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Optical Technique

Study of frequency stabilization of a diode laser at all optical Cs atom magnetometer

刘强 Liu Qiang, 李九兴 LI Jiuxing, 黄立明 HUANG Liming, 张军海 Zhang Junhai, Sun Weimin

Published Jan 1, 2012• 1 citation

Abstract

Theory of all optical cesium magnetometer is based on the optical testing which can be used in weak magnetic field measurement.The character of laser frequency stabilization would affect the magnetometer sensitivity directly.In this work,the principle of dichroic atomic vapor laser lock(DAVLL) is analyzed and compared with the other frequency stabilization methods.The method basing on traditional two-level atom is not applicable to cesium D2 transitional frequency stabilization.The DAVLL spectra of D2 line from ground states of Fg=4 and Fg=3 transitions at different magnetic field are measured.That the optimum magnetic field is about 16mT for two transitions is found out.The dependence of the frequency shift of the zero point of the frequency discrimination curve on the magnetic field strength is discussed.The result show that the magnetic field would make the zero point from ground state Fg =4 transition shift of 6MHz/mT relative to Fg=4→Fe=5 transition and shift of-9MHz/mT for ground Fg=3 transition relative to Fg=3→Fe=4 transition near the optimum field respectively.

DOI: 10.3788/gxjs20123803.0259

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Theory of all optical cesium magnetometer is based on the optical testing which can be used in weak magnetic field measurement.The character of laser frequency stabilization would affect the magnetometer sensitivity directly.In this work,the principle of dichroic atomic vapor laser lock(DAVLL) is analyzed and compared with the other frequency stabilization methods.The method basing on traditional two-level atom is not applicable to cesium D2 transitional frequency stabilization.The DAVLL spectra of D2 line from ground states of Fg=4 and Fg=3 transitions at different magnetic field are measured.That the optimum magnetic field is about 16mT for two transitions is found out.The dependence of the frequency shift of the zero point of the frequency discrimination curve on the magnetic field strength is discussed.The result show that the magnetic field would make the zero point from ground state Fg =4 transition shift of 6MHz/mT relative to Fg=4→Fe=5 transition and shift of-9MHz/mT for ground Fg=3 transition relative to Fg=3→Fe=4 transition near the optimum field respectively.

We present a method of laser frequency stabilization based on the linear dichroism signal in a transverse magnetic field. This method is similar to the DAVLL (Dichroic Atomic Vapor Laser Lock) method. It differs from DAVLL and from its existing modifications primarily by the fact that it uses signals of linearly polarized light caused by alignment, rather than circular refraction caused by orientation, and therefore allows us to obtain error signals at the magnetic field modulation frequency (or its second harmonic) by extremely simple means. The method allows the laser frequency to be stabilized in the vicinity of the low-frequency transition in the D1 line of Cs; it does not require strong magnetic fields or careful shielding of cells containing cesium atoms. Although the absorption line in a gas-filled cell is typically gigahertz wide, the achievable resolution, limited by the signal-to-noise ratio of photon shot noise, can reach units or tens of kilohertz in a one hertz bandwidth.

A robust laser-frequency-locking scheme to atomic transitions is proposed and demonstrated. In this scheme, dispersion of the Zeeman-shifted atoms instead of absorption in the dichroic atomic vapor laser lock (DAVLL) [Appl. Opt.37, 3295 (1998)] is measured and used as an error signal for stabilization feedback. The error signal of the proposed scheme can provide a wide locking range. Experimental demonstration with the transition between 5d 2D3/2 and 6p 2P1/2 of Ba+ is carried out for a grating feedback external-cavity laser diode at 650 nm.

We report the frequency stabilization of a diode laser by applying the dichroic-atomic-vapor laser lock (DAVLL) method to a thin Rb vapor cell. A 1-mm-long Rb vapor cell is used to obtain a sub-Doppler spectrum that is required for frequency locking, which is easier than in the case of using a saturated absorption spectrometer. A 794-nm diode laser is tuned to the Rb D 1 line, and sub-Doppler signals are observed by introducing a pumping beam and a probe beam in a perpendicular direction. We obtain error signals by subtracting the signals of σ+ polarized beams from that of σ- polarized beams in the presence of a magnetic field and stabilized the 794 nm diode laser frequency without modulating laser parameters. The stability of the 794-nm diode laser is evaluated using other independently stabilized diode laser.

Frequency stabilization of a diode laser at 480 nm is crucial for coherently exciting rubidium atoms to Rydberg states.A laser frequency stabilization technique is reported based on electromagnetically induced transparency in a ladder configuration with a polarization spectrum stabilized 780 nm diode laser as the probe laser and a 480 nm laser as the coupling laser.With a uniform magnetic field,a two-photon dichroic atomic vapor laser lock(DAVLL) spectroscopy was generated.Then this spectroscopy was fed back through two proportion-integral-differential circuits to lock the 480 nm diode laser.A combined linewidth of about 1 MHz is achieved during the locking period.

In order to availably solve the crosstalk of the traditionally optically pumped magnetometer,in which an oscillating magnetic field drives transitions between Zeeman magnetic sublevels,an all-optical cesium(Cs)atomic magnetometer based on Bell-Bloom structure has been investigated and demonstrated experimentally in this paper.When there is an external magnetic field,by analyzing the Larmor precession spectrum of the polarized ground state atoms induced by a modulated pump laser,the atomic magnetometer with high sensitivity is achieved.First,we present the operating principle of the magnetometer with amplitude modulation and set up the experimental system by means of a three-layer magnetic shield.Then in the case of 100 nT field by optimizing the experimental parameters,i.e.,the frequency and intensity of the pump laser,we have obtained the atomic precession spectrum with line width(full width at half maximum)of 22 Hz and signal noise ratio(SNR)of 3.2×104 per unit hertz band width,and then have evaluated the magnetometer with an intrinsic sensitivity of 100fT/Hz1/2 and spatial resolution smaller than 1.2cm,while the experimentally closed loop test shows that the cesium atomic magnetometer would have the sensitivity of 120fT/Hz1/2 and response time of 300 ms.