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Fibers 2013, 1(3), 93-100; doi:10.3390/fib1030093
Published: 10 December 2013
Abstract: Large-size 0.1 Yb2O3–1.0 Al2O3–98.9 SiO2 (mol%) core glass was prepared by the sol–gel method. Its optical properties were evaluated. Both large mode area double cladding fiber (LMA DCF) with core diameter of 48 µm and large mode area photonic crystal fiber (LMA PCF) with core diameter of 90 µm were prepared from this core glass. Transmission loss at 1200 nm is 0.41 dB/m. Refractive index fluctuation is less than 2 × 10−4. Pumped by 976 nm laser diode LD pigtailed with silica fiber (NA 0.22), the slope efficiency of 54% and “light-to-light” conversion efficiency of 51% were realized in large mode area double cladding fiber, and 81 W laser power with a slope efficiency of 70.8% was achieved in the corresponding large mode area photonic crystal fiber.
In recent years, the demands on high-power fiber lasers applied for Inertial Confinement Fusion (ICF)  and industrial laser processing application make Yb3+-doped silica fiber laser a hot research area [2,3,4,5]. Compared with the traditional double-clad fibers, large mode area double cladding fiber (LMA DCF) and large mode area photonic crystal fiber (LMA PCF) have unparalleled advantages, such as low power density at the pump end, high thermal damage threshold when pumped at high power, and single-mode transmission at certain designed structures [6,7].
The fabrication of LMA Yb3+-doped silica fiber needs large size core glass. It challenges the traditional modified chemical vapor deposition process (MCVD) method of active fiber preform. The MCVD, combined with solution doping with the merit of high purity and low optical loss, has been today’s standard production method of fiber preform for industrial applications . However, it is difficult to make large-diameter fiber core for LMA fiber under the condition of sustaining the initial homogeneity . The sol–gel method can address this issue. It has great flexibility to prepare the geometry of silica fiber core and different species of chemicals can be mixed at the molecular scale through the sol–gel process. Therefore, large-size cores with good doping-homogeneity can be realized by using the sol–gel method.
In this work, Yb3+-doped silica core glass was prepared using the sol–gel method. Al3+ was co-doped in silica glass to promote the solubility  of Yb3+ ions. The basic properties of this core glass were evaluated. LMA DCF and LMA PCF were prepared from this core glass. The 51% optical–optical efficiency wad realized in Yb3+-doped silica LMA DCF. We acquired 81 W laser output from Yb3+-doped silica LMA PCF, with a slope efficiency of 70.8%. To the best of our knowledge, this is the highest laser output power report for Yb3+-doped silica LMA PCF prepared by the sol–gel method.
2. Experimental Section
Starting from the sol–gel method, we made a fiber preform core glass rod sized Φ 5 × 80 mm with a composition of 0.1 Yb2O3–1.0 Al2O3–98.9 SiO2 (moL%). The preparation processing has been published in our previous work [11,12]. Slice glass cut from this rod with 2 mm thickness was used to test absorption spectrum, emission spectrum, fluorescent lifetime and refractive index. FTIR spectrum in 400–4000 cm−1 was detected to evaluate the residual hydroxyl in glass. Double cladding fiber preform was prepared by rod in tube method and Yb3+-doped silica LMA DCF was drawn in 2000 °C with plastic coating. It has a core diameter of 48 µm with core NA of 0.08, and outer diameter of 340 µm with NA of 0.46. Yb3+-doped silica LMA PCF was prepared by the stack-capillary-draw method at the drawing temperature of 2000 °C. It has a core diameter of 90 μm, and the outer diameter is 720 μm without plastic coating. The core NA is 0.08; and the inner cladding NA is 0.22.
To assess the homogeneity of the dopant distribution in the fiber core, the radial refractive index distribution of single cladding fiber prepared from the same core glass was measured (S14 Refractive Index Profiler, Photon Kinetics, Beaverton, USA). The transmission loss of the fiber core was also measured on the single cladding fiber by the standard cut back technique. The laser behaviors of both DCF and PCF fiber were tested on setup shown in Figure 1. The details are discussed in the succeeding sections.
3. Results and Discussion
3.1. Optical Properties of Yb3+-Doped Al2O3–SiO2 Glass
Figure 2a shows the absorption and emission cross-sections of Yb3+-doped Al2O3–SiO2 slice glass calculated using the Beer-Lambert equation  and Fuchbauer-Ladenburger method (F-L) , according to the measured absorption and fluorescence spectra, respectively. The maximum absorption cross section (σabs) at 976 nm is 2.4 pm2, and the emission cross section (σemi) near 1025 nm is 0.8 pm2. The corresponding fluorescence lifetime at 1025 nm is 896 µs by single exponent fitting of the measured photoluminescence decay curve. As can be seen from the FTIR spectrum shown in Figure 2b, there is almost no absorption peak at 2700 nm due to lower hydroxyl (OH) content. The hydroxyl content in our glass is calculated to be 1.45 ppm according to the method in reference .
|Table 1. Spectral parameters of Yb3+-doped silica glass derived from different preparation methods.|
|σabs (976 nm) (pm2)||2.4||2.7||1.74|
|σemi (~1 µm) (pm2)||0.8||~0.6|
Table 1 lists spectral parameters of Yb3+-doped silica glass derived from different preparation methods for comparison. It is found that Yb:Al:SiO2 glass prepared in this work shows longer fluorescent lifetime and higher stimulated emission cross section compared with those prepared by MCVD and other sol–gel method . The hydroxyl content (1.45 ppm) in our glass is compatible with that obtained in silica fiber prepared by Heraeus Conpany (2 ppm) and MCVD method (0.5 ppm).
3.2. Optical Loss Profile and Homogeneity of Yb3+-Doped Al2O3–SiO2 Fiber
In order to assess the homogeneity of core glass, the single cladding fiber was drawn using the same Al3+, Yb3+ co-doped silica glass as the core. The radial refractive index distribution of the fiber core was measured and shown in Figure 3a. The maximum refractive index fluctuation Δn in the core is smaller than 2 × 10−4. It indicates good optical homogeneity of the fiber core prepared by sol–gel method. Figure 3b shows the optical loss of the fiber core. The background attenuation at 1200 nm is 0.41 dB/m. Furthermore, there is an additional attenuation band at 1383 nm caused by OH. The OH-content of the fiber core is calculated to be 26 ppm from this absorption band . It is higher than that in slice glass (1.45 ppm). This may be caused by moisture during the fiber drawing process.
3.3. Laser Behavior of Yb3+-Doped Al2O3–SiO2 LMA DCF and PCF Fibers
A 976 nm laser diode pigtailed with a spot diameter of 400 μm and NA of 0.22 was used as pump source for both double cladding and PCF fibers. The pump light was collimated and focused by a couple of lenses (Figure 1) and then entered into the inner cladding of either LMA DCF or PCF fiber. The resonator is formed by a dichromatic mirror and the cleave fiber end. The dichromatic mirror is butt-coupled to the incident end of the fiber, which possesses high reflectivity (R > 99%) at 1040 nm and high transmittance (T > 99%) at 976 nm. The filter mirror (T > 99 at 1040 nm, R > 99% at 976 nm) is used when laser power is measured by the power meter.
Laser performance of a 5.5 m long LMA DCF Yb3+-doped Al2O3–SiO2 fiber was tested and its output versus input curve is given in Figure 4. The output power was limited to 30W due to the limit of pumping source. The slope efficiency of 54% and “light-to-light” conversion efficiency of 51% were achieved in this fiber. The overall absorption coefficient (including background loss) of the DCF at the pump wavelength (976 nm) was tested to be 1.6 dB/m.
The laser experiment was carried out on a 210-cm-long Yb3+-doped Al2O3–SiO2 LMA PCF. The overall absorption coefficient (including background loss) of the fiber at the pump wavelength (976 nm) was tested to be 3 dB/m.
Figure 5a shows laser spectrum of Al3+, Yb3+ co-doped silica LMA PCF. The laser wavelength is at 1040–1070 nm. The inset shows the laser mode pattern in the far field. It is multimode. The micrograph of LMA PCF cross section is given in the inset of Figure 5b. Figure 5b indicates the laser input-output curve of LMA PCF. The slope efficiency is 70.8%. The laser threshold is approximately 18.8 W evaluated from the linear fitting. The maximum output power is limited to 81 W by the available pumping power. At this laser lever, we did not observe the photodarkening in our silica fiber. But codoping moderate P2O5 with Al2O3 in Yb3+-doped silica fiber is necessary to greatly suppress photodarkening effect when the fiber is operating continuously at high-power. Further work to reduce optical loss and improve mode quality of output laser is continued.
Large-size 0.1 Yb2O3–1.0 Al2O3–98.9 SiO2 (mol%) silica fiber preform core glass sized Φ 5 × 80 mm was prepared by the sol–gel method. The spectral properties of this glass were discussed. The maximum absorption cross section (σabs) at 976 nm is 2.4 pm2, and the emission cross section (σemi) near 1025 nm is 0.8 pm2. The fluorescence lifetime at 1025 nm is 896 µs. Evaluated by single cladding fiber, the refractive index homogeneity of fiber core prepared from above core glass reaches 2 × 10−4; and the optical loss at 1200 nm is about 0.41 dB/m. The corresponding LMA DCF and LMA PCF were prepared by rod in tube and stack-capillary-draw, respectively. The NA values of core and cladding are 0.08 and 0.46 for LMA DCF. The NA values of the core and inner cladding are 0.08 and 0.22 for LMA PCF. The absorption coefficients of the LMA DCF and PCF at the pump wavelength (976 nm) are 1.6 dB/m and 3 dB/m, respectively. Slope efficiency of 54% and “light-to-light” conversion efficiency of 51% were achieved in Yb3+-doped silica LMA DCF. The maximum output power was limited to 81 W by the available pumping power with a slope efficiency of 70.8% in Yb3+-doped silica LMA PCF fiber .To the best of our knowledge, this is the highest laser power report for Yb3+-doped silica LMA PCF prepared by the sol–gel method.
This research is financially supported by the Chinese National Natural Science Foundation (No. 60937003).
Conflicts of Interest
The authors declare no conflict of interest.
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