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Updated: Apr 25, 2026

Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing
Published on: December 3, 2013
Dephasing time in graphene due to interaction with flexural phonons.
Konstantin S Tikhonov1, Wei L Z Zhao2, Alexander M Finkel'stein3
1Department of Physics and Astronomy, Texas A&M University, College Station, Texas 77843-4242, USA and Department of Condensed Matter Physics, The Weizmann Institute of Science, 76100 Rehovot, Israel and L. D. Landau Institute for Theoretical Physics, 117940 Moscow, Russia and Moscow Institute of Physics and Technology, 141700 Moscow, Russia.
Flexural phonons in graphene significantly impact electron decoherence, causing dephasing rates comparable to electron-electron interactions. This finding offers a new method to detect flexural phonons via electronic transport measurements.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Quantum Electronics
Background:
- Electron-electron interactions are a primary source of decoherence in graphene.
- The role of flexural phonons in electron decoherence is not fully understood.
- Standard theoretical approaches may not capture phonon-induced dephasing in certain regimes.
Purpose of the Study:
- To investigate the decoherence of electrons in graphene due to electron-flexural phonon interactions.
- To quantify the dephasing rate induced by flexural phonons across various temperatures and electron densities.
- To explore novel methods for identifying flexural phonons in graphene.
Main Methods:
- Theoretical investigation of electron-flexural phonon interaction in graphene.
- Calculation of the dephasing rate (τ_{ϕ}^{-1}) as a function of temperature (T) and electron density (n).
- Analysis of temperature dependence, including asymptotic regions and crossover behaviors.
- Evaluation of the dephasing rate's nonmonotonic dependence on electron density.
Main Results:
- Flexural phonons induce a dephasing rate comparable to electron-electron interactions.
- A significant temperature range exists where the golden rule fails to describe phonon-induced dephasing.
- The dephasing rate exhibits a crossover from T^{2} to T dependence with increasing temperature.
- The dephasing rate is a nonmonotonic function of electron density (n).
Conclusions:
- Electron-flexural phonon interaction is a significant contributor to decoherence in graphene.
- The unique temperature and density dependencies of this interaction provide a signature for identifying flexural phonons.
- Measuring weak-localization corrections in magnetoresistance can experimentally verify these findings and detect flexural phonons.
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