TY - JOUR
T1 - Hf0.4Zr0.6O2 Thickness-Dependent Transfer Characteristics of InxZn1-xOy Channel Ferroelectric FETs
AU - Jeong, Jiae
AU - Park, Hyoungjin
AU - Kim, Jihyun
AU - Moon, Hojin
AU - Choi, Hyeonsik
AU - Kim, Eunjin
AU - Jeon, Seonuk
AU - Kim, Yunsur
AU - Woo, Jiyong
N1 - Publisher Copyright:
© 2024 American Chemical Society.
PY - 2024/10/10
Y1 - 2024/10/10
N2 - We investigate how the threshold voltage (VT) is adjusted to create a memory window (MW) in ferroelectric field-effect transistors (FeFETs) composed of ferroelectric Hf0.4Zr0.6O2 and InZnO (In2O3:ZnO = 9:1 wt %). Temperature-dependent polarization measurements reveal a dipole switching in Hf0.4Zr0.6O2. The properties of the n-type InZnO channel are examined by fabricating an oxide transistor with an HfO2 gate dielectric. Upon replacement of HfO2 with Hf0.4Zr0.6O2 in the oxide transistor, a counterclockwise MW is observed. Specifically, as the Hf0.4Zr0.6O2 thickness increases from 16 to 24 nm, the VT of the FeFET after a + gate voltage (VG) sweep remains nearly constant, while the VT after a −VG sweep shifts significantly from −0.9 to 0.5 V. The enlarged MW of approximately 2 V, which is proportional to the Hf0.4Zr0.6O2 thickness in the FeFET, can be explained by considering the balance between VG controllability across the gate stack and the ferroelectric switching of Hf0.4Zr0.6O2
AB - We investigate how the threshold voltage (VT) is adjusted to create a memory window (MW) in ferroelectric field-effect transistors (FeFETs) composed of ferroelectric Hf0.4Zr0.6O2 and InZnO (In2O3:ZnO = 9:1 wt %). Temperature-dependent polarization measurements reveal a dipole switching in Hf0.4Zr0.6O2. The properties of the n-type InZnO channel are examined by fabricating an oxide transistor with an HfO2 gate dielectric. Upon replacement of HfO2 with Hf0.4Zr0.6O2 in the oxide transistor, a counterclockwise MW is observed. Specifically, as the Hf0.4Zr0.6O2 thickness increases from 16 to 24 nm, the VT of the FeFET after a + gate voltage (VG) sweep remains nearly constant, while the VT after a −VG sweep shifts significantly from −0.9 to 0.5 V. The enlarged MW of approximately 2 V, which is proportional to the Hf0.4Zr0.6O2 thickness in the FeFET, can be explained by considering the balance between VG controllability across the gate stack and the ferroelectric switching of Hf0.4Zr0.6O2
UR - https://www.scopus.com/pages/publications/85206019593
U2 - 10.1021/acs.jpclett.4c02201
DO - 10.1021/acs.jpclett.4c02201
M3 - Article
C2 - 39360934
AN - SCOPUS:85206019593
SN - 1948-7185
VL - 15
SP - 10258
EP - 10264
JO - Journal of Physical Chemistry Letters
JF - Journal of Physical Chemistry Letters
IS - 40
ER -