The patent badge is an abbreviated version of the USPTO patent document. The patent badge does contain a link to the full patent document.

The patent badge is an abbreviated version of the USPTO patent document. The patent badge covers the following: Patent number, Date patent was issued, Date patent was filed, Title of the patent, Applicant, Inventor, Assignee, Attorney firm, Primary examiner, Assistant examiner, CPCs, and Abstract. The patent badge does contain a link to the full patent document (in Adobe Acrobat format, aka pdf). To download or print any patent click here.

Date of Patent:
Jan. 21, 2025

Filed:

Nov. 15, 2022
Applicant:

Taiwan Semiconductor Manufacturing Company, Ltd., Hsinchu, TW;

Inventors:

Rainer Yen-Chieh Huang, Hsinchu, TW;

Hai-Ching Chen, Hsinchu, TW;

Chung-Te Lin, Tainan, TW;

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
H01L 29/78 (2006.01); H01L 21/28 (2006.01); H01L 29/51 (2006.01); H01L 29/66 (2006.01); H10B 51/30 (2023.01);
U.S. Cl.
CPC ...
H10B 51/30 (2023.02); H01L 29/40111 (2019.08); H01L 29/516 (2013.01); H01L 29/6684 (2013.01); H01L 29/78391 (2014.09);
Abstract

The present disclosure relates to an integrated circuit (IC) in which a memory structure comprises a ferroelectric structure without critical-thickness limitations. The memory structure comprises a first electrode and the ferroelectric structure. The ferroelectric structure is vertically stacked with the first electrode and comprises a first ferroelectric layer, a second ferroelectric layer, and a first restoration layer. The second ferroelectric layer overlies the first ferroelectric layer, and the first restoration layer is between and borders the first and second ferroelectric layers. The first restoration layer is a different material type than that of the first and second ferroelectric layers and is configured to decouple crystalline lattices of the first and second ferroelectric layers so the first and second ferroelectric layers do not reach critical thicknesses. A critical thickness corresponds to a thickness at and above which the orthorhombic phase becomes thermodynamically unstable, such that remanent polarization is lost.


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