2019
DOI: 10.1364/ome.9.003277
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UHV-CVD growth of high quality GeSn using SnCl4: from material growth development to prototype devices

Abstract: The persistent interest of the epitaxy of group IV alloy GeSn is mainly driven by the demand of efficient light source that could be monolithically integrated on Si for mid-infrared Si photonics. For chemical vapor deposition of GeSn, the exploration of parameter window is difficult from the beginning due to its non-equilibrium growth condition. In this work, we demonstrated the effective pathway to achieve the high quality GeSn with high Sn incorporation. The GeSn films were grown on Ge-buffered Si via ultra-… Show more

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Cited by 31 publications
(22 citation statements)
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“…In lighting configuration with SiO2 particles, the SiO2 was doped at the ratio of 1% to 3% of the phosphor material in the configuration. As a result, the refractive indices of the phosphor material in each layer were 1.428 and 1.445 [20]. The TFCalc32 simulation was employed as a tool to analyze the impacts of various refractive index in the layers.…”
Section: Introductionmentioning
confidence: 99%
“…In lighting configuration with SiO2 particles, the SiO2 was doped at the ratio of 1% to 3% of the phosphor material in the configuration. As a result, the refractive indices of the phosphor material in each layer were 1.428 and 1.445 [20]. The TFCalc32 simulation was employed as a tool to analyze the impacts of various refractive index in the layers.…”
Section: Introductionmentioning
confidence: 99%
“…Ge 1−x Sn x has attracted much research interest as an exciting material with potential applications in nextgeneration rechargeable lithium-ion battery anodes and optoelectronic devices, due to their high carrier mobilities [1][2][3] and a direct band gap which can be tuned by varying the tin concentration [4][5][6][7][8][9][10][11][12]. Additionally, cubic Ge 1−x Sn x allows the lattice dimensions to be tuned over a wide range, which is beneficial when used as a buffer layer to reduce strain arising from lattice mismatch between III-V or II-VI compounds with silicon or germanium substrates [13][14][15].…”
Section: Introductionmentioning
confidence: 99%
“…The synthesis of Ge 1−x Sn x is challenging due to the low solubility of tin in germanium (<1%) [16], large lattice mismatch (∼14%) and a tendency of metallic tin to segregate from germanium [17,18]. Ge 1−x Sn x alloys are commonly fabricated using ion implantation, laser melting [4,5,19], molecular beam epitaxy (MBE) [7], and chemical-vapor deposition(CVD) approaches [6,[20][21][22]. Apart from these thin film based preparations, there are limited reports of the synthesis of anisotropic Ge 1−x Sn x nanostructures by top-down and bottom-up approaches [12,[23][24][25][26][27][28].…”
Section: Introductionmentioning
confidence: 99%
“…Recently, Silicon-germanium-tin (SiGeSn) and Germaniumtin (GeSn) techniques have drawn much attention due to the success of developing all-group-IV alloy with outstanding material properties including (i) independent tuning of the lattice constant and bandgap by simultaneously varying the compositions of Si, Ge, and Sn (Jenkins and Dow, 1987); (ii) true direct-bandgap material (Zhou et al, 2019); (iii) wavelength coverage up to 12 µm (Du et al, 2016); and (iv) a low material growth temperature fully compatible with CMOS processes (Grant et al, 2019). The advantages of a SiGeSn approach are (i) compatibility with the proven high-performance Silicon on Insulator (SOI) passive and Electro-optic (EO) components, and (ii) enhanced dynamic range as two-photon absorption at 1.55 µm in Si under high laser power operation is effectively suppressed by shifting the operating wavelength to 2 µm and beyond (Cao et al, 2018).…”
Section: Introductionmentioning
confidence: 99%