Mechanism of high-temperature quantum dot operation in isoelectronic-trap-assisted tunnel FETs
ORAL
Abstract
Silicon spin qubit is one of the promising candidates as a building block of quantum computers. Recently, Si tunnel-FET (TFET)-type qubits have successfully operated at high temperatures up to 10 K, which employs the electronic state of the isoelectronic trap (IET) impurity as a quantum dot. To investigate the mechanism of their high-temperature operation, as a first step, we develop a device simulator reproducing their single-electron transistor (SET) operation. In this presentation, we report the device simulation clarifying the high-temperature SET operation mechanism.
This device operates as a SET with tunneling between the source and drain intermediated with the IET state. Firstly, short gate length must be employed such that tunneling distances are sufficiently short. Secondly, the quantum dot should be located far from the source and drain, to avoid Coulomb repulsion between a charged quantum dot and surrounding electrons hindering the charge up of the quantum dot. This requirement becomes stricter at high temperatures because the number of surrounding electrons increases. Thirdly, the localized IET state is preferred to produce a small quantum dot. This causes a deep potential distribution when the quantum dot is charged up, resulting in large charging energy. Satisfying these three requirements enables high-temperature SET operation of the devices.
This device operates as a SET with tunneling between the source and drain intermediated with the IET state. Firstly, short gate length must be employed such that tunneling distances are sufficiently short. Secondly, the quantum dot should be located far from the source and drain, to avoid Coulomb repulsion between a charged quantum dot and surrounding electrons hindering the charge up of the quantum dot. This requirement becomes stricter at high temperatures because the number of surrounding electrons increases. Thirdly, the localized IET state is preferred to produce a small quantum dot. This causes a deep potential distribution when the quantum dot is charged up, resulting in large charging energy. Satisfying these three requirements enables high-temperature SET operation of the devices.
* This work was supported by JST CREST Grant No. JPMJCR1871, and MEXT Quantum Leap Flagship Program (Q-LEAP) Grant No. JPMXS0118069228, Japan.
–
Presenters
-
Shota Iizuka
AIST
Authors
-
Shota Iizuka
AIST
-
Hidehiro Asai
AIST
-
Kimihiko Kato
AIST
-
Hiroshi Oka
AIST
-
Junichi Hattori
AIST
-
Koichi Fukuda
AIST
-
Takahiro Mori
AIST