Publication | Open Access
Tunnel oxide passivated rear contact for large area <em>n</em>-type front junction silicon solar cells providing excellent carrier selectivity
26
Citations
17
References
2016
Year
Large AreaEngineeringSemiconductor MaterialsOptoelectronic DevicesPhotovoltaicsSemiconductor DeviceSemiconductorsElectronic DevicesSolar Cell StructuresRear ContactCarrier SelectivityMaterials ScienceSemiconductor TechnologyElectrical EngineeringOxide ElectronicsOxide SemiconductorsSemiconductor MaterialSemiconductor Device FabricationBoron EmitterApplied PhysicsThin FilmsExcellent Carrier SelectivitySolar CellsCarrier-selective ContactSolar Cell Materials
Carrier-selective contact with low minority carrier recombination and efficient majority carrier transport is mandatory to eliminate metal-induced recombination for higher energy conversion efficiency for silicon (Si) solar cells. In the present study, the carrier-selective contact consists of an ultra-thin tunnel oxide and a phosphorus-doped polycrystalline Si (<em>poly</em>-Si) thin film formed by plasma enhanced chemical vapor deposition (PECVD) and subsequent thermal crystallization. It is shown that the <em>poly</em>-Si film properties (doping level, crystallization and dopant activation anneal temperature) are crucial for achieving excellent contact passivation quality. It is also demonstrated quantitatively that the tunnel oxide plays a critical role in this tunnel oxide passivated contact (TOPCON) scheme to realize desired carrier selectivity. Presence of tunnel oxide increases the implied <em>V<sub>oc</sub></em> (<em>iV<sub>oc</sub></em>) by ~ 125 mV. The <em>iV<sub>oc</sub></em> value as high as 728 mV is achieved on symmetric structure with TOPCON on both sides. Large area (239 cm<sup>2</sup>) <em>n</em>-type Czochralski (Cz) Si solar cells are fabricated with homogeneous implanted boron emitter and screen-printed contact on the front and TOPCON on the back, achieving 21.2% cell efficiency. Detailed analysis shows that the performance of these cells is mainly limited by boron emitter recombination on the front side.
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