IP Library Granted Patent US 12,638,556
Granted Patent B2
US 12,638,556 · App. 18/291,547 · Granted May 26, 2026

LiDAR device for scanning measurement of a distance to an object

Inventors: Vladan Blahnik (Oberkochen, DE); Holger Münz (Aalen, DE); Martin Peschka (Aalen, DE)
Assignee: Scantinel Photonics GmbH
G01S7/4815G01S7/4817G01S17/32G01S17/48G01S17/89G02B6/32G02B6/4206G01S17/931
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Quick Facts
Patent No.
US 12,638,556
App. No.
18/291,547
Granted
May 26, 2026
Kind
B2
Abstract

A LiDAR device ( 14 ) for scanning measurement of a distance to an object ( 12 ) comprises a photonic integrated circuit ( 52 ) with a plurality of optical waveguides ( 38 ) and a plurality of couplers 40 ). Each coupler ( 40 ) emits light guided in the optical waveguide ( 38 ) into free space and/or couples light propagating in free space into the optical waveguide ( 38 ). A collimating optical system ( 44 ) collimates light beams emitted by the couplers ( 40 ) and/or focuses collimated light beams. Microlenses ( 54; 54 a, 54 b ) form real or virtual images of associated couplers ( 40 ), said images being arranged in an object field ( 56 ) of the collimating optical system ( 44 ). The collimating optical system ( 44 ) has a collimator numerical aperture which is greater than each of the coupler numerical apertures. Each microlens ( 54; 54 a, 54 b ) has a collimator-side numerical aperture that is greater than its coupler-side numerical aperture. In this manner, insertion losses caused by NA mismatch are reduced.

Claims (46)

1 . A LiDAR device for scanning measurement of a distance to an object, wherein the device comprises:

a photonic integrated circuit comprising a plurality of optical waveguides and a plurality of couplers, wherein each coupler is

associated with one of the optical waveguides and

configured to couple light guided in the optical waveguide into free space and/or light propagating in free space into the optical waveguide,

a collimating optical system configured to collimate light beams emitted by the couplers and/or to focus collimated light beams, and

a plurality of microlenses, wherein

each microlens is associated with one of the couplers and

forms a real or virtual image of the associated coupler, wherein the images of the couplers are arranged in an object field of the collimating optical system,

wherein

each coupler has a coupler numerical aperture and the collimating optical system has a collimator numerical aperture which is greater than each of the coupler numerical apertures, and wherein

each microlens has, on a side pointing towards the couplers, a coupler-side numerical aperture, and on a side pointing towards the collimating optical system a collimator-side numerical aperture that is greater than the coupler-side numerical aperture.

2 . The device of claim 1 , wherein the coupler numerical aperture of each coupler differs from the coupler-side numerical aperture of the associated microlens by less than 10%, and wherein the collimator numerical aperture differs from the collimator-side numerical aperture of the microlenses by less than 10%.

3 . The device of claim 1 , wherein each microlens comprises two curved surfaces having a different refractive power.

4 . The device of claim 1 , wherein

the couplers are arranged in a surface of the photonic integrated circuit,

the couplers are configured to emit and/or to receive light beams each having a centroid ray that forms an angle with a local surface normal, wherein the angle is between 5° and 70°, and wherein

optical axes of the microlenses and directions of the associated centroid rays coincide and are parallel to an optical axis of the collimating optical system.

5 . The device of claim 4 , wherein the surface is planar and has a surface normal that forms a non-zero angle to the optical axis of the collimating optical system.

6 . The device of claim 1 , wherein the microlenses have different thicknesses.

7 . The device of claim 1 , wherein each microlens is configured to transform an input angular light energy distribution produced by the associated coupler into an output angular light energy distribution that is flatter and/or broader than the input angular light energy distribution.

8 . The device of claim 7 , wherein the output angular light energy distribution is a rectangular distribution.

9 . The device of claim 7 , wherein two or more microlenses are associated with each coupler.

10 . The device of claim 1 , wherein at least some microlenses have at least one aspherical lens surface.

11 . The device of claim 1 , wherein the object field of the collimating optics is curved.

12 . A LiDAR device for scanning measurement of a distance to an object, wherein the device comprises:

a photonic integrated circuit comprising a plurality of optical waveguides and a plurality of couplers, wherein each coupler is

associated with one of the optical waveguides and

configured to couple light guided in the optical waveguide into free space and/or light propagating in free space into the optical waveguide,

a collimating optical system configured to collimate light beams emitted by the couplers and/or to focus collimated light beams, and

a plurality of microlenses, wherein

each microlens is associated with one of the couplers and

forms a real or virtual image of the associated coupler, wherein the images of the couplers are arranged in an object field of the collimating optical system,

wherein

each coupler has a coupler numerical aperture and the collimating optical system has a collimator numerical aperture which is greater than each of the coupler numerical apertures, and wherein

each microlens has, on a side pointing towards the couplers, a coupler-side numerical aperture, and on a side pointing towards the collimating optical system a collimator-side numerical aperture that is greater than the coupler-side numerical aperture, and the LiDAR device comprising a transparent plane-parallel plate that is arranged between the microlenses and the collimating optical system.

13 . A LiDAR device for scanning measurement of a distance to an object, wherein the device comprises:

a photonic integrated circuit comprising a plurality of optical waveguides and a plurality of couplers, wherein each coupler is

associated with one of the optical waveguides and

configured to couple light guided in the optical waveguide into free space and/or light propagating in free space into the optical waveguide,

a collimating optical system configured to collimate light beams emitted by the couplers and/or to focus collimated light beams, and

a plurality of microlenses, wherein each microlens

is associated with one of the couplers,

forms a real or virtual image of the associated coupler, wherein the images of the couplers are arranged in an object field of the collimating optical system, and

is configured to transform an input angular light energy distribution produced by the associated coupler into an output angular light energy distribution that is flatter and/or broader than the input angular light energy distribution.

14 . The device of claim 13 , wherein the output angular light energy distribution is a rectangular distribution.

15 . The device of claim 13 , wherein two or more microlenses are associated with each coupler.

Assignments (2)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 6, 2026
From: SCANTINEL PHOTONICS GMBH
To: SCANTINEL GMBH
Reel/Frame 075353/0757 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jan 24, 2024
From: BLAHNIK, VLADAN; MÜNZ, HOLGER; PESCHKA, MARTIN
To: SCANTINEL PHOTONICS GMBH
Reel/Frame 066230/0140 →
Priority Claims (1)
EP 21187955 · Jul 27, 2021 · regional
Continuity (1)
Related Publication 20250093592A1 · Mar 20, 2025
References Cited (22)
US 10545289B1 · Chriqui · 2020 [cited by examiner]
US 11579356B2 · Swanson · 2023 [cited by examiner]
US 11796680B2 · Wu · 2023 [cited by examiner]
US 12140676B2 · Seok · 2024 [cited by examiner]
US 12313790B2 · Sutton · 2025 [cited by examiner]
US 12379605B2 · Lee · 2025 [cited by examiner]
US 20130206967A1 · Shpunt et al. · 2013 [cited by applicant]
US 20170371227A1 · Skirlo et al. · 2017 [cited by applicant]
US 20180329060A1 · Pacala et al. · 2018 [cited by applicant]
US 20190377135A1 · Mansouri Rad et al. · 2019 [cited by applicant]
US 20210116703A1 · Pulikkaseril et al. · 2021 [cited by applicant]
US 20210165102A1 · Crouch et al. · 2021 [cited by applicant]
US 20210316756A1 · Davydenko · 2021 [cited by applicant]
US 20220146903A1 · Watts · 2022 [cited by examiner]
US 20220236384A1 · Sutton et al. · 2022 [cited by applicant]
US 20230288638A1 · Balbás · 2023 [cited by examiner]
DE 102020110142A1 · 2021 [cited by applicant]
WO WO2021029969A1 · 2021 [cited by examiner]
WO WO2023006470A1 · 2023 [cited by applicant]
Scantinel Photonics GMBH, Extended European Search Report, EP Patent Application No. 21187955.6, Jan. 20, 2022, 9 pgs. [cited by applicant]
Scantinel Photonics GMBH, International Search Report and Written Opinion, PCT/EP2022/070036, Nov. 16, 2022, 12 pgs. [cited by applicant]
Scantinel Photonics GMBH, Korean Office Action, KR Patent Application No. 10-2024-7003608, Jan. 20, 2026, 10 pgs. [cited by applicant]