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[A(3)X][Ga(3)PS(8)] (A = K, Rb; X = Cl, Br): promising IR non-linear optical materials exhibiting concurrently strong second-harmonic generation and high laser induced damage thresholds
Mid-far infrared (IR) non-linear optical (NLO) materials are of great importance in military and civil fields. However, commercial IR-NLO crystals (such as AgGaS(2), AgGaSe(2) and ZnGeP(2)) do not currently satisfy the requirements of large second-harmonic generation (SHG) and high laser induced dam...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Royal Society of Chemistry
2016
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6024201/ https://www.ncbi.nlm.nih.gov/pubmed/30034768 http://dx.doi.org/10.1039/c6sc01907b |
Sumario: | Mid-far infrared (IR) non-linear optical (NLO) materials are of great importance in military and civil fields. However, commercial IR-NLO crystals (such as AgGaS(2), AgGaSe(2) and ZnGeP(2)) do not currently satisfy the requirements of large second-harmonic generation (SHG) and high laser induced damage thresholds (LIDTs), which seriously limits their practical applications. Herein, we have developed a new series of salt-inclusion chalcogenides, [A(3)X][Ga(3)PS(8)] (A = K, Rb; X = Cl, Br), which are constructed from alternate stacking of adamantane-like [Ga(3)PS(10)](6–) cluster layers and cationic [A(3)X](2+) salt layers. Importantly, they display both large SHG responses of several-fold and high LIDTs for dozens of times that of commercial AgGaS(2), which exhibit the highest LIDTs among the reported IR-NLO materials with a larger SHG conversion efficiency than that of AgGaS(2). These properties together with wide transparent region, type I phase-matching features and congruent-melting behaviors indicate they are promising IR-NLO materials. |
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