WO2020051924A1 - Détecteur magnétique de roche de type à balayage à réseau tmr - Google Patents

Détecteur magnétique de roche de type à balayage à réseau tmr Download PDF

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Publication number
WO2020051924A1
WO2020051924A1 PCT/CN2018/105903 CN2018105903W WO2020051924A1 WO 2020051924 A1 WO2020051924 A1 WO 2020051924A1 CN 2018105903 W CN2018105903 W CN 2018105903W WO 2020051924 A1 WO2020051924 A1 WO 2020051924A1
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tmr
sample
magnetic
demagnetization
rock
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PCT/CN2018/105903
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English (en)
Chinese (zh)
Inventor
刘双迟
秦华峰
刘青松
李金华
潘永信
朱日祥
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中国科学院地质与地球物理研究所
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Publication of WO2020051924A1 publication Critical patent/WO2020051924A1/fr

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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/12Measuring magnetic properties of articles or specimens of solids or fluids

Definitions

  • the invention relates to the technical field of magnetic measurement, in particular to a TMR array scanning type rock magnetic detector.
  • Rock contains magnetic minerals, and its magnetic properties are of great significance in geological research.
  • a special mineral using its type, particle size, and content information, it can sensitively track a variety of geological and environmental processes, such as mineral generation, migration, and transformation processes (called environmental magnetism).
  • magnetic minerals can be oriented in a geomagnetic field environment. The geomagnetic field at that time is recorded by mechanisms such as thermal remanence (volcanic rocks) and sedimentary remanence (sedimentary rocks or sediments). Information can restore the information of the geomagnetic field at that time (called paleomagnetism). Therefore, the magnetic properties of rocks can be widely used to study geological structure and environmental evolution, petroleum and mineral exploration, deep earth dynamics, sedimentary sequence dating, and archeology.
  • Paleomagnetic research generally uses superconducting magnetometers, rotating magnetometers, vibrating sample magnetometers, and variable gradient magnetometers to measure the magnetic properties of rock samples. These systems measure the residual magnetism carried by the entire rock sample, which is the superposition of information of all magnetic particles in the sample, but cannot distinguish and extract the information of a single magnetic particle in the sample. With the deepening of the research, in practical applications, we need to know exactly the spatial distribution of magnetic particles and the particle size distribution characteristics of magnetic particles in the sample at the micron level.
  • the distribution pattern of magnetic particles in meteorites carries rich meteorite evolution information; stalagmites and deep-sea manganese stones have lower deposition rates. If it can recognize the magnetism at the micron level, it can construct high-precision environmental evolution information, which will greatly promote the development of related disciplines, which has important scientific significance.
  • the magnetic field scanning technology came into being, which can sensitively measure the magnetic field distribution on the surface of rock samples, and further calculate the distribution characteristics of magnetic particles in the rock.
  • the residual magnetism of the entire sample can also be calculated statistically.
  • the superconducting technology is expensive; the second is limited by the need to equip a low temperature system, and the probe must be separated from the sample by a distance to reduce its spatial resolution.
  • TMR (TunnelMagnetoResistance) element is a new type of magnetoresistance effect sensor that has begun industrial applications in recent years. It uses the tunnel magnetoresistance effect of magnetic multilayer film materials to induce magnetic fields, which is more than previously discovered and practically applied.
  • AMR (Anisotropic Magneto Resistance) and GMR (Giant Magneto Resistance) elements have greater resistance change rates.
  • TMR element has better temperature stability, higher sensitivity, lower power consumption, better linearity than Hall element, and does not require additional magnetic ring structure; better temperature than AMR element Stability, higher sensitivity, wider linear range, no need for additional set / reset coil structure; better temperature stability, higher sensitivity, lower power consumption, wider Linear range. Based on the above advantages, this sensor has begun to be gradually applied to high-precision technology fields such as information technology, automotive electronics, and biomedicine.
  • the general rock magnetic scanning system can only measure the surface magnetism, and does not have the function of in-situ magnetization and demagnetization of the sample.
  • the sample needs to be taken out of the magnetic shielding room and processed by a special magnetization and demagnetization device. After putting it back into the scanning system, it is difficult to ensure that the rocks are placed in the same position before and after the processing, which is not conducive to comparing the magnetic distribution before and after.
  • the technical problem to be solved by the present invention is to provide a TMR array scanning type rock magnetic detector for one or more of the defects in the prior art.
  • the present invention provides a TMR array scanning rock magnetic detector, including:
  • a sample positioning system includes a three-dimensional sample moving stage for placing a rock specimen, and a sample stage controller for adjusting the position of the three-dimensional sample moving stage; a sample support rod is provided on the three-dimensional sample moving stage;
  • a TMR magnetic field detection system includes a TMR probe array and a TMR circuit for driving the TMR probe array for magnetic field detection;
  • Magnetization demagnetization system including a magnetization demagnetization coil set outside a rock specimen, and a coil control circuit connected thereto;
  • a data processing control system which is connected to the TMR circuit, the coil control circuit, and the sample stage controller, and is used to accept user input and send TMR scanning instructions, magnetization or demagnetization instructions, and sample stage movement instructions to the TMR circuit, coil control, respectively. Circuit and sample stage controller.
  • the coil control circuit includes:
  • a pulse power supply connected to the data processing control system through a data acquisition card, and configured to generate a magnetization pulse current corresponding to a current intensity according to a magnetization instruction issued by the data processing control system;
  • a signal source connected to the data processing control system, and configured to generate a sine wave demagnetizing electrical signal of a corresponding frequency according to a demagnetization instruction issued by the data processing control system;
  • a power amplifier connected to the signal source and configured to amplify the sine wave demagnetized electrical signal generated by the signal source to a corresponding amplitude and output;
  • a switch is connected to the pulse power source and the power amplifier, and is used to switch the magnetization pulse current or the amplified sine wave demagnetization electric signal to the magnetization demagnetization coil to generate a magnetic field of a predetermined strength, and to perform the function of switching magnetization or demagnetization the goal of.
  • the three-dimensional sample moving stage is provided with a stepping motor and a grating scale displacement sensor;
  • the sample stage controller includes: a motor controller, connected to the data processing control system, for receiving a movement command of the sample stage to generate a motor control signal, and using the position information fed back by the grating scale displacement sensor to implement closed-loop control.
  • the positioning of the sample support rod a motor driver connected to the motor controller and configured to receive a motor control electrical signal and generate a driving signal to the stepper motor.
  • the sample supporting rods are horizontally arranged; there are three stepping motors, which are respectively used to control the sample supporting rods to move in three dimensions. .
  • the length of the sample support rod is 30 cm to 100 cm.
  • the three-dimensional sample moving stage and the sample support rod are made of non-magnetic materials.
  • the stepping motor is a piezoelectric ceramic ultrasonic motor.
  • the TMR probe array, the three-dimensional sample moving stage, and the magnetization demagnetization coil are all placed in a magnetic shielding room.
  • the TMR array scanning type rock magnetic detector further includes a TMR probe array and a sample support rod that are sleeved outside the TMR probe array and the sample support rod during magnetic field detection.
  • Magnetic shielding cylinder the magnetic shielding chamber is used to shield the internal magnetic field to 100nT and below; the magnetic shielding cylinder is used to shield the internal magnetic field to 10nT and below.
  • the implementation of the TMR array scanning rock magnetic detector of the present invention has the following beneficial effects:
  • the present invention uses the TMR sensor array and a mobile platform to construct the TMR array scanning rock magnetic detector, which can realize high-precision and high-resolution magnetic scanning of rock specimens.
  • a special magnetization demagnetization system is set up to perform in-situ magnetization and demagnetization without moving the rock specimen, which is convenient for comparing the magnetic distribution before and after.
  • FIG. 1 is a schematic structural diagram of a TMR array scanning rock magnetic detector according to a first embodiment of the present invention
  • FIG. 2 is a schematic structural diagram of a TMR array scanning rock magnetic detector according to a second embodiment of the present invention.
  • FIG. 3 is a schematic diagram of a magnetizing circuit in a TMR array scanning rock magnetic detector according to a second embodiment of the present invention.
  • FIG. 4 is a schematic diagram of a demagnetization circuit in a TMR array scanning rock magnetic detector according to a second embodiment of the present invention.
  • FIG. 5 is a schematic structural diagram of a magnetization demagnetization coil in a TMR array scanning rock magnetic detector according to a second embodiment of the present invention.
  • FIG. 6 is a schematic structural diagram of a three-dimensional sample moving stage in a TMR array scanning rock magnetic detector according to the present invention.
  • FIG. 1 is a schematic structural diagram of a TMR array scanning rock magnetic detector according to a first embodiment of the present invention.
  • the TMR array scanning rock magnetic detector provided in this embodiment includes at least: a sample positioning system, a TMR magnetic field detection system, a magnetization demagnetization system, and a data processing control system.
  • the sample positioning system includes a three-dimensional sample moving stage 10 for placing a rock specimen 1, and a sample stage controller 20 for adjusting the position of the three-dimensional sample moving stage 10.
  • the three-dimensional sample moving stage is provided with a sample support rod 11 for placing a rock specimen 1.
  • the TMR magnetic field detection system includes a TMR probe array 30 and a TMR circuit 40 for driving the TMR probe array 30 for magnetic field detection.
  • the number of TMR sensors in the TMR probe array 30 is n * n.
  • the magnetization demagnetization system includes a magnetization demagnetization coil 50 sleeved outside the rock specimen 30 and a coil control circuit 60 connected to the magnetization demagnetization coil 50.
  • the data processing control system 70 is connected to the TMR circuit 40, the coil control circuit 60, and the sample stage controller 20, and is used to accept user input and send TMR scan instructions, magnetization or demagnetization instructions, and sample stage movement instructions to the TMR circuit 40, coil control, respectively. Circuit 60 and sample stage controller 20.
  • the data processing control system 70 can be implemented by, for example, a computer.
  • FIG. 2 is a schematic structural diagram of a TMR array scanning rock magnetic detector according to a second embodiment of the present invention. As shown in FIG. 2, on the basis of the first embodiment, a specific implementation manner of each system is provided.
  • the TMR circuit 40 includes a TMR controller 41 and a preamplifier 42.
  • the TMR controller 41 is connected to the data processing control system 70 through a data acquisition card 71, and is configured to receive a TMR scan instruction issued by the data processing control system 70 and generate a TMR control signal.
  • the preamplifier 42 is connected to the TMR controller 41 and is used to amplify and filter the TMR control signal and output a voltage proportional to the magnetic field signal to the TMR probe array 30.
  • the TMR probe array 30 in the present invention may be selected from a plurality of TMR sensors and arranged in a matrix.
  • the TMR sensor has a linear measurement range of ⁇ 50Oe, a magnetic field resolution of 2nT / Hz 1/2 @ 100Hz, and a measurement area of 1 ⁇ 2 microns, which is very suitable for scanning weak magnetic samples.
  • This TMR sensor will form a TMR matrix with a total of 16 sensors arranged in a matrix of 4 ⁇ 4.
  • the collection of array data can accelerate the measurement speed and achieve spatial resolution on the micrometer scale.
  • the preamplifier 42 can use a power supply with noise attenuation of more than 100 dB to reduce noise.
  • the coil control circuit 60 includes a pulse power source 61, a signal source 62, a power amplifier 63, and a circuit breaker 64.
  • the pulse power source 61 is connected to the data processing control system 70 through the data acquisition card 71, and is configured to generate a magnetized pulse current corresponding to the current intensity according to the magnetization instruction issued by the data processing control system 70.
  • FIG. 3 is a schematic diagram of a magnetizing circuit in a TMR array scanning rock magnetic detector according to a second embodiment of the present invention.
  • the pulse magnetization of the present invention can use a capacitor discharge pulse magnetization technique. Pulse power supply, the maximum voltage can reach 1500V, charge the internal capacitor balance current, the current is 1-1.5A, the magnetization demagnetizing coil inductance is 32.4mH, the resistance is 1.727ohm, when the capacitance value is 300 ⁇ F, the capacitor can be charged to 1300V.
  • the pulse power supply can have four signal interfaces, as shown in the figure:
  • Analog voltage input used to set the voltage across the capacitor. When the capacitor voltage reaches the set value, the hardware turns off the charging circuit;
  • Analog voltage output the voltage sensor returns the voltage across the capacitor to the data acquisition card 71;
  • the signal source 62 is connected to the data processing control system 70, and is configured to generate a sine wave demagnetizing electrical signal with a corresponding frequency according to a demagnetization instruction issued by the data processing control system 70.
  • the power amplifier 63 is connected to the signal source 62 and is used to amplify the sine wave demagnetized electrical signal generated by the signal source 62 to a corresponding amplitude and output.
  • FIG. 4 is a schematic diagram of a demagnetization circuit in a TMR array scanning rock magnetic detector according to a second embodiment of the present invention.
  • the AC demagnetization field uses a signal source 62 and a power amplifier 63 to drive the magnetization demagnetization coil.
  • the signal source 62 is realized by a single-chip microcomputer 622 and an AD9854 chip 621, and the output frequency is 400 Hz, and the voltage amplitude decreases linearly with a sine wave (the magnetic field 200mT is attenuated to 0mT).
  • the single-chip microcomputer 622 communicates with the computer 72 through the RS232 serial port and waits for the computer's demagnetization instruction.
  • the demagnetization instruction set by the PC can change the amplitude and frequency of the output signal, and the output instruction control signal source 62 outputs a signal to the power amplifier for demagnetization.
  • an audio power amplifier 631 can be used as the power amplifier.
  • the professional amplifier CA20 of commercial sound precision company is used, 8ohm stereo power is 1300w, 4ohm stereo power is 2000w, and 2ohm stereo power is 2600w.
  • a maximum current of 36A can be achieved with a 2ohm load.
  • the maximum voltage calculated by 8ohm can reach 102V.
  • AD9854DDS chip can output sine wave with adjustable frequency, phase and amplitude.
  • 32-bit frequency control word, frequency accuracy can reach 0.0466Hz
  • 14-bit amplitude control word 21A maximum current (200mT magnetic field)
  • control accuracy can reach 0.0013A (12.2 ⁇ T).
  • the frequency of demagnetization is selected as 400Hz.
  • the resistance of the magnetization demagnetization coil 50 is affected by the proximity effect and becomes 2.499ohm. Due to the presence of the inductance, the impedance of the entire load is very large.
  • Use capacitors for tuning For resistance only, tuning is performed with CBB capacitors in series and parallel. The tuning capacitor is 1.221 ⁇ F.
  • the switch 64 is connected to the pulse power source 61 and the power amplifier 63, and is used to switch the magnetization pulse current or the amplified sine wave demagnetization electric signal to the magnetization demagnetization coil 50 to generate a magnetic field of a predetermined strength and to perform the function of switching the magnetization and demagnetization. purpose.
  • pulse power source 61 the pulse power source 61
  • the signal source 62 the signal source 62
  • the power amplifier 63 the power amplifier 63 that can be applied in the prior art.
  • FIG. 5 is a schematic structural diagram of a magnetization demagnetization coil in a TMR array scanning rock magnetic detector according to a second embodiment of the present invention.
  • the measurement of saturated isothermal remanence requires magnetization and demagnetization of the sample, and the TMR probe array is used to measure the remanence signal of the rock specimen.
  • This part mainly includes the design of DC magnetizing magnetic field coil and alternating magnetic field coil, so that the generated magnetic field has high uniformity and resolution.
  • the manufactured magnetized demagnetizing coil is placed on a coil bobbin, and the coil bobbin may be epoxy material. Rock specimens are placed in the internal cavity of the magnetized demagnetization coil.
  • the sample positioning system of the present invention can realize three-dimensional precise movement and positioning of a sample.
  • the three-dimensional sample moving stage 10 is provided with a stepping motor 13 and a scale displacement sensor 14.
  • the sample stage controller 20 further includes a motor controller 21 and a motor driver 22.
  • the motor controller 21 is connected to the data processing control system 70, and is used to receive the sample table movement instruction to generate a motor control signal, and use the position information fed back by the scale displacement sensor 14 to implement closed-loop control of the movement positioning of the rock specimen on the sample support rod 11.
  • the motor driver 22 is connected to the motor controller 21, and is used for receiving a motor control signal and generating a driving electric signal to the stepping motor 13.
  • the three-dimensional movement and positioning of the three-dimensional sample moving stage 10 are realized by three stepping motors 13 respectively.
  • the stepping motor 13 is preferably a piezoelectric ceramic ultrasonic motor to reduce the residual magnetism of the motor itself.
  • the motor driver of the piezoelectric ceramic ultrasonic motor can be an AB1A driver.
  • the motor driver receives an analog signal instruction of +/- 10V from the motor controller and converts the control signal into an AC voltage to drive the motor.
  • the motor controller 21 uses the motion control card DMC 18X2, and the DMC18X2 control card is directly inserted into the PCI card slot of the computer. These two control cards can control 1-4 axes respectively, which can meet the control requirements of the three-dimensional mobile platform . It can provide +/- 10V analog signal command for standard servo system.
  • the design and production of the rock specimen rack of the present invention requires that the sample support rod 11 be non-magnetic material and is very close to the superconducting receiving coil of the TMR probe array, so as to reduce the attenuation loss of the residual magnetic signal of the rock specimen.
  • the invention can realize accurate X-Y-Z three-dimensional movement of the sample, and realize the residual magnetic measurement and scanning imaging of the biological sample. Mobile resolution: 20nm, mobile accuracy: 100nm.
  • both the three-dimensional sample moving stage 10 and the sample support rod 11 are made of non-magnetic material. Such as ceramics, organic plastics, quartz glass and so on.
  • the TMR probe array 30, the three-dimensional sample moving stage 10, and the magnetized demagnetizing coil 50 of the present invention are all placed in a magnetic shielding room 9.
  • the invention designs a special magnetic shielding room 9 to provide a zero magnetic field space experimental environment for the entire system, and realize shielding of the ambient static magnetic field and alternating magnetic field.
  • a high-permeability material is used to build a square shielded chamber, which can sufficiently accommodate the rock specimen magnetic detection system, experimental samples and experimental operators.
  • the internal magnetic field of the magnetically shielded chamber 9 constructed by the present invention is a high-standard zero magnetic space below 100 nT and a uniform area lower than 50 nT, which can provide an excellent test environment for the magnetic detection and analyzer of the scanning TMR array rock specimen.
  • the present invention further includes a magnetic shielding tube 8 sleeved outside the TMR probe array 30 and the sample support rod 11 during magnetic field detection.
  • This magnetic shield cylinder 8 is used only when detecting the magnetic field of the rock sample 1, and is withdrawn when it is demagnetized.
  • the above magnetic shielding room 9 is used to shield the internal magnetic field to 100nT and below, which removes the interference of the surrounding environment on the test; magnetic shielding, 8 is used to shield the internal magnetic field to 10nT and below, which can reduce the background magnetic field of the test more low.
  • FIG. 6 is a schematic structural diagram of a three-dimensional sample moving stage of a TMR array scanning rock magnetic detector according to the present invention.
  • the three-dimensional sample moving stage 10 is composed of a three-dimensional moving mechanism, and a horizontal sample supporting rod 12 is provided above.
  • the horizontal sample support rod 12 has a length of 50 cm to 70 cm.
  • the horizontal sample support rod 12 larger than 50cm can reduce the influence of the motor itself and the magnetic field generated during the movement on the measurement.
  • the TMR array scanning rock magnetic detector of the present invention can achieve the following technical indicators:
  • Magnetization field strength 0-1T, uniformity ⁇ 2%;
  • Demagnetization intensity 0-0.3T, uniformity ⁇ 2%;
  • Magnetic shielding index of test area 0-5 ⁇ 10-8T.
  • the TMR array scanning rock magnetic detector of the present invention has the following characteristics:
  • the present invention provides a scanning rock specimen magnetic detection and analyzer with in-situ magnetization and demagnetization functions.
  • a scanning rock specimen magnetic detection and analyzer with in-situ magnetization and demagnetization functions.
  • magnetometers are used to measure the magnetic moment of the entire sample, and the existing scanning magnetometers do not have the functions of magnetizing and demagnetizing the samples.
  • the present invention proposes to use a TMR probe array to perform two-dimensional scanning on rock specimens, and can use the obtained magnetic signals and the least squares algorithm and deconvolution to realize the measurement of natural remanence and saturated isothermal remanence. Perspective development on data parsing.
  • the TMR array scanning rock magnetic detector of the present invention can provide a powerful tool for China's geological and geophysical research, not only can it provide new research tools for traditional geosciences such as paleomagnetism, environmental magnetism, etc., but it can also promote biomagnetism
  • the development of such interdisciplinary subjects as meteorite magnetism also has broad application prospects in integrated circuit detection analysis and non-destructive testing of magnetic materials.

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  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Magnetic Variables (AREA)

Abstract

L'invention porte sur un détecteur magnétique de roche de type à balayage à réseau TMR (magnétorésistance à effet tunnel), comprenant : un système de positionnement d'échantillon, comportant une table de déplacement d'échantillon tridimensionnelle (10) permettant de placer un échantillon de roche (1), et un dispositif de commande de table d'échantillon (20) destiné à régler une position de la table de déplacement d'échantillon tridimensionnelle (10) ; un système de détection de champ magnétique TMR, comprenant un réseau de sondes TMR (30), et un circuit TMR (40) servant à commander le réseau de sondes TMR (30) pour effectuer une détection de champ magnétique ; un système de magnétisation et démagnétisation, comprenant une bobine de magnétisation et démagnétisation (50) emmanchée à l'extérieur de l'échantillon de roche (1) et un circuit de commande de bobine (60) connecté à celui-ci ; un système de commande de traitement de données (70), connecté au circuit TMR (40), au circuit de commande de bobine (60) et au dispositif de commande de table d'échantillon (20), et conçu pour recevoir une entrée d'un utilisateur et envoyer une instruction de balayage TMR, une instruction de magnétisation ou démagnétisation, et une instruction de déplacement de table d'échantillon, séparément. L'échantillon de roche (1) peut être soumis à un balayage magnétique avec une précision de mesure magnétique élevée et une résolution spatiale élevée ; en outre, un système de magnétisation et démagnétisation spécial est prévu, et une magnétisation et une démagnétisation in situ peuvent être effectuées sans déplacer l'échantillon de roche (1).
PCT/CN2018/105903 2018-09-12 2018-09-17 Détecteur magnétique de roche de type à balayage à réseau tmr WO2020051924A1 (fr)

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CN111413654B (zh) * 2020-04-14 2021-05-18 华中科技大学 一种降低隧道磁电阻传感器噪声的系统及方法
JP2023050897A (ja) * 2021-09-30 2023-04-11 ソニーセミコンダクタソリューションズ株式会社 磁気検出装置
CN116047382A (zh) * 2023-03-23 2023-05-02 浙江工业大学 一种冷原子芯片磁场信号检测装置及检测方法
CN117233670B (zh) * 2023-11-13 2024-03-19 之江实验室 一种用于弱电磁屏蔽内的高精度无磁平面扫描装置及方法

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