hw3
Differences
This shows you the differences between two versions of the page.
| Both sides previous revisionPrevious revisionNext revision | Previous revision | ||
| hw3 [2016/04/16 10:24] – [Journal reading (5 pts)] janet | hw3 [2020/03/06 09:14] (current) – external edit 127.0.0.1 | ||
|---|---|---|---|
| Line 21: | Line 21: | ||
| $$R = {h \over {2{e^2}}}{L \over {{\ell _{ph}}}}$$ | $$R = {h \over {2{e^2}}}{L \over {{\ell _{ph}}}}$$ | ||
| - | **c)** Show that the the above result is equivalent to the Drude formula, within a factor of 2, if we assume a free electron dispersion relation $E = {{{\hbar ^2}{k^2}} \over {2m}}$. | + | **c)** Show that the above result is equivalent to the Drude formula, within a factor of 2, if we assume a free electron dispersion relation $E = {{{\hbar ^2}{k^2}} \over {2m}}$. |
| $${\rho _{1d}} = {m \over {{n_{1d}}{e^2}{\tau _{e - ph}}}}$$ | $${\rho _{1d}} = {m \over {{n_{1d}}{e^2}{\tau _{e - ph}}}}$$ | ||
| Line 54: | Line 54: | ||
| Articles | Articles | ||
| - | Monte-Carlo simulation of nano-collected current from a silicon sample containing a linear arrangement of uncapped nanocrystals , Mohammed Ledra and Abdelillah El Hdiy J. Appl. Phys. 118, 115705 (2015); | + | * Monte-Carlo simulation of nano-collected current from a silicon sample containing a linear arrangement of uncapped nanocrystals , Mohammed Ledra and Abdelillah El Hdiy J. Appl. Phys. 118, 115705 (2015); |
| - | Picosecond photoresponse in van der Waals heterostructures, | + | |
| - | Determination of band alignment in the single-layer MoS2/WSe2 heterojunction, | + | |
| - | Electron-Phonon Coupling and Energy Flow in a Simple Metal beyond the Two-Temperature Approximation, | + | |
| - | The Valley Hall effect in MoS2 transistors. K. F. Mak et al Science 344, pp. 1489-1492 (2014) DOI: 10.1126/ | + | |
hw3.1460827464.txt.gz · Last modified: 2020/03/06 09:14 (external edit)