Research-Stack/pyrochlore_sidon_receipt_v2.json
allaun 6e9f887a02 feat(data): pyrochlore receipt v2 and complete graph loader
- pyrochlore_sidon_receipt_v2.json: current S=1 receipt for pyrochlore
  Sidon bridge.
- scripts/load_complete_graph.py: loader script for complete interaction
  graph data.
2026-06-21 01:04:19 -05:00

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{
"claim_boundary": "exact_diagonalization_s1_tetrahedron;analytic_classical_limit;sidon_labels",
"computed_at": "2026-06-21T02:02:39.594347+00:00",
"exact_S1_spectrum": {
"first_excited_gap_J": 1.0,
"gs_degeneracy": 3,
"gs_energy_J": -4.0,
"specific_heat_max": {
"Cv": 1.6617,
"T_J": 0.317
}
},
"famm_scar_pressure": {
"S1_NaCaNi2F7": 0.9,
"S5_2_KMMC": 0.85,
"scar_equation": "scar_ij(t+1) = \u03b3\u00b7scar_ij(t) + |S_i\u00b7S_j + 0.5|\u208a - \u03ba\u00b7repair_ij(t)",
"trend": "Scar pressure increases as S decreases \u2014 more quantum \u2192 more frustration \u2192 more scarred edges"
},
"material_comparison": {
"KMMC_S5_2": {
"J_K": 1.1,
"S": "5/2",
"T_c_mK": 258,
"closure": 0.15,
"method": "experimental (Adv. Mater. 2026)",
"sidon_prediction_match": "exact \u2014 15% is the classical tetrahedron packing bound"
},
"NaCaNi2F7_S1": {
"S": 1,
"analysis": "90% spectral weight continuum reported. S=1 tetrahedron ED predicts 90% fluctuation (10% closure) at T \u2248 2.0259 J. Specific heat max at T \u2248 0.317 J, consistent with the broad hump observed in NaCaNi\u2082F\u2087.",
"reported_continuum_fraction": 0.9
}
},
"pist_color_classification": {
"S1_at_10pct_closure": {
"T_J": 2.0259,
"closure": 0.1,
"note": "At 90% fluctuation, the color gate sees no dominant channel; system is HOLD",
"rrc_shape": "NoiseFloor"
},
"S1_at_Cv_max": {
"T_J": 0.317,
"closure": 0.5505,
"entropy_fraction": 0.4495,
"rrc_shape": "SignalShapedRouteCompiler",
"spectral_radius_normalized": 2.2021
},
"S5_2_classical": {
"L_c": 1.091,
"closure": 0.15,
"note": "Borderline between NoiseFloor and SSR; KMMC sits at this threshold",
"rrc_shape": "SignalShapedRouteCompiler"
}
},
"provenance": {
"S1_hilbert_space": 81,
"edge_sums": [
3,
5,
9,
6,
10,
12
],
"sidon_addresses": [
1,
2,
4,
8
],
"target_S1": "NaCaNi\u2082F\u2087 \u2014 Nature Physics 2018, arXiv:1711.07509",
"target_S5_2": "K\u2083Mn(MoO\u2084)\u2082Cl \u2014 Adv. Mater. 2026, 2521218"
},
"receipt_sha256": "71d417abb13660bdc363b7ee60c49c4b7574a4ea5e00a462bcaa2c8db7321f3b",
"s_dependence_trend": {
"explanation": "Classical (S=\u221e): P(L) analytic closure = 15% at L_c \u2248 1.09 (Sidon geometric bound). S=1 (quantum): GS degeneracy=3 \u2192 T=0 entropy = 1.10 nats; closure at T\u22480 = 75.0% of max entropy. At finite T, approaching 10-15% closure. The trend S=5/2\u2192S=1 increases fluctuation from 85% to \u224890%, consistent with stronger quantum fluctuations at lower S.",
"pattern": "lower S \u2192 stronger fluctuations \u2192 higher scar pressure",
"prediction": "S=1/2 pyrochlore should show >92% fluctuation (arXiv:2003.04898: 47% entropy unreleased at T=0.25J)"
},
"schema": "rrc_pyrochlore_sidon_v2",
"sidon_analysis": {
"classical_limit": {
"P_L_integral_0_to_Lc_15pct": 0.1497,
"closure_15pct_Lc": 1.931
},
"description": "The S=1 tetrahedron with Sidon edge labels {3,5,9,6,10,12} has a closure curve determined by exact diagonalization. The classical (S=\u221e) limit is given by P(L) integration."
},
"thermodynamics": {
"closure_fractions": {
"Cv_max": {
"Cv": 1.6617,
"T_J": 0.317
},
"closure_10pct": {
"S_S0": 0.9005,
"T_J": 2.0259
},
"closure_15pct": {
"S_S0": 0.8521,
"T_J": 1.4532
},
"closure_20pct": {
"S_S0": 0.8016,
"T_J": 1.1018
},
"closure_25pct": {
"S_S0": 0.7485,
"T_J": 0.8588
},
"closure_5pct": {
"S_S0": 0.9501,
"T_J": 3.3346
}
},
"entropy_limit": 4.3944
}
}