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The effective mass of the GaAs barrier is slightly reduced, due to the seed layer below the QDs in sample E1. A simple estimation of the fraction of InAs in the GaAs barrier leads to a reduction of the effective mass to approximately me* ≈0.058, an uncertainty of about 9%. However, the total accuracy of the tunneling barrier height-including the linearization uncertainty-is only 5%, due to the error propagation theorem.
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The effective mass of the GaAs barrier is slightly reduced, due to the seed layer below the QDs in sample E1. A simple estimation of the fraction of InAs in the GaAs barrier leads to a reduction of the effective mass to approximately me* ≈0.058, an uncertainty of about 9%. However, the total accuracy of the tunneling barrier height-including the linearization uncertainty-is only 5%, due to the error propagation theorem.
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If we assume a very poor accuracy of the Poole-Frenkel energy of about 50%, due to the limited knowledge of the QD height, the total accuracy of the localization energy is better than 8%.
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If we assume a very poor accuracy of the Poole-Frenkel energy of about 50%, due to the limited knowledge of the QD height, the total accuracy of the localization energy is better than 8%.
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