<p>We study the interior of black holes in the presence of charged scalar hair of small amplitude <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40818_2024_192_Article_IEq1.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="TEX">\(\epsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ϵ</mi> </math></EquationSource> </InlineEquation> on the event horizon and show their terminal boundary is a crushing Kasner-like singularity. These spacetimes are spherically symmetric, spatially homogeneous and they differ significantly from the hairy black holes with uncharged matter previously studied in <i>[M. Van de Moortel, Violent nonlinear collapse inside charged hairy black holes, Arch. Rational. Mech. Anal., 248, 89, 2024]</i> in that the electric field is dynamical and subject to the backreaction of charged matter. We prove this charged backreaction causes drastically different dynamics compared to the uncharged case that ultimately impact the formation of the spacelike singularity, exhibiting novel phenomena such as<UnorderedList Mark="Bullet"> <ItemContent> <p><Emphasis Type="Underline">Collapsed oscillations</Emphasis>: oscillatory growth of the scalar hair, nonlinearly induced by the collapse</p> </ItemContent> <ItemContent> <p>A <Emphasis Type="Underline">fluctuating collapse</Emphasis>: The final Kasner exponents’ dependency in <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40818_2024_192_Article_IEq1.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="TEX">\(\epsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ϵ</mi> </math></EquationSource> </InlineEquation> is via an expression of the form</p> <p><InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40818_2024_192_Article_IEq3.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="211" /> </InlineMediaObject> <EquationSource Format="TEX">\(|\sin \left( \omega _0 \cdot \epsilon ^{-2}+ O(\log (\epsilon ^{-1}))\right) |\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">|</mo> <mo>sin</mo> </mrow> <mfenced close=")" open="("> <msub> <mi>ω</mi> <mn>0</mn> </msub> <mo>·</mo> <msup> <mi>ϵ</mi> <mrow> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mo>+</mo> <mi>O</mi> <mrow> <mo stretchy="false">(</mo> <mo>log</mo> <mrow> <mo stretchy="false">(</mo> <msup> <mi>ϵ</mi> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mfenced> <mrow> <mo stretchy="false">|</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>.</p> </ItemContent> <ItemContent> <p>A <Emphasis Type="Underline">Kasner bounce</Emphasis>: a transition from an unstable Kasner metric to a different stable Kasner metric</p> </ItemContent> </UnorderedList> The Kasner bounce occurring in our spacetime is reminiscent of the celebrated BKL scenario in cosmology.</p><p>We additionally propose a construction indicating the relevance of the above phenomena – including Kasner bounces – to spacelike singularities inside more general (asymptotically flat) black holes, beyond the hairy case.</p><p>While our result applies to all values of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40818_2024_192_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Lambda \in \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Λ</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation>, in the <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40818_2024_192_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Lambda &lt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Λ</mi> <mo>&lt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> case, our spacetime corresponds to the interior region of a charged asymptotically Anti-de-Sitter stationary black hole, also known as a <i>holographic superconductor</i> in high-energy physics, and whose exterior region was rigorously constructed in the recent mathematical work [W. Zheng, <i>Asymptotically Anti-de Sitter Spherically Symmetric Hairy Black Holes</i>, arXiv.2410.04758].</p>

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Kasner Bounces and Fluctuating Collapse Inside Hairy Black Holes with Charged Matter

  • Warren Li,
  • Maxime Van de Moortel

摘要

We study the interior of black holes in the presence of charged scalar hair of small amplitude \(\epsilon \) ϵ on the event horizon and show their terminal boundary is a crushing Kasner-like singularity. These spacetimes are spherically symmetric, spatially homogeneous and they differ significantly from the hairy black holes with uncharged matter previously studied in [M. Van de Moortel, Violent nonlinear collapse inside charged hairy black holes, Arch. Rational. Mech. Anal., 248, 89, 2024] in that the electric field is dynamical and subject to the backreaction of charged matter. We prove this charged backreaction causes drastically different dynamics compared to the uncharged case that ultimately impact the formation of the spacelike singularity, exhibiting novel phenomena such as

Collapsed oscillations: oscillatory growth of the scalar hair, nonlinearly induced by the collapse

A fluctuating collapse: The final Kasner exponents’ dependency in \(\epsilon \) ϵ is via an expression of the form

\(|\sin \left( \omega _0 \cdot \epsilon ^{-2}+ O(\log (\epsilon ^{-1}))\right) |\) | sin ω 0 · ϵ - 2 + O ( log ( ϵ - 1 ) ) | .

A Kasner bounce: a transition from an unstable Kasner metric to a different stable Kasner metric

The Kasner bounce occurring in our spacetime is reminiscent of the celebrated BKL scenario in cosmology.

We additionally propose a construction indicating the relevance of the above phenomena – including Kasner bounces – to spacelike singularities inside more general (asymptotically flat) black holes, beyond the hairy case.

While our result applies to all values of \(\Lambda \in \mathbb {R}\) Λ R , in the \(\Lambda <0\) Λ < 0 case, our spacetime corresponds to the interior region of a charged asymptotically Anti-de-Sitter stationary black hole, also known as a holographic superconductor in high-energy physics, and whose exterior region was rigorously constructed in the recent mathematical work [W. Zheng, Asymptotically Anti-de Sitter Spherically Symmetric Hairy Black Holes, arXiv.2410.04758].