1995 Volume 64 Issue 7 Pages 2684-2696
We reported previously a series of unexpected emergences with anomalies of transient photoconductivity Q(T, , λ ) of Cu2O below 100, K with decreasing temperature in contrast to the submergences of Q(T, , λ ) observed in most of normal photoconductor such as AgCl, AgBr, CdS at low temperatures. Here, we have reexamined the temperature variation of effective electric fields applied on the specimens of Cu2O, both experimentally and numerically in detail. By estimating an influence of the effective electric fields on the magnitude of Q(T, , λ ), we obtained further corrected results of Q(T, , λ ) qualitatively common to various Cu2O specimens below 100, K. These corrections established the overall behaviours of the “anomalous temperature dependence'' of Q(T, , λ ) of Cu2O previously reported especially below 100, K to be not influenced by a spurious effect. We give further discussion on the phenomena in terms of the mobility μ (T) and/or of the life time τ (T) due to usual trapping processes of photocarriers based on the one-electron approximation, but without success. Here, we note a finite value of photocarrier density n0, sustained even down to T=1.6, K. We eventually have to invoke a many-body aspect in elucidating these anomalous phenomena of Q(T, , λ ) and n0(T) observed in Cu2O.
This article cannot obtain the latest cited-by information.