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光频梳精密测量543 nm稳频He-Ne激光波长方法研究

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报道了一种利用光频梳精密测量543 nm He-Ne激光波长的实验方法,该方法采用偏频锁定技术将1086 nm连续分布式反馈光纤激光器锁定至光学频率梳,然后通过非线性光学晶体周期性极化铌酸锂(PPLN)倍频产生高稳定的543 nm连续激光.以倍频产生的543 nm激光作为参考标准光源,通过光学拍频方式实现被测543 nm热稳频He-Ne激光器波长的精确测量.实验结果表明,分布式反馈光纤激光器与光频梳锁定后3 h内的频率波动极差为0.2 MHz,且能长时间保持可靠的锁定状态.被测543 nm热稳频He-Ne激光器的频率抖动极差为1.3 MHz,标准差为0.2 MHz,1s和1000 s的频率稳定度分别为2.1×10-10和1.1×10-10,波长复现性为0.2 MHz,该方法的测量结果与利用碘稳频543 nm He-Ne激光拍频测量的数据等效.将1086 nm激光与光频梳连接,再通过倍频方式实现低功率543 nm He-Ne稳频激光波长的测量,该方法能够直接实现激光波长测量向时间频率基准的溯源,有效保证了测量结果的准确性.
Precise Wavelength Measurement of 543-nm Frequency Stabilized He-Ne Laser Using Optical Frequency Comb
Objective The precise wavelength measurement of a 543-nm He-Ne laser traditionally relies on iodine-stabilized 543-nm He-Ne laser as the wavelength reference source,which is used to measure the thermally stabilized 543-nm He-Ne laser wavelength via beat frequency beating method.Usually,thermally stabilized 543-nm He-Ne laser employs as a secondary laser wavelength standard,which is widely used in precise measurement.Furthermore,iodine-stabilized 543-nm He-Ne laser is the internationally recommended standard laser frequency reference with its relative standard uncertainty of 4.5×10-11.The iodine-stabilized 543-nm He-Ne laser utilizes the intracavity saturation absorption frequency stabilization method,requiring the insertion of the iodine cell into the laser resonant cavity.However,the gain of the Ne atom at 543 nm is notably low,approximately 1%of that at 633 nm.Consequently,the output power of the single longitudinal mode is limited,reaching only approximately 50 μW.Influences,such as mechanical drift,device aging,and other factors,can lead to detuning of the laser resonator cavity,and mismatches with the iodine cell.Hence,prolonged absence in light might be experienced by the 543-nm iodine-stabilized laser,compromising its utility as a laser wavelength reference.Thus,the development of a new wavelength measurement method for the 543-nm He-Ne laser is deemed essential.Methods In this study,a new method for accurately measuring the wavelength of the 543-nm He-Ne laser with an optical frequency comb is reported.This method employs offset locking technology to lock the 1086-nm distributed feedback single frequency fiber laser to the optical frequency comb.A frequency-stabilized 543-nm laser is generated by the nonlinear crystal PPLN via a frequency doubling process.The beat notes,detected via the generated CW 543 nm laser and measured 543-nm thermally stabilized He-Ne laser,can achieve accurate wavelength measurement of the measured laser.Results and Discussions The innovative approach for accurately measuring the wavelength of the 543-nm He-Ne laser using an optical frequency comb addresses the challenges of low output power and low signal-to-noise ratio typically observed in beat frequency measurements at 543 nm.Experimental data indicates a signal-to-noise ratio of 41 dB between the 1086-nm single-frequency fiber laser and optical frequency comb.After locking the 1086-nm laser,a frequency fluctuation range of 0.2 MHz is observed over 3 h,with a standard deviation of 0.03 MHz.A frequency jitter range of 1.3 MHz is noted between the 543-nm laser,produced by frequency doubling,and tested He-Ne laser,with a standard deviation of 0.2 MHz.The short-term(1 s)frequency stability and long-term(1000 s)frequency stability of the assessed 543-nm He-Ne laser outperform with values better than 2.1 × 10 10 and 1.1 × 10-10,respectively.These findings closely match the direct measurement outcomes of the iodine-stabilized laser,which exhibits a frequency difference of 2.9 MHz.Conclusions In this study,the method for precise wavelength measurement of 543-nm He-Ne laser via optical frequency comb is reported.This method utilizes offset locking technology to lock the 1086-nm single frequency fiber laser to the optical frequency comb.Furthermore,a frequency-stabilized 543 nm laser,generated via frequency doubling with a PPLN crystal,serves as the reference for gauging the wavelength of the thermally frequency-stabilized He-Ne laser.Within 3 h after offset locking,the beat frequency fluctuation range between the single-frequency fiber laser and optical frequency comb is 0.2 MHz,and the standard deviation is 0.03 MHz.The frequency jitter difference between the 543-nm laser,generated by frequency doubling,and measured thermally stabilized He-Ne laser is 1.3 MHz,standard deviation is 0.2 MHz,short-term(1 s)frequency stability is better than 2.1× 10-10,and long-term(1000 s)frequency stability is better than 1.1 ×10-10.This method measuring the wavelength of 543 nm is equivalent to the direct beat frequency measurement of iodine stabilized laser.In this method,the low-power 543-nm He-Ne frequency stabilized laser wavelength measurement is realized via frequency doubling.The link between continuous laser and optical frequency combs is established and the laser wavelength measurement is directly traced to the time and frequency reference,which effectively ensures the accuracy of the measurement results.

measurementmetrologylaser frequency stabilizationoptical frequency comb543 nm He-Ne frequency-stabilized laserlaser wavelength measurementoffset locking

俞秋叶、王建波、殷聪、毕文文、雷李华、张宝武、孔明

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中国计量大学计量测试工程学院,浙江杭州 310018

中国计量科学研究院,北京 100029

上海市计量测试技术研究院,上海 201203

测量 计量学 激光稳频 光学频率梳 543 nm He-Ne稳频激光 光波长测量 偏频锁定

2024

中国激光
中国光学学会 中科院上海光机所

中国激光

CSTPCD北大核心
影响因子:2.204
ISSN:0258-7025
年,卷(期):2024.51(13)