{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:JUTDI4DFWDSBC5SJS7LL5BNRL5","short_pith_number":"pith:JUTDI4DF","schema_version":"1.0","canonical_sha256":"4d26347065b0e411764997d6be85b15f5f835837723f8e22a21857c3aa064761","source":{"kind":"arxiv","id":"2211.07074","version":4},"attestation_state":"computed","paper":{"title":"Transport properties in the Horndeski holographic two-currents model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Dan Zhang, Guoyang Fu, Jian-Pin Wu, Qiyuan Pan, Xi-Jing Wang","submitted_at":"2022-11-14T02:48:30Z","abstract_excerpt":"The transport features of the holographic two-currents model are investigated in the Horndeski gravity framework. This system displays metallic or insulating characteristics depending on whether the Horndeski coupling parameter $\\gamma$ is negative or positive, but is unaffected by other system parameters such as the strength of the momentum dissipation $\\hat{k}$, the doping $\\chi$ and the coupling between two gauge fields $\\theta$. Secondly, we demonstrate that the thermal conductivities are affected not only by the inherent properties of the black hole, but also by the model parameters. Furt"},"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":"2211.07074","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-11-14T02:48:30Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"853c1f2edb6b7fda881540c3e0b06a905d085e14093eb90988c86ba4de3599d6","abstract_canon_sha256":"84c55904768dfa3258d2eba6d8d50f5e0f949bf6e2ef3253ec5f3890df111ad6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:23:56.860515Z","signature_b64":"0BPHb4Q+JHI/7uvyo8qDy8pTx/BOy8KOSU7aBdlVgjHzfpcGEGKr6LSMIATQC3or3oB2bPEz2s1LxNi4JyK4CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4d26347065b0e411764997d6be85b15f5f835837723f8e22a21857c3aa064761","last_reissued_at":"2026-07-05T06:23:56.860027Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:23:56.860027Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Transport properties in the Horndeski holographic two-currents model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Dan Zhang, Guoyang Fu, Jian-Pin Wu, Qiyuan Pan, Xi-Jing Wang","submitted_at":"2022-11-14T02:48:30Z","abstract_excerpt":"The transport features of the holographic two-currents model are investigated in the Horndeski gravity framework. This system displays metallic or insulating characteristics depending on whether the Horndeski coupling parameter $\\gamma$ is negative or positive, but is unaffected by other system parameters such as the strength of the momentum dissipation $\\hat{k}$, the doping $\\chi$ and the coupling between two gauge fields $\\theta$. Secondly, we demonstrate that the thermal conductivities are affected not only by the inherent properties of the black hole, but also by the model parameters. Furt"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.07074","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/2211.07074/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":"2211.07074","created_at":"2026-07-05T06:23:56.860094+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.07074v4","created_at":"2026-07-05T06:23:56.860094+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.07074","created_at":"2026-07-05T06:23:56.860094+00:00"},{"alias_kind":"pith_short_12","alias_value":"JUTDI4DFWDSB","created_at":"2026-07-05T06:23:56.860094+00:00"},{"alias_kind":"pith_short_16","alias_value":"JUTDI4DFWDSBC5SJ","created_at":"2026-07-05T06:23:56.860094+00:00"},{"alias_kind":"pith_short_8","alias_value":"JUTDI4DF","created_at":"2026-07-05T06:23:56.860094+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/JUTDI4DFWDSBC5SJS7LL5BNRL5","json":"https://pith.science/pith/JUTDI4DFWDSBC5SJS7LL5BNRL5.json","graph_json":"https://pith.science/api/pith-number/JUTDI4DFWDSBC5SJS7LL5BNRL5/graph.json","events_json":"https://pith.science/api/pith-number/JUTDI4DFWDSBC5SJS7LL5BNRL5/events.json","paper":"https://pith.science/paper/JUTDI4DF"},"agent_actions":{"view_html":"https://pith.science/pith/JUTDI4DFWDSBC5SJS7LL5BNRL5","download_json":"https://pith.science/pith/JUTDI4DFWDSBC5SJS7LL5BNRL5.json","view_paper":"https://pith.science/paper/JUTDI4DF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.07074&json=true","fetch_graph":"https://pith.science/api/pith-number/JUTDI4DFWDSBC5SJS7LL5BNRL5/graph.json","fetch_events":"https://pith.science/api/pith-number/JUTDI4DFWDSBC5SJS7LL5BNRL5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JUTDI4DFWDSBC5SJS7LL5BNRL5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JUTDI4DFWDSBC5SJS7LL5BNRL5/action/storage_attestation","attest_author":"https://pith.science/pith/JUTDI4DFWDSBC5SJS7LL5BNRL5/action/author_attestation","sign_citation":"https://pith.science/pith/JUTDI4DFWDSBC5SJS7LL5BNRL5/action/citation_signature","submit_replication":"https://pith.science/pith/JUTDI4DFWDSBC5SJS7LL5BNRL5/action/replication_record"}},"created_at":"2026-07-05T06:23:56.860094+00:00","updated_at":"2026-07-05T06:23:56.860094+00:00"}