{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:55KHTSUPRUGBARSBUUXCB3ZREM","short_pith_number":"pith:55KHTSUP","schema_version":"1.0","canonical_sha256":"ef5479ca8f8d0c104641a52e20ef3123073f973bcc668471a860c5f2139e9372","source":{"kind":"arxiv","id":"hep-ph/9812510","version":4},"attestation_state":"computed","paper":{"title":"An effective field theory of QCD at high density","license":"","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Deog Ki Hong","submitted_at":"1998-12-28T15:56:06Z","abstract_excerpt":"We derive a (Wilsonian) effective field theory of QCD at finite density by integrating out the states in the Dirac sea when the chemical potential $\\mu\\gg\\Lambda_{\\rm QCD}$. The quark-gluon coupling is effectively (1+1)-dimensional and the theory contains four-quark operators which become relevant as we approach to the Fermi sea. By calculating the one-loop vacuum polarization tensor in the effective theory, we find the electric gluons have a screening mass, $M\\sim g_s\\mu$, while the static magnetic gluons are unscreened. We then investigate the gap equations for color anti-triplet Cooper pair"},"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":"hep-ph/9812510","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-12-28T15:56:06Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"ac2d64316f26184d6b87d5cb90da623fe416cf1d23396ea7cbe6b4980686e58c","abstract_canon_sha256":"e1d4e00573cb9f536727de1a6ce41ef2289b36dad9dceac5ad9da0d937cb5a02"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:09:39.054250Z","signature_b64":"73vQXjbipSOe+ZHR8EKhFVBRWSnl/eZs/O4ma7bpjcfppDW8hxotOUEiQZ1GqVYc4YigH+8QWgK8QoE1BdJPAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ef5479ca8f8d0c104641a52e20ef3123073f973bcc668471a860c5f2139e9372","last_reissued_at":"2026-07-04T16:09:39.053841Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:09:39.053841Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An effective field theory of QCD at high density","license":"","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Deog Ki Hong","submitted_at":"1998-12-28T15:56:06Z","abstract_excerpt":"We derive a (Wilsonian) effective field theory of QCD at finite density by integrating out the states in the Dirac sea when the chemical potential $\\mu\\gg\\Lambda_{\\rm QCD}$. The quark-gluon coupling is effectively (1+1)-dimensional and the theory contains four-quark operators which become relevant as we approach to the Fermi sea. By calculating the one-loop vacuum polarization tensor in the effective theory, we find the electric gluons have a screening mass, $M\\sim g_s\\mu$, while the static magnetic gluons are unscreened. We then investigate the gap equations for color anti-triplet Cooper pair"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9812510","kind":"arxiv","version":4},"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/hep-ph/9812510/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":"hep-ph/9812510","created_at":"2026-07-04T16:09:39.053909+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9812510v4","created_at":"2026-07-04T16:09:39.053909+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9812510","created_at":"2026-07-04T16:09:39.053909+00:00"},{"alias_kind":"pith_short_12","alias_value":"55KHTSUPRUGB","created_at":"2026-07-04T16:09:39.053909+00:00"},{"alias_kind":"pith_short_16","alias_value":"55KHTSUPRUGBARSB","created_at":"2026-07-04T16:09:39.053909+00:00"},{"alias_kind":"pith_short_8","alias_value":"55KHTSUP","created_at":"2026-07-04T16:09:39.053909+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.11713","citing_title":"Revisiting the Axial Anomaly and Chiral Magnetic Effect in Dense Matter, with Applications to Axion Dark Matter","ref_index":28,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/55KHTSUPRUGBARSBUUXCB3ZREM","json":"https://pith.science/pith/55KHTSUPRUGBARSBUUXCB3ZREM.json","graph_json":"https://pith.science/api/pith-number/55KHTSUPRUGBARSBUUXCB3ZREM/graph.json","events_json":"https://pith.science/api/pith-number/55KHTSUPRUGBARSBUUXCB3ZREM/events.json","paper":"https://pith.science/paper/55KHTSUP"},"agent_actions":{"view_html":"https://pith.science/pith/55KHTSUPRUGBARSBUUXCB3ZREM","download_json":"https://pith.science/pith/55KHTSUPRUGBARSBUUXCB3ZREM.json","view_paper":"https://pith.science/paper/55KHTSUP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9812510&json=true","fetch_graph":"https://pith.science/api/pith-number/55KHTSUPRUGBARSBUUXCB3ZREM/graph.json","fetch_events":"https://pith.science/api/pith-number/55KHTSUPRUGBARSBUUXCB3ZREM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/55KHTSUPRUGBARSBUUXCB3ZREM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/55KHTSUPRUGBARSBUUXCB3ZREM/action/storage_attestation","attest_author":"https://pith.science/pith/55KHTSUPRUGBARSBUUXCB3ZREM/action/author_attestation","sign_citation":"https://pith.science/pith/55KHTSUPRUGBARSBUUXCB3ZREM/action/citation_signature","submit_replication":"https://pith.science/pith/55KHTSUPRUGBARSBUUXCB3ZREM/action/replication_record"}},"created_at":"2026-07-04T16:09:39.053909+00:00","updated_at":"2026-07-04T16:09:39.053909+00:00"}