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Scientific Reports volume 6, Article number: 23759 (2016) Cite this article

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Super-flat supercontinua are generated from a double clad Tm-doped fiber amplifier. Two different laser configurations are investigated and compared. In the direct-output configuration, the long-wavelength edge of the supercontinuum spectra is extended to beyond 2.65 μm with a 10 dB bandwidth of 740 nm. In the passive pigtail configuration, the generated supercontinuum features excellent flatness with an intensity difference smaller than 1 dB in the wide central spectral range from 1.98 μm to 2.41 μm.

Supercontinuum has been studied for decades as its broadband spectral characteristics promise enormous potentials in many significant research fields and practical applications1,2,3. Up to now, many different supercontinuum sources have been developed with different pump sources, such as Yb-doped fiber lasers4,5 and Er-doped fiber laser6,7,8,9, in various fibers including conventional single mode fibers3,9, GeO2 fibers10,11,12, highly nonlinear fibers13,14, photonic crystal fibers5,15,16 and ZBLAN fibers17,18,19,20,21.

Besides, active fibers, especially Tm-doped fibers, have also been found to be an effective medium for supercontinuum generation8,9,10,22,23,24. And, along with the fast development of Tm-doped fiber lasers, 2 μm laser sources have demonstrated its unmatchable advantages as an ideal pump in the generation of mid-infrared supercontinuum17,18,19,20,21. As Tm-doped fiber could be used not only as the gain medium for 2 μm laser source but also as the nonlinear medium for supercontinuum generation, a Tm-doped fiber based supercontinuum system would be preferable. In Tm-doped fiber based supercontinuum systems, the supercontinuum generation process exhibits more complicated physical mechanisms from passive fibers as the 3F4-3H6 and 3H4-3H5 transitions in Tm ions also play an important role in the spectral broadening8,22,23,24,25.

As early as in 2007, S. Kivisto and his colleagues reported the supercontinuum generation in Tm/Ho codoped fiber amplifiers spanning from 1.95 μm to 2.25 μm26. In 2013, J. Liu demonstrated a high power supercontinuum source from a three-stage Tm-doped fiber amplifier, and the spectral range is extended to beyond 2.4 μm27. Later, in 2014, V. V. Dvoyrin extended the long-wavelength side to 2.5 μm with only one-stage amplifier28. However, in these reports, the flatness of the supercontinua generated is not satisfying with intensity differences of about 10 dB.

In our previous works, pulsed 2 μm laser sources were built29,30,31. In this report, exploiting the self-developed 2 μm laser source as the seed, together with a 793 nm LD as the pump, a Tm-doped fiber amplifier for supercontinuum generation is developed. And, two different supercontinuum generation configurations, namely the direct-output configuration and the passive pigtail configuration, are investigated. In the direct-output configuration, the laser output is directly measured at the output end of the double clad Tm-doped fiber. Differently, in the pigtail configuration, a section of passive fiber is spliced at the output end of the double clad Tm-doped fiber. And, the laser output is recorded at the angle cleaved output end of the passive fiber. Supercontinuum is observed in both schemes, but with different characteristics. In the direct-output configuration, the 3 dB bandwidth of the supercontinuum generated reaches about 600 nm, while, in the pigtail configuration, a super-flat supercontinuum is attained with an intensity difference of only 0.87 dB in the wide central spectral range from 1.98 μm to 2.41 μm.

In the laser system, the pulsed 2 μm laser seed exploited has a maximal output power of 1.1 W with the repetition rate tunable from 20 kHz to 100 kHz. At 20 kHz, repetition rate, the seed operates in the gain-switched mode-locking mode29,30,31 where the 100 ns gain-switched envelope contains tens of sub-pulses with durations of about 8 ns. At higher repetition rates, the seed works in the gain-switching mode with a pulse duration of about 50 ns. The amplification fiber is a section of 7 m long double clad Tm-doped fiber (Nufern, 10P/130) with an absorption coefficient of about 3 dB/m at 793 nm. The hexagonal fiber core has an NA of 0.15 and a core diameter of 10 μm. The cladding diameter of the fiber is 130 μm.

Firstly, output characteristics of the double clad Tm-doped fiber amplifier in the direct-output configuration at 60 kHz repetition rate are investigated. And, the results are given in Fig. 1 with Fig. 1(a) presenting the laser spectrum and Fig. 1(b) depicting the output power.

Output characteristics of the double clad Tm-doped fiber amplifier at 60 kHz repetition rate: (a) output spectrum of the amplifier; (b) output power versus the launched pump power.

The short dashed in Fig. 1(a) shows the measured spectrum of the pulsed 2 μm laser seed after propagation through the 7 m long double clad Tm-doped fiber. And, the dotted and solid line represent the amplified spontaneous emission (ASE) spectrum of the Tm-doped fiber and the output spectrum of the amplifier at 4 W 793 nm pump, respectively. As can be found, the seed spectrum centers around 1.95 μm with a 3 dB linewidth of about 14 nm, the ASE centers at 2 μm with a 3 dB bandwidth of about 45 nm, while the amplifier spectrum is the combination of the two. It should be noted that both the seed spectrum and the ASE spectrum come from the 3F4-3H6 transition in Tm ions25. The slope efficiency of the amplifier, shown in Fig. 1(b), is about 22.3% with a maximal output of 2.8W at 12.5 W pump, which is comparable with that in ref. 32.

In the pigtail configuration, the amplifier shows the same output characteristics at 60 kHz repetition rate.

Tuning the repetition rate of the 2 μm laser seed to 20 kHz, supercontinuum is generated in the Tm-doped fiber amplifier in both laser configurations even with no 793 nm pump, as illustrated in Fig. 2. Figure 2(a) presents the supercontinuum generated from the Tm-doped fiber amplifier with the direct-output configuration where there is no passive fiber at the output end of the double clad Tm-doped fiber, while Fig. 2(b) gives the supercontinuum generated from the Tm-doped fiber amplifier with the passive pigtail configuration where a section of 1 m long SMF28 passive fiber is spliced at the output end of the double clad Tm-doped fiber.

Supercontinuum generation from the Tm-doped fiber amplifier at 20 kHz repetition rate with no 793 nm pump power: (a) direct-output configuration with no passive fiber at the output end of the Tm-doped fiber; (b) pigtail configuration with 1 m long passive fiber at the output end of the Tm-doped fiber.

More supercontinua are recorded in Fig. 3 at different 793 nm pump powers. Figure 3(a) provides the laser spectra measured in the direct-output configuration at different 793 nm pump powers. And, laser spectra measured from the passive pigtail configuration are depicted in Fig. 3(b).

Supercontinuum generation from the Tm-doped fiber amplifier at 20 kHz repetition rate with different 793 nm pump powers: (a) direct-output configuration; (b) pigtail configuration.

The supercontinua generated at maximal pump power are shown in Fig. 4. And, output powers of the Tm-doped fiber amplifier is presented in Fig. 5.

Maximal supercontinuum generated from the Tm-doped fiber amplifier at 20 kHz repetition rate with 12.5 W 793 nm pump: (a) direct-output configuration; (b) pigtail configuration.

Output power of the Tm-doped fiber amplifier at 20 kHz repetition rate: (a) direct-output configuration; (b) pigtail configuration.

The output spectrum in Fig.1 (a) demonstrates that the 2 μm laser signal is not effectively amplified as ASE is generated during the amplification process.

As can be found in Fig. 2(a), the supercontinuum generated with no passive pigtail characterizes a wideband long-wavelength supercontinuum region with a 3 dB bandwidth of about 430 nm covering a wide wavelength range from 1.92 μm to 2.35 μm and a strong unabsorbed 2 μm laser signal which is about 6 dB higher than the long-wavelength supercontinuum. This phenomenon is also observed in refs 17, 18, 19, 20, 21. Different from that in Fig. 2(a), with the passive fiber, the 2 μm laser signal in Fig. 2(b) becomes much smaller. However, the spectrum becomes narrower with a 3 dB bandwidth of about 200 nm centering around 2.1 μm. This wide spectral peak around 2.1 μm is also observed in Fig. 2(a). We believe that this should be attributed to the 3H4-3H5 transition in Tm ions8,22,23,24.

In addition, both spectra in Fig. 2 mainly broaden towards the long-wavelength side which is quite different from those in in 1.6 μm pumped supercontinuum generation where the supercontinua generated broaden on both spectral sides6,7,24. The main reason for the generation of the red-shifted supercontinuum is modulation instability which leads to soliton fission and soliton self-frequency shift induced by Raman scattering9,18,19,24.

Similar with that in Fig. 2(a), the relatively strong 2 μm laser signal remains at different 793 nm pump powers in Fig. 3(a). Besides, ASE signal is observed around 2 μm. At 4 W pump, the 3 dB bandwidth of the supercontinuum generated broadens to about 600 nm, while the 10 dB bandwidth reaches 740 nm with the long-wavelength extending to beyond 2.6 μm. It can be found in Fig. 3(b) that, at 4 W 793 nm pump, the flat supercontinuum demonstrates a 3 dB bandwidth of 490 nm, more than doubled compared to that with no 793 nm pump in Fig. 2(b). Besides, the 2 μm laser signal gets almost eliminated through the propagation in the passive fiber, contributing to the flatness of the generated supercontinua which shows an intensity difference of only 1.1 dB from 1.99 μm to 2.40 μm as depicted in the inset of Fig. 3(b). And, it is obvious that the intensity difference is mainly caused by the strong ASE signal around 2 μm.

As marked in Fig. 4(a), at 12.5 W 793 nm pump, compared with the spectrum at 4 W 793 nm pump power, the bandwidth of the spectrum in the direct-output configuration is not further broadened , while the ASE signal gets stronger which is about 3 dB higher than the long-wavelength supercontinuum. On the contrary, in the passive pigtail configuration, the supercontinuum grows broader with the increase of the pump power, as shown in Fig. 4(b). The 3 dB and 10 dB bandwidths of the supercontinua in passive pigtail configuration reach 540 nm and 610 nm, respectively. And, the intensity difference of the central region of the supercontinuum between 1.98 μm and 2.41 μm is only 0.87 dB which is mainly caused by the strong ASE signal as depicted in the inset of Fig. 4(b), demonstrating excellent flatness of this laser system.

As plotted in Fig. 5(a), when there is no pigtail fiber, the maximal output power is about 2.7 W with a slope efficiency of about 21.1% which is very close to that at 60 kHz in Fig. 1(b), demonstrating that the output power is mainly the power of the 2 μm laser signal. Differently, in the passive pigtail configuration, the output power of the Tm-doped fiber amplifier is mainly the power of the supercontinuum since the 2 μm laser signal gets almost eliminated through the propagation in the passive fiber, as shown in Figs 3(b) and 4(b). However, the output power of the supercontinuum is much smaller with the maximal output of only 400 mW as shown in Fig. 5(b).

Super-flat supercontinua are generated from a Tm-doped fiber amplifier although the amplification of the seed is not ideal with the attendance of a strong ASE signal. Comparisons between different pump powers and laser configurations are discussed and analyzed. Compared with the passive pigtail configuration, the direct-output configuration enjoys a broader laser spectrum, while the passive pigtail configuration boasts a much flatter supercontinuum. This laser system would be applicable in broadband absorption spectroscopy applications. However, the power of the supercontinuum generated is still relatively low. And, further improvement in the output power and spectral extension should be considered.

The experimental setup of the Tm-doped fiber amplifier is depicted in Fig. 6. The pulsed 2 μm laser source takes a similar scheme to that described in ref. 25. The 2 μm laser source and the pump source from a 793 nm LD are coupled into a section of 7 m long double clad Tm-doped fiber (Nufern, 10P/130) through a pump combiner (PC).

Schematic diagram of the Tm-doped fiber amplifier.

The laser spectra are recorded with an Andor Shamrock 750 spectrum analyzer. It should be noted that the resolution of the spectrum analyzer is about 2 nm determined by the grating and the step length. And, a thermoelectrically cooled fast HgCdTe detector and a 4 GHz oscilloscope (Tektronix TDS 7404) are exploited to monitor the laser pulses.

How to cite this article: Tao, M. et al. Super-flat supercontinuum generation from a Tm-doped fiber amplifier. Sci. Rep. 6, 23759; doi: 10.1038/srep23759 (2016).

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This work is partially supported by the State Key Laboratory of Laser Interaction with Matter (SKLLIM) under Grant No. SKLLIM1409 and SKLLIM1503 and the Hundred Talents Program of the Chinese Academy of Sciences. The authors are also grateful to Yongsheng Zhang from the SKLLIM for his instructions on manuscript preparation.

State Key Laboratory of Laser Interaction with Matter, Northwest Institute of Nuclear Technology, 710024, Xi’an, P. R. China

Mengmeng Tao, Zhenbao Wang, Hongwei Chen, Yanlong Shen & Guobin Feng

Research Center of Space Laser Information Technology, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, 201800, Shanghai, P. R. China

Ting Yu & Xisheng Ye

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G.F. and X.Y. conceived the project; the experiments were designed by M.T., T.Y. and Z.W.; the pulsed 2 μm laser source was built by M.T.; H.C. and Y.S. measured the spectra of the laser output. All authors contributed to the interpretation of the results and the preparation of the manuscript.

Correspondence to Mengmeng Tao or Xisheng Ye.

The authors declare no competing financial interests.

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Tao, M., Yu, T., Wang, Z. et al. Super-flat supercontinuum generation from a Tm-doped fiber amplifier. Sci Rep 6, 23759 (2016). https://doi.org/10.1038/srep23759

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Received: 03 December 2015

Accepted: 14 March 2016

Published: 29 March 2016

DOI: https://doi.org/10.1038/srep23759

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