{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:WNOQC7GFHLYFXUKINGOSGJZEPZ","short_pith_number":"pith:WNOQC7GF","schema_version":"1.0","canonical_sha256":"b35d017cc53af05bd148699d2327247e560f4783edd066e1aaba6fafdc1e8da9","source":{"kind":"arxiv","id":"1412.0811","version":1},"attestation_state":"computed","paper":{"title":"Collective modes in anisotropic double layer systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"A. H. Castro Neto, A. S. Rodin","submitted_at":"2014-12-02T08:31:08Z","abstract_excerpt":"We study collective modes in anisotropic double layer systems. To this end, we derive a zero-$T$ dynamic polarization function for a conductor with a paraboloidal dispersion. Following this, we demonstrate the dependence of the plasmonic modes on the relative orientation, doping, and system anisotropy."},"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":"1412.0811","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-12-02T08:31:08Z","cross_cats_sorted":[],"title_canon_sha256":"26aaff61967d1bc8241d1296daa5a1369dd40f3db205305b4cb04f31ddd837f6","abstract_canon_sha256":"bc3aa16c7cb8f6abf61b3755d47168a70c3b5100ac2626c0690d5c7310f4c661"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:24.292532Z","signature_b64":"OCB6QtqB4ZgT/Ct4UWuvoLopEIThasIqr3zVFBR62VQkpMyeueJwbiAcxz2IZKZDEABAa9NouoBbFqUPppF8Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b35d017cc53af05bd148699d2327247e560f4783edd066e1aaba6fafdc1e8da9","last_reissued_at":"2026-05-18T01:41:24.291711Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:24.291711Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Collective modes in anisotropic double layer systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"A. H. Castro Neto, A. S. Rodin","submitted_at":"2014-12-02T08:31:08Z","abstract_excerpt":"We study collective modes in anisotropic double layer systems. To this end, we derive a zero-$T$ dynamic polarization function for a conductor with a paraboloidal dispersion. Following this, we demonstrate the dependence of the plasmonic modes on the relative orientation, doping, and system anisotropy."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.0811","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":""},"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":"1412.0811","created_at":"2026-05-18T01:41:24.291833+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.0811v1","created_at":"2026-05-18T01:41:24.291833+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.0811","created_at":"2026-05-18T01:41:24.291833+00:00"},{"alias_kind":"pith_short_12","alias_value":"WNOQC7GFHLYF","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_16","alias_value":"WNOQC7GFHLYFXUKI","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_8","alias_value":"WNOQC7GF","created_at":"2026-05-18T12:28:54.890064+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/WNOQC7GFHLYFXUKINGOSGJZEPZ","json":"https://pith.science/pith/WNOQC7GFHLYFXUKINGOSGJZEPZ.json","graph_json":"https://pith.science/api/pith-number/WNOQC7GFHLYFXUKINGOSGJZEPZ/graph.json","events_json":"https://pith.science/api/pith-number/WNOQC7GFHLYFXUKINGOSGJZEPZ/events.json","paper":"https://pith.science/paper/WNOQC7GF"},"agent_actions":{"view_html":"https://pith.science/pith/WNOQC7GFHLYFXUKINGOSGJZEPZ","download_json":"https://pith.science/pith/WNOQC7GFHLYFXUKINGOSGJZEPZ.json","view_paper":"https://pith.science/paper/WNOQC7GF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.0811&json=true","fetch_graph":"https://pith.science/api/pith-number/WNOQC7GFHLYFXUKINGOSGJZEPZ/graph.json","fetch_events":"https://pith.science/api/pith-number/WNOQC7GFHLYFXUKINGOSGJZEPZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WNOQC7GFHLYFXUKINGOSGJZEPZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WNOQC7GFHLYFXUKINGOSGJZEPZ/action/storage_attestation","attest_author":"https://pith.science/pith/WNOQC7GFHLYFXUKINGOSGJZEPZ/action/author_attestation","sign_citation":"https://pith.science/pith/WNOQC7GFHLYFXUKINGOSGJZEPZ/action/citation_signature","submit_replication":"https://pith.science/pith/WNOQC7GFHLYFXUKINGOSGJZEPZ/action/replication_record"}},"created_at":"2026-05-18T01:41:24.291833+00:00","updated_at":"2026-05-18T01:41:24.291833+00:00"}