2012
DOI: 10.1063/1.4764529
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Damage at hydrogenated amorphous/crystalline silicon interfaces by indium tin oxide overlayer sputtering

Abstract: Laser-silicon interaction for selective emitter formation in photovoltaics. I. Numerical model and validation J. Appl. Phys. 112, 114906 (2012) Influence of the pattern shape on the efficiency of front-side periodically patterned ultrathin crystalline silicon solar cells J. Appl. Phys. 112, 113107 (2012) Aluminum oxide-n-Si field effect inversion layer solar cells with organic top contact Appl. Phys. Lett. 101, 233901 (2012) Limiting efficiency of generalized realistic c-Si solar cells coupled to ideal u… Show more

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Cited by 214 publications
(155 citation statements)
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“…[111,130] As mentioned earlier, gentle deposition on underlying layers can also be a critical factor in electrode choice and raises questions about the use of well-established physical vapor deposition (PVD) techniques, such as sputtering or pulsed laser deposition for certain applications. Sputter damage, caused by UV radiation and particle bombardment, is a known phenomenon in organic, [16] SHJ, [15] and perovskite [169] solar cells as well as flexible displays. Solutions to overcome such damage include the use of remote plasma sources, [170] the use of gently deposited buffer layers [171] or further improvements to solution-based deposition processes to improve the density and purity of TCO films to achieve high electron mobilities at low temperatures.…”
Section: Fabrication Compatibilitymentioning
confidence: 99%
“…[111,130] As mentioned earlier, gentle deposition on underlying layers can also be a critical factor in electrode choice and raises questions about the use of well-established physical vapor deposition (PVD) techniques, such as sputtering or pulsed laser deposition for certain applications. Sputter damage, caused by UV radiation and particle bombardment, is a known phenomenon in organic, [16] SHJ, [15] and perovskite [169] solar cells as well as flexible displays. Solutions to overcome such damage include the use of remote plasma sources, [170] the use of gently deposited buffer layers [171] or further improvements to solution-based deposition processes to improve the density and purity of TCO films to achieve high electron mobilities at low temperatures.…”
Section: Fabrication Compatibilitymentioning
confidence: 99%
“…A shortfall of silicon heterojunction solar cells is the passivation damage and V OC loss induced by sputtering and e-beam evaporation [37]. In this sense, the contactless QuasiSteady-State Photoconductance (QSSPC) [38] Furthermore, by use of the methodology proposed by [39], we determined the emitter term of the saturation current density J 0e as a function of the effective lifetime τ eff : (1) where q is the elementary charge, n i the intrinsic carrier concentration in silicon, W the wafer thickness, N D the wafer doping concentration and Δn the minority excess carrier density (under high injection conditions).…”
Section: Transition Metal Oxide/n-si Solar Cellsmentioning
confidence: 99%
“…Also here, a crystallization step at 150-200 o C is key to get μ values up to 138 cm 2 /Vs. 7,16 Besides achieving such high mobility values, the main advantages of the ALD process are the low temperature processing (post-crystallization can take place at temperatures as low as 150 o C), the ability to conformally deposit on non-planar surfaces, and the fact that plasma-induced damage, typically encountered during sputtering ("sputter damage") 17 , is absent during ALD. 18,19 Despite the importance of the crystallization step in realizing high-mobility In2O3:H, little is known about the crystallization process itself.…”
Section: Introductionmentioning
confidence: 99%