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family
stringclasses
7 values
param
stringclasses
11 values
N
int64
12
2.89k
E
int64
16
3.5k
edge_depth
int64
0
8
n_edges
int64
4
2.57k
n_pairs
int64
6
3.3M
median_abs_cos
float64
0
0.22
mean_abs_cos
float64
0
0.42
p90_abs_cos
float64
0
0.95
participation_ratio
float64
2.36
2.51k
eff_dim_fraction
float64
0.14
1
{7,3}
L=1
35
42
0
35
595
0
0.002883
0
34.591248
0.988321
{7,3}
L=1
35
42
1
7
21
0.054178
0.149887
0.381311
5.396787
0.77097
{7,3}
L=2
112
140
0
98
4,753
0
0.001259
0
95.158156
0.971002
{7,3}
L=2
112
140
1
28
378
0.001148
0.057097
0.223132
16.221814
0.57935
{7,3}
L=2
112
140
2
7
21
0.013441
0.019444
0.039436
6.975369
0.996481
{7,3}
L=2
112
140
3
7
21
0.048561
0.089606
0.177414
6.533881
0.933412
{7,3}
L=3
315
399
0
259
33,411
0
0.000508
0
248.740267
0.960387
{7,3}
L=3
315
399
1
77
2,926
0.000034
0.021292
0.006768
42.630165
0.553639
{7,3}
L=3
315
399
2
21
210
0.000701
0.013087
0.038875
20.631261
0.982441
{7,3}
L=3
315
399
3
28
378
0.002306
0.035452
0.118657
22.952675
0.819738
{7,3}
L=3
315
399
4
7
21
0.01892
0.035056
0.080593
6.904917
0.986417
{7,3}
L=3
315
399
5
7
21
0.072391
0.134118
0.26194
6.050338
0.864334
{7,3}
L=4
847
1,078
0
679
230,181
0
0.000195
0
651.046581
0.958831
{7,3}
L=4
847
1,078
1
203
20,503
0.000001
0.008067
0.000144
111.62221
0.549863
{7,3}
L=4
847
1,078
2
56
1,540
0.000021
0.004909
0.003286
54.886555
0.980117
{7,3}
L=4
847
1,078
3
77
2,926
0.000023
0.013158
0.02059
61.393892
0.797323
{7,3}
L=4
847
1,078
4
21
210
0.000266
0.017008
0.042466
20.220481
0.96288
{7,3}
L=4
847
1,078
5
28
378
0.003799
0.03983
0.153582
22.126298
0.790225
{7,3}
L=4
847
1,078
6
7
21
0.033539
0.044061
0.095304
6.859801
0.979972
{7,3}
L=4
847
1,078
7
7
21
0.111173
0.164629
0.298735
5.750389
0.821484
{8,3}
L=1
48
56
0
48
1,128
0
0.001792
0
47.463468
0.988822
{8,3}
L=1
48
56
1
8
28
0.032244
0.129658
0.377937
6.200135
0.775017
{8,3}
L=2
200
240
0
184
16,836
0
0.000544
0
179.915163
0.9778
{8,3}
L=2
200
240
1
40
780
0.000406
0.035076
0.031301
24.500813
0.61252
{8,3}
L=2
200
240
2
8
28
0.018961
0.027291
0.069716
7.916855
0.989607
{8,3}
L=2
200
240
3
8
28
0.06762
0.059462
0.095611
7.750929
0.968866
{8,3}
L=3
768
928
0
688
236,328
0
0.000147
0
671.884528
0.976576
{8,3}
L=3
768
928
1
152
11,476
0.000002
0.009285
0.000397
91.076601
0.599188
{8,3}
L=3
768
928
2
32
496
0.000067
0.007567
0.01525
31.346806
0.979588
{8,3}
L=3
768
928
3
40
780
0.000188
0.017463
0.076871
34.134434
0.853361
{8,3}
L=3
768
928
4
8
28
0.034612
0.023722
0.044967
7.948656
0.993582
{8,3}
L=3
768
928
5
8
28
0.035457
0.073045
0.13656
7.610454
0.951307
{8,3}
L=4
2,888
3,496
0
2,568
3,296,028
0
0.000039
0
2,507.618579
0.976487
{8,3}
L=4
2,888
3,496
1
568
161,028
0
0.002477
0.000003
339.751054
0.598153
{8,3}
L=4
2,888
3,496
2
120
7,140
0
0.002021
0.000136
117.381286
0.978177
{8,3}
L=4
2,888
3,496
3
152
11,476
0.000001
0.004698
0.000415
127.6602
0.83987
{8,3}
L=4
2,888
3,496
4
32
496
0.000019
0.006974
0.025722
31.627226
0.988351
{8,3}
L=4
2,888
3,496
5
40
780
0.000253
0.018041
0.041503
34.831967
0.870799
{8,3}
L=4
2,888
3,496
6
8
28
0.027446
0.024701
0.052554
7.94357
0.992946
{8,3}
L=4
2,888
3,496
7
8
28
0.065294
0.089244
0.15057
7.488475
0.936059
{5,4}
L=1
20
25
0
25
300
0
0
0
25
1
{5,4}
L=2
60
80
0
75
2,775
0
0.001263
0
72.246377
0.963285
{5,4}
L=2
60
80
1
5
10
0.080367
0.080367
0.088988
4.872664
0.974533
{5,4}
L=3
165
225
0
200
19,900
0
0.000631
0
188.437089
0.942185
{5,4}
L=3
165
225
1
20
190
0.002477
0.023031
0.090801
18.39748
0.919874
{5,4}
L=3
165
225
2
5
10
0.090601
0.090601
0.139274
4.797035
0.959407
{5,4}
L=4
440
605
0
525
137,550
0
0.000249
0
492.709831
0.938495
{5,4}
L=4
440
605
1
55
1,485
0.000047
0.00881
0.005835
49.311538
0.896573
{5,4}
L=4
440
605
2
20
190
0.001931
0.023585
0.04701
18.893119
0.944656
{5,4}
L=4
440
605
3
5
10
0.097031
0.097031
0.175396
4.707102
0.94142
{5,4}
L=5
1,160
1,600
0
1,375
944,625
0
0.000095
0
1,289.660131
0.937935
{5,4}
L=5
1,160
1,600
1
145
10,440
0.000001
0.00336
0.000191
129.360405
0.892141
{5,4}
L=5
1,160
1,600
2
55
1,485
0.000037
0.008867
0.016905
51.277429
0.932317
{5,4}
L=5
1,160
1,600
3
20
190
0.002444
0.028285
0.059089
18.601541
0.930077
{5,4}
L=5
1,160
1,600
4
5
10
0.099315
0.099315
0.191632
4.657473
0.931495
{6,4}
L=1
30
36
0
36
630
0
0
0
36
1
{6,4}
L=2
120
150
0
144
10,296
0
0.000408
0
140.473535
0.975511
{6,4}
L=2
120
150
1
6
15
0.035958
0.061577
0.102465
5.856244
0.976041
{6,4}
L=3
456
576
0
540
145,530
0
0.000123
0
521.67336
0.966062
{6,4}
L=3
456
576
1
30
435
0.000171
0.013811
0.034213
28.191985
0.939733
{6,4}
L=3
456
576
2
6
15
0.057549
0.051606
0.059812
5.918702
0.98645
{6,4}
L=4
1,710
2,166
0
2,016
2,031,120
0
0.000033
0
1,945.918708
0.965237
{6,4}
L=4
1,710
2,166
1
114
6,441
0.000001
0.003664
0.000523
105.918088
0.929106
{6,4}
L=4
1,710
2,166
2
30
435
0.00028
0.012757
0.040454
28.803517
0.960117
{6,4}
L=4
1,710
2,166
3
6
15
0.069365
0.047119
0.071465
5.909599
0.984933
{4,5}
L=1
12
16
0
16
120
0
0
0
16
1
{4,5}
L=2
32
48
0
44
946
0
0.004189
0.003397
43.279527
0.983626
{4,5}
L=2
32
48
1
4
6
0.036577
0.062551
0.114501
3.937837
0.984459
{4,5}
L=3
80
124
0
108
5,778
0
0.001995
0.000076
104.8245
0.970597
{4,5}
L=3
80
124
1
16
120
0.010096
0.048547
0.152618
14.634883
0.91468
{4,5}
L=4
188
296
0
248
30,628
0
0.000925
0.000003
237.811486
0.958917
{4,5}
L=4
188
296
1
44
946
0.001065
0.020632
0.092015
39.149955
0.889772
{4,5}
L=4
188
296
2
4
6
0.026376
0.105656
0.264217
3.734123
0.933531
{4,5}
L=5
436
692
0
568
161,028
0
0.000395
0
545.621128
0.960601
{4,5}
L=5
436
692
1
104
5,356
0.000024
0.00867
0.010976
91.653052
0.881279
{4,5}
L=5
436
692
2
16
120
0.006665
0.035094
0.105933
14.663257
0.916454
{4,5}
L=5
436
692
3
4
6
0.036671
0.122426
0.293934
3.672803
0.918201
{4,5}
L=6
1,008
1,604
0
1,308
854,778
0
0.000171
0
1,256.875488
0.960914
{4,5}
L=6
1,008
1,604
1
240
28,680
0.000001
0.003816
0.000347
210.681772
0.877841
{4,5}
L=6
1,008
1,604
2
40
780
0.000201
0.01624
0.043742
35.956596
0.898915
{4,5}
L=6
1,008
1,604
3
16
120
0.03271
0.064021
0.274313
13.312542
0.832034
square
R=3
29
44
0
32
496
0
0.02152
0.03058
26.178531
0.818079
square
R=3
29
44
1
12
66
0.057716
0.097344
0.277998
9.872589
0.822716
square
R=6
113
200
0
80
3,160
0
0.010616
0.002562
57.807441
0.722593
square
R=6
113
200
1
44
946
0.00302
0.030805
0.124652
35.083686
0.797356
square
R=6
113
200
2
36
630
0.009247
0.058663
0.188326
23.478929
0.652192
square
R=6
113
200
3
28
378
0.069034
0.151099
0.378181
10.120992
0.361464
square
R=6
113
200
4
12
66
0.039285
0.343837
0.843411
3.242586
0.270216
square
R=10
317
592
0
144
10,296
0
0.006518
0.000327
101.691215
0.706189
square
R=10
317
592
1
92
4,186
0.000361
0.016482
0.024728
69.309338
0.753362
square
R=10
317
592
2
84
3,486
0.001265
0.032631
0.107853
48.607162
0.578657
square
R=10
317
592
3
76
2,850
0.004769
0.060174
0.20483
29.306635
0.385614
square
R=10
317
592
4
60
1,770
0.011365
0.087665
0.224121
19.098934
0.318316
square
R=10
317
592
5
52
1,326
0.057504
0.134237
0.385254
12.855582
0.247223
square
R=10
317
592
6
44
946
0.08159
0.208665
0.700476
7.576075
0.172184
square
R=10
317
592
7
28
378
0.023334
0.323755
0.80106
3.932129
0.140433
square
R=10
317
592
8
12
66
0.019465
0.419688
0.950851
2.361869
0.196822
triangular
R=3.225
37
87
0
53
1,378
0.000682
0.034399
0.057176
28.547269
0.538628
triangular
R=3.225
37
87
1
27
351
0.03545
0.093824
0.303843
16.830806
0.623363
triangular
R=3.225
37
87
2
7
21
0.188611
0.227472
0.518692
4.655768
0.66511
End of preview. Expand in Data Studio

Hyperbolic vs flat resistor networks: conditioning of the inverse conductance problem

Data accompanying the preprint Logarithmic boundary depth and the conditioning of the discrete inverse conductance problem on hyperbolic lattices (X. Callens, 2026), included as paper.pdf.

Contents

File What it contains
graphs/*.json Layer-truncated {7,3} tilings (L=1..6) and square/triangular lattice disks: node coordinates (Poincare disk / plane), edge list, boundary nodes (face incidence)
dtn/*.npz Dirichlet-to-Neumann map Lambda (unit conductances) for graphs with N <= 900
conditioning.csv log10 condition number of the DtN sensitivity Jacobian; empty and numerically_singular_float64=True where float64 cannot resolve it
probe_matched.csv DtN and Neumann-to-Dirichlet conditioning, full vs subsampled boundary
exact_rank.csv Exact Jacobian ranks over GF(p) for two primes; deficiency vs number of unmeasured degree-2 nodes; condition number on the identifiable subspace
exact_rank_full_boundary.csv Exact full-boundary Jacobian ranks over GF(p), two primes: full-rank certificates
conditioning_arb.csv (v1.1) log10 condition number in 512-bit ball arithmetic for the float64-singular flat lattices, with certified radii and the two unsaturated controls
disorder.csv (v1.1) log10 kappa (log-parametrised and raw Jacobian) under U[0.5,1.5] and log-uniform [0.1,10] conductances (5 seeds) and x100 / x0.01 defects
subspace_control.csv (v1.1) probe-matched dimensionality control: square lattice sigma_1/sigma_r vs hyperbolic identifiable-subspace kappa
tda_defect.csv (post-v1.1, not in the paper) persistent homology (Gudhi) of the boundary resistance metric with and without a bulk defect, vs a global-disorder null. The null was mis-sized; see TDA_RESULTS.md
tda_noise.csv (post-v1.1, not in the paper) defect detection vs measurement-noise level (eps_max), metric and H1 detectors
localize_defect.csv (post-v1.1, not in the paper) single-node defect localisation from two noisy NtD maps (oracle-dictionary matched filter); 60/60 cells perfect at noise 3e-4, so it is a ceiling, not a measurement of the failure boundary
tilings_kappa.csv (post-v1.1, not in the paper) log10 condition number for (7, 3), (8, 3), (5, 4), (6, 4), (4, 5) at L=1..6, with d_max and float64 error bounds (Gram-matrix method, controls in the repository)
localize_tolerance.csv (post-v1.1, not in the paper) localisation top-1 on random boards with component tolerance 0.1 %, 1 %, 5 % and an ideal-model decoder; tolerance has no effect in this differential setting
localize_noise.csv (post-v1.1, not in the paper) localisation top-1 vs noise level and eps_loc (largest noise with top-1 >= 0.9) at the deepest node, contrasts x1.25 and x2
tolerance_null.csv (post-v1.1, not in the paper) defect detection vs component tolerance (0.1 %, 1 %, 5 %), model-based and differential regimes; only the extreme x100 contrast is tested
exact_rank_tilings.csv (v1.2) exact full-column-rank certificates (random row-combination method, two primes) for 11 instances of {7,3}, {8,3}, {5,4}, {6,4}, {4,5} up to E = 1604
rc_benchmark_tilings.csv (v1.2) RC relaxation time, stiffness and the K1/K2 integrator controls (SciPy BDF and rusty-SUNDIALS CVODE) on {7,3} L=2, {8,3} L=2, {5,4} L=3, {6,4} L=2, {4,5} L=4
minimum_contrast.csv (v1.2) localisation top-1 vs true contrast (x0.5 to x2) and noise (1e-4 to 3e-3) at the deepest node of four lattices; both geometries localise +-10 % at the 3e-4 budget
hardware_noise.csv (v1.2) localisation top-1 under common-mode offset, gain drift and ADC quantisation at N~112, contrast x2; a floor (49/50 cells at 1.00), not a failure boundary
coherence_depth.csv (v1.2) per edge depth and instance: exhaustive abs-cosine statistics between Jacobian columns of equal-depth edges and the effective dimension fraction (participation ratio / count) of their normalised Gram matrix
coherence_matched.csv (v1.2) per depth on the largest instance of each family: log10 kappa of the Jacobian restricted to columns of depth <= d, the full-class effective dimension fraction and the six-column matched-size median of 50 draws
coherence_mechanism_test.csv (v1.2) test of the band-counting argument on unseen instances ({7,3} L=5, {4,5} L=7, square R=16, triangular R=10.75): effective dimension fraction and depth-restricted log10 kappa per depth
flat_rate_windows.csv (v1.2, exploratory) growth rate of the depth-restricted log10 kappa over windows fixed in relative depth on square R=6..22 and triangular R=3.2..17.2, with per-class effective dimension fraction and smallest normalised-Gram eigenvalue
spectral_gap.csv Dirichlet spectral gap, RC relaxation time and stiffness; exploratory=True rows were not preregistered
interior_degree.json Integer check that interior nodes of the {7,3} truncations have degree 3, and that the interior of G_L is G_(L-1) (coordinates and edge sets)
integrator_controls.csv K1 (matrix-exponential known answer) and K2 (steady state = DtN column) controls per integrator; rows with status other than run were not executed
rc_step_response.csv Reference (matrix-exponential) RC step response V_i(t), C=1, on {7,3} L=2 and square R=6

Provenance and reproduction

Generated from commit ccfc30dddab42c801d7aedb7d0ff99e0fff4139b of https://github.com/xaviercallens/SocrateAI-Scientific-CondensedMatterTheory, directory experiments/track_h_hyperbolic_network:

python3 hyperbolic_network.py --self-test && python3 hyperbolic_exact.py --self-test
python3 hyperbolic_exact.py && python3 probe_matched.py && python3 identifiability.py && python3 rc_network.py
python3 h2_explore.py && python3 interior_degree.py
python3 release/export.py

Each claim built on these data carries an evidence tier in docs/elenchus/ledger.json of that repository.

Known limitations

  • Condition numbers are float64 SVD values; "numerically singular" means unresolved, not infinite.
  • The two-integrator (SciPy BDF, rusty-SUNDIALS CVODE) cross-validation covers two networks of ~110 nodes.
  • The probe-matched identifiable-subspace metric was chosen post hoc (deviation from preregistration).

License

Data and paper: CC BY 4.0. Code (see the companion model repository and the Zenodo archive): MIT.

Citation

Callens, X. (2026). Logarithmic boundary depth and the conditioning of the discrete inverse conductance problem on hyperbolic lattices. Preprint.

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