The Kiselev black hole is neither perfect fluid, nor is it quintessence
Matt Visser (Victoria University of Wellington)

TL;DR
This paper clarifies that the Kiselev black hole spacetime is neither a perfect fluid nor quintessence, correcting common misconceptions and highlighting the importance of accurate terminology and interpretation in the literature.
Contribution
It provides a detailed analysis showing the Kiselev spacetime's pressure anisotropy and clarifies its non-equivalence to perfect fluid or quintessence models.
Findings
Kiselev spacetime has non-zero pressure anisotropy unless w=-1
The average pressure equals w times the energy density
Misinterpretations in literature regarding perfect fluid and quintessence are corrected
Abstract
The Kiselev black hole spacetime, \[ ds^2 = - \left(1-{2m\over r} - {K\over r^{1+3w}} \right) dt^2 + {dr^2\over1-{2m\over r} - {K\over r^{1+3w}}} + r^2 \,d\Omega_2^2, \] is an extremely popular toy model, with over 200 direct and indirect citations as of 2019. Unfortunately, despite repeated assertions to the contrary, this is not a perfect fluid spacetime. The relative pressure anisotropy and average pressure are easily calculated to satisfy \[ \Delta = {\Delta p\over \bar p} = {p_r - p_t \over {1\over3} (p_r+2p_t)} =- {3(1+w)\over 2 w}; \qquad\qquad {\bar p\over \rho} = {{1\over3} (p_r + 2p_t)\over \rho} = w. \] The relative pressure anisotropy is generally a non-zero constant, (unless , corresponding to Schwarzschild-(anti)-de Sitter spacetime). Kiselev's original paper was very careful to point this out in the calculation, but then in the discussion made a somewhat…
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