• 专利附录
  • 专利说明
  • 权利要求
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  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The invention relates to a magnetometer (10) comprising a cell (1) filled with a gas subjected to an ambient magnetic field, an optical pump source (2), a photodetector (3) and a loop servo system. closed magnetometer to operate in zero field. Said servo system comprises: - an optical cavity (11) delimited by mirrors (M1, M2) in which the cell (1) is arranged, - an optical excitation source (9) configured to illuminate the at least one an optical cavity with a circularly polarized beam and tuned to an excitation wavelength offset from the pumping wavelength; and - a regulator coupled to the photodetector and configured to drive the optical excitation source in a manner that is it induces, by Stark effect, the equivalent of a compensation magnetic field opposite to the ambient magnetic field and oriented in the direction of propagation of the light in the cavity.
    公开号:FR3062922A1
    申请号:FR1751217
    申请日:2017-02-15
    公开日:2018-08-17
    发明作者:Augustin Palacios Laloy
    申请人:Commissariat a lEnergie Atomique CEA；Commissariat a lEnergie Atomique et aux Energies Alternatives CEA；
    IPC主号:
    专利说明:

    DESCRIPTION
    TECHNICAL AREA
    The field of the invention is that of magnetometers with optical pumping controlled in zero field. The invention finds application in the imaging of biomagnetic fields, for example in magnetocardiography or in magnetoencephalography, in particular by means of magnetometers used in a network.
    PRIOR STATE OF THE ART
    Optically pumped magnetometers are based on a magnetic resonance between Zeeman lines amplified using optical pumping. These magnetometers use atomic gases confined in a cell (typically metastable helium or alkaline gases) as sensitive elements.
    These magnetometers, which can take different configurations, allow you to go back to the magnetic field by exploiting the following three processes which take place either sequentially or concomitantly:
    1) The use of polarized light sources (typically lasers) makes it possible to prepare atomic states characterized by a certain orientation or alignment of their spins.
    2) These states evolve comprehensively under the effect of the magnetic field, in particular under the Zeeman effect (shifts in energy levels dependent on the magnetic field).
    3) The optical properties of the atomic medium undergo modifications which depend on the state of the atoms. It is thus possible by optical measurement (for example of absorption) to go back to the Zeeman offset undergone, and from there to the magnetic field in which the cell is immersed.
    According to the different possible configurations, it is then possible to deduce either the module (for scalar magnetometers) or the different components of the magnetic field (for vector magnetometers) at the location of the cell.
    The level of sensitivity (also called low noise) and accuracy achievable with such magnetometers are very remarkable and clearly more favorable than those of most other magnetic measurement technologies (fluxgate, Hall effect, magnetoresistance, etc.). Only the SQUID magnetometer has a similar noise, but it requires cryogenic cooling of the sensitive element (using superconductors), which limits its practical field of application.
    To carry out a vectorial measurement of the magnetic field with a wide bandwidth, there are two well-known configurations: the first known as "Hanle effect" and the second which receives the name of "parametric resonance magnetometer". These configurations are described in particular in the article by J. DupontRoc, Determination by optical methods of the three components of a very weak magnetic field, Review of Applied Physics, vol. 5, no. 6, pp. 853-864, 1970. They operate at very low external magnetic field values (inducing a Zeeman offset lower than the relaxation rate of the Zeeman sub-levels of the atom, which for helium-4 sets a limit around 100 nT, 500 times less intense than the Earth's magnetic field).
    When a weak transverse static field is applied to the cell and swept around zero, the atoms under subject to a movement of precession and the number of absorbed photons coming from the laser of otic pumping undergoes resonant variations (Hanle effect). Analogous resonances called parametric resonances (i.e., in the presence of frequency modulated magnetic fields) are observed when an RF field, collinear with the ambient field and orthogonal to the direction of photon polarization, is applied. Under these conditions, the magnetic moment of each atom undergoes resonant oscillations at frequencies multiple of that of the excitation RF field. The measurement of the amplitude of these oscillations makes it possible to go back to the module of the magnetic field collinear with the RF field.
    In these two configurations, it is advantageous to operate the magnetometer "in closed loop" by constantly subjecting the sensitive element to a zero total magnetic field. This zero-slave operation has the advantage of being less sensitive to variations in experimental parameters (laser powers, density of the sensitive element, etc.).
    The zero total magnetic field is obtained by generating compensating magnetic fields by injecting currents into suitable coils which surround the sensitive element. These compensation fields cancel each of the components of the ambient magnetic field by means of closed-loop regulation of the injected currents. The measurement of the currents flowing in the coils makes it possible to deduce the fields which it is necessary to apply to cancel the various components of the ambient field, and therefore to have the value of these various components.
    However, in many environments the zero-field control of a magnetometer can be harmful. This is particularly the case when using magnetometers arranged according to a matrix network dedicated to the reconstruction of magnetic sources (for example for the imaging of nervous or cardiac currents). Indeed, the application of compensation fields on a magnetometer impacts the fields seen by the neighboring magnetometers (crosstalk effect) and therefore disturbs the measurements made by the neighboring magnetometers. In other applications (coupling with magnetostrictive sensors for example), the effect of the compensation fields can disturb the phenomena that one seeks to observe.
    STATEMENT OF THE INVENTION
    An objective of the invention is to make it possible to operate an optically pumped magnetometer in “zero field” regime without having to generate compensating magnetic fields, while the ambient fields to be compensated are significantly greater than 100 nT .
    To this end, the invention provides a magnetometer comprising a cell filled with a gas subjected to an ambient magnetic field, an optical pumping source capable of emitting towards the cell a laser beam tuned to a pumping wavelength , a photodetector receiving the laser beam having passed through the cell and a closed loop servo system of the magnetometer to operate it in zero field. The servo system includes:
    - an optical cavity delimited by mirrors in which the cell is arranged,
    an optical excitation source configured to illuminate the at least one optical cavity with a circularly polarized beam and tuned to an excitation wavelength offset from the pumping wavelength so as to allow induce in the cell, by Stark effect, the equivalent of a magnetic field oriented in a direction of propagation of light in the optical cavity, and
    - a closed loop regulator coupled to the photodetector and configured to control the optical excitation source so that it induces in the cell the equivalent of a compensating magnetic field opposite to the ambient magnetic field in said direction of propagation light.
    Some preferred but non-limiting aspects of this magnetometer are as follows:
    the optical cavity is a resonant cavity tuned to the excitation wavelength of the optical excitation source;
    - the optical cavity is a multi-passage cavity;
    - the mirrors of the optical cavity are formed on the walls of the cell;
    the optical cavity is arranged so that the direction of propagation of the light in the at least one optical cavity corresponds to a measurement axis of the magnetometer;
    the optical excitation source comprises a laser configured to deliver a laser beam tuned to the excitation wavelength and a circular polarizer;
    - the difference between the pumping wavelength and the excitation wavelength is between 0.25 and 2.5 times the optical width at half height of the line of the atomic transition activated by the source optical pumping;
    the optical excitation source comprises a laser configured to deliver a laser beam tuned to the pumping wavelength and an optical modulator able to shift the wavelength of the laser beam from the pumping wavelength to the excitation wavelength;
    - at the output of the modulator, the laser beam has two lateral bands of wavelength respectively above and below the pumping wavelength, and the distance between the two lateral bands is between 0.5 and 5 times the optical width at mid-height of the line of the atomic transition activated by the optical pumping source;
    - The optical excitation source further comprises an optical filter for filtering one of the two lateral bands and a polarizer for circularly polarizing the unfiltered lateral band;
    the optical excitation source further comprises two polarizing filters and a quarter-wave plate arranged in cascade, the two polarizing filters consisting of a first linear polarizer capable of vertically polarizing one of the side bands and of a second linear polarizer able to horizontally polarize the other of the lateral bands, the quarter-wave plate circularly polarizing each of the lateral bands respectively in the counterclockwise direction and in the clockwise direction;
    - the regulator includes an integrator;
    - It includes three optical cavities each associated with an axis of measurement of the magnetometer and illuminated by its own source of optical excitation.
    The invention also relates to a magnetometry device comprising a network of magnetometers each according to the invention, as well as to a method of servo-control in the zero field of a magnetometer.
    BRIEF DESCRIPTION OF THE DRAWINGS
    Other aspects, aims, advantages and characteristics of the invention will appear better on reading the following detailed description of preferred embodiments thereof, given by way of nonlimiting example, and made with reference to the accompanying drawings. on which ones :
    - Figure 1 is a diagram of a magnetometer according to the invention;
    - Figure 2 is a diagram showing a possible implementation of closed loop regulation according to the invention.
    DETAILED PRESENTATION OF PARTICULAR EMBODIMENTS
    With reference to FIG. 1, the invention relates to an optically pumped magnetometer 10. The magnetometer 10 comprises a cell 1 filled with a gas, for example helium-4 or an alkaline gas, subjected to a magnetic field ambient Bo. The ambient magnetic field Bo is broken down into three components Bx, By and Bz each along one of the measurement axes of the magnetometer x, y and z.
    The cell is illuminated by an optical pumping source 2 capable of emitting towards the cell a laser beam tuned to a pumping wavelength. The pumping wavelength is set on an atomic transition line, for example on the Do line at 1083 nm in the case of helium-4. The pump beam can be polarized rectilinearly in the z direction by means of a rectilinear polarizer (not shown). A photodetector 3 receives the laser beam having passed through the cell.
    In the case where the sensitive element is helium-4, the magnetometer 10 also comprises an HF discharge system, comprising an HF generator 4 and overvoltage coils 5. It also comprises an RF frequency generator 7 which supplies two coils 6 of orthogonal axes which surround the cell. The coils 6 generate two RF fields orthogonal to the direction of polarization of the pump beam. We thus find an RFx field and an RFy field on the x and y axes of respective pulses Ω and ω.
    Under these conditions, the magnetic moment of each atom in the cell undergoes resonant oscillations at frequencies multiple of that of the excitation RF fields. The amplitude of the oscillations makes it possible to measure the modulus of the collinear magnetic field with the field of radiofrequency. More particularly, the RFx field oscillating at the pulsation Ω is oriented along the x axis and the RFy field oscillating at the pulsation orient is oriented along the y axis. This then results in a modulation of the light transmitted in particular at the pulses Ω, ω and Ω ± ω. These signals are respectively proportional to the components of the total magnetic field at the cell level.
    The magnetometer 10 also includes an electronic processing card 8 which processes the electrical signal at the output of the photodetector 8 to supply the values of the components B x , B y and B z of the ambient field Bo. The card 8 also comes to control the RF frequency generator 7 and control the closed-loop control of the magnetometer to make it operate in zero field.
    Once the cell is turned on thanks to the HF discharge system, the optical beam passing through the cell is converted into an electrical signal by means of the photodetector 3. As shown in FIG. 2, the electronic processing card 8 comprises a closed loop regulator which separates the resulting signal into three channels: a first channel Vx for the detection of the signal at Ω / 2π (x axis), a second channel Vy for the detection of the signal at ω / 2π (y axis), and a third channel Vz for signal detection at Ω ± ω / 2 n (z axis). The signal on each of the first and second channels is first amplified and then filtered with a bandpass filter BPx, BPy corresponding to the appropriate central frequency (i.e. corresponding to that of the applied RF field, RFx and RFy respectively). The signal obtained is then multiplied by a reference signal and processed by a synchronous detector DSx, DSy followed by a low-pass filter LPx, LPy.
    The third channel Vz uses two synchronous detections in series (at ω / 2π then Ω / 2π) to go back to the amplitude modulated resonance at frequencies Ω ± ω / 2 n (Z axis). There is a BPz bandpass filter, a DSz synchronous detector and an LPz lowpass filter.
    Each of these three channels Vx, Vy, Vz includes an integrator Ix, ly, Iz making it possible to ensure closed-loop regulation by means of which the system is controlled in zero field. Here, closed-loop regulation does not control the injection of current into a set of three orthogonal coils to generate magnetic fields to compensate for the ambient field. According to the invention, in fact, the Stark effect is used to induce the equivalent of these compensation fields using optical excitations.
    More particularly, the invention exploits the phenomenon receiving the designation of "lightshift" (or alternative Stark offset, or even fictitious magnetic field induced by light) according to which optical excitations in circular polarization and slightly offset with respect to the lines of atomic resonances induce behavior equivalent to that of a static magnetic field. This phenomenon is notably described quantitatively in the article W. Happer and B. S. Mathur, Effective Operator Formalism in Optical Pumping, Phys. Rev., vol. 163, no. 1, pp. 12-25, Nov. 1967.
    The magnetometer 10 according to the invention integrates such an optical excitation source for each useful measurement axis, ie three sources in total, so as to induce a fictitious field Bcf x , Bcf y and Bcf z on each of the three measurement axes x, y and z.
    Thus, the magnetometer 10 comprises a closed loop servo system of the magnetometer to make it operate in zero field which includes these optical excitation sources, which are controlled by a closed loop regulator coupled to the photodetector 3 so as to induce Bcf x , Bcf y and Bcf z fictitious fields such as Bcf x = -B x , Bcf y = -B y and Bcf z = -B z . In the context of the invention, the integrators Ix, ly and Yz of the closed loop regulator of the processing card 8 supply control signals Ax, Ay and Ay to the optical excitation sources making it possible to ensure operation in the field no. These are in particular control signals relating to the amplitude of the light beams delivered by these excitation sources.
    A difficulty nevertheless resides in the fact that the intensity of the light necessary to induce the equivalent of the magnetic fields of compensation usually used is very high. For example, in the case of helium, the light intensity necessary to induce a fictitious field of the order of the terrestrial field is several W / cm 2 . This requires having high intensity sources (the intensity of the sources typically used in magnetometers with optical pumping being a few tens of mW). This also induces high electrical consumption, particularly for networks (matrices) of magnetometers which have several tens or even hundreds of magnetometers. Finally, the light power of these beams must be dissipated, which induces heating of the materials surrounding the cell, and therefore an increased difficulty for the thermal stabilization of the latter.
    In order to circumvent this difficulty, the invention proposes to play on the coupling of light with atoms so as to make more efficient “all optical” compensation by the Stark effect. For this, the cell containing the sensitive element is placed within a set of optical cavities (one cavity for each useful measurement axis, therefore a maximum of three). Indeed the confinement of light in these cavities has the effect of increasing the coupling between light and atoms, which allows to induce significant fictitious fields (tens of μΤ) with low light amplitudes (a few mW or tens of mW) at the output of the different excitation sources.
    Thus, within the framework of the invention and with reference to FIG. 1, the closed-loop servo device of the magnetometer to make it operate in zero field comprises an optical cavity 11 delimited by mirrors Ml, M2 in which is arranged cell 1. Light propagates in a direction of propagation in the optical cavity 11.
    The servo device further comprises an optical excitation source 9 configured to illuminate the at least one optical cavity 11 with a circularly polarized beam and tuned to an excitation wavelength offset from the length of pumping wave. Such a beam makes it possible to induce in the cell, by Stark effect, the equivalent of a magnetic field oriented along the direction of propagation of the light in the optical cavity.
    The servo device is supplemented by the aforementioned regulator which controls the optical excitation source so that it induces in the cell the equivalent of a compensating magnetic field opposite to the component of the ambient magnetic field in said direction of light propagation.
    Preferably, the optical cavity is arranged in such a way that the direction of propagation of the light in the optical cavity corresponds to an axis of measurement of the magnetometer. And there are of course preferably three optical cavities each associated with a measurement axis of the magnetometer and each illuminated by its own source of optical excitation.
    The optical cavity is more particularly delimited by a semi-reflecting mirror on the excitation source side and by a totally reflecting mirror. These mirrors can be interferometric filters produced by a stack of thin layers (in the sense that their thickness is less than the wavelength of light) of two materials having a high index contrast (for example titanium dioxide and silicon dioxide). In the stack, the layers of each of the materials are alternated with a distribution of thicknesses calculated according to techniques well known in the art, with the aim, for example, of reflecting the wavelength of the light used for compensation by effect. Stark, but to transmit a substantial level from that used for the optical pumping of atoms.
    In one possible embodiment, the optical cavity is a resonant cavity tuned to the excitation wavelength of the optical excitation source. It is for example a Fabry-Perot cavity whose transmittance as a function of the wavelength has regularly spaced peaks.
    In another possible embodiment, the optical cavity is a multi-passage cavity which differs from a resonant cavity in that there is no interference between the different passages of light. In such a cavity, the direction of propagation of light corresponds to the average of the directions of propagation of each of the passages, the average being weighted as a function of the light intensity on each of the passages.
    The mirrors of the optical cavity can be formed directly on the walls of the cell, these having been subjected to a reflective treatment, for example an interferometric filter produced by a stack of thin layers such as that described above deposited directly on the cell walls. It is possible to deposit, for example by evaporation or spraying processes, on the glass elements which will constitute the walls of the cell before these are assembled by molecular bonding or by thermal welding to constitute a closed container. and waterproof.
    The optical excitation source 9 can comprise a laser configured to deliver a laser beam tuned to the excitation wavelength and a circular polarizer. It is possible to provide for the difference between the pumping wavelength and the length excitation wave is between 0.25 and 2.5 times, preferably between 0.35 and 1.5 times, preferably 0.5 times, the optical width at half height of the line of the transition atomic activated by the optical pumping source.
    Alternatively, the optical excitation source 9 comprises a laser configured to deliver a laser beam tuned to a tuning wavelength and an optical modulator able to shift the wavelength of the laser beam by the wavelength d towards the excitation wavelength. At the output of the modulator, the laser beam has two lateral bands of wavelength respectively above and below the wavelength of agreement at λ ε ± Δλ, where À c corresponds to the wavelength of d agreement and Δλ represents the difference between the excitation wavelength and the pumping wavelength.
    The distance between the two lateral bands 2 * Δλ is preferably between 0.5 and 5 times, even more preferably between 0.7 and 3 times, and even more preferably equal to, the optical width at half height the line of the atomic transition activated by the optical pumping source.
    The tuning wavelength can correspond to the pumping wavelength, in which case the atomic transition line is equidistant from the side bands. In order for the laser to be tuned to the wavelength of the atomic transition used for optical pumping, its wavelength is controlled by methods well known in the field of atomic physics, in particular a method based on the dichroism of atomic vapor known in English as DAVLL for "Dichroic Atomic Vapor Laser Lock" and described for example in the following publication: B. Chéron, H. Gilles, J. Hamel, O. Moreau, and H. Sorel, Laser frequency stabilization using Zeeman effect, Journal of Physics III, vol. 4, no. 2, pp. 401-406, 1994.
    The side band above the chord wavelength makes it possible to induce a fictitious field whose sign is opposite to the fictitious field induced by the side band above the chord wavelength.
    Also, in one embodiment, the optical excitation source further comprises an optical filter, produced for example by an interferometric filter as described above, for filtering one of the two lateral bands and a polarizer for circularly polarizing the unfiltered side band.
    In another embodiment, one comes to play on the direction of polarization of each of these bands so that their virtual fields add up. The optical excitation source for this includes two polarizing filters and a quarter wave plate arranged in cascade. The two polarizing filters consist of a first linear polarizer capable of vertically polarizing one of the side bands and of a second linear polarizer capable of horizontally polarizing the other of the side bands. These are, for example, wire grid polarizers.
    The quarter-wave plate circularly polarizes each of the lateral bands respectively in the counterclockwise direction and in the clockwise direction. Insofar as the right circularly polarized light induces a fictitious field of sign opposite to that induced by the left circularly polarized light, there are at the output of the quarter wave plate side bands polarized inversely and therefore corresponding to fields fictitious which are added.
    The invention is not limited to a magnetometer as such (alone or used in a network of magnetometers of a magnetometry device) but also extends to the process of servo-control in the zero field of such a magnetometer with optical pumping. According to this method, the lighting of an optical cavity delimited by mirrors is carried out in a closed loop in which the cell is arranged by a circularly polarized beam and tuned to an excitation wavelength offset from at the pumping wavelength. This regulation is carried out so as to induce in the cell, by Stark effect, the equivalent of a compensating magnetic field opposite to the ambient magnetic field in the direction of propagation of the light in the optical cavity.
    The invention finds application in medical imaging of the heart and the brain. It also finds application in processes involving large magnetic fields: detection of NMR / MRI signals, relaxometry, nuclear quadrupole resonance (RQN) intended for the detection of explosives; as well as as a probe for active magnetic shields or magneto-elasticity measurements.
    权利要求:
    Claims (15)
    [1" id="c-fr-0001]
    1. Magnetometer (10) comprising a cell (1) filled with a gas subjected to an ambient magnetic field, an optical pumping source (2) capable of emitting towards the cell a laser beam tuned to a wavelength pumping, a photodetector (3) receiving the laser beam having passed through the cell and a closed loop servo system of the magnetometer to operate it in zero field, characterized in that said servo system comprises:
    - an optical cavity (11) delimited by mirrors (Ml, M2) in which the cell (1) is arranged,
    - an optical excitation source (9) configured to illuminate the at least one optical cavity with a circularly polarized beam and tuned to an excitation wavelength offset from the pumping wavelength so as to allow to induce in the cell, by Stark effect, the equivalent of a magnetic field oriented in a direction of propagation of light in the optical cavity, and
    - a closed loop regulator (Vx, Vy, Vz) coupled to the photodetector and configured to drive the optical excitation source so that it induces in the cell the equivalent of a magnetic field of compensation opposite to the field magnetic ambient in said direction of light propagation.
    [2" id="c-fr-0002]
    2. The magnetometer according to claim 1, in which the optical cavity (11) is a resonant cavity tuned to the excitation wavelength of the optical excitation source.
    [3" id="c-fr-0003]
    3. Magnetometer according to claim 1, in which the optical cavity (11) is a multi-passage cavity.
    [4" id="c-fr-0004]
    4. Magnetometer according to one of claims 1 to 3, wherein the mirrors (Ml, M2) of the optical cavity are formed on the walls of the cell (1).
    [5" id="c-fr-0005]
    5. Magnetometer according to one of claims 1 to 4, in which the optical cavity (11) is arranged so that the direction of propagation of the light in the at least one optical cavity corresponds with an axis of measurement of the magnetometer.
    [6" id="c-fr-0006]
    6. Magnetometer according to one of claims 1 to 5, wherein the optical excitation source (9) comprises a laser configured to deliver a laser beam tuned to the excitation wavelength and a circular poizer.
    [7" id="c-fr-0007]
    7. The magnetometer according to claim 6, in which the difference between the pumping wavelength and the excitation wavelength is between 0.25 and 2.5 times the optical width at half height of the line of the atomic transition activated by the optical pumping source.
    [8" id="c-fr-0008]
    8. Magnetometer according to one of claims 1 to 5, in which the optical excitation source (9) comprises a laser configured to deliver a laser beam tuned to the pumping wavelength and an optical modulator capable of shifting the wavelength of the laser beam from the pumping wavelength to the excitation wavelength.
    [9" id="c-fr-0009]
    9. The magnetometer according to claim 8, in which at the output of the modulator the laser beam has two lateral bands of wavelength respectively above and below the pumping wavelength, and in which the distance between the two bands lateral is between 0.5 and 5 times the optical width at mid-height of the line of the atomic transition activated by the optical pumping source.
    [10" id="c-fr-0010]
    10. The magnetometer according to claim 9, in which the optical excitation source (9) further comprises an optical filter for filtering one of the two lateral bands and a polarizer for circularly polarizing the unfiltered lateral band.
    [11" id="c-fr-0011]
    11. The magnetometer according to claim 9, in which the optical excitation source further comprises two polarizing filters and a quarter-wave plate arranged in cascade, the two polarizing filters consisting of a first linear polarizer capable of vertically polarizing one lateral bands and a second linear polarizer capable of horizontally polarizing the other of the lateral bands, the quarter-wave plate circularly polarizing each of the lateral bands respectively in the counterclockwise direction and in the clockwise direction.
    [12" id="c-fr-0012]
    12. Magnetometer according to one of claims 1 to 11, wherein the regulator comprises an integrator (ly, Iz, Ix).
    [13" id="c-fr-0013]
    13. Magnetometer according to one of claims 1 to 12, comprising three optical cavities each associated with a measurement axis of the magnetometer and illuminated by its own source of optical excitation.
    [14" id="c-fr-0014]
    14. A magnetometry device comprising a network of magnetometers each conforming to the magnetometer of any one of claims 1 to 13.
    [15" id="c-fr-0015]
    15. A method of servo-control in a zero field of a magnetometer comprising a cell filled with a gas subjected to an ambient magnetic field, an optical pumping source capable of emitting towards the cell a laser beam tuned to a length of pumping wave, the method comprising closed-loop regulation of the lighting of an optical cavity delimited by mirrors in which the cell is arranged by a circularly polarized beam and tuned to an excitation wavelength offset from at the pumping wavelength so as to induce in the cell, by the Stark effect, the equivalent of a compensating magnetic field opposite to the ambient magnetic field in the direction of propagation of light in the optical cavity.
    S. 61785
    1/2
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    同族专利:
    公开号 | 公开日
    EP3364204A1|2018-08-22|
    EP3364204B1|2019-09-11|
    FR3062922B1|2019-04-19|
    引用文献:
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    US20160116553A1|2014-10-24|2016-04-28|Korea Research Institute Of Standards And Science|Atomic magnetometer and operating method of the same|EP3907513A1|2020-05-06|2021-11-10|Commissariat à l'énergie atomique et aux énergies alternatives|Current sensor based on the faraday effect in an atomic gas|
    FR3090890B1|2018-12-21|2021-10-08|Commissariat Energie Atomique|Optical pumping magnetometer of a sensitive element with linearly polarized light and multi-pass in the sensitive element|
    FR3093816B1|2019-03-12|2021-04-16|Commissariat Energie Atomique|Zero-field slave magnetometer with low-frequency filtering of the compensation field|
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    FR3113737A1|2020-08-27|2022-03-04|Commissariat A L'energie Atomique Et Aux Energies Alternatives|Magnetometer in elliptical polarization with two radiofrequency field components for detection of parametric resonance in absorption|
    法律状态:
    2018-02-26| PLFP| Fee payment|Year of fee payment: 2 |
    2018-08-17| PLSC| Publication of the preliminary search report|Effective date: 20180817 |
    2020-02-28| PLFP| Fee payment|Year of fee payment: 4 |
    2021-11-12| ST| Notification of lapse|Effective date: 20211005 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1751217A|FR3062922B1|2017-02-15|2017-02-15|NUCLEAR FIELD-BASED MAGNETOMETER BY ALTERNATIVE STARK EFFECT EXACERBED BY AN OPTICAL CAVITY|
    FR1751217|2017-02-15|FR1751217A| FR3062922B1|2017-02-15|2017-02-15|NUCLEAR FIELD-BASED MAGNETOMETER BY ALTERNATIVE STARK EFFECT EXACERBED BY AN OPTICAL CAVITY|
    EP18156363.6A| EP3364204B1|2017-02-15|2018-02-12|Zero field magnetometer controlled by ac stark effect|
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