The 65h JSAP Spring Meeting, 2018

Presentation information

Oral presentation

13 Semiconductors » 13.2 Exploratory Materials, Physical Properties, Devices

[19p-F202-1~16] 13.2 Exploratory Materials, Physical Properties, Devices

Mon. Mar 19, 2018 1:45 PM - 6:15 PM F202 (61-202)

Takashi Suemasu(Univ. of Tsukuba), Kenji Yamaguchi(QST), Kosuke Hara(Univ. of Yamanashi)

2:15 PM - 2:30 PM

[19p-F202-3] Analysis of impurity conduction in n-type GaAs based on a Hubbard-band model

Yasutomo Kajikawa1 (1.Shimane Univ.)

Keywords:hopping conduction, Hall effect

The low-temperature data of Hall-effect measurements on weakly compensated n-GaAs samples with donor concentrations ND less than the critical concentration for the metal-insulator transition reported in literature have been analyzed on the basis of a Hubbard-band model, which includes not only the bottom Hubbard band formed from the neutral donor (D0) states but also the top Hubbard band formed from the negatively charged donor (D-) states. In the model, the drift mobility and the Hall factor of nearest-neighbor hopping (NNH) in the top Hubbard band are assumed to be expressed as μ2 = μ02(E2/kBT)3/2exp(-E2/kBT) and AH2 = (kBT/JH2)exp(KH2E2/kBT), respectively, according to the small-polaron model, while those of variable-range hopping (VRH) in the bottom Hubbard band are assumed to be expressed as μ3 = μ03(TES/T)1/2exp[-(TES/T)1/2] and AH3 = AH03(TES/T)1/2exp[(1 - ν) (TES/T)1/2] according to the Efros-Shklovskii (ES) model. For the sample with a donor concentration of ND = 1.3 ×1015cm-3 and a compensation ratio of K = 0.27, it is shown that the Hall mobility is dominated by NNH in the top Hubbard band in a temperature range of 3.5-15 K while it is dominated by ES VRH in the bottom Hubbard band below 3.3 K.