Related Experiment Video
Updated: Jan 10, 2026

Characterization of Thermal Transport in One-dimensional Solid Materials
Published on: January 26, 2014
Understanding thermal transport in polymer semiconductors via two-channel mechanism
Chunlin Xu1,2, Dongyang Wang3, Zhaodong Zhu4
1State Key Laboratory of Flexible Electronics Technology, Beijing Tsinghua Institute for Frontier Interdisciplinary Innovation, Tsinghua University, Beijing, PR China.
Abstract:
The vibrational thermal conductivity of polymer semiconductors is critical to the performance of organic electronic devices, yet its underlying mechanisms remain elusive. This work presents a two-channel model to elucidate the vibrational heat transport in semiconducting polymers with extended side chains. We reveal a striking splitting of vibrational modes along the polymer chain, driven by the substantial difference in force constants between the backbone and side chains. This gives rise to two distinct dispersive longitudinal branches: a backbone branch, characterized by phonon-like propagons that govern thermal conductivity, and a side chain branch, consisting of non-propagating diffusons that make minimal contributions to heat transport. The reduced maximum thermal conductivity of these polymer semiconductors, compared to their side chain-free counterparts, is attributed to phonon scattering by the low-frequency optical modes of the side chains. Our findings establish a foundation for strategically modifying side chains as a potent approach to fine-tuning thermal conductivity.
Related Concept Videos
Carrier Transport
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
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
Metal-Semiconductor Junctions
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Carrier Generation and Recombination
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
Fermi Level
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...

