{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:JJYH3TAVCLFNGRO7G7JJ7TXGP5","short_pith_number":"pith:JJYH3TAV","schema_version":"1.0","canonical_sha256":"4a707dcc1512cad345df37d29fcee67f4128fd1c806eee5cd5417da3bbb89d6e","source":{"kind":"arxiv","id":"1712.08813","version":2},"attestation_state":"computed","paper":{"title":"Hierarchy of Information Scrambling, Thermalization, and Hydrodynamic Flow in Graphene","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"J\\\"org Schmalian, Markus J. Klug, Mathias S. Scheurer","submitted_at":"2017-12-23T18:05:33Z","abstract_excerpt":"We determine the information scrambling rate $\\lambda_{L}$ due to electron-electron Coulomb interaction in graphene. $\\lambda_{L}$ characterizes the growth of chaos and has been argued to give information about the thermalization and hydrodynamic transport coefficients of a many-body system. We demonstrate that $\\lambda_{L}$ behaves for strong coupling similar to transport and energy relaxation rates. A weak coupling analysis, however, reveals that scrambling is related to dephasing or single particle relaxation. Furthermore, $\\lambda_{L}$ is found to be parametrically larger than the collisio"},"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":"1712.08813","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-12-23T18:05:33Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"307c649e4c44d0c10c36d44355ff9b83e43dc7d55af36c4cf295cbbf3f6a6d70","abstract_canon_sha256":"5e9723f19eb4396a60f78a39a7245c59e0acb91495b10a0e5a1cecdd5f4aac9a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:11:06.597700Z","signature_b64":"DR3ENC5MpNDeQHodpfvWc5N3QF9oXiKSTJ4/p2muGYtcU/CeFz5L4xAI3rnr97KhtoXZXZ+uAQlhm2FvG0dkDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4a707dcc1512cad345df37d29fcee67f4128fd1c806eee5cd5417da3bbb89d6e","last_reissued_at":"2026-05-18T00:11:06.596958Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:11:06.596958Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hierarchy of Information Scrambling, Thermalization, and Hydrodynamic Flow in Graphene","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"J\\\"org Schmalian, Markus J. Klug, Mathias S. Scheurer","submitted_at":"2017-12-23T18:05:33Z","abstract_excerpt":"We determine the information scrambling rate $\\lambda_{L}$ due to electron-electron Coulomb interaction in graphene. $\\lambda_{L}$ characterizes the growth of chaos and has been argued to give information about the thermalization and hydrodynamic transport coefficients of a many-body system. We demonstrate that $\\lambda_{L}$ behaves for strong coupling similar to transport and energy relaxation rates. A weak coupling analysis, however, reveals that scrambling is related to dephasing or single particle relaxation. Furthermore, $\\lambda_{L}$ is found to be parametrically larger than the collisio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.08813","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":""},"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":"1712.08813","created_at":"2026-05-18T00:11:06.597081+00:00"},{"alias_kind":"arxiv_version","alias_value":"1712.08813v2","created_at":"2026-05-18T00:11:06.597081+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.08813","created_at":"2026-05-18T00:11:06.597081+00:00"},{"alias_kind":"pith_short_12","alias_value":"JJYH3TAVCLFN","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_16","alias_value":"JJYH3TAVCLFNGRO7","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_8","alias_value":"JJYH3TAV","created_at":"2026-05-18T12:31:24.725408+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/JJYH3TAVCLFNGRO7G7JJ7TXGP5","json":"https://pith.science/pith/JJYH3TAVCLFNGRO7G7JJ7TXGP5.json","graph_json":"https://pith.science/api/pith-number/JJYH3TAVCLFNGRO7G7JJ7TXGP5/graph.json","events_json":"https://pith.science/api/pith-number/JJYH3TAVCLFNGRO7G7JJ7TXGP5/events.json","paper":"https://pith.science/paper/JJYH3TAV"},"agent_actions":{"view_html":"https://pith.science/pith/JJYH3TAVCLFNGRO7G7JJ7TXGP5","download_json":"https://pith.science/pith/JJYH3TAVCLFNGRO7G7JJ7TXGP5.json","view_paper":"https://pith.science/paper/JJYH3TAV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1712.08813&json=true","fetch_graph":"https://pith.science/api/pith-number/JJYH3TAVCLFNGRO7G7JJ7TXGP5/graph.json","fetch_events":"https://pith.science/api/pith-number/JJYH3TAVCLFNGRO7G7JJ7TXGP5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JJYH3TAVCLFNGRO7G7JJ7TXGP5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JJYH3TAVCLFNGRO7G7JJ7TXGP5/action/storage_attestation","attest_author":"https://pith.science/pith/JJYH3TAVCLFNGRO7G7JJ7TXGP5/action/author_attestation","sign_citation":"https://pith.science/pith/JJYH3TAVCLFNGRO7G7JJ7TXGP5/action/citation_signature","submit_replication":"https://pith.science/pith/JJYH3TAVCLFNGRO7G7JJ7TXGP5/action/replication_record"}},"created_at":"2026-05-18T00:11:06.597081+00:00","updated_at":"2026-05-18T00:11:06.597081+00:00"}