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A simple way to modify Eq. 18 is to add a k-independent decay channel: ρ k=-(Dk2+γα)ρk+ξk(t). This would lead to a Debye frequency dependence of the isothermal bulk modulus.
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Below the solidity length Eq. 18 and our derivation of the diffusion constant decoupling should still apply (although the k→0 limit of Sec. 6 would now be limited to lengths below the solidity length).
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Below the solidity length Eq. 18 and our derivation of the diffusion constant decoupling should still apply (although the k→0 limit of Sec. 6 would now be limited to lengths below the solidity length).
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