<p>Within AdS/CFT, focusing on the AdS-Rindler wedge, we show that when <i>N</i> is large but finite, correlation functions of reconstructed bulk operators grow exponentially with bulk momentum, overwhelming the usual 1<i>/N</i> suppression. The growth starts when the smeared operator’s ultraviolet scale goes beyond a critical value <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math display="inline"> <msub> <mi mathvariant="normal">Λ</mi> <mtext>crit</mtext> </msub> <mo>=</mo> <mfrac> <mn>2</mn> <mi>π</mi> </mfrac> <mo>ln</mo> <mi>N</mi> </math></EquationSource> <EquationSource Format="TEX">\( {\Lambda}_{\mathrm{crit}}=\frac{2}{\pi}\ln N \)</EquationSource> </InlineEquation>, which is far below the Planck scale. Above this logarithmic threshold, the large <i>N</i> expansion ceases to be reliable, and the would-be bulk operators cannot be consistently defined as observables in the full quantum gravity theory. Since the AdS-Rindler wedge describes the near-horizon region of black holes, this result implies a sharp ln <i>N</i> cutoff for reconstructing bulk operators across horizons. This has a direct impact on whether and how information from the black hole interior is encoded — a central question in the black hole information paradox.</p>

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Holography at finite N: breakdown of bulk reconstruction for subregions

  • Seiji Terashima

摘要

Within AdS/CFT, focusing on the AdS-Rindler wedge, we show that when N is large but finite, correlation functions of reconstructed bulk operators grow exponentially with bulk momentum, overwhelming the usual 1/N suppression. The growth starts when the smeared operator’s ultraviolet scale goes beyond a critical value Λ crit = 2 π ln N \( {\Lambda}_{\mathrm{crit}}=\frac{2}{\pi}\ln N \) , which is far below the Planck scale. Above this logarithmic threshold, the large N expansion ceases to be reliable, and the would-be bulk operators cannot be consistently defined as observables in the full quantum gravity theory. Since the AdS-Rindler wedge describes the near-horizon region of black holes, this result implies a sharp ln N cutoff for reconstructing bulk operators across horizons. This has a direct impact on whether and how information from the black hole interior is encoded — a central question in the black hole information paradox.