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Current flow mechanism at the recombination junction. a) Test structure for contact resistivity measurement and b) the corresponding dark J‐V characteristics with and without a TiO x layer between the Si wafer and the SnO 2 layer. Six identical Al pads were fabricated on a substrate and measured with both forward and backward voltage scans. Note that p ‐Si was used as substrate instead of n ‐Si to characterize the hole injection from Si to TiO x /SnO 2 recombination junction. c,d) Band diagrams of the test structures c) with TiO x and d) without TiO x layer obtained by a SCAPS <t>finite</t> <t>element</t> <t>device</t> simulation. E C and E V denote energy levels of conduction band and valence band, respectively. E F is the Fermi level.
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Current flow mechanism at the recombination junction. a) Test structure for contact resistivity measurement and b) the corresponding dark J‐V characteristics with and without a TiO x layer between the Si wafer and the SnO 2 layer. Six identical Al pads were fabricated on a substrate and measured with both forward and backward voltage scans. Note that p ‐Si was used as substrate instead of n ‐Si to characterize the hole injection from Si to TiO x /SnO 2 recombination junction. c,d) Band diagrams of the test structures c) with TiO x and d) without TiO x layer obtained by a SCAPS <t>finite</t> <t>element</t> <t>device</t> simulation. E C and E V denote energy levels of conduction band and valence band, respectively. E F is the Fermi level.
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Current flow mechanism at the recombination junction. a) Test structure for contact resistivity measurement and b) the corresponding dark J‐V characteristics with and without a TiO x layer between the Si wafer and the SnO 2 layer. Six identical Al pads were fabricated on a substrate and measured with both forward and backward voltage scans. Note that p ‐Si was used as substrate instead of n ‐Si to characterize the hole injection from Si to TiO x /SnO 2 recombination junction. c,d) Band diagrams of the test structures c) with TiO x and d) without TiO x layer obtained by a SCAPS <t>finite</t> <t>element</t> <t>device</t> simulation. E C and E V denote energy levels of conduction band and valence band, respectively. E F is the Fermi level.
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Current flow mechanism at the recombination junction. a) Test structure for contact resistivity measurement and b) the corresponding dark J‐V characteristics with and without a TiO x layer between the Si wafer and the SnO 2 layer. Six identical Al pads were fabricated on a substrate and measured with both forward and backward voltage scans. Note that p ‐Si was used as substrate instead of n ‐Si to characterize the hole injection from Si to TiO x /SnO 2 recombination junction. c,d) Band diagrams of the test structures c) with TiO x and d) without TiO x layer obtained by a SCAPS <t>finite</t> <t>element</t> <t>device</t> simulation. E C and E V denote energy levels of conduction band and valence band, respectively. E F is the Fermi level.
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COMSOL Inc finite element 1d thermal model
Current flow mechanism at the recombination junction. a) Test structure for contact resistivity measurement and b) the corresponding dark J‐V characteristics with and without a TiO x layer between the Si wafer and the SnO 2 layer. Six identical Al pads were fabricated on a substrate and measured with both forward and backward voltage scans. Note that p ‐Si was used as substrate instead of n ‐Si to characterize the hole injection from Si to TiO x /SnO 2 recombination junction. c,d) Band diagrams of the test structures c) with TiO x and d) without TiO x layer obtained by a SCAPS <t>finite</t> <t>element</t> <t>device</t> simulation. E C and E V denote energy levels of conduction band and valence band, respectively. E F is the Fermi level.
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Current flow mechanism at the recombination junction. a) Test structure for contact resistivity measurement and b) the corresponding dark J‐V characteristics with and without a TiO x layer between the Si wafer and the SnO 2 layer. Six identical Al pads were fabricated on a substrate and measured with both forward and backward voltage scans. Note that p ‐Si was used as substrate instead of n ‐Si to characterize the hole injection from Si to TiO x /SnO 2 recombination junction. c,d) Band diagrams of the test structures c) with TiO x and d) without TiO x layer obtained by a SCAPS finite element device simulation. E C and E V denote energy levels of conduction band and valence band, respectively. E F is the Fermi level.

Journal: Small (Weinheim an Der Bergstrasse, Germany)

Article Title: Monolithic Perovskite/Silicon Tandem Solar Cells Enabled by Multifunctional TiO x Interconnects

doi: 10.1002/smll.202500969

Figure Lengend Snippet: Current flow mechanism at the recombination junction. a) Test structure for contact resistivity measurement and b) the corresponding dark J‐V characteristics with and without a TiO x layer between the Si wafer and the SnO 2 layer. Six identical Al pads were fabricated on a substrate and measured with both forward and backward voltage scans. Note that p ‐Si was used as substrate instead of n ‐Si to characterize the hole injection from Si to TiO x /SnO 2 recombination junction. c,d) Band diagrams of the test structures c) with TiO x and d) without TiO x layer obtained by a SCAPS finite element device simulation. E C and E V denote energy levels of conduction band and valence band, respectively. E F is the Fermi level.

Article Snippet: To explain these results, device simulations were carried out for the same sample structures using the SCAPS_1D finite element device simulator.

Techniques: Injection