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Thermophysical properties of SnO sub(2)-based transparent conductive films: Effect of dopant species and structure compared with In sub(2)O sub(3)-, ZnO-, and TiO sub(2)-based films
Thermophysical properties of SnO sub(2)-based transparent conductive films: Effect of dopant species and structure compared with In sub(2)O sub(3)-, ZnO-, and TiO sub(2)-based films
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Thermophysical properties of SnO sub(2)-based transparent conductive films: Effect of dopant species and structure compared with In sub(2)O sub(3)-, ZnO-, and TiO sub(2)-based films
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Thermophysical properties of SnO sub(2)-based transparent conductive films: Effect of dopant species and structure compared with In sub(2)O sub(3)-, ZnO-, and TiO sub(2)-based films
Thermophysical properties of SnO sub(2)-based transparent conductive films: Effect of dopant species and structure compared with In sub(2)O sub(3)-, ZnO-, and TiO sub(2)-based films

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Thermophysical properties of SnO sub(2)-based transparent conductive films: Effect of dopant species and structure compared with In sub(2)O sub(3)-, ZnO-, and TiO sub(2)-based films
Thermophysical properties of SnO sub(2)-based transparent conductive films: Effect of dopant species and structure compared with In sub(2)O sub(3)-, ZnO-, and TiO sub(2)-based films
Journal Article

Thermophysical properties of SnO sub(2)-based transparent conductive films: Effect of dopant species and structure compared with In sub(2)O sub(3)-, ZnO-, and TiO sub(2)-based films

2014
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Overview
We investigate the effect of dopant species and structure on the thermal conductivity of Sb-doped SnO2 (ATO) and Ta-doped SnO2 (TTO) films and compare the results with those of In2O3-, ZnO-, and TiO2-based transparent conductive films. The thermal conductivities () of polycrystalline ATO and TTO films are 4.44.9 and 4.7 W m1 K1, respectively. The thermal conductivities via phonons (ph) are almost identical for both dopant species (Sb and Ta): 4.3 and 4.5 W m1 K1 for Sb and Ta, respectively, on average. These results for ph are larger than that for Sn-doped In2O3 films (3.8 W m1 K1) and considerably larger than that for amorphous ATO films (1.0 W m1 K1). These facts lead us to conclude that the base-material species (SnO2 or In2O3) and structure (polycrystalline or amorphous) affect the thermophysical properties of ATO and TTO much more than the dopant species.

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