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• The Exchange-Odd Majorana Order Parameter Has an Exact Global Kink, but No Wall if Exchange Is Weyl Gaugecorpus/claims/0700-0799/700_the_exchange_odd_majorana_order_parameter_has_an_exact_global_kink_but_no_wall_if_exchange_is_weyl_gauge.md · wider corpus
• Polarizing the Rank-Three Jordan Cubic Along the Discarded Face Gives the Spin(2,3) Rank-Two Determinantcorpus/claims/0700-0799/701_polarizing_the_rank_three_jordan_cubic_along_the_discarded_face_gives_the_spin23_rank_two_determinant.md · wider corpus
• The Exceptional Jordan Cubic Polarizes to H₂(O) and Reaches Spin(2,3) Only on the G₂-Fixed Real Slicecorpus/claims/0700-0799/702_the_exceptional_jordan_cubic_polarizes_to_h2o_and_reaches_spin23_only_on_the_g2_fixed_real_slice.md · wider corpus
• An Eight-Element Octonion-Automorphism Twirl Is a CP Dilation of the H₂(O)to H₂(R) Selectorcorpus/claims/0700-0799/703_an_eight_element_octonion_automorphism_twirl_is_a_cp_dilation_of_the_h2o_to_h2r_selector.md · wider corpus
• The Finite G₂ Selector Fixed Algebra Is Eight M₂ Blocks, and Symmetry Alone Cannot Synchronize Themcorpus/claims/0700-0799/704_the_finite_g2_selector_fixed_algebra_is_eight_m2_blocks_and_symmetry_alone_cannot_synchronize_them.md · wider corpus
• The Exceptional Cubic Does Not by Itself Fix the Transverse Synchronization Gapcorpus/claims/0700-0799/705_the_exceptional_cubic_does_not_by_itself_fix_the_transverse_synchronization_gap.md · wider corpus
• A Clifford-Multiplicity Conditional Expectation Exactly Selects H₂(R) Without the G₂ Fixed-Range Excesscorpus/claims/0700-0799/706_a_clifford_multiplicity_conditional_expectation_exactly_selects_h2r_without_the_g2_fixed_range_excess.md · wider corpus
• A Six-Jump Clifford Lindbladian Converges to H₂(R) with an Exact Gap, but Must Not Depolarize the Same Facecorpus/claims/0700-0799/707_a_six_jump_clifford_lindbladian_converges_to_h2r_with_exact_gap_but_must_not_depolarize_the_same_face.md · wider corpus
• The Topology Face and Clifford Carrier Must Be Separately Typed or the Joint Selector Collapses to Scalarscorpus/claims/0700-0799/708_the_topology_face_and_clifford_carrier_must_be_separately_typed_or_the_joint_selector_collapses_to_scalars.md · wider corpus
• Furey’s SU(3) Stabilizer Leaves a Circle of Clifford Response Lines Until Conjugation Parity Selects an Axiscorpus/claims/0700-0799/709_fureys_su3_stabilizer_leaves_a_circle_of_clifford_response_lines_until_conjugation_parity_selects_an_axis.md · wider corpus
• The Furey-Odd Imaginary Axis Also Has an Exact CP H₂(R) Selector, So Positivity Does Not Choose the Axiscorpus/claims/0700-0799/710_the_furey_odd_imaginary_axis_also_has_an_exact_cp_h2r_selector_so_positivity_does_not_choose_the_axis.md · wider corpus
• Symmetric Stress Cannot Linearly Source a Spacetime Pseudoscalar in a Lorentz-Invariant Vacuum, but Furey-Odd Is Not Yet Spacetime-Oddcorpus/claims/0700-0799/711_symmetric_stress_cannot_linearly_source_a_spacetime_pseudoscalar_in_a_lorentz_invariant_vacuum_but_furey_odd_is_not_yet_spacetime_odd.md · wider corpus
• A Mixed Clifford Response Line Has a Projective CP-Odd Invariant and Requires an Odd Cross-Kernelcorpus/claims/0700-0799/712_a_mixed_clifford_response_line_has_a_projective_cp_odd_invariant_and_requires_an_odd_cross_kernel.md · wider corpus
• The Higgs/Yukawa-Dressed Exchange Is Linear, Not an Antiunitary, and Does Not Select Clifford Response Paritycorpus/claims/0700-0799/713_the_higgs_yukawa_dressed_exchange_is_linear_not_an_antiunitary_and_does_not_select_clifford_response_parity.md · wider corpus
• The Standard-Model Color Module Is Two Complexified-Octonion Copies, but Not in the Prakash–Ramya Dirac-Face Factorizationcorpus/claims/0700-0799/714_the_standard_model_color_module_is_two_complexified_octonion_copies_but_not_in_the_prakash_ramya_dirac_face_factorization.md · wider corpus
• Electroweak Breaking and the Higgs Frame Select Two Crossed Octonion-Shaped Generation Modulescorpus/claims/0700-0799/715_electroweak_breaking_and_the_higgs_frame_select_two_crossed_octonion_shaped_generation_modules.md · wider corpus
• Channel-Local Hermitian Yukawa Kernels Align on the Even Clifford Axis, While CP-Odd Misalignment Requires Cross-Channel Flavor Datacorpus/claims/0700-0799/716_channel_local_hermitian_yukawa_kernels_align_on_the_even_clifford_axis_while_cp_odd_misalignment_requires_cross_channel_flavor_data.md · wider corpus
• A Majorana CP Invariant Exists with Two Families and Generically Misaligns the Up/Neutral Response If It Matches the Odd Axiscorpus/claims/0700-0799/717_a_majorana_cp_invariant_exists_with_two_families_and_generically_misaligns_the_up_neutral_response_if_it_matches_the_odd_axis.md · wider corpus
• The Majorana Alignment Obstruction Requires a Charged-Lepton Weak-Basis Invariant and Is High Spurion Ordercorpus/claims/0700-0799/718_the_majorana_alignment_obstruction_requires_a_charged_lepton_weak_basis_invariant_and_is_high_spurion_order.md · wider corpus
• A CP-Odd Flavor Spurion Conditionally Reopens the Vacuum Stress Odd Response, but Does Not Supply the Furey Parity Intertwinercorpus/claims/0700-0799/719_a_cp_odd_flavor_spurion_conditionally_reopens_the_vacuum_stress_odd_response_but_does_not_supply_the_furey_parity_intertwiner.md · wider corpus
• The Lowest-Dimension CP-Odd Response Sources Form a Gauge, Phase and Metric-Relevance Laddercorpus/claims/0700-0799/720_the_lowest_dimension_cp_odd_response_sources_form_a_gauge_phase_and_metric_relevance_ladder.md · wider corpus
• The Majorana Weak-Basis Word Is One Nambu TRO Compression, but Not an Internal Product of the Bare Furey Matter TROcorpus/claims/0700-0799/721_the_majorana_weak_basis_word_is_one_nambu_tro_compression_but_not_an_internal_product_of_the_bare_furey_matter_tro.md · wider corpus
• CP Equivariance Uniquely Sends One Odd Flavor Scalar to the Odd Response Axis, but Unbroken Response (Spin(2)) Forces the Map to Zerocorpus/claims/0700-0799/722_cp_equivariance_uniquely_sends_one_odd_flavor_scalar_to_the_odd_response_axis_but_unbroken_response_spin2_forces_the_map_to_zero.md · wider corpus
• The Fixed-Carrier (Spin(2)) and the Response-Embedding Selector (Spin(2)) Are Distinct, and Furey Conjugation Breaks Only the Lattercorpus/claims/0700-0799/723_the_fixed_carrier_spin2_and_the_response_embedding_selector_spin2_are_distinct_and_furey_conjugation_breaks_only_the_latter.md · wider corpus
• A Minimal CP-Spurion Kernel Generically Removes the Selector Circle and Gives the Response Angle a Calculable Curvaturecorpus/claims/0700-0799/724_a_minimal_cp_spurion_kernel_generically_removes_the_selector_circle_and_gives_the_response_angle_a_calculable_curvature.md · wider corpus
• The Full Complex Majorana Trace Supplies a Canonical CP-Even/Odd Pair with Selector Weight Twocorpus/claims/0700-0799/725_the_full_complex_majorana_trace_supplies_a_canonical_cp_even_odd_pair_with_selector_weight_two.md · wider corpus
• CP Equivariance Allows Two Response Coefficients, While the Furey Complex Structure Selects a Canonical Common-Coefficient Raycorpus/claims/0700-0799/726_cp_equivariance_allows_two_response_coefficients_while_the_furey_complex_structure_selects_a_canonical_common_coefficient_ray.md · wider corpus
• The Hermitian Exchanged TRO Is State-Phase Blind and Can Transport (Z₂) Only Through a Separately Typed Complex Probecorpus/claims/0700-0799/727_the_hermitian_exchanged_tro_is_state_phase_blind_and_can_transport_z2_only_through_a_separately_typed_complex_probe.md · wider corpus
• A Complex Probe Cannot Map Nontrivially and Completely Positively Directly to Hermitian Observables, but Its Minimal Two-Quadrature Lift Is (H₂(R))corpus/claims/0700-0799/728_a_complex_probe_cannot_map_nontrivially_and_completely_positively_directly_to_hermitian_observables_but_its_minimal_two_quadrature_lift_is_h2r.md · wider corpus
• Half the Trace of a Positive Two-Probe Spectral Gram Is the Canonical Carrier Coordinate, but (Z₂) Matching Remains a Form-Factor Gatecorpus/claims/0700-0799/729_half_the_trace_of_a_positive_two_probe_spectral_gram_is_the_canonical_carrier_coordinate_but_z2_matching_remains_a_form_factor_gate.md · wider corpus
• (Z₂) Matching to a Full Stress Spectral Kernel Requires Dimension (-4) and at Least Four Majorana Plus Four Charged-Lepton Mass Insertionscorpus/claims/0700-0799/730_z2_matching_to_a_full_stress_spectral_kernel_requires_dimension_minus_four_and_at_least_four_majorana_plus_four_charged_lepton_mass_insertions.md · wider corpus
• (I₂) Is the Lowest-Degree CP-Odd Single Trace in the Standard (H_ell,H_nu,G_ellnu) Covariant Algebra, So That Shortcut Is Closedcorpus/claims/0700-0799/731_i2_is_the_lowest_degree_cp_odd_single_trace_in_the_standard_hl_hnu_glnu_covariant_algebra_so_that_shortcut_is_closed.md · wider corpus
• A Two-Flavor LNV Amplitude Quartet Is the Minimal Rephasing-Invariant Majorana-CP Observable and Avoids Charged-Lepton Mass Spurionscorpus/claims/0700-0799/732_a_two_flavor_lnv_amplitude_quartet_is_the_minimal_rephasing_invariant_majorana_cp_observable_and_avoids_charged_lepton_mass_spurions.md · wider corpus
• A Two-Copy LNV Interferometer Embeds the Minimal Majorana-CP Quartet in a Positive (H₂(R)) Carriercorpus/claims/0700-0799/733_a_two_copy_lnv_interferometer_embeds_the_minimal_majorana_cp_quartet_in_a_positive_h2r_carrier.md · wider corpus
• The Four-Mode Majorana Pfaffian Contains the Quartet Interference, but a CP Rate Asymmetry Needs a Relative Kinematic Phasecorpus/claims/0700-0799/734_the_four_mode_majorana_pfaffian_contains_the_quartet_interference_but_a_cp_rate_asymmetry_needs_a_relative_kinematic_phase.md · wider corpus
• Pairing Exchange Can Cancel the Inclusive Majorana-Quartet Asymmetry, While a Signed Differential Moment Restores Itcorpus/claims/0700-0799/735_pairing_exchange_can_cancel_the_inclusive_majorana_quartet_asymmetry_while_a_signed_differential_moment_restores_it.md · wider corpus
• The Optimal Exchange-Odd Observable Is the CP Score and Recovers All Local Information Lost by the Inclusive Ratecorpus/claims/0700-0799/736_the_optimal_exchange_odd_observable_is_the_cp_score_and_recovers_all_local_information_lost_by_the_inclusive_rate.md · wider corpus
• An Unpolarized Spin Trace Can Erase the Majorana-Quartet Interference, While Polarization Restores It Unless the Paths Are Operator-Orthogonalcorpus/claims/0700-0799/737_an_unpolarized_spin_trace_can_erase_the_majorana_quartet_interference_while_polarization_restores_it_unless_the_paths_are_operator_orthogonal.md · wider corpus
• The Efficient CP Score Is the Nuisance-Orthogonal Jordan Tangent, and Its Schur Complement Is the Identifiability Testcorpus/claims/0700-0799/738_the_efficient_cp_score_is_the_nuisance_orthogonal_jordan_tangent_and_its_schur_complement_is_the_identifiability_test.md · wider corpus
• Detector Folding Is a Positive Markov Compression That Can Only Contract CP Fisher Informationcorpus/claims/0700-0799/739_detector_folding_is_a_positive_markov_compression_that_can_only_contract_cp_fisher_information.md · wider corpus
• Two Reversed Measurement Faces Can Break an Exact Single-Face CP–Acceptance Degeneracycorpus/claims/0700-0799/740_two_reversed_measurement_faces_can_break_an_exact_single_face_cp_acceptance_degeneracy.md · wider corpus
• Imperfect Face Reversal Remains Identifying Except at the Same-Sign Boundary, but Can Be Arbitrarily Ill-Conditionedcorpus/claims/0700-0799/741_imperfect_face_reversal_remains_identifying_except_at_the_same_sign_boundary_but_can_be_arbitrarily_ill_conditioned.md · wider corpus
• A Binary Pairing-Orientation Tag Retains the Square of Its Dilution in CP Fisher Informationcorpus/claims/0700-0799/742_a_binary_pairing_orientation_tag_retains_the_square_of_its_dilution_in_cp_fisher_information.md · wider corpus
• Multi-Face CP Identifiability Is a Design-Matrix Rank Problem and Requires a Direction Outside the Nuisance Spancorpus/claims/0700-0799/743_multiface_cp_identifiability_is_a_design_matrix_rank_problem_and_requires_a_direction_outside_the_nuisance_span.md · wider corpus
• The Two-Score Fisher Gram Is Exactly an H₂(R) Lorentz Cone, but Its Spin Group Is Spin₀(2,1), Not Spin₀(2,3)corpus/claims/0700-0799/744_the_two_score_fisher_gram_is_exactly_an_h2r_lorentz_cone_but_its_spin_group_is_spin21_not_spin23.md · wider corpus
• The Primitive Two-Forms of a Symplectic Four-Space Give the Genuine Five-Dimensional Spin₀(2,3) Modulecorpus/claims/0700-0799/745_the_primitive_two_forms_of_a_symplectic_four_space_give_the_genuine_five_dimensional_spin23_module.md · wider corpus
• An H₂(R) Carrier Embeds as a Signature-(1,2) Section of the Spin(2,3) Module but Leaves a Six-Parameter Embedding Degeneracycorpus/claims/0700-0799/746_an_h2r_carrier_embeds_as_a_signature12_section_of_the_spin23_module_but_leaves_a_six_parameter_embedding_degeneracy.md · wider corpus
• The Six Missing Spin(2,3) Generators Are Three Rotations and Three Boosts with Explicit Sp(4,R) Liftscorpus/claims/0700-0799/747_the_six_missing_spin23_generators_are_three_rotations_and_three_boosts_with_explicit_sp4_lifts.md · wider corpus
• The TKK Algebra Already Induces All Spin(2,3) Directions, and the Jordan Carrier Embeds Projectively in the Null Conecorpus/claims/0700-0799/748_the_tkk_algebra_already_induces_all_spin23_directions_and_the_jordan_carrier_embeds_projectively_in_the_null_cone.md · wider corpus
• The B-L Ward-Compatible Algebra Preserves a Maximal Null Plane and Is Affine, Not Full Spin(2,3)corpus/claims/0700-0799/749_the_bl_ward_compatible_algebra_preserves_a_maximal_null_plane_and_is_affine_not_full_spin23.md · wider corpus
• Majorana Breaking Enlarges the Fixed-Data Remnant from a Null-Plane Translation Algebra to a Null-Line Euclidean Algebra, Not Spin(2,3)corpus/claims/0700-0799/750_majorana_breaking_enlarges_the_fixed_data_remnant_from_a_null_plane_translation_algebra_to_a_null_line_euclidean_algebra_not_spin23.md · wider corpus
• Adjoining the Majorana-Breaking Channel Creates an H₃(C) Carrier Fork, and Spin(2,3) Returns Only After Two Independent Selectorscorpus/claims/0700-0799/751_adjoining_the_majorana_breaking_channel_creates_an_h3c_carrier_fork_and_spin23_returns_only_after_two_independent_selectors.md · wider corpus
• The Two-Stage Majorana Selector Has an Additive Finite-Gap, Coherence and Exchange Error Budgetcorpus/claims/0700-0799/752_the_two_stage_majorana_selector_has_an_additive_finite_gap_coherence_and_exchange_error_budget.md · wider corpus
• The H₂ Determinant Is the Exact Normal and Schur Residue of the H₃(C) Cubic Normcorpus/claims/0700-0799/753_the_h2_determinant_is_the_exact_normal_and_schur_residue_of_the_h3c_cubic_norm.md · wider corpus
• The Albert Cubic Normal Residue Is the H₂(O) Lorentz Norm, Not Directly the Spin(2,3) H₂(R) Normcorpus/claims/0700-0799/754_the_albert_cubic_normal_residue_is_the_h2o_lorentz_norm_not_directly_the_spin23_h2r_norm.md · wider corpus
• arXiv:2610.21879v1 Re-entry Audit and Current-Frontier Mapcorpus/claims/0700-0799/755_arxiv_2610_21879v1_reentry_audit_and_current_frontier_map.md · wider corpus
• The S₅ Puncture Cubic Lives on the Trivial Line and Cannot Symplectically Pair the Standard Four-Modulecorpus/claims/0700-0799/756_the_s5_puncture_cubic_lives_on_the_trivial_line_and_cannot_symplectically_pair_the_standard_four_module.md · wider corpus
• Only Four Subgroup Types of S₅ Make the Standard Four-Module Symplectic, and the Color/Weak Stabilizer Is Not Onecorpus/claims/0700-0799/757_only_four_subgroup_types_of_s5_make_the_standard_four_module_symplectic_and_the_color_weak_stabilizer_is_not_one.md · wider corpus
• The Higgs Crossed-Octonion Partition Reduces S₅ to S₄, or Physical S₃, but Still Does Not Select a Symplectic Four-Carriercorpus/claims/0700-0799/758_the_higgs_crossed_octonion_partition_reduces_s5_to_s4_or_physical_s3_but_still_does_not_select_a_symplectic_four_carrier.md · wider corpus
• Oriented Color C₃ Gives a Two-Area Symplectic Family, and Color Reflection Becomes Anti-Symplectic Only When Paired with Weak Exchangecorpus/claims/0700-0799/759_oriented_color_c3_gives_a_two_area_symplectic_family_and_color_reflection_becomes_antisymplectic_only_when_paired_with_weak_exchange.md · wider corpus
• Signed Color/Weak Covariance Uniquely Selects the Color-Average Index-Three Unimodular Overlattice—Conditional on Equal Areascorpus/claims/0700-0799/760_signed_color_weak_covariance_uniquely_selects_the_color_average_index_three_unimodular_overlattice_conditional_on_equal_areas.md · wider corpus
• The Color-Average Completion Has Canonical Sp(4,Z) Form and Primitive Lattice U⊕ U⊕langle-2rangle with Signed O(2,3) Actioncorpus/claims/0700-0799/761_the_color_average_completion_has_canonical_sp4z_form_and_primitive_lattice_u_plus_u_plus_minus2_with_signed_o23_action.md · wider corpus
• Modulo Three, the Color-Average Carrier Is an Abstract Two-Qutrit Pauli Phase Space, but No Field-Labelled Intertwiner Is Yet Selectedcorpus/claims/0700-0799/762_modulo_three_the_color_average_carrier_is_an_abstract_two_qutrit_pauli_phase_space_but_no_field_labelled_intertwiner_is_yet_selected.md · wider corpus
• The Physical Color Cycle Acts Trivially on Two-Puncture Code Logicals but Unipotently on the Arithmetic Carrier, So No Equivariant Identification Existscorpus/claims/0700-0799/763_the_physical_color_cycle_acts_trivially_on_two_puncture_code_logicals_but_unipotently_on_the_arithmetic_carrier_so_no_equivariant_identification_exists.md · wider corpus
• Pure D₅ Weyl Puncture Motion Has Only Identity or Swap Transport and Cannot Realize the Order-Three Carrier Color Cyclecorpus/claims/0700-0799/764_pure_d5_weyl_puncture_motion_has_only_identity_or_swap_transport_and_cannot_realize_the_order_three_carrier_color_cycle.md · wider corpus
• The Carrier Color Unipotent Is Exactly a One-Handle Inverse-Twist/Fourier Word—not a Microscopic Color Permutation or Mutual Gatecorpus/claims/0700-0799/765_the_carrier_color_unipotent_is_exactly_a_one_handle_inverse_twist_fourier_word_not_a_microscopic_color_permutation_or_mutual_gate.md · wider corpus
• Integral Handle Exchange Forces Equal or Opposite Carrier Areas but Is Not a Microscopic S₅ Symmetrycorpus/claims/0700-0799/766_integral_handle_exchange_forces_equal_or_opposite_carrier_areas_but_is_not_a_microscopic_s5_symmetry.md · wider corpus
• The Sewn Furey Ribbon Has Untyped Handle Exchange but No Standard-Model-Typed Exchange Between C and Dcorpus/claims/0700-0799/767_the_sewn_furey_ribbon_has_untyped_handle_exchange_but_no_standard_model_typed_exchange_between_c_and_d.md · wider corpus
• Left–Right Symmetry Is the Minimal Gauge Envelope of the Furey Handle Exchange, but Equal Area Requires an Invariant Response Phasecorpus/claims/0700-0799/768_left_right_symmetry_is_the_minimal_gauge_envelope_of_the_furey_handle_exchange_but_equal_area_requires_an_invariant_response_phase.md · wider corpus
• An Intertwined Left–Right Response Forces Equal Handle Areas in the Symmetric Phase but Allows Odd-Spurion Splittingcorpus/claims/0700-0799/769_an_intertwined_left_right_response_forces_equal_handle_areas_in_the_symmetric_phase_but_allows_odd_spurion_splitting.md · wider corpus
• Oriented Color, Signed Reflection and Left–Right Handle Exchange Select a Unique Full Symplectic Line with No Mixed-Block Loopholecorpus/claims/0700-0799/770_oriented_color_signed_reflection_and_left_right_handle_exchange_select_a_unique_full_symplectic_line_with_no_mixed_block_loophole.md · wider corpus
• The Three Carrier Selectors Generate a Hyperbolic Infinite-Order Word, so No Positive Unitary Matter Intertwiner Can Realize Them Allcorpus/claims/0700-0799/771_the_three_carrier_selectors_generate_a_hyperbolic_infinite_order_word_so_no_positive_unitary_matter_intertwiner_can_realize_them_all.md · wider corpus
• The Hyperbolic Selector Word Is a Reducible Pair of Trace-Three Handle Maps with Golden-Ratio-Squared Stretchcorpus/claims/0700-0799/772_the_hyperbolic_selector_word_is_a_reducible_pair_of_trace_three_handle_maps_with_golden_ratio_squared_stretch.md · wider corpus
• The Shortest Coupled Selector Word Uses the Unique Qutrit Mutual Shear and Has an Irreducible Partially Hyperbolic Quarticcorpus/claims/0700-0799/773_the_shortest_coupled_selector_word_uses_the_unique_qutrit_mutual_shear_and_has_an_irreducible_partially_hyperbolic_quartic.md · wider corpus
• The Shortest Fully Hyperbolic Coupled Word Has an Irreducible Quartic and a One-Plus-Two-Reciprocal-Pair Spin(2,3) Spectrumcorpus/claims/0700-0799/774_the_shortest_fully_hyperbolic_coupled_word_has_an_irreducible_quartic_and_a_one_plus_two_reciprocal_pair_spin23_spectrum.md · wider corpus
• The Fully Hyperbolic Selector Fixes a Negative-Norm Primitive Axis and Splits Its Orthogonal Complement into Two Boost Planescorpus/claims/0700-0799/775_the_fully_hyperbolic_selector_fixes_a_negative_norm_primitive_axis_and_splits_its_orthogonal_complement_into_two_boost_planes.md · wider corpus
• The Fully Hyperbolic Selector Requires Active Squeezing as a Canonical Step but Can Still Be a Passive Flux Transfer Matrixcorpus/claims/0700-0799/776_the_fully_hyperbolic_selector_requires_active_squeezing_as_a_canonical_step_but_can_still_be_a_passive_flux_transfer_matrix.md · wider corpus
• Complex Polarization Turns the Hyperbolic Symplectic Word into Pseudo-Unitary Transfer and Unitary Scattering, but the Spatial Real Structure Is the Gatecorpus/claims/0700-0799/777_complex_polarization_turns_the_hyperbolic_symplectic_word_into_pseudo_unitary_transfer_and_unitary_scattering_but_the_spatial_real_structure_is_the_gate.md · wider corpus
• The Furey Survivor Exchange Has Exactly the Spatial Flux-Reversal Real Structure but Preserves the Sewn Meridian Planecorpus/claims/0700-0799/778_the_furey_survivor_exchange_has_exactly_the_spatial_flux_reversal_real_structure_but_preserves_the_sewn_meridian_plane.md · wider corpus
• Handle, Survivor, Propagation and Nambu Are Four Distinct Binary Indices Whose Real Structures Can Leave Exactly Four Real Carrier Dimensionscorpus/claims/0700-0799/779_handle_survivor_propagation_and_nambu_are_four_distinct_binary_indices_whose_real_structures_can_leave_exactly_four_real_carrier_dimensions.md · wider corpus
• The Selected Unitary Scattering Checkpoint Embeds in a Reciprocal Rational Inner Response with Positive-Real Cayley Impedancecorpus/claims/0700-0799/780_the_selected_unitary_scattering_checkpoint_embeds_in_a_reciprocal_rational_inner_response_with_positive_real_cayley_impedance.md · wider corpus
• A Sideband-Exchange Real Structure Gives the Complex Scattering Checkpoint a Real-Time Reciprocal Passive Completioncorpus/claims/0700-0799/781_a_sideband_exchange_real_structure_gives_the_complex_scattering_checkpoint_a_real_time_reciprocal_passive_completion.md · wider corpus
• One Scattering Checkpoint Cannot Identify Furey Thresholds or Positive Residues When Hermitian Contact Terms Are Freecorpus/claims/0700-0799/782_one_scattering_checkpoint_cannot_identify_furey_thresholds_or_positive_residues_when_hermitian_contact_terms_are_free.md · wider corpus
• Scalar Dressing Forces Coherent Relational Residue Channels and Cannot Supply Nontrivial Coordinate-Local Furey Residuescorpus/claims/0700-0799/783_scalar_dressing_forces_coherent_relational_residue_channels_and_cannot_supply_nontrivial_coordinate_local_furey_residues.md · wider corpus
• All Four Scattering Eigenchannels Are Rank-One Relational Superpositions Touching Both Handles and Both Boundary Sidescorpus/claims/0700-0799/784_all_four_scattering_eigenchannels_are_rank_one_relational_superpositions_touching_both_handles_and_both_boundary_sides.md · wider corpus
• The Scattering Eigenchannel Quartet Is Not an Equivariant Permutation Copy of the Furey u,d,e,nu Gridcorpus/claims/0700-0799/785_the_scattering_eigenchannel_quartet_is_not_an_equivariant_permutation_copy_of_the_furey_udenu_grid.md · wider corpus
• Oriented Color and Handle Exchange Generate C₃× S₃, and the Hyperbolic Checkpoint Has a Regular 18-Background Spurion Orbitcorpus/claims/0700-0799/786_oriented_color_and_handle_exchange_generate_c3_times_s3_and_the_hyperbolic_checkpoint_has_a_regular_18_background_spurion_orbit.md · wider corpus
• Flux Reversal Does Not Normalize the Finite Selector Torsor, and Its Adjunction Generates an Infinite Hyperbolic Extensioncorpus/claims/0700-0799/787_flux_reversal_does_not_normalize_the_finite_selector_torsor_and_its_adjunction_generates_an_infinite_hyperbolic_extension.md · wider corpus
• The 18-Background Torsor Is Exactly Three Framed Matter Pairings Times a Central Three-Phase, but the Physical Source Map Is Opencorpus/claims/0700-0799/788_the_18_background_torsor_is_exactly_three_framed_matter_pairings_times_a_central_three_phase_but_the_physical_source_map_is_open.md · wider corpus
• Standard-Model Typing Uniquely Selects the Furey Double-Transversal Pairing and Leaves at Most a Six-Point Selector Stratumcorpus/claims/0700-0799/789_standard_model_typing_uniquely_selects_the_furey_double_transversal_pairing_and_leaves_at_most_a_six_point_selector_stratum.md · wider corpus
• The Central Selector (C₃) Is Not the Primitive Mutual Shear Even Modulo Three and Cannot Yet Be Called Framingcorpus/claims/0700-0799/790_the_central_selector_c3_is_not_the_primitive_mutual_shear_even_modulo_three_and_cannot_yet_be_called_framing.md · wider corpus
• Typed Coordinate Potapov Factors Preserve the Checkpoint, Passivity, Reciprocity and Reality, but Their Cayley Residues Remain Relationalcorpus/claims/0700-0799/791_typed_coordinate_potapov_factors_preserve_the_checkpoint_passivity_reciprocity_and_reality_but_their_cayley_residues_remain_relational.md · wider corpus
• Checkpoint Spectral Projectors Give an Explicit Positive Rank-One Relational-Residue Model, but Not Furey Typing or Threshold Predictioncorpus/claims/0700-0799/792_checkpoint_spectral_projectors_give_an_explicit_positive_rank_one_relational_residue_model_but_not_furey_typing_or_threshold_prediction.md · wider corpus
• Fixed UV Data and Known Poles Turn Residue Recovery into a Cauchy-Rank Problem with an Exact Minimum-Data Theoremcorpus/claims/0700-0799/793_fixed_uv_and_known_poles_turn_residue_recovery_into_a_cauchy_rank_problem_with_an_exact_minimum_data_theorem.md · wider corpus
• 2n Moments Generically Recover n Positive Thresholds and Weights per Coherent Channel, while 2n-1 Do Notcorpus/claims/0700-0799/794_two_n_moments_generically_recover_n_positive_thresholds_and_weights_per_coherent_channel_while_two_n_minus_one_do_not.md · wider corpus
• Vacuum Total Stress Has at Most Two Nonlocal Form-Factor Moments and Cannot Tomograph Four Relational Projector Channelscorpus/claims/0700-0799/795_vacuum_total_stress_has_at_most_two_nonlocal_form_factor_moments_and_cannot_tomograph_four_relational_projector_channels.md · wider corpus
• Four Higgs-Dressed Yukawa Gram Sources Can Supply Rank-Four Tomography Only in the nu_R-Completed Branchcorpus/claims/0700-0799/796_four_higgs_dressed_yukawa_gram_sources_can_supply_rank_four_tomography_only_in_the_nu_right_completed_branch.md · wider corpus
• Positive Unital Source-to-Projector Maps Reduce to 24 Order Isomorphisms, but Regular-Torsor Covariance Selects Nonecorpus/claims/0700-0799/797_positive_unital_source_to_projector_maps_reduce_to_24_order_isomorphisms_but_regular_torsor_covariance_selects_none.md · wider corpus
• The Checkpoint Projectors Form a Handle-by-Side Bias Square Matching the Furey Handle-by-Channel Square up to One Global Reversalcorpus/claims/0700-0799/798_the_checkpoint_projectors_form_a_handle_by_side_bias_square_matching_the_furey_handle_by_channel_square_up_to_one_global_reversal.md · wider corpus
• The Handle-by-Side Bias Square Survives All 18 Selector Backgrounds and Globally Labels the Discrete Eigenbundlecorpus/claims/0700-0799/799_the_handle_by_side_bias_square_survives_all_18_selector_backgrounds_and_globally_labels_the_discrete_eigenbundle.md · wider corpus