2012
DOI: 10.1063/1.4746752
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Photocarrier lifetime and transport in silicon supersaturated with sulfur

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Cited by 29 publications
(28 citation statements)
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“…Charge carriers in hyperdoped silicon have short carrier lifetimes on the order of picoseconds 23 , so the hyperdoped layer must be thin enough to allow carriers to be transported out of the layer before recombination occurs. The transport length for holes in sulfur-hyperdoped silicon was estimated in one study to be around 100 nm, 25 but in general the transport length can be expected to depend on a number of factors, including the dopant concentration, the material microstructure, and electrostatic fields set up by the dopant concentration gradient. If the electrostatic fields set up by the dopant concentration gradient prove to be a limiting factor in carrier transport, then it might necessary to control the dopant concentration gradient 58 59 (e.g., producing a monotonic dopant concentration profile with depth) in order to fabricate efficient hyperdoped intermediate band photovoltaics or subbandgap photodetectors.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…Charge carriers in hyperdoped silicon have short carrier lifetimes on the order of picoseconds 23 , so the hyperdoped layer must be thin enough to allow carriers to be transported out of the layer before recombination occurs. The transport length for holes in sulfur-hyperdoped silicon was estimated in one study to be around 100 nm, 25 but in general the transport length can be expected to depend on a number of factors, including the dopant concentration, the material microstructure, and electrostatic fields set up by the dopant concentration gradient. If the electrostatic fields set up by the dopant concentration gradient prove to be a limiting factor in carrier transport, then it might necessary to control the dopant concentration gradient 58 59 (e.g., producing a monotonic dopant concentration profile with depth) in order to fabricate efficient hyperdoped intermediate band photovoltaics or subbandgap photodetectors.…”
Section: Discussionmentioning
confidence: 99%
“…Second, the thickness of the hyperdoped layer should be less than the carrier transport lengths. (The transport length for holes in sulfur-hyperdoped silicon, for example, was estimated in one study to be at least 100 nm under an internal field produced by the dopant concentration gradient 25 ). Because the transport length is generally less than the optical absorption depth, light trapping strategies, such as geometric light trapping from surface structures or plasmonic light trapping from metal nanoparticles, should be used to increase absorption within the hyperdoped layer.…”
Section: Introductionmentioning
confidence: 99%
“…13 Microwave photoconductivity decay and low-temperature photoconductivity measurements on carrier dynamics in this material lack the time-resolution required to measure the lifetime directly. [14][15][16] Similar to microwaves, THz radiation is long-wavelength electromagnetic radiation and is sensitive to free charge carriers. Moreover, subpicosecond-duration THz pulses can be straightforwardly generated, enabling direct mapping of the carrier recombination dynamics on picosecond time scales.…”
Section: à3mentioning
confidence: 99%
“…3,4,18 In this article, we will focus on the latter concept, which has been studied extensively from a materials standpoint in two primary material systems: silicon hyperdoped with Ti (Si:Ti) [19][20][21][22][23][24][25][26] and silicon hyperdoped with sulfur (Si:S). [27][28][29][30][31][32][33][34][35] Despite significant efforts on these impurity-band materials, no high-efficiency devices have been demonstrated. We present an experimental framework that predicts whether a candidate impurity-band material system will actually enhance the efficiency of a photovoltaic (PV) device.…”
Section: Introductionmentioning
confidence: 99%