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US20020051117A1 - Scanner - Google Patents

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Publication number
US20020051117A1
US20020051117A1 US09/886,172 US88617201A US2002051117A1 US 20020051117 A1 US20020051117 A1 US 20020051117A1 US 88617201 A US88617201 A US 88617201A US 2002051117 A1 US2002051117 A1 US 2002051117A1
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US
United States
Prior art keywords
deflecting element
electromagnetic radiation
scanning
scanner
scanner according
Prior art date
Legal status (The legal status 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 status listed.)
Granted
Application number
US09/886,172
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US6419360B1 (en
Inventor
Christoph Hauger
Werner Poltinger
Wilhelm Ulrich
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Carl Zeiss AG
Original Assignee
Individual
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 Individual filed Critical Individual
Assigned to CARL-ZEISS-STIFTUNG TRADING AS CARL ZEISS reassignment CARL-ZEISS-STIFTUNG TRADING AS CARL ZEISS ASSIGNMENT OF ASSIGNORS INTEREST (SEE DOCUMENT FOR DETAILS). Assignors: HAUGER, CHRISTOPH, ULRICH, WILHELM, POLTINGER, WERNER
Publication of US20020051117A1 publication Critical patent/US20020051117A1/en
Application granted granted Critical
Publication of US6419360B1 publication Critical patent/US6419360B1/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/24Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures
    • G01B11/25Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures by projecting a pattern, e.g. one or more lines, moiré fringes on the object
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B26/00Optical devices or arrangements for the control of light using movable or deformable optical elements
    • G02B26/08Optical devices or arrangements for the control of light using movable or deformable optical elements for controlling the direction of light
    • G02B26/10Scanning systems
    • G02B26/108Scanning systems having one or more prisms as scanning elements

Definitions

  • the invention relates to a scanner for optical coherence tomography for linear scanning of an object with electromagnetic radiation.
  • a scanner of this kind is known from EP 0 581 871 B1, particularly from FIGS. 3B, 3C, 3D and 6, and from U.S. Pat. No. 5,537,162, particularly from FIG. 1.
  • the invention has as its object to further improve a scanner of the category concerned.
  • This object is attained by a deflecting element which is rotatable around a rotation axis and which deflects radiation coming from a radiation source toward the object of study and effects, by its rotation, a linear scanning of the object of study.
  • a beam-forming optics is arranged between this deflecting element and the object of study, and concentrates the radiation coming from the deflecting element toward the object.
  • the rotation axis of the rotatable deflecting element is parallel to the direction of incidence of the radiation.
  • the scanner according to the invention is mechanically constructed in a simple manner and can be especially compact. Furthermore, expanded possibilities of use result from the invention.
  • the scanner according to the invention can, for example, be compact enough to be constructed as a hand-held scanner, in particular.
  • the beam-forming optics includes a telecentric scanning objective, so that the exact focusing state of the scanning beam has no effect on the position of the scan line in the object.
  • a collimator for the incident radiation is arranged on the side of the rotatable deflecting element remote from the object.
  • the scanning radiation can thereby be optimized in relation to the beam forming optics.
  • a beamsplitter is arranged on the object side of the telecentric scanning objective. In this manner, the scanned region of the object of study can be made visible to an operator. This is useful for the control or guiding of a scanner constructed as a hand-held device.
  • the beamsplitter is dichroic, scanning radiation lying outside the visible wavelength region, e.g. in the infrared, can be efficiently concentrated onto the object, and at the same time the scan line can be optimally observed.
  • the observation conditions for an operator can be further optimized with a magnifying optics arranged on the side of the beamsplitter remote from the object.
  • Particularly reliable monitoring of the scan line can be attained with an end window on the object side, marked with the scan line or scanning line.
  • Electromagnetic radiation is deflected in the scanner 1 , along a beam path 3 onto an object 5 to be studied; an optical fiber 9 end surface 7 , acting as a radiation source, is imaged on the object 5 .
  • This image of the radiation source is moved over the object 5 in a scan line which extends transversely of the plane of the FIGURE and thus transversely of the direction of propagation of the radiation.
  • a deflecting element 13 rotating around a rotation axis 11 deflects the beam path 3 in different directions depending on its rotational position, and thereby effects, in cooperation with the subsequent optical elements of the scanner 1 which are fixed to the scanner, the linear scanning of the object 5 .
  • the rotation axis 11 is parallel to and collinear with the section of the beam path 3 situated between the end surface 7 and the deflecting element 13 , that is, parallel to the direction of incidence of the radiation.
  • the deflecting element 13 which deflects the beam path 3 through 90° has a planar deflecting surface oriented at 45° to the direction of incidence of the radiation, and is rotated around the rotation axis 11 by a rotary motor 15 .
  • the radiation coming from the optical fiber 9 is collimated by a collimator lens element 17 before it is deflected by the rotatable deflecting element 13 .
  • the incident pencil of rays is deflected a further time by means of a deflecting element 18 , fixed to the scanner and having a planar reflecting surface extending orthogonal to the plane of the FIGURE.
  • the pencil of rays is thereafter concentrated toward the object 5 by a beam-forming optics 23 which is fixed to the scanner and consists of a telecentric scanning objective including the lenses 19 and 21 .
  • a beamsplitter 25 arranged between the beam forming optics 23 and the object 5 reflects the scanning radiation onto the object 5 through an end window 27 which has a marking of the scan line.
  • the beamsplitter 25 is reflective for the scanning radiation coming from the optical fiber 9 and is transparent in the visible wavelength region.
  • the scanned region of the object 5 of study can thus be observed and monitored through a magnifying glass 29 .
  • a source 31 for visible electromagnetic radiation, arranged within the scanner 1 then provides particularly favorable observation conditions.

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Computer Vision & Pattern Recognition (AREA)
  • Optics & Photonics (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)
  • Lenses (AREA)
  • Mechanical Optical Scanning Systems (AREA)

Abstract

A scanner for optical coherence tomography for linear scanning of an object with electromagnetic radiation, in which the scanning direction runs transversely of the direction of propagation of the electromagnetic radiation, includes a deflecting element rotatable around a rotation axis that deflects the electromagnetic radiation, incident along a direction of incidence, toward the object and, by its rotation, effects the linear scanning of the object. A beam forming optics is arranged on the object side of the rotatable deflecting element and concentrates electromagnetic radiation coming from the deflecting element. The rotation axis of the rotary deflecting element is parallel to the direction of incidence of the electromagnetic radiation.

Description

    STATEMENT REGARDING FEDERALLY SPONSORED RESEARCH OR DEVELOPMENT
  • Not applicable. [0001]
  • CROSS-REFERENCES TO RELATED APPLICATIONS
  • Not applicable. [0002]
  • BACKGROUND OF THE INVENTION
  • The invention relates to a scanner for optical coherence tomography for linear scanning of an object with electromagnetic radiation. [0003]
  • A scanner of this kind is known from EP 0 581 871 B1, particularly from FIGS. 3B, 3C, 3D and 6, and from U.S. Pat. No. 5,537,162, particularly from FIG. 1. [0004]
  • SUMMARY OF THE INVENTION
  • The invention has as its object to further improve a scanner of the category concerned. [0005]
  • This object is attained by a deflecting element which is rotatable around a rotation axis and which deflects radiation coming from a radiation source toward the object of study and effects, by its rotation, a linear scanning of the object of study. A beam-forming optics is arranged between this deflecting element and the object of study, and concentrates the radiation coming from the deflecting element toward the object. The rotation axis of the rotatable deflecting element is parallel to the direction of incidence of the radiation. The scanner according to the invention is mechanically constructed in a simple manner and can be especially compact. Furthermore, expanded possibilities of use result from the invention. The scanner according to the invention can, for example, be compact enough to be constructed as a hand-held scanner, in particular. [0006]
  • In a particular embodiment, the beam-forming optics includes a telecentric scanning objective, so that the exact focusing state of the scanning beam has no effect on the position of the scan line in the object. [0007]
  • In a further embodiment, a collimator for the incident radiation is arranged on the side of the rotatable deflecting element remote from the object. The scanning radiation can thereby be optimized in relation to the beam forming optics. A beamsplitter is arranged on the object side of the telecentric scanning objective. In this manner, the scanned region of the object of study can be made visible to an operator. This is useful for the control or guiding of a scanner constructed as a hand-held device. [0008]
  • When the beamsplitter is dichroic, scanning radiation lying outside the visible wavelength region, e.g. in the infrared, can be efficiently concentrated onto the object, and at the same time the scan line can be optimally observed. [0009]
  • The observation conditions for an operator can be further optimized with a magnifying optics arranged on the side of the beamsplitter remote from the object. Particularly reliable monitoring of the scan line can be attained with an end window on the object side, marked with the scan line or scanning line.[0010]
  • BRIEF DESCRIPTION OF THE DRAWINGS
  • The invention is described in an embodiment example, using the accompanying FIGURE, in which the scanner [0011] 1 according to the invention, shown in a schematic sectional representation, is illustrated by way of example.
  • DETAILED DESCRIPTION OF INVENTION
  • Electromagnetic radiation is deflected in the scanner [0012] 1, along a beam path 3 onto an object 5 to be studied; an optical fiber 9 end surface 7, acting as a radiation source, is imaged on the object 5. This image of the radiation source is moved over the object 5 in a scan line which extends transversely of the plane of the FIGURE and thus transversely of the direction of propagation of the radiation.
  • For this purpose, a deflecting [0013] element 13 rotating around a rotation axis 11 deflects the beam path 3 in different directions depending on its rotational position, and thereby effects, in cooperation with the subsequent optical elements of the scanner 1 which are fixed to the scanner, the linear scanning of the object 5.
  • The [0014] rotation axis 11 is parallel to and collinear with the section of the beam path 3 situated between the end surface 7 and the deflecting element 13, that is, parallel to the direction of incidence of the radiation. The deflecting element 13 which deflects the beam path 3 through 90° has a planar deflecting surface oriented at 45° to the direction of incidence of the radiation, and is rotated around the rotation axis 11 by a rotary motor 15.
  • The radiation coming from the [0015] optical fiber 9 is collimated by a collimator lens element 17 before it is deflected by the rotatable deflecting element 13. After the rotatable deflecting element 13, the incident pencil of rays is deflected a further time by means of a deflecting element 18, fixed to the scanner and having a planar reflecting surface extending orthogonal to the plane of the FIGURE. The pencil of rays is thereafter concentrated toward the object 5 by a beam-forming optics 23 which is fixed to the scanner and consists of a telecentric scanning objective including the lenses 19 and 21. A beamsplitter 25 arranged between the beam forming optics 23 and the object 5 reflects the scanning radiation onto the object 5 through an end window 27 which has a marking of the scan line.
  • The [0016] beamsplitter 25 is reflective for the scanning radiation coming from the optical fiber 9 and is transparent in the visible wavelength region. The scanned region of the object 5 of study can thus be observed and monitored through a magnifying glass 29. A source 31 for visible electromagnetic radiation, arranged within the scanner 1, then provides particularly favorable observation conditions.

Claims (7)

What is claimed is:
1. A scanner for optical coherence tomography for linear scanning of an object with electromagnetic radiation in a scanning direction running transversely of the direction of propagation of said electromagnetic radiation, comprising:
a deflecting element that is rotatable around a rotation axis and deflects said electromagnetic radiation, incident along a direction of incidence, toward said object and, by its rotation, effects linear scanning of said object, and beam forming optics arranged on the object side of said rotatable deflecting element that concentrates toward said object said electromagnetic radiation coming from said deflecting element,
wherein said rotation axis of said rotatable deflecting element is parallel to said direction of incidence of said electromagnetic radiation.
2. The scanner according to claim 1, wherein said beam forming optics comprises a telecentric scanning objective.
3. The scanner according to claim 1, further comprising a collimator for incident radiation arranged on the side of said rotatable deflecting element remote from said object.
4. The scanner according to claim 2, further comprising a beamsplitter arranged on the object side of said telecentric scanning objective.
5. The scanner according to claim 4, wherein said beamsplitter comprises a dichroic beamsplitter.
6. The scanner according to claim 4, further comprising a magnifying optics arranged on the side of said beamsplitter remote from said object.
7. The scanner according to claim 3, further comprising an end window on said object side of said telecentric scanning objective, said end window having a marking of a scanning line.
US09/886,172 2000-07-01 2001-06-20 Scanner Expired - Lifetime US6419360B1 (en)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
DE10032067.8 2000-01-07
DE10032067 2000-07-01
DE10032067A DE10032067A1 (en) 2000-07-01 2000-07-01 Hand-held scanner for one-dimensional optical coherence tomography, includes deflection prism whose rotation axis is parallel to electromagnetic radiation incidence axis

Publications (2)

Publication Number Publication Date
US20020051117A1 true US20020051117A1 (en) 2002-05-02
US6419360B1 US6419360B1 (en) 2002-07-16

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US09/886,172 Expired - Lifetime US6419360B1 (en) 2000-07-01 2001-06-20 Scanner

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DE (1) DE10032067A1 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7017812B1 (en) 2003-11-26 2006-03-28 The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration Variable distance angular symbology reader

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US7190464B2 (en) * 2004-05-14 2007-03-13 Medeikon Corporation Low coherence interferometry for detecting and characterizing plaques
US20050254059A1 (en) * 2004-05-14 2005-11-17 Alphonse Gerard A Low coherence interferometric system for optical metrology
US7242480B2 (en) * 2004-05-14 2007-07-10 Medeikon Corporation Low coherence interferometry for detecting and characterizing plaques
US7474408B2 (en) * 2004-05-14 2009-01-06 Medeikon Corporation Low coherence interferometry utilizing phase
US7327463B2 (en) 2004-05-14 2008-02-05 Medrikon Corporation Low coherence interferometry utilizing magnitude
US7184148B2 (en) 2004-05-14 2007-02-27 Medeikon Corporation Low coherence interferometry utilizing phase
US7488930B2 (en) * 2006-06-02 2009-02-10 Medeikon Corporation Multi-channel low coherence interferometer
EP3597100B1 (en) 2011-12-05 2024-10-23 Leica Microsystems NC, Inc. Optical imaging systems having input beam shape control and path length control
US8777412B2 (en) 2012-04-05 2014-07-15 Bioptigen, Inc. Surgical microscopes using optical coherence tomography and related methods
JP6373366B2 (en) 2013-06-04 2018-08-15 バイオプティジェン, インコーポレイテッドBioptigen, Inc. Method of operating scanning beam type system and optical scanning beam type system
WO2015017375A2 (en) 2013-07-29 2015-02-05 Bioptigen, Inc. Procedural optical coherence tomography (oct) for surgery and related systems and methods
CN105612453B (en) 2013-08-28 2018-03-27 拜尔普泰戈恩公司 The HUD of surgery microscope is integrated for optical coherence tomography
US10152998B2 (en) * 2014-04-07 2018-12-11 Seagate Technology Llc Features maps of articles with polarized light
CN110461213A (en) 2016-12-21 2019-11-15 奥克塞拉有限公司 Small mobile low-cost optical coherence tomography system based on home ophthalmology application
US10827919B2 (en) 2017-05-02 2020-11-10 Alcon Inc. Reconfigurable optical coherence tomography (OCT) system
CN112638233B (en) 2018-06-20 2024-06-14 奥克塞拉有限公司 Miniature mobile low cost optical coherence tomography system for home-based ophthalmic applications
JP2023508946A (en) 2019-12-26 2023-03-06 アキュセラ インコーポレイテッド Optical Coherence Tomography Patient Alignment System for Home-Based Ophthalmic Applications
US10959613B1 (en) 2020-08-04 2021-03-30 Acucela Inc. Scan pattern and signal processing for optical coherence tomography
AU2021324968A1 (en) 2020-08-14 2023-03-02 Acucela Inc. System and method for optical coherence tomography a-scan decurving
US11393094B2 (en) 2020-09-11 2022-07-19 Acucela Inc. Artificial intelligence for evaluation of optical coherence tomography images
US11911105B2 (en) 2020-09-30 2024-02-27 Acucela Inc. Myopia prediction, diagnosis, planning, and monitoring device
WO2022204622A1 (en) 2021-03-24 2022-09-29 Acucela Inc. Axial length measurement monitor

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JP3479069B2 (en) 1991-04-29 2003-12-15 マサチューセッツ・インステチュート・オブ・テクノロジー Method and apparatus for optical imaging and measurement
US5537162A (en) 1993-12-17 1996-07-16 Carl Zeiss, Inc. Method and apparatus for optical coherence tomographic fundus imaging without vignetting
ATA107495A (en) * 1995-06-23 1996-06-15 Fercher Adolf Friedrich Dr COHERENCE BIOMETRY AND TOMOGRAPHY WITH DYNAMIC COHERENT FOCUS
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US7017812B1 (en) 2003-11-26 2006-03-28 The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration Variable distance angular symbology reader

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US6419360B1 (en) 2002-07-16
DE10032067A1 (en) 2002-01-10

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