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 - Funding Information:
A.K.I and J.H. contributed equally to this work. A.K.I, J.H., D.G., V.G., and M.G.K. acknowledge the Air Force Office of Scientific Research grant number FA9550-18-S-0003. J.H. also received partial support from the National Science Foundation through the Penn State 2D Crystal Consortium-Materials Innovation Platform (2DCC-MIP) under NSF cooperative agreement DMR-2039351. The IMSERC PCM facility at Northwestern University used in this work received support from the Soft and Hybrid Nanotechnology Experimental (SHyNE) Resource (NSF ECCS-2025633). D.Y.C and M.G.K. acknowledges that the work at Argonne (material purification and crystal growth) was supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences, and Engineering Division. Scientific discussions and advice from Gary Cook, Carl M. Liebig, Ryan K. Feaver, and Sean A. McDaniel of the Air Force Research Laboratory (AFRL) are gratefully acknowledged.
Funding Information:
A.K.I and J.H. contributed equally to this work. A.K.I, J.H., D.G., V.G., and M.G.K. acknowledge the Air Force Office of Scientific Research grant number FA9550‐18‐S‐0003. J.H. also received partial support from the National Science Foundation through the Penn State 2D Crystal Consortium‐Materials Innovation Platform (2DCC‐MIP) under NSF cooperative agreement DMR‐2039351. The IMSERC PCM facility at Northwestern University used in this work received support from the Soft and Hybrid Nanotechnology Experimental (SHyNE) Resource (NSF ECCS‐2025633). D.Y.C and M.G.K. acknowledges that the work at Argonne (material purification and crystal growth) was supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences, and Engineering Division. Scientific discussions and advice from Gary Cook, Carl M. Liebig, Ryan K. Feaver, and Sean A. McDaniel of the Air Force Research Laboratory (AFRL) are gratefully acknowledged.
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.
KW - chalcogenides
KW - crystals
KW - Infrared laser
KW - polymorphic transitions
KW - Second Harmonic Generation
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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 -