{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:MXUWK7WOWQJWF4WYVJMEX7T4RU","short_pith_number":"pith:MXUWK7WO","schema_version":"1.0","canonical_sha256":"65e9657eceb41362f2d8aa584bfe7c8d2ca85a1d734f24f024b6f4702bbe8337","source":{"kind":"arxiv","id":"2606.25613","version":1},"attestation_state":"computed","paper":{"title":"Holographic correlation functions of fermions in anisotropic plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Si-wen Li, Yan-qing Zhao","submitted_at":"2026-06-24T09:22:02Z","abstract_excerpt":"By using the gauge-gravity duality, we study the holographic fermionic correlation functions in strongly coupled anisotropic plasmas. Starting from the isotropic black AdS background, we revisit the prescription for computing the retarded Green\\textquoteright s function of a probe Dirac fermion and then generalize the formulas with respect to the anisotropic geometries. The method is applied to three distinct holographic models that capture different physical origins of anisotropy: axion-induced, magnetic-field-induced and unquenched-flavor-induced. Numerical results for the holographic correl"},"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":"2606.25613","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-06-24T09:22:02Z","cross_cats_sorted":[],"title_canon_sha256":"563e5323edc60cea8f0d39743ba46e5652fe10cc0b6b0a2c40099e900f99198d","abstract_canon_sha256":"55680c90de608b9f1645829d0f920a41e3ddd6082a7ef47ab8cf551b82e8286e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-25T01:18:10.435644Z","signature_b64":"zHeWMgtdEvf2Ba7BSxSMOihDaKBxXQtto9AlaoQpVIybAw0cuisK13Ikb3PcMVmbLFVrxnSmT90WQ5NMht8GCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"65e9657eceb41362f2d8aa584bfe7c8d2ca85a1d734f24f024b6f4702bbe8337","last_reissued_at":"2026-06-25T01:18:10.435231Z","signature_status":"signed_v1","first_computed_at":"2026-06-25T01:18:10.435231Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic correlation functions of fermions in anisotropic plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Si-wen Li, Yan-qing Zhao","submitted_at":"2026-06-24T09:22:02Z","abstract_excerpt":"By using the gauge-gravity duality, we study the holographic fermionic correlation functions in strongly coupled anisotropic plasmas. Starting from the isotropic black AdS background, we revisit the prescription for computing the retarded Green\\textquoteright s function of a probe Dirac fermion and then generalize the formulas with respect to the anisotropic geometries. The method is applied to three distinct holographic models that capture different physical origins of anisotropy: axion-induced, magnetic-field-induced and unquenched-flavor-induced. Numerical results for the holographic correl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.25613","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/2606.25613/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":"2606.25613","created_at":"2026-06-25T01:18:10.435292+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.25613v1","created_at":"2026-06-25T01:18:10.435292+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.25613","created_at":"2026-06-25T01:18:10.435292+00:00"},{"alias_kind":"pith_short_12","alias_value":"MXUWK7WOWQJW","created_at":"2026-06-25T01:18:10.435292+00:00"},{"alias_kind":"pith_short_16","alias_value":"MXUWK7WOWQJWF4WY","created_at":"2026-06-25T01:18:10.435292+00:00"},{"alias_kind":"pith_short_8","alias_value":"MXUWK7WO","created_at":"2026-06-25T01:18:10.435292+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/MXUWK7WOWQJWF4WYVJMEX7T4RU","json":"https://pith.science/pith/MXUWK7WOWQJWF4WYVJMEX7T4RU.json","graph_json":"https://pith.science/api/pith-number/MXUWK7WOWQJWF4WYVJMEX7T4RU/graph.json","events_json":"https://pith.science/api/pith-number/MXUWK7WOWQJWF4WYVJMEX7T4RU/events.json","paper":"https://pith.science/paper/MXUWK7WO"},"agent_actions":{"view_html":"https://pith.science/pith/MXUWK7WOWQJWF4WYVJMEX7T4RU","download_json":"https://pith.science/pith/MXUWK7WOWQJWF4WYVJMEX7T4RU.json","view_paper":"https://pith.science/paper/MXUWK7WO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.25613&json=true","fetch_graph":"https://pith.science/api/pith-number/MXUWK7WOWQJWF4WYVJMEX7T4RU/graph.json","fetch_events":"https://pith.science/api/pith-number/MXUWK7WOWQJWF4WYVJMEX7T4RU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MXUWK7WOWQJWF4WYVJMEX7T4RU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MXUWK7WOWQJWF4WYVJMEX7T4RU/action/storage_attestation","attest_author":"https://pith.science/pith/MXUWK7WOWQJWF4WYVJMEX7T4RU/action/author_attestation","sign_citation":"https://pith.science/pith/MXUWK7WOWQJWF4WYVJMEX7T4RU/action/citation_signature","submit_replication":"https://pith.science/pith/MXUWK7WOWQJWF4WYVJMEX7T4RU/action/replication_record"}},"created_at":"2026-06-25T01:18:10.435292+00:00","updated_at":"2026-06-25T01:18:10.435292+00:00"}