustrates an axial spherical aberration, an astigmatism field curvature, and a distortion of the zoom lens LA according to Embodiment 1 at the telephoto end. It should be noted that, curvature S in the figures is a field curvature for a sagittal image plane, and T is a field curvature for a meridional image plane, which are the same for Embodiments 2-5. It can be known that the zoom lens LA of the embodiment 1 becomes compact as TTL=7.870 when contracted, while the zoom lens becomes bright when FNO=1.96 at the wide-angle end, and the zoom ratio=2.044 and the zoom lens has good optical properties, as shown in FIG. 2 and FIG. 3.

Embodiment 2

[0121] FIG. 4 is a schematic diagram of a zoom lens LA according to Embodiment 2 of the present invention. The curvature radiuses R of the image side surfaces and object side surfaces of the first lens L1 to the sixth lens L6 of the camera lens LA according to the Embodiment 2, the on-axis thicknesses of the lenses or on-axis distances d between the lenses, refractive indexes nd, abbe numbers vd are shown in Table 5. Values of A-D during imaging and in the contracted state are shown in Table 6; conic coefficients k and aspheric coefficients are shown in Table 7; and FNO, 2ω, f, TTL, LB, f1, fG2, f2, f3, f4, f5, f6, IH and zoom ratios are shown in Table 8.

TABLE-US-00005 TABLE 5 R d nd νd Effective radius (mm) S1 R1 7.85611 d1 0.755 nd1 1.4959 ν1 81.655 4.400 S2 R2 4.27586 D12 d2 A 3.928 Stop ∞ d3 −1.181  2.653 S3 R3 3.34061 d4 2.249 nd2 1.5438 ν2 56.029 2.665 S4 R4 −9.29516 d5 0.348 2.505 S5 R5 5.01403 d6 0.369 nd3 1.6153 ν3 25.936 2.167 S6 R6 2.47207 d7 0.575 1.920 S7 R7 −7.39526 d8 0.372 nd4 1.6700 ν4 19.392 1.916 S8 R8 13.50619 d9 B 1.883 S9 R9 7.95199  d10 0.790 nd5 1.6153 ν5 25.936 1.976 S10 R10 −7.40039  d11 C 1.957 S11 R11 6.04949  d12 0.400 nd6 1.5346 ν6 55.695 2.633 S12 R12 3.88313  d13 0.367 2.825 S13 R13 ∞  d14 0.210 ndg 1.5168 νg 64.167 2.891 S14 R14 ∞  d15 D 2.933 Reference wavelength = 587.6 nm

TABLE-US-00006 TABLE 6 Imaging Wide Tele Contracted A 10.027 1.382 1.381 B  0.228 0.737 0.200 C  3.932 1.873 0.200 D  1.040 5.909 0.890

TABLE-US-00007 TABLE 7 Cone coefficient Aspheric surface coefficient k A4 A6 A8 A10 S1 0.0000E+00 −5.7385E−03 3.6299E−04 −2.0970E−05 1.3349E−06 S2 0.0000E+00 −8.2258E−03 6.3034E−04 −9.4459E−05 1.2558E−05 S3 −3.4604E−01 7.4776E−04 5.9198E−04 −4.1787E−04 1.7321E−04 S4 0.0000E+00 1.2256E−02 −2.4500E−03 5.9863E−04 −1.3437E−04 S5 0.0000E+00 −3.8659E−02 3.8995E−03 1.7269E−03 −9.8686E−04 S6 −7.3622E+00 −4.0242E−03 −1.6553E−02 1.4133E−02 −6.3262E−03 S7 −4.9931E+01 7.0086E−03 3.1047E−03 −2.8514E−03 1.8458E−03 S8 0.0000E+00 2.2997E−02 5.1423E−03 −8.1196E−03 5.3772E−03 S9 0.0000E+00 5.6199E−03 6.3134E−03 −7.5190E−03 4.4893E−03 S10 0.0000E+00 1.5263E−02 −1.0533E−02 9.9879E−03 −5.5760E−03 S11 −1.0309E+01 −1.7153E−02 2.6433E−03 −3.2400E−04 4.3365E−05 S12 −1.3533E+01 −5.1779E−03 −1.6955E−03 7.6430E−04 −1.4174E−04 Cone coefficient Aspheric surface coefficient k A12 A14 A16 S1 0.0000E+00 −8.1503E−08 3.1114E−09 −4.9180E−11 S2 0.0000E+00 −1.1269E−06 5.4030E−08 −1.0782E−09 S3 −3.4604E−01 −3.7552E−05 4.1525E−06 −1.9096E−07 S4 0.0000E+00 1.6965E−05 −1.2495E−06 4.1593E−08 S5 0.0000E+00 2.3274E−04 −2.6947E−05 1.3007E−06 S6 −7.3622E+00 1.9197E−03 −3.4188E−04 2.6649E−05 S7 −4.9931E+01 −5.7675E−04 8.1320E−05 −4.3265E−06 S8 0.0000E+00 −1.9020E−03 3.3746E−04 −2.4089E−05 S9 0.0000E+00 −1.3925E−03 2.1756E−04 −1.2913E−05 S10 0.0000E+00 1.8776E−03 −3.4725E−04 2.7684E−05 S11 −1.0309E+01 −1.2835E−05 1.8482E−06 −9.0136E−08 S12 −1.3533E+01 9.1737E−06 1.6138E−07 −2.8105E−08

TABLE-US-00008 TABLE 8 Wide Tele Fno  1.96  2.78 2ω (°) 46.91 24.64 f (mm)  7.110 14.220 Wide Tele Contracted TTL (mm) 20.481 15.154  7.925 LB (mm)  1.617  6.486  1.467 f1 (mm) −20.341 fG2 (mm) 16.293 f2 (mm) 4.821 f3 (mm) −8.389 f4 (mm) −7.081 f5 (mm) 6.354 f6 (mm) −21.678 IH (mm) 3.074 Zoom ratio 2.000

[0122] As shown in the table 21, the embodiment 2 satisfies the conditions (1)˜(8).

[0123] FIG. 5 illustrates an axial spherical aberration, an astigmatism field curvature, and a distortion of the zoom lens LA according to Embodiment 2 at the wide-angle end. FIG. 6 illustrates an axial spherical aberration, an astigmatism field curvature, and a distortion of the zoom lens LA according to Embodiment 2 at the telephoto end. It can be known that the zoom lens LA of the embodiment 2 becomes compact when TTL=7.925 in the contracted state, while the zoom lens becomes bright when FNO=1.96 at the wide-angle end, and the zoom ratio=2.000 and the zoom lens has good optical properties, as shown in FIG. 5 and FIG. 6.

Embodiment 3

[0124] FIG. 7 is a schematic diagram of a zoom lens LA according to Embodiment 3 of the present invention. The curvature radiuses R of the image side surfaces and object side surfaces of the first lens L1 to the sixth lens L6 of the camera lens LA according to the Embodiment 3, the on-axis thicknesses of the lenses or on-axis distances d between the lenses, refractive indexes nd, abbe numbers vd are shown in Table 9. Values of A-D during imaging and in the contracted state are shown in Table 10; conic coefficients k and aspheric coefficients are shown in Table 11; and FNO, 2ω, f, TTL, LB, f1, fG2, f2, f3, f4, f5, f6, IH and zoom ratios are shown in Table 12.

TABLE-US-00009 TABLE 9 R d nd νd Effective radius (mm) S1 R1 7.46267 d1 0.664 nd1 1.4959 ν1 81.655 4.380 S2 R2 4.26720 d2 A 3.945 Stop ∞ D12 d3 −1.198  2.656 S3 R3 3.42597 d4 2.105 nd2 1.5438 ν2 56.029 2.659 S4 R4 −10.42114 d5 0.575 2.505 S5 R5 6.09062 d6 0.350 nd3 1.6153 ν3 25.936 2.123 S6 R6 2.43733 d7 0.554 1.927 S7 R7 −5.83850 d8 0.383 1.917 S8 R8 −1.8486E+04 d9 B nd4 1.6700 ν4 19.392 1.862 S9 R9 10.01671  d10 0.848 nd5 1.6153 ν5 25.936 1.920 S10 R10 −5.79361  d11 C 1.907 S11 R11 7.72372  d12 0.495 nd6 1.5346 ν6 55.695 2.593 S12 R12 4.55751  d13 0.228 2.825 S13 R13 ∞  d14 0.210 ndg 1.5168 νg 64.167 2.877 S14 R14 ∞  d15 D 2.924 Reference wavelength = 587.6 nm

TABLE-US-00010 TABLE 10 Imaging Wide Tele Contracted A 10.778 1.398 1.398 B  0.200 0.655 0.200 C  4.269 1.836 0.200 D  1.040 6.323 0.890

TABLE-US-00011 TABLE 11 Cone coefficient Aspheric surface coefficient k A4 A6 A8 A10 S1 0.0000E+00 −5.7385E−03 3.6299E−04 −2.0970E−05 1.3349E−06 S2 0.0000E+00 −8.2258E−03 6.3034E−04 −9.4459E−05 1.2558E−05 S3 −2.9795E−01 7.4776E−04 5.9198E−04 −4.1787E−04 1.7321E−04 S4 0.0000E+00 1.2256E−02 −2.4500E−03 5.9863E−04 −1.3437E−04 S5 0.0000E+00 −3.8659E−02 3.8995E−03 1.7269E−03 −9.8686E−04 S6 −1.6152E+01 3.3119E−02 −5.2214E−02 3.1740E−02 −1.1387E−02 S7 −2.8609E+01 7.0086E−03 3.1047E−03 −2.8514E−03 1.8458E−03 S8 0.0000E+00 7.5818E−02 −6.9821E−02 5.9611E−02 −3.0265E−02 S9 0.0000E+00 5.3072E−02 −6.7867E−02 5.2936E−02 −2.3826E−02 S10 0.0000E+00 4.7580E−02 −7.0519E−02 6.4055E−02 −3.3541E−02 S11 −1.6562E+01 −1.7153E−02 2.6433E−03 −3.2400E−04 4.3365E−05 S12 −1.9405E+01 −5.1779E−03 −1.6955E−03 7.6430E−04 −1.4174E−04 Cone coefficient Aspheric surface coefficient k A12 A14 A16 S1 0.0000E+00 −8.1503E−08 3.1114E−09 −4.9180E−11 S2 0.0000E+00 −1.1269E−06 5.4030E−08 −1.0782E−09 S3 −2.9795E−01 −3.7552E−05 4.1525E−06 −1.9096E−07 S4 0.0000E+00 1.6965E−05 −1.2495E−06 4.1593E−08 S5 0.0000E+00 2.3274E−04 −2.6947E−05 1.3007E−06 S6 −1.6152E+01 2.7453E−03 −4.0346E−04 2.6885E−05 S7 −2.8609E+01 −5.7675E−04 8.1320E−05 −4.3265E−06 S8 0.0000E+00 8.8179E−03 −1.3829E−03 9.0597E−05 S9 0.0000E+00 6.2820E−03 −8.9843E−04 5.4650E−05 S10 0.0000E+00 1.0269E−02 −1.7013E−03 1.1907E−04 S11 −1.6562E+01 −1.2835E−05 1.8482E−06 −9.0136E−08 S12 −1.9405E+01 9.1737E−06 1.6138E−07 −2.8105E−08

TABLE-US-00012 TABLE 12 Wide Tele Fno  1.97  2.77 2ω (°) 45.18 24.53 f (mm)  7.110 14.220 Wide Tele Contracted TTL (mm) 21.500 15.425  7.902 LB (mm)  1.478  6.761  1.328 f1 (mm) −21.582 fG2 (mm) 19.983 f2 (mm) 5.009 f3 (mm) −6.854 f4 (mm) −8.716 f5 (mm) 6.090 f6 (mm) −21.995 IH (mm) 3.074 Zoom ratio 2.000

[0125] As shown in the table 21, the embodiment 3 satisfies the conditions (1)˜(8).

[0126] FIG. 8 illustrates an axial spherical aberration, an astigmatism field curvature, and a distortion of the zoom lens LA according to Embodiment 3 at the wide-angle end. FIG. 9 illustrates an axial spherical aberration, an astigmatism field curvature, and a distortion of the zoom lens LA according to Embodiment 3 at the telephoto end. It can be known that the zoom lens LA of the embodiment 3 becomes compact when TTL=7.902 in the contracted state, while the zoom lens becomes bright when FNO=1.97 at the wide-angle end, and the zoom ratio=2.000 and the zoom lens has good optical properties, as shown in FIG. 8 and FIG. 9.

Embodiment 4

[0127] FIG. 10 is a schematic diagram of a zoom lens LA according to Embodiment 4 of the present invention. The curvature radiuses R of the image side surfaces and object side surfaces of the first lens L1 to the sixth lens L6 of the camera lens LA according to the Embodiment 4, the on-axis thicknesses of the lenses or on-axis distances d between the lenses, refractive indexes nd, abbe numbers vd are shown in Table 13. Values of A-D during imaging and in the contracted state are shown in Table 14; conic coefficients k and aspheric coefficients are shown in Table 15; and FNO, 2ω, f, TTL, LB, f1, fG2, f2, f3, f4, f5, f6, IH and zoom ratios are shown in Table 16.

TABLE-US-00013 TABLE 13 R d nd νd Effective radius (mm) S1 R1 7.81273 d1 0.742 nd1 1.4959 ν1 81.655 4.404 S2 R2 4.27534 d2 A 3.939 Stop ∞ D12 d3 −1.236  2.657 S3 R3 3.27848 d4 2.318 nd2 1.5438 ν2 56.029 2.663 S4 R4 −8.84845 d5 0.292 2.490 S5 R5 4.48611 d6 0.405 nd3 1.6153 ν3 25.936 2.129 S6 R6 2.29388 d7 0.596 1.847 S7 R7 −12.45891 d8 0.361 nd4 1.6700 ν4 19.392 1.836 S8 R8 6.64514 d9 B 1.878 S9 R9 6.79743  d10 0.803 nd5 1.6153 ν5 25.936 2.029 S10 R10 −8.18206  d11 C 1.995 S11 R11 8.46501  d12 0.400 nd6 1.5346 ν6 55.695 2.633 S12 R12 4.97780  d13 0.210 2.818 S13 R13 ∞  d14 0.210 ndg 1.5168 νg 64.167 2.873 S14 R14 ∞  d15 D 2.918 Reference wavelength = 587.6 nm

TABLE-US-00014 TABLE 14 Imaging Wide Tele Contracted A 10.147 1.436 1.436 B  0.273 0.828 0.200 C  3.860 1.547 0.270 D  1.040 6.193 0.890

TABLE-US-00015 TABLE 15 Cone coefficient Aspheric surface coefficient k A4 A6 A8 A10 S1 0.0000E+00 −5.7385E−03 3.6299E−04 −2.0970E−05 1.3349E−06 S2 0.0000E+00 −8.2258E−03 6.3034E−04 −9.4459E−05 1.2558E−05 S3 −3.7362E−01 7.4776E−04 5.9198E−04 −4.1787E−04 1.7321E−04 S4 0.0000E+00 1.2256E−02 −2.4500E−03 5.9863E−04 −1.3437E−04 S5 0.0000E+00 −3.8659E−02 3.8995E−03 1.7269E−03 −9.8686E−04 S6 −5.6048E+00 −5.8591E−03 −1.4051E−02 1.3274E−02 −6.2680E−03 S7 −5.0000E+01 7.0086E−03 3.1047E−03 −2.8514E−03 1.8458E−03 S8 0.0000E+00 −3.2339E−03 2.8613E−02 −2.4274E−02 1.2332E−02 S9 0.0000E+00 −6.4725E−03 1.7074E−02 −1.3119E−02 5.7531E−03 S10 0.0000E+00 1.3225E−02 −1.0171E−02 1.1465E−02 −7.1844E−03 S11 −6.3466E+00 −1.7153E−02 2.6433E−03 −3.2400E−04 4.3365E−05 S12 −2.1190E+01 −5.1779E−03 −1.6955E−03 7.6430E−04 −1.4174E−04 Cone coefficient Aspheric surface coefficient k A12 A14 A16 S1 0.0000E+00 −8.1503E−08 3.1114E−09 −4.9180E−11 S2 0.0000E+00 −1.1269E−06 5.4030E−08 −1.0782E−09 S3 −3.7362E−01 −3.7552E−05 4.1525E−06 −1.9096E−07 S4 0.0000E+00 1.6965E−05 −1.2495E−06 4.1593E−08 S5 0.0000E+00 2.3274E−04 −2.6947E−05 1.3007E−06 S6 −5.6048E+00 2.0450E−03 −3.9314E−04 3.3783E−05 S7 −5.0000E+01 −5.7675E−04 8.1320E−05 −4.3265E−06 S8 0.0000E+00 −3.6625E−03 5.7130E−04 −3.6576E−05 S9 0.0000E+00 −1.4046E−03 1.7690E−04 −8.2968E−06 S10 0.0000E+00 2.5340E−03 −4.6865E−04 3.6007E−05 S11 −6.3466E+00 −1.2835E−05 1.8482E−06 −9.0136E−08 S12 −2.1190E+01 9.1737E−06 1.6138E−07 −2.8105E−08

TABLE-US-00016 TABLE 16 Wide Tele Fno  1.96  2.78 2ω (°) 46.67 24.54 f (mm)  7.110 14.220 Wide Tele Contracted TTL (mm) 20.422 15.105  7.898 LB (mm) 1.460 6.613  1.310 f1 (mm) −20.462 fG2 (mm) 15.801 f2 (mm) 4.716 f3 (mm) −8.207 f4 (mm) −6.419 £5 (mm) 6.160 f6 (mm) −23.544 IH (mm) 3.074 Zoom ratio 2.000

[0128] As shown in the table 21, the embodiment 4 satisfies the conditions (1)˜(8).

[0129] FIG. 11 illustrates an axial spherical aberration, an astigmatism field curvature, and a distortion of the zoom lens LA according to Embodiment 4 at the wide-angle end. FIG. 12 illustrates an axial spherical aberration, an astigmatism field curvature, and a distortion of the zoom lens LA according to Embodiment 4 at the telephoto end. It can be known that the zoom lens LA of the embodiment 4 becomes compact when TTL=7.898 in the contracted state, while the zoom lens becomes bright when FNO=1.96 at the wide-angle end, and the zoom ratio=2.000 and the zoom lens has good optical properties, as shown in FIG. 11 and FIG. 12.

Embodiment 5

[0130] FIG. 13 is a schematic diagram of a zoom lens LA according to Embodiment 5 of the present invention. The curvature radiuses R of the image side surfaces and object side surfaces of the first lens L1 to the sixth lens L6 of the camera lens LA according to the Embodiment 4, the on-axis thicknesses of the lenses or on-axis distances d between the lenses, refractive indexes nd, abbe numbers vd are shown in Table 17. Values of A-D during imaging and in the contracted state are shown in Table 18; conic coefficients k and aspheric coefficients are shown in Table 19; and FNO, 2ω, f, TTL, LB, f1, fG2, f2, f3, f4, f5, f6, IH and zoom ratios are shown in Table 20.

TABLE-US-00017 TABLE 17 R d nd νd Effective radius (mm) S1 R1 7.70579 d1 0.756 nd1 1.4959 ν1 81.655 4.247 S2 R2 4.14214 D12 d2 A 3.755 Stop ∞ d3 −1.162  2.622 S3 R3 3.34187 d4 2.301 nd2 1.5438 ν2 56.029 2.631 S4 R4 −8.40418 d5 0.239 2.493 S5 R5 4.77669 d6 0.517 nd3 1.6153 ν3 25.936 2.206 S6 R6 2.22266 d7 0.617 1.885 S7 R7 −5.49224 d8 0.350 nd4 1.6700 ν4 19.392 1.862 S8 R8 35.94148 d9 B 1.876 S9 R9 6.54571  d10 0.774 nd5 1.6153 ν5 25.936 1.957 S10 R10 −7.56969  d11 C 1.982 S11 R11 19.40691  d12 0.400 nd6 1.5346 ν6 55.695 2.600 S12 R12 7.02181  d13 0.161 2.809 S13 R13 ∞  d14 0.210 ndg 1.5168 νg 64.167 2.882 S14 R14 ∞  d15 D 2.928 Reference wavelength = 587.6 nm

TABLE-US-00018 TABLE 18 Imaging Wide Tele Contracted A 9.208 1.362 1.362 B 0.218 0.659 0.200 C 4.000 1.641 0.250 D 1.040 6.424 0.890

TABLE-US-00019 TABLE 19 Cone coefficient Aspheric surface coefficient k A4 A6 A8 A10 S1 0.0000E+00 −6.3542E−03 4.0075E−04 −2.2871E−05 1.4974E−06 S2 0.0000E+00 −8.9455E−03 6.2478E−04 −8.8072E−05 1.1746E−05 S3 −3.3426E−01 1.1348E−03 6.3258E−04 −4.4703E−04 1.7448E−04 S4 0.0000E+00 1.1410E−02 −2.4589E−03 5.8475E−04 −1.3561E−04 S5 0.0000E+00 −4.3633E−02 4.5756E−03 1.6932E−03 −9.9040E−04 S6 −3.7020E+00 −3.0930E−02 1.4048E−03 5.4655E−03 −2.6803E−03 S7 −5.0000E+01 1.2295E−02 3.0404E−03 −2.8075E−03 1.7203E−03 S8 0.0000E+00 4.2716E−02 −1.1983E−02 4.6692E−03 −1.2865E−03 S9 0.0000E+00 −2.3237E−03 5.0431E−03 −3.8428E−03 1.9235E−03 S10 0.0000E+00 4.4127E−03 1.9464E−03 −1.2628E−03 5.6504E−04 S11 4.6432E+01 −1.2665E−02 2.1486E−03 −5.2449E−04 1.0829E−04 S12 −3.1439E+01 −5.6632E−03 −3.7959E−04 2.6270E−04 −6.1321E−05 Cone coefficient Aspheric surface coefficient k A12 A14 A16 S1 0.0000E+00 −8.5424E−08 2.9280E−09 −4.2182E−11 S2 0.0000E+00 −1.0825E−06 5.3958E−08 −1.1519E−09 S3 −3.3426E−01 −3.7121E−05 4.1253E−06 −1.9615E−07 S4 0.0000E+00 1.7300E−05 −1.1907E−06 3.4435E−08 S5 0.0000E+00 2.3183E−04 −2.6671E−05 1.2887E−06 S6 −3.7020E+00 8.3121E−04 −1.6594E−04 1.4556E−05 S7 −5.0000E+01 −5.7979E−04 8.1237E−05 −4.3620E−06 S8 0.0000E+00 1.4095E−04 −3.8184E−06 1.7913E−07 S9 0.0000E+00 −5.5964E−04 8.6588E−05 −5.2664E−06 S10 0.0000E+00 −1.4733E−04 1.8623E−05 −5.2950E−07 S11 4.6432E+01 −1.9436E−05 1.9010E−06 −7.8844E−08 S12 −3.1439E+01 6.4413E−06 −3.7189E−07 1.0931E−08

TABLE-US-00020 TABLE 20 Wide Tele Fno  1.95  2.81 2ω (°) 47.29 24.66 f (mm)  7.110 14.220 Wide Tele Contracted TTL (mm) 19.627 15.249  7.864 LB (mm)  1.411  6.795  1.261 f1 (mm) −19.426 fG2 (mm) 16.652 f2 (mm) 4.723 f3 (mm) −7.321 f4 (mm) −7.086 f5 (mm) 5.827 f6 (mm) −20.816 IH (mm) 3.074 Zoom ratio 2.000

[0131] As shown in the table 21, the embodiment 5 satisfies the condition (1)˜(8).

[0132] FIG. 14 illustrates an axial spherical aberration, an astigmatism field curvature, and a distortion of the zoom lens LA according to Embodiment 5 at the wide-angle end. FIG. 15 illustrates an axial spherical aberration, an astigmatism field curvature, and a distortion of the zoom lens LA according to Embodiment 5 at the telephoto end. It can be known that the zoom lens LA of the embodiment 5 becomes compact when TTL=7.864 in the contracted state, while the zoom lens becomes bright when FNO=1.95 at the wide-angle end, and the zoom ratio=2.000 and the zoom lens has good optical properties, as shown in FIG. 14 and FIG. 15.

[0133] The Table 21 shows the corresponding values of the parameters defined in the conditions (1) to (8) of Embodiments 1-5.

TABLE-US-00021 TABLE 21 Embodiment 1 Embodiment 2 Embodiment 3 Embodiment 4 Embodiment 5 Notes f_Tele/f_Wide 2.044 2.000 2.000 2.000 2.000 Condition (1) f3/f2 −1.745 −1.740 −1.368 −1.740 −1.550 Condition (3) 2f4/f2 −1.451 −1.469 −1.740 −1.361 −1.500 Condition (3) f1/fG2 −1.238 −1.248 −1.080 −1.295 −1.167 Condition (4) f5/fG2 0.395 0.390 0.305 0.390 0.350 Condition (5) f6/fG2 −1.495 −1.330 −1.101 −1.490 −1.250 Condition (6) LB_Tele/LB_Wide 4.950 4.010 4.575 4.529 4.816 Condition (7) ν1 76.860 81.655 81.655 81.655 81.655 Condition (8)

[0134] It can be appreciated by one having ordinary skills in the art that the description above is only embodiments of the present invention. In practice, the one having ordinary skills in the art can make various modifications to these embodiments in forms and details without departing from the scope of the present invention.