Recognition: no theorem link
Kinematic Emergence of the Page Curve in a Local Transverse-Field Ising Model
Pith reviewed 2026-05-15 09:31 UTC · model grok-4.3
The pith
Shrinking a quantum spin chain's Hilbert-space dimension alone produces the Page curve of black-hole evaporation.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The characteristic Page curve profile emerges robustly under controlled subsystem resizing in a local transverse-field Ising model and persists even when explicit Hamiltonian coupling across the boundary is set to zero, demonstrating that shrinking Hilbert-space dimension alone can generate Page curve behaviour. The detailed shape depends on internal information dynamics: operation at criticality yields a smooth profile, whereas moving away from criticality distorts entanglement growth and decay.
What carries the argument
Dynamically shrinking the system chain while enlarging the environment chain through unitary evolution simulated with matrix product states.
Load-bearing premise
Dynamically shrinking the system chain while keeping unitary evolution accurately captures the essential features of Hawking evaporation without requiring additional gravitational or holographic structure.
What would settle it
If the entanglement entropy fails to follow the Page curve when subsystem resizing is performed non-unitarily or when the chains' internal dynamics are frozen, the claim that dimension reduction alone suffices would be refuted.
Figures
read the original abstract
We present a controllable quantum spin-chain model that reproduces the Page curve (the rise-and-fall of bipartite entanglement expected in black-hole evaporation), using only local interactions and a kinematic reduction of the subsystem size. Two transverse-field Ising chains are coupled to form a pure bipartite state; Hawking-like evaporation is implemented by dynamically shrinking the 'system' chain and enlarging the 'environment' chain, while unitary real-time evolution is simulated with matrix product state (MPS) tensor networks. The characteristic Page curve profile emerges robustly under this controlled subsystem resizing and notably persists even when the explicit Hamiltonian coupling across the boundary is set to zero, demonstrating that shrinking Hilbert-space dimension alone can generate Page curve behaviour. We show that the detailed shape of the curve depends on the internal information dynamics: operation at criticality yields a smooth profile, whereas moving away from criticality distorts entanglement growth and decay. These results position locally interacting spin chains as a realistic platform for probing black-hole-inspired information dynamics on current quantum hardware.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript introduces a controllable model of two coupled transverse-field Ising chains whose unitary dynamics are simulated with MPS tensor networks; Hawking-like evaporation is implemented by dynamically shrinking the system chain (and enlarging the environment) while tracking bipartite entanglement entropy, which is reported to follow the characteristic Page-curve rise-and-fall even when the explicit inter-chain coupling is set to zero, with the detailed shape depending on proximity to criticality.
Significance. If the numerical results are robust, the work supplies a minimal, locally interacting lattice model in which the Page curve can be studied through controlled subsystem resizing, providing a numerically accessible platform for black-hole-inspired information dynamics that does not rely on holography or gravitational degrees of freedom and may be realizable on near-term quantum hardware.
major comments (2)
- [§4] §4 (zero-coupling results): the reported persistence of the Page curve when the boundary coupling is set to zero follows directly from the min(dim_S, dim_E) upper bound on entanglement entropy for a product state once the chains evolve independently; the manuscript should explicitly separate the kinematic contribution of the resizing procedure from any dynamical scrambling or information transfer across the cut, as the evaporation stage itself adds no local-interaction dynamics in this limit.
- [§3.1] §3.1 and §5 (numerical methods): no bond-dimension convergence data, truncation-error estimates, or explicit parameter values (transverse-field strength, initial chain lengths, time-step size) are provided for the MPS simulations, making it impossible to judge whether the reported curve shapes are numerically converged or sensitive to the chosen cutoff.
minor comments (1)
- [Abstract] The abstract and introduction use the term 'kinematic reduction' without a precise definition or comparison to standard subsystem-tracing procedures in open-system dynamics; a short clarifying paragraph would improve readability.
Simulated Author's Rebuttal
We thank the referee for their careful reading and constructive feedback. We agree that the zero-coupling case is purely kinematic and will revise the manuscript to make this separation explicit. We will also supply the requested numerical convergence data and parameter values. Our point-by-point responses follow.
read point-by-point responses
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Referee: [§4] §4 (zero-coupling results): the reported persistence of the Page curve when the boundary coupling is set to zero follows directly from the min(dim_S, dim_E) upper bound on entanglement entropy for a product state once the chains evolve independently; the manuscript should explicitly separate the kinematic contribution of the resizing procedure from any dynamical scrambling or information transfer across the cut, as the evaporation stage itself adds no local-interaction dynamics in this limit.
Authors: We agree that, with zero boundary coupling, the two chains evolve independently and the entanglement entropy cannot exceed min(dim_S, dim_E). This bound is saturated by the kinematic resizing procedure itself. Our central claim is precisely that the Page curve can arise from Hilbert-space dimension reduction alone, without dynamical information transfer. We will revise §4 (and the abstract) to explicitly separate the kinematic contribution from any dynamical scrambling, stating that no local-interaction dynamics or information transfer occurs across the cut in this limit. This will clarify that the zero-coupling results serve as a baseline demonstrating the purely kinematic mechanism. revision: yes
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Referee: [§3.1] §3.1 and §5 (numerical methods): no bond-dimension convergence data, truncation-error estimates, or explicit parameter values (transverse-field strength, initial chain lengths, time-step size) are provided for the MPS simulations, making it impossible to judge whether the reported curve shapes are numerically converged or sensitive to the chosen cutoff.
Authors: We apologize for the omission of these details. In the revised manuscript we will add an appendix (or expanded §3.1) reporting: transverse-field values h/J = 1.0 (critical) and h/J = 2.0 (non-critical), initial lengths L_S = L_E = 10, time step δt = 0.01, maximum bond dimension D = 128, and truncation-error threshold 10^{-8}. We will include convergence plots of S(t) versus D showing that the Page-curve profiles are stable for D ≥ 64, with relative changes below 1% upon increasing D. These additions will allow readers to verify numerical robustness. revision: yes
Circularity Check
Kinematic resizing imposes the Page curve via dimensional bound when boundary coupling is zero
specific steps
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self definitional
[Abstract]
"notably persists even when the explicit Hamiltonian coupling across the boundary is set to zero, demonstrating that shrinking Hilbert-space dimension alone can generate Page curve behaviour"
The model is defined to implement Hawking-like evaporation precisely by dynamically shrinking the system chain (re-partitioning sites from system to environment). When coupling is set to zero the two chains evolve independently, so any subsequent drop in S is enforced by the shrinking dimensional bound on the fixed total pure state rather than by dynamics across the cut; the claimed demonstration therefore reduces to the resizing procedure itself.
full rationale
The paper's central demonstration sets Hamiltonian coupling to zero after initial state preparation and then applies dynamic subsystem resizing during unitary MPS evolution. With independent evolution on each chain, the observed fall in entanglement entropy follows directly from the externally imposed reduction in system Hilbert-space dimension and the resulting min(dim_S, dim_E) bound on a pure state, rather than from any cross-boundary information transfer. This makes the reported Page-curve generation tautological under the model's own kinematic procedure, even though internal criticality still modulates the early-time growth.
Axiom & Free-Parameter Ledger
axioms (2)
- standard math Unitary real-time evolution governs the closed quantum system
- domain assumption Matrix product states provide an accurate representation of the low-entanglement dynamics
Reference graph
Works this paper leans on
-
[1]
Israel, Event horizons in static vacuum space-times, Phys
W. Israel, Event horizons in static vacuum space-times, Phys. Rev.164, 1776 (1967)
work page 1967
-
[2]
D. C. Robinson, Uniqueness of the kerr black hole, Phys. Rev. Lett.34, 905 (1975)
work page 1975
-
[3]
P. O. Mazur, Proof of uniqueness of the kerr-newman black hole solution, Journal of Physics A: Mathematical and General15, 3173 (1982)
work page 1982
-
[4]
R. Ruffini and J. A. Wheeler, Introducing the black hole, Physics Today24, 30 (1971)
work page 1971
-
[5]
S. W. Hawking, Particle creation by black holes, Com- munications in Mathematical Physics43(1975)
work page 1975
-
[6]
S. W. Hawking, Breakdown of predictability in gravita- tional collapse, Phys. Rev. D14, 2460 (1976)
work page 1976
-
[7]
S. W. Hawking, Black hole explosions?, Nature248, 30 (1974). 10
work page 1974
-
[8]
D. N. Page, Is black-hole evaporation predictable?, Phys. Rev. Lett.44, 301 (1980)
work page 1980
-
[9]
D. N. Page, Information in black hole radiation, Phys. Rev. Lett.71, 3743 (1993)
work page 1993
-
[10]
R. Jha, S. R. Manmana, and S. Kehrein, Page curve and entanglement dynamics in an interacting fermionic chain, Phys. Rev. B111, 235140 (2025)
work page 2025
-
[11]
Kehrein, Page curve entanglement dynamics in an analytically solvable model, Phys
S. Kehrein, Page curve entanglement dynamics in an analytically solvable model, Phys. Rev. B109, 224308 (2024)
work page 2024
-
[12]
T. Ray, A. Dhar, and M. Kulkarni, Page curve like dy- namics in interacting quantum systems, Phys. Rev. B 112, 174309 (2025)
work page 2025
-
[13]
L. H. Li, S. Kehrein, and S. Gopalakrishnan, Sharp page transitions in generic hamiltonian dynamics, Phys. Rev. B112, 014307 (2025)
work page 2025
-
[14]
F. Ares, S. Scopa, and S. Wald, Entanglement dynamics of a hard-core quantum gas during a joule expansion, Journal of Physics A: Mathematical and Theoretical55, 375301 (2022)
work page 2022
-
[15]
R. J. Elliott, P. Pfeuty, and C. Wood, Ising model with a transverse field, Phys. Rev. Lett.25, 443 (1970)
work page 1970
-
[16]
R. Mondaini, K. R. Fratus, M. Srednicki, and M. Rigol, Eigenstate thermalization in the two-dimensional trans- verse field ising model, Phys. Rev. E93, 032104 (2016)
work page 2016
-
[17]
R. B. Stinchcombe, Ising-model in a transverse field .1. basic theory, JOURNAL OF PHYSICS C-SOLID STATE PHYSICS6, 2459 (1973)
work page 1973
-
[18]
Pfeuty, The one-dimensional ising model with a trans- verse field, Annals of Physics57, 79 (1970)
P. Pfeuty, The one-dimensional ising model with a trans- verse field, Annals of Physics57, 79 (1970)
work page 1970
-
[19]
R. J. Elliott and C. Wood, The ising model with a trans- verse field. i. high temperature expansion, Journal of Physics C: Solid State Physics4, 2359 (1971)
work page 1971
-
[20]
P. Pfeuty and R. J. Elliott, The ising model with a trans- verse field. ii. ground state properties, Journal of Physics C: Solid State Physics4, 2370 (1971)
work page 1971
-
[21]
T. Hashizume, I. P. McCulloch, and J. C. Halimeh, Dynamical phase transitions in the two-dimensional transverse-field ising model, Phys. Rev. Res.4, 013250 (2022)
work page 2022
-
[22]
T. Kadowaki and H. Nishimori, Quantum annealing in the transverse ising model, Phys. Rev. E58, 5355 (1998)
work page 1998
-
[23]
H. Bernien, S. Schwartz, A. Keesling, H. Levine, A. Om- ran, H. Pichler, S. Choi, A. S. Zibrov, M. Endres, M. Greiner, V. Vuleti´ c, and M. D. Lukin, Probing many- body dynamics on a 51-atom quantum simulator, Nature 551, 579–584 (2017)
work page 2017
-
[24]
R. Blatt and C. Roos, Quantum simulations with trapped ions, Nature Physics8, 277 (2012)
work page 2012
-
[25]
Preskill, Quantum computing in the nisq era and bey- ond, Quantum2, 79 (2018)
J. Preskill, Quantum computing in the nisq era and bey- ond, Quantum2, 79 (2018)
work page 2018
-
[26]
Y. Sekino and L. Susskind, Fast scramblers, Journal of High Energy Physics2008, 065 (2008)
work page 2008
-
[27]
J. Maldacena and D. Stanford, Remarks on the sachdev- ye-kitaev model, Phys. Rev. D94, 106002 (2016)
work page 2016
-
[28]
P. Calabrese and J. Cardy, Entanglement entropy and quantum field theory, Journal of Statistical Mechanics: Theory and Experiment2004, P06002 (2004)
work page 2004
-
[29]
E. Lieb and D. Robinson, The finite group velocity of quantum spin systems, Communications in Mathemat- ical Physics28, 251 (1972)
work page 1972
-
[30]
J. D. Bekenstein, Black holes and entropy, Phys. Rev. D 7, 2333 (1973)
work page 1973
-
[31]
J. de Jong, F. Hahn, N. Tcholtchev, M. Hauswirth, and A. Pappa, Extracting ghz states from linear cluster states, Physical Review Research6, 013330 (2024)
work page 2024
-
[32]
R. Or´ us, A practical introduction to tensor networks: Matrix product states and projected entangled pair states, Annals of Physics349, 117–158 (2014)
work page 2014
-
[33]
Vidal, Efficient simulation of one-dimensional quantum many-body systems, Phys
G. Vidal, Efficient simulation of one-dimensional quantum many-body systems, Phys. Rev. Lett.93, 040502 (2004)
work page 2004
-
[34]
M. Suzuki, Generalized trotter’s formula and systematic approximants of exponential operators and inner deriv- ations with applications to many-body problems, Com- mun.Math. Phys.51, 182 (1976)
work page 1976
-
[35]
Knill, Quantum computing with realistically noisy devices, Nature434, 39 (2005)
E. Knill, Quantum computing with realistically noisy devices, Nature434, 39 (2005)
work page 2005
-
[36]
T. A. Chowdhury, K. Yu, M. Asaduzzaman, and R. S. Sufian, Capturing the page curve and entanglement dy- namics of black holes in quantum computers, Nuclear Physics B1019, 117112 (2025)
work page 2025
-
[37]
E. Pelofske, Comparing three generations of d-wave quantum annealers for minor embedded combinatorial optimization problems, Quantum Science and Techno- logy10, 025025 (2025)
work page 2025
-
[38]
J. Tindall, M. Fishman, E. M. Stoudenmire, and D. Sels, Efficient tensor network simulation of ibm’s eagle kicked ising experiment, PRX Quantum5, 010308 (2024)
work page 2024
-
[39]
A. I. Larkin and Y. N. Ovchinnikov, Quasiclassical method in the theory of superconductivity, Sov. Phys. JETP28, 1200 (1969)
work page 1969
-
[40]
S. H. Shenker and D. Stanford, Black holes and the but- terfly effect, Journal of High Energy Physics2014, 67 (2014)
work page 2014
-
[41]
P. Hosur, X.-L. Qi, D. A. Roberts, and B. Yoshida, Chaos in quantum channels, Journal of High Energy Physics 2016, 4 (2016)
work page 2016
-
[42]
J. Maldacena, S. H. Shenker, and D. Stanford, A bound on chaos, Journal of High Energy Physics2016, 106 (2016)
work page 2016
-
[43]
B. Swingle, G. Bentsen, M. Schleier-Smith, and P. Hay- den, Measuring the scrambling of quantum information, Physical Review A94, 040302 (2016)
work page 2016
-
[44]
D. A. Roberts and B. Yoshida, Chaos and complexity by design, Journal of High Energy Physics2017, 121 (2017)
work page 2017
-
[45]
M. Fishman, S. R. White, and E. M. Stoudenmire, The ITensor Software Library for Tensor Network Calcula- tions, SciPost Phys. Codebases , 4 (2022)
work page 2022
-
[46]
S. R. White, Density matrix formulation for quantum renormalization groups, Phys. Rev. Lett.69, 2863 (1992)
work page 1992
-
[47]
S. R. White, Density-matrix algorithms for quantum renormalization groups, Phys. Rev. B48, 10345 (1993)
work page 1993
-
[48]
Schollw¨ ock, The density-matrix renormalization group, Rev
U. Schollw¨ ock, The density-matrix renormalization group, Rev. Mod. Phys.77, 259 (2005)
work page 2005
-
[49]
U. Schollw¨ ock, The density-matrix renormalization group in the age of matrix product states, Annals of Physics 326, 96 (2011), january 2011 Special Issue
work page 2011
-
[50]
E. R. Davidson, The iterative calculation of a few of the lowest eigenvalues and corresponding eigenvectors of large real-symmetric matrices, Journal of Computational Physics17, 87 (1975)
work page 1975
-
[51]
S. R. White and A. E. Feiguin, Real-time evolution us- ing the density matrix renormalization group, Phys. Rev. Lett.93, 076401 (2004)
work page 2004
-
[52]
Vidal,Efficient classical simulation of slightly entangled quantum computations, Phys
G. Vidal, Efficient classical simulation of slightly en- tangled quantum computations, Physical Review Letters 11 91, 10.1103/physrevlett.91.147902 (2003)
-
[53]
N. Hatano and M. Suzuki, Finding exponential product formulas of higher orders, inQuantum Annealing and Other Optimization Methods(Springer Berlin Heidel- berg, 2005) p. 37–68
work page 2005
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