TFPT scientific source excerpt Original repository path: experiments/theory-contracts/mixed-current-origin-20261014/neutral-pairs-and-vector-wards-results.json Original file SHA-256: 3181894c8896cbdbfa2d6041ecbe1c6f21f6d41938d9b97f1cffddb92b415dad Inclusive original lines: 1-97 Line numbers below refer to the original source. This bounded excerpt is source evidence; it is not a new proof/checker run. Conversation metadata and personal execution details are omitted where indicated. 000001 | { 000002 | "date": "2026-10-22", 000003 | "verdict": "ORIGINAL_NEUTRAL_DEFECT_PAIR_CONSTRUCTED_NOT_SINGLE_SPINOR_SECTOR", 000004 | "register_grade": 0, 000005 | "global_cover_holonomy_changed": false, 000006 | "uniform_eight_sheet_interval_sign_exact": true, 000007 | "finite_band_factorization": [ 000008 | { 000009 | "occupied_modes_per_residue": 1, 000010 | "one_block_determinant": "0", 000011 | "full_expectation": "0" 000012 | }, 000013 | { 000014 | "occupied_modes_per_residue": 2, 000015 | "one_block_determinant": "-4/pi**2", 000016 | "full_expectation": "65536/pi**16" 000017 | }, 000018 | { 000019 | "occupied_modes_per_residue": 3, 000020 | "one_block_determinant": "0", 000021 | "full_expectation": "0" 000022 | }, 000023 | { 000024 | "occupied_modes_per_residue": 4, 000025 | "one_block_determinant": "256/(9*pi**4)", 000026 | "full_expectation": "18446744073709551616/(43046721*pi**32)" 000027 | } 000028 | ], 000029 | "finite_band_has_second_Fermi_edge": true, 000030 | "complement_determinant_controls": [ 000031 | { 000032 | "alpha": "1/4", 000033 | "exact": true, 000034 | "single_component_phase_nonzero": true 000035 | }, 000036 | { 000037 | "alpha": "3/4", 000038 | "exact": true, 000039 | "single_component_phase_nonzero": true 000040 | } 000041 | ], 000042 | "original_four_mark_central_forms": [ 000043 | "2*I", 000044 | "-2*I", 000045 | "0" 000046 | ], 000047 | "same_source_time_unitary_separation_energy_controls": [ 000048 | { 000049 | "return_width": "pi/8", 000050 | "H1_ramp_exact_DeltaK": "32", 000051 | "all_smooth_profiles_lower_bound": "16" 000052 | }, 000053 | { 000054 | "return_width": "pi/16", 000055 | "H1_ramp_exact_DeltaK": "48", 000056 | "all_smooth_profiles_lower_bound": "32" 000057 | }, 000058 | { 000059 | "return_width": "pi/32", 000060 | "H1_ramp_exact_DeltaK": "80", 000061 | "all_smooth_profiles_lower_bound": "64" 000062 | }, 000063 | { 000064 | "return_width": "pi/64", 000065 | "H1_ramp_exact_DeltaK": "144", 000066 | "all_smooth_profiles_lower_bound": "128" 000067 | } 000068 | ], 000069 | "actual_QWZ_full_covariance_controls": [ 000070 | { 000071 | "quarter_register_sector": 1, 000072 | "all_occupied_modes_retained": 256, 000073 | "left_right_edge_covariance_change": [ 000074 | 0.6445068385917867, 000075 | 0.6445068385917875 000076 | ], 000077 | "neutral_parity_expectation_real": 5.494331843494137e-27, 000078 | "neutral_parity_expectation_imag": 9.117879367472679e-44, 000079 | "global_seam_unchanged": true 000080 | }, 000081 | { 000082 | "quarter_register_sector": 3, 000083 | "all_occupied_modes_retained": 256, 000084 | "left_right_edge_covariance_change": [ 000085 | 0.6445068385917865, 000086 | 0.6445068385917873 000087 | ], 000088 | "neutral_parity_expectation_real": 5.49433184349402e-27, 000089 | "neutral_parity_expectation_imag": -6.189225609857311e-44, 000090 | "global_seam_unchanged": true 000091 | } 000092 | ], 000093 | "source_sha256": "5053d08ad5448f33f2c6d141f92ed1e06f5dfb9762f92af2bab9816c0ad161b8", 000094 | "infinite_determinant_or_continuum_limit_claimed": false, 000095 | "single_128_spinor_generators_constructed": false, 000096 | "physical_chiral_measure_selected": false 000097 | }