scholarly journals Dielectric properties of ultrathin metal films around the percolation threshold

2010 ◽  
Vol 81 (3) ◽  
Author(s):  
Martin Hövel ◽  
Bruno Gompf ◽  
Martin Dressel
2000 ◽  
Vol 113 (15) ◽  
pp. 6330-6333 ◽  
Author(s):  
Oliver Krauth ◽  
Gerhard Fahsold ◽  
Norbert Magg ◽  
Annemarie Pucci

2011 ◽  
Vol 20 (4) ◽  
pp. 047201 ◽  
Author(s):  
Jun Quan ◽  
Ying Tian ◽  
Jun Zhang ◽  
Le-Xi Shao

1991 ◽  
Vol 46 (1) ◽  
pp. 241-246 ◽  
Author(s):  
P. Tippmann-Krayer ◽  
W. Meisel ◽  
U. Höhne ◽  
H. Möhwald

2009 ◽  
Vol 95 (24) ◽  
pp. 243114 ◽  
Author(s):  
Y. Liu ◽  
T. Miller ◽  
T.-C. Chiang

2019 ◽  
Vol 2019 ◽  
pp. 1-8
Author(s):  
Darya Meisak ◽  
Jan Macutkevic ◽  
Dzmitry Bychanok ◽  
Algirdas Selskis ◽  
Juras Banys ◽  
...  

A series of polymer composites based on epoxy resin with a 5–40 vol.% concentration of goethite (Fe2O3·H2O) nanorods was produced. The electrical percolation threshold in these composites was determined as 30 vol.% of nanorods. The dielectric properties of the composites both below and above the percolation threshold were studied in a wide temperature (200 K–450 K) and frequency (from Hz to THz) ranges. The dielectric properties of composites below the percolation threshold are mainly determined by the relaxation in a pure polymer matrix. The electrical properties of composites above the percolation threshold are determined by the percolation network, which is formed by the goethite nanorods inside the polymer matrix. Due to the finite conductivity of the epoxy resin, the electrical conductivity at high temperatures occurs in the composites both above and below the percolation threshold.


Sign in / Sign up

Export Citation Format

Share Document