TY - JOUR
T1 - Hall factor in ultrathin-body silicon-on-insulator n-type metal-oxide-semiconductor field-effect transistors
AU - Kobayashi, Shigeki
AU - Saitoh, Masumi
AU - Nakabayshi, Yukio
AU - Ishihara, Takamitsu
AU - Numata, Toshinori
AU - Uchida, Ken
PY - 2010/4
Y1 - 2010/4
N2 - Hall factor (γH) is investigated experimentally in the ultrathin-body (UTB) silicon-on-insulator (SOI) n-type metal-oxide-semiconductor field-effect transistors (MOSFETs) with the SOI thicknesses (TSOI) of less than 10 nm. It is demonstrated experimentally for the first time that when T SOI is thicker than 4.2 nm, γH decreases slightly with a reduction of TSOI, whereas when TSOI is thinner than 4.2 nm, γH decreases drastically and becomes almost unity in TSOI of 2.5 nm. The γH is calculated considering only phonon scattering. Then, calculated γH is compared with γH obtained experimentally. In addition, it is found that in phonon scattering γH is determined dominantly by the intravalley scatterings of the twofold valleys. The dominance of the intravalley scatterings of the twofold valleys in the γH determination is attributed to the energy levels of subbands whereby most of the scatterings are the intravalley scatterings of the twofold valleys.
AB - Hall factor (γH) is investigated experimentally in the ultrathin-body (UTB) silicon-on-insulator (SOI) n-type metal-oxide-semiconductor field-effect transistors (MOSFETs) with the SOI thicknesses (TSOI) of less than 10 nm. It is demonstrated experimentally for the first time that when T SOI is thicker than 4.2 nm, γH decreases slightly with a reduction of TSOI, whereas when TSOI is thinner than 4.2 nm, γH decreases drastically and becomes almost unity in TSOI of 2.5 nm. The γH is calculated considering only phonon scattering. Then, calculated γH is compared with γH obtained experimentally. In addition, it is found that in phonon scattering γH is determined dominantly by the intravalley scatterings of the twofold valleys. The dominance of the intravalley scatterings of the twofold valleys in the γH determination is attributed to the energy levels of subbands whereby most of the scatterings are the intravalley scatterings of the twofold valleys.
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U2 - 10.1143/JJAP.49.04DC23
DO - 10.1143/JJAP.49.04DC23
M3 - Article
AN - SCOPUS:77952728263
SN - 0021-4922
VL - 49
JO - Japanese journal of applied physics
JF - Japanese journal of applied physics
IS - 4 PART 2
M1 - 04DC23
ER -