Definition H

HJT (Heterojunction) Solar Cell

A high-efficiency solar cell that combines crystalline silicon with thin amorphous silicon layers, achieving superior passivation, lower temperature coefficients, and module efficiencies above 22%.

Updated Mar 2026 5 min read
Rainer Neumann

Written by

Rainer Neumann

Content Head · SurgePV

Keyur Rakholiya

Edited by

Keyur Rakholiya

CEO & Co-Founder · SurgePV

Key Takeaways

  • HJT cells combine crystalline and amorphous silicon for excellent surface passivation
  • Achieve cell efficiencies of 25–26% and module efficiencies of 22–23.5%
  • Lowest temperature coefficients in commercial production (−0.24 to −0.26%/°C)
  • Bifacial by nature — rear-side gains of 5–15% depending on ground albedo
  • Higher manufacturing cost than PERC and TOPCon limits market share to the premium segment
  • Ideal for hot climates and space-constrained installations where per-panel output matters

What Is an HJT Solar Cell?

An HJT (heterojunction) solar cell is a photovoltaic cell that sandwiches a crystalline silicon (c-Si) wafer between thin layers of amorphous silicon (a-Si). This heterojunction structure — the junction of two different semiconductor materials — creates exceptionally effective surface passivation, meaning fewer charge carriers are lost at the wafer surfaces. The result is higher voltage, higher efficiency, and better real-world performance than conventional solar cells.

The HJT concept was pioneered by Sanyo (now Panasonic) in the early 1990s under the trade name “HIT” (Heterojunction with Intrinsic Thin layer). Since the patents expired in 2010, multiple manufacturers have adopted and refined the technology. Today, HJT cells are produced by companies including REC, Meyer Burger, Huasun, and LONGi, competing with TOPCon as the leading N-type cell architecture.

HJT cells hold the current silicon solar cell efficiency record at 26.81% (LONGi, 2024). Their low-temperature processing also enables thinner wafers — down to 120 microns — reducing silicon consumption by 25% compared to standard cells.

How HJT Solar Cells Work

The HJT cell’s superior performance comes from its multi-layer structure and low-temperature manufacturing process:

1

N-Type Silicon Wafer Base

The cell starts with an N-type monocrystalline silicon wafer, which has higher carrier lifetimes and lower light-induced degradation compared to P-type wafers used in conventional PERC cells.

2

Intrinsic Amorphous Silicon Layer

A very thin (5–10 nm) undoped amorphous silicon layer is deposited on both surfaces of the wafer. This intrinsic layer passivates surface defects, dramatically reducing recombination losses.

3

Doped Amorphous Silicon Layers

P-doped a-Si is deposited on one side and N-doped a-Si on the other, creating the heterojunction that generates the electric field for charge separation.

4

Transparent Conductive Oxide (TCO)

Indium tin oxide (ITO) or similar TCO layers are applied to both surfaces. These layers are electrically conductive and optically transparent, collecting current without blocking light.

5

Metallization

Silver or copper contacts are screen-printed or plated onto the TCO layers. Because the process temperature stays below 200°C (vs. 800°C+ for PERC), HJT is compatible with thinner wafers and low-temperature pastes.

Core Formula
Cell Efficiency = (Voc × Isc × Fill Factor) / (Incident Irradiance × Cell Area) × 100

Types of HJT Solar Cell Configurations

HJT technology is deployed in several module configurations depending on performance goals and application.

Standard

Monofacial HJT Module

Single-sided light capture with an opaque backsheet. Simpler to install and model. Module efficiencies of 21.5–23%. Suitable for residential rooftop applications where rear-side light gain is minimal.

Premium

Bifacial HJT Module

Glass-glass construction capturing light on both faces. Rear-side gains of 5–15% depending on ground reflectivity. Ideal for ground-mount, carport, and elevated installations with reflective surfaces below.

Advanced

HJT with SmartWire (SWCT)

Replaces traditional busbars with a mesh of thin wires, reducing silver consumption by 30% and improving light capture. Meyer Burger pioneered this approach. Achieves slightly higher efficiency at lower material cost.

Next-Gen

Perovskite-on-HJT Tandem

A perovskite layer is deposited on top of an HJT cell, creating a tandem cell that captures a wider light spectrum. Lab efficiencies exceed 33%. Expected to reach commercial production in 2027–2029.

Designer’s Note

When modeling HJT panels in solar design software, pay close attention to the temperature coefficient input. HJT’s advantage (−0.24%/°C vs. −0.35%/°C for PERC) can mean 3–5% higher annual production in hot climates. Using the wrong temperature coefficient erases this advantage in your simulation.

Key Metrics & Calculations

HJT cells are evaluated on several performance parameters that distinguish them from competing technologies:

MetricUnitHJT Typical Value
Cell Efficiency%24.5–26.8%
Module Efficiency%22–23.5%
Temperature Coefficient (Pmax)%/°C−0.24 to −0.26
Open Circuit Voltage (Voc)V0.74–0.76 (per cell)
Bifaciality Factor%85–95%
Annual Degradation Rate%/yr0.25–0.40%
Temperature-Adjusted Output Formula
Actual Power = STC Power × [1 + Temp Coefficient × (Cell Temp − 25°C)]

Practical Guidance

HJT panels require specific considerations for design, installation, and sales:

  • Model bifacial gain accurately. Use ground albedo values specific to the site — concrete reflects 25–30%, grass 15–20%, white roofing membrane 60–80%. Overestimating albedo leads to over-promised production.
  • Leverage the temperature advantage. In hot climates (Phoenix, Dubai, India), HJT panels can produce 5–8% more annual energy than PERC panels of the same wattage. Model this with correct temperature coefficients.
  • Size strings for higher voltage. HJT cells have higher Voc than PERC cells. Check that cold-temperature string voltages don’t exceed inverter input limits — this is especially critical in northern climates.
  • Use solar design software with HJT-specific parameters. Ensure your simulation tool applies the correct temperature model and degradation rate for HJT, not generic silicon defaults.
  • Handle bifacial glass-glass panels carefully. Bifacial HJT modules are heavier (24–28 kg vs. 20–22 kg for standard panels) and more fragile on the rear side. Use proper lifting techniques and avoid stacking face-to-face.
  • Ensure proper grounding. The TCO layers in HJT panels may require specific grounding procedures. Follow the manufacturer’s installation manual exactly — some HJT panels require positive grounding.
  • Maximize rear-side exposure for bifacial models. On ground mounts, maintain adequate clearance (1 m+) between the rear glass and the ground. On rooftops, use standoff heights that allow light to reach the back surface.
  • Avoid mixing HJT with other cell types. HJT panels have different I-V characteristics than PERC or TOPCon. Mixing them on the same string causes mismatch losses that negate the efficiency advantage.
  • Sell the hot-climate advantage. In regions with high temperatures, HJT’s lower temperature coefficient is a measurable, quantifiable advantage. Show customers the production difference in kWh and dollars.
  • Highlight the degradation warranty. HJT panels typically guarantee 92% output at year 25 vs. 84% for standard panels. Over 25 years, this compounds to significantly more energy and savings.
  • Position HJT as premium, not expensive. Frame the price difference in terms of lifetime value: “This panel costs $50 more upfront but produces $400 more electricity over its lifetime.”
  • Explain bifaciality in simple terms. “This panel captures sunlight from both sides — like double-sided solar. On your white roof, it can produce up to 10% more energy than a standard panel.”

Model HJT Panel Performance Accurately

SurgePV’s simulation engine uses manufacturer-specific temperature coefficients and bifacial parameters for precise HJT energy modeling.

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Real-World Examples

Residential: Hot Climate Performance

A homeowner in Phoenix, Arizona, compares quotes for a 8 kW system using PERC panels (−0.37%/°C) vs. HJT panels (−0.25%/°C). Average cell temperature during peak production is 65°C. The PERC system produces 13,200 kWh/year; the HJT system produces 14,050 kWh/year — a 6.4% advantage from the temperature coefficient alone. Over 25 years, the HJT system generates 21,250 more kWh, worth approximately $4,250 at current rates.

Commercial: Bifacial Ground Mount

A 500 kW commercial ground-mount installation in Spain uses bifacial HJT panels mounted 1.5 meters above a white gravel surface (albedo 0.40). The rear-side gain contributes an additional 12% production compared to a monofacial installation. Annual production reaches 875 MWh vs. 780 MWh for an equivalent monofacial PERC system — an additional 95 MWh worth approximately €9,500/year.

Utility-Scale: Thin Wafer Cost Reduction

A panel manufacturer produces HJT cells on 130-micron wafers instead of the standard 170-micron wafers. The 23% reduction in silicon usage lowers wafer costs by $0.015/W. Across a 100 MW production run, this saves $1.5 million in raw material costs while maintaining cell efficiency above 25.5%. The thinner wafers also reduce the carbon footprint per panel by approximately 18%.

Impact on System Design

HJT panels influence design decisions differently than conventional technologies:

Design DecisionHJT PanelsStandard PERC Panels
Temperature Derating2–3% loss at 65°C cell temp5–7% loss at 65°C cell temp
String VoltageHigher Voc per cell — shorter strings possibleStandard Voc — typical string lengths
Bifacial Modeling85–95% bifaciality factor70% (if bifacial PERC) or N/A
Degradation Modeling0.25–0.40%/year0.45–0.55%/year
25-Year Production92–94% of nameplate84–87% of nameplate
Pro Tip

When comparing HJT vs. TOPCon panels for a project, run a 25-year energy simulation — not just year-1 production. HJT’s lower degradation rate means the gap widens over time. A panel that produces 2% more in year 1 may produce 5% more in year 20 due to compounding degradation differences.

Frequently Asked Questions

What is an HJT solar cell?

An HJT (heterojunction) solar cell combines a crystalline silicon wafer with thin layers of amorphous silicon deposited on both surfaces. This hybrid structure provides excellent surface passivation, reducing energy losses and achieving higher efficiency than conventional cells. HJT cells reach 25–26% efficiency at the cell level and 22–23.5% at the module level.

Is HJT better than TOPCon?

Neither is universally better — each has strengths. HJT has a lower temperature coefficient (performs better in heat), lower degradation rates, and higher bifaciality. TOPCon has lower manufacturing costs, is easier to produce on existing PERC production lines, and has closed the efficiency gap significantly. In hot climates, HJT has a measurable advantage. In cost-sensitive projects with ample space, TOPCon often delivers better ROI.

Why are HJT panels more expensive?

HJT manufacturing requires specialized equipment for amorphous silicon deposition and TCO sputtering that cannot be retrofitted from existing PERC lines. The cells also use more silver for metallization and require indium tin oxide (ITO), a more expensive material. However, costs are declining as production scales up, thinner wafers reduce silicon usage, and copper metallization replaces silver.

How long do HJT solar panels last?

HJT panels are warrantied for 25–30 years by most manufacturers, with output guarantees of 90–92% at year 25. Their lower degradation rate (0.25–0.40%/year vs. 0.45–0.55% for PERC) means they retain more of their original capacity over time. Real-world data from early Sanyo/Panasonic HIT installations suggests functional lifetimes of 30–35 years with proper maintenance.

About the Contributors

Author
Rainer Neumann
Rainer Neumann

Content Head · SurgePV

Rainer Neumann is Content Head at SurgePV and a solar PV engineer with 10+ years of experience designing commercial and utility-scale systems across Europe and MENA. He has delivered 500+ installations, tested 15+ solar design software platforms firsthand, and specialises in shading analysis, string sizing, and international electrical code compliance.

Editor
Keyur Rakholiya
Keyur Rakholiya

CEO & Co-Founder · SurgePV

Keyur Rakholiya is CEO & Co-Founder of SurgePV and Founder of Heaven Green Energy Limited, where he has delivered over 1 GW of solar projects across commercial, utility, and rooftop sectors in India. With 10+ years in the solar industry, he has managed 800+ project deliveries, evaluated 20+ solar design platforms firsthand, and led engineering teams of 50+ people.

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