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Volumn 90, Issue 8, 2014, Pages

Simple holographic insulator

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[No Author keywords available]

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EID: 84908258406     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.90.084042     Document Type: Article
Times cited : (54)

References (35)
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    • With an equal number of positive and negative charge carriers, the charge current and momentum decouple since an applied electric field induces a current, but the net momentum stays zero.
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    • For stability of the gravity solution, we also require that (Equation presented) can be derived from a certain superpotential, as we will discuss shortly.
    • For stability of the gravity solution, we also require that (Equation presented) can be derived from a certain superpotential, as we will discuss shortly.
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    • From here on, we set (Equation presented).
    • From here on, we set (Equation presented).
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    • Even though this term diverges at the horizon, at nonzero temperature (Equation presented) vanishes linearly, so the horizon is a regular singular point of (21). This is no longer true when (Equation presented).
    • Even though this term diverges at the horizon, at nonzero temperature (Equation presented) vanishes linearly, so the horizon is a regular singular point of (21). This is no longer true when (Equation presented).
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    • This is of course only valid at nonzero (Equation presented) where we have harmonic time dependence. We compute the low frequency conductivity and then take (Equation presented).
    • This is of course only valid at nonzero (Equation presented) where we have harmonic time dependence. We compute the low frequency conductivity and then take (Equation presented).
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    • This effect is unique to two (spatial) dimensions where phase coherence falloffs are algebraic, (Equation presented) with (Equation presented) [33].
    • This effect is unique to two (spatial) dimensions where phase coherence falloffs are algebraic, (Equation presented) with (Equation presented) [33].


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