{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:CC4GHVT7V5ADJORXPPCXPE7LQB","short_pith_number":"pith:CC4GHVT7","schema_version":"1.0","canonical_sha256":"10b863d67faf4034ba377bc57793eb806ebec9d9a3f2df4cd12e0787c227527f","source":{"kind":"arxiv","id":"2202.09957","version":1},"attestation_state":"computed","paper":{"title":"Scale symmetry and composition of compact star matter","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Long-Qi Shao, Yong-Liang Ma","submitted_at":"2022-02-21T02:50:17Z","abstract_excerpt":"The dense compact star matter is studied by using the skyrmion crystal approach. The chiral effective theory used includes the lightest scalar meson, the lowest-lying vector mesons as well as pions. Consistency with the vector manifestation and the dilaton limit fixed point at high density constrains the anomalous dimension of the gluon field $1.0 \\lesssim |\\gamma_{G^2}| \\lesssim 2.0$ and leads to the significance of the scale symmetry breaking in the intrinsic parity-odd part of the effective theory. The speed of sound $v_s^2 \\simeq 1/3$ and the polytropic index $\\gamma \\simeq 1$ -- both sati"},"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":"2202.09957","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2022-02-21T02:50:17Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"71460acda1b0ff0aa02487648831ec967e8ba446d9ed8020b8f623789ac8c173","abstract_canon_sha256":"ed536a0a3f15efee11d11fc5c064b8d8eac431b89ec581cd450ca4c3d6d7a078"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:52:48.964765Z","signature_b64":"ho4Q4MNdbhTKza/tGRs78AtodV9ETdjQTbXV0iYNphduWawXrsN4vdPfN5JV5W0rW8D1kvYA7j6p/pVNbMAuCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"10b863d67faf4034ba377bc57793eb806ebec9d9a3f2df4cd12e0787c227527f","last_reissued_at":"2026-07-05T04:52:48.964330Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:52:48.964330Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scale symmetry and composition of compact star matter","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Long-Qi Shao, Yong-Liang Ma","submitted_at":"2022-02-21T02:50:17Z","abstract_excerpt":"The dense compact star matter is studied by using the skyrmion crystal approach. The chiral effective theory used includes the lightest scalar meson, the lowest-lying vector mesons as well as pions. Consistency with the vector manifestation and the dilaton limit fixed point at high density constrains the anomalous dimension of the gluon field $1.0 \\lesssim |\\gamma_{G^2}| \\lesssim 2.0$ and leads to the significance of the scale symmetry breaking in the intrinsic parity-odd part of the effective theory. The speed of sound $v_s^2 \\simeq 1/3$ and the polytropic index $\\gamma \\simeq 1$ -- both sati"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.09957","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/2202.09957/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":"2202.09957","created_at":"2026-07-05T04:52:48.964389+00:00"},{"alias_kind":"arxiv_version","alias_value":"2202.09957v1","created_at":"2026-07-05T04:52:48.964389+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.09957","created_at":"2026-07-05T04:52:48.964389+00:00"},{"alias_kind":"pith_short_12","alias_value":"CC4GHVT7V5AD","created_at":"2026-07-05T04:52:48.964389+00:00"},{"alias_kind":"pith_short_16","alias_value":"CC4GHVT7V5ADJORX","created_at":"2026-07-05T04:52:48.964389+00:00"},{"alias_kind":"pith_short_8","alias_value":"CC4GHVT7","created_at":"2026-07-05T04:52:48.964389+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.03138","citing_title":"Suppression of dynamical momentum-space shell by chiral symmetry","ref_index":53,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CC4GHVT7V5ADJORXPPCXPE7LQB","json":"https://pith.science/pith/CC4GHVT7V5ADJORXPPCXPE7LQB.json","graph_json":"https://pith.science/api/pith-number/CC4GHVT7V5ADJORXPPCXPE7LQB/graph.json","events_json":"https://pith.science/api/pith-number/CC4GHVT7V5ADJORXPPCXPE7LQB/events.json","paper":"https://pith.science/paper/CC4GHVT7"},"agent_actions":{"view_html":"https://pith.science/pith/CC4GHVT7V5ADJORXPPCXPE7LQB","download_json":"https://pith.science/pith/CC4GHVT7V5ADJORXPPCXPE7LQB.json","view_paper":"https://pith.science/paper/CC4GHVT7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2202.09957&json=true","fetch_graph":"https://pith.science/api/pith-number/CC4GHVT7V5ADJORXPPCXPE7LQB/graph.json","fetch_events":"https://pith.science/api/pith-number/CC4GHVT7V5ADJORXPPCXPE7LQB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CC4GHVT7V5ADJORXPPCXPE7LQB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CC4GHVT7V5ADJORXPPCXPE7LQB/action/storage_attestation","attest_author":"https://pith.science/pith/CC4GHVT7V5ADJORXPPCXPE7LQB/action/author_attestation","sign_citation":"https://pith.science/pith/CC4GHVT7V5ADJORXPPCXPE7LQB/action/citation_signature","submit_replication":"https://pith.science/pith/CC4GHVT7V5ADJORXPPCXPE7LQB/action/replication_record"}},"created_at":"2026-07-05T04:52:48.964389+00:00","updated_at":"2026-07-05T04:52:48.964389+00:00"}