journal article·2022-02

Nonlinear optical properties of a new polar bismuth tellurium oxide fluoride, Bi3F(TeO3)(TeO2F2)3

Jee Yoon Chung, Seongbeom Yeon, Hongsun Ryu, Tae-Soo You, Joon I. Jang, Kang Min Ok

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Abstract

Abstract A novel noncentrosymmetric polar bismuth tellurium oxide fluoride, Bi3F(TeO3)(TeO2F2)3, has been hydrothermally synthesized by using Bi2O3, TeO2, and HF solution at 230 °C. The structural backbone of Bi3F(TeO3)(TeO2F2)3 is composed of several polyhedra with lone pair cations, such as BiO6F3, TeO2F2, and TeO3. The asymmetric geometric features found from the polyhedra of Bi3+ and Te4+ should be attributed to the lone pairs on the cations. The overall framework of Bi3F(TeO3)(TeO2F2)3 can be considered as a three-dimensional hexagonal tungsten oxide-like topology. The UV-vis diffuse reflectance spectral data suggest that the title compound has a wide band gap of ca. 3.85 eV due to the distortions of the asymmetric units, as well as the electronegative fluoride anions. Second-harmonic generation (SHG) measurements using a 1064 nm radiation indicate that Bi3F(TeO3)(TeO2F2)3 reveals a nonphase-matching behavior and ca. 9 times larger SHG counts than that of α-SiO2. The near-static value of the second-order nonlinear optical susceptibility, χS(2), of the reported compound is calculated to be ca. 5.1 ± 0.6 pm/V. The wavelength-dependent SHG measurements indicate that the SHG counts of Bi3F(TeO3)(TeO2F2)3 decrease as the excitation wavelength increases from 1064 to 1600 nm.
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Research context

OpenAlex topics: Crystal Structures and Properties · Inorganic Fluorides and Related Compounds · High-pressure geophysics and materials

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References (48)

Show source-provided references
1. Parametric generation of tunable picosecond pulses in the medium infrared using AgGaS2 crystals10.1063/1.94782 ↗
2. Nonlinear optical materials10.1126/science.253.5017.281 ↗
3. Deep-UV nonlinear optical crystal KBe2BO3F2—discovery, growth, optical properties and applications10.1007/s00340-009-3554-4 ↗
4. Hot charge-transfer excitons set the time limit for charge separation at donor/acceptor interfaces in organic photovoltaics10.1038/nmat3500 ↗
5. Deep ultraviolet nonlinear optical materials10.1021/acs.chemmater.6b02366 ↗
6. Chemistry-Inspired adaptable framework structures10.1021/acs.accounts.7b00033 ↗
7. Learning from a mineral structure toward an ultra-narrow-band blue-emitting silicate phosphor RbNa3(Li3 SiO4)4:Eu210.1002/anie.201807087 ↗
8. Noncentrosymmetric oxides10.1021/cm980140w ↗
9. Bulk characterization methods for non-centrosymmetric materials: second-harmonic generation, piezoelectricity, pyroelectricity, and ferroelectricity10.1039/b511119f ↗
10. Noncentrosymmetric YVSe2O8 and centrosymmetric YVTe2O8: macroscopic centricities influenced by the size of lone pair cation linkers10.1021/ic402929m ↗
11. A cation size effect on the framework structures in ABi2SeO3F5 (A = K and Rb): first examples of alkali metal bismuth selenite fluorides10.1039/C8DT00450A ↗
12. Remarkable multimember-ring configurations in a new family of Na7MIISb5S12 (MII = Zn, Cd, Hg) exhibiting various three-dimensional tunnel structures10.1039/C8CC04639E ↗
13. Functional layered materials with heavy metal lone pair cations, Pb2+, Bi3+, and Te4+10.1039/C9CC06778G ↗
14. Unique synthesis, structure determination, and optical properties of seven new layered rare earth tellurite nitrates, RE(TeO3)(NO3) (RE = La, Nd, Eu, Gd, Dy, Er, and Y10.1016/j.jallcom.2020.156855 ↗
15. ACdCO3F (A = K and Rb): new noncentrosymmetric materials with remarkably strong second-harmonic generation (SHG) responses enhanced via π-interaction10.1039/C5RA17209H ↗
16. Hydrogen bonding assisted construction of graphite-like deep-UV optical materials with two types of parallel π-conjugated units10.1021/acs.cgd.8b00804 ↗
17. SrB5O7F3 functionalized with [B5O9F3]6- chromophores: accelerating the rational design of deep-ultraviolet nonlinear optical materials10.1002/anie.201802058 ↗
18. Refractive index modulates second-harmonic responses in RE8O(CO3)3(OH)15X (RE = Y, Lu; X = Cl, Br): rare-earth halide carbonates as ultraviolet nonlinear optical materials10.1021/acs.chemmater.9b00068 ↗
19. Layered bismuth oxyfluoride nitrates revealing large second-harmonic generation and photocatalytic properties10.1021/acs.inorgchem.8b03343 ↗
20. Place of death and factors associated with hospital death in patients who have died from liver disease in England: a national population-based study10.1021/acs.chemmater.8b04428 ↗
21. Zeolitic open-framework borates with noncentrosymmetric structures and nonlinear optical properties10.1021/acs.inorgchem.9b00101 ↗
22. Toward the rational design of novel noncentrosymmetric materials: factors influencing the framework structures10.1021/acs.accounts.6b00452 ↗
23. Bi3(SeO3)3(Se2O5)F: a polar bismuth selenite fluoride with polyhedra of highly distortive lone pair cations and strong second-harmonic generation response10.1021/acs.chemmater.0c02167 ↗
24. Targeting the next generation of deep-ultraviolet nonlinear optical materials: expanding from borates to borate fluorides to fluorooxoborates10.1021/acs.accounts.8b00649 ↗
25. Hydroxyfluorooxoborate Na[B3O3F2(OH)2]⋅[B(OH)3]: optimizing the optical anisotropy with heteroanionic units for deep ultraviolet birefringent crystals10.1002/anie.202107291 ↗
26. SHELXS-2013/1, A program for the solution of crystal structures
27. Acta crystallogr
28. Kubelka · Z. Tech. Phys. · 1931 · 12 · 593
29. Absorption edge and internal electric fields in amorphous semiconductors10.1016/0025-5408(70)90112-1 ↗
30. A powder technique for the evaluation of nonlinear optical materials10.1063/1.1656857 ↗
31. Outstanding laser damage threshold in Li2MnGeS4 and tunable optical nonlinearity in diamond-like semiconductors10.1021/ic502981r ↗
32. Linear methods in band theory10.1103/PhysRevB.12.3060 ↗
33. Doxapram (Dopram)10.1103/PhysRevLett.53.2571 ↗
34. Minimal basis sets in the linear muffin-tin orbital method: application to the diamond-structure crystals C, Si, and Ge10.1103/PhysRevB.34.2439 ↗
35. O. Jepsen, A. Burkhardt, O.K. Andersen, in, Max-Plank-Institut fur Festkorperforschung, Shuttgart, Germany, 1999.
36. Andersen · 1985
37. Calculated electronic structure of the sandwichd 1 metals LaI2 and CeI2: application of new LMTO techniques10.1007/BF01317585 ↗
38. VESTA 3for three-dimensional visualization of crystal, volumetric and morphology data10.1107/S0021889811038970 ↗
39. Improved tetrahedron method for Brillouin-zone integrations10.1103/PhysRevB.49.16223 ↗
40. Bond-valence parameters obtained from a systematic analysis of the Inorganic Crystal Structure Database10.1107/S0108768185002063 ↗
41. Bond-valence parameters for solids10.1107/S0108768190011041 ↗
42. New bismuth selenium oxides: syntheses, structures, and characterizations of centrosymmetric Bi2(SeO3)2(SeO4) and Bi2(TeO3)2(SeO4) and noncentrosymmetric Bi(SeO3)(HSeO3)10.1021/ic4002384 ↗
43. Layered bismuth oxyfluoride nitrates revealing large second-harmonic generation and photocatalytic properties10.1021/acs.inorgchem.8b03343 ↗
44. Ba(MoO2F)2(XO3)2 (X = Se and Te): first cases of noncentrosymmetric fluorinated molybdenum oxide selenite/tellurite through unary substitution for enlarging band gaps and second harmonic generation10.1021/acsami.0c15444 ↗
45. New anion-conducting solid solutions Bi1−xTex(O,F)2+δ (x>0.5) and glass–ceramic material on their base10.1016/j.jfluchem.2011.06.042 ↗
46. Sidgwick · Proc. Roy. Soc. A · 1940 · 176 · 153
47. The electron-pair repulsion model for molecular geometry10.1021/ed047p18 ↗
48. Non-phase-matched optical third-harmonic generation in noncentrosymmetric media: Cascaded second-order contributions for the calibration of third-order nonlinearities10.1103/PhysRevB.61.10688 ↗