TY - JOUR
T1 - Passively Q-switched 1.56 μm all-fiberized laser based on evanescent field interaction with bulk-structured bismuth telluride topological insulator
AU - Koo, Joonhoi
AU - Lee, Junsu
AU - Chi, Cheolhwan
AU - Lee, Ju Han
PY - 2014/9/1
Y1 - 2014/9/1
N2 - We experimentally investigated the use of a bulk-structured bismuth telluride (Bi2Te3) topological insulator (TI) as a saturable absorption material for passive Q-switching of a fiber laser at ∼1.56 μm. Unlike previous TI-based Q-switched laser implementations that employed high-quality nanostructured TI saturable absorbers, we chose to use a bulk-structured Bi2Te3 TI film because it is easy to fabricate. Our saturable absorber was constructed by depositing a bulk-structured, ∼13 μm thick Bi2Te3 TI film, which was prepared by using a mechanical exfoliation method, on the flat side of a side-polished fiber. The modulation depth of the evanescent field interaction-based saturable absorber was measured to be ∼10.8% at ∼1.56 μm. Passively Q-switched pulses were readily obtained by incorporating the saturable absorber into an all fiberized erbium fiber-based ring cavity. The minimum temporal width was measured to be ∼2.81 μs at a repetition rate of ∼42.8 kHz. Through an output performance comparison between our Q-switched laser and recently demonstrated Q-switched fiber lasers incorporating nanostructured TI-based saturable absorbers, the pros and cons of our bulk-structured Bi2Te3 TI-based saturable absorbers were analyzed.
AB - We experimentally investigated the use of a bulk-structured bismuth telluride (Bi2Te3) topological insulator (TI) as a saturable absorption material for passive Q-switching of a fiber laser at ∼1.56 μm. Unlike previous TI-based Q-switched laser implementations that employed high-quality nanostructured TI saturable absorbers, we chose to use a bulk-structured Bi2Te3 TI film because it is easy to fabricate. Our saturable absorber was constructed by depositing a bulk-structured, ∼13 μm thick Bi2Te3 TI film, which was prepared by using a mechanical exfoliation method, on the flat side of a side-polished fiber. The modulation depth of the evanescent field interaction-based saturable absorber was measured to be ∼10.8% at ∼1.56 μm. Passively Q-switched pulses were readily obtained by incorporating the saturable absorber into an all fiberized erbium fiber-based ring cavity. The minimum temporal width was measured to be ∼2.81 μs at a repetition rate of ∼42.8 kHz. Through an output performance comparison between our Q-switched laser and recently demonstrated Q-switched fiber lasers incorporating nanostructured TI-based saturable absorbers, the pros and cons of our bulk-structured Bi2Te3 TI-based saturable absorbers were analyzed.
UR - http://www.scopus.com/inward/record.url?scp=84906880312&partnerID=8YFLogxK
U2 - 10.1364/JOSAB.31.002157
DO - 10.1364/JOSAB.31.002157
M3 - Article
AN - SCOPUS:84906880312
SN - 0740-3224
VL - 31
SP - 2157
EP - 2162
JO - Journal of the Optical Society of America B: Optical Physics
JF - Journal of the Optical Society of America B: Optical Physics
IS - 9
ER -