Abstract
We experimentally demonstrated a passively mode-locked picosecond Tm,Ho:LiLuF4 laser with low threshold and high efficiency. The stable continuous-wave (CW) mode-locked operation with 12 ps pulse width is obtained by using a five-mirror cavity structure and semiconductor saturable absorber mirrors (SESAMs). The results indicate that the laser offers a mode-locked threshold power of 1.03 W and maximum mode-locked output power of 350 mW. The repetition rate of mode-locked pulse sequence is 98.04 MHz, corresponding a maximum single pulse energy of 3.51 nJ.
Introduction
In recent years, 2 μm ultrashort-pulsed lasers based on doped Tm3+ or co-doped Tm3+& Ho3+ are one of the frontier research contents of ultrafast laser technology. The emission peak of a Tm3+ doped laser is located near the strong absorption peak of water, at 1.93 μm, so it has the characteristics of a low penetration depth and has important applications in ophthalmic laser surgery, tumorectomy [1, 2]. Moreover, the laser has excellent atmospheric permeability and will play an important role in military and space communication fields. The laser spectrum is also located in the “fingerprint” region of the reaction molecule's absorption characteristics, so it has important application value in the field of accurate time-resolved molecular spectroscopy [3]. As a pump source, it has an important application in 3–5 μm mid-infrared band generation, mid-infrared supercontinuum generation and THz band pulse generation [4]. However, realizing a mode-locked operation is one of the technical difficulties it faces due to Q-switching, caused by water molecular absorption and gain medium spectral modulation.
Compared with other matrix materials, Tm,Ho:LiLuF4 (Tm,Ho:LLF) is an excellent laser crystal with relatively low phonon energy, lower laser threshold and small up-conversion loss [5]. In 2010, Peng et al. reported a CW Tm,Ho:LLF laser with a central wavelength of 2.05 um and an output power of 50 mW [6]. In 2013, Zhang et al. used Cr2+:ZnS as a saturated absorber to realize Q-switching and Q-switching mode-locking operation of Tm,Ho:LLF laser [7, 8]. It was not until 2018 that Ling et al. realized the Q-switched mode locking operation of Tm:LLF laser [9].
It is well known that the passively mode-locked operation of a 2 μm band can be obtained by periodically controlling the loss of the resonator with the saturable absorber (SA). Based on characteristics of tunable material non-linear absorption coefficient, short relaxation time and recovery time and low optical loss, more and more optical materials have been applied in the field of lasers, such as SESAM, graphene, graphene oxide, topological insulators (TI), single-walled carbon nanotubes (SWCNT), etc. [10–12]. The SESAM is a major mode-locked element with mature commercial performance and stable mode locking characteristics. Picosecond or femtosecond mode-locking operation has been realized in crystals Tm: CLNGG [13], Tm,Ho:NaY (WO4)2 [14], Tm: Sc2O3 [15], Tm:CaGdAlO4 [16], Tm: CaYAlO4 [17], Tm: Lu2O3 ceramics [18], Tm,Ho:CNGG [19], and Tm,Ho:CLNGG [20]. Ma et al. Comprehensively analyzed the mode-locked characteristics of this kind of lasers [21].
In this paper, we demonstrate a low threshold and high efficiency mode-locked Tm,Ho:LLF laser by using a five-mirror cavity structure. The results show that the crystal achieves the current highest efficiency of 53.6% under CW operation; the maximum mode-locked output power is 350 mW at 1,895 nm, and the typical pulse width is 12 ps. Moreover, the minimum CW threshold power is 59 mW, and the mode-locked threshold power is 1.03 W. Because the output power of Ti: sapphire laser is positively correlated with the cost, the low threshold design of the laser can not only effectively reduce the cost, but also provide a new idea for the application of laser.
Experimental Setup
The experimental setup of CW mode-locked Tm,Ho:LLF laser is shown in Figure 1. The five-mirror cavity system mainly includes a typical X- type four-mirror folded cavity and focused concave mirror. The resonator has an oscillating spot of tens of microns, which greatly reduces the laser threshold. The laser efficiency can be improved easily by optimizing the matching of pumping and oscillating spots. The pump source is a self-made Ti-doped sapphire laser. Figure 2 shows the absorption spectrum of Tm,Ho:LLF. From Figure 2, it is observed that the central wavelength of the strongest absorption peak of Tm,Ho:LLF crystal is 780.5 nm, and the half-width is 1 nm. Tm,Ho:LLF crystal is cut at the angle of Brewster. The two end faces are polished. The doped concentrations of Tm3+ and Ho3+ are 5 and 0.5%, respectively. The size of the crystal is 3 × 3 × 8 mm. The laser crystal is wrapped in indium foil and clamped in a copper radiator. The copper clamp is cooled by 8°C constant temperature circulating water cooling system. The focal length of the focusing lens L2 is 120 mm. The focal length of the pumping concave mirror M9 is 100 mm, and the focal length of the M10 is 75 mm, which has a transmittance of more than 95% at 770–1,050 nm and reflectance of more than 99.9% at 1,800–2,075 nm. The transmittance of output coupling (OC) mirror M11 is 3%. The radius of concave mirror M12 is 100 mm. M13 is a plane high-reflectivity mirror with a reflectivity of more than 99.9% at 1,800–2,075 nm. The SESAM is GaAs-SESAM with a modulation depth of 1.2% and a relaxation time of 10 ps (BATOP, Germany). The waist radius of SESAM is about 180 μm, and the energy flux is 117 μJ/cm2, which is larger than SESAM saturated flux of 70 μJ/cm. P1 and P2 are CaF2 prism pairs with a distance of 35 cm, which mainly compensate for the second-order dispersion produced by intracavity crystals and self-phase modulation.
Figure 1
Figure 2
Experimental Results and Discussion
The folding mirror is composed of M10 and M9. The radius of curvature of M9 is 100 mm. In order to achieve high efficiency and low threshold operation by mode matching of pumping light and oscillating light, the curvature radius of the folding mirror M10 is 100, 75, and 50 mm, respectively. The corresponding folding cavity is marked as (100, 100), (100, 75), (100, 50). The absorption efficiency of the crystal is shown in Figure 3A. It can be seen that the absorption efficiency of the crystal is 35.3% without laser oscillation. After the laser oscillation, the absorption efficiency of the crystal increases due to the consumption of a large number of upper-level particles and varies with the coupling ratio of the output mirror. The transmittance of the output mirror is 1.5 and 3% respectively. When M10 is 100 and 50 mm, the absorption efficiency of the crystal is at the highest. When M10 is 75 mm, the absorption efficiency of the crystal is between 57.9 and 60.8%. When SESAM and CaF2 prisms are added into the cavity, M10 is chosen as 75 mm, and the absorption efficiency of the crystal is about 59%. It can be seen that the beam waist radius of the oscillating light in the crystal will be determined by the choice of different folding mirrors, which will affect the absorption efficiency of the crystal. At the same pump power, CW and mode-locked operation will not affect the absorption efficiency of the crystal.
Figure 3
As can be seen from Table 1, the 1.5% OC and (100, 75) cavity can achieve the operation of low threshold and high efficiency. The CW threshold power is as low as 59 mW, the slope efficiency is up to 53.6%, the maximum output power is 1.04 W, and the corresponding optical-optical conversion efficiency is 30.09%. So (100, 75) cavity is chosen as mode-locked cavity in the experiment. When the M13 plane reflector is replaced by SESAM and the CaF2 prism is inserted into the cavity to compensate dispersion, the laser threshold is increased to 67 mW. When the absorption pump power is >1.03 W, the stable CW mode-locked operation is realized, and the maximum output power is 203 mW, and the slope efficiency is 12.9%. With 3% output mirror, the CW threshold power is 88 mW, and the pump power is gradually increased. When the absorption pump power is >1.3 W, a stable CW mode-locked operation is obtained. The maximum output power is 350 mW and the slope efficiency is 21.8%.
Table 1
| M9 (mm) | M10 (mm) | M11 OC (%) | threshold power (mW) | Crystal absorption efficiency (%) | Slope efficiency (%) | Output average power (mW) | Optical to optical efficiency (%) |
|---|---|---|---|---|---|---|---|
| 100 | 100 | 1.5% | 108 | 77.6% | 39.1% | 979 | 28.88% |
| 100 | 75 | 1.5% | 59 | 57.9% | 53.6% | 1,044 | 30.09% |
| 100 | 75 | 3% | 88 | 60.7% | 53.1% | 1,064 | 30.93% |
| 100 | 50 | 1.5% | 81 | 76.6% | 39.2% | 1,024 | 29.01% |
| 100 | 50 | 3% | 104 | 79.3% | 39.7% | 1,064 | 30.14% |
The continuous wave parameters of different pump mirrors.
It is found that the difference between the mode-locked threshold power of 1.5% output coupling mirror and that of 3% OC is little; the mode-locking threshold of 1.5% is 1.03 W and that of 3% output coupling mirror is 1.3 W. The main reason for this is that the passive mode-locking is soliton mode-locking [22–24], and the threshold of mode-locking is mainly determined by the energy flux density on the surface of SESAM. So when mode locking is started, the energy flux density on the surface of SESAM for 3% OC and 1.5% OC should be the same, i.e., corresponding to the same cavity power. So theoretically, the output power of 3% OC should be twice that of 1.5% OC. From Figure 3B, it can be seen that when mode locking is started, the output power of 3% OC is 260 mw, which is approximately twice the output power 128 mW of 1.5% OC, which is consistent with our theoretical prediction.
Because the central wavelength of the mode-locked spectrum is 1,895 nm, which is near the absorption band of water molecules, in order to achieve stable mode-locked operation, we use the dehumidifier to reduce the indoor air relative humidity to about 30%, and the decrease of air humidity can also reduce the cooling temperature of crystal to a lower level without condensation water. In this experiment, the cooling temperature of the crystal is 8°C, which greatly reduces the thermal lens effect of the crystal. Thermal noise generated by heat accumulation on SESAM also affects the stability of mode-locking. Therefore, we designed a water-cooling device for SESAM, which can keep the temperature of SESAM stable at about 8°C. This cooling device improves the stability of mold locking and prolongs the operation time of mold locking.
The detection of CW mode-locked pulse sequence is realized by connecting a 200 MHz digital oscilloscope (RIGOL, DS4024) with a fast photodiode (EOT, ET-5000). Figure 4 shows a CW mode-locked pulse sequence with repetition rate of 98.04 MHz, which is obtained with scanning time of 1 ms and 10 ns. As shown in the inset of Figure 5, the spectrum of the mode-locked pulse is measured by a spectral analyzer (AvaSpec-NIR256-2.5TEC). The central wavelength of the output CW mode-locked pulse is 1,895 nm, and the half-width of the spectrum is 14 nm. The autocorrelation envelope pulse width measured by autocorrelator (APE, pulse check 50) is 17 ps, and the actual pulse width is 12 ps by sech2 function fitting, as shown in Figure 5.
Figure 4
Figure 5
Conclusion
In summary, the folding mirrors with different curvatures are selected for a comprehensive comparison at CW operation. It is concluded that the laser cavity (100, 75) has the best comprehensive output performance under a 1.5% OC mirror. The laser threshold power is as low as 59 mW, the maximum power is 1.04 W, the slope efficiency is 53.6%, and the optical-optical conversion efficiency is 30.09%. So we choose (100, 75) cavity to study mode-locked operation. Using GaAs-SESAM as a mode-locked starter and self-made water cooling system to eliminate the thermal noise of SESAM, a high efficiency CW mode-locked operation of Tm,Ho:LLF laser is realized. Under 3% OC mirror, the maximum power of 350 mW, the shortest pulse width of 12 ps and the repetition rate of 98.04 MHz are obtained, corresponding to the maximum single pulse energy of 3.51 nJ. In the next step, we will use graphene, SWCNT or other low loss SA to reduce the loss of the whole cavity and achieve shorter mode-locked pulse with reasonable dispersion compensation.
Statements
Data availability statement
All datasets generated for this study are included in the article/supplementary material.
Author contributions
WL was the author of the experimental scheme and the general director of the project. TX, RS, and CC were graduate students of the research group, who implement the experimental scheme. QX and YZ were the specific guidance for postgraduates during the experiment.
Funding
This work was supported by the National Natural Science Foundation of China (Nos. 11774257, 61564008, 11647008, 11504416), the International Science & Technology Cooperation and Exchanges Project of Shaanxi (No. 2014KW07-01), and the Key Sciences and Technology Project of Baoji City (No. 2015CXNL-1-3).
Conflict of interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
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Summary
Keywords
TmHo:LLF laser, resonant cavity, low threshold, continuous-wave mode locking, semiconductor saturable absorber mirrors
Citation
Ling W, Xia T, Sun R, Chen C, Xu Q and Zhang Y (2020) Low Threshold, High Efficiency Passively Mode-Locked Picosecond Tm,Ho:LiLuF4 Laser. Front. Phys. 7:216. doi: 10.3389/fphy.2019.00216
Received
23 October 2019
Accepted
27 November 2019
Published
10 January 2020
Volume
7 - 2019
Edited by
Xueming Liu, Zhejiang University, China
Reviewed by
Jiangfeng Zhu, Xidian University, China; Guoqiang Xie, Shanghai Jiao Tong University, China
Updates
Copyright
© 2020 Ling, Xia, Sun, Chen, Xu and Zhang.
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*Correspondence: Weijun Ling wjlingts@sina.comYani Zhang yanizhang1@163.com
This article was submitted to Optics and Photonics, a section of the journal Frontiers in Physics
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