|
|
|
|
LEADER |
01000caa a22002652 4500 |
001 |
NLM366438239 |
003 |
DE-627 |
005 |
20240329000321.0 |
007 |
cr uuu---uuuuu |
008 |
231229s2024 xx |||||o 00| ||eng c |
024 |
7 |
|
|a 10.1002/adma.202304338
|2 doi
|
028 |
5 |
2 |
|a pubmed24n1353.xml
|
035 |
|
|
|a (DE-627)NLM366438239
|
035 |
|
|
|a (NLM)38153167
|
040 |
|
|
|a DE-627
|b ger
|c DE-627
|e rakwb
|
041 |
|
|
|a eng
|
100 |
1 |
|
|a Daw, Debottam
|e verfasserin
|4 aut
|
245 |
1 |
0 |
|a Ultrafast Negative Capacitance Transition for 2D Ferroelectric MoS2/Graphene Transistor
|
264 |
|
1 |
|c 2024
|
336 |
|
|
|a Text
|b txt
|2 rdacontent
|
337 |
|
|
|a ƒaComputermedien
|b c
|2 rdamedia
|
338 |
|
|
|a ƒa Online-Ressource
|b cr
|2 rdacarrier
|
500 |
|
|
|a Date Revised 28.03.2024
|
500 |
|
|
|a published: Print-Electronic
|
500 |
|
|
|a Citation Status PubMed-not-MEDLINE
|
520 |
|
|
|a © 2024 Wiley‐VCH GmbH.
|
520 |
|
|
|a Negative capacitance gives rise to subthreshold swing (SS) below the fundamental limit by efficient modulation of surface potential in transistors. While negative-capacitance transition is reported in polycrystalline Pb(Zr0.2Ti0.8)O3 (PZT) and HfZrO2 (HZO) thin-films in few microseconds timescale, low SS is not persistent over a wide range of drain current when used instead of conventional dielectrics. In this work, the clear nano-second negative transition states in 2D single-crystal CuInP2S6 (CIPS) flakes have been demonstrated by an alternative fast-transient measurement technique. Further, integrating this ultrafast NC transition with the localized density of states of Dirac contacts and controlled charge transfer in the CIPS/channel (MoS2/graphene) a state-of-the-art device architecture, negative capacitance Dirac source drain field effect transistor (FET) is introduced. This yields an ultralow SS of 4.8 mV dec-1 with an average sub-10 SS across five decades with on-off ratio exceeding 107, by simultaneous improvement of transport and body factors in monolayer MoS2-based FET, outperforming all previous reports. This approach could pave the way to achieve ultralow-SS FETs for future high-speed and low-power electronics
|
650 |
|
4 |
|a Journal Article
|
650 |
|
4 |
|a Dirac source
|
650 |
|
4 |
|a negative capacitance
|
650 |
|
4 |
|a subthreshold‐swing
|
650 |
|
4 |
|a transient measurements
|
650 |
|
4 |
|a van der Waals ferroelectrics
|
700 |
1 |
|
|a Bouzid, Houcine
|e verfasserin
|4 aut
|
700 |
1 |
|
|a Jung, Moonyoung
|e verfasserin
|4 aut
|
700 |
1 |
|
|a Suh, Dongseok
|e verfasserin
|4 aut
|
700 |
1 |
|
|a Biswas, Chandan
|e verfasserin
|4 aut
|
700 |
1 |
|
|a Hee Lee, Young
|e verfasserin
|4 aut
|
773 |
0 |
8 |
|i Enthalten in
|t Advanced materials (Deerfield Beach, Fla.)
|d 1998
|g 36(2024), 13 vom: 27. März, Seite e2304338
|w (DE-627)NLM098206397
|x 1521-4095
|7 nnns
|
773 |
1 |
8 |
|g volume:36
|g year:2024
|g number:13
|g day:27
|g month:03
|g pages:e2304338
|
856 |
4 |
0 |
|u http://dx.doi.org/10.1002/adma.202304338
|3 Volltext
|
912 |
|
|
|a GBV_USEFLAG_A
|
912 |
|
|
|a SYSFLAG_A
|
912 |
|
|
|a GBV_NLM
|
912 |
|
|
|a GBV_ILN_350
|
951 |
|
|
|a AR
|
952 |
|
|
|d 36
|j 2024
|e 13
|b 27
|c 03
|h e2304338
|