Arrangement for optical autocorrelation

• US 5,581,383 A
• Filed: 02/28/1995
• Issued: 12/03/1996
• Est. Priority Date: 03/14/1994
• Status: Expired due to Fees

• Current Assignee: Jenoptik Technologie GmbH (Jenoptik AG)
• Original Assignee: Jenoptik Technologie GmbH (Jenoptik AG)
• Inventors: Reichel, Frank, Gaertner, Ernst
• Primary Examiner(s): NOT, DEFINED
• Assistant Examiner(s): Parker, Kenneth
• Application Number:
  US08/395,669
• Time in Patent Office: 644 Days
• Field of Search: 359/93, 359/94, 359/95, 359/45, 359/72, 359/559, 359/99, 359/102, 359/561, 359/63, 250/550, 382/278, 382/211, 382/209, 356/345, 364/822, 364/819, 364/827
• US Class Current: 349/116
• CPC Class Codes: G01P 3/366 by using diffraction of light for measuring speed of fluids G01P5/26
• CPC Class Codes: G01P 5/001 Full-field flow measurement, e.g. determining flow velocity and direction in a whole region at the same time, flow visualisation
• CPC Class Codes: G02B 27/48 Laser speckle optics

Abstract

An arrangement for optical autocorrelation of laser speckle photography (LSP) photographs or particle image velocimetry (PIV) photographs using optical Fourier transforms is disclosed. The object of providing an electro-optical arrangement for optical correlation of LSP film recordings and PIV film recordings which is simple to produce and accurate is met by using an optically addressable liquid crystal SLM (spatial light modulator) for producing the Young'"'"'s fringe patterns which contains a uniaxial double-refracting liquid crystal layer and is read out with linearly polarized light of a laser light source, wherein the polarization direction of the laser light source on the readout side coincides with the extraordinary semi-axis of the refractive index ellipsoid of the liquid crystal layer.

Claims

1. An arrangement for optical autocorrelation of film recordings of laser speckle photography or particle image velocimetry with a laser light source comprising:

a laser light source having light which penetrates a laser speckle photographic or particle image velocimetry recording so that Young'"'"'s fringe patterns occur in the image-side focal plane of a Fourier transform objective;

an optically addressable liquid crystal SLM on which the fringe pattern is imaged;

a second laser light source which reads out the liquid crystal SLM and, by a second Fourier transform objective, produces a diffraction pattern corresponding to the Fourier-transformed Young'"'"'s fringes;

a camera for recording the diffraction pattern;

said liquid crystal SLM containing a uniaxial double-refracting liquid crystal layer which is read out with linearly polarized light of the second laser light source on the readout side; and

wherein the polarization direction of said second laser light source coincides with the extraordinary semi-axis of the refractive index ellipsoid of said liquid crystal layer.

2. The arrangement according to claim 1, wherein the liquid crystal layer of the liquid crystal SLM contains nematic liquid crystals with positive dielectric anisotropy.

3. The arrangement according to claim 1, wherein the liquid crystals are non-twisted.

4. The arrangement according to claim 1, wherein the sensitivity distribution of the liquid crystal SLM is radially symmetric and its curve is inversely proportional to the intensity distribution of an Airy disk.

5. The arrangement according to claim 1, wherein a point receiver is arranged in the zero order of a diffraction pattern, whose output signal regulates the frequency of the SLM operating voltage by means of an operating unit in such a way that the intensity of the undiffracted light of the zero order reaches a minimum.

6. The arrangement according to claim 1, wherein the polarization directions of the write-in light and readout light of the liquid crystal SLM extend at right angles to one another and a polarization filter is arranged in front of the camera in the autocorrelation plane for blocking the residual write-in light.

7. The arrangement according to claim 1, wherein the wavelengths of the laser light sources are different so that the residual write-in light can be blocked by an optical filter in front of the camera in the autocorrelation plane.