Calibration device and method for measuring weak field of Hall magnetometer based on spin noise spectrum

A noise spectrum and measurement technology, applied in measurement devices, measuring electrical variables, instruments, etc., can solve the problems of measurement accuracy limitation, pressure broadening, collision frequency shift, etc., and achieve high signal-to-noise ratio, narrow line width, signal and The effect of line width optimization

Active Publication Date: 2022-01-28
SHANXI UNIV
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  • Abstract
  • Description
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  • Application Information

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Problems solved by technology

However, the measurement accuracy of such sensors is limited by quantum polarization noise (photon shot noise), so the use of polarization-squeezed light can solve this problem to some extent
[0007] Although the high-pressure inert buffer gas in the atomic gas chamber slows down the diffusion speed of atoms to the inner wall of the gas chamber, at the same time, due to the introduction of the buffer gas, at a certain temperature, additional pressure expansion and collision frequency shift will occur inside the atomic gas chamber

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  • Calibration device and method for measuring weak field of Hall magnetometer based on spin noise spectrum
  • Calibration device and method for measuring weak field of Hall magnetometer based on spin noise spectrum
  • Calibration device and method for measuring weak field of Hall magnetometer based on spin noise spectrum

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Embodiment 1

[0062] Such as figure 1 As shown, Embodiment 1 of the present invention provides a calibration device for measuring weak field of Hall magnetometer based on spin noise spectrum, including: a detection light source, the light output by the detection light source passes through the Flipper mirror 12 and becomes The first probe light and the second probe light are two beams, wherein the first probe light enters the atomic gas chamber 18 along the X direction after passing through the first half-wave plate 28, the first polarizer 29 and the first lens 30, and then passes through the second After two half-wave plates 32, the first Wollaston prism 33 is detected by the first balance detector 34; the second detection light passes through the third half-wave plate 13, the second polarizer 14, the second lens 15, the first After the rectangular prism 16 is incident to the atomic gas chamber 18 along the Y direction, then through the second rectangular prism 20, the third reflector 21, ...

Embodiment 2

[0093] Embodiment 2 of the present invention provides a calibration device for weak-field Hall magnetometer measurement based on spin noise spectrum, which includes: a detection light source, the first detection light output by the detection light source passes through the first half-wave plate 28. After the first polarizer 29 and the first lens 30, it is incident to the atomic gas chamber 18 along the X direction, and then is detected by the first balance detector 34 after passing through the second half-wave plate 32 and the first Wollaston prism 33 The atomic gas chamber 18 is arranged in the magnetic shielding cylinder 36, and the magnetic shielding cylinder 36 is provided with the first Helmholtz coil 17 for providing a magnetic field along the Y direction; the output of the first balance detector 34 The terminals are respectively connected to the first fast Fourier transform dynamic signal analyzer 35; the first fast Fourier transform dynamic signal analyzer 35 is used to...

Embodiment 3

[0096] Embodiment 3 of the present invention provides a method for calibrating weak fields of Hall magnetometers based on spin noise spectrum, which is realized by using the device described in Embodiment 2, and includes the following steps:

[0097] S1. Let the first detection light pass through the atomic gas cell 18, and use the first balance detector 34 to detect the signal when no magnetic field is applied.

[0098] S2 , passing different currents to the first Helmholtz coil 17 , applying different magnetic fields along the X direction, and detecting signals under each current through the first balance detector 34 ; wherein at least 5 groups of different currents are provided.

[0099] S3. Subtract the signal obtained in step S2 and step S1 to obtain the spin noise signal; and calculate the corresponding magnetic field according to the spin noise signal, and perform linear fitting according to the calculated magnetic field and the corresponding current value, and the propo...

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Abstract

The invention belongs to the technical field of atomic measurement, and discloses a calibration device for weak field measurement of Hall magnetometer based on spin noise spectrum, comprising: a detection light source, the first detection light output by the detection light source passes through the first half After the wave plate, the first polarizer and the lens, it enters the atomic gas chamber along the X direction, and then is detected by the first balance detector after passing through the second half-wave plate and the first Wollaston prism; the atomic gas chamber is set In the magnetic shielding cylinder, the first Helmholtz coil for providing a magnetic field along the Y direction is arranged in the magnetic shielding cylinder; the output ends of the first balance detector are respectively connected to the first fast Fourier transform dynamic signal Analyzer; the first fast Fourier transform dynamic signal analyzer is used to analyze the detection signal to obtain the corresponding Larmor precession frequency. The invention can realize the calibration of the Hall magnetometer and can be widely used in the field of magnetometer calibration.

Description

technical field [0001] The invention belongs to the technical field of atomic measurement, and in particular relates to a calibration device and method for measuring a weak field of a Hall magnetometer based on a spin noise spectrum. Background technique [0002] Aleksandrov and Zapasskii demonstrated that the spin noise of alkali metal atoms can be detected by an unperturbed detuned probe laser. The basic principle of spin noise spectroscopy is to map the random spin fluctuations of atoms onto linearly polarized light, which is reflected by the rotation of the polarization plane. For an atomic system in thermal equilibrium, the mean value of the spin polarization m z = (N↑ − N↓) / (N↑ + N↓) is 0 after long-term average, where N↑ and N↓ represent the number of spin-up and spin-down particles respectively, and N↑ + N↓ represents The total number of spin particles detected by the laser. However, due to the existence of thermal fluctuations, there are random fluctuations in N...

Claims

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Application Information

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Patent Type & Authority Patents(China)
IPC IPC(8): G01R35/00
CPCG01R35/005
Inventor 王军民白乐乐张露露杨永彪温馨何军王彦华
Owner SHANXI UNIV
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