Impact of Saturated Spontaneous Polarization on the Endurance Fatigue of Si FeFET With Metal/Ferroelectric/Interlayer/Si Gate Structure
Min Liao, Hao Xu, Jiahui Duan, Shujing Zhao, Fengbin Tian, Junshuai Chai, Kai Han, Yibo Jiang, Jinjuan Xiang, Wenwu Wang, Xiaolei Wang
Abstract
We investigate the impact of saturated spontaneous polarization ( <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${P}_{\text {s}}{)}$ </tex-math></inline-formula> of the ferroelectric on endurance fatigue of Si FeFET with Metal/Ferroelectric/Interlayer/Si (MFIS) gate structure. We tune the <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${P}_{\text {s}}$ </tex-math></inline-formula> in the range of 25.9– <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$6.4 \mu \text{C}$ </tex-math></inline-formula> /cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> by changing the gate structure, such as the insertion of a dielectric layer and annealing temperature. When the <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${P}_{\text {s}}$ </tex-math></inline-formula> decreases from 12.1 to <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$6.4 \mu \text{C}$ </tex-math></inline-formula> /cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> , the memory window of the device decreases while the endurance improves. When the <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${P}_{\text {s}}$ </tex-math></inline-formula> decreases from 12.1 to <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$8.1 \mu \text{C}$ </tex-math></inline-formula> /cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> , the memory window disappears. However, when the <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${P}_{\text {s}}$ </tex-math></inline-formula> is lower than <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$8.1 \mu \text{C}$ </tex-math></inline-formula> /cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> , the memory window reappears. Smaller <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${P}_{\text {s}}$ </tex-math></inline-formula> leads to a smaller memory window, which reduces the read noise margin of the memory and is disadvantageous to endurance. Whereas smaller <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${P}_{\text {s}}$ </tex-math></inline-formula> leads to weaker charge trapping behavior, which is advantageous to endurance. Our work shows that the endurance characteristic is determined by the competition between the above two processes.