CN112816926B - Three-dimensional coil coefficient calibration method based on optical pump nuclear magnetic resonance - Google Patents
Three-dimensional coil coefficient calibration method based on optical pump nuclear magnetic resonance Download PDFInfo
- Publication number
- CN112816926B CN112816926B CN202011590765.7A CN202011590765A CN112816926B CN 112816926 B CN112816926 B CN 112816926B CN 202011590765 A CN202011590765 A CN 202011590765A CN 112816926 B CN112816926 B CN 112816926B
- Authority
- CN
- China
- Prior art keywords
- coil
- magnetic field
- current
- frequency
- amplitude
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Active
Links
Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
- G01R33/44—Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
Abstract
A three-dimensional coil coefficient calibration method based on optical pump nuclear magnetic resonance is characterized in that an atomic glass air chamber filled with cesium atoms and buffer gas is arranged in the center of a three-dimensional coil, current is applied to the coil in any one or two directions in the three-dimensional coil respectively to generate a direct-current magnetic field, the atomic air chamber is irradiated by left-handed circularly polarized light, the irradiation direction of the circularly polarized light and the applied direct-current magnetic field are in the same plane, a radio-frequency magnetic field with fixed frequency is applied in the direction perpendicular to the direct-current magnetic field and the plane of the circularly polarized light, the optical pump nuclear magnetic resonance state is achieved by adjusting the current, at the moment, light penetrating through the atomic air chamber is maximally modulated by the cesium atoms, the amplitude of emergent light is obtained after photoelectric conversion and demodulation are carried out, and when the current value corresponding to the maximum amplitude is obtained, coil coefficient calibration is achieved. The method has the advantages of high precision, no need of using other magnetic field measuring instruments, simple operation and good universality, and can be conveniently applied to the coil coefficient determination of the three-dimensional coil of the nuclear magnetic resonance gyroscope.
Description
Technical Field
The invention relates to a technology in the field of nuclear magnetic resonance, in particular to a three-dimensional coil coefficient calibration method based on optical pump nuclear magnetic resonance.
Background
The nuclear magnetic resonance gyroscope has wide application prospects in the fields of aviation, aerospace, navigation, traffic and the like, wherein performance indexes of the three-dimensional coil serving as a core component have great influence on the detection precision of the nuclear magnetic resonance gyroscope, but the three-dimensional coil of the nuclear magnetic resonance gyroscope is a small-size special-shaped coil and is difficult to calibrate in a conventional mode. The prior art adopts a micro three-axis fluxgate, adopts nuclear magnetic resonance calibration and carries out coil calibration based on an SERF magnetometer, and because the coil volume is small, a magnetometer probe is limited by the size and the shape of the magnetometer probe and cannot be placed at the center of the coil, so that the large calibration error precision can be caused, and the magnetometer probe cannot be applied to the calibration of a three-dimensional coil of a nuclear magnetic resonance gyroscope.
Disclosure of Invention
Aiming at the defects in the prior art, the invention provides the three-dimensional coil coefficient calibration method based on the optical pump nuclear magnetic resonance, which has the advantages of high characteristic precision, no need of using other magnetic field measuring instruments, simple operation and good universality, and can be conveniently applied to the coil coefficient measurement of the three-dimensional coil of the nuclear magnetic resonance gyroscope.
The invention is realized by the following technical scheme:
the atomic glass gas chamber filled with cesium atoms and some buffer gases is arranged in the center of a three-dimensional coil, current is respectively applied to the coil in any one or two directions in the three-dimensional coil to generate a direct-current magnetic field, the atom gas chamber is irradiated by left-handed circularly polarized light, the irradiation direction of the circularly polarized light and the applied direct-current magnetic field are on the same plane, a radio-frequency magnetic field with fixed frequency is applied in the direction perpendicular to the direct-current magnetic field and the plane of the circularly polarized light, the nuclear magnetic resonance state of an optical pump is achieved by adjusting the current, at the moment, the light penetrating through the atom gas chamber is subjected to the maximum modulation of the cesium atoms, the amplitude of emergent light is obtained after the photoelectric conversion and demodulation of the emergent light, and when the current value corresponding to the maximum amplitude is obtained, the coil coefficient calibration is realized.
The optical pump nuclear magnetic resonance state is as follows: frequency omega ═ gamma B of radio frequency magnetic field0Wherein: gamma is the gyromagnetic ratio of cesium atoms, being a fixed constant, B0The field strength of the DC magnetic field and the field strength B of the radio frequency magnetic field1cosωt。
The current value corresponding to the maximum amplitude value obtains the amplitude value of the emergent light after photoelectric conversion and demodulation are carried out on the emergent light, and the maximum modulation point is obtained when the amplitude value is maximum. The corresponding current value I satisfies ω ═ γ I λ, thereby obtaining a coil coefficient λ of the coil in the corresponding direction.
Technical effects
The invention integrally solves the technical problems that the center point of the coil cannot be accurately and effectively calibrated due to the limitation of the volume shape of the coil, the volume shape of the magnetometer and the like when the traditional fluxgate magnetometer is used for calibrating the coil, the calibration is not accurate due to the limitation of the volume shape of a probe of the magnetometer and the complicated installation process is caused by the calibration of a three-dimensional coil.
Compared with the prior art, the invention can accurately calibrate the center of the three-dimensional coil by the optical pump magnetic resonance effect, has high precision and avoids using other magnetic field measuring instruments. The size and shape of the atomic gas chamber used in the invention are easy to change, the minimum size can reach 1mm level at present, and the size of the atomic gas chamber can not be influenced by the shape and size of the calibrated coil. Meanwhile, the coil coefficients of each dimension are calibrated without being assembled and disassembled, so that the method has the advantages of simplicity in operation and good universality, and can be conveniently applied to coil coefficient determination of three-dimensional coils of the nuclear magnetic resonance gyroscope.
Drawings
FIG. 1 is a block diagram of the present invention;
FIGS. 2 and 3 are schematic views of an exemplary detection device;
FIGS. 4 and 5 are schematic diagrams illustrating effects of the embodiment;
in the figure: the device comprises a pump laser light source 1, a linear polarizer 2, a lambda/4 wavelength optical lens 3, a magnetic shielding cylinder 4, an x-axis Helmholtz coil 5, a y-axis Helmholtz coil 6, a cesium atom air chamber 7, a z-axis Helmholtz coil 8, a photoelectric detector 9 and a lock-in amplifier 10.
Detailed Description
As shown in fig. 1 to fig. 3, the present embodiment relates to a three-dimensional coil coefficient calibration apparatus based on optical pump nuclear magnetic resonance, including: set up pump laser light source 1, linear polarizer 2, lambda/4 wavelength optical lens 3 in proper order in magnetism shielding section of thick bamboo 4 side to and set up photoelectric detector 9 and lock-in amplifier 10 in proper order in magnetism shielding section of thick bamboo 4 side, wherein: three-dimensional Helmholtz coils 5, 6 and 8 are arranged in the center of a magnetic shielding cylinder 4 after being assembled from inside to outside, a cesium atom air chamber 7 is fixed in the center of the three-dimensional Helmholtz coils, laser generated by a pump laser light source 1 is sequentially converted into left-handed circularly polarized light through a linear polarizer 2 and a lambda/4 wavelength optical lens 3, and emergent light of the left-handed circularly polarized light which is transmitted to the cesium atom air chamber 7 in a space free light form is detected by a photoelectric detector 9 and demodulated by a phase-locked amplifier 10 to obtain the amplitude of a photoelectric signal.
The pump laser light source 1 is electrified to generate laser with the wavelength of 894.2 nm.
The linear polarizer 2 is used for converting the light generated at the pump laser light source 1 into linearly polarized light.
The lambda/4 wavelength optical lens 3 is used for converting the linearly polarized light after passing through the linear polarizer 2 into left circularly polarized light.
The magnetic shielding cylinder 4 is used for shielding the interference of an environmental magnetic field, and the coil calibration in the magnetic shielding cylinder is more accurate.
The Helmholtz coils 5, 6 and 8 are mutually perpendicular three-dimensional coils to be calibrated and can be used for generating a direct current or alternating current magnetic field.
The cesium atom gas chamber 7 is a square glass bubble, cesium atom gas and buffer gas are filled in the cesium atom gas chamber, and the size of the cesium atom gas chamber is 4 mm.
The photodetector 9 is used for receiving the light emitted from the cesium atom gas chamber 7 and converting the light into a voltage signal.
The lock-in amplifier 10 is used for demodulating the voltage signal output by the photodetector 9, and the lock-in amplifier 10 can obtain the amplitude of the specific frequency component signal from the complex signal.
The embodiment relates to a calibration method of the device, which comprises the following steps:
x-axis direction coil coefficient lambdaxCalibration:
1.1) polarization of cesium atoms in the x-direction by the pumping direction from a pump laser source 1, generating a magnetic field B parallel to the direction of the pump laser when a current is applied to a Helmholtz coil 5 of the x-axis parallel to the direction of the pump laser0＝IxλxWherein: i isxFor reading the value of the current applied to the coil 5 by means of a multimeter, lambdaxThe coil coefficients for the x-axis helmholtz coil. While applying a radio frequency magnetic field B on the y-axis helmholtz coil 6 (or z-axis helmholtz coil 8) perpendicular to the direction of the pump light1cosωt，Wherein the frequency omega of the radio frequency magnetic field is a determined value.
1.2) increasing the current I gradually from zeroxSo that the magnetic field parallel to the direction of the pump laser corresponds to B0Increasing until optical pump magnetic resonance occurs, wherein the intensity of transmitted light is modulated by cesium atoms at the frequency of the maximum amplitude of RF magnetic field frequency ω (γ B)0Wherein: gamma is the gyromagnetic ratio of cesium atoms. The sine wave detected by the photoelectric detector 9 is input into the phase-locked amplifier 10 and phase-locked by the reference signal with the frequency omega to obtain the amplitude of the signal, and I is adjustedxThe output of the phase-locked amplifier is maximized, and the current I corresponding to the maximum signal amplitude is searchedxmax. By using a multimeter to read the value of the current I applied to the coil 5 at that timexmaxCalculating to obtain corresponding coil coefficient
X coefficient of coil in y-axis directionyCalibration:
2.1) Pump laser light Source 1 emits a Pump Direction to polarize Cesium atoms in the x-direction while applying Current I to both the x-axis Helmholtz coil 5 and the y-axis Helmholtz coil 6x、IyThen two orthogonal magnetic field vector sums are generated
Wherein: current I applied to the coilx、IyRead out separately by a multimeter. At the time of being perpendicular to the magnetic field B0Is applied with a radio frequency magnetic field B on the planar z-axis Helmholtz coil 81cos ω t, the frequency ω of the RF magnetic field is set to a certain value.
2.2) constant Current IxWhile not changing, the current I is gradually increased from zeroyUntil the optical pump magnetic resonance phenomenon is generated, the light intensity of the transmitted light is modulated by the cesium atoms at the frequency with the maximum amplitude of the radio frequency magnetic field frequency omega, wherein omega is gamma B0Wherein: gamma is the gyromagnetic ratio of cesium atoms. The sine wave detected by the photoelectric detector 9 is input into the phase-locked amplifier 10 for useAnd the amplitude of the signal can be obtained by phase-locking the reference signal with the frequency omega. Regulation IyThe output of the phase-locked amplifier is maximized, and the current I corresponding to the maximum signal amplitude is searchedymax. By using a multimeter to read the value of the current I applied to the coil 6 at that timeymaxCombining the coil coefficient lambda obtained in the step IxCalculating to obtain corresponding coil coefficient
③ coil coefficient lambda in the z-axis directionzIs calibrated with lambdaySimilarly:
3.1) polarization of Cesium atoms in the X-direction in the pumping direction of the pump laser source 1, when a current I is applied to the X-direction coil 5 and the Z-direction coil 8 respectivelyx、IzThe magnitude of the magnetic field generated at this time is the sum of two orthogonal magnetic field vectors
Current I applied to the coilx、IzCan be read out separately by a multimeter. In a direction perpendicular to the magnetic field B0A radio frequency magnetic field B is applied to the planar y-direction coil1cos ω t, the frequency ω of the RF magnetic field is set to a certain value.
Setting the current I on the x-direction coil 5xIs a fixed value, and gradually increases the current I on the coil 8 in the z direction from zerozUntil the optical pump magnetic resonance phenomenon is generated, the light intensity of the transmitted light is modulated by the cesium atoms at the frequency with the maximum amplitude of the radio frequency magnetic field frequency omega, wherein omega is gamma B0Wherein: gamma is the gyromagnetic ratio of cesium atoms. The sine wave detected by the photodetector 9 is input to the lock-in amplifier 10 and is phase-locked by the reference signal with frequency omega to obtain the amplitude of the signal. Regulation IzThe output of the phase-locked amplifier is maximized, and the current I corresponding to the maximum signal amplitude is searchedzmax. The current applied to coil 8 at this time is read by using a multimeterFlow value IzmaxCombining the coil coefficient lambda obtained in the step IxCalculating to obtain corresponding coil coefficient
By mounting the device of fig. 1 on an optical bench, the atomic gas cell and its fixture are shown in fig. 2, and the coil and magnetic shield are shown in fig. 3. Through specific practical experiments, the coil coefficients of the three-dimensional coil obtained by the method are respectively as follows: lambda [ alpha ]x＝285.17nT/mA，λy＝350.26nT/mA，λz381.79 nT/mA. The phase-locked amplifier outputs the maximum output by adjusting the current on the corresponding coil, and a phase-locked output curve can be obtained by scanning the current value as shown in fig. 4 and 5, so as to find the current value corresponding to the output maximum point.
Compared with the prior art, the size of the cesium atom gas chamber of the sensitive substance used in the method is only 4mm square, and the calibration of the magnetic field generated by the center of the coil is more accurate.
The foregoing embodiments may be modified in many different ways by those skilled in the art without departing from the spirit and scope of the invention, which is defined by the appended claims and all changes that come within the meaning and range of equivalency of the claims are therefore intended to be embraced therein.
Claims (4)
1. A three-dimensional coil coefficient calibration method based on optical pump nuclear magnetic resonance is characterized in that an atomic glass air chamber filled with cesium atoms and buffer gas is arranged in the center of a three-dimensional coil, current is respectively applied to coils in any one or two directions in the three-dimensional coil to generate a direct current magnetic field, the atomic air chamber is irradiated by left-handed circularly polarized light, the irradiation direction of the circularly polarized light and the applied direct current magnetic field are in the same plane, a radio frequency magnetic field with fixed frequency is applied in the direction perpendicular to the direct current magnetic field and the plane of the circularly polarized light, the optical pump nuclear magnetic resonance state is achieved by adjusting the magnitude of the current, at the moment, the light penetrating through the atomic air chamber is subjected to the maximum modulation of the cesium atoms, the amplitude of emergent light is obtained after photoelectric conversion and demodulation are carried out, and when the current value corresponding to the maximum amplitude is obtained, the coil coefficient calibration is achieved.
2. The method for calibrating the three-dimensional coil coefficient based on the optical pumping nuclear magnetic resonance as claimed in claim 1, wherein the optical pumping nuclear magnetic resonance state is as follows: frequency omega ═ gamma B of radio frequency magnetic field0Wherein: gamma is the gyromagnetic ratio of cesium atoms, being a fixed constant, B0The field strength of the DC magnetic field and the field strength B of the radio frequency magnetic field1cosωt。
3. The method for calibrating the three-dimensional coil coefficient based on the optical pump nuclear magnetic resonance as claimed in claim 1, wherein the amplitude of the emergent light is obtained by performing photoelectric conversion and demodulation on the emergent light at the current value corresponding to the maximum amplitude, and when the amplitude is the maximum modulation point, the corresponding current value I satisfies ω ═ γ I λ, so as to obtain the coil coefficient λ of the coil in the corresponding direction.
4. The method for calibrating the three-dimensional coil coefficient based on the optical pump nuclear magnetic resonance as claimed in any one of claims 1 to 3, which is characterized by comprising the following steps:
x-axis direction coil coefficient lambdaxCalibration:
1.1) poling cesium atoms in the x-direction by the pumping direction from a pump laser source, and generating a magnetic field B parallel to the direction of the pump laser by applying a current to a Helmholtz coil of the x-axis parallel to the direction of the pump laser0＝IxλxWherein: i isxReading the current value of the current applied to the coil by means of a multimeter, lambdaxIs the coil coefficient of the x-axis Helmholtz coil, and applies a radio frequency magnetic field B on the y-axis Helmholtz coil or the z-axis Helmholtz coil perpendicular to the direction of the pumping light1cos ω t, where the radio frequency magnetic field frequency ω is a determined value;
1.2) increasing the current I gradually from zeroxSo that the magnetic field parallel to the direction of the pump laser corresponds to B0Increase until an optical pumping magnetic resonance phenomenon is generated, whichThe intensity of time-transmitted light is modulated by cesium atoms at the frequency of the maximum amplitude of RF magnetic field frequency omega, where omega is gamma B0Wherein: gamma is the gyromagnetic ratio of cesium atom, sine wave waveform obtained by detection of photoelectric detector is input into phase-locked amplifier and phase-locked with reference signal with frequency of omega to obtain amplitude of signal, and I is regulatedxThe output of the phase-locked amplifier is maximized, and the current I corresponding to the maximum signal amplitude is searchedxmaxReading the current value I applied to the coil at the moment by using a multimeterxmaxCalculating to obtain corresponding coil coefficient
X coefficient of coil in y-axis directionyCalibration:
2.1) polarization of Cs atoms in the x-direction in the pumping direction from the pump laser source, and applying a current I to the Helmholtz coil in the x-axis and Helmholtz coil in the y-axis simultaneouslyx、IyThen two orthogonal magnetic field vector sums are generated
Wherein: current I applied to the coilx、IyRead out separately by a multimeter, in this case perpendicular to the magnetic field B0Is applied with a radio frequency magnetic field B on a plane z-axis Helmholtz coil1cos omegat, setting the frequency omega of the radio frequency magnetic field as a determined value;
2.2) constant Current IxWhile not changing, the current I is gradually increased from zeroyUntil the optical pump magnetic resonance phenomenon is generated, the light intensity of the transmitted light is modulated by the cesium atoms at the frequency with the maximum amplitude of the radio frequency magnetic field frequency omega, wherein omega is gamma B0Wherein: gamma is the gyromagnetic ratio of cesium atom, sine wave waveform obtained by detection of photoelectric detector is input into phase-locked amplifier and phase-locked with reference signal with frequency of omega to obtain amplitude of signal, and I is regulatedyThe output of the phase-locked amplifier is maximized, and the current I corresponding to the maximum signal amplitude is searchedymaxReading the point by using a multimeterCurrent value applied to coil IymaxCombining the coil coefficient lambda obtained in the step IxCalculating to obtain corresponding coil coefficient
③ coil coefficient lambda in the z-axis directionzIs calibrated with lambdaySimilarly:
3.1) polarization of cesium atoms in the x-direction in the pumping direction from a pump laser source, when currents I are applied to the x-direction coil and the z-direction coil, respectivelyx、IzThe magnitude of the magnetic field generated at this time is the sum of two orthogonal magnetic field vectors
Current I applied to the coilx、IzCan be read out by a multimeter respectively and is perpendicular to the magnetic field B0A radio frequency magnetic field B is applied to the planar y-direction coil1cos omegat, setting the frequency omega of the radio frequency magnetic field as a determined value;
setting the current I on the x-direction coilxIs a fixed value, and gradually increases the current I on the coil in the z direction from zerozUntil the optical pump magnetic resonance phenomenon is generated, the light intensity of the transmitted light is modulated by the cesium atoms at the frequency with the maximum amplitude of the radio frequency magnetic field frequency omega, wherein omega is gamma B0Wherein: gamma is the gyromagnetic ratio of cesium atom, sine wave waveform obtained by detection of photoelectric detector is input into phase-locked amplifier and phase-locked with reference signal with frequency of omega to obtain amplitude of signal, and I is regulatedzThe output of the phase-locked amplifier is maximized, and the current I corresponding to the maximum signal amplitude is searchedzmaxReading the current value I applied to the coil at the moment by using a multimeterzmaxCombining the coil coefficient lambda obtained in the step IxCalculating to obtain corresponding coil coefficient
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202011590765.7A CN112816926B (en) | 2020-12-29 | 2020-12-29 | Three-dimensional coil coefficient calibration method based on optical pump nuclear magnetic resonance |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202011590765.7A CN112816926B (en) | 2020-12-29 | 2020-12-29 | Three-dimensional coil coefficient calibration method based on optical pump nuclear magnetic resonance |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN112816926A CN112816926A (en) | 2021-05-18 |
| CN112816926B true CN112816926B (en) | 2022-02-25 |
Family
ID=75854505
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN202011590765.7A Active CN112816926B (en) | 2020-12-29 | 2020-12-29 | Three-dimensional coil coefficient calibration method based on optical pump nuclear magnetic resonance |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN112816926B (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN113687278B (en) * | 2021-07-16 | 2023-12-01 | 兰州空间技术物理研究所 | Measuring device and method for sinusoidal alternating current based on quantum natural reference |
Family Cites Families (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7038450B2 (en) * | 2002-10-16 | 2006-05-02 | Trustees Of Princeton University | High sensitivity atomic magnetometer and methods for using same |
| US20050096534A1 (en) * | 2003-10-31 | 2005-05-05 | Yudong Zhu | Systems and methods for calibrating coil sensitivity profiles |
| CN108392195A (en) * | 2018-01-23 | 2018-08-14 | 上海交通大学 | Active magnetic protected type laser pump (ing) magnetometer for magnetocardiogram measurement |
| CN108919146A (en) * | 2018-04-20 | 2018-11-30 | 浙江大学 | A kind of Cs atom magnetometer |
| CN109827559B (en) * | 2019-03-21 | 2020-08-11 | 中国科学院武汉物理与数学研究所 | Nuclear magnetic resonance gyroscope device for improving atomic polarization uniformity |
| CN110426651B (en) * | 2019-06-17 | 2020-11-27 | 北京航空航天大学 | Three-dimensional in-situ magnetic coil calibration experimental device and method based on SERF magnetometer |
| CN110927635B (en) * | 2019-12-23 | 2021-06-22 | 北京航空航天大学 | Small magnetometer magnetic closed-loop control system based on extremely weak magnetic measurement and design method |
| CN112114279A (en) * | 2020-08-25 | 2020-12-22 | 北京航天控制仪器研究所 | Chip type high-precision triaxial vector atom magnetometer |
-
2020
- 2020-12-29 CN CN202011590765.7A patent/CN112816926B/en active Active
Also Published As
| Publication number | Publication date |
|---|---|
| CN112816926A (en) | 2021-05-18 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN109738837B (en) | Residual magnetic field in-situ compensation method for single-beam SERF atomic magnetometer | |
| CN108287322B (en) | Atomic magnetometer without response blind zone and method for measuring external magnetic field by atomic magnetometer | |
| CN106842074B (en) | Three axial vector atom magnetometers and application method based on longitudinal magnetic field modulation | |
| CN105301541B (en) | The measuring device and method of the magnetic coil X of atom magnetometer, Y-axis non-orthogonal angles | |
| Fang et al. | In situ triaxial magnetic field compensation for the spin-exchange-relaxation-free atomic magnetometer | |
| JP6222974B2 (en) | Optical pumping magnetometer and magnetic sensing method | |
| CN106886000B (en) | It is a kind of to realize the stable device and method of magnetic field amplitude using nuclear magnetic resonance | |
| CN108717168B (en) | Scalar magnetic field gradient measuring device and method based on light field amplitude modulation | |
| CN105929458A (en) | Aeromagnetic field vector detecting device and detecting method | |
| CN112924910B (en) | In-situ magnetometer-based method for measuring residual magnetism in shielding barrel | |
| CN103969604A (en) | Radio-frequency atom magnetometer and method for measuring nuclear magnetic resonance (NMR) signal by same | |
| CN107490775B (en) | Triaxial coil constant and non-orthogonal angle integrated measurement method | |
| CN109358302B (en) | Passive magnetic shielding-free atomic magnetometer device and magnetism measuring method | |
| CN107656219A (en) | A kind of rubidium atom magnetometer | |
| Zhang et al. | On-site synchronous determination of coil constant and nonorthogonal angle based on electron paramagnetic resonance | |
| CN112816926B (en) | Three-dimensional coil coefficient calibration method based on optical pump nuclear magnetic resonance | |
| Bai et al. | Research on an improved resonant cavity for overhauser geomagnetic sensor | |
| CN107656220A (en) | A kind of method based on rubidium atom magneto-optic rotation effect measurement magnetic field | |
| CN113447860A (en) | Residual magnetic field triaxial component in-situ measurement method under shielding environment | |
| Kernevez et al. | Weak field NMR and ESR spectrometers and magnetometers | |
| CN114089243B (en) | Vector atomic magnetometer device and method based on magnetic field rotation modulation method | |
| Li et al. | In situ simultaneous measurement of magnetic coil constants and nonorthogonal angles using atomic magnetometers | |
| CN114137448B (en) | Single-beam non-modulation type triaxial magnetic field measuring device and method | |
| Guo et al. | Active magnetic compensation based on parametric resonance magnetometer | |
| CN109613456A (en) | A kind of full optics atom magnetometer and method |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PB01 | Publication | ||
| PB01 | Publication | ||
| SE01 | Entry into force of request for substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| GR01 | Patent grant | ||
| GR01 | Patent grant |