TY - GEN
T1 - A Polarization Maintaining Cladding Light Stripper with Ultra-low Backscattering, Based on 20/400-mm Double Clad Fiber
AU - Kim, Jihwan
AU - Lee, Ju Han
N1 - Publisher Copyright:
© 2025 IEEE.
PY - 2025
Y1 - 2025
N2 - High-power optical fiber laser systems are currently widely used in various applications such as materials processing, medicine, and defense [1]. High-power optical fiber laser technologies employ large mode area (LMA), double clad fibers (DCFs) to increase output power by using a cladding pumping scheme [2]. For the successful implementation of LMA DCF-based high power fiber lasers one of the key components is the cladding light stripper (CLS). It is well-known that a non-negligible amount of residual pump power always exists at the output end of a gain medium based on rare-earth ion-doped LMA DCF after the launched pump beam was used to induce stimulated emission. The residual pump beam together with undesired signal beam within the inner cladding of a LMA DCF is known to degrade output beam quality and potentially damage fiber splicing points. In implementing CLSs, one critical issue is the backward scattering of cladding light since it can induce fiber heating and burning [3]. It was also reported that conventional CLS designs based on randomly roughened surface structures or periodically V-grooved structures are vulnerable to the residual pump backscattering [4, 5].
AB - High-power optical fiber laser systems are currently widely used in various applications such as materials processing, medicine, and defense [1]. High-power optical fiber laser technologies employ large mode area (LMA), double clad fibers (DCFs) to increase output power by using a cladding pumping scheme [2]. For the successful implementation of LMA DCF-based high power fiber lasers one of the key components is the cladding light stripper (CLS). It is well-known that a non-negligible amount of residual pump power always exists at the output end of a gain medium based on rare-earth ion-doped LMA DCF after the launched pump beam was used to induce stimulated emission. The residual pump beam together with undesired signal beam within the inner cladding of a LMA DCF is known to degrade output beam quality and potentially damage fiber splicing points. In implementing CLSs, one critical issue is the backward scattering of cladding light since it can induce fiber heating and burning [3]. It was also reported that conventional CLS designs based on randomly roughened surface structures or periodically V-grooved structures are vulnerable to the residual pump backscattering [4, 5].
UR - https://www.scopus.com/pages/publications/105016253610
U2 - 10.1109/CLEO/EUROPE-EQEC65582.2025.11109674
DO - 10.1109/CLEO/EUROPE-EQEC65582.2025.11109674
M3 - Conference contribution
AN - SCOPUS:105016253610
T3 - 2025 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference, CLEO/Europe-EQEC 2025
BT - 2025 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference, CLEO/Europe-EQEC 2025
PB - Institute of Electrical and Electronics Engineers Inc.
T2 - 2025 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference, CLEO/Europe-EQEC 2025
Y2 - 23 June 2025 through 27 June 2025
ER -