MINIATURE TELEPHOTO LENS MODULE AND A CAMERA UTILIZING SUCH A LENS MODULE

Abstract

The presently disclosed subject matter includes a mobile electronic comprising an integrated camera, comprising a Wide camera unit comprising a Wide lens unit, and a Telephoto camera unit comprising a telephoto lens unit, the telephoto lens unit and the wide lens unit having respectively TTL/EFL ratios smaller and larger than 1 and defining separate telephoto and wide optical paths.

Claims

1. A mobile electronic device comprising an integrated camera, wherein the camera comprises a Wide camera unit comprising a Wide lens unit and a Telephoto camera unit comprising a Telephoto lens unit, the Telephoto lens unit and the Wide lens unit having respectively TTL/EFL ratios smaller and larger than 1 and defining separate Telephoto and Wide optical paths.

2. The mobile electronic device of claim 1, wherein light receiving outer surfaces of the Wide and Telephoto lens units are located substantially in the same plane, thereby reducing shadowing and light blocking effects therebetween.

3. The mobile electronic device of claim 1, wherein the Wide and Telephoto camera units are mounted on separate printed circuit boards.

4. The mobile electronic device of claim 3, wherein the printed circuit boards are located in different spaced-apart substantially parallel planes.

5. The mobile electronic device of claim 1, wherein the Wide and Telephoto camera units are mounted directly on a single printed circuit board.

6. The mobile electronic device of claim 1, wherein the Wide and Telephoto camera units are spaced from one another a distance d of about 1 mm.

7. (canceled)

8. The mobile electronic device of claim 1, wherein the Telephoto lens unit has a TTL less than 6.5 mm.

9. The mobile electronic device of claim 8, wherein the Telephoto lens has TTL is less than 5.9 mm.

10. The mobile electronic device of claim 1, wherein the Telephoto lens unit comprises multiple lens elements made of at least two different polymer materials having different Abbe numbers, wherein the multiple lens elements comprise a first group of at least three lens elements configured to form a telephoto lens assembly, and a second group of at least two lens elements wherein the second group of at least two lens elements is spaced from the telephoto lens assembly by a predetermined effective gap equal to or larger than ⅕ of the TTL of the Telephoto lens unit.

11. The mobile electronic device of claim 10, wherein the at least two different polymer materials comprise at least one plastic material with the Abbe number larger than 50, and at least one plastic material with the Abbe number smaller than 30.

12. The mobile electronic device of claim 10, wherein the first group of at least three lens elements comprises, in order from an object plane to an image plane along an optical axis of the telephoto lens unit, a first lens having positive optical power and a pair of second and third lenses having together negative optical power such that the telephoto lens assembly provides a telephoto optical effect of the telephoto lens unit, and such that the second and third lenses are each made of one of the at least two different polymer materials having a different Abbe number, for reducing chromatic aberrations of the telephoto lens, and wherein the second group of lens elements is configured to correct field curvature of the telephoto lens assembly and comprises two or more of the lens elements made of the different polymer materials respectively having different Abbe numbers and is configured to compensate for residual chromatic aberrations of the telephoto lens assembly dispersed during light passage through the effective gap between the telephoto and field lens assemblies.

13. The mobile electronic device of claim 12, wherein the first, third and fifth lens elements have each an Abbe number greater than 50, and the second and fourth lens elements have each an Abbe number smaller than 30.

14. (canceled)

15. The mobile electronic device of claim 14, wherein the lens elements of the field lens assembly are spaced from one another an effective air gap smaller than 1/50 of the TTL of the Telephoto lens unit.

16. The mobile electronic device of claim 10, wherein the Telephoto lens unit has a TTL smaller than 5.5 mm, an EFL larger than 5.9 mm, and an optical diameter smaller than 4 mm, thereby enabling to provide an image on an entire area of a ¼″ image sensor.

17. The mobile electronic device of claim 10, wherein the Telephoto lens unit has a TTL smaller than 6.2 mm, an EFL larger than 6.8 mm, and an optical diameter smaller than 5 mm, thereby enabling to provide an image on an entire area of a ⅓″ image sensor.

18. A camera for integrating in a mobile electronic device, the camera comprising a Wide camera unit and a Telephoto camera unit comprising respectively a Wide lens unit and a Telephoto lens unit having TTL/EFL ratios larger and smaller than 1, respectively, and defining wide and telephoto optical paths.

19. The camera of claim 18, wherein lens elements of at least the Telephoto lens unit are made of one or more polymer materials.

20. The mobile electronic device of claim 1, wherein the Telephoto lens unit is smaller than 0.9.

21. The mobile electronic device of claim 8, wherein the Telephoto TTL is less than 5.5 mm.

22. The mobile electronic device of claim 1, wherein the Telephoto lens unit EFL is greater than 5.9 mm.

23. The mobile electronic device of claim 1, wherein the Telephoto lens unit EFL is greater than 6.8 mm.

24. The mobile electronic device of claim 1, wherein the Telephoto lens unit has a field of view no larger than 44 degrees.

25. The mobile electronic device of claim 10, wherein the Telephoto lens unit has a field of view no larger than 44 degrees.

26. The camera of claim 19, wherein the Telephoto lens unit has a field of view no larger than 44 degrees.

27. The mobile electronic device of claim 20, wherein the Telephoto lens unit EFL is greater than 5.9 mm.

28. The mobile electronic device of claim 20, wherein the Telephoto lens unit EFL is greater than 6.8 mm.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0051] In order to better understand the subject matter that is disclosed herein and to exemplify how it may be carried out in practice, embodiments will now be described, by way of non-limiting example only, with reference to the accompanying drawings, in which:

[0052] FIG. 1A is a schematic illustration demonstrating shadowing and light-blocking problems caused by height differences between Wide and Tele cameras in a dual-aperture camera;

[0053] FIG. 1B is a schematic illustration of a mobile phone device (constituting a portable electronic device) utilizing a camera unit as disclosed herein which is fully integrated inside the smartphone device;

[0054] FIG. 1C is a schematic illustration of a telephoto lens unit according to the presently disclosed subject matter;

[0055] FIG. 2A is a schematic illustration of a specific configuration of the telephoto lens unit, according to a first example of the presently disclosed subject matter;

[0056] FIG. 2B shows a graph plotting the modulus of the optical transfer function (MTF) vs. focus shift of the entire optical lens unit of FIG. 2A for various fields;

[0057] FIG. 2C shows a graph plotting the distortion vs. field angle (+Y direction) for the lens unit of FIG. 2A;

[0058] FIG. 3A is a schematic illustration of another possible configuration of the telephoto lens unit, according to a first example of the presently disclosed subject matter;

[0059] FIG. 3B shows a graph plotting the MTF vs. focus shift of the entire optical lens assembly for various fields in the lens unit of FIG. 3B, according to the second example of the presently disclosed subject matter;

[0060] FIG. 3C shows a graph plotting the distortion +Y in percent for the lens unit of FIG. 3A;

[0061] FIG. 4A is a schematic illustration of a specific configuration of the telephoto lens unit, according to a first example of the presently disclosed subject matter;

[0062] FIG. 4B shows a graph plotting the MTF vs. focus shift of the entire optical lens system for various fields in the lens unit of FIG. 4A;

[0063] FIG. 4C shows a graph plotting the distortion +Y in percent for the lens unit of FIG. 4A;

[0064] FIG. 5 is a schematic illustration showing the concept of an effective air gap between adjacent lenses in an optical lens unit, according to the presently disclosed subject matter;

[0065] FIG. 6A is a schematic illustration, in perspective cross section, of an example of a dual-aperture zoom camera, with each camera on a separate printed circuit board (PCB), according to the presently disclosed subject matter;

[0066] FIG. 6B is a schematic illustration, in perspective cross section, of another example of a dual-aperture zoom camera, with each camera on a separate PCB, according to the presently disclosed subject matter;

[0067] FIG. 7 is a schematic illustration, in perspective cross section, of yet another example of a dual-aperture zoom camera, where both cameras are mounted on a single PCB, according to the presently disclosed subject matter;

[0068] FIG. 8 is a schematic illustration of an example of a dual-aperture zoom camera that includes an OIS mechanism, according to the presently disclosed subject matter; and

[0069] FIG. 9 shows schematically a functional block diagram of the camera example of FIG. 8, according to the presently disclosed subject matter.

DETAILED DESCRIPTION OF EMBODIMENTS

[0070] The present invention includes novel configuration of a lens unit in a portable camera, advantageously applicable in a portable electronic device. This is schematically illustrated in FIG. 1B. In this example, such a portable electronic device 10 is constituted by a mobile phone device (e.g. smartphone). The mobile device is typically a few millimeters thick, e.g. 4 mm-15 mm.

[0071] However, as explained above and exemplified further below, the problems solved by the technique disclosed herein are relevant for any modern electronic device equipped with a camera 15 and suitable to be implemented in any such device. This is so since any modern electronic device of the kind specified (i.e. a device including an integral camera unit) is to be as slim as possible, as light as possible, and is to acquire pictures with as good quality as possible.

[0072] Modern cameras typically require zooming functions. When such a camera is used in an electronic device, such as a mobile phone device, the zooming function is often implemented with static optics. The problems which may arise when trying to incorporate Wide and Tele lenses into a common housing due to the difference in their heights are described above with reference to FIG. 1A.

[0073] As mentioned above, the presently disclosed subject matter includes a novel mobile electronic device 10 which includes an integrated camera unit 15 which is mounted inside the device casing 14. The camera 15 includes at least one telephoto lens unit (not shown here) which is made of polymer materials. The telephoto lens unit is configured such that its total track lens (TTL) is less than 15 mm and even less than 10 mm, e.g. less than 6 mm or even less than 4 mm. Thus, enabling the camera to be fully integrated in the portable device (substantially not protruding from the device casing).

[0074] Reference is made to FIG. 1C showing schematically the configuration of a telephoto lens unit 20 of the present invention. The telephoto lens unit 20 is composed of multiple lens elements made of different polymer materials, i.e. materials having different Abbe numbers. The multiple lens elements are configured and arranged to define a telephoto lens assembly 22A and a field lens assembly 22B arranged along an optical axis OA with a predetermined effective gap G between them (as will be described more specifically further below). The telephoto lens assembly 22A is configured to provide the telephoto optical effect of the telephoto lens unit 20. The field lens assembly 22B spaced from the telephoto lens assembly 22A by the predetermined effective gap G is configured for correcting field curvature of the telephoto lens assembly 22A and to compensate for residual chromatic aberrations of the telephoto lens assembly dispersed during light passage through the effective gap G.

[0075] The telephoto lens unit 20 is characterized by a total track lens (TTL) and an effective focal lens (EFL) such that TTL<EFL. This will be exemplified further below. According to the invention, the effective gap G between assemblies 22A and 22B is selected to be larger than TTL/5 of the telephoto lens unit 22A, thereby enabling correction of field curvature of telephoto lens assembly 22A by the field lens assembly 22B.

[0076] The telephoto lens assembly 22A includes three lens elements (generally three or more) L1, L2, L3 (which are shown here schematically and not to scale), where lens L1 has positive optical power and lenses L2 and L3 have together negative optical power. Lenses L2 and L3 are made of the first polymer material having a first Abbe number selected for reducing chromatic aberrations of the telephoto lens assembly 22A. The field lens assembly 22B includes two (or more) lens elements L4 and L5 which are made of different polymer materials respectively having different Abbe numbers. These lenses are configured to compensate for residual chromatic aberrations of the telephoto lens assembly 22A dispersed during light passage through the effective gap G between the 22A and 22B.

[0077] Lenses L1-L5 can be made for example of two plastic materials, one having an Abbe number greater than 50 and the other—smaller than 30. For example, Lenses L1, L3 and L5 are made of plastic with an Abbe number greater than 50, and lenses L2 and L4 are made of plastic having an Abbe number smaller than 30.

[0078] The following are several specific, but non-limiting, examples of the implementation and operation of the telephoto lens unit of the invention described above with reference to FIG. 1C. In the following description, the shape (convex or concave) of a lens element surface is defined as viewed from the respective side (i.e. from an object side or from an image side).

[0079] FIG. 2A shows a schematic illustration of an optical lens unit 100, according to a first example of the presently disclosed subject matter. FIG. 2B shows the MTF vs. focus shift of the entire optical lens unit for various fields in the lens unit configuration 100. FIG. 2C shows the distortion +Y in percent vs. field.

[0080] According to the example illustrated in FIG. 2A, lens unit 100 includes, in order from an object side to an image side, a first plastic lens element 102 (also referred to as “L1”) with positive refractive power having a convex object-side surface 102a and a convex or concave image-side surface 102b; a second plastic lens element 104 (also referred to as “L2”) with negative refractive power and having a meniscus convex object-side surface 104a, with an image side surface marked 104b; a third plastic lens element 106 (also referred to as “L3”) with negative refractive power having a concave object-side surface 106a with an inflection point and a concave image-side surface 106b. These lens elements define together the telephoto lens assembly (22A in FIG. 1C). Further provided in lens unit 100 is a fourth plastic lens element 108 (also referred to as “L4”) with positive refractive power having a positive meniscus, with a concave object-side surface marked 108a and an image-side surface marked 108b; and a fifth plastic lens element 110 (also referred to as “L5”) with negative refractive power having a negative meniscus, with a concave object-side surface marked 110a and an image-side surface marked 110b. These two lenses define together the field lens assembly (22B in FIG. 1C). The optical lens unit 100 may further optionally include a stop element 101. The telephoto lens unit 100 defines an image plane 114 in which image sensor(s) is/are located, which is not shown here. Also, as exemplified in the figure, an optional glass window 112 is disposed between the image-side surface 110b of fifth lens element 110 and the image plane 114.

[0081] In the example of the telephoto lens unit 100, all lens element surfaces are aspheric. Detailed optical data is shown in Table 1, and aspheric surface data is shown in Table 2, wherein the units of the radius of curvature (R), lens element thickness and/or distances between elements along the optical axis and diameter are expressed in mm. “Nd” is the refraction index. The equation of the aspheric surface profiles is expressed by:

[00001]$z=\frac{{\mathrm{cr}}^2}{1+\sqrt{1-\left(1+k\right).Math.c^2.Math.r^2}}+{\alpha }_1.Math.r^2+{\alpha }_2.Math.r^4+{\alpha }_3.Math.r^6+{\alpha }_4.Math.r^8+{\alpha }_5.Math.r^{10}+{\alpha }_6.Math.r^{12}+{\alpha }_7.Math.r^{14}$

[0082] where r is the distance from (and is perpendicular to) the optical axis, k is the conic coefficient, c=1/R where R is the radius of curvature, and α are coefficients given in Table 2.

[0083] In the equation above as applied to the telephoto lens unit, coefficients α.sub.1 and α.sub.7 are zero. It should be noted that the maximum value of r “max r”=Diameter/2. It should also be noted that in Table 1 (and in Tables 3 and 5 below), the distances between various elements (and/or surfaces) are marked “Lmn” (where m refers to the lens element number, n=1 refers to the element thickness and n=2 refers to the air gap to the next element) and are measured on the optical axis z, wherein the stop is at z=0. Each number is measured from the previous surface. Thus, the first distance—0.466 mm is measured from the stop to surface 102a, the distance L11 from surface 102a to surface 102b (i.e. the thickness of first lens element 102) is 0.894 mm, the air gap L12 between surfaces 102b and 104a is 0.020 mm, the distance L21 between surfaces 104a and 104b (i.e. thickness d2 of second lens element 104) is 0.246 mm, etc. Also, L21=d.sub.2 and L51=d.sub.5. The lens elements in Tables 1 and 2 (as well as in Tables 3-6) are designed to provide an image on an entire ⅓″ sensor having

TABLE-US-00001 TABLE 1 Radius R Distances Diameter # Comment [mm] [mm] Nd/Vd [mm] 1 Stop Infinite −0.466 2.4 2 L11 1.5800 0.894 1.5345/57.095 2.5 3 L12 −11.2003 0.020 2.4 4 L21 33.8670 0.246 1.63549/23.91  2.2 5 L22 3.2281 0.449 1.9 6 L31 −12.2843 0.290 1.5345/57.095 1.9 7 L32 7.7138 2.020 1.8 8 L41 −2.3755 0.597 1.63549/23.91  3.3 9 L42 −1.8801 0.068 3.6 10 L51 −1.8100 0.293 1.5345/57.095 3.9 11 L52 −5.2768 0.617 4.3 12 Window Infinite 0.210 1.5168/64.17  3.0 13 Infinite 0.200 3.0
dimensions of approximately 4.7×3.52 mm. The optical diameter in all of these lens assemblies is the diameter of the second surface of the fifth lens element.

TABLE-US-00002 TABLE 2 Conic # coefficient k α.sub.2 α.sub.3 α.sub.4 α.sub.5 α.sub.6 2 −0.4668 7.9218E−03 2.3146E−02 −3.3436E−02 2.3650E−02 −9.2437E−03 3 −9.8525 2.0102E−02 2.0647E−04 7.4394E−03 −1.7529E−02 4.5206E−03 4 10.7569 −1.9248E−03 8.6003E−02 1.1676E−02 −4.0607E−02 1.3545E−02 5 1.4395 5.1029E−03 2.4578E−01 −1.7734E−01 2.9848E−01 −1.3320E−01 6 0.0000 2.1629E−01 4.0134E−02 1.3615E−02 2.5914E−03 −1.2292E−02 7 −9.8953 2.3297E−01 8.2917E−02 −1.2725E−01 1.5691E−01 −5.9624E−02 8 0.9938 −1.3522E−02 −7.0395E−03 1.4569E−02 −1.5336E−02 4.3707E−03 9 −6.8097 −1.0654E−01 1.2933E−02 2.9548E−04 −1.8317E−03 5.0111E−04 10 −7.3161 −1.8636E−01 8.3105E−02 −1.8632E−02 2.4012E−03 −1.2816E−04 11 0.0000 −1.1927E−01 7.0245E−02 −2.0735E−02 2.6418E−03 −1.1576E−04

[0084] Lens unit 100 provides a field of view (FOV) of 44 degrees, with EFL=6.90 mm, F#=2.80 and TTL of 5.904 mm. Thus and advantageously, the ratio TTL/EFL=0.855. Advantageously, the Abbe number of the first, third and fifth lens element is 57.095. Advantageously, the first air gap between lens elements 102 and 104 (the gap between surfaces 102b and 104a) has a thickness (0.020 mm) which is less than a tenth of thickness d.sub.2 (0.246 mm). Advantageously, the Abbe number of the second and fourth lens elements is 23.91. Advantageously, an effective third air gap G (see below with reference to Table 9) between lens elements 106 and 108 (i.e. the telephoto and field lens assemblies) is greater than TTL/5. Advantageously, an effective fourth air gap (see below with reference to Table 9) between lens elements 108 and 110 is smaller than TTL/50.

[0085] The focal length (in mm) of each lens element in lens unit 100 is as follows: f1=2.645, f2=−5.578, f3=−8.784, f4=9.550 and f5=−5.290. The condition 1.2×|f3|>|f2|<1.5×f1 is clearly satisfied, as 1.2×8.787>5.578>1.5×2.645. f1 also fulfills the condition f1<TTL/2, as 2.645<2.952.

[0086] FIG. 3A shows a schematic illustration of an optical lens unit 200, according to another example of the presently disclosed subject matter. FIG. 3B shows the MTF vs. focus shift of the entire optical lens system for various fields in embodiment 200. FIG. 3C shows the distortion +Y in percent vs. field.

[0087] According to the example illustrated in FIG. 3A, lens unit 200 comprises, in order from an object side to an image side: an optional stop 201; a telephoto lens assembly including a first plastic lens element 202 with positive refractive power having a convex object-side surface 202a and a convex or concave image-side surface 202b, a second plastic lens element 204 with negative refractive power, having a meniscus convex object-side surface 204a, with an image side surface marked 204b, and a third plastic lens element 206 with negative refractive power having a concave object-side surface 206a with an inflection point and a concave image-side surface 206b; and a field lens assembly including a fourth plastic lens element 208 with positive refractive power having a positive meniscus, with a concave object-side surface marked 208a and an image-side surface marked 208b, and a fifth plastic lens element 210 with negative refractive power having a negative meniscus, with a concave object-side surface marked 110a and an image-side surface marked 210b. The optical lens unit 200 further optionally includes a glass window 212 disposed between the image-side surface 210b of fifth lens element 210 and an image plane 214.

[0088] In the lens unit 200, all lens element surfaces are aspheric. Detailed optical data is given in Table 3, and the aspheric surface data is given in Table 4, wherein the markings and units are the same as in, respectively, Tables 1 and 2. The equation of the aspheric surface profiles is the same as for lens unit 100 described above.

TABLE-US-00003 TABLE 3 Radius R Distances Diameter # Comment [mm] [mm] Nd/Vd [mm] 1 Stop Infinite −0.592 2.5 2 L11 1.5457 0.898 1.53463/56.18  2.6 3 L12 −127.7249 0.129 2.6 4 L21 6.6065 0.251 1.91266/20.65  2.1 5 L22 2.8090 0.443 1.8 6 L31 9.6183 0.293 1.53463/56.18  1.8 7 L32 3.4694 1.766 1.7 8 L41 −2.6432 0.696 1.632445/23.35   3.2 9 L42 −1.8663 0.106 3.6 10 L51 −1.4933 0.330 1.53463/56.18  3.9 11 L52 −4.1588 0.649 4.3 12 Window Infinite 0.210 1.5168/64.17  5.4 13 Infinite 0.130 5.5

TABLE-US-00004 TABLE 4 Conic # coefficient k α.sub.2 α.sub.3 α.sub.4 α.sub.5 α.sub.6 2 0.0000 −2.7367E−03 2.8779E−04 −4.3661E−03 3.0069E−03 −1.2282E−03 3 −10.0119 4.0790E−02 −1.8379E−02 2.2562E−02 −1.7706E−02 4.9640E−03 4 10.0220 4.6151E−02 5.8320E−02 −2.0919E−02 −1.2846E−02 8.8283E−03 5 7.2902 3.6028E−02 1.1436E−01 −1.9022E−02 4.7992E−03 −3.4079E−03 6 0.0000 1.6639E−01 5.6754E−02 −1.2238E−02 −1.8648E−02 1.9292E−02 7 8.1261 1.5353E−01 8.1427E−02 −1.5773E−01 1.5303E−01 −4.6064E−02 8 0.0000 −3.2628E−02 1.9535E−02 −1.6716E−02 −2.0132E−03 2.0112E−03 9 0.0000 1.5173E−02 −1.2252E−02 3.3611E−03 −2.5303E−03 8.4038E−04 10 −4.7688 −1.4736E−01 7.6335E−02 −2.5539E−02 5.5897E−03 −5.0290E−04 11 0.00E+00 −8.3741E−02 4.2660E−02 −8.4866E−03 1.2183E−04 7.2785E−05

[0089] Lens unit 200 provides a FOV of 43.48 degrees, with EFL=7 mm, F#=2.86 and TTL=5.90 mm. Thus, advantageously, the ratio TTL/EFL=0.843. Advantageously, the Abbe number of the first, third and fifth lens elements is 56.18. The first air gap between lens elements 202 and 204 has a thickness (0.129 mm) which is about half the thickness d.sub.2 (0.251 mm). Advantageously, the Abbe number of the second lens element is 20.65 and of the fourth lens element is 23.35. Advantageously, the effective third air gap G between lens elements 206 and 208 is greater than TTL/5. Advantageously, the effective fourth air gap between lens elements 208 and 210 is smaller than TTL/50.

[0090] The focal length (in mm) of each lens element in lens unit 200 is as follows: f1=2.851, f2=−5.468, f3=−10.279, f4=7.368 and f5=−4.536. The condition 1.2×|f3|>|f2|<1.5×f1 is clearly satisfied, as 1.2×10.279>5.468>1.5×2.851. f1 also fulfills the condition f1<TTL/2, as 2.851<2.950.

[0091] FIG. 4A shows a schematic illustration of an optical lens unit 300, according to yet a further example of the presently disclosed subject matter. FIG. 4B shows the MTF vs. focus shift of the entire optical lens system for various fields in embodiment 300. FIG. 4C shows the distortion +Y in percent vs. field.

[0092] Lens unit 300 comprises, in order from an object side to an image side, an optional stop 301; a telephoto lens assembly including a first plastic lens element 302 with positive refractive power having a convex object-side surface 302a and a convex or concave image-side surface 302b, a second plastic lens element 204 with negative refractive power, having a meniscus convex object-side surface 304a, with an image side surface marked 304b, a third plastic lens element 306 with negative refractive power having a concave object-side surface 306a with an inflection point and a concave image-side surface 306b; and a field lens assembly including a fourth plastic lens element 308 with positive refractive power having a positive meniscus, with a concave object-side surface marked 308a and an image-side surface marked 308b, and a fifth plastic lens element 310 with negative refractive power having a negative meniscus, with a concave object-side surface marked 310a and an image-side surface marked 310b. Also, an optional glass window 312 may be disposed between the image-side surface 310b of fifth lens element 310 and an image plane 314.

[0093] According to the present example of lens unit 300, all lens element surfaces are aspheric. Detailed optical data is given in Table 5, and the aspheric surface data is given in Table 6, wherein the markings and units are the same as in, respectively, Tables 1 and 2. The equation of the aspheric surface profiles is the same as for lens units 100 and 200.

TABLE-US-00005 TABLE 5 Radius R Distances Diameter # Comment [mm] [mm] Nd/Vd [mm] 1 Stop Infinite −0.38 2.4 2 L11 1.5127 0.919 1.5148/63.1 2.5 3 L12 −13.3831 0.029 2.3 4 L21 8.4411 0.254 1.63549/23.91 2.1 5 L22 2.6181 0.426 1.8 6 L31 −17.9618 0.265  1.5345/57.09 1.8 7 L32 4.5841 1.998 1.7 8 L41 −2.8827 0.514 1.63549/23.91 3.4 9 L42 −1.9771 0.121 3.7 10 L51 −1.8665 0.431  1.5345/57.09 4.0 11 L52 −6.3670 0.538 4.4 12 Window Infinite 0.210  1.5168/64.17 3.0 13 Infinite 0.200 3.0

TABLE-US-00006 TABLE 6 Conic # coefficient k α.sub.2 α.sub.3 α.sub.4 α.sub.5 α.sub.6 2 −0.534 1.3253E−02 2.3699E−02 −2.8501E−02 1.7853E−02 −4.0314E−03 3 −13.473 3.0077E−02 4.7972E−03 1.4475E−02 −1.8490E−02 4.3565E−03 4 −10.132 7.0372E−04 1.1328E−01 1.2346E−03 −4.2655E−02 8.8625E−03 5 5.180 −1.9210E−03 2.3799E−01 −8.8055E−02 2.1447E−01 −1.2702E−01 6 0.000 2.6780E−01 1.8129E−02 −1.7323E−02 3.7372E−02 −2.1356E−02 7 10.037 2.7660E−01 −1.0291E−02 −6.0955E−02 7.5235E−02 −1.6521E−02 8 1.703 2.6462E−02 −1.2633E−02 −4.7724E−04 −3.2762E−03 1.6551E−03 9 −1.456 5.7704E−03 −1.8826E−02 5.1593E−03 −2.9999E−03 8.0685E−04 10 −6.511 −2.1699E−01 1.3692E−01 −4.2629E−02 6.8371E−03 −4.1415E−04 11 0.000 −1.5120E−01 8.6614E−02 −2.3324E−02 2.7361E−03 −1.1236E−04

[0094] Lens unit 300 provides a FOV of 44 degrees, EFL=6.84 mm, F#=2.80 and TTL=5.904 mm. Thus, advantageously, the ratio TTL/EFL=0.863. Advantageously, the Abbe number of the first lens element is 63.1, and of the third and fifth lens elements is 57.09. The first air gap between lens elements 302 and 304 has a thickness (0.029 mm) which is about 1/10.sup.th the thickness d.sub.2 (0.254 mm). Advantageously, the Abbe number of the second and fourth lens elements is 23.91. Advantageously, the effective third air gap G between lens elements 306 and 308 is greater than TTL/5. Advantageously, the effective fourth air gap between lens elements 308 and 310 is smaller than TTL/50.

[0095] The focal length (in mm) of each lens element in embodiment 300 is as follows: f1=2.687, f2=−6.016, f3=−6.777, f4=8.026 and f5=−5.090. The condition 1.2×|f3|>|f2|<1.5×f1 is clearly satisfied, as 1.2×6.777>6.016>1.5×2.687. f1 also fulfills the condition f1<TTL/2, as 2.687<2.952.

[0096] Tables 7 and 8 provide respectively detailed optical data and aspheric surface data for a fourth embodiment of an optical lens system disclosed herein. The markings and units are the same as in, respectively, Tables 1 and 2. The equation of the aspheric surface profiles is the same as for lens systems 100, 200 and 300. The lens elements in Tables 7 and 8 are designed to provide an image on an entire ¼″ sensor having dimensions of approximately 3.66×2.75 mm.

TABLE-US-00007 TABLE 7 Radius R Distances Diameter # Comment [mm] [mm] Nd/Vd [mm] 1 Stop Infinite −0.427 2.1 2 L11 1.3860 0.847 1.534809/55.66  2.2 3 L12 −8.5270 0.073 2.1 4 L21 11.1443 0.239 1.639078/23.253 1.9 5 L22 1.8641 0.504 1.7 6 L31 19.7342 0.239 1.534809/55.66  1.7 7 L32 3.9787 1.298 1.7 8 L41 −3.3312 0.522 1.639078/23.253 2.8 9 L42 −1.7156 0.079 3.1 10 L51 −1.7788 0.298 1.534809/55.66  3.5 11 L52 −12.6104 0.792 3.7 12 Window Infinite 0.210  1.5168/64.17 4.5 13 Infinite 0.177 4.6

TABLE-US-00008 TABLE 8 Conic # coefficient k α2 α3 α4 α5 α 6 2 −0.326 8.776E−03 2.987E−02 −6.001E−02 6.700E−02 −2.849E−02 3 −10.358 4.266E−02 −2.240E−02 2.914E−02 −3.025E−02 3.108E−03 4 11.447 −3.257E−02 9.780E−02 −1.143E−02 −3.844E−02 1.005E−02 5 −0.026 −3.631E−02 2.928E−01 −2.338E−01 3.334E−01 −2.760E−02 6 0.000 1.578E−01 −2.229E−02 −4.991E−02 1.663E−01 −1.298E−01 7 3.860 2.044E−01 5.451E−02 −3.199E−01 5.619E−01 −3.663E−01 8 4.094 3.706E−02 −5.931E−02 4.662E−02 −4.654E−02 1.606E−02 9 −9.119 −7.980E−02 −1.376E−03 5.622E−03 −6.715E−03 2.127E−03 10 −12.777 −2.695E−01 1.894E−01 −5.690E−02 8.689E−03 −5.269E−04 11 0.000 −1.807E−01 1.278E−01 −4.504E−02 6.593E−03 −2.357E−04

[0097] The focal length (in mm) of each lens element according to this example is as follows: f1=2.298, f2=−3.503, f3=−9.368, f4=4.846 and f5=−3.910. The condition 1.2×|f31|>|f2|<1.5×f1 is clearly satisfied, as 1.2×9.368>3.503>1.5×2.298. f1 also fulfills the condition f1<TTL/2, as 2.298<2.64. Generally, with regard to the effective air gap between the adjacent lens elements, the following should be noted.

[0098] In each one of the lens units exemplified above, the first three lens elements (L1, L2 and L3) achieve essentially a telephoto effect for all fields (angles of object orientation relative to the optical axis), i.e. achieve a strong concentration (by L1) followed by partial collimation (mainly by L2 but also by L3). The fact that all fields need to have essentially the same telephoto effect leads to relatively small distances (small air gaps) between the three lens elements, e.g. especially between L1 and L2 (air gap 1). L4 and L5 are mainly field lens elements for reducing field curvature, i.e. their main effect is to cause the focal point for all fields (where the object distance is approximately infinity) to reside on the sensor plane. To achieve this, it is advantageous that for every field, the corresponding rays hit L4 and L5 at different locations, thus enabling separate adjustment for every field (“field separation”).

[0099] The inventors have found that the desired fields' separation is obtainable in a lens unit design characterized by an “effective air gap” G between lenses L3 and L4 (between the telephoto and field lens assemblies, where a larger G leads to larger separation between the fields).

[0100] FIG. 5 illustrates the concept of the effective air gap between the two adjacent lens elements. First, an “air gap per field” D.sub.f−n is defined as the length of the n.sup.th field's chief ray along the respective chief ray between adjacent lens elements. Effective gap D.sub.Leff is then defined as the average of N air gaps per field for field angles α separated evenly between α=0 (for ray 1, air gap D.sub.f−1) to α=α.sub.max (for ray N, air gap D.sub.f−n), where ray N hits the end pixel on the image sensor diagonal. In other words, between each pair of adjacent lens elements (e.g. between L3 and L4 and between L4 and L5):

D.sub.Leff=(Σ.sub.n=1.sup.N D.sub.f−n)/N

[0101] In essence, the effective air gap between adjacent lens elements reflects an average effective distance between the two surfaces bounding the air gap between the two adjacent lens elements. Exemplarily, in FIG. 5 there are N=9 chief rays (and 9 related field air gaps) and the chief rays are distributed angularly evenly between α=0 for ray 1 and α.sub.max for ray 9. At α.sub.max, ray 9 hits the end pixel on the image sensor diagonal.

[0102] Table 9 shows data on TTL, D.sub.Leff-3, D.sub.Leff-4, and ratios between the TTL and the effective air gaps for each of lens units 100, 200 and 300 above. D.sub.Leff-3 and D.sub.Leff-4 were calculated using 9 chief rays, as shown in FIG. 4.

TABLE-US-00009 TABLE 9 Embodiment TTL D.sub.Leff-3 = G D.sub.Leff-4 D.sub.Leff-3/TTL D.sub.Leff-4/TTL 100 5.903 1.880 0.086 0.319 0.015 200 5.901 1.719 0.071 0.291 0.012 300 5.904 1.925 0.094 0.326 0.016 400 5.279 1.263 0.080 0.246 0.015
Using D.sub.Leff-3=G instead of the commonly used distance along the optical axis between L3 and L4 ensures better operation (for the purpose of reduction of field curvature) of lens elements L4 and L5 for all the fields. As seen in Table 9, good field separation may exemplarily be achieved if D.sub.Leff-3=G>TTL/5.

[0103] A compact optical design requires that the diameter of L5 be as small as possible while providing the required performance. Since the lens and camera footprint is determined by L5 diameter, a small effective air gap, D.sub.Leff-4, between lenses L4 and L5 is advantageous in that it allows a small diameter of lens L5 without degrading the optical performance Effective air gap D.sub.Leff-4 is a better indicator of the L5 diameter than the commonly used air gap along the optical axis between L4 and LS. An adequately small L5 diameter may exemplarily be achieved if the effective air gap between the field lenses L4 and L5 is D.sub.Leff-4<TTL/50.

[0104] It should be noted that an effective air gap D.sub.Leff can be calculated in principle using any combination of two or more chief rays (for example ray 1 and ray 9 in FIG. 4). However, the “quality” of D.sub.Leff calculation improves while considering an increased number of chief rays.

[0105] The miniature telephoto lens units described above with reference to FIGS. 1C and 2 to 5 are designed with a TTL shorter than EFL. Accordingly, due to shorter TTL, such lens units have a smaller field of view, as compared to standard mobile phone lens units. Therefore, it would be particularly useful to use such a telephoto lens unit as a Tele sub-camera lens unit in a dual aperture zoom camera. Such a dual aperture zoom camera is described in the above-mentioned WO14199338 of the same assignee as the present application.

[0106] As mentioned above, a problem associated with the use of conventional Wide and Tele lens modules in a camera is associated with the different lengths/heights of the lenses which can cause shadowing and light blocking effects. According to the presently disclosed subject matter it is suggested to eliminate or at least significantly reduce these shadowing and light blocking effects by replacing the conventional Tele lens module by the miniature telephoto lens unit described above in the dual aperture camera.

[0107] Thus, according to the presently disclosed subject matter, the problem discussed above posed by a difference in the TTL/EFL ratios of the conventional Tele and Wide lenses may be solved through use of a standard lens for the Wide camera (TTL.sub.W/EFL.sub.W>1.1, typically 1.3) and of a special Telephoto lens design for the Tele camera (TTL.sub.T/EFL.sub.T<1, e.g. 0.87), where the telephoto lens unit is configured as described above, providing the miniature telephoto lens unit.

[0108] Using the above described miniature telephoto lens unit enables to reduce the TTL.sub.T (according to one non-limiting example down to 7×0.87=6.09 mm) leading to a camera height of less than 7 mm (which is an acceptable height for a smartphone or any other mobile electronic device). The height difference between the telephoto lens unit and the Wide lens unit is also reduced to approximately 1.65 mm, thus reducing shadowing and light blocking problems.

[0109] According to some examples of a dual-aperture camera disclosed herein, the ratio “e”=EFL.sub.T/EFL.sub.T, is in the range 1.3-2.0. In some embodiments, the ratio TTL.sub.T/TTL.sub.W<0.8e. In some embodiments, TTL.sub.T/TTL.sub.W is in the range 1.0-1.25. According to some examples disclosed herein, EFL.sub.W may be in the range 2.5-6 mm and EFL.sub.T may be in the range 5-12 mm.

[0110] Referring now to the figures, FIG. 6A shows schematically in perspective cross section an example of a dual-aperture zoom camera device 600. Camera device 600 includes two camera unit 602 and 604. It should be understood that the two camera units may be associated with common or separate detectors (pixel matrix and their associated read out circuits). Thus, the two camera units are actually different in their optics, i.e. in the imaging channels defined by the wide and telephoto lens units. Each camera unit may be mounted on a separate PCB (respectively 605a and 605b) including the read out circuit, and includes a lens unit (respectively 606 and 608), and an image sensor including a pixel matrix (respectively 614 and 616), and an actuator (respectively 610 and 612) associated with a focusing mechanism. In this embodiment, the two PCBs lie in the same plane. It should be understood that in the embodiment where the readout circuits of the two imaging channels are in the same plane, a common PCB can be used, as will be described further below. The two camera units are connected by a case 618. For example, camera 602 includes a Wide lens unit and camera 604 includes a Telephoto lens unit, the TTL.sub.T of the lens unit defining the respective camera height H. For example, the Wide and Telephoto lens units provide respectively main and auxiliary optical/imaging paths, enabling to use the main image for interpreting the auxiliary image data.

[0111] FIG. 6B shows schematically, in perspective cross, another example of a dual-aperture zoom camera 600′ utilizing the principles of the invention. Camera 600′ is generally similar to the above-described camera 600, and the common components are shown in the figure in a self-explanatory manner and thus are not indicated by reference numbers. As in camera 600, in the camera 600′, the camera unit 602 (e.g. a Wide lens camera) and camera unit 604 (e.g. a Telephoto lens camera) are mounted on separate PCBs (respectively 605a and 605b). However, in contrast with camera 600, in camera 600′ the two PCBs lie in different planes. This enables the object side principal planes of the Wide and Telephoto lens units to be close one to the other, thus reducing the dependency of magnification factor in the two units on the object distance.

[0112] For example, camera dimensions for the cameras shown in FIGS. 6A and 6B may be as follows: a length L of the camera (in the Y direction) may vary between 13-25 mm, a width W of the camera (in the X direction) may vary between 6-12 mm, and a height H of the camera (in the Z direction, perpendicular to the X-Y plane) may vary between 4-12 mm. More specifically, considering a smartphone camera example disclosed herein, L=18 mm, W=8.5 mm and H=7 mm.

[0113] FIG. 7 shows schematically, in perspective cross section, yet another example of a dual-aperture zoom camera 700. Camera 700 is similar to cameras 600 and 600′ in that it includes two camera units 702 and 704 with respective lens units 706 and 708, respective actuators 710 and 712 and respective image sensors 714 and 716. However, in camera 700, the two camera units 702 and 704 are mounted on a single (common) PCB 705. The mounting on a single PCB and the minimizing of a distance “d” between the two camera units minimizes and may even completely avoid camera movement (e.g. associated with mishaps such as drop impact). In general, the dimensions of camera 700 may be in the same range as those of cameras 600 and 600′. However, for the same sensors and optics, the footprint W×L and the weight of camera 700 are smaller than that of cameras 600 and 600′. Mishaps such as drop impact may cause a relative movement between the two cameras after system calibration, changing the pixel matching between the Tele and Wide images and thus preventing fast reliable fusion of the Tele and Wide images. Therefore, such effects should preferably be eliminated.

[0114] As described above, the high-quality imaging is also associated with the implementation of standard optical image stabilization (OIS) in such a dual-aperture zoom camera. Standard OIS compensates for camera tilt (“CT”), i.e., image blur, by a parallel-to-the image sensor (exemplarily in the X-Y plane) lens movement (“LMV”). The amount of LMV (in millimeters) needed to counter a given camera tilt depends on the camera lens EFL, according to the relation:

LMV=CT*EFL,

where “CT” is in radians and EFL is in mm.

[0115] Since the Wide and telephoto lens units have significantly different EFLs, both lenses cannot move together and achieve optimal tilt compensation for both of the respective camera units. More specifically, since the tilt is the same for both camera units, a movement that will compensate for the tilt for the Wide camera unit will be insufficient to compensate for the tilt for the Telephoto camera unit, and vice versa. Using separate OIS actuators for the two camera units respectively can achieve simultaneous tilt compensation for both of them, but the entire system would be complex and costly, which is undesirable for portable electronic devices.

[0116] In this connection, reference is made to FIG. 8 which shows an example of a dual-aperture zoom camera 800 (similar to the above-described camera 700) that includes two camera units 802 and 804 mounted either on a single PCB 805 (as shown in this example) or on separate PCBs. Each camera unit includes a lens unit (respectively 806 and 808), an actuator (respectively 810 and 812) and an image sensor (respectively 814 and 816). The two actuators are rigidly mounted on a rigid base 818 that is flexibly connected to the PCB (or PCBs) through flexible elements 820. Base 818 is movable by an OIS mechanism (not shown) controlled by an OIS controller 902 (shown in FIG. 9). The OIS controller 902 is coupled to, and receives camera tilt information from a tilt sensor (e.g. a gyroscope) 904 (FIG. 9). More details of an example of an OIS procedure as disclosed herein are given below with reference to FIG. 9. The two camera units are separated by a small distance “d”, e.g. 1 mm. This small distance between camera units also reduces the perspective effect enabling smoother zoom transition between the camera units.

[0117] As indicated above, the two image sensors 814 and 816 may be mounted on separate PCBs that are rigidly connected, thereby enabling adaptation of an OIS mechanism to other system configurations, for example those described above with reference to FIGS. 6A and 6B.

[0118] In some embodiments, and optionally, a magnetic shield plate may be used, e.g. as described in co-owned U.S. patent application Ser. No. 14/365,718 titled “Magnetic shielding between voice coil motors in a dual-aperture camera”, which is incorporated herein by reference in its entirety. Such a magnetic shield plate may be inserted in the gap (with width d) between the Wide and Tele camera units.

[0119] In general, the dimensions of camera 800 may be in the same range as those of cameras 600, 600′ and 700.

[0120] Reference is made to FIG. 9, which exemplifies the camera operation, utilizing a tilt sensor 904 which dynamically measures the camera tilt (which is the same for both the Wide and Tele camera units). As shown, an OIS controller 902 (electronic circuit including hardware/software components) is provided, which is coupled to the actuators of both camera units (e.g. through base 818), and receives a CT input from the tilt sensor 904 and a user-defined zoom factor, and controls the lens movement of the two camera units to compensate for the tilt. The LMV is for example in the X-Y plane. The OIS controller 902 is configured to provide a LMV equal to CT*EFL.sub.ZF, where “EFL.sub.ZF” is chosen according to the user-defined zoom factor, ZF. According to one example of an OIS procedure, when ZF=1, LMV is determined by the Wide camera unit's EFL.sub.W (i.e. EFL.sub.ZF=EFL.sub.W and LMV=CT*EFL.sub.W). Further, when ZF>e (i.e. ZF>EFL.sub.T/EFL.sub.W), LMV is determined by the telephoto camera unit's EFL.sub.T (i.e. EFL.sub.ZF=EFL.sub.T and LMV=CT* EFL.sub.T). Further yet, for a ZF between 1 and e, the EFL.sub.ZF may shift gradually from EFL.sub.W to EFL.sub.T according to EFL.sub.ZF=ZF*EFL.sub.W.

[0121] Thus, the present invention provides a novel approach for configuring a camera device suitable for use in portable electronic devices, in particular smart phones. The present invention solves various problems associated with the requirements for physical parameters of such devices (weight, size), high image quality and zooming effects.