2013
DOI: 10.7567/jjap.53.014201
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Physical modeling of program and erase speeds of metal–oxide–nitride–oxide–silicon cells with three-dimensional gate-all-around architecture

Abstract: We present an investigation of the program and erase speed characteristics of three-dimensional (3D) gate-all-around (GAA) metal–oxide–SiN X –oxide–silicon (MONOS) cells. The effect of the tunneling oxide layer thickness in 3D GAA MONOS cells has been experimentally investigated and studied by 3D technology computer-aided design (TCAD) simulation. In particular, we considered physical parameters such as trap density, capture cross section, and trap level in order to analy… Show more

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Cited by 10 publications
(5 citation statements)
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“…The trap concentration considered in this work was fixed at 10 19 cm −3 with trap energy level 1 eV. The considered trap energy level is consistent with the work reported by authors in Reference 43. Models used for the analysis of the flash device are consistent with the published literature 44 and calibrated against the experimental results 45…”
Section: Device Design and Simulation Methodologymentioning
confidence: 58%
See 1 more Smart Citation
“…The trap concentration considered in this work was fixed at 10 19 cm −3 with trap energy level 1 eV. The considered trap energy level is consistent with the work reported by authors in Reference 43. Models used for the analysis of the flash device are consistent with the published literature 44 and calibrated against the experimental results 45…”
Section: Device Design and Simulation Methodologymentioning
confidence: 58%
“…The simulations were carried out using field, and concentration-dependent mobility models, drift-diffusion transport phenomena, and Shockley-Read-Hall model. 42 The high field phenomenon, like the hot electron effect, will not be prevalent at an applied drain bias of 1 V. 43 The transient analysis was performed to analyze the trapping and detrapping of the charge carriers in the nitride layer. 42 The charge transport through the dielectric layers has been considered through the Poole-Frenkel model.…”
Section: Device Design and Simulation Methodologymentioning
confidence: 99%
“…where the effective mass (m * n) and the capture-cross section of electron in the SiN layer (σn) are 0.42m0 and 1×10 -14 cm 2 , respectively [11], [32].…”
Section: Figure 6 (A) 2-d Conduction Energy Band Diagram (Ec) Along the Channel Direction (A-a') And (B) The Vertical Direction (B-b')mentioning
confidence: 99%
“…Channel doping concentration N A (cm −3 ) 1 0 16 S=D doping concentration N D (cm −3 ) 1 0 20 Grain boundary trap states N GB 23,24) (cm −2 eV −1 ) 1 0 12 -10 14 energy levels of electrons and holes were assumed to be 1.2 and 2.5 eV, respectively. 25,26) The program bias condition was a 16 V single pulse with a 1 ms hold time, and the read bias increased up to 4 V at various V d values. The program operation of the adjacent cell was performed to examine the influence of stored charges in the adjacent cell, as shown in Fig.…”
Section: Simulation Structure and Bias Conditionsmentioning
confidence: 99%