Abstract
The ultrafast carrier dynamics in graphene has been intensively investigated in recent years. From the theoretical side the graphene Bloch equations have been successfully applied to explain linear absorption and various features observed in optical pump-probe experiments. Here, we present a detailed derivation of the graphene Bloch equations and discuss different contributions resulting from the electron-electron and electron-phonon interaction.
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Notes
- 1.
This work is part of the dissertation of Torben Winzer.
- 2.
In the following the optical matrix element will be denoted only with a single electron wave vector. Nevertheless, it still contains the Kronecker \(\delta _{\mathbf{k},\mathbf{k}^\prime}\).
- 3.
Due to the Kronecker \(\delta _{\mathbf{k}_{\mathbf{ 1}}+\mathbf{k}_{\mathbf{ 2}},\mathbf{k}_{\mathbf{ 3}}+\mathbf{k}_{\mathbf{ 4}}}\) in the Coulomb matrix element only the dynamics of momentum conserving correlations have to be determined. Nevertheless, for a more clear notation the equation of motion for a general \(\Lambda _{\mathbf{ 34}}^{\mathbf{ 12}c}\) is derived.
- 4.
In this derivation the spatial homogeneity applied form the beginning.
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Acknowledgements
We acknowledge the financial support from the Deutsche Forschungsgemeinschaft through SPP 1459. Ermin Malić thanks the Einstein Foundation Berlin. We thank Faris Kadi (TU Berlin) for fruitful discussions.
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Winzer, T., Malić, E., Knorr, A. (2013). Graphene Bloch Equations. In: Egger, R., Matrasulov, D., Rakhimov, K. (eds) Low-Dimensional Functional Materials. NATO Science for Peace and Security Series B: Physics and Biophysics. Springer, Dordrecht. https://doi.org/10.1007/978-94-007-6618-1_4
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