中国激光2024,Vol.51Issue(5) :128-134.DOI:10.3788/CJL231346

22 W,240fs高功率中红外飞秒光学频率梳

22-W,240-fs High-Power Mid-Infrared Femtosecond Optical Frequency Comb

蔡宇 田昊晨 曹士英 秦冠仕 胡明列
中国激光2024,Vol.51Issue(5) :128-134.DOI:10.3788/CJL231346

22 W,240fs高功率中红外飞秒光学频率梳

22-W,240-fs High-Power Mid-Infrared Femtosecond Optical Frequency Comb

蔡宇 1田昊晨 2曹士英 3秦冠仕 4胡明列1
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作者信息

  • 1. 天津大学精密仪器与光电子工程学院超快激光研究室&光电信息技术教育部重点实验室,天津 300072
  • 2. 中国计量科学研究院时间频率计量研究所,北京 100029
  • 3. 中国计量科学研究院时间频率计量研究所,北京 100029;国家市场监管重点实验室(时间频率与重力计量基准),北京 100029
  • 4. 吉林大学电子科学与工程学院集成光电子学国家重点实验室,吉林长春 130012
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摘要

中红外飞秒光学频率梳在天文学、药物检测、生物化学、大气检测和材料科学等领域中有着广阔的应用前景.报道了一个高功率中红外飞秒光学频率梳系统,该系统主要由掺铒光纤飞秒光学频率梳、超连续谱产生装置、双包层掺铥光纤放大器和基于透射式衍射光栅对的压缩器四部分构成.掺铒光纤光学频率梳输出平均功率为350 mW、中心波长为1565 nm、重复频率为198 MHz、脉冲宽度为55 fs的飞秒激光,并将其注入到一段正色散高非线性光纤中,产生1100~2200 nm超连续光谱.超连续光通过由掺铥光纤构成的自泵浦放大器,产生中心波长为1925 nm、平均功率为50 mW的飞秒脉冲.将此脉冲作为双包层掺铥光纤放大器的种子源,功率被放大到36.07 W,压缩后得到平均功率为22.72 W、脉冲宽度为240 fs的飞秒激光脉冲输出.

Abstract

Objective The femtosecond optical frequency comb(FOFC)comprises a series of ultra-short laser pulses with the same temporal separation in the time domain and discrete,equidistant,and stable phase-related frequency components in the frequency domain.The FOFC can accurately measure the absolute frequency of an atomic clock and serve as a natural time-frequency reference.Currently,the most stable and compact light source is the mode-locked erbium-doped fiber laser with a central wavelength of 1.55 μm,typically employing highly nonlinear fibers to broaden the spectrum across the entire transparent range of silica fiber(350-2400 nm).However,the output power of the erbium-doped fiber FOFC is generally in the range of a few hundred milliwatts.Therefore,increasing the output power of the FOFC remains a crucial challenge.The mid-infrared FOFC holds significant application value in next-generation spectroscopy,as it can be used to detect gases such as carbon dioxide and ammonia and extend the FOFC wavelength to the molecular fingerprint spectrum range(3-20 μm)through nonlinear crystals.This spectrum range is vital for chemical composition analysis,making the development of high-power mid-infrared FOFCs a pressing need.Methods This system comprises an erbium-doped fiber FOFC,a super-continuum converter,a double-cladding thulium-doped fiber amplifier system,and a transmission diffraction grating pulse compressor.Initially,the erbium-doped fiber FOFC utilizes a highly nonlinear fiber with normal dispersion for frequency broadening.Additionally,a self-pump amplifier composed of thulium-doped fiber generates a femtosecond seed with a central wavelength of 1925 nm.This seed is injected into a chirped pulse amplification system comprising a 55 m long highly nonlinear fiber with normal dispersion,a three-stage thulium-doped fiber amplifier,and a transmission diffraction grating pulse compressor.To characterize the noise of the high-power mid-infrared FOFC,we analyze the relative intensity noise and the phase noise of the pulse train using a signal source analyzer.Moreover,we co-couple the super-continuum laser generated by the high-power mid-infrared FOFC in the fluorotellurite fiber with a 1064 nm iodine-stabilized Nd∶YAG laser to detect the beat signal and verify the performance of the high-power mid-infrared FOFC.Results and Discussions The 1.55 μm femtosecond laser output from the erbium-doped fiber femtosecond optical frequency comb is symmetrically broadened to the spectral range of 1100-2200 nm by the highly nonlinear fiber with normal dispersion(Fig.2).The resultant super-continuum laser is injected into the self-pump pre-amplifier to obtain a femtosecond seed with a central wavelength of 1925 nm and an average power of 50 mW[as indicated by the dashed line in Fig.3(a)].This seed is then broadened to hundreds of picoseconds through the normal dispersion fiber and amplified by the three-stage double-cladding thulium-doped fiber amplifier to yield a picosecond pulse with a central wavelength of 2000 nm and an average power of 36.07 W.After compression,a femtosecond pulse with an average power of 22.72 W and a pulse width of 240 fs is obtained[Fig.3(b)].The integral values of relative intensity noise and timing jitter are 1.16%and 472 fs,respectively(integral range of 10 Hz-1 MHz)(Figs.4 and 5).The super-continuum laser(Fig.6)generated by the high-power mid-infrared FOFC and the 1064 nm laser produce a beat signal with a signal-to-noise ratio of 40 dB,meeting the counting requirements of the counter(Fig.8).Conclusions We demonstrate a high-power FOFC based on an erbium-doped FOFC,generating a 2 μm femtosecond seed through a highly nonlinear fiber with normal dispersion and self-pump pre-amplifier.The highly nonlinear optical fiber with normal dispersion effectively overcomes noise sensitivity issues associated with nonlinear dynamics of abnormal dispersion,such as soliton self-frequency shift and Raman soliton,during super-continuum generation.The femtosecond pulse,obtained with an average power of 22.72 W and a pulse width of 240 fs,marks a significant advancement in developing high-power mid-infrared FOFCs.This development contributes to the spectroscopic analysis of molecular structures and dynamics and facilitates the expansion of optical frequency combs into the molecular fingerprint spectrum range(3-20 μm).

关键词

非线性光学/光学频率梳/飞秒激光/啁啾脉冲放大/中红外波段

Key words

nonlinear optics/optical frequency comb/femtosecond laser/chirped pulse amplification/mid-infrared band

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基金项目

国家自然科学基金(61827821)

国家自然科学基金青年科学基金(62105237)

出版年

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
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