• Acta Physica Sinica
  • Vol. 68, Issue 2, 024208-1 (2019)
Min-Qiang Gai1、2, Ying Wang1, and Shi-Lie Pan1、*
Author Affiliations
  • 1CAS Key Laboratory of Functional Materials and Devices for Special Environments, Xinjiang Key Laboratory of Electronic Information Materials and Devices, the Xinjiang Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Urumqi 830011, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.7498/aps.68.20182145 Cite this Article
    Min-Qiang Gai, Ying Wang, Shi-Lie Pan. Exploration of the deep-ultraviolet nonlinear optical materials in the derivatives of KBe2BO3F2[J]. Acta Physica Sinica, 2019, 68(2): 024208-1 Copy Citation Text show less
    Crystal structure model of KBBF family.KBBF族晶体结构模型
    Fig. 1. Crystal structure model of KBBF family.KBBF族晶体结构模型
    Second harmonic generation evolution from KBBF to Pb2BO3I.从KBBF 到Pb2BO3I的倍频效应演进
    Fig. 2. Second harmonic generation evolution from KBBF to Pb2BO3I. 从KBBF 到Pb2BO3I的倍频效应演进
    Ball-and-stick representations of NH4Be2BO3F2(ABBF)[79,80].NH4Be2BO3F2 (ABBF)晶体结构模型[79,80]
    Fig. 3. Ball-and-stick representations of NH4Be2BO3F2(ABBF)[79,80]. NH4Be2BO3F2 (ABBF)晶体结构模型[79,80]
    Ball-and-stick representations of AZn2BO3X2 (A = K, Rb, NH4) series[63−81]: (a) NH4Zn2BO3Cl2; (b) KZn2BO3Cl2; (c) RbZn2BO3Cl2.AZn2BO3X2 (A = K, Rb, NH4)系列晶体结构模型[63−81] (a) NH4Zn2BO3Cl2; (b) KZn2BO3Cl2; (c) RbZn2BO3Cl2
    Fig. 4. Ball-and-stick representations of AZn2BO3X2 (A = K, Rb, NH4) series[6381]: (a) NH4Zn2BO3Cl2; (b) KZn2BO3Cl2; (c) RbZn2BO3Cl2. AZn2BO3X2 (A = K, Rb, NH4)系列晶体结构模型[6381]  (a) NH4Zn2BO3Cl2; (b) KZn2BO3Cl2; (c) RbZn2BO3Cl2
    Ball-and-stick representations of KABO series[50−52]: (a) K2Al2B2O7; (b) -Rb2Al2B2O7.KABO系列晶体结构模型[50−52] (a) K2Al2B2O7; (b) -Rb2Al2B2O7
    Fig. 5. Ball-and-stick representations of KABO series[5052]: (a) K2Al2B2O7; (b) -Rb2Al2B2O7. KABO系列晶体结构模型[5052]  (a) K2Al2B2O7; (b) -Rb2Al2B2O7
    Ball-and-stick representations of Ba3Mg3(BO3)3F3[87]: (a) Sr2Be2B2O7; (b) Ba3Mg3(BO3)3F3.Ba3Mg3(BO3)3F3晶体结构模型[87] (a) Sr2Be2B2O7; (b) Ba3Mg3(BO3)3F3
    Fig. 6. Ball-and-stick representations of Ba3Mg3(BO3)3F3[87]: (a) Sr2Be2B2O7; (b) Ba3Mg3(BO3)3F3. Ba3Mg3(BO3)3F3晶体结构模型[87]  (a) Sr2Be2B2O7; (b) Ba3Mg3(BO3)3F3
    Ball-and-stick representations of Sr2Be2B2O7 and BaAl2B2O7.Sr2Be2B2O7和BaAl2B2O7晶体结构模型
    Fig. 7. Ball-and-stick representations of Sr2Be2B2O7 and BaAl2B2O7. Sr2Be2B2O7和BaAl2B2O7晶体结构模型
    Ball-and-stick representations of K3Sr3Li2Al4B6O20F and K3Ba3Li2Al4B6O20F (KBLABF).K3Sr3Li2Al4B6O20F和K3Ba3Li2Al4B6O20F (KBLABF)的晶体结构模型
    Fig. 8. Ball-and-stick representations of K3Sr3Li2Al4B6O20F and K3Ba3Li2Al4B6O20F (KBLABF). K3Sr3Li2Al4B6O20F和K3Ba3Li2Al4B6O20F (KBLABF)的晶体结构模型
    Relationship of active group balance of fluorooxoborates among bandgap, NLO coefficient and birefringence[68].氟化硼酸盐的活性基团平衡“倍频效应-透过范围-双折射率”的关系[68]
    Fig. 9. Relationship of active group balance of fluorooxoborates among bandgap, NLO coefficient and birefringence[68]. 氟化硼酸盐的活性基团平衡“倍频效应-透过范围-双折射率”的关系[68]
    Crystal structures of the MB4O6F family[92].MB4O6F族氟化硼酸盐的晶体结构[92]
    Fig. 10. Crystal structures of the MB4O6F family[92]. MB4O6F族氟化硼酸盐的晶体结构[92]
    Crystal structures of the series borates contain B—O covalent bond.层间由B—O共价键连接的系列硼酸盐晶体结构
    Fig. 11. Crystal structures of the series borates contain B—O covalent bond.层间由B—O共价键连接的系列硼酸盐晶体结构
    化合物空间群结构层间连接紫外截止边/nmdeff (KDP)或dij/pm·V—1
    注: 上标a为计算值.
    NaBe2BO3F2[20]C2 [Be2BO3F2]Na+—F155deff = 1.7 × deff (NH4H2PO4)
    KBe2BO3F2[20]R32 [Be2BO3F2]K+—F147d11 = 0.47 ± 0.01
    RbBe2BO3F2[21]R32 [Be2BO3F2]Rb+—F160d11 = 0.45 ± 0.01
    CsBe2BO3F2[22]R32 [Be2BO3F2]Cs+—F151d11 = 0.5
    NH4Be2BO3F2[48]R32 [Be2BO3F2]N—H·F1531.2
    \begin{document}$\gamma $\end{document}-Be2BO3F[48]R32 [Be2BO3F2]Be2+—F144.82.3
    RbZn2BO3Cl2[63,81]R32 [Zn2BO3Cl2]Rb+—Cl1982.9
    KZn2BO3Cl2[63,81]R32 [Zn2BO3Cl2]K+—Cl1933.0
    NH4Zn2BO3Cl2[63]R32 [Zn2BO3Cl2]N—H·Cl1862.8
    Be2(BO3)F[43]C2 [Be2BO3F2]Be2+—F150a0.25
    BaBe2BO3F3[43]P63[Be2BO3F2]Ba2+—F< 1850.1
    K2Al2B2O7[50,52]P321 [Al3B3O6]Al3+—O2−1800.45
    K2(1-x)Na2xAl2BO7[88](0 < x < 0.6) P321 [Al3B3O6]Al3+—O2−1800.45
    K2(1−x)Rb2xAl2B2O7[82] (0 < x < 0.75) P321 [Al3B3O6]Al3+—O2−0.7
    K0.67Rb1.33Al2B2O7[83]P321 [Al3B3O6]Al3+—O2−1880.9
    \begin{document}$\beta$\end{document}-Rb2Al2B2O7[51]P321 [Al3B3O6]Al3+—O2−< 2002.0
    BaAlBO3F2[84]\begin{document}$ P{\overline 6}2c$\end{document}[AlBO3F2]Ba2+—F1652.0
    Rb3Al3B3O10F[54]P31c [Al3(BO3)OF]Al3+—FAl3+—O2−< 2001.2
    BaZnBO3F[64]\begin{document}$ P{\overline 6}$\end{document}[ZnBO3F]Zn2+—O2−3 × deff
    Ba3Mg3(BO3)3F3[87]Pna21[Mg3O2F3(BO3)2]Ba2+—F184d33 = 0.51
    Table 1.

    Cmparison of structural and optical properties of some deep-UV NLO materials of KBBF family with adjacent layers connected by ionic bond and hydrogen bond.

    层间含有离子键和氢键连接的类KBBF结构硼酸盐深紫外NLO材料的结构和光学性能比较

    化合物空间群结构层间连接紫外截止边/nm倍频效应(KDP)或dij//pm·V−1
    Sr2Be2B2O7[39]\begin{document}$ P{\overline 6}c2$\end{document}[Be2(BO3)2O]Sr2+—O2−1552.5
    Ba2Be2B2O7[40,73]\begin{document}$ P{\overline 6}2c$\end{document}[Be2(BO3)2O]Ba2+—O2−2152.0
    BaAl2B2O7[52]R32 [Al6B6O12]Al3+—O2−d11 = 0.75
    NaCaBe2B2O6F[41]Cc[Be3B3O6F3]Ca2+—O2−1900.3
    K3Ba3Li2Al4B6O20F[55]\begin{document}$ P{\overline 6}2c$\end{document}[Li2Al4B6O20F]Ba2+—O2−1901.5
    Rb3Ba3Li2Al4B6O20F[89]\begin{document}$ P{\overline 6}2c$\end{document}[Li2Al4B6O20F]Ba2+—O2−1951.4
    K3Sr3Li2Al4B6O20F[57]R32 [Li2Al4B6O20F]Sr2+—O2−1901.7 (0.9)
    Cs2Al2(B3O6)2O[90]P63[Al2(B3O6)2O] Al3+—O2−185d31 = 0.032
    Table 2.

    Comparison of structural and optical properties of some deep-UV NLO materials of SBBO family.

    SBBO型硼酸盐深紫外NLO材料的结构和光学性能比较

    化合物空间群结构层间连接方式紫外截止边/nm倍频效应(KDP)
    NH4B4O6F[69]Pna21[B4O6F]N—H·F1563.0
    CsB4O6F[71]Pna21[B4O6F]Cs+—F1551.9
    RbB4O6F[70]Pna21[B4O6F]Rb+—F< 1900.8
    CsKB8O12F2[70]P321 [B4O6F]Cs/K+—F< 1901.9
    CsRbB8O12F2[70]\begin{document}$ P{\overline 6}2c$\end{document}[B4O6F]Cs/K+—F< 1901.1
    NaB4O6F[72]C2 [B4O6F]Na+—F< 1800.9
    SrB5O7F3[98]Cmc21[B5O7F3]Sr2+—F< 1801.6
    Sr2B10O14F6[99]< 2002.5
    CaB5O7F3[97]Cmc21[B5O7F3]Ca2+—F< 1802.0
    Ca2B10O14F6[99]< 2002.3
    Table 3.

    Comparison of structural and optical properties of some fluorooxoborates deep-UV NLO materials.

    部分氟化硼酸盐深紫外NLO材料的结构和光学性能比较

    化合物空间群结构层间连接方式紫外截止边/nm倍频效应(KDP)
    \begin{document}$ \beta $\end{document}-KBe2B3O7[44]Pmn21[Be2BO5][BO2]< 2000.75
    \begin{document}$\gamma $\end{document}-KBe2B3O7[44]P21[Be2BO5][B3O6] < 2000.68
    RbBe2B3O7[44]Pmn21[Be2BO5][BO2]< 2000.79
    Na2CsBe6B5O15[45]C2 [Be2BO5][BO3] < 2001.17
    Na2Be4B4O11[46]P1 [Be2BO5][B2O5] 1711.30
    LiNa5Be12B12O23[46]Pc[Be2BO5][B2O5] 1691.40
    Li4Sr(BO3)2[67]Cc[SrBO3][B2O3] 1862.00
    Table 4.

    Comparison of structural and optical properties of some deep-UV NLO materials of KBBF family with adjacent layers connected by rigid B—O groups.

    层间含有B—O共价键连接的类KBBF结构硼酸盐深紫外NLO材料的结构和光学性能比较

    Min-Qiang Gai, Ying Wang, Shi-Lie Pan. Exploration of the deep-ultraviolet nonlinear optical materials in the derivatives of KBe2BO3F2[J]. Acta Physica Sinica, 2019, 68(2): 024208-1
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