# US 7,609,384 B2 · Device for generating a carrier in an interferogram > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 7,609,384 B2 - Document ID: US7609384B2 - Status: Granted - Kind: B2 - Application number: 10/547,966 - Filed: 2004-03-10 - Published: 2006-07-13 - Granted: 2009-10-27 - Earliest claimed: 2003-03-11 - Assignees: Centre National de la Recherche Scientifique (CNRS); Universite Paris-Sud - Inventors: Gerald Roosen; Gilles Pauliat - Web page: https://patentgrep.com/patent/US7609384B2 ## CPC - G01B 9/021: using holographic techniques - G03H 2001/0204: {Object characteristics} - G03H 2001/0445: {Off-axis recording arrangement (G03H2001/0456 takes precedence)} - G03H 2001/0471: {Object light being transmitted through the object, e.g. illumination through living cells} - G01B: MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS - G03H: HOLOGRAPHIC PROCESSES OR APPARATUS (holograms, e.g. point holograms, used as ordinary optical elements G02B5/32; producing stereoscopic or other three-dimensional effects G02B30/00; diffraction-grating systems G02B27/44; systems using moiré fringes G02B27/60; optical logic elements G02F3/00; stereo-photography G03B35/00; photosensitive materials or processes for photographic purposes G03C; {stereo-photographic or similar processes G03C9/00}; apparatus for processing exposed photographic materials G03D; analogue computers performing mathematical operations with the aid of optical elements G06E3/00; authentication by radiation, of concealed information carried by holograms or diffraction gratings G06K19/16; holographic storage G11B7/0065, G11C13/04; {stereoscopic or other three dimensional effects in television systems H04N13/00}) ## Abstract A process for generating a carrier in an interferogram in interferometry device either of the “real-time holographic interferometry” type or of the “double-exposure holographic interferometry” type, including recording a first wave front on a hologram, the first wave front coming from an object; generating a second wave front, in which two wave fronts are superimposed orthogonally polarizing said first and second wave fronts, either naturally or by a modification stage; and passing the orthogonally polarized two wave fronts through a birefringent crystal, a polarizer and a detector to make the two wave fronts interfere. ## Claims ### Claim 1 A device for generating a carrier in an interferogram of the real-time holographic interferometry type or of the double-exposure holographic interferometry type, comprising: a recorder that records a first wave front hologram, by recording interference of an object beam and a reference beam, the object beam diffused by an object and transmitted to a material of holographic environment, and the reference beam transmitted to the material of holographic environment, wherein a first wave front is comprised of the object beam and the reference beam; a plurality of lenses through which the first wave front and a second wave front pass, the second wave front comprised of at least an object beam diffused by the object and transmitted to the material of holographic environment at a time later than the object beam of the first wave front; a birefringent crystal through which the two wave fronts pass that orthogonally polarizes the two wave fronts; at least one common polarizer through which the two wave fronts pass; and at least one detector on which an interference between the two wave fronts is formed. ### Claim 2 (depends on 1) The device according to claim 1, wherein the birefringent crystal is in the form of a birefringent biprism. ### Claim 3 (depends on 1) The device according to claim 1, wherein the birefringent crystal is in the form of a birefringent lamina. ### Claim 4 (depends on 3) The device according to claim 3, wherein the birefringent lamina is situated at infinity, from an optical viewpoint, relative to the object observed. ### Claim 5 (depends on 4) The device according to claim 4, wherein the biprism is placed in proximity of an image of the object. ### Claim 6 A process for generating a carrier in an interferogram in either of a real-time holographic interferometry device or a double-exposure holographic interferometry device, comprising: receiving an object beam and a reference beam; recording a first wave front hologram by recording interference of the object beam and the reference beam, the object beam diffused by an object and transmitted to a material of holographic environment, and the reference beam transmitted to the material of holographic environment, wherein a first wave front is comprised of the object beam and the reference beam; restoring the first wave front by a readback of the first wave front hologram by the reference beam; generating a second wave front comprised of at least an object beam diffused by the object and transmitted to the material of holographic environment at a time later than the object beam of the first wave front; passing the first and second wave fronts through a birefringent crystal to orthogonally polarize the first and second wave fronts; passing the first and second wave fronts through a common polarizer; and forming an interference between the first and second wave fronts on a detector. ### Claim 7 (depends on 6) The process according to claim 6, wherein the first wave front is restored in the case of real-time interferometry by readback of the hologram by a reference beam, which first wave front is superimposed on the second wave front coming from the object observed. ### Claim 8 (depends on 6) The process according to claim 6, wherein the second wave front is obtained in the case of double-exposure interferometry by recording a new wave front coming from the object. ### Claim 9 (depends on 6) The process according to claim 6, wherein modifying comprises modification of the wave coming from the object or of the wave of the reference beam in the case of interferometry in real time, or of one of the two reference beams in the case of double-exposure interferometry with an electro-optical switch, which modification of the polarization of one of the waves takes place after recording the hologram. ### Claim 10 (depends on 6) The process according to claim 6, wherein the material of holographic environment used in the interferometry device is an anisotropic material.