Related Experiment Video
Updated: Mar 30, 2026

Morphology Control for Fully Printable Organic–Inorganic Bulk-heterojunction Solar Cells Based on a Ti-alkoxide and Semiconducting Polymer
Published on: January 10, 2017
Low bandgap semiconducting polymers for polymeric photovoltaics
Chang Liu1, Kai Wang1, Xiong Gong1
1College of Polymer Science and Polymer Engineering, Department of Polymer Engineering, The University of Akron, Akron, OH 44325, USA. xgong@uakron.edu.
Developing high-performance polymer solar cells (PSCs) and ultrasensitive photodetectors (PDs) requires designing low-bandgap (LBG) semiconducting polymers. Key strategies include optimizing electronic properties, broadening spectral absorption from UV to NIR, and enhancing charge carrier mobility for efficient energy conversion and sensing applications.
Area of Science:
- Materials Science
- Organic Electronics
- Photovoltaics
- Optoelectronics
Background:
- High-performance polymer solar cells (PSCs) and ultrasensitive photodetectors (PDs) require efficient light harvesting across the solar spectrum (UV to NIR).
- Low-bandgap (LBG) semiconducting polymers are crucial for achieving broad spectral response and high photocurrents in these devices.
- Current LBG polymers face limitations in charge carrier mobility, impacting device response times.
Purpose of the Study:
- To review effective design rules for developing LBG semiconducting polymers with enhanced optical and electronic properties.
- To explore strategies for improving molar absorptivity, energy levels, charge carrier mobility, and solubility.
- To discuss advancements in LBG polymers for efficient PSCs and ultrasensitive broadband PDs.
Main Methods:
- Overview of five key design rules for LBG semiconducting polymers.
- Strategies include fused heterocycles, bridging groups, electron-withdrawing units, donor-acceptor (D-A) copolymerization, and 2D conjugation.
- Analysis of polymer properties such as bandgap (Eg), absorption spectra, and charge carrier mobility.
Main Results:
- LBG semiconducting polymers with high molar absorptivity, suitable energy levels, and high solubility are achievable through rational design.
- D-A copolymerization and 2D conjugation effectively narrow the bandgap (Eg), enabling broad UV-NIR absorption (down to 0.8 eV, 1450 nm).
- Polymers exhibit excellent electronic and optic properties, making them promising for efficient PSCs and ultrasensitive PDs.
Conclusions:
- Rational design of LBG semiconducting polymers is essential for high-performance PSCs and ultrasensitive broadband PDs.
- Achieving broad spectral response requires lowering the bandgap, while improving response time necessitates enhanced hole mobility.
- Further advancements in hole mobility are critical for realizing uncooled, ultrasensitive broadband polymer PDs.
More Related Videos
06:49In situ Grazing Incidence Small Angle X-ray Scattering on Roll-To-Roll Coating of Organic Solar Cells with Laboratory X-ray Instrumentation
Published on: March 2, 2021
09:32Well-aligned Vertically Oriented ZnO Nanorod Arrays and their Application in Inverted Small Molecule Solar Cells
Published on: April 25, 2018
Related Concept Videos
Semiconductors
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Types of Semiconductors
P-N junction
Types of Step-Growth Polymers: Polyesters
Polyesters are commonly prepared from terephthalic acid and ethylene glycol; the crude product is known as poly(ethylene terephthalate) or PET. However, polyesters are synthesized industrially by transesterification of dimethyl terephthalate with ethylene glycol at 150 °C. The two reactants and the polymer...
Band Theory
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
Energy Bands in Solids
Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states...