2015 IEEE 42nd Photovoltaic Specialist Conference (PVSC) 2015
DOI: 10.1109/pvsc.2015.7356143
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Carrier-selective contacts in silicon solar cells

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Cited by 10 publications
(8 citation statements)
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“…Thus, with increasing overpotentials, the charge separation increasingly relies on the different conductivities for H + and OH – inside of each membrane to establish the required current asymmetry, i.e, σ OH – α · ∇μ̅ OH – α ≫ σ H + α · ∇μ̅ H + α and σ OH – ω · ∇μ̅ OH – ω ≪ σ H + ω · ∇μ̅ H + ω . This situation is similar to a solar cell for which charge carrier-selective contacts are of prime importance for efficient operation. ,, …”
mentioning
confidence: 94%
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“…Thus, with increasing overpotentials, the charge separation increasingly relies on the different conductivities for H + and OH – inside of each membrane to establish the required current asymmetry, i.e, σ OH – α · ∇μ̅ OH – α ≫ σ H + α · ∇μ̅ H + α and σ OH – ω · ∇μ̅ OH – ω ≪ σ H + ω · ∇μ̅ H + ω . This situation is similar to a solar cell for which charge carrier-selective contacts are of prime importance for efficient operation. ,, …”
mentioning
confidence: 94%
“…This situation is similar to a solar cell for which charge carrier-selective contacts are of prime importance for efficient operation. 46,98,99 Figure 5c and d show the chemical potential and electric potential, respectively. At electrochemical equilibrium (black dashed lines), the electric potential compensates the chemical potential fully.…”
mentioning
confidence: 99%
“…7,16 Also, we showed in Section 3.2 that the approximation of independent pinhole and tunneling currents is appropriate. We therefore verify the remaining blocks of our model independently, that is, the calculation of the tunneling current density J tun and the surface recombination velocity We estimate the normalized bulk resistivity between this base contact (pad 2 in Figure 9) and the junction contact (pad 1 in Figure 9) to ρ series = (100 ± 16) mΩcm 2 . The voltage drop V across the POLO junction is then extracted from the applied voltage V Bias as eters to the fit.…”
Section: Verification Of the Model By Comparison With Experimental mentioning
confidence: 78%
“…The quantification of selectivity of contacts for charge carrier extraction from solar cell absorbers has attracted recent research interest. [1][2][3][4][5] Following the picture of Brendel et al, the ideal contact of a solar cell shows no recombination (as quantified by the recombination parameter J 0 for most contact schemes) and no resistive losses (as quantified by the contact resistance ρ C ). The figure of merit for the efficiency potential of a real, that is, non-ideal contact, the selectivity…”
Section: Introductionmentioning
confidence: 99%
“…9,10 In addition, the use of n or p type a-Si:H (a-Si:H(n), a-Si:H(p)) as a carrier selective layer allows efficient carrier collection. 11 In addition, a transparent conductive oxide film (TCO) such as tin-doped indium oxide(ITO), tungsten-doped indium oxide (IWO) and aluminum-doped zinc oxide (AZO) is used to compensate for the high sheet resistance loss of the n or a-Si:H(p) layer. 9,[12][13][14] The finger and busbar electrodes are formed on the TCO film by screen printing on the photosensitive surface to collect generated carries.…”
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confidence: 99%