2018
DOI: 10.1002/zaac.201800430
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Crystal and Electronic Structure and Optical Properties of AE2SiP4 (AE = Sr, Eu, Ba) and Ba4Si3P8

Abstract: Three new compounds in the AE-Si-P (AE = Sr, Eu, Ba) systems are reported. Sr 2 SiP 4 and Eu 2 SiP 4 , the first members of their respective ternary systems, are isostructural to previously reported Ba 2 SiP 4 and crystallize in the noncentrosymmetric I42d (no. 122) space group. Ba 4 Si 3 P 8 crystallizes in the new structure type, in P2 1 /c (no. 14) space group, mP-120 Pearson symbol, Wyckoff sequence e 30 . In the crystal structures of Sr 2 SiP 4 and Eu 2 SiP 4 all SiP 4 tetrahedral building blocks are conn… Show more

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Cited by 18 publications
(34 citation statements)
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“…The versatility in bonding in the polyanion results in crystal structures with different dimensionality ranging from 0D (Li8SiP4, AE4TtP4; AE = Ca, Sr, Ba; Tt = Si, Ge), 1D (K2SiP2, Ba4Si3P8, Ca3Si2P4), 2D (LiGe3As3, Li3Si7As8, Ca2Si2P4, NaGe6As6, Ba3Si4P6), and 3D (Li2SiP2, MgSiAs2, Mg3Si6As8, AE2SiP4; AE = Sr, Eu, Ba). 13,[21][22][23][24][25][26][27][28] One potential application of ternary tetrel-pnictides is infrared non-linear optical materials, where the non-centrosymmetric crystal structure is a prerequisite coupled with a suitable bandgap, high laser damage threshold, good chemical and thermal stability, and moderate mechanical properties, such as hardness. [29][30][31][32][33][34][35] This field is dominated by lateand post-transition metal chalcogenide materials.…”
Section: Introductionmentioning
confidence: 99%
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“…The versatility in bonding in the polyanion results in crystal structures with different dimensionality ranging from 0D (Li8SiP4, AE4TtP4; AE = Ca, Sr, Ba; Tt = Si, Ge), 1D (K2SiP2, Ba4Si3P8, Ca3Si2P4), 2D (LiGe3As3, Li3Si7As8, Ca2Si2P4, NaGe6As6, Ba3Si4P6), and 3D (Li2SiP2, MgSiAs2, Mg3Si6As8, AE2SiP4; AE = Sr, Eu, Ba). 13,[21][22][23][24][25][26][27][28] One potential application of ternary tetrel-pnictides is infrared non-linear optical materials, where the non-centrosymmetric crystal structure is a prerequisite coupled with a suitable bandgap, high laser damage threshold, good chemical and thermal stability, and moderate mechanical properties, such as hardness. [29][30][31][32][33][34][35] This field is dominated by lateand post-transition metal chalcogenide materials.…”
Section: Introductionmentioning
confidence: 99%
“…The global aim of our work is to find materials with stronger covalent bonding between earth-abundant elements, such as Si and P. Synthesizing non-centrosymmetric phases is no straightforward task, however analysis of the reported compounds in AE-Tt-Pn systems (AE = alkaline-earth metal) reveals that a large fraction of ternary tetrel-pnictides crystallize in non-centrosymmetric structures. 21,23,24,27 We hypothesized that the repulsion of the electron-lone pairs located on pnictogen atoms is responsible for such unusually high abundance of non-centrosymmetric compounds. Typically, AE-Tt-Pn compounds are electron-balanced with bandgaps suitable for infrared applications.…”
Section: Introductionmentioning
confidence: 99%
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“…The possibility of the formation of homonuclear phosphorus bonding distinguishes the family of phosphidosilicates from the oxido‐ and nitridosilicates. Isolated P–P bonding was described in AlSiP 3 , Ca 3 Si 8 P 14 , Ba 2 Si 3 P 6 and Ba 4 Si 3 P 8 , for example, whereas in LaSi 2 P 6 up to four different polyphosphide anions (P n ) –( n +2) with n = 3–6 and in Li 3 Si 3 P 7 [4a] polyphosphide chains exist. Tetragonal Ba 2 SiP 4 ‐ tI 28 is the first example where all SiP 4 tetrahedra are connected by P–P bonds.…”
Section: Introductionmentioning
confidence: 99%