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Additional info for Nonequilibrium carrier dynamics in semiconductors : proceedings of the 14th international conference, July 25-29, 2005, Chicago, USA
Phys. Lett. 75, 3593 (1999) 5. T. F. , Appl. Phys. Lett. 78, 276 (2001) 6. T. S. , Phys. Rev. B 57, R9423 (1998) 7. , Appl. Phys. Lett. 83, 3572 (2003) 8. U. Bockelmann, and G. Bastard, Phys. Rev. B 42, 8947 (1990) 9. H. , Phys. Rev. B 44, 10945 (1991) 10. T. R. , Phys. Rev. B 69, 235314 Influence of Surfaces on the Pure Dephasing of Quantum Dots T. Kuhn, B. Krummheuer and V. M. Axt Institut ftir Festkorpertheorie, Westfalische Wilhelms-Universitat Munster, Wilhelm-Klemm-Str. 10, 48149 Munster, Germany Summary.
4. (a) Spectrally resolved FWM signal in the direction 2ki-k2 without the second phase-locked pulse, (b) Both phase-locked pulses were used. Spectra of the FWM signal at different delay times A/,>,, are shown. direction ki shows the modes hhi to hh4. In Fig. 4b the two-pulse FWM spectra for different delay times Ati^^t exhibit a change in the signal intensity of the polariton modes with changing delay time. The maximum intensities of the modes occurs at different delay times, respectively. This variation of the signal intensity is again due to constructive and destructive interference of the respective polarizations.
To conclude, we have presented a guideline to observe super-Poissonian noise in tunneling through two vertically coupled QDs. e. the tunneling of electrons through the resonance of single-particle states and the two-particle states at the same bias voltage. Acknowledgments: We acknowledge helpful discussions with F. Hohls regarding the experiment. This work was supported by Deutsche Forschungsgemeinschaft in the framework of Sfb 296. 1. Blanter, Y. M. , Phys. , 336, 7, 2000. 2. , and Haug, R. ,phys.