{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:RLTTALPZGU3VPT4TDRPS4IXCWU","short_pith_number":"pith:RLTTALPZ","schema_version":"1.0","canonical_sha256":"8ae7302df9353757cf931c5f2e22e2b51d6f74a36c294d596381adf5a32c2b07","source":{"kind":"arxiv","id":"1512.09004","version":5},"attestation_state":"computed","paper":{"title":"Thermal smearing of the magneto-Kohn anomaly for Dirac materials and comparison with the two-dimensional electron liquid","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Antonios Balassis, Dipendra Dahal, Godfrey Gumbs, M. L. Glasser","submitted_at":"2015-12-30T16:37:51Z","abstract_excerpt":"We compute and compare the effects due to a uniform perpendicular magnetic field as well as temperature on the static polarization functions for monolayer graphene (MLG), associated with the Dirac point, with that for the two-dimensional electron liquid (2DEL) with the use of comprehensive numerical calculations. Previous results for the 2DEL are discussed and, in particular, we point out a flaw in a reported analytic derivation which was carried out to exhibit the smearing of the Fermi surface for 2DEL. The relevance of our study to the Kohn anomaly in low-dimensional structures and the Fried"},"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":"1512.09004","kind":"arxiv","version":5},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-12-30T16:37:51Z","cross_cats_sorted":[],"title_canon_sha256":"d8061bae42381efb5bc284c667f4aa46286d5fa16f0a27cd3f8bd9ed0c50de50","abstract_canon_sha256":"1560cdef88ea3f667a9e8a1034e3ceb13e14304add180e8bb6287cbed8667bd7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:57:17.801097Z","signature_b64":"73MBe3ghiMQsTQUhypL1oqDNpQ6EEryeUu6zzzKcJJ8nWKzlo27CiNgiqLS+lLQvuSm2kxb64Thp9OK4nS8BCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8ae7302df9353757cf931c5f2e22e2b51d6f74a36c294d596381adf5a32c2b07","last_reissued_at":"2026-05-18T00:57:17.800417Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:57:17.800417Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermal smearing of the magneto-Kohn anomaly for Dirac materials and comparison with the two-dimensional electron liquid","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Antonios Balassis, Dipendra Dahal, Godfrey Gumbs, M. L. Glasser","submitted_at":"2015-12-30T16:37:51Z","abstract_excerpt":"We compute and compare the effects due to a uniform perpendicular magnetic field as well as temperature on the static polarization functions for monolayer graphene (MLG), associated with the Dirac point, with that for the two-dimensional electron liquid (2DEL) with the use of comprehensive numerical calculations. Previous results for the 2DEL are discussed and, in particular, we point out a flaw in a reported analytic derivation which was carried out to exhibit the smearing of the Fermi surface for 2DEL. The relevance of our study to the Kohn anomaly in low-dimensional structures and the Fried"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.09004","kind":"arxiv","version":5},"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":"1512.09004","created_at":"2026-05-18T00:57:17.800520+00:00"},{"alias_kind":"arxiv_version","alias_value":"1512.09004v5","created_at":"2026-05-18T00:57:17.800520+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.09004","created_at":"2026-05-18T00:57:17.800520+00:00"},{"alias_kind":"pith_short_12","alias_value":"RLTTALPZGU3V","created_at":"2026-05-18T12:29:39.896362+00:00"},{"alias_kind":"pith_short_16","alias_value":"RLTTALPZGU3VPT4T","created_at":"2026-05-18T12:29:39.896362+00:00"},{"alias_kind":"pith_short_8","alias_value":"RLTTALPZ","created_at":"2026-05-18T12:29:39.896362+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/RLTTALPZGU3VPT4TDRPS4IXCWU","json":"https://pith.science/pith/RLTTALPZGU3VPT4TDRPS4IXCWU.json","graph_json":"https://pith.science/api/pith-number/RLTTALPZGU3VPT4TDRPS4IXCWU/graph.json","events_json":"https://pith.science/api/pith-number/RLTTALPZGU3VPT4TDRPS4IXCWU/events.json","paper":"https://pith.science/paper/RLTTALPZ"},"agent_actions":{"view_html":"https://pith.science/pith/RLTTALPZGU3VPT4TDRPS4IXCWU","download_json":"https://pith.science/pith/RLTTALPZGU3VPT4TDRPS4IXCWU.json","view_paper":"https://pith.science/paper/RLTTALPZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1512.09004&json=true","fetch_graph":"https://pith.science/api/pith-number/RLTTALPZGU3VPT4TDRPS4IXCWU/graph.json","fetch_events":"https://pith.science/api/pith-number/RLTTALPZGU3VPT4TDRPS4IXCWU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RLTTALPZGU3VPT4TDRPS4IXCWU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RLTTALPZGU3VPT4TDRPS4IXCWU/action/storage_attestation","attest_author":"https://pith.science/pith/RLTTALPZGU3VPT4TDRPS4IXCWU/action/author_attestation","sign_citation":"https://pith.science/pith/RLTTALPZGU3VPT4TDRPS4IXCWU/action/citation_signature","submit_replication":"https://pith.science/pith/RLTTALPZGU3VPT4TDRPS4IXCWU/action/replication_record"}},"created_at":"2026-05-18T00:57:17.800520+00:00","updated_at":"2026-05-18T00:57:17.800520+00:00"}