“…Very little work has been reported in the area of tellurite fiber lasers at wavelengths beyond 1560 nm, where there is a high demand for new compact laser systems with medium power for applications, such as chemical and remote sensing, medicine, atmospheric monitoring, and eye-safe lidar. A 1.57 mE r 3+ -doped silica fiber laser was previously been used to pump Tm 3+ ions in a silica fiber to produce lasing at 1.9 m. In this case the 1.57 m pump was very close to the absorption peak of the Tm 3+ : 3 H 6 → 3 F 4 transition, and a slope efficiency of 71% was achieved [6]. The low phonon energy of tellurite glass compared to silicate hosts is manifested by prolonged lifetimes of the 3 F 4 level in tellurite, which is 2.4 ms compared with 630 si n silicates, and suggests that a laser device based on a tellurite fiber should have a lower laser threshold and higher slope efficiency for a ϳ2 m laser.…”
“…Very little work has been reported in the area of tellurite fiber lasers at wavelengths beyond 1560 nm, where there is a high demand for new compact laser systems with medium power for applications, such as chemical and remote sensing, medicine, atmospheric monitoring, and eye-safe lidar. A 1.57 mE r 3+ -doped silica fiber laser was previously been used to pump Tm 3+ ions in a silica fiber to produce lasing at 1.9 m. In this case the 1.57 m pump was very close to the absorption peak of the Tm 3+ : 3 H 6 → 3 F 4 transition, and a slope efficiency of 71% was achieved [6]. The low phonon energy of tellurite glass compared to silicate hosts is manifested by prolonged lifetimes of the 3 F 4 level in tellurite, which is 2.4 ms compared with 630 si n silicates, and suggests that a laser device based on a tellurite fiber should have a lower laser threshold and higher slope efficiency for a ϳ2 m laser.…”
“…Tm-doped fibers with low output power (<20mW). pumped near 1.6 µm, with slope efficiency as high as 71 % (for silica fibers [15]) and 84 % (for fluoride fibers [16]) have been reported previously. As far as we are aware, this approach for power scaling of Tm-doped fiber lasers has not attracted much interest, perhaps, because it requires a high power Er,Yb fiber source.…”
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PERFORMING ORGANIZATION NAME(S) AND ADDRESS(ES)University of Southampton Southampton SO17 1BJ United Kingdom
PERFORMING ORGANIZATION REPORT NUMBERN/A
SPONSOR/MONITOR'S ACRONYM(S) 9. SPONSORING/MONITORING AGENCY NAME(S) AND ADDRESS(ES)EOARD PSC 821 BOX 14 FPO 09421-0014
SPONSOR/MONITOR'S REPORT NUMBER(S)Grant 03-3057
DISTRIBUTION/AVAILABILITY STATEMENTApproved for public release; distribution is unlimited.
SUPPLEMENTARY NOTES
ABSTRACTThis report results from a contract tasking University of Southampton as follows: The Grantee will investigate a) optimization of the claddingpumped Er-Yb doped fiber laser (EYDFL) for efficient pumping of Tm-doped fibers. b) Investigation of core-pumping of Tm-doped fibers using the EYDFL developed in task a, c) design, fabrication and demonstration of a high-power, core-pumped, multimode Tm-doped fiber laser, and d) demonstration of high-power, single-mode output from the core-pumped Tm-doped fiber laser.
SUBJECT TERMS
“…They can efficiently pumped at ∼ 790, ∼ 1200, or ∼ 1600 nm [14][15][16][17] , similar to the case of ytterbium erbium doped fiber [19][20]. In this paper, a thulium ytterbium co-doped fiber laser (TYDFL) is demonstrated by using a newly developed double-clad Tm 3+ /Yb 3+ co-doped alumino-silicate fiber (TYDF) as a gain medium.…”
19 ions/cc, respectively. The fiber laser operates at wavelength of 1948.4 and 1947.2 nm with pump power thresholds of 0.6 and 1.0 W for 915 and 940 nm pumping, respectively. The maximum output power of 10.5 mW was achieved with the 915 nm pumping at the maximum pump power of 1.5 W. It is found that the laser is more efficient with 915 nm pumping compared to 940 nm pumping.
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