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PHYS 620 Lecture 12: Excitons III
08 Apr 2013 | Online Presentations | Contributor(s): Roberto Merlin
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PHYS 620 Lecture 13: Metals
12 May 2013 | Online Presentations | Contributor(s): Roberto Merlin
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PHYS 620 Lecture 14 : Surface Plasmons
22 Apr 2013 | Online Presentations | Contributor(s): Roberto Merlin
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PHYS 620 Lecture 15: Plasmons in Nanoparticles
12 Apr 2013 | Online Presentations | Contributor(s): Roberto Merlin
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ECE 595E Lecture 13: Programming with FFTW
14 Feb 2013 | Online Presentations | Contributor(s): Peter Bermel
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ECE 595E Lecture 14: Beam Propagation Method I
14 Feb 2013 | Online Presentations | Contributor(s): Peter Bermel
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ECE 595E Lecture 15: Beam Propagation Method II
19 Feb 2013 | Online Presentations | Contributor(s): Peter Bermel
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nanoHUB-U TE L1.1: Lattice Structure - Introduction and Atomic Bonding
18 Mar 2013 | Online Presentations | Contributor(s): Timothy S Fisher
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nanoHUB-U TE L1.2: Lattice Structure - Mathematical Description of the Lattice
18 Mar 2013 | Online Presentations | Contributor(s): Timothy S Fisher
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nanoHUB-U TE L1.3: Lattice Structure - Lattice Vibrations and Phonons
18 Mar 2013 | Online Presentations | Contributor(s): Timothy S Fisher
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nanoHUB-U TE L1.4: Lattice Structure - Free Electrons
18 Mar 2013 | Online Presentations | Contributor(s): Timothy S Fisher
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nanoHUB-U TE L1.5: Lattice Structure - Example—1D Diatomic Chain
18 Mar 2013 | Online Presentations | Contributor(s): Timothy S Fisher
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nanoHUB-U TE L1.6: Lattice Structure - Week 1 Wrap Up
18 Mar 2013 | Online Presentations | Contributor(s): Timothy S Fisher
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ECE 695A Lecture 13: Introductory Lecture on HCI Degradation
19 Feb 2013 | Online Presentations | Contributor(s): Muhammad Alam
Outline:
Background and features of HCI Degradation
Phenomenological observations
Origin of Hot carriers
Theory of Si-H Bond Dissociation
Theory of Si-O Bond Dissociation
Conclusions
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ECE 695A Lecture 13R: Review Questions
19 Feb 2013 | Online Presentations | Contributor(s): Muhammad Alam
Review Questions:
Both SiH and SiO are involved in HCI degradation. Give two evidences.
Why doesn’t HCI occur during NBTI stress condition?
I suggested that HCI curve can shifted horizontally to form a universal curve, do you believe that I can do a corresponding vertical shift to form …
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ECE 695A Lecture 14a: Voltage Dependent HCI I
19 Feb 2013 | Online Presentations | Contributor(s): Muhammad Alam
Outline:
Background and Empirical Observations
Theory of Hot Carriers: Hydrodynamic Model
Theory of Hot Carriers: Monte Carlo Model
Theory of Hot Carriers: Universal Scaling
Conclusion
Appendices
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ECE 695A Lecture 14b: Voltage Dependent HCI II
19 Feb 2013 | Online Presentations | Contributor(s): Muhammad Alam
Outline:
Background and Empirical Observations
Theory of Hot Carriers: Hydrodynamic Model
Theory of Hot Carriers: Monte Carlo Model
Theory of Hot Carriers: Universal Scaling
Conclusion
Appendices
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ECE 695A Lecture 14R: Review Questions
19 Feb 2013 | Online Presentations | Contributor(s): Muhammad Alam
Review Questions
Why is Isub called a thermometer of hot electron distribution? Why can you not simply measure hot electrons by looking at the drain current?
What are the three methods of HCI voltage acceleration?
If theory of universal scaling is so good, why not use it all the time? (Hint: …
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ECE 595E Lecture 16: Applications of the Beam Propagation Method I
21 Feb 2013 | Online Presentations | Contributor(s): Peter Bermel
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Optical Absorption in B13 Cluster: A Time-dependent Density Functional Approach
19 Feb 2013 | Publications | Contributor(s): Ravindra L Shinde, Meenakshi Tayade
The linear optical absorption spectra of three isomers of planar boron cluster B13 are calculated using time dependent spin-polarized density functional approach. The geometries of these cluster are optimized at the B3LYP/6-311+G* level of theory. Even though the isomers are almost degenerate, the …