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Collimating lens and projection module

A lens and collimation technology, applied in the field of camera lens, can solve the problems of low yield, larger image point, difficult production and processing, etc., and achieve the effect of low cost and stable focal length

Active Publication Date: 2020-06-23
JIANGXI LIANYI OPTICS CO LTD
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

AI Technical Summary

Problems solved by technology

[0004] However, in the existing smartphones, as the temperature of the use environment changes, the focal length f of the lens changes greatly, resulting in a significant change in the angle of the lens projected light, which will change the original light information, resulting in the entire There are errors in the calculation of the system, which affect the accuracy of the contour restoration of the three-dimensional object. There is also the case that the projected image point becomes larger with the change of temperature, which will also lead to a decrease in the definition of the three-dimensional object restored by the system. Therefore, with the use of When the ambient temperature changes, it is particularly important that the field of view angle and the size of the spot of the light information projected to the measured object do not change greatly
[0005] In addition, the first lens of the traditional collimator lens close to the laser transmitter is a molded glass lens. This molded glass lens is too small, difficult to produce and process, low yield, and difficult to mass-produce, which greatly increases the production cost.

Method used

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  • Collimating lens and projection module

Examples

Experimental program
Comparison scheme
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no. 1 example

[0087] see figure 1 , a schematic structural diagram of a collimating lens 10 provided in this embodiment, the laser emitter end is set as the object side S0, the measured object end is the image side S7, and the sequence from the object side S0 to the image side S7 includes: the first lens L1, second lens L2, third lens L3 and stop ST.

[0088] The first lens L1 has positive refractive power, the object side S1 of the first lens L1 is a convex surface, and the image side S2 of the first lens L1 is a concave surface.

[0089] The second lens L2 has negative refractive power, and both the object side S3 and the image side S4 of the second lens L2 are concave.

[0090] The third lens L3 has positive refractive power, the object side S5 of the third lens L3 is concave and the image side S6 is convex.

[0091] The stop ST is located between the third lens L3 and the object to be measured. The optical centers of each lens are located on the same straight line, and each lens is m...

no. 2 example

[0105] The structural representation of the collimating lens 20 of the present embodiment can refer to Figure 5 . This embodiment is roughly similar to the lens structure diagram of the first embodiment, except that the relevant parameters of each lens are different.

[0106] The relevant parameters of each lens in the collimating lens 20 in this embodiment are shown in Table 3.

[0107] table 3

[0108] Surface serial number surface type r d n d

Vd object plane S0 sphere — 0.420 S1 first lens Aspherical 0.646 0.395 1.640 23.529 S2 Aspherical 1.289 0.823 S3 second lens Aspherical -0.513 0.266 1.516 57.038 S4 Aspherical 14.889 0.657 S5 third lens Aspherical 5.288 0.525 1.640 23.529 S6 Aspherical -1.233 0.350 ST aperture sphere — 300.000 S7 Image surface sphere — —

[0109] The aspherical parameters of each lens in this embodiment...

no. 3 example

[0115] The structural representation of the collimating lens 30 of the present embodiment can refer to Figure 9 , this embodiment is roughly similar to the lens structure diagram of the first embodiment, except that the relevant parameters of each lens are different.

[0116] The relevant parameters of each lens in the collimating lens 30 in this embodiment are shown in Table 5.

[0117] table 5

[0118] Surface serial number surface type r d n d

Vd object plane S0 sphere — 0.250 S1 first lens Aspherical 0.647 0.524 1.640 23.529 S2 Aspherical 1.412 0.592 S3 second lens Aspherical -0.726 0.170 1.640 23.529 S4 Aspherical 1.232 0.773 S5 third lens Aspherical 21.774 0.641 1.640 23.529 S6 Aspherical -1.054 0.400 ST aperture sphere — 300.000 S7 Image surface sphere — —

[0119] The aspheric parameters of each lens in this embodiment ar...

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Abstract

The invention provides a collimating lens and a projection module. The end of the laser emitter is set as the object side, and the end of the object to be measured is set as the image side. Along the optical axis from the object side to the image side, it includes: A lens, a second lens with negative power, a third lens with positive power and a stop. The object side of the first lens is convex; the object side of the second lens is concave; the object side of the third lens is convex or near plane and the image side is convex; the aperture is located between the third lens and the measured object. The first lens, the second lens, and the third lens are all made of plastic; the collimating lens satisfies the following conditional formula: (dn / dt) 1 <‑30×10 ‑6 / °C; (dn / dt) 2 <‑30×10 ‑6 / °C; (dn / dt) 3 <‑30×10 ‑6 / °C; The collimating lens and projection module provided by the present invention clearly define the rate of change of the refractive index of the three lenses with temperature, which is used to reasonably match the thermal expansion characteristics of the lens, so as to achieve stable focal length, and is suitable for different temperatures occasion.

Description

technical field [0001] The invention relates to the field of camera lens technology, in particular to a collimator lens and a projection module. Background technique [0002] With the rapid development of smart phones, innovative technologies are constantly emerging in the camera functions of mobile phones, such as the 3D imaging technology promoted by Apple, which is an optical sensing technology based on 3D structured light, which can be used for face and gesture recognition, enhanced The camera function brings new AR applications, transforming optical images from the past two-dimensional space to three-dimensional space, thus bringing a more real and clear perception experience. [0003] 3D structured light means that after specific laser information is projected onto the surface of an object, it is collected by a camera, and information such as the position and depth of the object is calculated according to the change of light information caused by the object, and then t...

Claims

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Application Information

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Patent Type & Authority Patents(China)
IPC IPC(8): G02B19/00G03B15/02G02B1/04
CPCG02B19/0014G02B19/0047G03B15/02G02B1/041G02B13/0035G02B7/008H04M1/0264H04M2250/52G01B11/2513G01B5/0014H04N23/55G02B13/0055G02B27/30H04N9/3161
Inventor 刘绪明曾昊杰曾吉勇
Owner JIANGXI LIANYI OPTICS CO LTD
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