TFPT scientific source excerpt Original repository path: experiments/theory-contracts/tfpt-unified-source-derivation-20261029/aps_source_review/QUARTER-TOWER-HIGGS-INVERSE.json Original file SHA-256: f5e606f849a47a329b46bc1eb624ea058eb40ac1205562e76b839bc14ca47524 Inclusive original lines: 601-800 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. 000601 | "alpha": 0.75, 000602 | "n": 1, 000603 | "H": "(0j, 0j)", 000604 | "occupation": 0.9999999997185731 000605 | }, 000606 | { 000607 | "alpha": 0.75, 000608 | "n": 1, 000609 | "H": "(0.6j, (0.8+0j))", 000610 | "occupation": 0.8048867663244699 000611 | }, 000612 | { 000613 | "alpha": 0.75, 000614 | "n": 1, 000615 | "H": "(0j, (2+0j))", 000616 | "occupation": 0.6795151642099694 000617 | }, 000618 | { 000619 | "alpha": 0.75, 000620 | "n": 3, 000621 | "H": "(0j, 0j)", 000622 | "occupation": 1.0 000623 | }, 000624 | { 000625 | "alpha": 0.75, 000626 | "n": 3, 000627 | "H": "(0.6j, (0.8+0j))", 000628 | "occupation": 0.9275028805493829 000629 | }, 000630 | { 000631 | "alpha": 0.75, 000632 | "n": 3, 000633 | "H": "(0j, (2+0j))", 000634 | "occupation": 0.818033254729222 000635 | } 000636 | ], 000637 | "physical_Y_values_selected": false 000638 | }, 000639 | "cross_channel_original_diagnostics": [ 000640 | { 000641 | "p": "0.25", 000642 | "direct_original96": 0.6750624664140237, 000643 | "shared_law_prediction": 0.6750624664140236, 000644 | "new_Y_fit": false 000645 | }, 000646 | { 000647 | "p": "1.25", 000648 | "direct_original96": 0.8688558277780223, 000649 | "shared_law_prediction": 0.8688558277780223, 000650 | "new_Y_fit": false 000651 | } 000652 | ], 000653 | "original_free_source_reader": [ 000654 | { 000655 | "samples": 2, 000656 | "F_interval": [ 000657 | 0.8490193252646291, 000658 | 0.99627207622075 000659 | ], 000660 | "source": "actual given elliptic zero-H right complement", 000661 | "carrier_identity_is_hypothesis": true, 000662 | "positive_radial_law_forced": "delta_u0 only within this marked conditional identification" 000663 | }, 000664 | { 000665 | "samples": 4, 000666 | "F_interval": [ 000667 | 0.9551859835709214, 000668 | 0.99627207622075 000669 | ], 000670 | "source": "actual given elliptic zero-H right complement", 000671 | "carrier_identity_is_hypothesis": true, 000672 | "positive_radial_law_forced": "delta_u0 only within this marked conditional identification" 000673 | }, 000674 | { 000675 | "samples": 8, 000676 | "F_interval": [ 000677 | 0.9852243852852324, 000678 | 0.99627207622075 000679 | ], 000680 | "source": "actual given elliptic zero-H right complement", 000681 | "carrier_identity_is_hypothesis": true, 000682 | "positive_radial_law_forced": "delta_u0 only within this marked conditional identification" 000683 | } 000684 | ], 000685 | "finite_pairwise_bounds": [ 000686 | { 000687 | "samples_per_quarter": 1, 000688 | "occupation_pairwise_bound": "2/15" 000689 | }, 000690 | { 000691 | "samples_per_quarter": 2, 000692 | "occupation_pairwise_bound": "2/63" 000693 | }, 000694 | { 000695 | "samples_per_quarter": 8, 000696 | "occupation_pairwise_bound": "2/1023" 000697 | }, 000698 | { 000699 | "samples_per_quarter": 32, 000700 | "occupation_pairwise_bound": "2/16383" 000701 | }, 000702 | { 000703 | "samples_per_quarter": 1000, 000704 | "occupation_pairwise_bound": "2/15999999" 000705 | } 000706 | ], 000707 | "finite_source_reader_diagnostics": [ 000708 | { 000709 | "samples": 2, 000710 | "F_target": 0.36510529507925826, 000711 | "F_interval": [ 000712 | 0.3314863450726984, 000713 | 0.4094075912015353 000714 | ], 000715 | "occupation_interval": [ 000716 | 0.6657431725363492, 000717 | 0.7047037956007677 000718 | ], 000719 | "physical_law_selected": false 000720 | }, 000721 | { 000722 | "samples": 4, 000723 | "F_target": 0.36510529507925826, 000724 | "F_interval": [ 000725 | 0.35323063088106144, 000726 | 0.3708723399973492 000727 | ], 000728 | "occupation_interval": [ 000729 | 0.6766153154405307, 000730 | 0.6854361699986746 000731 | ], 000732 | "physical_law_selected": false 000733 | }, 000734 | { 000735 | "samples": 8, 000736 | "F_target": 0.36510529507925826, 000737 | "F_interval": [ 000738 | 0.3621577131817057, 000739 | 0.36611628701772386 000740 | ], 000741 | "occupation_interval": [ 000742 | 0.6810788565908529, 000743 | 0.683058143508862 000744 | ], 000745 | "physical_law_selected": false 000746 | }, 000747 | { 000748 | "samples": 16, 000749 | "F_target": 0.36510529507925826, 000750 | "F_interval": [ 000751 | 0.3643876108480452, 000752 | 0.36519957436954414 000753 | ], 000754 | "occupation_interval": [ 000755 | 0.6821938054240226, 000756 | 0.6825997871847721 000757 | ], 000758 | "physical_law_selected": false 000759 | } 000760 | ], 000761 | "exact_deconvolution": { 000762 | "original_radial_atoms": { 000763 | "0": "1/5", 000764 | "1/2": "1/4", 000765 | "7/3": "1/3", 000766 | "20/3": "13/60" 000767 | }, 000768 | "range": "30", 000769 | "recovered_nonzero_atoms": { 000770 | "0": "1/5", 000771 | "1/2": "1/4", 000772 | "7/3": "1/3", 000773 | "20/3": "13/60" 000774 | }, 000775 | "inferred_candidate_atoms": 57, 000776 | "physical_law_selected": false 000777 | }, 000778 | "noncompact_infinite_mean_diagnostic": [ 000779 | { 000780 | "p": "0.25", 000781 | "F": 0.15062715326130818, 000782 | "finite_mean_assumed": false 000783 | }, 000784 | { 000785 | "p": "1.25", 000786 | "F": 0.4993122050904376, 000787 | "finite_mean_assumed": false 000788 | } 000789 | ], 000790 | "R062_extra_mode_discrepancy": 2.1843012276435023e-05, 000791 | "finite_prefix_counterexample": { 000792 | "modes": [ 000793 | "0.25", 000794 | "1.25" 000795 | ], 000796 | "common_radial_support": [ 000797 | "0.0", 000798 | "0.25", 000799 | "1.0", 000800 | "4.0"