Patents by Inventor Jean-Paul Pocholle
Jean-Paul Pocholle has filed for patents to protect the following inventions. This listing includes patent applications that are pending as well as patents that have already been granted by the United States Patent and Trademark Office (USPTO).
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Patent number: 10014647Abstract: The invention relates a power fiber laser system including at least one single-mode fiber laser, emitting at a signal wavelength, the fiber including at least one outer cladding and a core, in which the core of the fiber has a radially graded index. The fiber includes, at least over a part of its length, a geometrical section having a graded fiber-core radius that decreases between an input end of the section and an output end of the section, the core radius and the index variation between the cladding and the fiber at the input end being such that the normalized frequency at the signal wavelength is less than the normalized cutoff frequency at which the fiber becomes unimodal.Type: GrantFiled: March 27, 2009Date of Patent: July 3, 2018Assignee: THALESInventors: Jean-Paul Pocholle, François-Xavier Doittau
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Patent number: 8587788Abstract: A laser gyro for measuring the angular velocity or the angular position relative to a defined rotation axis includes: an optical ring cavity; a solid-state amplifying medium; and a non-reciprocal magneto-optic device; which are arranged so that four linearly polarized propagation modes can propagate within the cavity, the magneto-optic device introducing a frequency bias between the modes propagating in a first direction and the modes propagating in the opposite direction. In the device, the cavity also includes a stabilizer device for stabilizing the intensity of the four propagation modes at substantially equivalent levels, said device comprising at least one optical element made of a non-linear crystal of the frequency-doubling type.Type: GrantFiled: May 6, 2011Date of Patent: November 19, 2013Assignee: ThalesInventors: Sylvain Schwartz, Gilles Feugnet, Jean-Paul Pocholle
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Patent number: 8379216Abstract: The general field of the invention is that of gyrolasers comprising at least one ring-shaped optical cavity comprising at least three mirrors, a solid state amplifying medium pumped by a laser diode whose optical emission power is determined by a current supply source, the cavity and the amplifying medium being such that two so-called contra-rotating optical modes propagate in opposite directions to each other within the said optical cavity, the gyrolaser being a class B gyrolaser, the gyrolaser also comprising means of measuring the difference in optical frequency existing between the two optical modes. The gyrolaser comprises means of measuring the total optical power circulating in the optical cavity and first means of control of the current delivered by the supply source in such a way as to maintain the total optical power substantially constant in a narrow spectral band centred on the relaxation frequency of the laser.Type: GrantFiled: November 12, 2009Date of Patent: February 19, 2013Assignee: ThalesInventors: Sylvain Schwartz, Gilles Feugnet, Francois Gutty, Etienne Bonnaudet, Mehdi Alouini, Jean-Paul Pocholle
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Patent number: 8301407Abstract: Solid-state gyrolaser having a device for stabilizing the intensities making it possible to maintain equilibrium of the two counter-propagating modes having at least a means for calculating a rotation measurement (?, I?) of the gyrolaser on the basis of the counter-propagating modes having a frequency difference (??mes) between them, by assuming that the frequency difference (??mes) between the two counter-propagating modes is induced only by the rotation of the cavity.Type: GrantFiled: June 22, 2010Date of Patent: October 30, 2012Assignee: ThalesInventors: François Gutty, Schwartz Sylvain, Jean-Paul Pocholle, Gilles Feugnet
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Patent number: 8290316Abstract: The general field of the invention is that of fiber-optic sensors comprising at least one measurement optical fiber having an optically pumped doped amplifying medium, the optical characteristics of which are sensitive to a physical quantity, the fiber having at least one Bragg grating. The fiber is designed so as to generate, in the amplifying medium, two optical waves having different optical frequencies that propagate in the same direction after reflection on the Bragg grating and are emitted by the amplifying medium, the two optical frequencies depending on the physical quantity. The two waves may be generated using either a birefringent polarization-maintaining fiber or a DBR (Distributed Bragg Reflector) laser cavity. Notably, this sensor may be used as a hydrophone.Type: GrantFiled: March 16, 2009Date of Patent: October 16, 2012Assignee: ThalesInventors: Stéphanie Molin, Daniel Dolfi, Jean-Pierre Huignard, Martine Doisy, Loïc Morvan, Jean-Paul Pocholle
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Publication number: 20110273720Abstract: A laser gyro for measuring the angular velocity or the angular position relative to a defined rotation axis includes: an optical ring cavity; a solid-state amplifying medium; and a non-reciprocal magneto-optic device; which are arranged so that four linearly polarized propagation modes can propagate within the cavity, the magneto-optic device introducing a frequency bias between the modes propagating in a first direction and the modes propagating in the opposite direction. In the device, the cavity also includes a stabilizer device for stabilizing the intensity of the four propagation modes at substantially equivalent levels, said device comprising at least one optical element made of a non-linear crystal of the frequency-doubling type.Type: ApplicationFiled: May 6, 2011Publication date: November 10, 2011Applicant: THALESInventors: Sylvain SCHWARTZ, Gilles FEUGNET, Jean-Paul POCHOLLE
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Patent number: 8035818Abstract: The field of the invention is that of solid-state laser gyros used for the measurements of rotation speed or relative angular positions. This type of equipment is notably used for aeronautical applications. The object of the invention is to complete the optical devices necessary to control the instability of lasers by specific optical devices enabling elimination of the dead zone and of population inversion gratings exiting in the amplifying medium. An “all optical” solid-state laser is hence obtained without moveable parts, stable and without a dead zone. To this end, the laser gyro according to the invention comprises notably and optical assembly enabling a nonreciprocal optical phase-shift to be introduced between the counterpropagating modes; and control means allowing the phase-shift amplitude to be varied periodically around a mean value that is very approximately zero.Type: GrantFiled: December 7, 2006Date of Patent: October 11, 2011Assignee: ThalesInventors: Sylvain Schwartz, Gilles Feugnet, Jean-Paul Pocholle
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Publication number: 20110235658Abstract: The invention relates a power fiber laser system including at least one single-mode fiber laser, emitting at a signal wavelength, the fiber including at least one outer cladding and a core, in which the core of the fiber has a radially graded index. The fiber includes, at least over a part of its length, a geometrical section having a graded fiber-core radius that decreases between an input end of the section and an output end of the section, the core radius and the index variation between the cladding and the fiber at the input end being such that the normalized frequency at the signal wavelength is less than the normalized cutoff frequency at which the fiber becomes unimodal.Type: ApplicationFiled: March 27, 2009Publication date: September 29, 2011Applicant: THALESInventors: Jean-Paul Pocholle, Francois-Xavier Doittau
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Publication number: 20110194119Abstract: The field of the invention is that of solid-state laser gyros used for the measurements of rotation speed or relative angular positions. This type of equipment is notably used for aeronautical applications. The object of the invention is to complete the optical devices necessary to control the instability of lasers by specific optical devices enabling elimination of the dead zone and of population inversion gratings exiting in the amplifying medium. An “all optical” solid-state laser is hence obtained without moveable parts, stable and without a dead zone. To this end, the laser gyro according to the invention comprises notably and optical assembly enabling a nonreciprocal optical phase-shift to be introduced between the counterpropagating modes; and control means allowing the phase-shift amplitude to be varied periodically around a mean value that is very approximately zero.Type: ApplicationFiled: December 7, 2006Publication date: August 11, 2011Applicant: THALESInventors: Sylvain Schwartz, Gilles Feugnet, Jean-Paul Pocholle
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Patent number: 7978334Abstract: The general field of the invention is that of rate gyros, of the matter-wave type, allowing the measurement of a speed of rotation in a given direction of measurement. This type of rate gyro works by the Sagnac effect and uses ultracold atoms to perform the measurement. It necessarily comprises an atom trap allowing a cloud of ultracold atoms to be immobilized in a given configuration and means for separation-displacement-recombination of the cloud into two packets of atoms so as to make them trace out a given area.Type: GrantFiled: January 27, 2009Date of Patent: July 12, 2011Assignee: ThalesInventors: Sylvain Schwartz, Jean-Paul Pocholle
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Publication number: 20110122417Abstract: A sensor is used to measure a physical quantity and includes at least: a measurement optical fiber including at least one Bragg grating; optical means designed to inject, into the fiber, a first, “pump” wave at a first optical frequency and a second, “probe” wave at a second optical frequency, the second optical frequency being different from the first optical frequency, the Bragg grating being designed to reflect the first and second optical waves, and the optical power of the first wave being sufficient to give, after interaction with the second wave reflected by stimulated Brillouin scattering, a “Stokes” wave, the frequency of which is representative of the physical quantity to be measured; and means for analyzing the difference in frequency between the two, “pump” and “Stokes”, optical waves. The sensor may notably be used as a hydrophone.Type: ApplicationFiled: June 25, 2009Publication date: May 26, 2011Applicant: THALESInventors: Stéphanie Molin, Daniel Dolfi, Jean-Pierre Huignard, Jean-Paul Pocholle, Martine Doisy
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Patent number: 7930967Abstract: The present invention relates to a method for antimissile protection of vehicles having a very short response time with practically no false alarms and not requiring the use of means such as decoys or conventional laser jammers, while providing the best possible protection. It is characterized in that at least one curtain of plasma filaments is created between these vehicles and the probable launch point of these missiles, this curtain being intended to blind the target-seeking device of the missiles.Type: GrantFiled: June 7, 2006Date of Patent: April 26, 2011Assignee: ThalesInventors: Emmanuel Marquis, Jean-Paul Pocholle
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Publication number: 20110071787Abstract: Solid-state gyrolaser having a device for stabilizing the intensities making it possible to maintain equilibrium of the two counter-propagating modes having at least a means for calculating a rotation measurement (?, I?) of the gyrolaser on the basis of the counter-propagating modes having a frequency difference (??mes) between them, by assuming that the frequency difference (??mes) between the two counter-propagating modes is induced only by the rotation of the cavity.Type: ApplicationFiled: June 22, 2010Publication date: March 24, 2011Inventors: François GUTTY, Sylvain Schwartz, Jean-Paul Pocholle, Gilles Feugnet
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Publication number: 20110019179Abstract: The general field of the invention is that of fiber-optic sensors comprising at least one measurement optical fiber having an optically pumped doped amplifying medium, the optical characteristics of which are sensitive to a physical quantity, the fiber having at least one Bragg grating. The fiber is designed so as to generate, in the amplifying medium, two optical waves having different optical frequencies that propagate in the same direction after reflection on the Bragg grating and are emitted by the amplifying medium, the two optical frequencies depending on the physical quantity. The two waves may be generated using either a birefringent polarization-maintaining fiber or a DBR (Distributed Bragg Reflector) laser cavity. Notably, this sensor may be used as a hydrophone.Type: ApplicationFiled: March 16, 2009Publication date: January 27, 2011Applicant: THALESInventors: Stephanie Molin, Daniel Dolfi, Jean-Pierre Huignard, Martine Doisy, Loic Morvan, Jean-Paul Pocholle
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Publication number: 20100272320Abstract: A system for pointing a laser beam is provided.Type: ApplicationFiled: December 5, 2008Publication date: October 28, 2010Applicant: THALESInventors: François-Xavier Doittau, Jean-Paul Pocholle
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Publication number: 20100265601Abstract: A mirror for optical imaging includes a reflecting device having a reflective face. The reflecting device incorporates a light-emitting device of which one emitting end is situated in said reflective face in a zone which is not or not very reflective.Type: ApplicationFiled: December 5, 2008Publication date: October 21, 2010Applicant: THALESInventors: François-Xavier Doittau, Jean-Paul Pocholle
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Publication number: 20100265513Abstract: A multioscillator ring laser gyro includes an optical ring cavity, a solid-state amplifying medium and a measurement device arranged in such a way that a first linearly polarized propagation mode and a second linearly polarized propagation mode, perpendicular to the first mode, propagate in a first direction in the cavity and in such a way that a third linearly polarized propagation mode parallel to the first mode and a fourth linearly polarized propagation mode parallel to the second mode propagate in the opposite direction. The amplifying medium is a crystal of cubic symmetry having an entry face and an exit face, the crystal being cut so that said faces are approximately perpendicular to the <100> crystallographic direction, the various modes propagating in directions approximately perpendicular to said faces.Type: ApplicationFiled: December 1, 2008Publication date: October 21, 2010Applicant: THALESInventors: Sylvain Schwartz, Gilles Feugnet, Jean-Paul Pocholle
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Publication number: 20100177317Abstract: The general field of the invention is that of rate gyros, of the matter-wave type, allowing the measurement of a speed of rotation in a given direction of measurement. This type of rate gyro works by the Sagnac effect and uses ultracold atoms to perform the measurement. It necessarily comprises an atom trap allowing a cloud of ultracold atoms to be immobilized in a given configuration and means for separation-displacement-recombination of the cloud into two packets of atoms so as to make them trace out a given area.Type: ApplicationFiled: January 27, 2009Publication date: July 15, 2010Applicant: ThalesInventors: Sylvain Schwartz, Jean-Paul Pocholle
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Publication number: 20100147071Abstract: The general field of the invention is that of gravimeters, of the matter-wave type, allowing the measurement of the gravitational field or of an acceleration in a given direction of measurement. This type of gravimeter uses ultracold atoms to take the measurement. It necessarily comprises an atom trap (5) making it possible to immobilize an ultracold atom cloud (10) in a determined configuration and means (7) for splitting-recombining the cloud into two atom packets placed at different heights so as to create a phase shift due to gravity.Type: ApplicationFiled: January 27, 2009Publication date: June 17, 2010Applicant: ThalesInventors: Sylvain Schwartz, Jean-Paul Pocholle
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Publication number: 20100123901Abstract: The general field of the invention is that of gyrolasers comprising at least one ring-shaped optical cavity comprising at least three mirrors, a solid state amplifying medium pumped by a laser diode whose optical emission power is determined by a current supply source, the cavity and the amplifying medium being such that two so-called contra-rotating optical modes propagate in opposite directions to each other within the said optical cavity, the gyrolaser being a class B gyrolaser, the gyrolaser also comprising means of measuring the difference in optical frequency existing between the two optical modes. The gyrolaser comprises means of measuring the total optical power circulating in the optical cavity and first means of control of the current delivered by the supply source in such a way as to maintain the total optical power substantially constant in a narrow spectral band centred on the relaxation frequency of the laser.Type: ApplicationFiled: November 12, 2009Publication date: May 20, 2010Applicant: ThalesInventors: Sylvain Schwartz, Gilles Feugnet, Francois Gutty, Etienne Bonnaudet, Mehdi Alouini, Jean-Paul Pocholle