USR-2026-0058 · Information
The thermofield double behaves exactly as ER=EPR describes a two-sided black hole: one side alone is perfectly thermal (trace distance 2.7×10⁻¹⁵ from the Gibbs state), the two-sided correlations equal the imaginary-time bridge correlator to 3.3×10⁻¹⁶, entanglement falls monotonically with β (hotter = more bridge), and the cross-side commutator is exactly zero.
PROVISIONAL
one side exactly thermal (2.7e-15); bridge identity to 3.3e-16; commutator exactly 0
reproduced ≠ discovered
re-run & confirmed 2026-07-26 (R0 — founder CI; independence pending)
Maldacena 2003 TFD structure at toy scale. No gravity is computed and none is claimed: this is the state structure — each side featureless heat, the pair one pure state, correlation without causation.
Falsify-box — how to kill this claim
SURVIVED
the reduced state deviates from thermal beyond roundoff, the bridge identity fails, or the commutator is nonzero
Verification record — every quoted number, re-run 2026-07-26
| quantity | measured | verdict |
|---|---|---|
| thermality trace distance | 2.688e-15 | MATCH |
| bridge-identity discrepancy | 3.331e-16 | MATCH |
| cross-side commutator | 0.0 exactly, by two methods | MATCH |
Provenance
script: information_seam/thermofield_double.py
script status: PRESENT
datasets: information-seam-scripts (downloadable from /data — run it yourself)
re-run: 2026-07-26
script status: PRESENT
datasets: information-seam-scripts (downloadable from /data — run it yourself)
re-run: 2026-07-26
Status, honestly
verified by adversarial re-run (workflow, 2026-07-26); admitted from MCP intake INTAKE-655992b339. Status here is computed from evidence — the author cannot set it, and neither can we. Independent reproduction would move it; nothing else will.
§ Reproduction
thermofield_double.py
The founder's own run of this script, captured verbatim. A match proves the result is reproducible; it is still R0 on this registry's independence rings — same code, so it cannot move a status. Only an outside run does that.
A · Recorded
founder's machine · 2026-08-02
========================================================================
TEST 9: THERMOFIELD DOUBLE -- the wormhole-like state in hand
(REPRODUCED, NOT DISCOVERED: Maldacena 2003 TFD; ER=EPR state
structure at toy scale. Machinery check only -- no gravity
computed, none claimed.)
========================================================================
Model: TFIM H = -sum sz.sz - h sum sx, N=8, open chain, h=1.05
Hilbert space: 256 states per side; TFD lives in 256x256 = 65536 dims
scipy available: True
Hamiltonian symmetry check |H - H^T|_max: 0.000e+00
Ground energy E0: -10.142410910259
Gap E1 - E0: 0.443817514654
------------------------------------------------------------------------
TFD per beta: |TFD> = (1/sqrt Z) sum_n e^{-beta E_n/2} |n>_L |n>_R
------------------------------------------------------------------------
beta= 0.5: norm_err=6.661e-16 trace_dist(rho_L, thermal)=9.841e-16 S(rho_L)=4.108975 nats
beta= 1.0: norm_err=2.220e-16 trace_dist(rho_L, thermal)=1.420e-15 S(rho_L)=2.404683 nats
beta= 2.0: norm_err=0.000e+00 trace_dist(rho_L, thermal)=1.894e-15 S(rho_L)=1.098229 nats
beta= 4.0: norm_err=1.110e-16 trace_dist(rho_L, thermal)=2.044e-15 S(rho_L)=0.476279 nats
HEADLINE (a) max thermality trace-distance over beta: 2.044e-15
-> an observer with one side alone sees a perfect thermal
state, indistinguishable from 'just heat'.
HEADLINE (b) max bridge-identity discrepancy (all beta, sites [1, 4, 8]): 4.441e-16
-> L-R correlations ARE the imaginary-time-displaced thermal
correlator: correlations run THROUGH the Euclidean bridge,
exactly. (Machine-precision agreement of two independent
numerical routes; a consistency check, not a sigma.)
------------------------------------------------------------------------
HEADLINE (c) hotter = more bridge: two-sided correlator <O_L O_R> vs beta
(O = sigma_z; sites are 1-indexed; S in nats, max = ln 256 = 5.5452)
------------------------------------------------------------------------
beta site 1:<OLOR> site 4:<OLOR> site 8:<OLOR> S(rho_L)
0.5 0.886136338 0.895108069 0.886136338 4.108975
1.0 0.690641075 0.747977787 0.690641075 2.404683
2.0 0.419181173 0.581083133 0.419181173 1.098229
4.0 0.202650347 0.408334079 0.202650347 0.476279
correlator strictly decreasing with beta at every site: True
entanglement entropy S(rho_L) strictly decreasing with beta: True
one-sided <O>_thermal (Z2-symmetric, expect 0): max |<O>| = 4.552e-15
-> so the two-sided correlator above is pure CROSS-correlation,
strongest at small beta (hot, near-maximal entanglement),
dying away as beta grows (cold, product-like TFD).
------------------------------------------------------------------------
HEADLINE (d) no signaling: [O_L, O_R] = 0 identically
------------------------------------------------------------------------
exact sparse commutator Frobenius norm, max over sites [1, 4, 8]: 0.0
max |(O_L O_R - O_R O_L) v| over TFD states + 3 rng(42) vectors: 0.0e+00
-> O_L and O_R act on different tensor factors and commute
IDENTICALLY: correlation without causation. Nothing
traverses the bridge; no signal can be sent L -> R.
========================================================================
SUMMARY (all reproduced-not-discovered; toy scale, no gravity):
(a) each side alone is EXACTLY thermal (max trace dist 2.0e-15)
(b) L-R correlations = Euclidean bridge (max discrepancy 4.4e-16)
(c) hotter = more bridge (monotone: corr True, S True)
(d) zero commutator, no signaling (norm 0.0)
This is the exact state structure ER=EPR identifies with a
two-sided black hole: featureless heat on each side, one pure
state overall, cross-correlations through an Euclidean bridge,
and nothing crossing. A state-structure demonstration only.
========================================================================
B · Yours
not runnable in-browser
This script needs data files, a heavy dependency, or more time than a browser tab should take. Download it from /data and run it locally.