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Minimal basis set used (SZ); I did a separate calculation for an isolated CNT (3,3) and obtained a band gap of 1.76 eV (SZ) and 1.49 eV (DZP). Armchair CNTs are metallic; to close the gap we need kpts in the z-direction.
The main peak in the X structure is located at ~5 V, which is close to the value from the inline structure (~5.5 V). This indicates that the qualitative features in the conductance derive from the CNT while the magnitude of the conductance is set by the contacts. The extra peaks seen on the right may be due to incomplete Notice the difference in the yaxis. The X structure (below) carries a current which is about one order of magnitude smaller than the CNT inline with the contacts (left)
Page 1 and 2: Ab-initio Assisted Process and Devi
Page 3 and 4: 1. Semiconductor Technology Scaling
Page 5 and 6: Role of Ab-Initio Methods on Nanosc
Page 7 and 8: Bridging the Length Scales: Ab-Init
Page 9 and 10: Buczko et al. Abrupt vs. Diffuse In
Page 11 and 12: intensity (a.u.) 70 60 50 40 30 20
Page 13 and 14: site and momentum resolved DOS Si-L
Page 15 and 16: 0.5 nm nm Si Combining Theory and E
Page 17 and 18: Band Line-Up Si/SiO 2 Real-space ba
Page 19 and 20: Intensity Z-Contrast Ge/SiO Interfa
Page 21 and 22: Monte Carlo Results - Animation •
Page 23 and 24: 0.5 nm Si Intensity Si/SiO vs. Ge/S
Page 25 and 26: Conclusions 2 • Atomic-scale char
Page 27 and 28: I p ( ) ( ) 2 V = ∫ T , ( ) ( ) =
Page 29 and 30: The Molecular Transport Problem I E
Page 31 and 32: Accelerated Molecular Dynamics •
Page 33 and 34: Carbon Nanotube on Pt • From work
Page 35 and 36: Carbon Nanotube on Ti •Large rela
Page 37 and 38: Contact Dependence of I-V Curve for
Page 39 and 40: Contact Dependence of I-V Curve for
Page 41 and 42: Funding • Semiconductor Research
Page 43: Right: • Ti below 10 a.u. and abo
Page 47 and 48: Current (A)
Page 49 and 50: Previous calculations and new ones.
Page 51 and 52: MD smoothes out most of the conduct
Page 53 and 54: MOSFET Scaling: Ultrashallow Juncti
Page 55 and 56: Ab-Initio Calculations - Standard C
Page 57 and 58: How To Find Migration Barriers I
Page 59 and 60: Calculation of Diffusion Prefactors
Page 61 and 62: T( o C) Reason for Deactivation - S
Page 63 and 64: Cluster Formation - Reaction Barrie
Page 65 and 66: Activation and Clusters 30 min anne
Page 67 and 68: *A. Asenov Statistical Effects in N
Page 69 and 70: Vacuum level E F Lead CNT VB CNT-FE
Page 71 and 72: The main peak in the X structure is
Page 73: PDOS for the relaxed CNT in line wi

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