# US 10,371,764 B2 · All-optical and isotropic magnetometer > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 10,371,764 B2 - Document ID: US10371764B2 - Status: Granted - Kind: B2 - Application number: 15/204,230 - Filed: 2016-07-07 - Published: 2017-01-12 - Granted: 2019-08-06 - Earliest claimed: 2015-07-08 - Assignees: Commissariat A L'energie Atomique Et Aux Energies Alternatives - Applicants: Commissariat A L'Energie Atomique et aux Energies Alternatives - Inventors: Sophie Morales; Mathieu Baicry; Francois Bertrand; Matthieu Le Prado; Jean-Michel Leger; Umberto Rossini; Jaroslaw Rutkowski - Web page: https://patentgrep.com/patent/US10371764B2 ## CPC - G01R 33/26: using optical pumping - G01R: MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES (indicating correct tuning of resonant circuits H03J3/12) ## Abstract An optical pumping and isotropic measurement magnetometer. The magnetometer is all-optical in the sense that resonance between Zeeman sub-levels is induced by modulating the intensity or the frequency of the pump beam. Resonance is detected either using the pump beam itself or an unmodulated probe beam. The pump beam is linearly polarised and its polarisation direction is kept constant relative to the direction of the magnetic field to be measured, so that a measurement independent of the orientation of the field can be made. ## Claims ### Claim 1 An optical pumping magnetometer comprising: a cell filled with a gas; a laser source emitting a laser beam; a polarization module adapted to linearly polarize the laser beam and to rotate a polarization such that the laser beam is polarized in a polarization direction; a photodetector receiving the polarized laser beam after the polarized laser beam has passed through the cell and outputting an electrical signal; first slaving means to keep a constant angle between the polarization direction and a magnetic field to be measured, wherein the first slaving means includes modulation means to modulate at least a first part of the laser beam so as to generate a pump beam modulated by a modulation frequency (fm), wherein the modulation means includes a beam intensity modulator that generates the pump beam and is disposed between the laser source and the polarization module; second slaving means to keep said modulation frequency equal to a Larmor frequency of the gas or one of a plurality of harmonics of the Larmor frequency, a value of the magnetic field to be measured being obtained from said modulation frequency; and a frequency synthesizer that generates the modulation frequency (fm), based on a measurement signal generated by the second slaving means, and sends the modulation frequency (fm) as feedback to the beam intensity modulator. ### Claim 2 (depends on 1) The optical pumping magnetometer according to claim 1, wherein the modulation means make an intensity modulation at the Larmor frequency and at twice a frequency of the Larmor frequency. ### Claim 3 (depends on 2) The optical pumping magnetometer according to claim 2, wherein the photodetector receives the pump beam and in that the electrical signal resulting from conversion of the pump beam by the photodetector is output to the first and second slaving means. ### Claim 4 (depends on 2) The optical pumping magnetometer according to claim 2, wherein the magnetometer comprises an optical separator on an input side of the polarization module to form a first part and a second part of the laser beam, the pump beam (P) being obtained by modulating the first part of the laser beam by said modulation means, the second part of the laser beam forming a probe beam (S) not modulated by said modulation means, the electrical signal resulting from conversion of the probe beam being input to the first and to the second slaving means. ### Claim 5 (depends on 4) The optical pumping magnetometer according to claim 4, wherein the probe beam and the pump beam are parallel and are separated by a distance less than a diffusion length of gas atoms in the cell. ### Claim 6 (depends on 4) The optical pumping magnetometer according to claim 4, wherein the probe beam and the pump beam intersect in the cell at an angle less than 90°. ### Claim 7 (depends on 1) The optical pumping magnetometer according to claim 1, wherein the first slaving means perform a demodulation at the Larmor frequency. ### Claim 8 (depends on 1) The optical pumping magnetometer according to claim 1, wherein the second slaving means perform an amplitude detection on the peak of a DC line, an anti-symmetric error signal being obtained by a demodulation at a harmonic of a second modulation frequency (fmod_BF) superposed on the modulation frequency (fm). ### Claim 9 (depends on 2) The optical pumping magnetometer according to claim 2, wherein the modulation means are composed of an acousto-optic modulator. ### Claim 10 (depends on 2) The optical pumping magnetometer according to claim 2, wherein the modulation means are composed of an electro-optic modulator. ### Claim 11 (depends on 1) The optical pumping magnetometer according to claim 1, wherein the laser source is a laser diode that comprises third slaving means receiving said electrical signal and controlling a power supply current and/or a temperature of the laser diode such that a wavelength of the laser beam is constant. ### Claim 12 (depends on 1) The optical pumping magnetometer according to claim 1, wherein the modulation means make a frequency modulation at the Larmor frequency. ### Claim 13 (depends on 12) The optical pumping magnetometer according to claim 12, wherein the modulation means comprise an alternating current/direct current (AC/DC) AC/DC coupler to superpose a modulation current on a laser power supply current. ### Claim 14 (depends on 12) The optical pumping magnetometer according to claim 12, wherein the first slaving means perform a demodulation at the Larmor frequency. ### Claim 15 (depends on 12) The optical pumping magnetometer according to claim 12, wherein the second slaving means perform an amplitude detection on the peak of a DC line, an anti-symmetric error signal being obtained by demodulation at a harmonic of a second modulation frequency (fmod_BF) superposed on the modulation frequency (fm). ### Claim 16 (depends on 12) The optical pumping magnetometer according to claim 12, wherein the laser source is a laser diode that comprises third slaving means receiving said electrical signal and controlling a power supply current and/or a temperature such that a laser beam carrier frequency is constant. ### Claim 17 (depends on 4) The optical pumping magnetometer according to claim 4, wherein the probe beam and the pump beam intersect in the cell at an angle less than 10°. ### Claim 18 (depends on 4) The optical pumping magnetometer according to claim 4, wherein the probe beam and the pump beam intersect in the cell at an angle less than 5°. ### Claim 19 An optical pumping magnetometer comprising: a cell filled with a gas; a laser source emitting a laser beam; a polarization module adapted to linearly polarize the laser beam and to rotate a polarization such that the laser beam is polarized in a polarization direction; a photodetector receiving the polarized laser beam after the polarized laser beam has passed through the cell and outputting an electrical signal; first slaving means to keep a constant angle between the polarization direction and a magnetic field to be measured, wherein the first slaving means includes modulation means to modulate at least a first part of the laser beam so as to generate a pump beam modulated by a modulation frequency (fm); second slaving means to keep said modulation frequency equal to a Larmor frequency of the gas or one of a plurality of harmonics of the Larmor frequency, a value of the magnetic field to be measured being obtained from said modulation frequency; and a frequency synthesizer that generates the modulation frequency (fm), based on a measurement signal generated by the second slaving means, and sends the modulation frequency (fm) as feedback to the modulation means, wherein the modulation means make an intensity modulation at the Larmor frequency and at twice a frequency of the Larmor frequency, the magnetometer comprises an optical separator on an input side of the polarization module to form a first part and a second part of the laser beam, the pump beam (P) being obtained by modulating the first part of the laser beam by said modulation means, the second part of the laser beam forming a probe beam (S) not modulated by said modulation means, the electrical signal resulting from conversion of the probe beam being input to the first and to the second slaving means, and the probe beam and the pump beam are parallel and are separated by a distance less than a diffusion length of gas atoms in the cell.