A Search for Evidence of the Radioactive Decomposition of by Rachel Ruth Comroe

By Rachel Ruth Comroe

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34 34 34 36 37 38 39 41 41 April 9, 2008 16:17 34 World Scientific Review Volume - 9in x 6in semiconductor G. J. Beirne, M. Jetter, and P. 4 Asymmetric InP/GaInP Vertical Quantum Dot Pairs . . 1 Sample growth and post-growth structuring . . 3 Time-resolved photoluminescence measurements . 5 Conclusions . . . . . . . . . . . . . References . . . . . . . . . . . . . . . . . . . . . . thicknesses . . . . . . . .

79 nm. 4aB . 85aB . The gate is positioned 14aB above the two-dimensional electron gas and a voltage of −|e|V = 10R is applied to it to create the symmetric triangular triple quantum dot. 0636R. With the single-particle orbitals and their energies obtained in the RSP calculation, in the next step we consider a system of three confined electrons. To this end we use April 9, 2008 16:17 26 World Scientific Review Volume - 9in x 6in M. Korkusinski and P. Hawrylak the configuration interaction approach (CI), in which we create all possible configurations of our electrons on nine lowest molecular orbitals.

Units) April 9, 2008 semiconductor G. J. Beirne, M. Jetter, and P. 90 Energy (eV) Fig. 5. 5 nm spacer with significant inter-dot electron and hole tunneling. This parasitic coupling (from the viewpoint of the SD) is only clearly apparent when emission from the SD emerges at high power densities as a direct result of state filling in the LD. For a 10 nm spacer layer [Fig. 5(b)], however, the situation changes considerably and the LD emission is now fifteen times more intense than that of SD at the lowest investigated power.

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