Strategies for a Wide Memory Window of Ferroelectric FET for Multilevel Ferroelectric VNAND Operation
Ilho Myeong, Hyoseok Kim, Seung‐Hyun Kim, Suhwan Lim, Kwangsu Kim, Wanki Kim, Daewon Ha, Sujin Ahn, Jaihyuk Song
Abstract
Basic gate stack structure of the Ferroelectric FET is Metal-ferroelectric-insulator-silicon (MFIS), where the memory window (M.W) is 2*(P <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">r</sub> -Q <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">it</sub> )/C <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">FE</sub> considering the trapped charge. However, in Metal - insulator - ferroelectric - insulator - silicon (MIFIS) gate-stacked FeFETs, the M.W is 2*{(P <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">r</sub> -Q <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">it</sub> )/C <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">FE</sub> + (Q’ <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">it</sub> -Q <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">it</sub> )/C <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">G.IL</sub> )}, which allows the M.W to widen in case the Q’ <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">it</sub> injected from the gate side is larger than the Q <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">it</sub> injected from the channel side. In this paper, we propose a band engineered (BE) gate insulator in MIFIS gate-stacked FeFETs. This lowers the energy barrier of the hole when applying the program voltage, thereby increasing the amount of hole injected from the gate side, and consequently widening the M.W. Furthermore, it is demonstrated by TCAD simulation that the physical origins of Vt shift of PGM state is hole injection. In addition, in the case of BE-MIFIS gate-stacked FeFETs, the maximum ISPP slope is increased by about 2 times compared to conventional MIFIS, which is an important feature in ferroelectric VNAND (FeVNAND) operated at low voltage.