2011
DOI: 10.1364/ome.1.001292
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Nonlinear, dispersive, and phase-matching properties of the new chalcopyrite CdSiP_2 [Invited]

Abstract: We compare the nonlinear and dispersive properties of the recently discovered mid-infrared nonlinear crystal CdSiP 2 with other chalcopyrite materials to establish its potential for super-continuum generation through a second-order nonlinear process.

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Cited by 42 publications
(14 citation statements)
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“…In 2010, Zawilski and Schunemann reported the growth of a large crack-free CdSiP 2 single crystal with dimensions of 70 Â 25 Â 8 mm 3 grown for the first time using the transparent horizontal gradient freezing method. This result demonstrated that large single crystal CdSiP 2 can be grown from the melt [29], and the nonlinearity, and phase matching properties of the crystal has been studied in following papers [30,31]. In this paper, for the first time, to the best of our knowledge, we report the synthesis of high purity polycrystalline CdSiP 2 in a single-temperature zone furnace and the growth of single crystal CdSiP 2 with a diameter of 8 mm, and a length of 40 mm using the vertical Bridgman method.…”
Section: Introductionmentioning
confidence: 71%
“…In 2010, Zawilski and Schunemann reported the growth of a large crack-free CdSiP 2 single crystal with dimensions of 70 Â 25 Â 8 mm 3 grown for the first time using the transparent horizontal gradient freezing method. This result demonstrated that large single crystal CdSiP 2 can be grown from the melt [29], and the nonlinearity, and phase matching properties of the crystal has been studied in following papers [30,31]. In this paper, for the first time, to the best of our knowledge, we report the synthesis of high purity polycrystalline CdSiP 2 in a single-temperature zone furnace and the growth of single crystal CdSiP 2 with a diameter of 8 mm, and a length of 40 mm using the vertical Bridgman method.…”
Section: Introductionmentioning
confidence: 71%
“…But over the past few decades, most of the research in this field is concentrated in the non‐centrosymmetric metal chalcogenides, [6] which results in many IR‐NLO chalcogenides with excellent comprehensive properties, such as BaGa 4 S 7 , [7] BaGa 4 Se 7 , [8] SnGa 4 S 7 , [9] Sn 2 Ga 2 S 5 , [10] Hg 3 P 2 S 8 , [11] γ‐NaAsSe 2 , [12] Li 2 CdGeS 4 , [13] α‐Li 2 ZnGeS 4 , [14] La 4 InSbS 9 , [15] Na 2 ZnGe 2 S 6 , [16] CsGa 2 SnSe 6 , [17] Li 2 ZnSiS 4 , [18] Li 2 BaGeS 4 , [19] CuHgPS 4 , [20] BaHgGeSe 4 , [21] Sr 5 ZnGa 6 S 15 , [22] [Li 2 Cs 2 Cl][Ga 3 S 6 ], [23] [Rb 3 Br][PGa 3 S 8 ], [24] [CsBa 2 Cl][Ga 4 S 8 ], [25] [Ba 4 Cl 2 ][ZnGa 4 S 10 ] [26] and so on and so forth. Compared with a large number of research results in IR‐NLO chalcogenides, only a few IR‐NLO pnictides are discovered in this area [28–61] and the major research works are still focused on classical binary or ternary semiconductors, such as GaAs, [27] ZnGeP 2 , [5] CdSiP 2 [7] and CdGeAs 2 [29] . Generally, pnictides exhibit small band gaps (E g <2.5 eV) and are difficult to synthesize, which limit their development in the IR‐NLO field.…”
Section: Introductionmentioning
confidence: 99%
“…There is still much to understand about models of conduction and their effect at THz frequencies, which requires application of THz-TDS to bulk crystals without contacts or other forms of device processing. One material class that has been interesting to the optics community is II-IV-V2 chalcopyrite crystals due to their high nonlinearity, composition-tunable band gaps, wide transparency windows and high damage threshold [12][13][14][15]. Chalcopyrite crystals have been explored for electromagnetic (EM) screening, spintronic [16,17], and photovoltaic applications [18], making them good as optical and optoelectronic materials.…”
Section: Introductionmentioning
confidence: 99%