2005
DOI: 10.1021/cm049029i
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Role of the Background Gas in the Morphology and Optical Properties of Laser-Microstructured Silicon

Abstract: We irradiated silicon with a train of femtosecond pulses in the presence of SF6, H2S, H2, SiH4, and a mixture of Ar and SF6 in order to analyze the role of the background gas in determining the morphology and the optical properties of the resultant surfaces. We discuss factors that affect the surface morphology created during irradiation and show that the presence of sulfur in these gases is important in creating sharp microstructures. We also show that the presence of sulfur is necessary to create the near-un… Show more

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Cited by 153 publications
(106 citation statements)
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“…While the sub-band-gap absorption phenomenon is still not understood, dilute chalcogen atoms are known to form deep levels in the silicon band gap [18]. It has been proposed that, due to the high concentration of substitutional chalcogen incorporation, impurity bands within the Si forbidden gap may form and lead to the observed broad sub-band-gap absorption [8,19].…”
Section: Resultsmentioning
confidence: 99%
“…While the sub-band-gap absorption phenomenon is still not understood, dilute chalcogen atoms are known to form deep levels in the silicon band gap [18]. It has been proposed that, due to the high concentration of substitutional chalcogen incorporation, impurity bands within the Si forbidden gap may form and lead to the observed broad sub-band-gap absorption [8,19].…”
Section: Resultsmentioning
confidence: 99%
“…22 Second, carrier lifetimes, 23 carrier mobilities, 24 25 and absorption coefficients 26 1 in chalcogen-hyperdoped crystalline silicon have been measured and imply that the dopant concentration that maximizes carrier extraction from a hyperdoped silicon layer of a given optical thickness is around 0.03 atomic % (1.4×10 19 cm -3 ), 23 which is about two orders of magnitude greater than the equilibrium solubility limit for chalcogens in silicon of 0.0001 atomic % (5×10 16 cm -3 ). 27 Third, microstructural investigations of hyperdoped black silicon have shown that after fabrication with femtosecond laser irradiation, the light-trapping surface structures (typically cones that are 1-10 micrometers tall) are often polyphasic, containing amorphous and various pressure-induced crystalline silicon phases, and the dopants are incorporated within a thin layer on the surface which is typically 20-200 nm thick. 28 29 10 Fourth, thermal annealing increases the crystallinity of hyperdoped black silicon and can improve electrical rectification at the homojunction between the hyperdoped layer and the substrate, but thermal annealing also deactivates the sub-bandgap optical absorptance of the material in a manner consistent with the dopants diffusing to optically inactive sites in the silicon lattice (with diffusion lengths < 1 micrometer).…”
Section: Introductionmentioning
confidence: 99%
“…12 The resulting material, socalled black silicon, presents strong optical absorption even at energies below the Si band gap. Near-unity absorptance has been found for photon energies down to approximately 0.5 eV.…”
Section: Introductionmentioning
confidence: 99%