Solid solutions of the form, Cu2-xAgxHgI4, were characterized by using differential scanning calorimetry and electrical conductivity techniques. Tetragonal phases were found over the entire range, apart for x-values of between 1.14 and 1.30; where a single cubic phase existed. It was found that the conductivity increased by 2 orders of magnitude at the transition temperature. The composition with x = 1.14 exhibited the highest room-temperature conductivity (table 257).
A.M.Sukeshini, K.Hariharan: Solid State Communications, 1991, 78[2], 85-7
Table 257
Room-Temperature Conductivity of Cu2AgHgI4
x | Temperature (K) | σ (S/cm) | Q (eV) |
0 | 303 | 3.0 x 10-8 | 0.64 |
0 | 333 | 2.1 x 10-6 | 0.64 |
0.2 | 303 | 6.0 x 10-8 | 0.61 |
0.2 | 333 | 2.7 x 10-6 | 0.61 |
0.6 | 303 | 1.7 x 10-6 | 0.52 |
0.6 | 333 | 2.0 x 10-4 | 0.52 |
0.8 | 303 | 1.8 x 10-6 | 0.50 |
0.8 | 333 | 2.2 x 10-4 | 0.50 |
1.0 | 303 | 3.1 x 10-6 | 0.47 |
1.0 | 333 | 4.7 x 10-4 | 0.47 |
1.14 | 303 | 1.8 x 10-5 | 0.47 |
1.14 | 333 | 9.9 x 10-4 | 0.47 |
1.3 | 303 | 1.47 x 10-5 | 0.47 |
1.3 | 333 | 1.35 x 10-3 | 0.47 |
1.4 | 303 | 6.6 x 10-6 | 0.44 |
1.4 | 333 | 1.03 x 10-3 | 0.44 |
1.6 | 303 | 6.2 x 10-6 | 0.45 |
1.6 | 333 | 1.38 x 10-3 | 0.45 |
1.8 | 303 | 2.2 x 10-6 | 0.41 |
1.8 | 333 | 1.38 x 10-3 | 0.41 |
2.0 | 303 | 6.5 x 10-6 | 0.39 |
2.0 | 333 | 1.26 x 10-3 | 0.39 |