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Strictly speaking the various acoustic damping mechanisms and their frequency and size dependences should be included in Eq. 3. This is beyond the scope of the present work, and damping is introduced by the single phenomenological parameter τ.
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Strictly speaking the various acoustic damping mechanisms and their frequency and size dependences should be included in Eq. 3. This is beyond the scope of the present work, and damping is introduced by the single phenomenological parameter τ.
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Due to the high repetition rate of the pump laser the experiments are performed on a steady-state background of excited e-h pairs.
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Due to the high repetition rate of the pump laser the experiments are performed on a steady-state background of excited e-h pairs.
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After a convergence check N=201 has been used in the calculations.
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After a convergence check N=201 has been used in the calculations.
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