{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:CWNEKM6QSRDDF3YM2CEKLTPGU3","short_pith_number":"pith:CWNEKM6Q","schema_version":"1.0","canonical_sha256":"159a4533d0944632ef0cd088a5cde6a6fd596982aec2d35498b22aa6e268a740","source":{"kind":"arxiv","id":"2606.13611","version":1},"attestation_state":"computed","paper":{"title":"Cosmological Dynamics of the Thermal Scalar Near the Hagedorn Temperature","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Arnab Pradhan, Luis Rufino, Scott Watson","submitted_at":"2026-06-11T17:24:53Z","abstract_excerpt":"We study the cosmological dynamics of the thermal scalar the winding string mode that becomes massless at the Hagedorn transition by coupling it to the string-frame gravi dilaton effective action. This provides a field-theoretic framework for investigating winding mode dynamics near the Hagedorn temperature and their role in string cosmology.\n  Below the Hagedorn temperature, the phase space contains static configurations in which the thermal scalar balances the shifted dilaton evolution. These configurations are boundary states rather than attractors, and when the thermal scalar mass depends "},"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":"2606.13611","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"hep-th","submitted_at":"2026-06-11T17:24:53Z","cross_cats_sorted":[],"title_canon_sha256":"164fa90baae883bf1f371d9af85a2913978093276166039b79f55bb7dc84ace7","abstract_canon_sha256":"ff85a1122ec4d4aed843a4cc8cd3c145d12bd5e450d5ae4f80376a281ee356ee"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-12T01:10:13.109326Z","signature_b64":"J1VwPvoUylxkInOmF6TqbM7dTbBQbepaBPFLNYCzrODS05Y1oYgrztn/MY9BppN4ov1XSVpokUX3xK7cns4WBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"159a4533d0944632ef0cd088a5cde6a6fd596982aec2d35498b22aa6e268a740","last_reissued_at":"2026-06-12T01:10:13.108638Z","signature_status":"signed_v1","first_computed_at":"2026-06-12T01:10:13.108638Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Cosmological Dynamics of the Thermal Scalar Near the Hagedorn Temperature","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Arnab Pradhan, Luis Rufino, Scott Watson","submitted_at":"2026-06-11T17:24:53Z","abstract_excerpt":"We study the cosmological dynamics of the thermal scalar the winding string mode that becomes massless at the Hagedorn transition by coupling it to the string-frame gravi dilaton effective action. This provides a field-theoretic framework for investigating winding mode dynamics near the Hagedorn temperature and their role in string cosmology.\n  Below the Hagedorn temperature, the phase space contains static configurations in which the thermal scalar balances the shifted dilaton evolution. These configurations are boundary states rather than attractors, and when the thermal scalar mass depends "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.13611","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/2606.13611/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":"2606.13611","created_at":"2026-06-12T01:10:13.108736+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.13611v1","created_at":"2026-06-12T01:10:13.108736+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.13611","created_at":"2026-06-12T01:10:13.108736+00:00"},{"alias_kind":"pith_short_12","alias_value":"CWNEKM6QSRDD","created_at":"2026-06-12T01:10:13.108736+00:00"},{"alias_kind":"pith_short_16","alias_value":"CWNEKM6QSRDDF3YM","created_at":"2026-06-12T01:10:13.108736+00:00"},{"alias_kind":"pith_short_8","alias_value":"CWNEKM6Q","created_at":"2026-06-12T01:10:13.108736+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/CWNEKM6QSRDDF3YM2CEKLTPGU3","json":"https://pith.science/pith/CWNEKM6QSRDDF3YM2CEKLTPGU3.json","graph_json":"https://pith.science/api/pith-number/CWNEKM6QSRDDF3YM2CEKLTPGU3/graph.json","events_json":"https://pith.science/api/pith-number/CWNEKM6QSRDDF3YM2CEKLTPGU3/events.json","paper":"https://pith.science/paper/CWNEKM6Q"},"agent_actions":{"view_html":"https://pith.science/pith/CWNEKM6QSRDDF3YM2CEKLTPGU3","download_json":"https://pith.science/pith/CWNEKM6QSRDDF3YM2CEKLTPGU3.json","view_paper":"https://pith.science/paper/CWNEKM6Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.13611&json=true","fetch_graph":"https://pith.science/api/pith-number/CWNEKM6QSRDDF3YM2CEKLTPGU3/graph.json","fetch_events":"https://pith.science/api/pith-number/CWNEKM6QSRDDF3YM2CEKLTPGU3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CWNEKM6QSRDDF3YM2CEKLTPGU3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CWNEKM6QSRDDF3YM2CEKLTPGU3/action/storage_attestation","attest_author":"https://pith.science/pith/CWNEKM6QSRDDF3YM2CEKLTPGU3/action/author_attestation","sign_citation":"https://pith.science/pith/CWNEKM6QSRDDF3YM2CEKLTPGU3/action/citation_signature","submit_replication":"https://pith.science/pith/CWNEKM6QSRDDF3YM2CEKLTPGU3/action/replication_record"}},"created_at":"2026-06-12T01:10:13.108736+00:00","updated_at":"2026-06-12T01:10:13.108736+00:00"}