{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:337NTUT342X2VYWLPFFYAE37NV","short_pith_number":"pith:337NTUT3","schema_version":"1.0","canonical_sha256":"defed9d27be6afaae2cb794b80137f6d690eac61f2f339ef426bf44a6f20b7bf","source":{"kind":"arxiv","id":"1911.06810","version":1},"attestation_state":"computed","paper":{"title":"Turbulent hydrodynamics in strongly correlated Kagome metals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"David Rodriguez Fernandez, Domenico Di Sante, Erik van Loon, Ioannis Matthaiakakis, Johanna Erdmenger, Martin Greiter, Rene Meyer, Ronny Thomale, Tim Wehling","submitted_at":"2019-11-15T18:59:59Z","abstract_excerpt":"A current challenge in condensed matter physics is the realization of strongly correlated, viscous electron fluids. These fluids are not amenable to the perturbative methods of Fermi liquid theory, but can be described by holography, that is, by mapping them onto a weakly curved gravitational theory via gauge/gravity duality. The canonical system considered for realizations has been graphene, which possesses Dirac dispersions at low energies as well as significant Coulomb interactions between the electrons. In this work, we show that Kagome systems with electron fillings adjusted to the Dirac "},"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":"1911.06810","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2019-11-15T18:59:59Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"98c169920cc252bcb3d4013f48a66d25a4171447eacefaa90fe610496559df09","abstract_canon_sha256":"4e7b55f512e20cde2709d24aa208ce40d0ad9a7282826b86c37e910cb159e201"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:30:23.932323Z","signature_b64":"20MR0rbyk+PUMz12eabhXU0YaSGBonuZpX+qUHLiakaFf2HE+Hh5De0HrZNBIjF7nEjldiuFcWCb7nZ8ZR0SCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"defed9d27be6afaae2cb794b80137f6d690eac61f2f339ef426bf44a6f20b7bf","last_reissued_at":"2026-07-05T01:30:23.931890Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:30:23.931890Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Turbulent hydrodynamics in strongly correlated Kagome metals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"David Rodriguez Fernandez, Domenico Di Sante, Erik van Loon, Ioannis Matthaiakakis, Johanna Erdmenger, Martin Greiter, Rene Meyer, Ronny Thomale, Tim Wehling","submitted_at":"2019-11-15T18:59:59Z","abstract_excerpt":"A current challenge in condensed matter physics is the realization of strongly correlated, viscous electron fluids. These fluids are not amenable to the perturbative methods of Fermi liquid theory, but can be described by holography, that is, by mapping them onto a weakly curved gravitational theory via gauge/gravity duality. The canonical system considered for realizations has been graphene, which possesses Dirac dispersions at low energies as well as significant Coulomb interactions between the electrons. In this work, we show that Kagome systems with electron fillings adjusted to the Dirac "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1911.06810","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/1911.06810/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":"1911.06810","created_at":"2026-07-05T01:30:23.931949+00:00"},{"alias_kind":"arxiv_version","alias_value":"1911.06810v1","created_at":"2026-07-05T01:30:23.931949+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1911.06810","created_at":"2026-07-05T01:30:23.931949+00:00"},{"alias_kind":"pith_short_12","alias_value":"337NTUT342X2","created_at":"2026-07-05T01:30:23.931949+00:00"},{"alias_kind":"pith_short_16","alias_value":"337NTUT342X2VYWL","created_at":"2026-07-05T01:30:23.931949+00:00"},{"alias_kind":"pith_short_8","alias_value":"337NTUT3","created_at":"2026-07-05T01:30:23.931949+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/337NTUT342X2VYWLPFFYAE37NV","json":"https://pith.science/pith/337NTUT342X2VYWLPFFYAE37NV.json","graph_json":"https://pith.science/api/pith-number/337NTUT342X2VYWLPFFYAE37NV/graph.json","events_json":"https://pith.science/api/pith-number/337NTUT342X2VYWLPFFYAE37NV/events.json","paper":"https://pith.science/paper/337NTUT3"},"agent_actions":{"view_html":"https://pith.science/pith/337NTUT342X2VYWLPFFYAE37NV","download_json":"https://pith.science/pith/337NTUT342X2VYWLPFFYAE37NV.json","view_paper":"https://pith.science/paper/337NTUT3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1911.06810&json=true","fetch_graph":"https://pith.science/api/pith-number/337NTUT342X2VYWLPFFYAE37NV/graph.json","fetch_events":"https://pith.science/api/pith-number/337NTUT342X2VYWLPFFYAE37NV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/337NTUT342X2VYWLPFFYAE37NV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/337NTUT342X2VYWLPFFYAE37NV/action/storage_attestation","attest_author":"https://pith.science/pith/337NTUT342X2VYWLPFFYAE37NV/action/author_attestation","sign_citation":"https://pith.science/pith/337NTUT342X2VYWLPFFYAE37NV/action/citation_signature","submit_replication":"https://pith.science/pith/337NTUT342X2VYWLPFFYAE37NV/action/replication_record"}},"created_at":"2026-07-05T01:30:23.931949+00:00","updated_at":"2026-07-05T01:30:23.931949+00:00"}