TY - JOUR
T1 - Stabilization of the Polar Structure and Giant Second-Order Nonlinear Response of Single Crystal γ-NaAs0.95Sb0.05Se2
AU - Iyer, Abishek K.
AU - He, Jingyang
AU - Xie, Hongyao
AU - Goodling, Devin
AU - Chung, Duck Young
AU - Gopalan, Venkatraman
AU - Kanatzidis, Mercouri G.
N1 - Publisher Copyright:
© 2022 Wiley-VCH GmbH.
PY - 2023/2/23
Y1 - 2023/2/23
N2 - The dearth of suitable materials significantly restricts the practical development of infrared (IR) laser systems with highly efficient and broadband tuning. Recently, γ-NaAsSe2 is reported, and it exhibits a large nonlinear second-harmonic generation (SHG) coefficient of 590 pm V−1 at 2 µm. However, the crystal growth of γ-NaAsSe2 is challenging because it undergoes a phase transition to centrosymmetric δ-NaAsSe2. Herein, the stabilization of non-centrosymmetric γ-NaAsSe2 by doping the As site with Sb, which results in γ-NaAs0.95Sb0.05Se2 is reported. The congruent melting behavior is confirmed by differential thermal analysis with a melting temperature of 450 °C and crystallization temperature of 415 °C. Single crystals with dimensions of 3 mm × 2 mm are successfully obtained via zone refining and the Bridgman method. The purification of the material plays a significant role in crystal growth and results in a bandgap of 1.78 eV and thermal conductivity of 0.79 Wm−1 K−1. The single-crystal SHG coefficient of γ-NaAs0.95Sb0.05Se2 exhibits an enormous value of |d11| = 648 ± 74 pm V−1, which is comparable to that of γ-NaAsSe2 and ≈20× larger than that of AgGaSe2. The bandgap of γ-NaAs0.95Sb0.05Se2 (1.78 eV) is similar to that of AgGaSe2, thus rendering it highly attractive as a high-performing nonlinear optical material.
AB - The dearth of suitable materials significantly restricts the practical development of infrared (IR) laser systems with highly efficient and broadband tuning. Recently, γ-NaAsSe2 is reported, and it exhibits a large nonlinear second-harmonic generation (SHG) coefficient of 590 pm V−1 at 2 µm. However, the crystal growth of γ-NaAsSe2 is challenging because it undergoes a phase transition to centrosymmetric δ-NaAsSe2. Herein, the stabilization of non-centrosymmetric γ-NaAsSe2 by doping the As site with Sb, which results in γ-NaAs0.95Sb0.05Se2 is reported. The congruent melting behavior is confirmed by differential thermal analysis with a melting temperature of 450 °C and crystallization temperature of 415 °C. Single crystals with dimensions of 3 mm × 2 mm are successfully obtained via zone refining and the Bridgman method. The purification of the material plays a significant role in crystal growth and results in a bandgap of 1.78 eV and thermal conductivity of 0.79 Wm−1 K−1. The single-crystal SHG coefficient of γ-NaAs0.95Sb0.05Se2 exhibits an enormous value of |d11| = 648 ± 74 pm V−1, which is comparable to that of γ-NaAsSe2 and ≈20× larger than that of AgGaSe2. The bandgap of γ-NaAs0.95Sb0.05Se2 (1.78 eV) is similar to that of AgGaSe2, thus rendering it highly attractive as a high-performing nonlinear optical material.
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U2 - 10.1002/adfm.202211969
DO - 10.1002/adfm.202211969
M3 - Article
AN - SCOPUS:85144287403
SN - 1616-301X
VL - 33
JO - Advanced Functional Materials
JF - Advanced Functional Materials
IS - 9
M1 - 2211969
ER -