Symmetry overChemistry: Harmonic Generation of Low-DimensionalAlkali Chalcopnictates RbMP<sub>2</sub>S<sub>6</sub> (M = Sb, Bi)

We have discovered RbSbP<sub>2</sub>S<sub>6</sub> and β-RbBiP<sub>2</sub>S<sub>6</sub>, two alkali chalcopnictates that crystallize as one-dimensional chains. These near-isostructural analogs differ primarily in the coordination environment of the central metal: Sb has a coordination number (CN) of 4, while Bi exhibits a CN of 5. Notably, β-RbBiP<sub>2</sub>S<sub>6</sub> is another form of a Rb/Bi/P/S compound with a 1126 stoichiometry. The β-phase, detailed in this work, is synthesized via direct combination, whereas the previously reported α-phase forms through a reactive Rb/Bi salt flux. The α- and β-phases also differ primarily by the Bi coordination sphere: α-phase Bi CN = 7; β-phase Bi CN = 5. RbSbP<sub>2</sub>S<sub>6</sub> and β-RbBiP<sub>2</sub>S<sub>6</sub> are both semiconductors. RbSbP<sub>2</sub>S<sub>6</sub> has a bandgap of 2.68 eV while β-RbBiP<sub>2</sub>S<sub>6</sub> has a bandgap of 2.06 eV. Neither material is congruently melting, but both have successfully been grown into large single crystals via slow cooling of the melt. Nonlinear optical (NLO) results in powder samples show that the symmetry breaking, which leads to lower dimensionality, also leads to significantly lower second harmonic generation (SHG) intensity (∼0.1x AgGaSe<sub>2</sub> for β-RbBiP<sub>2</sub>S<sub>6</sub> vs ∼12x AgGaS<sub>2</sub> for α-RbBiP<sub>2</sub>S<sub>6</sub>). Third Harmonic Generation (THG) in powder samples show similar intensities (∼0.3x AgGaSe<sub>2</sub> for β-RbBiP<sub>2</sub>S<sub>6</sub> and ∼0.1x AgGaSe<sub>2</sub> for RbSbP<sub>2</sub>S<sub>6</sub>). These are corroborated by single crystal SHG results for β-RbBiP<sub>2</sub>S<sub>6</sub> (∼0.5x AgGaSe<sub>2</sub>). The nonzero NLO coefficients <i>d</i><sub>14</sub>, <i>d</i><sub>25</sub>, and <i>d</i><sub>36</sub> at 1550 nm fundamental wavelength are measured to be 9.5 ± 2.4, 17.2 ± 3.2, and 3.6 ± 2.3 pm/V, respectively. β-RbBiP<sub>2</sub>S<sub>6</sub> has a comparable laser-induced damage threshold (LIDT) to AgGaSe<sub>2</sub> while RbSbP<sub>2</sub>S<sub>6</sub> has a LIDT approximately 3x that of β-RbBiP<sub>2</sub>S<sub>6</sub> attributed to its higher bandgap.

Publication Details

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Figshare
Published
2025-03-21
DOI
https://doi.org/10.1021/acs.chemmater.5c00140.s003
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Crystal Structures and Properties
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Symmetry overChemistry: Harmonic Generation of Low-DimensionalAlkali Chalcopnictates RbMP2S6 (M = Sb, Bi)

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Crystal Structures and Properties
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Symmetry overChemistry: Harmonic Generation of Low-DimensionalAlkali Chalcopnictates RbMP2S6 (M = Sb, Bi)

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Abstract

We have discovered RbSbP<sub>2</sub>S<sub>6</sub> and β-RbBiP<sub>2</sub>S<sub>6</sub>, two alkali chalcopnictates that crystallize as one-dimensional chains. These near-isostructural analogs differ primarily in the coordination environment of the central metal: Sb has a coordination number (CN) of 4, while Bi exhibits a CN of 5. Notably, β-RbBiP<sub>2</sub>S<sub>6</sub> is another form of a Rb/Bi/P/S compound with a 1126 stoichiometry. The β-phase, detailed in this work, is synthesized via direct combination, whereas the previously reported α-phase forms through a reactive Rb/Bi salt flux. The α- and β-phases also differ primarily by the Bi coordination sphere: α-phase Bi CN = 7; β-phase Bi CN = 5. RbSbP<sub>2</sub>S<sub>6</sub> and β-RbBiP<sub>2</sub>S<sub>6</sub> are both semiconductors. RbSbP<sub>2</sub>S<sub>6</sub> has a bandgap of 2.68 eV while β-RbBiP<sub>2</sub>S<sub>6</sub> has a bandgap of 2.06 eV. Neither material is congruently melting, but both have successfully been grown into large single crystals via slow cooling of the melt. Nonlinear optical (NLO) results in powder samples show that the symmetry breaking, which leads to lower dimensionality, also leads to significantly lower second harmonic generation (SHG) intensity (∼0.1x AgGaSe<sub>2</sub> for β-RbBiP<sub>2</sub>S<sub>6</sub> vs ∼12x AgGaS<sub>2</sub> for α-RbBiP<sub>2</sub>S<sub>6</sub>). Third Harmonic Generation (THG) in powder samples show similar intensities (∼0.3x AgGaSe<sub>2</sub> for β-RbBiP<sub>2</sub>S<sub>6</sub> and ∼0.1x AgGaSe<sub>2</sub> for RbSbP<sub>2</sub>S<sub>6</sub>). These are corroborated by single crystal SHG results for β-RbBiP<sub>2</sub>S<sub>6</sub> (∼0.5x AgGaSe<sub>2</sub>). The nonzero NLO coefficients <i>d</i><sub>14</sub>, <i>d</i><sub>25</sub>, and <i>d</i><sub>36</sub> at 1550 nm fundamental wavelength are measured to be 9.5 ± 2.4, 17.2 ± 3.2, and 3.6 ± 2.3 pm/V, respectively. β-RbBiP<sub>2</sub>S<sub>6</sub> has a comparable laser-induced damage threshold (LIDT) to AgGaSe<sub>2</sub> while RbSbP<sub>2</sub>S<sub>6</sub> has a LIDT approximately 3x that of β-RbBiP<sub>2</sub>S<sub>6</sub> attributed to its higher bandgap.

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Symmetry overChemistry: Harmonic Generation of Low-DimensionalAlkali Chalcopnictates RbMP<sub>2</sub>S<sub>6</sub> (M = Sb, Bi) · Figshare (2025) | TGRS Research Map | TGRS