IP Library Granted Patent US 10,985,247
Granted Patent B2
US 10,985,247 · App. 16/214,864 · Granted Apr 20, 2021

Layer, multilevel element, method for fabricating multilevel element, and method for driving multilevel element

Inventors: Myung Mo Sung (Seoul, KR); Jinwon Jung (Suwon-si, KR); Hongbum Kim (Seoul, KR); Jin Seon Park (Seoul, KR)
Assignee: IUCF-HYU (INDUSTRY-UNIVERSITY COOPERATION FOUNDATION HANYANG UNIVERSITY)
H01L29/151H01L29/04H01L29/122H01L29/15H01L29/152H01L29/22H01L29/2206H01L29/41725H01L29/4232H01L29/517H01L29/66969H01L29/7606H01L29/7613H01L29/7869H01L29/78693H01L29/78696H01L51/0562H01L29/66977
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Quick Facts
Patent No.
US 10,985,247
App. No.
16/214,864
Granted
Apr 20, 2021
Kind
B2
Abstract

A layer according to one embodiment of the present invention may exhibit a first number of electron states in a low-level electron energy range in a conduction band, and exhibit a second number of electron states in a high-level electron energy range higher than the low-level electron energy level in the conduction band, wherein localized states may exist between the low-level electron energy range and the high-level electron energy level.

Claims (12)

1. A layer comprising an amorphous region and a plurality of crystalline regions having a size of a few nanometers and surrounded by the amorphous region, wherein the layer has a thickness of 1.5 nm or more and 9 nm or less, and quantized conduction states of the layer are provided by resonant energy matching between any first energy state among first localized energy states of the amorphous region and any second energy state among second localized energy states of the plurality of crystalline regions.

2. The layer of claim 1 , wherein the plurality of crystalline regions exhibit a quantum confinement effect.

3. The layer of claim 2 , wherein the quantum confinement effect of the plurality of crystalline regions is exhibited in a triaxial direction.

4. The layer of claim 1 , wherein the quantized conduction states are provided at higher electron energy than a mobility edge which is the lowest energy state in which electrons are capable of existing in the conduction band.

5. The layer of claim 1 , wherein the plurality of crystalline regions are randomly distributed in the amorphous region and two-dimensionally arranged.

6. The layer of claim 1 , wherein the quantized conduction states exist in a predetermined electron energy range.

7. The layer of claim 6 , wherein localized states exist in a higher electron energy range than the predetermined electron energy range.

8. The layer of claim 7 , wherein conduction states exist in a higher electron energy range than an electron energy range corresponding to the non-conduction states.

9. The layer of claim 1 , wherein the number of the first energy states is larger than the number of the second energy states.

10. The layer of claim 1 , wherein the resonant energy matching provides a number of quantized electron states in a higher energy range than the mobility edge in terms of the density of states (DOS).

11. The layer of claim 1 , wherein the resonant energy matching provides at least two discrete electron states in a higher energy range than the mobility edge in terms of the density of states (DOS).

12. The layer of claim 1 , wherein the quantized conduction states limit an amount of current flowing through the layer.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jan 9, 2019
From: SUNG, MYUNG MO; JUNG, JINWON; KIM, HONGBUM; PARK, JIN SEON
To: IUCF-HYU (INDUSTRY-UNIVERSITY COOPERATION FOUNDATION HANYANG UNIVERSITY)
Reel/Frame 047943/0271 →
Priority Claims (3)
KR 10-2017-0134978 · Oct 18, 2017 · national
KR 10-2018-0124635 · Oct 18, 2018 · national
KR 10-2018-0124645 · Oct 18, 2018 · national
Continuity (2)
Continuation PCTKR2018012365 · Oct 18, 2018
Related Publication 20190115431A1 · Apr 18, 2019