PV Module Damp Heat, Freeze-Thaw Test Chamber Model: CHT-19-12-3
Hot and heat test box Model: CHT-19-12-2
Thermal cycle environment test box Model: CHT-19-12-3
Optical aging stability test box Model: CHT-1800
Steady-state simulation test box Model: CHT-WTBBA
UV accelerated aging test box Model: CHT-UVDC28
Current Continuity Test System Model: CHT-11D
Diode Thermal Performance Test System Model: CHT-12D
Pulse voltage test system Model: CHT-14D
PV Module Salt Spray Corrosion Test Chamber:CHT-16D
Optical senescence test box / photovoltaic module test LID: CHT-18D
Insulation withstand voltage tester Model: CHT-2813W
Wet leakage test system Model: CHT-3621W
Outdoor sun exposure test system model: CHT-H206
Dynamic Load Test Machine Model: CHT-20D
Static load test machine model: CHT-26D
PID Test System Model: CHT-PID
Component crushing tester Model: CHT-30D
Grounding continuity Tester Model: CHT-2813W
Lead end strength test machine Model: CHT-31
Appearance table Model: CHT-W26
Drop ball impact test machine Model: CHT-10
Photovoltaic welding strip stripping force testing machine
photovoltaic welding strip stripping force integrated machine
Universal material testing machine
Photovoltaic glass four-point bending test machine model: CHT-4 WQJN
Crosslinking degree test System Model: EVA-CC
2nd element image instrument model: CHT-3020
Two-dimensional image instrument
Acetic acid test box Model: CHT-YW 400
High pressure Accelerated aging test box Model: CHT-HAST-800
Differential Scanning Calorimeter (DSC) Model: CHT-CS300
Spectrophotometer Model: CHT-3400
Fourier transform infrared spectrometer model: CHT-H8030
Photovoltaic welding strip stripping force testing machine
Photovoltaic welding strip stripping force integrated machine
Universal material testing machine
Full-spectrum Ellipsometer Model: CHT-TP 01
Water vapor transmission and filtration rate Model: CHT-40B
No-rotor vulcanizer model: CHT-LH 06
Atomic force microscope Model: CHT-AFM
Solar cell TLM grid line contact resistance analyzer model: CHT-6070 TLM
Battery cell light aging box Model: CHT-DCPBBA
Photovoltaic cell PL detector model: CHT-80D
Scan four-probe square resistance meter Model: CHT-4500 RH
Location:Home > Solutions > Chalcogenide
Perovskite - The third-generation solar cell technology with a promising future market.
In terms of technological development, solar cells can be divided into three generations:
Represented mainly by polycrystalline silicon and monocrystalline silicon batteries, they currently have relatively high technical maturity, photoelectric conversion efficiency and commercialization degree, and dominate the photovoltaic market. At present, the laboratory conversion efficiency of crystalline silicon batteries is getting closer and closer to its theoretical efficiency limit of 29.4%. The technical maturity and industrial chain have been highly developed, and there is limited room for further improvement.
It mainly includes types of solar cells such as gallium arsenide (GaAs). These batteries have the advantages of low raw material consumption, lighter weight and high flexibility of active materials, and can meet a variety of different application requirements. However, due to the toxicity or scarcity of some active materials used in these batteries, they cannot be used as a large-scale mass production technology at present.
It mainly includes new batteries represented by perovskite solar cells. These batteries have multiple advantages such as non-toxic raw materials, abundant reserves, low cost, simple process and flexible preparation. The theoretical conversion efficiency of single-junction perovskite solar cells reaches 33%. When combined with crystalline silicon batteries to form a tandem cell, the conversion efficiency will be further improved, and the future development prospects are broad. At present, most of the industry is still in the pilot line stage, and some leading enterprises will successively start the construction of GW-level production lines.
Perovskite solar cells belong to the third-generation battery technology.
Data Source: "Research on the Preparation of High-efficiency Perovskite Solar Cells at Low Cost" by Lv Feng, Huachuang Securities
It gets its name because its photoelectric conversion layer uses materials with a perovskite structure, referring to a class of materials with the general chemical formula ABX3. In the ABX3 crystal, BX6 forms a regular octahedron, and BX6 is connected by sharing the vertex X to form a three-dimensional framework, and A is embedded in the octahedral gap to stabilize the crystal structure. Among them, A is a monovalent cation with a large radius (such as methylammonium cation MA+, formamidinium cation FA+, cesium ion Cs+, etc.), B is a divalent cation with a small radius (such as lead ion Pb2+, tin ion Sn2+, germanium ion Ge2+, etc.), and X is usually a halogen anion (such as fluoride ion F-, chloride ion Cl-, bromide ion Br-, iodide ion I-, etc.). Common perovskite materials mainly include FAPbI3, MAPbI3, etc.
Figure: The Lattice Structure of Typical Perovskite Materials
Data Source: "Research Progress of Perovskite/Crystalline Silicon Tandem Solar Cells" by Li Chunjing, etc.
Figure: Diversified Application Scenarios
Figure: The Conversion Efficiency Rapidly Catches up with That of Crystalline Silicon Batteries
Figure: Important Nodes of the Conversion Efficiency of Perovskite Solar Cells
The maximum theoretical conversion efficiency of a single-junction perovskite battery is 33%. The bandgap of perovskite materials can be adjusted within a certain range according to different compositions, and the theoretical limit efficiency can reach 33%, which is close to the theoretical conversion efficiency limit of a single-junction battery of 33.7% (corresponding to an ideal bandgap of 1.34 eV), and higher than the theoretical limit of crystalline silicon of 29.4%.
Figure: The Expectation of Cost Reduction and Efficiency Improvement of Perovskite Solar Cells
Tandem cells composed of multi-junction cells can further improve the conversion efficiency. Taking a dual-junction cell as an example, a material with a wide bandgap is usually selected as the top cell, and a material with a narrow bandgap is selected as the bottom cell. Tandem cells have a wider spectral response range and higher conversion efficiency. The theoretical conversion efficiencies of dual-junction and triple-junction cells can reach 45% and 49% respectively.
The stability of perovskite materials is poor, and they are prone to decomposition. Perovskite materials are often used in environments with factors such as humidity, high temperature, and ultraviolet light. In such environments, the materials have poor stability and are prone to decomposition, resulting in changes in the internal structure of the materials, and ultimately causing the photoelectric conversion efficiency of perovskite solar cells to decline continuously.
Compared with other types of photovoltaic batteries, as the battery area increases, the conversion efficiency of perovskite batteries decreases more significantly.
Since the crystallization time of perovskite materials is very short, usually the process window is only a few seconds, and the preparation of large-area perovskite batteries requires a longer coating time, and the uniformity of crystallization will be difficult to control. During the crystallization process, if there is a defect, it will affect the conversion efficiency of the entire battery. Therefore, the coating process of the perovskite layer puts forward higher requirements for the stability of production equipment and processes.