{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:WPC4OSFTQK3CKPMDVPQWN6XR2Y","short_pith_number":"pith:WPC4OSFT","schema_version":"1.0","canonical_sha256":"b3c5c748b382b6253d83abe166faf1d61000f92e64cf969f202b51c3cfcf2564","source":{"kind":"arxiv","id":"2311.03142","version":2},"attestation_state":"computed","paper":{"title":"Plasmons in a layered strange metal using the gauge-gravity duality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"C.F.J. Flipse, H.T.C. Stoof, S.T. Van den Eede, T.J.N. van Stralen","submitted_at":"2023-11-06T14:39:08Z","abstract_excerpt":"In an attempt to understand the density-density response of the cuprate superconductors, we study plasmons in a layered strange metal using the Gubser-Rocha model. The latter is a well-known bottom-up holographic model for a strange metal that is used here to describe the strongly repulsive on-site interactions between the electrons in each copper-oxide (CuO$_2$) layer, whereas the long-range Coulomb interactions are incorporated by a so-called double-trace deformation. To be able to model the bilayer cuprates more realistically, we consider in particular the case of two closely-spaced CuO$_2$"},"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":"2311.03142","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2023-11-06T14:39:08Z","cross_cats_sorted":[],"title_canon_sha256":"34dd794835a17500fb275e7d7e27e23fd1d88e2ac7d87d8905c7ee749b8c65c8","abstract_canon_sha256":"77c018c1b9f18537922a22a0431426e127b3a5e140ed0667b0e9dd860fc15907"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:10:51.052683Z","signature_b64":"B3hRglXD2sT260Xq1Lf5b7rcIpncMK+ciejYW/mEe5cnAdo/Z+x3h54VRA9P/GsGSBYV3fYr0Om5iTFdrI3nAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b3c5c748b382b6253d83abe166faf1d61000f92e64cf969f202b51c3cfcf2564","last_reissued_at":"2026-07-05T07:10:51.052221Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:10:51.052221Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Plasmons in a layered strange metal using the gauge-gravity duality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"C.F.J. Flipse, H.T.C. Stoof, S.T. Van den Eede, T.J.N. van Stralen","submitted_at":"2023-11-06T14:39:08Z","abstract_excerpt":"In an attempt to understand the density-density response of the cuprate superconductors, we study plasmons in a layered strange metal using the Gubser-Rocha model. The latter is a well-known bottom-up holographic model for a strange metal that is used here to describe the strongly repulsive on-site interactions between the electrons in each copper-oxide (CuO$_2$) layer, whereas the long-range Coulomb interactions are incorporated by a so-called double-trace deformation. To be able to model the bilayer cuprates more realistically, we consider in particular the case of two closely-spaced CuO$_2$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.03142","kind":"arxiv","version":2},"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/2311.03142/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":"2311.03142","created_at":"2026-07-05T07:10:51.052276+00:00"},{"alias_kind":"arxiv_version","alias_value":"2311.03142v2","created_at":"2026-07-05T07:10:51.052276+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.03142","created_at":"2026-07-05T07:10:51.052276+00:00"},{"alias_kind":"pith_short_12","alias_value":"WPC4OSFTQK3C","created_at":"2026-07-05T07:10:51.052276+00:00"},{"alias_kind":"pith_short_16","alias_value":"WPC4OSFTQK3CKPMD","created_at":"2026-07-05T07:10:51.052276+00:00"},{"alias_kind":"pith_short_8","alias_value":"WPC4OSFT","created_at":"2026-07-05T07:10:51.052276+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/WPC4OSFTQK3CKPMDVPQWN6XR2Y","json":"https://pith.science/pith/WPC4OSFTQK3CKPMDVPQWN6XR2Y.json","graph_json":"https://pith.science/api/pith-number/WPC4OSFTQK3CKPMDVPQWN6XR2Y/graph.json","events_json":"https://pith.science/api/pith-number/WPC4OSFTQK3CKPMDVPQWN6XR2Y/events.json","paper":"https://pith.science/paper/WPC4OSFT"},"agent_actions":{"view_html":"https://pith.science/pith/WPC4OSFTQK3CKPMDVPQWN6XR2Y","download_json":"https://pith.science/pith/WPC4OSFTQK3CKPMDVPQWN6XR2Y.json","view_paper":"https://pith.science/paper/WPC4OSFT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2311.03142&json=true","fetch_graph":"https://pith.science/api/pith-number/WPC4OSFTQK3CKPMDVPQWN6XR2Y/graph.json","fetch_events":"https://pith.science/api/pith-number/WPC4OSFTQK3CKPMDVPQWN6XR2Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WPC4OSFTQK3CKPMDVPQWN6XR2Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WPC4OSFTQK3CKPMDVPQWN6XR2Y/action/storage_attestation","attest_author":"https://pith.science/pith/WPC4OSFTQK3CKPMDVPQWN6XR2Y/action/author_attestation","sign_citation":"https://pith.science/pith/WPC4OSFTQK3CKPMDVPQWN6XR2Y/action/citation_signature","submit_replication":"https://pith.science/pith/WPC4OSFTQK3CKPMDVPQWN6XR2Y/action/replication_record"}},"created_at":"2026-07-05T07:10:51.052276+00:00","updated_at":"2026-07-05T07:10:51.052276+00:00"}