MEASUREMENTS OF HOT-ELECTRON MAGNETOPHONON RESONANCE IN GAAS/GAALAS HETEROSTRUCTURES by Leadley, D, Brummell, M, Nicholas, R, Harris, J, Foxon, C

Detection of terahertz radiation by hot electron effects in coupled quantum well photodiodes by Stone, R, Michels, J, Wong, S, Foxon, C, Nicholas, R, Fox, A

Detection of intersubband transitions in gallium arsenide coupled quantum wells by hot electron effects by Tomlinson, A, Chang, C, Stone, R, Foxon, C, Nicholas, R, Fox, A

A STUDY OF THE ENERGY-LOSS MECHANISMS FOR HOT-ELECTRONS IN CDTE AND CDS FROM OSCILLATORY PHOTOCONDUCTIVITY AND THE MAGNETOPHONON EFFECT by Nicholas, R, Carter, A, Fung, S, Stradling, R, Portal, J, Houlbert, C

Weak localization scattering lengths in epitaxial, and CVD graphene by Baker, A, Alexander-Webber, J, Altebaeumer, T, Janssen, T, Tzalenchuk, A, Lara-Avila, S, Kubatkin, S, Yakimova, R, Lin, C, Li, L, Nicholas, R

“…We demonstrate that currents as low as 0.01 nA are required in smaller devices to avoid hot-electron artifacts in measurements of the quantum corrections to conductivity. © 2012 American Physical Society.…”

Magnetotransport in graphene and related two-dimensional systems by Huang, N

“…In Chapter 6, energy relaxation of hot carriers in graphene bilayer systems is investigated from measurements on Shubnikovde Haas oscillations and weak localisation. The hot-electron energy loss rate follows the predicted <em>T</em>⁴ power-law at carrier temperatures from 1.4 up to about 100 K, due to electron-acoustic phonon interactions. …”

Electron-phonon interactions in low dimensional structures by Leadley, D, David Romwald Leadley

“…At higher electric fields the 'normal' MPR maxima invert, starting at low magnetic fields, to form 'hot electron' MPR minima, with maximum amplitude at ~60K. …”