CN109946628A - A method of separation magnetic field strength and magnetic field gradient influence high temperature optically pumped magnetometer line width - Google Patents

A method of separation magnetic field strength and magnetic field gradient influence high temperature optically pumped magnetometer line width Download PDF

Info

Publication number
CN109946628A
CN109946628A CN201910232031.2A CN201910232031A CN109946628A CN 109946628 A CN109946628 A CN 109946628A CN 201910232031 A CN201910232031 A CN 201910232031A CN 109946628 A CN109946628 A CN 109946628A
Authority
CN
China
Prior art keywords
magnetic field
line width
high temperature
optically pumped
pumped magnetometer
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.)
Pending
Application number
CN201910232031.2A
Other languages
Chinese (zh)
Inventor
周斌权
韩邦成
刘刚
尹彦
陆吉玺
吴文峰
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Beihang University
Original Assignee
Beihang University
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Beihang University filed Critical Beihang University
Priority to CN201910232031.2A priority Critical patent/CN109946628A/en
Publication of CN109946628A publication Critical patent/CN109946628A/en
Priority to CN201910806588.2A priority patent/CN110426654B/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/0023Electronic aspects, e.g. circuits for stimulation, evaluation, control; Treating the measured signals; calibration
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/02Measuring direction or magnitude of magnetic fields or magnetic flux
    • G01R33/032Measuring direction or magnitude of magnetic fields or magnetic flux using magneto-optic devices, e.g. Faraday or Cotton-Mouton effect

Landscapes

  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Measuring Magnetic Variables (AREA)

Abstract

The present invention provides a kind of separation magnetic field strength and the method that is influenced on high temperature optically pumped magnetometer line width of magnetic field gradient, wherein high temperature optically pumped magnetometer line width test device of the present invention, including high temperature optically pumped magnetometer system, tests coil, shields bucket, current source.High temperature optically pumped magnetometer system is placed in test coil central axes, and test coil is placed in shielding bucket and coaxial, and current source is used for test coil input current to generate controllable magnetic field.The formant line width generated in high temperature optically pumped magnetometer by magnetic fields can be tested using above-mentioned apparatus, line width finally characterizes magnetometer sensitivity.Since magnetic field strength has an impact line width by different mechanism from magnetic field gradient, influence of the two to it is separated by control variate method, the quantitative relationship that the two influences line width is finally obtained, is compared with theoretical formula.High temperature optically pumped magnetometer system model can be improved using the method, measure its gradient tolerance, while having positive effect to line width is narrowed to reach more highly sensitive.

Description

A kind of separation magnetic field strength and magnetic field gradient influence high temperature optically pumped magnetometer line width Method
Technical field
The present invention relates to magnetic survey technical fields, and in particular to a kind of high temperature optically pumped magnetometer system, and separation magnetic The method that field intensity and magnetic field gradient influence high temperature optically pumped magnetometer line width, adopting said method can improve high temperature optically pumped magnetometer System model measures its gradient tolerance, while having positive effect to line width is narrowed to reach more highly sensitive.
Background technique
Optically pumped magnetometer is utilized by the polarized high density hot atom of specific frequency circular polarization pumping light (about 140 DEG C), with It will do it Larmor precession under the consistent external magnetic field of pumping light direction, precession frequency ω and external magnetic field B are in a certain range It is interior directly proportional, ω=γ B.Applying a branch of linear polarization detection light perpendicular to pumping light direction, using Faraday effect come Detect the variation of atom assemblage.Applying transverse rotating magnetic field with external magnetic field vertical plane, when its speed and precession frequency It resonates when consistent, detected amplitude reaches maximum, to complete the purpose in measurement magnetic field.When magnetic field strength is larger, magnetic is total Vibration can be divided further inside peak, and the line width of whole magnetic resonance is caused to increase.Sensitive source hot atom is loaded in glass gas chamber, when When gas chamber is in gradient magnetic, due to the bulk of glass gas chamber cause not homoatomic assemblage experience field strength values not Unanimously, it is finally reflected when on formant, increases its line width.And when using test coil to simulate magnetic field to be measured, magnetic field Intensity can change simultaneously with magnetic field gradient, can not determine which factor leads to widening for magnetic resonance in the two.Therefore, in order to more High temperature optically pumped magnetometer system is accurately described, on the basis of existing high temperature optically pumped magnetometer test macro, needs to find one Kind can separate the method that magnetic field strength and magnetic field gradient influence high temperature optically pumped magnetometer line width.
Summary of the invention
It is an object of the invention to separate magnetic field strength and magnetic field gradient to influence high temperature optically pumped magnetometer line width, height is improved Warm optically pumped magnetometer system model.In addition, adopting said method can measure its its gradient tolerance, while to narrowing line width to reach It is more highly sensitive to have positive effect.
To achieve the goals above, The technical solution adopted by the invention is as follows:
A kind of high temperature optically pumped magnetometer line width test device, including high temperature optically pumped magnetometer system, test coil, shielding Bucket, current source.Wherein, high temperature optically pumped magnetometer system is located at test coil center, and test coil is located at front and back inside shielding bucket Concordant and coaxial, current source is located at outside, is connect between test coil with cable.
In above-mentioned high temperature optically pumped magnetometer line width test device, high temperature optically pumped magnetometer system uses and is heated to 140 DEG C high-temperature high-density K atom do sensitive source, sensitive direction is the direction z.
In above-mentioned high temperature optically pumped magnetometer line width test device, test coil forms not similar shape by copper conductor coiling Shape can be controlled by current source, generate the magnetic field of x, y, z direction varying strength, the uniformity.
In above-mentioned high temperature optically pumped magnetometer line width test device, shielding bucket is a kind of commonly used equipment, outer for shielding The external world can be greatly reduced to the interference of internal magnetic field strength and the interference of magnetic noise in ground magnetic environment in boundary simultaneously.
In above-mentioned high temperature optically pumped magnetometer line width test device, current source is a kind of commonly used equipment, output connection In test lead-out wires of coil, for supplying power for.
A method of separation magnetic field strength and magnetic field gradient influence high temperature optically pumped magnetometer line width, including walk as follows It is rapid:
(1) current source applies a constant current in test coil, and high temperature optically pumped magnetometer is placed in test coil central axes And mobile different location, test the magnetic field value and magnetic resonance line width at different location.It is fitted the 4 of out position and magnetic field strength Secondary curve.
(2) to Magnetic field strength curve figure derivation, 3 curve graphs of you can get it position and magnetic field gradient.
(3) change different current values, repeat step 1, obtain different magnetic field intensity, position curve figure.
(4) change different current values, repeat step 2, obtain different magnetic field gradient, position curve figure.
(5) magnetic field strength, position curve figure are indicated on same figure, and an auxiliary line is drawn at particular magnetic field strength value, Obtain itself and line width corresponding to the intersection point of different curves.This can obtain one timing of magnetic field strength, the pass of magnetic field gradient and line width It is formula.
(6) magnetic field gradient, position curve figure are indicated on same figure, and an auxiliary line is drawn at specific magnetic fields gradient value, Obtain itself and line width corresponding to the intersection point of different curves.This can obtain one timing of magnetic field gradient, the pass of magnetic field strength and line width It is formula.
Compared with prior art, the present invention having the following beneficial effects:
(1) method that separation magnetic field strength of the invention and magnetic field gradient influence high temperature optically pumped magnetometer line width, is passing On the basis of high temperature optically pumped magnetometer system of uniting, the magnetic field strength of different location on test coil central axes is surveyed with line width Amount, by obtaining magnetic field gradient position curve to curve derivation.It is compared to center magnetic field gradient in traditionally shielding bucket The reduction for being zero, can be more accurately perfect to model.
(2) method that separation magnetic field strength of the invention and magnetic field gradient influence high temperature optically pumped magnetometer line width, finally It can obtain the expression formula that magnetic field gradient influences line width, in conjunction with the physical size of sensitive source gas room, can finally obtain high temperature optical pumping The gradient tolerance of magnetometer system.
(3) method that separation magnetic field strength of the invention and magnetic field gradient influence high temperature optically pumped magnetometer line width, finally More accurately system model is obtained, based on this, bucking coil is superimposed on the basis of testing coil, optimizes sensitive source gas room The magnetic field gradient of present position narrows line width, promotes sensitivity.
Detailed description of the invention
Fig. 1 be high temperature optically pumped magnetometer line width test device of the invention, wherein 1 be high temperature optically pumped magnetometer system, 2 To test coil, 3 be shielding bucket, and 4 be current source, and 5 be support plate.
Fig. 2 is relevant high temperature optically pumped magnetometer system schematic in the present invention.
Fig. 3 is magnetic field strength and positional diagram of the invention.
Fig. 4 is magnetic field gradient and positional diagram of the invention.
Specific embodiment
The present invention is further described in detail with reference to the accompanying drawing:
As shown in Figure 1, high temperature optically pumped magnetometer line width test device of the invention, including high temperature optically pumped magnetometer system 1, Test coil 2, shielding bucket 3, current source 4.Wherein, high temperature optically pumped magnetometer system 1 is located at 2 center of test coil, tests coil 2 Concordant and coaxial positioned at 3 inside front and back of shielding bucket, current source 4 is located at outside, is connect between test coil 2 with cable.
As shown in Fig. 2, the high temperature optically pumped magnetometer system 1 done using the high-temperature high-density K atom for being heated to 140 DEG C it is quick Sense source, sensitive direction are the direction z.It include that conventional important component has: laser source, lens group, excitation coil, heating in the system Device, electronic measurement and control and data acquisition device.Laser source chooses energy level transition D1 line or D2 line, i.e. wavelength corresponding to K atom For 770.7nm or 766.7nm.Lens group is for changing the polarizability and stability for passing through light, to reach necessary requirement.Excitation Coil is the executing agency of rotating excitation field.Heating device is for measuring and stablizing gas chamber temperature.When by scanning transverse rotation magnetic When field frequencies range, at the Frequency point consistent with Larmor precession frequency, magnetometer output signal is reinforced, and it is total that an envelope is integrally formed Shake peak, so as to complete the conversion measured from magnetic field signal to formant line width.
The test coil 2 forms different shape by copper conductor coiling, is controlled by current source 4, generates x, y, z direction not The magnetic field of same intensity, the uniformity.9449 coils are generally used, the uniformity in coil center is relatively high, with offset from center, Field strength values increase in 4 powers, therefore its magnetic field gradient value changes in 3 powers.The coil constant of used test coil is about 500nT/mA。
In above-mentioned high temperature optically pumped magnetometer line width test device, shielding bucket 3 is a kind of commonly used equipment, outer for shielding The external world can be greatly reduced to the interference of internal magnetic field strength and the interference of magnetic noise in ground magnetic environment in boundary simultaneously.Shielding used Bucket shields bucket for 4 layers of permalloy, and armoured magnetic field decay factor is 10-5, internal diameter 40cm has sufficiently large space to load Coil 2 and high temperature optically pumped magnetometer 1 are tested, while can guarantee that there is certain field homogeneity area in coil center.
In above-mentioned high temperature optically pumped magnetometer line width test device, current source 4 is a kind of commonly used equipment, output connection In test 2 lead-out wire of coil, for supplying power for.Current source used is the LDC205C of Thorlabs company.
Using high temperature optically pumped magnetometer line width test device of the present invention, separation magnetic field strength and magnetic field gradient are realized On the method that high temperature optically pumped magnetometer line width influences, as shown in Figure 1, including the following steps:
1) current source applies a constant current in test coil, and high temperature optically pumped magnetometer is placed in test coil central axes simultaneously Mobile different location tests magnetic field value and magnetic resonance line width at different location.It is fitted 4 times of out position and magnetic field strength Curve.
2) to Magnetic field strength curve figure derivation, 3 curve graphs of you can get it position and magnetic field gradient.
3) change different current values, repeat step 1, obtain different magnetic field intensity, position curve figure.
4) change different current values, repeat step 2, obtain different magnetic field gradient, position curve figure.
5) magnetic field strength, position curve figure are indicated on same figure, an auxiliary line are drawn at particular magnetic field strength value, such as Shown in Fig. 3, itself and line width corresponding to the intersection point of different curves are obtained.This can obtain the timing of magnetic field strength one, magnetic field gradient with The relational expression of line width.Simulation curve expression formula in Fig. 3 are as follows:
Y (n)=nx4+2(n-1)
Wherein, y indicates magnetic field strength, and x indicates position, and n is Curve numberings.Particular magnetic field strength chooses 10, and corresponding 4 are not Same position, line width herein are influenced by magnetic field gradient completely, are no longer influenced by magnetic field strength.
6) magnetic field gradient, position curve figure are indicated on same figure, an auxiliary line are drawn at specific magnetic fields gradient value, such as Shown in Fig. 4, itself and line width corresponding to the intersection point of different curves are obtained.This can obtain the timing of magnetic field gradient one, magnetic field strength with The relational expression of line width.Simulation curve expression formula in Fig. 4 are as follows:
Z (n)=4nx3
Wherein, z indicates that magnetic field gradient, x indicate position, and n is Curve numberings.Specific magnetic fields gradient chooses 30, and corresponding 4 are not Same position, line width herein are influenced by magnetic field strength completely, are no longer influenced by magnetic field gradient.
The foregoing is merely a specific implementation methods of the invention, but protection scope of the present invention is not limited to This, any related personnel for being familiar with the art in the technical scope disclosed by the present invention, the variation that can readily occur in or Person's replacement, should all cover within protection scope of the present invention.
The content that description in the present invention is not described in detail belongs to the well-known technique of professional and technical personnel in the field.

Claims (6)

1. a kind of high temperature optically pumped magnetometer line width test device, it is characterised in that: including high temperature optically pumped magnetometer system (1), survey Try coil (2), shielding bucket (3) and current source (4), wherein high temperature optically pumped magnetometer system (1) is located at test coil (2) center, It tests coil (2) and is located at that the internal front and back of shielding bucket (3) is concordant and coaxial, and current source (4) is located at outside, between test coil (2) It is connected with cable.
2. a kind of high temperature optically pumped magnetometer line width test device as described in claim 1, it is characterised in that: the high temperature optical pumping Magnetometer system (1) does sensitive source using the high-temperature high-density K atom for being heated to 140 DEG C, and sensitive direction is the direction z.
3. a kind of high temperature optically pumped magnetometer line width test device as described in claim 1, it is characterised in that: the test coil (2) different shape is formed by copper conductor coiling, can be controlled by current source (4), generate x, y, z direction varying strength, the uniformity Magnetic field.
4. a kind of high temperature optically pumped magnetometer line width test device as described in claim 1, it is characterised in that: the shielding bucket (3) it is a kind of commonly used equipment, for shielding extraneous ground magnetic environment, the external world can be greatly reduced simultaneously, internal magnetic field strength is done Disturb the interference with magnetic noise.
5. a kind of high temperature optically pumped magnetometer line width test device as described in claim 1, it is characterised in that: the current source It (4) is a kind of commonly used equipment, output is connected to test coil (2) lead-out wire, for supplying power for.
6. a kind of method that separation magnetic field strength and magnetic field gradient influence high temperature optically pumped magnetometer line width, it is characterised in that: packet Include following steps:
1) current source applies a constant current in test coil, and high temperature optically pumped magnetometer is placed in test coil central axes and movement Different location tests magnetic field value and magnetic resonance line width at different location, is fitted 4 songs of out position and magnetic field strength Line;
2) to Magnetic field strength curve figure derivation, 3 curve graphs of you can get it position and magnetic field gradient;
3) change different current values, repeat step 1, obtain different magnetic field intensity, position curve figure;
4) change different current values, repeat step 2, obtain different magnetic field gradient, position curve figure;
5) magnetic field strength, position curve figure are indicated on same figure, and an auxiliary line is drawn at particular magnetic field strength value, obtains it From line width corresponding to the intersection point of different curves, this can obtain one timing of magnetic field strength, the relational expression of magnetic field gradient and line width;
6) magnetic field gradient, position curve figure are indicated on same figure, and an auxiliary line is drawn at specific magnetic fields gradient value, obtains it From line width corresponding to the intersection point of different curves, this can obtain one timing of magnetic field gradient, the relational expression of magnetic field strength and line width.
CN201910232031.2A 2019-03-26 2019-03-26 A method of separation magnetic field strength and magnetic field gradient influence high temperature optically pumped magnetometer line width Pending CN109946628A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
CN201910232031.2A CN109946628A (en) 2019-03-26 2019-03-26 A method of separation magnetic field strength and magnetic field gradient influence high temperature optically pumped magnetometer line width
CN201910806588.2A CN110426654B (en) 2019-03-26 2019-08-29 Method for separating influence of magnetic field intensity and magnetic field gradient on line width of high-temperature optical pump magnetometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201910232031.2A CN109946628A (en) 2019-03-26 2019-03-26 A method of separation magnetic field strength and magnetic field gradient influence high temperature optically pumped magnetometer line width

Publications (1)

Publication Number Publication Date
CN109946628A true CN109946628A (en) 2019-06-28

Family

ID=67010747

Family Applications (2)

Application Number Title Priority Date Filing Date
CN201910232031.2A Pending CN109946628A (en) 2019-03-26 2019-03-26 A method of separation magnetic field strength and magnetic field gradient influence high temperature optically pumped magnetometer line width
CN201910806588.2A Active CN110426654B (en) 2019-03-26 2019-08-29 Method for separating influence of magnetic field intensity and magnetic field gradient on line width of high-temperature optical pump magnetometer

Family Applications After (1)

Application Number Title Priority Date Filing Date
CN201910806588.2A Active CN110426654B (en) 2019-03-26 2019-08-29 Method for separating influence of magnetic field intensity and magnetic field gradient on line width of high-temperature optical pump magnetometer

Country Status (1)

Country Link
CN (2) CN109946628A (en)

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103033786B (en) * 2011-10-08 2015-07-08 中国科学院空间科学与应用研究中心 Quadrature calibration method and device of triaxial vector magnetometer
CN203799001U (en) * 2014-02-28 2014-08-27 中国船舶重工集团公司第七一〇研究所 Dual uniform zone type magnetic field gradient magnetometer calibration device
CN103885019B (en) * 2014-02-28 2016-05-04 中国船舶重工集团公司第七一〇研究所 For two homogeneity range type magnetic field generation devices and the calibration steps of magnetometer calibration
CN104730484B (en) * 2015-03-23 2017-06-16 东南大学 A kind of decision method of atomic spin magnetometer SERF states
CN106872917B (en) * 2017-03-03 2019-08-23 电子科技大学 It is a kind of test magnetic material ferromagnetic resonance line width face in distribution method and system

Also Published As

Publication number Publication date
CN110426654A (en) 2019-11-08
CN110426654B (en) 2020-11-24

Similar Documents

Publication Publication Date Title
CN106405457B (en) A kind of device and method detected for material ferromagnetism and magnetization property
CN105651649A (en) Real-time online atomic density measuring method suitable for atom magnetometer
CN108717168B (en) Scalar magnetic field gradient measuring device and method based on light field amplitude modulation
CN107192633A (en) Under a kind of SERF states in on-line measurement atom magnetometer air chamber alkali metal density method
CN106872917B (en) It is a kind of test magnetic material ferromagnetic resonance line width face in distribution method and system
CN108776356A (en) The design method of Transient electromagnetic measure device
CN109358302B (en) Passive magnetic shielding-free atomic magnetometer device and magnetism measuring method
Bai et al. Research on an improved resonant cavity for overhauser geomagnetic sensor
CN107656219A (en) A kind of rubidium atom magnetometer
Ma et al. A novel low-noise Mu-metal magnetic shield with winding shape
CN106772180B (en) A kind of optical pumped magnetometer gradient tolerance measuring device
Yang et al. Improved measurement of the low-frequency complex permeability of ferrite annulus for low-noise magnetic shielding
Gao et al. A low-noise multilayer mu-metal thin shell magnetic shield for ultra-highly sensitive atomic sensors
US7315168B2 (en) Shimming with MRI gradient
CN107656220A (en) A kind of method based on rubidium atom magneto-optic rotation effect measurement magnetic field
CN108534770B (en) A kind of129Xe-Rb spin exchange rate rapid measurement method
CN109061318B (en) Magnetic shielding effectiveness measuring method and system
CN105896237B (en) A kind of axial magnetic field adjustment device and method of adjustment in optical pumping pump apparatus
CN109686552B (en) Voltage transformer based on rydberg atomic stark effect
CN110426654A (en) A method of separation magnetic field strength and magnetic field gradient influence high temperature optically pumped magnetometer line width
CN115718273B (en) Device for measuring object magnetic susceptibility based on magnetic induction intensity and measuring method thereof
Wang et al. A time-domain feedback calibration method for air-coil magnetic sensor
Shen et al. Investigation of the eddy current effect on the high frequency response of the Mirnov probe on J-TEXT
CN112816928A (en) On-site calibration device of magnetic shielding device and on-site testing method of shielding effectiveness of on-site calibration device
Dinale Magnetic Test Facility-Sensor and Coil Calibrations.

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
WD01 Invention patent application deemed withdrawn after publication
WD01 Invention patent application deemed withdrawn after publication

Application publication date: 20190628