{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:XGUABVX2LOAGZGZYROMS7KJZDU","short_pith_number":"pith:XGUABVX2","schema_version":"1.0","canonical_sha256":"b9a800d6fa5b806c9b388b992fa9391d24e47198f8e8767616a6417d0c211d32","source":{"kind":"arxiv","id":"1908.01585","version":1},"attestation_state":"computed","paper":{"title":"Exact Recession Velocity and Cosmic Redshift Based on Cosmological Principle and Yang-Mills Gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.gen-ph","authors_text":"Jong-Ping Hsu, Leonardo Hsu","submitted_at":"2019-08-01T15:07:25Z","abstract_excerpt":"Based on the cosmological principle and quantum Yang-Mills gravity in the super-macroscopic limit, we obtain an exact recession velocity and cosmic redshift z, as measured in an inertial frame $F\\equiv F(t,x,y,z).$ For a matter-dominated universe, we have the effective cosmic metric tensor $G_{\\mu\\nu}(t)=(B^2(t),-A^2(t),-A^2(t),-A^2(t)), \\ A\\propto B\\propto t^{1/2}$, where $t$ has the operational meaning of time in $F$ frame. We assume a cosmic action $S\\equiv S_{cos}$ involving $G_{\\mu\\nu}(t)$ and derive the `Okubo equation' of motion, $G^{\\mu\\nu}(t)\\partial_\\mu S \\partial_\\nu S - m^2=0$, for"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1908.01585","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2019-08-01T15:07:25Z","cross_cats_sorted":[],"title_canon_sha256":"0cf8210bc1d0b659f38dbf91304ee900d618deca18fddd0a7a0d03860f1def3f","abstract_canon_sha256":"3f5e76bd9af8ae7d0c8b4c2d2270a481425eae9a42ad9782a897d84f9f210a6e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T23:51:31.891623Z","signature_b64":"hStFJZRfh0FzfdZVlAfUECmFDZUGBbrxQa3B6t6Q+JW+xnSr31615CDQY7XGzFlftSOoNL63tC1FNEraKRipCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b9a800d6fa5b806c9b388b992fa9391d24e47198f8e8767616a6417d0c211d32","last_reissued_at":"2026-07-04T23:51:31.891280Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T23:51:31.891280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exact Recession Velocity and Cosmic Redshift Based on Cosmological Principle and Yang-Mills Gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.gen-ph","authors_text":"Jong-Ping Hsu, Leonardo Hsu","submitted_at":"2019-08-01T15:07:25Z","abstract_excerpt":"Based on the cosmological principle and quantum Yang-Mills gravity in the super-macroscopic limit, we obtain an exact recession velocity and cosmic redshift z, as measured in an inertial frame $F\\equiv F(t,x,y,z).$ For a matter-dominated universe, we have the effective cosmic metric tensor $G_{\\mu\\nu}(t)=(B^2(t),-A^2(t),-A^2(t),-A^2(t)), \\ A\\propto B\\propto t^{1/2}$, where $t$ has the operational meaning of time in $F$ frame. We assume a cosmic action $S\\equiv S_{cos}$ involving $G_{\\mu\\nu}(t)$ and derive the `Okubo equation' of motion, $G^{\\mu\\nu}(t)\\partial_\\mu S \\partial_\\nu S - m^2=0$, for"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.01585","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1908.01585/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1908.01585","created_at":"2026-07-04T23:51:31.891337+00:00"},{"alias_kind":"arxiv_version","alias_value":"1908.01585v1","created_at":"2026-07-04T23:51:31.891337+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.01585","created_at":"2026-07-04T23:51:31.891337+00:00"},{"alias_kind":"pith_short_12","alias_value":"XGUABVX2LOAG","created_at":"2026-07-04T23:51:31.891337+00:00"},{"alias_kind":"pith_short_16","alias_value":"XGUABVX2LOAGZGZY","created_at":"2026-07-04T23:51:31.891337+00:00"},{"alias_kind":"pith_short_8","alias_value":"XGUABVX2","created_at":"2026-07-04T23:51:31.891337+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XGUABVX2LOAGZGZYROMS7KJZDU","json":"https://pith.science/pith/XGUABVX2LOAGZGZYROMS7KJZDU.json","graph_json":"https://pith.science/api/pith-number/XGUABVX2LOAGZGZYROMS7KJZDU/graph.json","events_json":"https://pith.science/api/pith-number/XGUABVX2LOAGZGZYROMS7KJZDU/events.json","paper":"https://pith.science/paper/XGUABVX2"},"agent_actions":{"view_html":"https://pith.science/pith/XGUABVX2LOAGZGZYROMS7KJZDU","download_json":"https://pith.science/pith/XGUABVX2LOAGZGZYROMS7KJZDU.json","view_paper":"https://pith.science/paper/XGUABVX2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1908.01585&json=true","fetch_graph":"https://pith.science/api/pith-number/XGUABVX2LOAGZGZYROMS7KJZDU/graph.json","fetch_events":"https://pith.science/api/pith-number/XGUABVX2LOAGZGZYROMS7KJZDU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XGUABVX2LOAGZGZYROMS7KJZDU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XGUABVX2LOAGZGZYROMS7KJZDU/action/storage_attestation","attest_author":"https://pith.science/pith/XGUABVX2LOAGZGZYROMS7KJZDU/action/author_attestation","sign_citation":"https://pith.science/pith/XGUABVX2LOAGZGZYROMS7KJZDU/action/citation_signature","submit_replication":"https://pith.science/pith/XGUABVX2LOAGZGZYROMS7KJZDU/action/replication_record"}},"created_at":"2026-07-04T23:51:31.891337+00:00","updated_at":"2026-07-04T23:51:31.891337+00:00"}