2019
DOI: 10.1109/temc.2018.2830182
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Dielectric Surface Roughness Scattering Limited Performance of MLGNR Interconnects

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Cited by 28 publications
(29 citation statements)
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“…where P represents the Padé order. The polynomial matrices P(ψl) and P(-ψl) are divided into four sub-block matrices in order to obtain the approximated cos hyperbolic and sin hyperbolic functions of ( 27) and are shown by ( 31) and (32).…”
Section: B Proposed Mra Model For Hybrid Cu-cnt Interconnectsmentioning
confidence: 99%
See 1 more Smart Citation
“…where P represents the Padé order. The polynomial matrices P(ψl) and P(-ψl) are divided into four sub-block matrices in order to obtain the approximated cos hyperbolic and sin hyperbolic functions of ( 27) and are shown by ( 31) and (32).…”
Section: B Proposed Mra Model For Hybrid Cu-cnt Interconnectsmentioning
confidence: 99%
“…The proposed model is implemented at larger interconnect lengths and is parameterized to incorporate the effects due to the surface roughness variations of the dielectric in which the hybrid Cu-CNT interconnect is placed. The dielectric surface roughness range is considered from 10-180 pm [32]. The entire 1-D grid for dielectric surface roughness variation is divided into 180 grid points.…”
Section: Table 5 Inphase Switching Delay (Ps) Comparison Between Cu-c...mentioning
confidence: 99%
“…The MFP associated with scattering due to crystal defects and static impurities, λ d , is assumed to be 1 μm. 29 Assuming Harrison type dependence for C-C hopping energy, the MFP due to surface roughness scattering, λ sr , can be written as λ sr ¼ c=δ 4 sr 29 in which c = 2.07 Â 10 9 is a fitting parameter and δ sr (in picometers) represents the root mean square of surface roughness amplitude. The underlying dielectric material is assumed to be boron nitride for carbon-based interconnects.…”
Section: Mlgnr Interconnectsmentioning
confidence: 99%
“…[ 25 ] This is due to the interaction and scattering of charge carriers with acoustic and optical phonons, resonant scatterers, rough edges, and dielectric‐induced sources like trapped charge impurities, polar phonons, and atomic roughness of corrugated dielectric surfaces. [ 25,28 ] Although dielectric‐induced scattering sources are considered dominant factors in reducing the MFP and conductivity of GNRs, [ 29,30 ] it has been shown that structural edge roughness (SER) can critically deteriorate the electronic properties and performance of GNRs as an on‐chip interconnect. [ 31 ] Several MFP and circuit models have been proposed considering all the scattering sources except SER.…”
Section: Introductionmentioning
confidence: 99%