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Frequency Stabilization Technology of 1560 nm Fiber Laser Based on Rubidium Modulation Transfer Spectroscopy | IEEE Journals & Magazine | IEEE Xplore

Frequency Stabilization Technology of 1560 nm Fiber Laser Based on Rubidium Modulation Transfer Spectroscopy


Impact Statement:MTS frequency stabilization devices, the cooling and repumping lasers of rubidium fountain clock. 1560-nm external cavity semiconductor seed laser, erbium-doped fiber amp...Show More

Abstract:

The modulation transfer spectroscopy (MTS) technique used to stabilize two different transition lines of rubidium, required for laser cooling of atoms, is investigated. T...Show More
Impact Statement:
MTS frequency stabilization devices, the cooling and repumping lasers of rubidium fountain clock. 1560-nm external cavity semiconductor seed laser, erbium-doped fiber amplifier, frequency double, PPLN crystal, temperature-enhanced MTS signal, F = 1 → F′ = 0 transition, frequency shifts, AOMs, error signal and feedback voltage fluctuations, laser linewidth and the Allan variance of beat signals, frequency instability.

Abstract:

The modulation transfer spectroscopy (MTS) technique used to stabilize two different transition lines of rubidium, required for laser cooling of atoms, is investigated. The laser source is based on a 1560 nm semiconductor laser diode that is amplified by an erbium doped fiber amplifier (EDFA). The laser output is frequency doubled with a fiber coupled periodically poled Lithium Niobate (PPLN) crystal to 780 nm. To address the weak spectral features of repumping laser, a theoretical study is conducted followed by experimental verification. The 87Rb D2 line F = 1 → F′ = 0 transition temperature-enhanced MTS signal is observed, which provides a choice to stabilize the repumping laser frquency on the F = 1 → F′ = 2 transition using frequency shifting with acousto-optic modulators (AOMs). Compared with the orignal MTS signal, this method is shown to be more stable and accurate for laser frequency locking. Laer frequency locking is realized by controlling the driving current of the seed laser using digital PID feedback. After locking, the laser linewidth is 35.36 kHz.
Published in: IEEE Photonics Journal ( Volume: 16, Issue: 5, October 2024)
Article Sequence Number: 7101506
Date of Publication: 20 May 2024

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