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Smooth horizons from topology change in canonical quantum gravity

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Smooth Horizons from Topology Change in Canonical Quantum Gravity

The black hole information paradox signals a profound incompatibility between general relativity and quantum mechanics. Specifically, the "firewall paradox" suggests that if black hole evaporation is a unitary process—meaning information is preserved—an infalling observer must encounter a violent wall of high-energy radiation at the event horizon. This contradicts the smooth passage predicted by Einstein. Scientists have sought to reconcile this by proposing that the black hole interior is mathematically identified with the radiation emitted far outside. However, a rigorous gravitational mechanism explaining how the universe performs this identification has remained elusive.

The Conflict of Sequential Measurements

The core question investigated by Venkatesa Chandrasekaran in this paper is whether the firewall paradox can be resolved by treating the black hole interior as a dynamic entity capable of changing its topological connectivity (the way parts of a space are connected). The author asks: how can the laws of quantum gravity allow an infalling observer to perceive a smooth vacuum while ensuring that early Hawking radiation remains entangled with late radiation? This is not merely a question of whether information escapes. It is a question of how the gravitational Hilbert space—the mathematical arena of all possible quantum states—manages the conflicting requirements of locality and unitarity.

Cracks in the Semiclassical Picture

Until recently, the consensus relied on semiclassical approximations. These treat the gravitational background as a smooth, fixed stage. In this view, the interior and exterior of a black hole are distinct, independent subsystems. As illustrated in the conceptual setup of, an observer falling into an "old" black hole faces a logical deadlock.

Figure 1
Figure 1. Penrose diagram of the AMPS setup for a one sided black hole in JT gravity with a dynamical end of the world brane. The interval from T0 to T1 denotes the O(S0) evolution needed to reach the Page time.

An old black hole has passed its Page time, the point where it has radiated half its entropy.

According to the AMPS (Almheiri, Marolf, Polchinski, and Sully) protocol, the observer could perform two measurements. First, they could verify that the early radiation is "pure" (carrying the information). Second, they could verify that the horizon is a smooth vacuum. Quantum monogamy—the principle that a particle cannot be maximally entangled with two different things at once—suggests these two measurements cannot both succeed. If the radiation is entangled with the past, it cannot be entangled with the interior partner. This implies the entanglement at the horizon is broken, creating a high-energy "firewall."

Investigating Topology Change

The investigation proceeds by moving toward a "third quantized" description of gravity. In this framework, the number of black hole interiors can fluctuate. The author employs JT (Jackiw-Teitelboim) gravity, a simplified model of black hole horizons, to explore how the topology of the interior might evolve. The central mechanism is a "pair of pants" interaction. This is a cubic Hamiltonian term (an operator representing energy and dynamics) that allows a single interior sector to split into two connected interior branches .

Figure 3
Figure 3. Pair of pants topology changing vertex in the extended Hilbert space description of the black hole interior. The lower horizon slot ˆy is the parent interior leg and the upper slots ˆx1, ˆx2 are the two daughter interior legs.

To track this evolution while maintaining a view of the exterior, the researcher utilizes an "extended phase space." This involves mathematically "cutting" the spacetime slice at the event horizon. This cut introduces new degrees of freedom called "boost edge modes" at the corners .

Figure 2
Figure 2. The red curve is the infalling observer worldline γ, and the red endpoint is the event γT selected by the clock. The cyan curve is the full interval 3While there is a single observer throughout the AMPS experiment, the nature of the clock changes between the purity measurement phase and the horizon

These edge modes act as a gravitational "dressing." This means any matter particle becomes inextricably linked to the local geometry of the horizon. The author then simulates the AMPS experiment using three steps: 1. Relational Time Evolution: Using an infalling observer's own clock to define when measurements occur. 2. Topology Transition: Allowing the Hamiltonian to drive the system from a one-leg to a two-leg interior state .

Figure 4
Figure 4. One starts from the smooth interval ΣT , applies the cutting map Cε H , evolves the interior sector through the 1 →2 →1 topology changing process generated by a pair of pants interaction Hamiltonian ˆVpants, and obtains two candidate contraction channels before gluing.
  1. The Gluing Map: Reconstructing the smooth spacetime by "gluing" the interior and exterior back together.

The Emergence of the Exchange Channel

The findings suggest the firewall is not an inevitability. Instead, it is a consequence of choosing the wrong topological branch. The author reports that the topology-changing Hamiltonian drives the system toward a "connected branch" where the interior has effectively doubled. When analyzing how quantum information connects during the AMPS experiment, two distinct paths emerge .

The first is the "direct channel," which maintains the semiclassical assignment of particles. The author shows that this channel carries a non-zero "gluing phase"—a mathematical mismatch in the boost angles across the horizon. Consequently, when the interior is glued back to the exterior, this branch is annihilated by the gravitational constraints.

The second is the "exchange channel," where the particle indices are swapped. Crucially, the author demonstrates that this exchange channel is a "zero mode" of the boost generator. This means it is perfectly compatible with smooth gluing. The author uses a crossed product algebra (a mathematical structure where one algebra acts on another) to show that this channel is the smooth survivor.

The quantitative result is significant. By the Page time, the probability of the system transitioning into this connected, smooth branch approaches unity ($P_{conn} \approx 1 - O(e^{-cS_0})$). On this surviving branch, the horizon vacuum measurement and the early radiation purity measurement become the same Dirac observable. In essence, a large diffeomorphism (a smooth transformation of the spacetime coordinates) induced by the topology change identifies the interior Hawking partner with the decoded early radiation.

Implications for Gravitational Theory

This work shifts the resolution of the information paradox from kinematic properties to dynamical processes. The implications are threefold:

First, it provides a concrete Lorentzian mechanism for "island" formulas and entanglement wedge reconstruction. While previous work suggested these connections existed, this paper derives them from the fundamental requirement of relational time evolution and topology change.

Second, it offers a first-principles derivation of the "observer rule." It suggests that how an observer perceives the bulk depends on the finite resolution of their local clock. This bridges the gap between abstract holographic descriptions and the experience of a local probe.

Third, it demonstrates that the "smoothness" of a horizon is a protected feature of the gravitational constraints. The firewall is not a physical object that exists in the physical Hilbert space. Instead, it is a mathematical artifact of a branch that the theory's own constraints refuse to realize.

The next step for the field would be to extend this "pair of pants" interaction model to more realistic, higher-dimensional black hole geometries. Researchers must see if the suppression of the firewall branch holds outside the simplified JT gravity limit.

Figures from the paper

Figure 5
Figure 5. This reduces the growth of the connected branch to an ordinary rate equation, dPconn dT = Λ(T) 1 −Pconn(T)  , Λ(T) ∼|λ|2σ(T)kρeff, (1.8) where ρeff is the effective density of the boost generator, k = dim H ˜E is the effective number of unobserved environment degrees of freedom traced out in the
Figure 6
Figure 6. This leads us to our final result. Let U(T2, T1) denote the relational time evolution operator between the two clock readings T1 and T2 measured by the infalling observer, with the same 9 Vs(T1) Πbeb Trenv b ˜b1 eE |Φ⟩b˜b1 |χ0⟩e E eb |Φ⟩beb
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#quantum gravity#black hole information paradox#JT gravity#topology change#firewall paradox
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