Monocrystalline solar panels vs. N-type TOPCon | LID, Conversion Efficiency, Degradation Rate

May 28, 2026

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Mono-crystalline PERC modules experience typical first-year degradation of 3% (measured average 1.92%) due to boron-oxygen (B-O) complex defects, leading to significant power generation loss over the lifecycle;

while N-type TOPCon, utilizing phosphorus-doped wafers, avoids the BO-LID mechanism, achieving first-year degradation <1% (outdoor demonstration only 0.51%).

 

 

Yinchuan demonstration data shows: Under equivalent irradiation, TOPCon modules degrade less than 37% of PERC modules after 6000 hours.

TOPCon's tunnel oxide layer and poly-silicon passivation structure simultaneously suppress surface recombination, resulting in a lab light-induced degradation rate as low as 0.26%.

Lower degradation combined with 24%-26% conversion efficiency advantage enables TOPCon to achieve 3-5 year power gain covering the initial cost premium in large-scale power plants, reshaping high-efficiency module selection logic.

 

Causes

 

Formation and Activation of Boron-Oxygen Complexes

The core mechanism of LID is the formation of boron-oxygen complexes (B-O) under illumination. In P-type wafers doped with boron, boron atoms combine with interstitial oxygen to form unstable B-O defects:

· Formation Condition: Under illumination intensity >1 mW/cm², the boron-oxygen complex enters an active state (State B), causing minority carrier lifetime to drop from 1000μs to below 500μs.

· Temperature Influence: For every 10°C temperature increase, the B-O complex formation rate increases 2-3 times. For example, at 75°C, the LID degradation rate of PERC modules is 4.7 times that at 25°C.

· Oxygen Content Difference: Mono-crystalline silicon, grown using quartz crucibles, has a high oxygen content of 10-14 ppma, while multi-crystalline silicon from casting has only 1-2 ppma. This leads to 2-3 times higher LID degradation in mono-Si compared to multi-Si.

Process Parameter Amplification Effect on LID

Cell manufacturing processes directly affect the activity of B-O complexes:

·Sintering Temperature: When sintering peak temperature >850°C, hydrogen from the passivation layer diffuses into the silicon substrate, combining with boron to form reversible defects. Experiments show that for every 50°C increase in sintering temperature, the LeTID degradation rate increases by 0.8%.

·Metal Contamination: Iron (Fe) impurities combine with boron to form Fe-B pairs, which decompose into Feⁱ and Bⁱ⁰ under illumination, creating additional recombination centers. 1 ppm iron contamination can increase LID degradation by 0.5%.

·Insufficient Hydrogen Passivation: When hydrogen content in the passivation layer (e.g., AlOx/SiNx) is <1×10¹⁹ atoms/cm³, it cannot effectively passivate B-O defects. TOPCon requires 40% less hydrogen due to the absence of boron doping, improving defect regeneration efficiency.

Correlation Between Cell Structure and LID Sensitivity

Different cell structures show significant differences in LID response:

·PERC Cells: The rear passivation layer increases long-wavelength light absorption, leading to higher carrier concentration and enhanced B-O complex activity. Measurements show PERC LID degradation is 1.8 times that of conventional aluminum back surface field (Al-BSF) cells.

·TOPCon Cells: When the tunnel oxide layer (SiOx) thickness is controlled at 1.5nm, surface recombination velocity is <0.5 cm/s, suppressing defect activation. Lab data indicates TOPCon's LID degradation rate is 82% lower than PERC.

·Heterojunction (HJT) Cells: The amorphous silicon passivation layer introduces additional defects, but 90% of interface states can be repaired by hydrogen annealing, keeping LID degradation below 0.3%.

Environmental Factors and Dynamic Response of LID

Mechanisms of outdoor environment accelerating LID:

·UV Radiation: Ultraviolet light (280-320nm) induces oxygen vacancy generation, which combines with boron to form complexes. Zhangbei demonstration data shows, in regions with annual UV irradiation >2000 kWh/m², PERC modules experience an additional 0.7% LID.

·High Temperature and Humidity: Under 85°C/85%RH conditions, moisture penetration causes hydrolysis of boron-oxygen complexes, generating mobile ions and accelerating recombination center diffusion. Damp heat test (1000 hours) caused PERC module LID degradation of 1.2%.

·Mechanical Stress: Module encapsulation stress causes micro-cracks in wafers. Oxygen concentration gradients at crack tips trigger local B-O complex formation. During thermal cycling (-40°C~85°C) tests, cracked modules had 0.9% higher LID degradation than intact modules.

Data-Driven LID Prediction Model

Physics-based LID prediction requires integrating multi-dimensional parameters:

·Key Variables: Boron concentration (B), Oxygen concentration (O), Effective carrier concentration (Δn), Temperature (T).

·Empirical Formula: LID degradation rate (%) = 0.003×B×O×exp(-Ea/(kT)), where Ea=0.85eV (activation energy of boron-oxygen recombination), k is Boltzmann constant.

·Measurement Verification: Statistics on 1000 PERC cells show formula prediction error <±0.2%, can guide wafer doping process optimization.

Degradation Rate Comparison

Laboratory Light-Induced Degradation Test Conditions and Data

Standardized LID laboratory testing procedure:

·Illumination Dose: 5 kWh/m² (AM1.5G spectrum, 1000 W/m² intensity)

·Temperature Control: 25°C constant temperature

·Test Duration: Continuous illumination for 100 hours

 

Technology Improvement

 

Boron Doping Alternatives

Root Problem: P-type PERC cells suffer first-year degradation up to 3% (lab data) due to boron-oxygen complexes (BO-LID).

Solutions:

·Gallium (Ga) Doping: Replace boron with gallium as dopant, avoiding BO-LID reaction pathway. Gallium's segregation coefficient (0.35) is lower than boron's (0.8), requiring adjustment of thermal field distribution:

o Crystal growth temperature: 1450°C → 1520°C (reduces Ga volatilization)

o Radial temperature gradient: <5°C/cm (improves crystal quality)

o Measured effect: LID degradation reduced from 3% to 0.7%, but resistivity fluctuation ±12%.

·Indium (In) Co-doping: Boron-indium co-doping (B: In=10:1) further reduces oxygen solubility:

o Oxygen content: 10ppma → 5ppma

o Minority carrier lifetime: 500μs → 800μs

o Cost increase: Wafer price increased by $0.005/W.

Annealing Process:

·Low-Temperature Annealing (LTA):

o Temperature: 200°C → 300°C

o Time: 10 minutes → 30 minutes

o Effect: Activates hydrogen passivation, repairs boron-oxygen defects

o Data: PERC cell LID degradation reduced by 0.5%.

Passivation Layer Upgrade

Surface Passivation Technology:

·AlOx/SiNx Stack:

o Thickness control: AlOx 3nm + SiNx 80nm

o Surface recombination velocity: <10 cm/s (conventional PERC 20 cm/s)

o Lab data: Minority carrier lifetime increased to >1500μs.

Rear Passivation Optimization:

·SiNx Thickness Adjustment:

o Conventional: 120nm → Optimized: 150nm

o Effect: Reduces boron diffusion to rear, suppresses LeTID

o Result: LeTID degradation reduced from 1.17% to 0.3%.

Conversion Efficiency

 

Mass production efficiency reaches 25.4% (SunPower Maxeon 7), laboratory record 26.8%, approaching the 28.7% theoretical limit;

PERC is stagnant at 23.5%. TOPCon's temperature coefficient is -0.29%/°C, bifaciality 85%+ increasing energy yield by 20%, degradation rate <0.4% per year, 30-year power retention 87%.

Theoretical Limits

Physical Boundary of Mono-crystalline PERC

Mono-crystalline PERC cells, based on P-type wafers, have a theoretical efficiency limit of 24.5% (Shockley-Queisser limit).

This value is determined by silicon's bandgap (1.1 eV) and solar spectrum match.

In mass production, boron doping leads to boron-oxygen complexes (B-O) causing light-induced degradation (LID), with first-year efficiency loss of 2-3%.

 

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