TY - JOUR
T1 - Emission and absorption cross-sections of Mg/Er-codoped near-stoichiometric LiNbO3crystals
AU - Zhang, De Long
AU - Gao, Jian
AU - Vallés, Juan Antonio
AU - Xu, Chao
AU - Sun, Liang
AU - Xu, Yu Heng
AU - Pun, Edwin Yue Bun
PY - 2010
Y1 - 2010
N2 - Near-stoichiometric (NS) (Mg:) LiNbO3crystals crystals were grown from melts (Li2O]n}[Nb2O5]=1:1) containing 0.0/0.5, 0.5/0.5, and 1.0/0.5 mol%/mol% MgO/Er2O 3. OH absorption study shows that the optical damage threshold Mg concentration of the Er/Mg-codoped NS crystal is just near 1.0 mol%. Polarized visible and near infrared, and unpolarized mid-infrared (2. 7μ4I11/2→413/2) emission spectra of Er3+ ion in these crystals were measured. From measured emission spectra, the emission and absorption cross-section spectra were calculated based upon McCumber theory, and compared with the data of congruent Er:LiNbO3 bulk material and/or Ti-diffused Er:LiNbO3 strip waveguide and the results obtained from the direct unpolarized optical absorption measurements. The 550, 980, and 1530 nm emission lifetimes were also measured, and compared with the Judd-Ofelt theoretical values and the measured values of the congruent material. The results show that the polarized absorption cross-section data derived from the emission spectra are comparable to the unpolarized cross-section data from direct absorption measurements. The emission and absorption cross-sections, their polarization dependences as well as the lifetime all change definitely as the crystal composition shifts from the congruent point to the near-stoichiometry. In the NS crystal, the Er 3+ ion has smaller emission and absorption cross-sections, and longer lifetimes. In contrast, MgO codoping has less effect on the emission and absorption cross-sections, and lifetime.
AB - Near-stoichiometric (NS) (Mg:) LiNbO3crystals crystals were grown from melts (Li2O]n}[Nb2O5]=1:1) containing 0.0/0.5, 0.5/0.5, and 1.0/0.5 mol%/mol% MgO/Er2O 3. OH absorption study shows that the optical damage threshold Mg concentration of the Er/Mg-codoped NS crystal is just near 1.0 mol%. Polarized visible and near infrared, and unpolarized mid-infrared (2. 7μ4I11/2→413/2) emission spectra of Er3+ ion in these crystals were measured. From measured emission spectra, the emission and absorption cross-section spectra were calculated based upon McCumber theory, and compared with the data of congruent Er:LiNbO3 bulk material and/or Ti-diffused Er:LiNbO3 strip waveguide and the results obtained from the direct unpolarized optical absorption measurements. The 550, 980, and 1530 nm emission lifetimes were also measured, and compared with the Judd-Ofelt theoretical values and the measured values of the congruent material. The results show that the polarized absorption cross-section data derived from the emission spectra are comparable to the unpolarized cross-section data from direct absorption measurements. The emission and absorption cross-sections, their polarization dependences as well as the lifetime all change definitely as the crystal composition shifts from the congruent point to the near-stoichiometry. In the NS crystal, the Er 3+ ion has smaller emission and absorption cross-sections, and longer lifetimes. In contrast, MgO codoping has less effect on the emission and absorption cross-sections, and lifetime.
KW - emission and absorption cross-sections
KW - near-stoichiometric LiNbO crystalscrystal
KW - photorefractive effect
UR - https://www.scopus.com/pages/publications/77955144900
U2 - 10.1109/JQE.2010.2050863
DO - 10.1109/JQE.2010.2050863
M3 - 文章
AN - SCOPUS:77955144900
SN - 0018-9197
VL - 46
SP - 1332
EP - 1341
JO - IEEE Journal of Quantum Electronics
JF - IEEE Journal of Quantum Electronics
IS - 9
M1 - 5518512
ER -