WO2023099952A1 - Appareil optomécanique pour applications optiques à grand angle - Google Patents

Appareil optomécanique pour applications optiques à grand angle Download PDF

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Publication number
WO2023099952A1
WO2023099952A1 PCT/IB2021/061401 IB2021061401W WO2023099952A1 WO 2023099952 A1 WO2023099952 A1 WO 2023099952A1 IB 2021061401 W IB2021061401 W IB 2021061401W WO 2023099952 A1 WO2023099952 A1 WO 2023099952A1
Authority
WO
WIPO (PCT)
Prior art keywords
monocentric
optomechanical
ball lens
spherical
spherical hemisphere
Prior art date
Application number
PCT/IB2021/061401
Other languages
English (en)
Inventor
Mónica Catarina COSTA CERQUIDO
André ALBUQUERQUE
Pedro Nelson SAMPAIO BARBOSA
Alexandre Manuel CORREIA
João André MORAIS GOMES DOS SANTOS
Sandro Filipe CARDOSO HORA
Jorge Miguel NUNES DOS SANTOS CABRAL
Original Assignee
Bosch Car Multimedia Portugal, S.A.
Universidade Do Minho
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Bosch Car Multimedia Portugal, S.A., Universidade Do Minho filed Critical Bosch Car Multimedia Portugal, S.A.
Publication of WO2023099952A1 publication Critical patent/WO2023099952A1/fr

Links

Classifications

    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
    • G01S7/481—Constructional features, e.g. arrangements of optical elements
    • G01S7/4818—Constructional features, e.g. arrangements of optical elements using optical fibres
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S17/00—Systems using the reflection or reradiation of electromagnetic waves other than radio waves, e.g. lidar systems
    • G01S17/88—Lidar systems specially adapted for specific applications
    • G01S17/93—Lidar systems specially adapted for specific applications for anti-collision purposes
    • G01S17/931—Lidar systems specially adapted for specific applications for anti-collision purposes of land vehicles
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
    • G01S7/481—Constructional features, e.g. arrangements of optical elements
    • G01S7/4816—Constructional features, e.g. arrangements of optical elements of receivers alone
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B7/00—Mountings, adjusting means, or light-tight connections, for optical elements
    • G02B7/02—Mountings, adjusting means, or light-tight connections, for optical elements for lenses
    • G02B7/027—Mountings, adjusting means, or light-tight connections, for optical elements for lenses the lens being in the form of a sphere or ball

Definitions

  • This application discloses an optomechanical apparatus for wide-angle optical applications .
  • Optomechanical systems are a sub-discipline of optical and mechanical engineering in which optics such as lenses , mirrors , fibers and prisms are integrated into mechanical structures , for example cells , housings , trusses , among others , to form an optical instrument .
  • Wide-angle optical applications become more attractive from the emerging necessity of the systems being able to accommodate and capture big scenario imaging, with large field of view ( FoV) .
  • Wide-angle systems can be used in di f ferent application fields , li ke , autonomous driving, to measure the Time-Of-Flight ( TOF) , Transmit/Receive ( Tx/Rx ) , etc, patterns emission to deep field 3D cameras , image camera systems , fiber laser emission with high power, etc .
  • TOF Time-Of-Flight
  • Tx/Rx Transmit/Receive
  • the optical elements are usually installed close to heat sources ( electronic components ) , and, therefore , are signi ficantly af fected by this temperature gradient ;
  • the optical aperture is small compared to the lens si ze ;
  • the present invention describes an optomechanical apparatus to increase angular resolution and measurement range of LiDAR systems comprising : an optomechanical hollow tube ; a monocentric ball lens support , installed in one end of the optomechanical hollow tube ; a monocentric ball lens installed in the center of the monocentric ball lens support , crossing said support from one side to the other ; and a spherical hemisphere installed in the same end of the optomechanical hollow tube covering both the monocentric ball lens support and the monocentric ball lens ; wherein the monocentric ball lens comprises at least two types of material of di f ferent refractive index .
  • the monocentric ball lens comprises a smaller diameter than the hollow tube and the spherical hemisphere .
  • the spherical hemisphere comprises a hollow dome shape with a uni form distribution of optical fibers throughout the interior surface of the hollow dome shape , which pierces its structural wall , providing a mechanical support and an optical connection of said optical fibers to the outside of the hollow dome shape .
  • the monocentric ball lens comprises an inside portion, internal dual monocentric spherical hemisphere (Nl ) , with lower refractive index, and an outer portion, external dual monocentric spherical hemisphere (N2 ) , with higher refractive index .
  • the internal dual monocentric spherical hemisphere (Nl ) comprises two identical monocentric spherical hemispheres bonded together .
  • the external dual monocentric spherical hemisphere (N2 ) comprises an external portion and an internal portion, the external portion being located on one side of the monocentric ball lens support inside of the optomechanical hollow tube , and the internal portion being located on the oppos ite side of the monocentric ball lens support inside of the spherical hemisphere .
  • the external portion of the external dual monocentric spherical hemisphere (N2 ) is adapted to capture incoming light beams inside of the optomechanical hollow tube and evenly reflect and distribute components of the light beams through the inner surface of the spherical hemisphere .
  • the optical fibers are adapted to ensure the connection and the correct light beam transmission between the inner surface of spherical hemisphere and an avalanche photodiode arrangement .
  • the external portion and an internal portion of the external dual monocentric spherical hemisphere (N2 ) comprise nonidentical geometric formats bonded together and also bonded with the outer surface of the internal dual monocentric spherical hemisphere (Nl ) .
  • the present application describes an optomechanical apparatus that can be integrated in LiDAR systems , being used to measure the Time-Of-Fl ight ( TOF) , providing an increased angular resolution and measurement range .
  • TOF Time-Of-Fl ight
  • the disclosed optomechanical apparatus herein described represents enormous advantages for a receptor sensor .
  • This solution allows to , as previously anticipated, minimi ze the imaging optical aberrations , minimi ze the background light ef fects , simpli fy the wavelength filtering, isolate the path for the reflected light and allow a high ratio between system aperture and si ze of sensor .
  • a LiDAR sensor emits and receives light beams reflected from a target point .
  • the target reflected light is transmitted through a glass cover to an opto-electro-mechanical system .
  • the herein disclosed Opto-electro-mechanical system comprises a Optomechanical tube , a Monocentric Ball lens , Multi-mode Optical fibers or Waveguides , Avalanche Photodiodes , transimpedance ampli bombs ( TIA) and electronic/mechanical elements .
  • a Monocentric ball lens can be described as a ball shaped lens , which in the proposed solution, comprises at least two di f ferent materials .
  • the selected materials can comprise a selection of adapted glass or polymers , or a combination thereof .
  • the typical structure of these lens can accommodate a large FOV, miniaturi zation and high image quality .
  • the center of all refractive surfaces coincides with each other, and the image surface plane is f ormed/ref lected in a single hemisphere .
  • the inside portion of the lens comprises a lower refractive index when compared with the external portion of said lens .
  • the inside portion of the lens comprises a lower refractive index when compared with the external portion of said lens .
  • the Opto-electro-mechanical system will receive the target reflected light , which will be trans ferred from the outside to the inside of the housing system, by a glass cover .
  • the system acquires the light sources which additionally can pass through a narrow band wavelength filter in order to obtain a speci fic light wavelength beam, which will then propagate inside an optomechanical tube until it reaches the monocentric lens .
  • This filter can be located inside the optical tube , or on the surface of the monocentric lens .
  • the Optomechanical tube it is necessary to guide the captured light towards the system avoiding the loss of irradiance .
  • the filtered light beam When the filtered light beam reaches the spherical monocentric lens , it is refracted on a speci fic spot of the opposite spherical hemisphere .
  • the refractive lens which comprises an array set of multimode optical fibers arranged along the entire inner surface .
  • the optical fibers are fixed and secured through a troughhole arrangement that allow the evenly distribution around all the inner surface of the outer hemisphere plane , providing a mechanical support to the fiber arrays and a light connection between the inside and the outside of the hemispherical plane .
  • the light beam is propagated inside these optical fibers , until it reaches an arrangement of avalanche photodiodes (APD) .
  • APD avalanche photodiodes
  • an APD arrangement will receive the propagated optical light beam, transducing it into an electrical signal .
  • Each optical fiber is terminated with a conventional state-of-the-art connector, for example , one of a FC or LC or SC fiber optical connector .
  • the APD electrical signal is then classi fied as a di f ferential signal , and it is transmitted to the filter and ampli fication modules , which are composed by the TIA ampli bombs . There , the noise will be filtered, and the APD response signal ampli fied .
  • the voltage output of the TIA ampli fier module it is acquired on a TDC ( Time Division Converter ) and analyzed .
  • FIG. 1 - illustrates the overall view of proposed
  • Optomechanical apparatus (100) .
  • Fig. 2 - illustrates the proposed Optomechanical apparatus (100) in a longitudinal sectional view, where the numerical references are related to:
  • Fig. 3 - illustrates a tree-dimensional view of the lenses, where the numerical references are related to:
  • Fig. 4 - illustrates a longitudinal sectional view of the lenses and the hemisphere, where the numerical references are related to:
  • the proposed optomechanical apparatus (100) comprises an optomechanical closed hollow tube (1) with a predetermined length, which in one of its ends comprises a monocentric ball lens support (3) circularly closing the entire end of said tube, and which further comprises a monocentric ball lens (2) in the center of said support (3) , preferably with a smaller diameter with regard to the inner diameter of the tube (1) .
  • the mentioned end of the tube (1) is additionally sealed with a spherical hemisphere (4) with a wider diameter than the diameter of the lens (2) , and inferior, or at least equal, to the inner diameter of the tube (1) .
  • the spherical hemisphere (4) having a hollow dome shape, incorporates a uniform distribution of optical fibers (5) throughout all its interior surface, which pierces the structural wall of the dome providing a mechanical support to the fiber array, allowing an optical connection of the fibers (5) to the outside of the structure the spherical hemisphere (4) .
  • the monocentric ball lens (2) is composed of at least two different materials, evenly distributed over each face of the lens, comprising one of a polymers and/or glass.
  • the monocentric ball lens (2) inside portion i.e., the internal dual monocentric spherical hemisphere (Nl)
  • Nl internal dual monocentric spherical hemisphere
  • N2 external dual monocentric spherical hemisphere
  • the monocentric ball lens (2) comprises several distinctive components.
  • the ball lens (2) comprises and internal dual monocentric spherical hemisphere (Nl) and an external dual monocentric spherical hemisphere (N2) .
  • the internal dual monocentric spherical hemisphere (Nl) is composed by two identical monocentric spherical hemispheres which are bonded together.
  • the external portion of the external dual monocentric spherical hemisphere (N2) of the lens (2) is considered to be the hemisphere which captures the light beams coming from the inside of the hollow tube (1) .
  • the internal portion of the external dual monocentric spherical hemisphere (N2) of the lens (2) is located in the opposite hemisphere of the external portion, transferring the captured beams, diffracting them through the inner surface of the spherical hemisphere (4) where the optical fibers are evenly distributed .
  • the inner portion (Nl) of the lens (2) comprises a lower refractive index when compared with the external portion (Higher refractive index) (N2) of said lens (2) .
  • the optical fiber array that ensures the connection and the correct light beam transmission between the spherical hemisphere (4) and the APD arrangement, in one of the proposed embodiments, incorporates multi-mode optical fibers with step index, each fiber (5) comprising a core of fused silica within a range of 50pm to 100pm and a cladding diameter of fluorine doped silica within a range of 125pm to 140.
  • the numeric aperture of each fiber (5) will be comprising ranges between 0.12 and 0.26 and will terminated in one of a FC or LC or SC fiber optical connector, in order to ensure the connection to the APD arrangement.

Landscapes

  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Optics & Photonics (AREA)
  • Electromagnetism (AREA)
  • Optical Couplings Of Light Guides (AREA)

Abstract

La présente technologie se rapporte au domaine des systèmes lidars pour la conduite autonome et, plus précisément, à la partie réceptrice du capteur. La technologie concerne l'utilisation d'un système optomécanique compact (100) qui conjugue l'utilisation de lentilles (2), de photodétecteurs et de fibres optiques ou de guides d'ondes, pour détecter et améliorer le faisceau de lumière lidar réfléchi. Bien que la technologie décrite ici se rapporte aux systèmes lidars, elle peut également être utilisée pour d'autres applications, telles que les systèmes de caméras d'imagerie et l'émission laser à fibre.
PCT/IB2021/061401 2021-11-30 2021-12-07 Appareil optomécanique pour applications optiques à grand angle WO2023099952A1 (fr)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
PT11761221 2021-11-30
PT117612 2021-11-30

Publications (1)

Publication Number Publication Date
WO2023099952A1 true WO2023099952A1 (fr) 2023-06-08

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PCT/IB2021/061401 WO2023099952A1 (fr) 2021-11-30 2021-12-07 Appareil optomécanique pour applications optiques à grand angle

Country Status (1)

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WO (1) WO2023099952A1 (fr)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2017106791A1 (fr) * 2015-12-18 2017-06-22 The Regents Of The University Of California Imagerie à diaphragme par réflexion interne totale
US20210048656A1 (en) * 2019-08-12 2021-02-18 Gojoya, Inc. Virtual stop optical systems, methods, and structures

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2017106791A1 (fr) * 2015-12-18 2017-06-22 The Regents Of The University Of California Imagerie à diaphragme par réflexion interne totale
US20210048656A1 (en) * 2019-08-12 2021-02-18 Gojoya, Inc. Virtual stop optical systems, methods, and structures

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
KARBASI SALMAN ET AL: "Curved fiber bundles for monocentric lens imaging", PROCEEDINGS OF SPIE, IEEE, US, vol. 9579, 3 September 2015 (2015-09-03), pages 95790G - 95790G, XP060059951, ISBN: 978-1-62841-730-2, DOI: 10.1117/12.2188901 *

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