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Prepared pair orientations are conditional; no cross-depth spatial map, full core response or measured coupling." }, "retained_tower": { "experiment": "two-current-grade-zero-tower", "rows": [ { "depth": 2, "indices": [ 76, 81, 95 ], "rank": 2, "isolated_target_excess": 2.220446049250313e-16, "isolated_probe_excess": -5.551115123125783e-17, "isolated_source_norms": [ 3.450423302889156e-16, 1.2222108709692242e-16 ], "pair_energy": 0.018926970923754727, "pair_formula_error": 1.0408340855860843e-16, "reciprocal_source_derivative_relative_errors": [ 4.568856404318922e-11, 1.337048805005736e-10 ] }, { "depth": 3, "indices": [ 1, 4, 16, 17 ], "rank": 2, "isolated_target_excess": 0.0, "isolated_probe_excess": 0.0, "isolated_source_norms": [ 8.966356948277505e-16, 3.162446572035138e-16 ], "pair_energy": 0.5232114718671532, "pair_formula_error": 6.661338147750939e-16, "reciprocal_source_derivative_relative_errors": [ 3.3407487887160414e-10, 3.5071982072379596e-12 ] }, { "depth": 4, "indices": [ 3, 20, 72 ], "rank": 4, "isolated_target_excess": -2.220446049250313e-16, "isolated_probe_excess": -1.1102230246251565e-16, "isolated_source_norms": [ 5.12494078415642e-16, 4.96746768566487e-16 ], "pair_energy": 1.3659035877745351, "pair_formula_error": 4.440892098500626e-16, "reciprocal_source_derivative_relative_errors": [ 4.883192861443126e-10, 1.952951186618086e-10 ] }, { "depth": 5, "indices": [ 10, 15, 22 ], "rank": 4, "isolated_target_excess": 6.661338147750939e-16, "isolated_probe_excess": -1.1102230246251565e-16, "isolated_source_norms": [ 8.847557534732069e-16, 2.3955897827667343e-16 ], "pair_energy": 2.16200163909326, "pair_formula_error": 8.881784197001252e-16, "reciprocal_source_derivative_relative_errors": [ 1.23395782480884e-09, 9.737686212929475e-10 ] }, { "depth": 6, "indices": [ 13, 35 ], "rank": 8, "isolated_target_excess": 1.7763568394002505e-15, "isolated_probe_excess": 4.440892098500626e-16, "isolated_source_norms": [ 2.826074705879811e-15, 6.509995487736282e-16 ], "pair_energy": 4.01538045111449, "pair_formula_error": 2.6645352591003757e-15, "reciprocal_source_derivative_relative_errors": [ 1.1858286364001484e-09, 3.89623000529582e-10 ] }, { "depth": 10, "indices": [ 23 ], "rank": 32, "isolated_target_excess": 0.0, "isolated_probe_excess": -8.881784197001252e-16, "isolated_source_norms": [ 6.740450281499978e-15, 2.092126784357659e-15 ], "pair_energy": 15.74225508329701, "pair_formula_error": 7.105427357601002e-15, "reciprocal_source_derivative_relative_errors": [ 6.747969836776876e-09, 1.2761726836053355e-09 ] } ], "scope": "Actual retained grade-zero maps with grade-two/grade-one coherent fields at all six depths. The order-zero quartic contact is grade independent, but higher assigned grades are represented by the exact coherent-ray contraction rather than full arrays. No spatial profile or observed vertex is included." }, "spatial_overlap": { "experiment": "two-current-quartic-displaced-core", "rows": [ { "depth": 2, "indices": [ 76, 81, 95 ], "partner_rank": 2, "analytic_core_unit_norm_possible": false, "dimensionless_norm_integral": null, "dimensionless_pair_integral": 1.0471975511965976, "dimensionless_positive_sum_coincident_integral": 3.141592653589793, "unit_norm_small_displacement_coefficient_times_radius_power": null, "barrier_separation_over_radius": 1.7166074788159984, "barrier_shape_factor": 0.7923722642428106, "checks": [ { "separation_over_radius": 0.1, "hypergeometric_factor": 0.994025619371249, "feynman_relative_error": 2.233791570336801e-16, "positive_sum_pair_factor": 3.1259577034748056, "direct_convolution_relative_error": 2.133113821536655e-16 }, { "separation_over_radius": 1.0, "hypergeometric_factor": 0.5863851666508875, "feynman_relative_error": 3.7866681756844057e-16, "positive_sum_pair_factor": 2.0902780233689384, "direct_convolution_relative_error": 1.8080008740268285e-16 }, { "separation_over_radius": 3.0, "hypergeometric_factor": 0.06247128947123449, "feynman_relative_error": 1.1107332604527572e-16, "positive_sum_pair_factor": 0.7992517250541774, "direct_convolution_relative_error": 0.0 } ] }, { "depth": 3, "indices": [ 1, 4, 16, 17 ], "partner_rank": 2, "analytic_core_unit_norm_possible": true, "dimensionless_norm_integral": 9.869604401089358, "dimensionless_pair_integral": 0.5397439906845743, "dimensionless_positive_sum_coincident_integral": 1.23370055013617, "unit_norm_small_displacement_coefficient_times_radius_power": 0.011082004460880696, "barrier_separation_over_radius": 1.1918799677731964, "barrier_shape_factor": 0.44260450164899845, "checks": [ { "separation_over_radius": 0.1, "hypergeometric_factor": 0.9904157825006187, "feynman_relative_error": 2.241933224896814e-16, "positive_sum_pair_factor": 1.2222093927359174, "direct_convolution_relative_error": null }, { "separation_over_radius": 1.0, "hypergeometric_factor": 0.4242285714285715, "feynman_relative_error": 2.6170397266891486e-16, "positive_sum_pair_factor": 0.5605935299818757, "direct_convolution_relative_error": null }, { "separation_over_radius": 3.0, "hypergeometric_factor": 0.011844323177959956, "feynman_relative_error": 0.0, "positive_sum_pair_factor": 0.0592639317526286, "direct_convolution_relative_error": null } ] }, { "depth": 4, "indices": [ 3, 20, 72 ], "partner_rank": 4, "analytic_core_unit_norm_possible": true, "dimensionless_norm_integral": 4.934802200544679, "dimensionless_pair_integral": 0.23499058097831804, "dimensionless_positive_sum_coincident_integral": 0.4934802200544679, "unit_norm_small_displacement_coefficient_times_radius_power": 0.009649636537365502, "barrier_separation_over_radius": 0.9649135788865741, "barrier_shape_factor": 0.30613936524637253, "checks": [ { "separation_over_radius": 0.1, "hypergeometric_factor": 0.986772078002593, "feynman_relative_error": 4.500423347496623e-16, "positive_sum_pair_factor": 0.4869549608317846, "direct_convolution_relative_error": 1.1969690787074209e-16 }, { "separation_over_radius": 1.0, "hypergeometric_factor": 0.3055027732979886, "feynman_relative_error": 0.0, "positive_sum_pair_factor": 0.1581532084466402, "direct_convolution_relative_error": 2.706341931515693e-15 }, { "separation_over_radius": 3.0, "hypergeometric_factor": 0.0021820726590960193, "feynman_relative_error": 7.949888692961595e-16, "positive_sum_pair_factor": 0.004473573410190614, "direct_convolution_relative_error": 4.281694115202802e-13 } ] }, { "depth": 5, "indices": [ 10, 15, 22 ], "partner_rank": 4, "analytic_core_unit_norm_possible": true, "dimensionless_norm_integral": 2.5838563900249847, "dimensionless_pair_integral": 0.09020787689784494, "dimensionless_positive_sum_coincident_integral": 0.18167740242363173, "unit_norm_small_displacement_coefficient_times_radius_power": 0.013511629171721275, "barrier_separation_over_radius": 0.83152108562294, "barrier_shape_factor": 0.23374079625837543, "checks": [ { "separation_over_radius": 0.1, "hypergeometric_factor": 0.983120494366971, "feynman_relative_error": 3.387854380983158e-16, "positive_sum_pair_factor": 0.17858635598874092, "direct_convolution_relative_error": null }, { "separation_over_radius": 1.0, "hypergeometric_factor": 0.21952268531468527, "feynman_relative_error": 0.0, "positive_sum_pair_factor": 0.04138304394264014, "direct_convolution_relative_error": null }, { "separation_over_radius": 3.0, "hypergeometric_factor": 0.00039565284659443624, "feynman_relative_error": 1.3701432730962574e-16, "positive_sum_pair_factor": 0.00030509785526552946, "direct_convolution_relative_error": null } ] }, { "depth": 6, "indices": [ 13, 35 ], "partner_rank": 8, "analytic_core_unit_norm_possible": true, "dimensionless_norm_integral": 1.2919281950124923, "dimensionless_pair_integral": 0.03131947139424224, "dimensionless_positive_sum_coincident_integral": 0.061520390238690104, "unit_norm_small_displacement_coefficient_times_radius_power": 0.009382264562385306, "barrier_separation_over_radius": 0.7413436706159707, "barrier_shape_factor": 0.1889481431688617, "checks": [ { "separation_over_radius": 0.1, "hypergeometric_factor": 0.9794710011874365, "feynman_relative_error": 5.667462453095635e-16, "positive_sum_pair_factor": 0.06024386320932825, "direct_convolution_relative_error": 2.261956460629129e-16 }, { "separation_over_radius": 1.0, "hypergeometric_factor": 0.15754822328068632, "feynman_relative_error": 1.7617193667858668e-16, "positive_sum_pair_factor": 0.009989025756074061, "direct_convolution_relative_error": 1.2304681219979206e-15 }, { "separation_over_radius": 3.0, "hypergeometric_factor": 7.101419896466317e-05, "feynman_relative_error": 1.9084249845319734e-15, "positive_sum_pair_factor": 1.886940248537558e-05, "direct_convolution_relative_error": 8.801174522824545e-13 } ] }, { "depth": 10, "indices": [ 23 ], "partner_rank": 32, "analytic_core_unit_norm_possible": true, "dimensionless_norm_integral": 0.045538643569238306, "dimensionless_pair_integral": 0.00021931235293062823, "dimensionless_positive_sum_coincident_integral": 0.0004121144214410706, "unit_norm_small_displacement_coefficient_times_radius_power": 0.013219435996665915, "barrier_separation_over_radius": 0.5491245623002748, "barrier_shape_factor": 0.10684324986638144, "checks": [ { "separation_over_radius": 0.1, "hypergeometric_factor": 0.9649597519205134, "feynman_relative_error": 4.60215266974828e-16, "positive_sum_pair_factor": 0.0003975183346538403, "direct_convolution_relative_error": 6.403950883999945e-16 }, { "separation_over_radius": 1.0, "hypergeometric_factor": 0.041570070692869776, "feynman_relative_error": 0.0, "positive_sum_pair_factor": 1.7433643087640273e-05, "direct_convolution_relative_error": 1.1149045611430133e-15 }, { "separation_over_radius": 3.0, "hypergeometric_factor": 6.974559394719606e-08, "feynman_relative_error": 1.0626532615216206e-14, "positive_sum_pair_factor": 1.2979530431840512e-10, "direct_convolution_relative_error": null } ] } ], "exact_formula": "For analytic stereographic cores with rho=A^2(1+|x|^2/R^2)^(1-d), the prepared difference-current pair potential per eta*omega0*h_k*s^k is 4*r*A^4*R^d*h^2*J_d*F_d(h), h=delta/R, J_d=pi^(d/2)*Gamma(3d/2)/Gamma(2d), F_d=2F1(3d/2,d;d+1/2;-h^2/4). The positive-sum quartic prepared pair per 4*g*r*A^4*R^d*s^k is J_base*F_base(h)-h^2*J_d*F_d(h), with J_base=pi^(d/2)*Gamma(3d/2-2)/Gamma(2d-2) and F_base=2F1(3d/2-2,d-1;d-1/2;-h^2/4).", "scope": "Same-depth translated analytic upper cores only. d=2 has divergent canonical norm; odd-depth stereographic polarization lacks the maintained Clifford realization. This is an initial potential, not a solved encounter or bound composite." }, "depth_two_polarization": { "experiment": "depth-two-transverse-polarization-control", "comparisons": [ { "first": "linear_x", "second": "linear_x", "jones_overlap_squared": 1.0, "quartic_pair_factor": 3.999999999999999, "common_physical_rotation_errors": [ 8.881784197001252e-16, 1.7763568394002505e-15, 8.881784197001252e-16 ] }, { "first": "linear_x", "second": "linear_y", "jones_overlap_squared": 3.749399456654644e-33, "quartic_pair_factor": -4.625929269271486e-16, "common_physical_rotation_errors": [ 0.0, 0.0, 0.0 ] }, { "first": "linear_x", "second": "linear_45", "jones_overlap_squared": 0.5000000000000001, "quartic_pair_factor": 2.0, "common_physical_rotation_errors": [ 0.0, 0.0, 0.0 ] }, { "first": "circular_right", "second": "circular_left", "jones_overlap_squared": 5.305320603296788e-32, "quartic_pair_factor": -4.625929269271486e-16, "common_physical_rotation_errors": [ 0.0, 0.0, 0.0 ] }, { "first": "circular_right", "second": "circular_right", "jones_overlap_squared": 1.0, "quartic_pair_factor": 3.999999999999999, "common_physical_rotation_errors": [ 2.6645352591003757e-15, 8.881784197001252e-16, 8.881784197001252e-16 ] }, { "first": "elliptical_a", "second": "elliptical_b", "jones_overlap_squared": 0.27794285808655483, "quartic_pair_factor": 1.1117714323462184, "common_physical_rotation_errors": [ 8.881784197001252e-16, 8.881784197001252e-16, 0.0 ] } ], "relative_rotations": [ { "relative_rotation": 0.0, "linear_pair_factor": 3.999999999999999, "circular_pair_factor": 3.999999999999999 }, { "relative_rotation": 0.3, "linear_pair_factor": 3.650671229819356, "circular_pair_factor": 3.999999999999999 }, { "relative_rotation": 0.8, "linear_pair_factor": 1.941600955397422, "circular_pair_factor": 3.999999999999999 }, { "relative_rotation": 1.5707963267948966, "linear_pair_factor": -4.625929269271486e-16, "circular_pair_factor": 3.999999999999999 } ], "identity": "For normalized transverse Jones vectors e,f, B_e=2ee^dagger-I obeys Tr B_e B_f=4|e^dagger f|^2-2. The positive-sum two-current prepared pair factor is 2+Tr B_e B_f=4|e^dagger f|^2.", "scope": "Explicit linear, circular and elliptical transverse Jones controls with common and relative physical-plane rotations. Identifying these Jones vectors with occupied IDWT photon states and their field equation remains a physical premise." }, "shared_shell_grade_response": { "experiment": "two-current-shared-shell-pair-response", "rows": [ { "depth": 2, "maintained_indices": [ 76, 81, 95 ], "samples": [ { "ray_overlap": 0.0, "pair_sum_by_particle_index": { "76": 1.0, "81": 1.0, "95": 1.0 }, "lowest_to_highest_pair_sum_ratio": 1.0, "infinite_shell_sum": 1.0, "lowest_index_saturation_fraction": 1.0 }, { "ray_overlap": 0.1, "pair_sum_by_particle_index": { "76": 1.2345679012345678, "81": 1.2345679012345678, "95": 1.2345679012345678 }, "lowest_to_highest_pair_sum_ratio": 1.0, "infinite_shell_sum": 1.2345679012345678, "lowest_index_saturation_fraction": 1.0 }, { "ray_overlap": 0.3, "pair_sum_by_particle_index": { "76": 2.0408163265306123, "81": 2.0408163265306123, "95": 2.0408163265306123 }, "lowest_to_highest_pair_sum_ratio": 1.0, "infinite_shell_sum": 2.0408163265306123, "lowest_index_saturation_fraction": 1.0 }, { "ray_overlap": 0.5, "pair_sum_by_particle_index": { "76": 4.0, "81": 4.0, "95": 4.0 }, "lowest_to_highest_pair_sum_ratio": 1.0, "infinite_shell_sum": 4.0, "lowest_index_saturation_fraction": 1.0 }, { "ray_overlap": 0.8, "pair_sum_by_particle_index": { "76": 24.999982529954572, "81": 24.99999392204611, "95": 24.999999689172988 }, "lowest_to_highest_pair_sum_ratio": 0.9999993136312548, "infinite_shell_sum": 25.00000000000001, "lowest_index_saturation_fraction": 0.9999993011981825 }, { "ray_overlap": 1.0, "pair_sum_by_particle_index": { "76": 2926.0, "81": 3321.0, "95": 4560.0 }, "lowest_to_highest_pair_sum_ratio": 0.6416666666666667, "infinite_shell_sum": null, "lowest_index_saturation_fraction": null } ] }, { "depth": 3, "maintained_indices": [ 1, 4, 16, 17 ], "samples": [ { "ray_overlap": 0.0, "pair_sum_by_particle_index": { "1": 1.0, "4": 1.0, "16": 1.0, "17": 1.0 }, "lowest_to_highest_pair_sum_ratio": 1.0, "infinite_shell_sum": 1.0, "lowest_index_saturation_fraction": 1.0 }, { "ray_overlap": 0.1, "pair_sum_by_particle_index": { "1": 1.0, "4": 1.37, "16": 1.371742112482836, "17": 1.3717421124828513 }, "lowest_to_highest_pair_sum_ratio": 0.7290000000000011, "infinite_shell_sum": 1.371742112482853, "lowest_index_saturation_fraction": 0.7290000000000001 }, { "ray_overlap": 0.3, "pair_sum_by_particle_index": { "1": 1.0, "4": 2.71, "16": 2.9154509055966518, "17": 2.9154515642114833 }, "lowest_to_highest_pair_sum_ratio": 0.34300003892208764, "infinite_shell_sum": 2.9154518950437325, "lowest_index_saturation_fraction": 0.3429999999999999 }, { "ray_overlap": 0.5, "pair_sum_by_particle_index": { "1": 1.0, "4": 5.25, "16": 7.9947509765625, "17": 7.9970855712890625 }, "lowest_to_highest_pair_sum_ratio": 0.12504555454429236, "infinite_shell_sum": 8.0, "lowest_index_saturation_fraction": 0.125 }, { "ray_overlap": 0.8, "pair_sum_by_particle_index": { "1": 1.0, "4": 12.360000000000003, "16": 91.082265306366, "17": 95.38883245003903 }, "lowest_to_highest_pair_sum_ratio": 0.010483407484033954, "infinite_shell_sum": 125.00000000000009, "lowest_index_saturation_fraction": 0.007999999999999995 }, { "ray_overlap": 1.0, "pair_sum_by_particle_index": { "1": 1.0, "4": 20.0, "16": 816.0, "17": 969.0 }, "lowest_to_highest_pair_sum_ratio": 0.0010319917440660474, "infinite_shell_sum": null, "lowest_index_saturation_fraction": null } ] }, { "depth": 4, "maintained_indices": [ 3, 20, 72 ], "samples": [ { "ray_overlap": 0.0, "pair_sum_by_particle_index": { "3": 1.0, "20": 1.0, "72": 1.0 }, "lowest_to_highest_pair_sum_ratio": 1.0, "infinite_shell_sum": 1.0, "lowest_index_saturation_fraction": 1.0 }, { "ray_overlap": 0.1, "pair_sum_by_particle_index": { "3": 1.5, "20": 1.5241579027587258, "72": 1.5241579027587258 }, "lowest_to_highest_pair_sum_ratio": 0.9841500000000001, "infinite_shell_sum": 1.5241579027587258, "lowest_index_saturation_fraction": 0.9841500000000001 }, { "ray_overlap": 0.3, "pair_sum_by_particle_index": { "3": 3.0999999999999996, "20": 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At s=1 this is D_M=binom(M+d,d); for 0<=s<1 the infinite sum is (1-s)^(-d).", "scope": "Exact retained-order weight comparison on prepared same-depth pairs. It does not determine the physical ray overlap, encounter rate, or cross-depth embedding." }, "constant_density_self_mass": { "experiment": "one-quartic-contact-constant-density", "algebra": [ { "depth": 2, "indices": [ 76, 81, 95 ], "rank": 2, "mixing": -1.0, "coefficient_for_unit_self_frequency": 0.25, "self_energy_at_unit_density": 1.0, "energy_over_frequency_times_canonical_norm": 0.5, "self_source_relative_error": 0.0, "aligned_pair_cross_energy_per_rho_sigma": 2.0, "opposite_polarization_pair_cross_energy_per_rho_sigma": 0.0 }, { "depth": 2, "indices": [ 76, 81, 95 ], "rank": 2, "mixing": -0.5, "coefficient_for_unit_self_frequency": 0.3333333333333333, "self_energy_at_unit_density": 1.0, "energy_over_frequency_times_canonical_norm": 0.5, "self_source_relative_error": 0.0, "aligned_pair_cross_energy_per_rho_sigma": 2.0, "opposite_polarization_pair_cross_energy_per_rho_sigma": 0.6666666666666666 }, { "depth": 2, "indices": [ 76, 81, 95 ], "rank": 2, "mixing": 0.0, 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"max_imaginary_frequency": 2.6078916566919563 } ], "maxima": [ { "depth": 2, "mixing": -1.0, "max_imaginary_frequency": 2.58025123842548e-15 }, { "depth": 2, "mixing": -0.5, "max_imaginary_frequency": 1.0352866401313251e-15 }, { "depth": 2, "mixing": 0.0, "max_imaginary_frequency": 1.0550788041319055e-15 }, { "depth": 2, "mixing": 0.25, "max_imaginary_frequency": 0.6301917940761476 }, { "depth": 2, "mixing": 0.5, "max_imaginary_frequency": 1.295238830647337 }, { "depth": 2, "mixing": 0.75, "max_imaginary_frequency": 2.607891656691937 }, { "depth": 4, "mixing": -1.0, "max_imaginary_frequency": 1.054017984003508e-14 }, { "depth": 4, "mixing": -0.5, "max_imaginary_frequency": 7.087580878215172e-15 }, { "depth": 4, "mixing": 0.0, "max_imaginary_frequency": 1.9984014443252818e-14 }, { "depth": 4, "mixing": 0.25, "max_imaginary_frequency": 0.6301917940761607 }, { "depth": 4, "mixing": 0.5, "max_imaginary_frequency": 1.2952388306473486 }, { "depth": 4, "mixing": 0.75, "max_imaginary_frequency": 2.6078916566919483 }, { "depth": 6, "mixing": -1.0, "max_imaginary_frequency": 2.185751579730777e-14 }, { "depth": 6, "mixing": -0.5, "max_imaginary_frequency": 3.552713678800501e-14 }, { "depth": 6, "mixing": 0.0, "max_imaginary_frequency": 2.0872192862952943e-14 }, { "depth": 6, "mixing": 0.25, "max_imaginary_frequency": 0.6301917940761638 }, { "depth": 6, "mixing": 0.5, "max_imaginary_frequency": 1.2952388306473526 }, { "depth": 6, "mixing": 0.75, "max_imaginary_frequency": 2.6078916566919563 } ], "formula": "U=g sum_k h_k (Tr C_k^2-q Tr K_k^2); on a coherent constant-density upper field rho, omega_N=2g(1-q)rho D_N and the same law gives pair cross energy 2g rho sigma [r-q Tr(B_A B_B)] s^k.", "scope": "One quartic contact on an assumed constant-density, spatial zero-mode branch. No common physical compact geometry, self-consistent Q, spatial localization, cross-depth scale, or full stability has been derived." } }, "component_sha256": { "two-current-quartic-batch.py": "d57f4dcdce49fc41ed9a735ad9ef8e08dd9a90974453154d7c25c6212560b758", "two-current-tower.py": "b197a0ce401d30fe83e11ba7524daced4bc6ef7bc94e7a7c8a4eaba2cfc40309", "two-current-spatial-overlap.py": "e620efe597e54c51ef76a9bf64807ef9c05a44340fec45f9b4396a487bc6b014", "two-current-photon-control.py": "090fab27b49472522491a718699f830168053ca0061cd1cc7bf7e0c5708c9d9a", "two-current-grade-response.py": "eb1c0b98743afe1685ad3c44636bc8d20e71a2c159a2d2ccf1c86391171c170b", "unified-quartic-constant-density.py": "86b37844a7aac838405482f4535f5e0d370c1e843753b9e946edc75c87f4fa0a" }, "scope": "One comparison of smooth same-field quartic pair contact, full retained order-zero source, conditional displaced analytic cores, and a single-quartic constant-density self-mass branch. None derives the common physical carrier, cross-depth normalization, or complete stable mass operator.", "sources": { "experiments/two-current-quartic-batch.py": "d57f4dcdce49fc41ed9a735ad9ef8e08dd9a90974453154d7c25c6212560b758", "experiments/two-current-tower.py": "b197a0ce401d30fe83e11ba7524daced4bc6ef7bc94e7a7c8a4eaba2cfc40309", "experiments/two-current-spatial-overlap.py": "e620efe597e54c51ef76a9bf64807ef9c05a44340fec45f9b4396a487bc6b014", "experiments/two-current-photon-control.py": "090fab27b49472522491a718699f830168053ca0061cd1cc7bf7e0c5708c9d9a", "experiments/two-current-grade-response.py": "eb1c0b98743afe1685ad3c44636bc8d20e71a2c159a2d2ccf1c86391171c170b", "experiments/unified-quartic-constant-density.py": "86b37844a7aac838405482f4535f5e0d370c1e843753b9e946edc75c87f4fa0a", "experiments/two-current-decision-batch.py": "e7ffd1e1c45b5f3bc045808222b1fce232b925e5844692fe3c368117fab2b7cb", "experiments/localized_current_model.py": "bea8db856f55959328e92d99c089ed26db3b35e717533c67a14c9444d5f1a2e4", "experiments/localized_partner_tower.py": "4021f8ed6f4e0b77b7d53530503a23625bac6389a93eda7985d29852aeea2a5b", "experiments/graded_current_tower.py": "cf0f72cb6d078df086ec594550155d6518b00255ed46a16d669790edb093a602", "experiments/coherent_mode_algebra.py": "4fbcbb6a1fbaa5a1a7de387746eda4d00f69fe22bbdb1e906c8795f8bb786dff" } }