
SHJ has the highest efficiency amongst crystalline silicon solar cells in both laboratory (world record efficiency) and commercial production (average efficiency). In 2023, the average efficiency for commercial SHJ cells was 25.0%, compared with 24.9% for n-type TOPCon and 23.3% for p-type PERC. The high efficiency is owed mostly to very high open-circuit voltages—consistently over 700 mV—as a result of excellent surface passivation. Since 2023, SHJ bottom cells in Per. [pdf]
They are a hybrid technology, combining aspects of conventional crystalline solar cells with thin-film solar cells. Silicon heterojunction-based solar panels are commercially mass-produced for residential and utility markets.
Heterojunction solar cells (HJT), variously known as Silicon heterojunctions (SHJ) or Heterojunction with Intrinsic Thin Layer (HIT), are a family of photovoltaic cell technologies based on a heterojunction formed between semiconductors with dissimilar band gaps.
Silicon heterojunction (SHJ) solar cells have reached high power conversion efficiency owing to their effective passivating contact structures. Improvements in the optoelectronic properties of these contacts can enable higher device efficiency, thus further consolidating the commercial potential of SHJ technology.
The application of silicon heterojunction solar cells for ultra-high efficiency perovskite/c-Si and III-V/c-Si tandem devices is also reviewed. In the last, the perspective, challenge and potential solutions of silicon heterojunction solar cells, as well as the tandem solar cells are discussed. 1. Introduction
In the case of front grids, the grid geometry is optimised such to provide a low resistance contact to all areas of the solar cell surface without excessively shading it from sunlight. Heterojunction solar cells are typically metallised (ie. fabrication of the metal contacts) in two distinct methods.
Chinese solar module manufacturer Longi has developed a heterojunction back contact (BC) solar cell using a laser-enhanced contact optimization process that reportedly has a total effective processing time of about one-third compared to that of mainstream technologies such as PERC and TOPCon.

A "front-junction" heterojunction solar cell is composed of a p–i–n–i–n-doped stack of silicon layers; the middle being an n-type crystalline silicon wafer and the others being amorphous . Then, overlayers of a (TCO) antireflection coating and metal grid are used for light and current collection. Due to the high bifaciality of the SHJ structure, the similar n–i–n–i–p "rear-junction" configuration is also used by manufacturers and may have adv. [pdf]
Like all conventional solar cells, heterojunction solar cells are a diode and conduct current in only one direction. Therefore, for metallisation of the n -type side, the solar cell must generate its own plating current through illumination, rather than using an external power supply.
In the last few years, the performance of organic solar cells (OSCs) based on bulk heterojunction (BHJ) structure has remarkably improved. However, for a large scale roll to roll (R2R) manufacturing of this technology and precise device fabrication, further improvements are critical.
Conversion efficiencies of the cell can be described as a carrier generation efficiency times a carrier transport efficiency, as illustrated in Fig. 17.4B. Ordinary heterojunction solar cells are high efficiency if the carrier mobility and electrical conductivity of the D and A layers are high.
They are a hybrid technology, combining aspects of conventional crystalline solar cells with thin-film solar cells. Silicon heterojunction-based solar panels are commercially mass-produced for residential and utility markets.
Later in the early 1990s, the discovery of ultrafast charge transfer from polymer to fullerene initiated the research field of bulk hetero-junction (BHJ) solar cells.
Amongst the potential dopants, tungsten, zirconium and cerium were reported to enable highly efficient devices [, , ]. The interplay between the electrode and the rest of the device is stringent in Si heterojunction solar cells, and this calls for a holistic approach to fully harvest the potential of this technology.

The unusual optical characteristics, combined with the semiconducting properties of silicon make this material interesting for sensor applications. Potential applications include: • with increased sensitivity• • with high-efficiency through increased absorption. Black silicon (b-Si) is a nano-scaled surface texture which significantly reduces optical losses in solar cells and provides potential for higher efficiency cells on a range of substrates[1]. [pdf]
Black silicon is layered on the front surface, usually with another passivation layer. In a recent study by Savin et al. , they have reported a record-breaking b-Si solar cell efficiency of 22.1% using an IBC configuration. Fig. 12 (b) shows the configuration of the solar cell used in their study.
Black silicon is a surface modification of silicon where a nanoscale surface structure is formed through etching. The resulting nanoscale structure (from porous surface to bulk silicon) provides an extremely low reflectivity of close to 0% , , .
One notable direction in the photovoltaics technology is the usage of black silicon (b-Si) for solar cells. Black-Si has textured surface, which can assist light trapping and improves efficiency of solar cells. Black-Si was first fabricated by Jansen et al. in 1995, and it exhibits a characteristic black surface colour.
Black silicon has become a major asset to the solar photovoltaic industry as it enables greater light to electricity conversion efficiency of standard crystalline silicon solar cells, which significantly reduces their costs. SEM micrograph of black silicon formed by cryogenic RIE.
We demonstrate that efficiencies above 22% can be reached, even in thick interdigitated back-contacted cells, where carrier transport is very sensitive to front surface passivation. This means that the surface recombination issue has truly been solved and black silicon solar cells have real potential for industrial production.
Photograph of a black silicon-based solar cell with a reflectance of 1.79% by the PIII method is shown in Fig. 22 . The black silicon-based solar cell had an efficiency of 15.68% with a fill factor of 0.783. In contrast, the reference cell had an efficiency of 17.5% with a fill factor of 0.78. Fig. 22.
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