Sub-40-fs high-power Yb:CALYO laser pumped by single-mode fiber laser Download: 666次
1 Introduction
All-solid-state femtosecond lasers that deliver high peak power and extremely narrow pulse width are of great interest in many fields such as scientific research, industry, medical treatment, and high speed communication. In particular, ytterbium-based solid-state lasers have attracted increasing attention because of their excellent optical and thermal properties. Recently, a great number of Yb-doped materials including Yb:CaF2[1, 2], Yb:CALGO[3–5], Yb:CALYO[6], Yb:KYW[7], Yb:KGW[8–10] and Yb:Lu2O3[11] crystals as well as Yb:LuAG ceramic[12] have shown their capacity in generating sub-100-fs pulses with watt level average power via either pure Kerr-lens mode-locking (KLM) or combination of KLM and saturable absorber-based passive mode-locking. Among them, Yb-doped calcium aluminate crystals including Yb:CALGO and Yb:CALYO are the most attractive candidates for high-power sub-50-fs pulses generation, due to their flat emission spectra with more than 70 nm bandwidths as well as high thermal conductivity. Regarding sub-50-fs pulses generation, Yb:CALGO and Yb:CALYO crystals have already been proven their abilities by Zaouter et al.[13], Agnesi et al.[14], Gao et al.[15] and Ma et al.[16], respectively. Up to more than 3 W average power with 45-fs pulses was obtained by Manjooran et al.[5]. Still, most of the obtained average powers from above literatures were only on the order of several tens of milli-watt, due to either the small pump power of the single-mode fiber coupled laser diodes (LDs) or the critical cavity setup restrained by the low-brightness multi-mode LDs. One way to cope with the issue raised by the low-brightness LDs is to use a double confocal cavity which separates the gain medium and Kerr medium. Paradis et al. demonstrated the generations of 35-fs pulses with 1.5-W average power and 49-fs pulses with 4.5-W average power from the KLM Yb:Lu2O3 thin-disk laser, respectively, with 76-W and 96-W pump power,[17]. However, the corresponding optical-to-optical efficiency is only 2.1% and 4.7%, respectively. In terms of the KLM Yb:CALGO thin-disk laser, although down to 30-fs pulses were delivered, the average power was only 150 mW, due to the low gain and limited disk quality[18]. And for Yb:CALYO thin-disk lasers, no relevant mode-locking result has been reported so far. On the other hand, compared to the low-power single-mode fiber coupled LDs, single-mode fiber laser emitting at 976 nm emerging recently has not only higher average power up to 10 W[19], but also excellent beam quality with
In this letter, we demonstrated the single-mode fiber-laser-pumped high-power Yb:CALYO lasers passively mode-locked by semiconductor saturable absorption mirror (SESAM) and pure Kerr-lens mode-locking, respectively. 103-fs pulses with up to 3.1-W average power are obtained from passive mode-locking, corresponding to the optical-to-optical efficiency of 31%. In addition, as short as 36-fs pulses with up to 2-W average power are obtained from the pure KLM with extra-cavity dispersion compensation. With the repetition rate of 84 MHz, the pulse energies and peak powers for SESAM-based passive mode-locking and KLM are 37 nJ, 0.31 MW and 24 nJ, 0.58 MW, respectively.
2 Experimental setup
A schematic diagram of the experimental setup is shown in Figure
Fig. 1. The sketch for the experimental setup of the single-mode fiber-laser-pumped mode-locked Yb:CALYO laser. HWP: half-wave plate; L: lens; C1–C3: concave mirrors; GTI1–GTI4: Gires–Tournois interferometer mirrors; OC: output coupler; SESAM: semiconductor saturable absorption mirror.
3 Results and discussion
At first, the cavity was optimized in a continuous-wave (CW) operation, which delivers 4.2 or 3.6-W output powers with 15% or 10% OCs. The absorption efficiency of the crystal for pump laser is up to 99.5% under lasing. Then, to investigate the performance of a passive mode-locking operation, a commercial SESAM (SAM-1040-0.7-1ps-x from BATOP GmbH) with 0.4% modulation depth at 1040 nm was utilized. With 10% transmittance OC, a stable mode-locking operation with up to 3.1-W average power was achieved when the total group delay dispersion (GDD) per round trip introduced by the three GTIs was
Fig. 2. (a) Optical spectrum and (b) the corresponding auto-correlation trace of the passively mode-locked Yb:CALYO laser. The black dot and red solid curve in (b) stand for the experimental data and sech2-fitting, respectively.
Fig. 3. (a) Spectra; (b) output powers and pulse durations of different pure KLM operations realized by detuning the cavity with $\unicode[STIX]{x0394}L$ ; output properties under different pump power for KLM operation at $\unicode[STIX]{x0394}L=-6.126~\text{mm}$ : (c) evolution of spectra and (d) changing in average power as well as pulse duration.
For pure Kerr-lens mode-locking operation, the SESAM was replaced by a fourth GTI mirror. When the dispersion provided by GTI4 per bounce was
For a given position of GTI4 (
Fig. 4. (a) The auto-correlation trace of the compressed pulses. Black and red curves are experimental result and sech2 fitting, respectively. The blue curve is the auto-correlation trace of the Fourier transformation of the corresponding optical spectrum. (b) The corresponding RF spectrum of the 36-fs pulses measured with frequency windows of 3 MHz at 1 kHz of RBW and 0.6 GHz at 100 kHz of RBW (inset), respectively.
To reduce the residual chirp of the femtosecond pulses, extra-cavity compression was implemented by using a pair of GTI mirrors with
To claim the status of the KLM operation, the radio frequency (RF) spectra were measured via a photodetector (PD) with bandwidth of 1 GHz and a commercial RF spectrum analyzer (Agilent E4407B). As described in Figure
4 Conclusion
In conclusion, regarding the excellent optical property of the Yb:CALYO crystal, we have studied the KLM Yb:CALYO laser pumped by a single-mode fiber laser. Using an output coupler of 15% transmittance, different states have been realized by detuning the cavity. As the cavity was getting closer to the edge of stable region, the Kerr strength increased so that the modulation depth was rising accordingly. As a result, broader spectra as well as shorter pulses were obtained. The broadest spectrum was able to cover the wavelength from 980 to 1090 nm, which supports 34-fs pulses with zero chirp. By extra-cavity chirp compensation, near transform-limited pulses of 36 fs have been demonstrated. The average power after compression was 2 W, meaning that the single pulse energy and peak power were up to 24 nJ and 0.67 MW, respectively. An overview of the state-of-the-art performance of ultrafast Yb solid-state oscillators generating sub-40-fs pulses is given in Table
Table 1. Overview of the state-of-the-art performance of ultrafast Yb solid-state oscillators generating sub-40-fs pulses.a
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Compared to the previous works in sub-40-fs generation from Yb solid-state lasers, we have presented, to the best of our knowledge, the highest average power as well as the largest single pulse energy within bulk geometry. Since no saturation in average power and multi-pulse operation was observed, sub-50-fs pulses with higher average power are believed to produce from such a single-mode fiber-laser-pumped Yb:CALYO laser with higher pump power or longer crystal. It is noticed that the shorter wavelength (980 nm–1040 nm) of the spectrum has relatively lower intensity due to the re-absorption. Another possibility is using a gain-matched output coupler[23] to realize smoother spectrum, which is possible to support pulses with only a few cycles of pulse duration. Above all, the broad spectrum as well as good power stability of the laser provides a unique ultrafast source for seeding the femtosecond solid-state amplifier.
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Wenlong Tian, Geyang Wang, Dacheng Zhang, Jiangfeng Zhu, Zhaohua Wang, Xiaodong Xu, Jun Xu, Zhiyi Wei. Sub-40-fs high-power Yb:CALYO laser pumped by single-mode fiber laser[J]. High Power Laser Science and Engineering, 2019, 7(4): 04000e64.