Two-state zoom folded camera
11635596 · 2023-04-25
Assignee
Inventors
- Gil Bachar (Tel Aviv, IL)
- Gal Shabtay (Tel Aviv, IL)
- Ephraim Goldenberg (Ashdod, IL)
- Roy Rudnick (Tel Aviv, IL)
- Michael Dror (Nes Ziona, IL)
- Noy Cohen (Tel Aviv, IL)
Cpc classification
G02B13/18
PHYSICS
H04N23/55
ELECTRICITY
International classification
G02B13/00
PHYSICS
Abstract
A zoom camera comprising an optical path folding element (OPFE) for folding the light from a first optical path to a second optical path, a first lens having a first optical axis and a first effective focal length EFL.sub.L1, the first optical axis being along the second optical path, a collimating lens having a second optical axis, and an image sensor located on the second optical path, wherein the collimating lens is movable between at least a first state and a second state, wherein in the first state the collimating lens is positioned in the second optical path between the OPFE and the first lens such that light entering the first lens arrives only from the image side of the collimating lens, and wherein in the second state the collimating lens is positioned outside the first optical path such that light entering the first lens does not arrive from the image side of the collimating lens.
Claims
1. A zoom camera comprising: a) a single optical path folding element (OPFE) for folding the light from a first optical path to a second optical path; b) a first lens having a first optical axis and a first effective focal length EFL.sub.L1, the first optical axis being along the second optical path; c) a collimating lens having a second optical axis; and d) an image sensor located on the second optical path, wherein the collimating lens is movable to provide at least a first state and a second state, wherein in the first state the collimating lens is positioned in the second optical path between an image side of the single OPFE and the first lens such that light entering the first lens arrives only from the image side of the collimating lens, and wherein in the second state the collimating lens is positioned outside the second optical path such that light entering the first lens arrives directly from the image side of the single OPFE and does not arrive from the image side of the collimating lens.
2. The zoom camera of claim 1, wherein in the first state the camera has a first combined effective camera focal length EFL.sub.c1 different than EFL.sub.L1, and wherein in the second state the camera has a second combined effective camera focal length EFL.sub.c2 equal to EFL.sub.L1.
3. The zoom camera of claim 2, wherein a difference between EFL.sub.L1 and EFL.sub.c2 is of at least ±10%.
4. The zoom camera of claim 3, wherein the first lens is operative to move along the first optical axis to change camera focus in both the first state and second state.
5. The zoom camera of claim 2, wherein a difference between EFL.sub.L1 and EFL.sub.c2 is of at least ±50%.
6. The zoom camera of claim 5, wherein the first lens is operative to move along the first optical axis to change camera focus in both the first state and second state.
7. The zoom camera of claim 2, wherein a difference between EFL.sub.L1 and EFL.sub.c2 is of at least ±80%.
8. The zoom camera of claim 7, wherein the first lens is operative to move along the first optical axis to change camera focus in both the first state and second state.
9. The zoom camera of claim 1, wherein the collimating lens is a telescopic lens.
10. The zoom camera of claim 1, wherein the first lens is operative to move along the first optical axis to change camera focus in both the first state and second state.
11. The zoom camera of claim 2, wherein the collimating lens is a telescopic lens.
12. The zoom camera of claim 2, wherein the first lens is operative to move along the first optical axis to change camera focus in both the first state and second state.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1) Aspects, embodiments and features disclosed herein will become apparent from the following detailed description when considered in conjunction with the accompanying drawings.
(2)
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DETAILED DESCRIPTION
(8)
(9) Imaging lens 104 and collimating lens 108 may comprise each a single lens element or a plurality of lens elements. Embodiments of lenses 104 and 108 are shown in
(10) In zoom camera 100, collimating lens 108 may shift mechanically between at least two operational states (or simply “states”).
(11)
(12)
(13)
(14) The optical design of collimating lens 108 is such that EFL.sub.C2 is different from EFL.sub.C1. According to an example, collimating lens 108 may be a telescopic lens, such that the introduction of the collimating lens 108 into the second optical path 116 increases or decreases EFL.sub.C from EFL.sub.C2 to EFL.sub.C1. According to an example, EFL.sub.C2 is different (smaller or larger) by more than 10% from EFL.sub.C1. According to an example, EFL.sub.C2 is different by more than 80% from EFL.sub.C2. According to an example, EFL.sub.C2 is in the range of 10-18 mm and EFL.sub.C1 is in the range of 20-36 mm According to an example, EFL.sub.C2 is in the range of 10-18 mm and EFL.sub.C1 is in the range of 5-9 mm.
(15)
(16) Tables 1-3 below provide the optical design of camera 200. The surfaces of various optical elements are listed starting from the sensor 112 (image) side to the prism 102 (object) side. Table 1 provide data for all the surfaces except the prism surfaces: “type” is the surface type (flat or aspheric), R is the surface radius of curvature, T is the surface thickness, Nd is the surface refraction index, Vd is the surface Abbe number, D/2 is the surface semi diameter. Table 2 provide aspheric data for aspheric surfaces in Table 1, according to the following formula:
(17) Q type 1 surface sag formula:
(18)
where {z, r} are the standard cylindrical polar coordinates, c is the paraxial curvature of the surface, k is the conic parameter, r.sub.max is one half of the surfaces clear aperture, and A.sub.n are the polynomial coefficients shown in lens data tables.
(19) Table 3 provide data for surfaces of prism 202 only: A is the prism (without bevel) face length, W is the face width, and other fields are like in Table 1. Note that a prism may or may not have a bevel.
(20) In camera 200, first lens 104 has an EFL of 15 mm. The design of second (collimating) lens 108 is of a telescopic lens. Lens 108 in camera 200 has a magnification ratio of 2: two lens elements L1 and L2 form a positive doublet with a focal length of 15 mm and two lens elements L3 and L4 form a negative doublet with a focal length of −7.5 mm. As a result, when in the first operational state, the camera has an EFL of EFL.sub.C1=30 mm. When in the second operation state, the camera has an EFL of EFL.sub.C2=EFL.sub.C1=15 mm. In another example, replacing collimating lens 108 with a lens having a magnification ratio of 0.5 (e.g. by using a first negative doublet with a focal length of −15 mm and a second positive doublet with a focal length of 7.5 mm) would result in decreasing EFL.sub.C by factor of 2. Thus, in this example, the ratio EFL.sub.C1/EFL.sub.C2 in cameras 100 and 200 can be in the range of 0.2 to 5.
(21) The telescopic design of collimating lens 108 allows for a less accurate positioning of collimating lens 108 relative to first lens 104: a shift and/or tilt of collimating lens 108 in any direction (in particular shift along first optical axis 106, shift perpendicular to first optical axis 106, and/or rotation of the lens) will not change the magnification ratio. For example, relative to a nominal position (presented in
(22) Note that in the first state, the first and second optical axes are parallel and a change in distance between the two optical axes does not change EFL.sub.C1. Similarly, a change in distance between the first and collimating lenses does not change EFL.sub.C1. That is, in the first state, EFL.sub.C1 is substantially independent of the distance between optical axes of, or distances between lenses 104 and 108.
(23)
(24) In cameras 100 and 200, focusing in both operational states may be performed by moving first lens 104 along first optical axis 106. In both cameras, optical image stabilization (OIS) in both operational states may be performed by moving first lens 104 perpendicular to optical axis 106 and/or by tilting OPFE 102 and/or by combining shift of first lens 104 and tilt of OPFE 102. These actions may be performed using actuators or mechanisms known in the art.
(25) TABLE-US-00001 TABLE 1 Com- D/2 # ment Type R [mm] T [mm] Nd Vd [mm] S.sub.1 Image flat Infinity 0.500 1.878 S.sub.2 IR flat Infinity 0.210 1.516 64.167 1.900 Filter S.sub.3 flat Infinity 5.460 1.900 S.sub.4 L.sub.5S.sub.2 Q-Type Aspheric −13.571 0.853 1.650 21.513 1.831 S.sub.5 L.sub.5S.sub.1 Q-Type Aspheric −2.840 0.079 1.797 S.sub.6 L.sub.4S.sub.2 Q-Type Aspheric −3.728 0.436 1.534 55.663 1.706 S.sub.7 L.sub.4S.sub.1 Q-Type Aspheric 6.712 0.368 1.648 S.sub.8 L.sub.3S.sub.2 Q-Type Aspheric −248.667 0.883 1.534 55.663 1.654 S.sub.9 L.sub.3S.sub.1 Q-Type Aspheric −4.471 0.081 1.706 S.sub.10 L.sub.2S.sub.2 Q-Type Aspheric −5.197 0.518 1.650 21.513 1.706 S.sub.11 L.sub.2S.sub.1 Q-Type Aspheric 9.451 2.152 1.895 S.sub.12 L.sub.1S.sub.2 Q-Type Aspheric −24.950 1.523 1.484 84.146 2.250 S.sub.13 L.sub.1S.sub.1 Q-Type Aspheric −3.349 −0.840 2.250 S.sub.14 Stop flat Infinity 2.435 2.250 S.sub.15 Z.sub.4S.sub.2 Q-Type Aspheric −3.166 0.500 1.829 42.726 2.230 S.sub.16 Z.sub.4S.sub.1 Q-Type Aspheric 38.480 0.060 2.230 S.sub.17 Z.sub.3S.sub.2 Q-Type Aspheric 12.476 1.111 1.650 21.513 2.230 S.sub.18 Z.sub.3S.sub.1 Q-Type Aspheric −11.693 3.270 2.230 S.sub.19 Z.sub.2S.sub.2 Q-Type Aspheric 88.558 2.000 1.665 55.117 2.300 S.sub.20 Z.sub.2S.sub.1 Q-Type Aspheric −5.530 0.060 2.300 S.sub.21 Z.sub.1S.sub.2 Q-Type Aspheric −5.556 0.500 2.005 21.000 2.300 S.sub.22 Z.sub.1S.sub.1 Q-Type Aspheric −7.644 0.500 2.300
(26) TABLE-US-00002 TABLE 2 # k r.sub.max A.sub.0 A.sub.1 A.sub.2 A.sub.3 A.sub.4 A.sub.5 S.sub.4 −0.834 1.858 3.55E−02 −6.06E−03 2.26E−04 5.15E−04 −2.26E−04 −2.10E−05 S.sub.5 −6.008 1.858 1.50E−02 −1.73E−02 6.19E−03 −1.50E−03 7.16E−05 −1.84E−05 S.sub.6 −17.754 1.833 3.32E−02 −1.56E−02 6.87E−03 −4.24E−03 1.27E−03 −4.59E−04 S.sub.7 −8.169 1.833 1.56E−01 −1.90E−02 4.15E−03 −8.86E−04 5.73E−03 4.55E−04 S.sub.8 116.131 1.903 2.11E−03 2.66E−02 3.50E−02 1.36E−02 1.03E−02 2.09E−03 S.sub.9 −1.064 1.903 7.70E−02 −3.48E−03 9.94E−03 −3.66E−03 −1.75E−03 −1.37E−03 S.sub.10 −1.581 1.953 −1.10E−01 −8.34E−02 −4.32E−02 −2.31E−02 −9.94E−03 −2.84E−03 S.sub.11 −3.312 1.953 −7.74E−02 3.73E−03 −3.48E−03 5.87E−04 −3.68E−04 5.19E−05 S.sub.12 −81.481 2.754 −8.12E−02 6.15E−03 4.95E−05 1.13E−04 −6.61E−05 −1.87E−06 S.sub.13 −0.263 2.754 −6.88E−02 −8.71E−03 −1.15E−03 −1.54E−05 −6.84E−07 9.92E−08 S.sub.15 −0.624 3.600 8.51E−01 −2.00E−01 2.69E−02 −4.74E−03 0.00E+00 0.00E+00 S.sub.16 −99.998 3.600 5.34E−02 −3.81E−01 1.98E−02 −1.08E−02 0.00E+00 0.00E+00 S.sub.17 5.259 3.600 1.69E+00 1.57E−01 6.69E−02 −5.86E−03 0.00E+00 0.00E+00 S.sub.18 −3.735 3.600 2.85E+00 6.02E−01 8.16E−02 2.81E−04 0.00E+00 0.00E+00 S.sub.19 −29.541 3.750 5.18E−02 2.26E−02 −2.67E−03 −7.68E−04 0.00E+00 0.00E+00 S.sub.20 −0.096 3.750 −4.51E−02 2.86E−02 3.54E−03 2.66E−04 0.00E+00 0.00E+00 S.sub.21 0.022 3.750 −5.04E−02 3.29E−02 9.80E−03 2.21E−03 0.00E+00 0.00E+00 S.sub.22 0.548 3.750 −1.41E−02 −1.70E−02 −4.03E−03 −7.61E−04 0.00E+00 0.00E+00
(27) TABLE-US-00003 TABLE 3 R T A/2 W/2 # Type [mm] [mm] Nd Vd [mm] [mm] S.sub.23 Prism Infinity 3.050 1.840 23.000 2.850 3.000 Object side S.sub.24 Prism Infinity −2.650 1.840 23.000 — — Reflective face S.sub.25 Prism Infinity — 2.850 3.000 Image side
(28) While this disclosure has been described in terms of certain embodiments and generally associated methods, alterations and permutations of the embodiments and methods will be apparent to those skilled in the art. The disclosure is to be understood as not limited by the specific embodiments described herein, but only by the scope of the appended claims.