{"claim_boundary":{"prohibited":["Hardware performance, flight readiness, a new field, reactionless thrust or evidence that Pathfinder is buildable.","Independent external replication, unseen-data confirmation, statistical significance or general continuum convergence.","Fixed electrical power or fixed radiated power: each prescribed source has unit integrated amplitude and phases can change emitted energy."],"supported":["If primary obligations pass, bounded reproducibility of phase-steered radiation recoil and conservation for the exact frozen prescribed-source scalar model and ten cases."]},"cohort":{"exclusion":["The coarser exploratory rows remain qualification diagnostics and are not silently included as primary successes.","No post-freeze additions, dropped rows, adaptive refinement, changed inputs or result-based retry.","Orthogonal-channel cancellation remains a periodic qualification control; no transient multi-channel primary claim is made."],"inclusion":["Exactly the ten ordered scenarios in the identified scalar contract, each once after successful qualification.","All six base width/phase cases and both forward time/domain controls are required."],"scenario_ids":["PF-S-001","PF-S-002","PF-S-003","PF-S-004","PF-S-005","PF-S-006","PF-S-007","PF-S-008","PF-S-009","PF-S-010"]},"contract_identity":"sha256:aabb1809d1bce58f5b92bea5cb38329cb2ed23554908b1d5d3f57e3367f4e31f","hypotheses":{"primary":"Both source widths produce negative forward and positive reversed integrated reaction with magnitude at least 0.01 model momentum units, an in-phase null, and complete conservation and independent-reference checks within the registered limits.","secondary":["The selected source representation meets separate 0.1% energy and non-null reaction allocations without cancellation against field propagation error.","The registered half-time-step and enlarged-domain forward comparisons satisfy their paired limits. Monotonic convergence is not required or claimed."]},"id":"TT/PF-001","input_identities":["sha256:73173ff5693ad623564ab6f2bf8ad731b36ca32917f16208b395ec286088514d","sha256:d7125b5c67a2731b7389fbfb3e34275829831391ada1713d862979744ed92163","sha256:bc8909d6132208cd0916dcc3c81203dc7430d2bdd3e4f51df02c57c79c550aed","sha256:736699197cc4796a8ee318c5714dcfe4b380faff27cb8a76778d77fedb3b5749","sha256:565430a82b27b3b41e588e7f1a71eeac295f74a7351e3c34b2c149772f9691ee","sha256:66eaf456ff800e95fcd017a84c3fd40fe94a197cd4b9faaac433bef69526b8ee","sha256:495fa379960f68814a62fee4df1ee85f6bb56560ac73852d65cdd8d83a26121e","sha256:c02dad4ad84cb793f75456f106603136b3770c54bc96498f32bc1646bdba33a5","sha256:b370c4d41064751b15fe82ed63a2481ac5dcd8ce35a7d2741d757a9f7d364ecb","sha256:792e72741b8edff0b6e89a53b598bc7b9af53ec2819828816a68abc6274da607","sha256:1460d45c19bdef698c665d24315355c6e5c7377353b624c7ec9908648cdfdb84","sha256:00ba766bd1732421120b10b32fa3616ec30e1725a0ea525b0dd4a0725cf93b26","sha256:9a1ac6ac92a1b96e9e7881801e720c4c32e8b6417fd05fc51af051d3afeea073"],"limits":{"horizon_steps":1408,"input_bytes":1048576,"memory_bytes":6442450944,"output_bytes":1048576,"processes":1,"retries":0,"trace_rows":10000,"wall_time_ms":7200000},"metrics":[{"description":"max relative source-energy discrepancy against 65-node reference","id":"source-energy-relative","unit":"1"},{"description":"max relative non-null source-reaction discrepancy against 65-node reference","id":"source-reaction-relative","unit":"1"},{"description":"max relative 33/65-node energy disagreement","id":"reference-energy-relative","unit":"1"},{"description":"max relative non-null 33/65-node reaction disagreement","id":"reference-reaction-relative","unit":"1"},{"description":"max absolute field versus matched-source radiated energy difference","id":"field-energy-absolute","unit":"model-energy"},{"description":"max absolute field versus matched-source outward axial momentum difference","id":"field-momentum-absolute","unit":"model-momentum"},{"description":"max relative non-null field versus matched-source integrated reaction difference","id":"field-reaction-relative","unit":"1"},{"description":"max absolute terminal energy plus outgoing energy minus source work","id":"internal-energy-absolute","unit":"model-energy"},{"description":"max absolute terminal axial momentum plus outgoing momentum plus source reaction","id":"internal-momentum-absolute","unit":"model-momentum"},{"description":"max nonnegative energy retained at end of observation","id":"terminal-energy","unit":"model-energy"},{"description":"max absolute terminal axial momentum","id":"terminal-momentum-absolute","unit":"model-momentum"},{"description":"max absolute sum of forward and reverse integrated reactions for each width","id":"phase-reversal-absolute","unit":"model-momentum"},{"description":"max absolute in-phase reaction, outgoing momentum, terminal momentum and null reference reaction","id":"null-absolute","unit":"model-momentum"},{"description":"max absolute standard/enlarged-domain difference of each like-unit scalar field measurement","id":"outer-domain-absolute","unit":"model-unit"},{"description":"max absolute standard/half-step difference of outgoing energy and source work","id":"paired-energy-absolute","unit":"model-energy"},{"description":"max absolute standard/half-step outgoing momentum difference","id":"paired-momentum-absolute","unit":"model-momentum"},{"description":"max absolute standard/half-step reaction difference divided by dense forward reaction magnitude","id":"paired-reaction-relative","unit":"1"},{"description":"minimum magnitude of integrated non-null reaction; must also have the declared phase sign","id":"minimum-nonnull-reaction","unit":"model-momentum"},{"description":"minimum fraction of required case and paired obligations with valid terminal evidence","id":"obligation-coverage","unit":"1"}],"model_boundaries":["Dimensionless model time and coordinates with wave speed and angular carrier frequency equal to one; no physical-unit calibration.","Stationary normalized truncated Gaussian sources, one real scalar channel, finite pulse and zero initial field.","No moving craft, actuator, power supply, losses, electromagnetic hardware, thermal or structural model.","Only widths 0.25 and 0.2, phases -pi/2, 0, +pi/2 and the named configurations. No instantaneous coincident-source force regularization.","Owner-maintained field and analytic radiation paths share source geometry and pulse assumptions, but not the field stencil or surface gradients.","Exploratory results informed design and all ten primary configurations have been seen. The later fresh run tests reproducibility after an immutable freeze, not unseen discovery."],"question":"For the frozen two-source scalar pulse model, does changing relative phase reverse a resolvable axial source reaction while independent radiation and control-volume energy and momentum checks satisfy every registered error allocation?","required_obligations":["PF-SOURCE","PF-REFERENCE","PF-FIELD","PF-ENERGY","PF-MOMENTUM","PF-TERMINAL","PF-PHASE","PF-NULL","PF-DOMAIN","PF-TIME","PF-COVERAGE"],"revision":1,"schema_version":"tt.experiment.v1","seeds":[0],"stopping_rule":"Verify frozen input identities and qualification first. Execute all ten ordered primary scenarios once, serially, without cache reuse, random draws or retry. Numerical obligation failures are retained while remaining safe cases run. Stop on malformed input/output, identity drift, missing required evidence, timeout or resource breach; retain partial observations and mark all unrun obligations unavailable, never accepted. Any changed question, input, threshold, tolerance, baseline, cohort or stopping rule requires a new revision. No tuning or case substitution after observing primary results.","thresholds":{"field-energy-absolute":"0.004","field-momentum-absolute":"0.0022","field-reaction-relative":"0.005","internal-energy-absolute":"0.006","internal-momentum-absolute":"0.0005","minimum-nonnull-reaction":"0.01","null-absolute":"0.00000001","obligation-coverage":"1","outer-domain-absolute":"0.0000001","paired-energy-absolute":"0.004","paired-momentum-absolute":"0.0022","paired-reaction-relative":"0.005","phase-reversal-absolute":"0.00000001","reference-energy-relative":"0.00001","reference-reaction-relative":"0.00001","source-energy-relative":"0.001","source-reaction-relative":"0.001","terminal-energy":"0.0001","terminal-momentum-absolute":"0.00001"},"title":"Can changing the phase steer radiation recoil in a finite-source model?","tolerances":{"field-energy-absolute":"0","field-momentum-absolute":"0","field-reaction-relative":"0","internal-energy-absolute":"0","internal-momentum-absolute":"0","minimum-nonnull-reaction":"0","null-absolute":"0","obligation-coverage":"0","outer-domain-absolute":"0","paired-energy-absolute":"0","paired-momentum-absolute":"0","paired-reaction-relative":"0","phase-reversal-absolute":"0","reference-energy-relative":"0","reference-reaction-relative":"0","source-energy-relative":"0","source-reaction-relative":"0","terminal-energy":"0","terminal-momentum-absolute":"0"}}