Description
Learn
about tandem solar cells, their working principle, structure, efficiency,
advantages, challenges, and future.
Introduction
The theoretical limits of single solar cell are 30%. The William
Shockley and Hans Joachim Queisser made discovery about 50 years ago, called it
Shockley – Quisser limit. They theoretically calculated that solar panels with
one single layer suffer efficiency limitations as they are unable to absorb
full solar light. In the tandem cell, two solar cells stack one on top of the
other in which top cells are transparent, convert high energy photons into
electricity. The bottom cell absorbs lower energy photons. The solar spectrum
splits into two layers dramatically reduces thermalization losses. This will
enable theoretically efficiency far better than single layer cells.
Operating Principle
In a tandem cell, the incident sunlight passes through the top sub
cell first. High energy photons (blue and green wavelengths) are absorbed by
the wide band gap perovskite layer, converting them at higher voltage similarly
lower energy photons (red and near-infrared) transmitted through the top cell
are captured by the silicon bottom cell. This spectrum splitting dramatically
reduces thermalization losses in single junction cells.
Structure
The tandem
devices are commonly fabricated in either two terminals or four terminals’
configurations. The sub cells are electrically connected in series and same
current flows through all layers in the two terminals tandems. This design
offers simple module integration and reduced wiring complexity but current
matching between top and bottom cells.
The perovskite
silicon tandem solar cells have strong efficiency potential. The perovskite
layer absorbs high energy protons, while the silicon cell converts the lower
energy photons. The structure of Perovskite tandem solar cell and function of
each layer is explained here.
Structure
of Perovskite Tandem solar cell
The
function of each layer is given here.
|
Layer |
Function |
|
Glass substrate |
Provide mechanical support and protects solar cell from
environment |
|
Anti reflection coating (ARC) |
Minimizes light reflection and increases the amount of sunlight
entering the cell |
|
Transparent conductive oxide (TCO) |
Conducts electrical current, when sunlight pass through it |
|
Electron transport layer (ETL) |
Extracts and transports electrons from the perovskite absorber
to the electrode while blocking holes. |
|
Perovskite absorber (Top Cell) |
Absorbs high energy (short-wavelength) sunlight and generates
electron-hole pairs |
|
Hole transport layer (HTL) |
Extracts and transports holes from the perovskite layer while
blocking electrons |
|
Recombination / Interconnection Layer |
Electrically connects the top and bottom cells and enables
carrier recombination between them |
|
N type silicon layer |
Selectively collects electrons and reduces recombination losses
in the silicon cell. |
|
Silicon absorber (Bottom Cell) |
Absorbs lower energy (long wavelength) light that passes through
the perovskite layer |
|
P type Silicon Layer |
Collects holes generated in the silicon absorber and transports
them to the electrode |
|
Rear TCO (if present) |
Provides a conductive path and improves current collection. |
Recombination Junction
The junction is the most critical component unique to tandem
cells. It must allow electrons flow from the bottom sub cell to recombine with
holes from the top sub cell (completing the internal circuit) with minimal
optical absorption and electrical resistance. Transparent conductive oxides
(ITO, AZO) or ultrathin metallic layers are commonly used.
Current Matching
In a two terminal series connected tandem, the sub-cell generating
the lower photocurrent than total output — a condition known as current
matching. The perovskite layer thickness and band gap must be precisely tuned
so that both sub cells produce equal photocurrents under the AM1.5G (Air mass
1.5 Global) solar spectrum.
AM1.5G* - Air mass is the path length in which light takes through
atmosphere normalized to the shortest possible path length to surface when sun
is directly overhead. The 1.5 means sun light travelled through path length 1.5
times longer than direct overhead sunlight at sea level (AM 1.0G)
Salient Feature of the Perovskite Tandem Solar Cells
The following are the salient feature of the Perovskite Tandem
Solar Cells.
•
The
laboratory efficiency as per LONGI (Green energy Technology Company) achieves
33.9% efficiency in 2024.
•
The
theoretical efficiency of two junction solar cell roughly 45% to 47% under
concentrated sunlight.
•
It can
capture both high energy and low energy solar photons
•
The standard
monocrystalline silicon solar panel efficiency around 22 – 24% in commercial
models. Its efficiency needs to reach around 33 – 36% to produce 50% more
efficiency per unit area. An individual solar cell cannot achieve this due to
Shockley – Queisser limit caps them at around 29.4%. The tandem solar cells
drastically increase power output.
•
The
perovkites degraded when exposed to heat, moisture, UV light during fabrication
processes.
•
In a
monolithic two terminal tandems, the entire device output is limited by lowest
performing sub cell.
• The mismatch of wavelength lead to unused photons resulting significant leakage current.
FAQs
What are tandem solar cells?
Tandem
solar cells combine two photovoltaic materials to improve efficiency.
How efficient are tandem solar
cells?
Laboratory
efficiencies exceed 33%, with theoretical efficiencies of about 45–47% under
concentrated sunlight.
Why is perovskite used?
It
efficiently absorbs high-energy photons while silicon absorbs lower-energy
photons.
What are the challenges?
Stability,
moisture, UV degradation, and current matching.
Are tandem solar cells the future?
They are among the most promising next-generation solar technologies.

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