TY - JOUR
T1 - Determination of the impurity concentration in heavily doped inhomogeneous semiconductors from the measurement of the low-temperature conductivity
AU - Shlimak, I.
AU - Ussyshkin, R.
AU - Resnick, L.
AU - Ginodman, V.
PY - 1995/8
Y1 - 1995/8
N2 - A method has been developed for determining the effective concentration of shallow impurities N* reponsible for the low-temperature conductivity in the vicinity of the metal-insulator transition for inhomogeneous samples of n-Ge:As. The method is based on the measurement of two ratios of sample resistance γ-R(4.2 K)/R(300 K), β=R(2.0 K)/R(4.2 K) and the conductivity σ(4.2 K). The next step consists of plotting and σ(4.2) vs β. Assuming that β is the most reliable parameter, one can calculate, after an averaging procedare, the corrected values of γ*, π*(4.2) and the resistivity at room temperature ρ*(300)=[γ*π*(4.2)]-1. Finally, using the known dependence ρ(300)=f(N) for homogeneous samples, one can obtain the values of N*. The dependences of N* on β and on γ are plotted. The scaling behavior of the conductivity of the Ge:As samples with corrected values of π*(4.2) and N* has been observed down to T=100 mK.
AB - A method has been developed for determining the effective concentration of shallow impurities N* reponsible for the low-temperature conductivity in the vicinity of the metal-insulator transition for inhomogeneous samples of n-Ge:As. The method is based on the measurement of two ratios of sample resistance γ-R(4.2 K)/R(300 K), β=R(2.0 K)/R(4.2 K) and the conductivity σ(4.2 K). The next step consists of plotting and σ(4.2) vs β. Assuming that β is the most reliable parameter, one can calculate, after an averaging procedare, the corrected values of γ*, π*(4.2) and the resistivity at room temperature ρ*(300)=[γ*π*(4.2)]-1. Finally, using the known dependence ρ(300)=f(N) for homogeneous samples, one can obtain the values of N*. The dependences of N* on β and on γ are plotted. The scaling behavior of the conductivity of the Ge:As samples with corrected values of π*(4.2) and N* has been observed down to T=100 mK.
KW - 72.20
KW - 81.40
UR - http://www.scopus.com/inward/record.url?scp=0029356494&partnerID=8YFLogxK
U2 - 10.1007/BF01538375
DO - 10.1007/BF01538375
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AN - SCOPUS:0029356494
SN - 0947-8396
VL - 61
SP - 115
EP - 118
JO - Applied Physics A: Materials Science and Processing
JF - Applied Physics A: Materials Science and Processing
IS - 2
ER -