Preparation of Ho³⁺/Tm³⁺ Co-doped Lanthanum Tungsten Germanium Tellurite Glass Fiber and Its Laser Performance for 2.0 μm

Abstract

Ho³⁺/Tm³⁺ co-doped 50TeO₂-25GeO₂-3WO₃-5La₂O₃-3Nb₂O₅-5Li₂O-9BaF₂ glass fiber is prepared with the rod-tube drawing method of 15 μm core diameter and 125 μm inner cladding diameter applied in the 2.0 μm-infrared laser. The 2.0 μm luminescence properties of the core glass are researched and the fluorescence intensity variation for different Tm³⁺ doping concentration is systematically analyzed. The results show that the 2.0 μm luminescence of Ho³⁺ is greatly influenced by the doping concentration ratio of Ho³⁺ to Tm³⁺ and that the maximum fluorescence intensity of the core glass can be obtained and its emission cross section can reach 0.933 × 10⁻²¹ cm² when the sensitized proportion of holmium to thulium is 0.3 to 0.7 (mol%). Simultaneously, the maximum phonon energy of the core glass sample is 753 cm⁻¹, which is significantly lower than that of silicate, gallate and germanate glass and the smaller matrix phonon energy can be conductive to the increase 2.0 μm-band emission intensity. The continuous laser with the maximum laser output power of 0.993 W and 2051 nm -wavelength of 31.9%-slope efficiency is output within the 0.5 m glass fiber and the experiment adopts 1560 nm erbium-doped fiber laser(EDFL) as the pump source and the self-built all-fiber laser. Therefore, the glass fiber has excellent laser characteristics and it is suitable for the 2.0 μm-band laser.

Introduction

Compared with conventional solid and gas lasers, fiber lasers have many advantages, such as good beam quality, high efficiency, good cooling effect, simple structure and easy operation, and it has become the research focus in the field of laser in recent years^1,2,3. Especially, mid-infrared fiber lasers within 2.0 μm-band have broad application prospects and important applications in the long-range laser communications, laser-guided, optoelectronics confrontation, remote sensing, laser surgery of a new generation and other medical and military fields because its laser wavelength is placed in the atmosphere transmission window and it is harmless to the human eyes^4,5,6,7. Currently, Tm³⁺ and Ho³⁺ are the main active ions to produce 2.0 μm band laser and the radiative transitions of Tm³⁺ ion from energy level ³F₄ to ³H₆ and Ho³⁺ ion from ⁵I₇ to ⁵I₈ are one of the effective ways to achieve mid-infrared emission of 2.0 μm-wavelength^8,9.

Typically, the tuning range is from 1.87 μm to 2.16 μm for the solid laser with the single Tm³⁺-doped as the luminescent center, and the fluorescence lifetime of the Tm³⁺ ion is very long, which is conducive to high energy Q-switched laser output. However, higher pumping energy is required to overcome the high threshold power due to the small stimulated emission cross section and quasi-three-level structure for Tm³⁺ at room temperature, which easily leads to excited state absorption of Tm³⁺ and causes inversion consumption^10,11. Compared with Tm³⁺ ions, the stimulated emission cross section of Ho³⁺ is approximately five times as that of Tm³⁺ and the fluorescence lifetime is up to 8ms, which facilitates storage. However, in the single Ho³⁺-doped glass, laser generation efficiency is relatively low because of the non-radiative transitions dominance and Ho³⁺ ions does not correspond to absorption energy levels of 808 nm and 980 nm bands, which lacks of effective pumping source, thereby the single Ho³⁺-doped fiber laser applicability is reduced^12,13. In order to better improve the Ho³⁺ laser performance of 2.0 μm, the sensitized technology is employed usually to improve the luminous efficiency, therefore, researchers began to work on a multi-ions co-doped fiber laser.

The reports of the Tm³⁺-doped, Ho³⁺-doped and Ho³⁺/Tm³⁺ co-doped 2.0 μm luminescent materials focus on the quartz glass, silicate glass, fluoride glass, sulfide glass, tellurite glass and germanate glass^{14,15,16,17,18}. In 1994, Ghisler et al. Of Bern University in Switzerland implemented the laser output of 2.04 μm with 809 nm AlGaAs laser diode pumping Ho³⁺/Tm³⁺ co-doped silica fiber firstly, however, the laser output power was only 5.8 mW. Until 2008, Jackson et al. of University of Manchester adopted a 793 nm semiconductor laser to pump Ho³⁺/Tm³⁺ co-doped double-clad silica fibers and obtained a 83-W, 2.015-μm laser output with a slope efficiency of 42%. This is the current highest record for Ho³⁺/Tm³⁺ co-doped laser. In 2009, PFMoulton et al. reported a 885 W multimode laser output with a center wavelength of 2.04 μm and a slope efficiency of 49.2%, using a 790 nm diode-pumped double-clad Tm³⁺-doped quartz fiber, which is the current maximum laser output power for the 2.0 μm band Tm³⁺ -doped quartz fiber. Although the output power of 885 W for the 2.0 μm band laser has been realized in Tm³⁺ -doped quartz glass, the quartz glass substrate has the characteristics of high phonon energy, the non-radiative transition energy loss due to multi-phonon relaxation at lower energy level occupies a dominant position, leading to the decrease of radiation quantum efficiency and fluorescence quenching effect, which is disadvantageous to the miniaturization and high gain of fiber lasers and this limits the further improvement of the performance of the 2.0 μm band quartz fiber lasers^19,20. Although fluoride and sulfide substrate glass have lower phonon energy, they have some defects, such as poor chemical stability and mechanical properties, difficult preparation, splice difficulties with standard quartz fiber and low laser damage threshold^21,22. The tellurite glass and the germanate glass have a greater solubility for the rare earth ions, the doping concentration of rare earth ions is high with high refractive index, good chemical stability and thermal stability, which is suitable for drawing the fiber. Instantaneously, its relatively low phonon energy can effectively inhibit the non-radiation transitions of rare earth ions to improve the luminous efficiency for the Ho³⁺/Tm³⁺ co-doped 2.0 μm band^23,24,25,26. Therefore, the tellurite glass and the germanate glass are ideal gain matrix materials of fiber laser.

In recent years, there are some research reports of 2.0 μm-band spectroscopic properties for the Ho³⁺/Tm³⁺ co-doped germanate glass or tellurite glass, but there are few reports for that of Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber. Therefore, the Ho³⁺/Tm³⁺ ions co-doped lanthanum tungsten germanium tellurite glass fiber is prepared with the rod-tube drawing method, based on the Ho³⁺/Tm³⁺ ions co-doped lanthanum tungsten germanium tellurite glass formulations of 50TeO₂-25GeO₂-3WO₃-5La₂O₃-3Nb₂O₅-5Li₂O-9BaF₂, the spectrum properties of prepared fiber is researched, the influences of 2.0 μm luminescence intensity for the different doping concentrations are discussed and the 2051 nm mid-infrared laser output is implemented in the Ho³⁺/Tm³⁺ ions co-doped lanthanum tungsten germanium tellurite glass fiber with self-designed all-fiber laser.

Experiments

Glass melting and fiber preparation

A group of lanthanum tungsten germanium tellurite glasses with good physical and chemical properties are selected as the matrix materials for the fiber core and cladding based on the extensive literature^{27,28,29,30,31} and experimental work. The formulations for the core and cladding glass are 50TeO₂-25GeO₂-3WO₃-5La₂O₃-3Nb₂O₅-5Li₂O-9BaF₂-xTm³⁺-0.3Ho³⁺ and 39TeO₂-36GeO₂- 3WO₃-5La₂O₃-3Nb₂O₅-5Li₂O-9BaF₂ respectively. The doping concentration x (mol%) of the Tm³⁺ in the core glass material are 0.3, 0.5, 0.7 and 1.0 and the obtained core glass samples are numbered by C₁, C₂, C₃ and C₄, while the cladding glass sample is numbered by C₅. All preparation materials of the sample glasses are weighed precisely as the formulations and mixed, which are of analytical reagent grade, stirred evenly and placed in a platinum crucible, then melted for an hour at about 1300 °C in an electric furnace with silicon molybdenum rods heating, after that the clarified molten glass is cast in a preheated steel mold for forming, and then quickly shift to the muffle furnace to anneal precisely, keep the temperature close to the glass transition temperature of T_g for 3 hours and then the temperature is down to the room temperature at the speed of 10 °C/h. The quenched glasses are cut, ground and polished and the samples are made as a glass block with both sides polished of 10 mm × 10 mm × 2 mm, a core rod and a cladding tube. The glass block is used for the spectra, while the core rod and cladding tube are assembled as the rod and tube composing, drawing with the rod and tube combination methods.

The drawing technique process with the rod-tube assembly is as follows. Firstly, the core glass rod is put into the cladding glass tube and pulled to a preform with 5 mm-diameter with the optical fiber drawing machine. The preform is placed again in the cladding glass tube for drawing. Eventually, it formed a core diameter of 15 μm, cladding diameter of 125 μm of Ho³⁺/Tm³⁺ ions co-doped lanthanum tungsten germanium tellurite glass fiber is prepared with the twice drawing method. Nitrogen, helium and argon simultaneously protected in the fiber drawing process.

Performance Testing

The reflection index of the glass bulk sample is measured by the prism coupler. Characteristic temperature is measured with the differential scanning calorimetry (DSC) method and the measurement instrument employs the TAS-100-type thermal analyzer of the Japanese Rigaku Corporation. Absorption spectrum is measured by the Lambda-950-type spectrophotometer with measurement range of 400 nm–2200 nm. Raman spectra measurement employs the inVia Raman microscope of the British Renishaw Company, whose measurement range is from 100 cm⁻¹ to 2000 cm⁻¹ and the excitation wavelength is 532 nm. Fluorescence spectroscopy measurement adopts the Triax320-type fluorescence spectrometer of French J-Y Company, semiconductor laser pump source of 808 nm is pumped with 2 W-power when measured and the transmitted signal is amplified by the detector, monochromator and lock-in amplifier and the fluorescence decay curve is recorded. The laser output spectrum of the experimental drawn Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber is measured by the self-designed all-fiber laser, the 1560 nm erbium-doped fiber laser (EDFL) is selected as the pump source with pump power of 3 W when measured and the output laser after collimation is input to the spectrum analyzer through the attenuator to record the laser spectroscopy. All of the above measurements are carried out at the room temperature if no special instructions.

Results and Discussions

Matching and differential thermal analysis of material properties

Fiber core glass and cladding glass refractive index matching is a problem to be considered firstly for the fiber design and the refractive index of the core glass is generally higher than that of the cladding glass³². In this study, the reflective index of the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite core glass and cladding glass samples are given in Table 1. From Table 1, the refractive index of glass samples is increased gradually with the increasing of rare earth ions’ concentration and decreased with the increasing of the GeO₂, wherein the refractive index difference between the core and the cladding glass is in the range of 0.0268–0.0298, thus the light wave-guide transmission conditions are satisfied in the optical fiber and the optical fiber with the theoretical numerical aperture of 0.3293 or more can be matched.

Table 1 The refractive index and characteristics temperature of the glass samples.

The differential thermal of the glass samples is measured to study their thermal stability, the temperature range is from 200 °C to 1000 °C. Thermodynamic stability of the glass is commonly measured with the difference between the T_x and Tg, that is ΔT = T_x − T_g, where T_g is the transition temperature of glass and T_x is the crystallization initiation temperature. Greater value of ΔT means better thermal stability of the glass and the specific data are listed in Table 1. It can be seen from Table 1 that ΔT of all the glass samples are greater than 150 °C, which means that the lanthanum tungsten germanium tellurite glass has good thermal stability and the difference of the transition temperatures between the core and cladding glass does not exceed 35 °C to meet the drawing temperature unanimous requests of the lanthanum tungsten germanium tellurite glass fiber and be suitable for drawing. Furthermore, it can also be seen from Table 1 that ΔT increases from 162 °C to 177 °C when GeO₂ content is increased from 25% to 36%. Experiments show that the increase of the GeO₂ content in the glass matrix helps improve the thermal stability of lanthanum tungsten germanium tellurite glass and expands the drawing scope of the lanthanum tungsten germanium tellurite glass fiber.

In order to prevent the optical fiber burst due to too much thermal stress and the fiber cladding partial loss because of the weak bond of the core and cladding glass interface during the drawing process, the general requirements for thermal expansion coefficient difference between the core and cladding glass is no more than ± 20 × 10⁻⁷/°C to ensure the mechanical strength and the geometry structure integrity of the optical fiber³³. As it can be seen from Table 1 of the thermal expansion coefficient of α-data that the maximum difference of the thermal expansion coefficients between the core and cladding glass is 11.7 × 10⁻⁷/°C, which is in full compliance with the requirements of fiber drawing. The above data analysis shows that the performance matching of the core and cladding glass is good and the experimental designed core and cladding matrix glass is very suitable for the preparation of glass fiber.

Analysis of absorption spectrum

Figure 1 shows the absorption spectrum in the range of 400 nm–2200 nm of the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite core glass sample and the corresponding excited state energy level has been marked in the figure. It can be seen from Fig. 1 that there are six main absorption bands of the Ho³⁺ ion in the glass sample and the wavelengths are located at the peak of 1953 nm, 1178 nm, 646 nm, 539 nm, 460 nm and 420 nm, which correspond to the absorption transition of Ho³⁺ ion from the ground level of ⁵I₈ to the excited state levels of ⁵I₇, ⁵I₆, ⁵F₅, (⁵S₂, ⁵F₄), ⁵F₃ and ⁵G₆, while the energy levels absorption of the other excited states have been overshadowed by the matrix absorption. There are four important absorption bands of the Tm³⁺ ion in the glass sample, the wavelengths are located at the 1680 nm, 1210 nm, 793 nm ad 687 nm, which correspond to the absorption transition of Tm³⁺ from the ground level of ³H₆ to the excited state levels of ³F₄, ³H₅, ³H₄ and ³F_2.3, while the energy levels absorption of the other excited states have been overshadowed by the matrix absorption. The energy level of Tm³⁺:³F₄ which transmits energy has a very obvious, alone absorption peak, which lays a good foundation for the energy level of Ho³⁺:⁵I₇ which receives energy to produce 2.0 μm-laser. In addition, since there also is an alone obvious absorption peak in the vicinity of 793 nm-wavelength for the Tm³⁺, the drawn fiber glass sample can choose a lower-cost 808 nm- wavelength laser pump source of LD for the effective pumping.

Figure 1

The absorption spectra of the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass.

It can also be observed from Fig. 1 that the intensity of the absorption peaks gradually increase and the absorption peaks gradually strengthen of Ho³⁺ as Tm³⁺ doping concentration increases. The absorption peak is strongest when Tm³⁺ ion concentration is 1.0 mol%. The intensity of the absorption is maximum when the Ho³⁺/Tm³⁺ concentration ratio (mol%) is 0.3 to 1.0, while the each absorption peak shape and intensity of Ho³⁺ have no significant changes, which indicates that the different doping ratios for Ho³⁺ to Tm³⁺ has little influences for the 2.0 μm absorption of Ho³⁺ ion. In addition, the spectrum shape and the absorption peak position of the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass are similar to those of the other oxyfluoride and fluorine germanate glass matrix reported in the literature^16,17.

Fluorescence spectroscopy and Raman spectroscopy

Figure 2 is the fluorescence spectra for the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite core glass pumped at the 808 nm-wavelength LD. From Fig. 2, there are three fluorescence emission bands of 1.47 μm, 1.80 μm and 2.0 μm in the range of 1300 nm–2200 nm, which correspond to the energy level transitions from ³H₄ to ³F₄, from ³F₄ to ³H₆ of the Tm³⁺ ion and from ⁵I₇ to ⁵I₈ of the Ho³⁺ ion. It can be seen clearly from Fig. 2 that when the doping concentration of the Ho³⁺ remains 0.3 mol%, the intensity change of 1.47 μm-fluorescence produced by the ³H₄ to ³F₄ energy level transition of the Tm³⁺ is smaller as the increasing of the Tm³⁺ concentration and the transition peak of the 1.80 μm caused by the ³F₄ to ³H₆ energy level transition of the Tm³⁺ is in a strengthening trend, while the intensity of 2.0 μm-fluorescence generated by ⁵I₇ to ⁵I₈ energy level transition of Ho³⁺ increases sharply. Figure 1 of the absorption spectra shows that Ho³⁺ ions has no significant absorption for the 808 nm pumping light, and therefore 2.0 μm luminescence is only from Tm³⁺ energy transfer, which indicates that there exists a strong energy transfer process between Tm³⁺(³F₄) and Ho³⁺(⁵I₇). The fluorescence intensity reaches maximum in the vicinity of 2.0 μm for the Ho³⁺ of sample C₃ when the doping concentration of Tm³⁺ ions reaches 0.7 mol%. However, when Tm³⁺-doped concentration reaches 1.0 mol%, the sensitization of Ho³⁺ decreases due to the Tm³⁺ concentration quenching effect, the anti-cross relaxation effect of ions and the reverse energy transfer from Ho³⁺(⁵I₇) to Tm³⁺(³F₄), thus, the 2.0 μm-fluorescence intensity of C₄ sample begins to decrease significantly. This shows that there exists an optimal sensitized ratio of 0.3 to 0.7 for the Ho³⁺/Tm³⁺ ions co-doped of lanthanum tungsten germanium tellurite glass matrix and the fluorescence spectra intensity decreases significantly when the sensitized ratio exceeds it.

Figure 2

The fluorescence spectra of Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite core glass.

Figure 3 shows the Raman spectra of glass samples C₃ and it can be seen from the figure that there are four Raman peaks located at the positions of 346 cm⁻¹, 463 cm⁻¹, 679 cm⁻¹, and 753 cm⁻¹. Raman characteristic peak of 346 cm⁻¹ corresponds to W-O-W bending vibration in the octahedron of [WO₆], Raman characteristic peak of 463 cm⁻¹ corresponds to the symmetric bending vibration of Te-O-Te bond and stretching vibration of O-Ge-O in [GeO₄], Raman characteristic peak of 679 cm⁻¹ belongs to the biconical stretching vibration in [TeO₄], and Raman characteristic peak of 753 cm⁻¹ corresponding to the maximum phonon energy, belongs to the stretching vibration of O-Ge-O bond in [GeO₆] and the tripartite cone stretching vibration in [TeO₃] or [TeO₃₊₁]. Therefore, the maximum phonon energy of the glass sample C₃ is 753 cm⁻¹ and it is significantly lower than that of the silicate glass, gallate glass and germanate glass^34,35,36. As for the Ho³⁺ and Tm³⁺ co-doped 2.0 μm-emitting, such low phonon energy can reduce the non-radiative transition probability of multi-phonon, which helps to increase the 2.0 μm-band emission intensity.

Figure 3

The Raman spectroscopy of the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass.

Calculation and comparative analysis for the spectral parameters

Judd-Ofelt theory is usually employed to calculate the spectral strength parameters (Ω₂, Ω₄, Ω₆) of the rare earth ions in different glass matrix to analyze the ordering of the glass structure, symmetry of rare earth ions ligand field and so on. It is generally believed that the greater Ω₂ means the lower symmetry and stronger covalence of the material rare earth ions ligand field, the greater Ω6 indicates the weaker covalence of the glass rare earth ions and anions, while the ratio of Ω₄ to Ω₆ determines the spectral quality of the matrix glass^22,37.

According to the absorption spectroscopy obtained by experiments, the J-O theory is employed to calculate the line parameters of Ho³⁺ ions in the sample C₃ and they are compared with the spectral parameters of different glass matrix with the values listed in Table 2. Table 2 shows that the value of Ω₂ of Ho³⁺ in the lanthanum tungsten germanium tellurite glass is 6.13 × 10⁻²⁰ cm², much larger than that of the germanate, tellurite and silicate glass, which indicates that the covalence of the glass is relatively stronger, the symmetry of the glass rare earth ions and ligand field is lower to be excited easily. While, the value of Ω₆ of Ho³⁺ in the lanthanum tungsten germanium tellurite glass is 1.39 × 10⁻²⁰ cm², greater than that of silicate, gallate and germanate, but lower than that of tellurite and fluorophosphate glass, which indicates that non-bridging oxygen ions of the lanthanum tungsten germanium tellurite glass is less than that of the tellurite glass and fluorophosphate glass, therefore, the stability of the system is preferably better than that of the tellurite glass and fluorophosphate glass. The spontaneous emission transition probability from ⁵I₇ energy level to ⁵I₈ energy level for the Ho³⁺ in the glass sample C₃ of Ar is calculated as 259.13 s⁻¹ with the calculated spectral intensity parameter values, which is close to the parameter data reported in the literature²² and has higher spontaneous radiative transition probability compared with the other fluorophosphate, gallate, germanate and silicates listed in Table 2, meaning that the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass can produce stronger 2.0 μm-fluorescence emission.

Table 2 The comparison of the spectra parameters for Ho³⁺ in different glass matrix.

The doped rare earth ions absorption cross-section of and the stimulated emission cross section of of the Lanthanum tungsten germanium tellurite glass can be calculated from the absorption spectra measured in the Fig. 1 and the Lambert-Beer law and McCumber theory.

where, I₀ is the incident light intensity, I is the transmitted light intensity, N is the number of the doped rare earth ions per unit volume, L is the thickness of the sample (which is 2 mm), ε is the free energy of the rare earth ions transition from the ground state to the excited state, λ is the emission light wavelength, k is the Boltzmann constant, h is Planck’s constant, c is the light speed and T is the sample temperature. Figure 4 shows the absorption and emission cross section of Ho³⁺ near 2.0 μm. Figure 4 shows that the maximum absorption cross section of the Ho³⁺ ions in the C₃ glass sample is located at the 1953 nm-wavelength of  = 8.109 × 10⁻²¹ cm² and the maximum emission cross section is located at 2051 nm-wavelength of  = 0.933 × 10⁻²¹ cm². It can be seen from Fig. 4 and Table 2 that C₃ glass sample have the largest absorption cross section and the largest emission cross section, which are bigger than those of tellurite glass and are nearly double of the other fluorophosphate, gallate and germanate glasses. This is determined by the higher refractive index of the lanthanum tungsten germanium tellurite glass because the glass substrate with a larger refractive index can produce higher spontaneous emission transition probabilities and larger emission cross sections. Therefore, C₃ glass sample is expected to become an important matrix material of 2.0 μm fiber laser.

Figure 4

2.0 μm-absorption and emission cross section for Ho³⁺ of lanthanum tungsten germanium tellurite glass.

Testing and analysis of the laser performances

The laser output characteristics of the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber is tested and analyzed using self-built all-fiber laser and the pumping source selects erbium-doped fiber lasers with the output wavelength of 1560 nm. In this study, a multimode fiber grating with 90%-reflectance is employed as a pre-mirror and a single-mode fiber grating with 10%-reflectance is employed as a post-mirror, thereby, a laser resonator is constituted. The gain fiber of the seed source is the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber of C₃ drawn in the experiment. The fiber grating is written directly with a phase mask method at a length of 0.5 m of Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber³⁹. Since the diameter of the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber is different from the diameter of erbium-doped fiber laser pigtail, a tapered fiber is used in the experiment in order to ensure high efficient welding couple, and the fusion technology is employed to achieve the low-loss connections between the optical fibers and the high efficiency pump laser power delivery, thus ensuring high pump light coupling efficiency.

The EDFL pumping power is 3 W and the output laser of the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber laser is collimated, input to the spectrum analyzer by the attenuator and measured by the laser spectroscopy. The output laser spectrum is shown in Fig. 5. As can be seen from Fig. 5 that the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber can produce laser with a wavelength of 2051 nm. The relationship curve between the laser output power and the into-fiber pumping power measured by the optical power meter is shown in Fig. 6. Experimental results show that there is laser output when the input pumping threshold power reaches 0.336 W. When the pumping power is 2.97 W, the maximum output power generated by the laser is 0.993w with the slope efficiency of 31.9%. It can be seen from Fig. 6 that there is a good linear relationship between the laser output power and input pumping power and there is no saturation phenomenon when the maximum output power of the laser reaches 0.993w. The fiber in the article is compared with the Ho³⁺/Tm³⁺ double-doped laser fiber of similar data and attribute and its laser output power and slope efficiency are higher than those of the fiber reported in the literature^40,41,42,43, showing that the optical fiber with the Ho³⁺/Tm³⁺ co-doped makes full use of the photo-sensitivity of Tm³⁺ and on the other hand the doping concentration of Ho³⁺ ions is reduced, thereby reducing the laser re-absorption. Therefore, high concentration of Tm³⁺ and Ho³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber can achieve higher laser output power and slope efficiency, which has excellent laser characteristics.

Figure 5

The output laser spectrum of the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber laser.

Figure 6

The output power curve of the Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber laser.

Conclusions

The Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber with the excellent thermal stability and optical properties is prepared. Studies have found that 2.0 μm-band fluorescence emission intensity is maximum with its emission cross section of 0.933 × 10⁻²¹ cm² when the molar concentration ration of Ho³⁺ to Tm³⁺ reaches 0.3:0, 7 in the lanthanum tungsten germanium tellurite core glass with system of 50TeO₂-25GeO₂-3WO₃-5La₂O₃-3Nb₂O₅-5Li₂O-9BaF₂. This is the highest emission cross section of the Ho³⁺/Tm³⁺ ions co-doped germanium tellurite glass in current reports and the emission cross section of the glass is nearly doubled as that of the other fluorophosphate, gallate and germanate glass. In addition, the maximum phonon energy of the lanthanum tungsten germanium tellurite glass samples is 753 cm⁻¹, which is significantly lower than that of the silicate, gallate and germanate glasses. As for the 2.0 μm luminous of the Ho³⁺ and Tm³⁺ co-doped glass, the results show that the lower phonon energy can reduce the non-radiative transition probability of multi-phonons, which is conducive to increase 2.0 μm-band emission intensity.

A 1560 nm-pumped 2.0 μm-band Ho³⁺/Tm³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber laser is self-built during laser performance testing. The 2051 nm-laser output is achieved with this laser. Laser testing finds that the laser threshold power is 0.336 W at this length. When the pumping power is 2.97 W, the maximum output power of the laser is 0.993w and the slope efficiency is 31.9%. Comparative analysis of the drawn Ho³⁺/Tm³⁺ ions co-doped lanthanum tungsten germanium tellurite glass fiber with the tellurite and germanate glasses of similar properties find that high concentrations of Tm³⁺ and Ho³⁺ co-doped lanthanum tungsten germanium tellurite glass fiber can get higher laser output power and slope efficiency, which has excellent laser characteristics and is an ideal mid-infrared laser material.