Bare open-string-metric areas do not reproduce the flavour entanglement entropy in the finite-density D3-D7 system, so this proposed shortcut is not a general entropy functional.
A First Law of Entanglement Rates from Holography
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abstract
For a perturbation of the state of a Conformal Field Theory (CFT), the response of the entanglement entropy is governed by the so-called "first law" of entanglement entropy, in which the change in entanglement entropy is proportional to the change in energy. Whether such a first law holds for other types of perturbations, such as a change to the CFT Lagrangian, remains an open question. We use holography to study the evolution in time $t$ of entanglement entropy for a CFT driven by a $t$-linear source for a conserved $U(1)$ current or marginal scalar operator. We find that although the usual first law of entanglement entropy may be violated, a first law for the rates of change of entanglement entropy and energy still holds. More generally, we prove that this first law for rates holds in holography for any asymptotically $(d+1)$-dimensional Anti-de Sitter metric perturbation whose $t$ dependence first appears at order $z^d$ in the Fefferman-Graham expansion about the boundary at $z=0$.
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Testing bare open-string-metric areas against flavour entanglement in finite-density D3-D7
Bare open-string-metric areas do not reproduce the flavour entanglement entropy in the finite-density D3-D7 system, so this proposed shortcut is not a general entropy functional.