EP2092282A1 - Polarimetrisches abbildungssystem mit einer matrix programmierbarer verzögerungsplatten auf der basis eines materials mit einem isotropen elektrooptischen sensor - Google Patents

Polarimetrisches abbildungssystem mit einer matrix programmierbarer verzögerungsplatten auf der basis eines materials mit einem isotropen elektrooptischen sensor

Info

Publication number
EP2092282A1
EP2092282A1 EP07821380A EP07821380A EP2092282A1 EP 2092282 A1 EP2092282 A1 EP 2092282A1 EP 07821380 A EP07821380 A EP 07821380A EP 07821380 A EP07821380 A EP 07821380A EP 2092282 A1 EP2092282 A1 EP 2092282A1
Authority
EP
European Patent Office
Prior art keywords
imaging system
electrodes
programmable
polarimetric imaging
matrix
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.)
Withdrawn
Application number
EP07821380A
Other languages
English (en)
French (fr)
Inventor
Jérôme BOURDERIONNET
Daniel Dolfi
Sébastien Breugnot
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.)
Thales SA
Original Assignee
Thales SA
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 Thales SA filed Critical Thales SA
Publication of EP2092282A1 publication Critical patent/EP2092282A1/de
Withdrawn legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J4/00Measuring polarisation of light
    • G01J4/04Polarimeters using electric detection means
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/03Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect
    • G02F1/055Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect the active material being a ceramic
    • G02F1/0551Constructional details
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F2203/00Function characteristic
    • G02F2203/12Function characteristic spatial light modulator
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F2203/00Function characteristic
    • G02F2203/50Phase-only modulation

Definitions

  • a standard device programmable waveguide and fixed analyzer then sequentially performs the n combinations of analyzes required.
  • the programmable waveguide function is performed by mechanical rotation of a wave plate or by means of a polarization controller based on liquid crystals (P.CIémenceau, S. Breugnot, L. Collot, "Apparatus for Polarimetric Imaging, Patent 2,769,980 (1997)).
  • P.CIémenceau, S. Breugnot, L. Collot "Apparatus for Polarimetric Imaging, Patent 2,769,980 (1997).
  • response time 10 to 100ms for the nematic liquid crystals
  • the response time of the component is also significantly important in the case where the system must be mounted on a mobile platform (drone type, with travel speeds of the order of 50km / h).
  • the focal length f of the first lens corresponds to the following equation: where O h m is the angular acceptance of the programmable waveplate and at the surface defined by the intersection of the half-angle cone at the vertex ⁇
  • the polarimetric imaging system comprises at least:
  • these materials have a broad transmission band (transparent from 500 nm to 7000 nm (G. Haertiing, CE Land, "Hot-pressed (Pb, La) (Zr, Ti) O 3 ferroelectric ceramics for electrooptic applications", J.
  • FIG. 10 illustrates a detailed view of the programmable waveguide array in the third variant of a polarimetric imaging system according to the invention.
  • the first variant of a polarimetric imaging system comprises an objective 32, a programmable waveguide 33, a detection means 35 and a polarizer 34 located between said programmable waveguide and said detection means 35.
  • the polarizer projects the polarization along its (fixed) axis.
  • the combination of the waveguide and polarizer allows projection of the polarization along any axis.
  • the system measures the state of polarization of the light backscattered by an object 31, illuminated by a light source.
  • the programmable wave plate 33 comprises in particular a block of a material with an isotropic electro-optical tensor, and comprising a set of at least three electrodes. An exemplary embodiment of such a programmable waveguide is illustrated in FIG. 4.
  • the programmable waveguide 33 is in the form of a block of parallelepipedic electro-optical material 45 on whose edges there are four electrodes E, referenced 44, 41, 42 and 43 in FIG.
  • the electrodes 61, 62, 63 and 64 are formed by through holes, substantially cylindrical and metallized, pierced in the thickness of the material with an isotropic electro-optical tensor.
  • the electrodes 61, 62, 63 and 64 are made in the volume of the material to optimize on the one hand the overlap between the optical wave and the applied electric field and, on the other hand, the homogeneity of the applied electric field. This has the effect of optimizing the effectiveness of the component.
  • the pixels of the matrix are collectively controlled, a possible variation of pixel pixel characteristics that can be corrected to the calibration processing.
  • the generated electric fields are opposite for two adjacent pixels. This does not influence the operation of the device since the electro-optical effect used is quadratic, therefore independent of the polarity of the electric field. It is also possible to envisage an individual addressing of each pixel.

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Ceramic Engineering (AREA)
  • Nonlinear Science (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Optics & Photonics (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)
  • Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
EP07821380A 2006-10-20 2007-10-16 Polarimetrisches abbildungssystem mit einer matrix programmierbarer verzögerungsplatten auf der basis eines materials mit einem isotropen elektrooptischen sensor Withdrawn EP2092282A1 (de)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
FR0609230A FR2907547B1 (fr) 2006-10-20 2006-10-20 Systeme d'imagerie polarimetrique a matrice de lames d'onde programmables a base de materiau avec un tenseur electro-optique isotrope.
PCT/EP2007/061014 WO2008046820A1 (fr) 2006-10-20 2007-10-16 Systeme d'imagerie polarimetrique a matrice de lames d'onde programmables a base de materiau avec un tenseur electro-optique isotrope

Publications (1)

Publication Number Publication Date
EP2092282A1 true EP2092282A1 (de) 2009-08-26

Family

ID=38024294

Family Applications (1)

Application Number Title Priority Date Filing Date
EP07821380A Withdrawn EP2092282A1 (de) 2006-10-20 2007-10-16 Polarimetrisches abbildungssystem mit einer matrix programmierbarer verzögerungsplatten auf der basis eines materials mit einem isotropen elektrooptischen sensor

Country Status (4)

Country Link
US (1) US20100039646A1 (de)
EP (1) EP2092282A1 (de)
FR (1) FR2907547B1 (de)
WO (1) WO2008046820A1 (de)

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2932929B1 (fr) 2008-06-20 2010-06-04 Thales Sa Dispositif laser comportant des moyens de mise en phase d'un grand nombre de sources coherentes
FR2945348B1 (fr) 2009-05-07 2011-05-13 Thales Sa Procede d'identification d'une scene a partir d'images polarisees multi longueurs d'onde
US8407950B2 (en) 2011-01-21 2013-04-02 First Solar, Inc. Photovoltaic module support system
JP6482308B2 (ja) * 2015-02-09 2019-03-13 キヤノン株式会社 光学装置および撮像装置
CN110470608A (zh) * 2019-08-15 2019-11-19 杭州电子科技大学 一种利用偏振成像测定物体光滑度的方法及装置
CN113624690B (zh) * 2021-07-19 2023-10-13 清华大学深圳国际研究生院 一种能够实现任意偏振态调制的起偏器及其优化方法

Family Cites Families (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6122404A (en) * 1998-05-28 2000-09-19 Trw Inc. Visible stokes polarimetric imager
JP3429236B2 (ja) * 1999-11-16 2003-07-22 シャープ株式会社 液晶変調素子の光学変調特性の評価方法、それを用いて作製された液晶表示装置、液晶変調素子の光学変調特性の評価装置、および液晶変調素子の光学変調特性を評価するプログラムを格納したコンピュータ読み取り可能な記録媒体
FR2819061B1 (fr) * 2000-12-28 2003-04-11 Thomson Csf Dispositif de controle de polarisation dans une liaison optique
JP2003161810A (ja) * 2001-11-28 2003-06-06 Citizen Electronics Co Ltd 密着イメージセンサー用紫外線硬化型液晶マイクロレンズ
US6890874B1 (en) * 2002-05-06 2005-05-10 Corning Incorporated Electro-optic ceramic material and device
US6746618B2 (en) * 2002-05-21 2004-06-08 Corning Incorporated Electro-optic ceramic material and device
US7116419B1 (en) * 2002-11-15 2006-10-03 Purdue Research Foundation Wavelength-parallel polarization measurement systems and methods
US7173698B2 (en) * 2004-04-13 2007-02-06 The United States Of America As Represented By The Secretary Of The Army Simultaneous 4-stokes parameter determination using a single digital image
FR2880204B1 (fr) * 2004-12-23 2007-02-09 Thales Sa Source laser a recombinaison coherente de faisceaux

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
See references of WO2008046820A1 *

Also Published As

Publication number Publication date
FR2907547A1 (fr) 2008-04-25
FR2907547B1 (fr) 2009-04-17
US20100039646A1 (en) 2010-02-18
WO2008046820A1 (fr) 2008-04-24

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