{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:VXWT7M7XUWG66ZD7WIV5YUIRC3","short_pith_number":"pith:VXWT7M7X","schema_version":"1.0","canonical_sha256":"aded3fb3f7a58def647fb22bdc511116f6e0a865452677f3a5ab5efbd37b6c23","source":{"kind":"arxiv","id":"1802.01175","version":1},"attestation_state":"computed","paper":{"title":"Interaction-disorder-driven characteristic momentum in graphene, approach of multi-body distribution functions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"M. N. Najafi","submitted_at":"2018-02-04T19:07:16Z","abstract_excerpt":"Multi-point probability measures along with the dielectric function of Dirac Fermions in mono-layer graphene containing particle-particle and white-noise (out-plane) disorder interactions on an equal footing in the Thomas-Fermi-Dirac approximation is investigated. By calculating the one-body carrier density probability measure of the graphene sheet, we show that the density fluctuation ($\\zeta^{-1}$) is related to the disorder strength ($n_i$), the interaction parameter ($r_s$) and the average density ($\\bar{n}$) via the relation $\\zeta^{-1}\\propto r_sn_i^2\\bar{n}^{-1}$ for which $\\bar{n}\\righ"},"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":"1802.01175","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-02-04T19:07:16Z","cross_cats_sorted":[],"title_canon_sha256":"ec1a7867f59c81f21f9a59bfe70cda39caf448ae5675b0203063d99fa3500a6a","abstract_canon_sha256":"f6d4f088ca909a44cce9f03639abe0996681038b82b377af889db026d937f5d9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:24:27.137525Z","signature_b64":"aPKTxI1xuPXZ8FRl78cq32rn3UiwE5Mf/F3fj4u8fujwPO2A7xTLVvkMMLiD5KcWlD9xfHmPh/9EiVghNdYZDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aded3fb3f7a58def647fb22bdc511116f6e0a865452677f3a5ab5efbd37b6c23","last_reissued_at":"2026-05-18T00:24:27.136816Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:24:27.136816Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Interaction-disorder-driven characteristic momentum in graphene, approach of multi-body distribution functions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"M. N. Najafi","submitted_at":"2018-02-04T19:07:16Z","abstract_excerpt":"Multi-point probability measures along with the dielectric function of Dirac Fermions in mono-layer graphene containing particle-particle and white-noise (out-plane) disorder interactions on an equal footing in the Thomas-Fermi-Dirac approximation is investigated. By calculating the one-body carrier density probability measure of the graphene sheet, we show that the density fluctuation ($\\zeta^{-1}$) is related to the disorder strength ($n_i$), the interaction parameter ($r_s$) and the average density ($\\bar{n}$) via the relation $\\zeta^{-1}\\propto r_sn_i^2\\bar{n}^{-1}$ for which $\\bar{n}\\righ"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.01175","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":"1802.01175","created_at":"2026-05-18T00:24:27.136923+00:00"},{"alias_kind":"arxiv_version","alias_value":"1802.01175v1","created_at":"2026-05-18T00:24:27.136923+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.01175","created_at":"2026-05-18T00:24:27.136923+00:00"},{"alias_kind":"pith_short_12","alias_value":"VXWT7M7XUWG6","created_at":"2026-05-18T12:32:59.047623+00:00"},{"alias_kind":"pith_short_16","alias_value":"VXWT7M7XUWG66ZD7","created_at":"2026-05-18T12:32:59.047623+00:00"},{"alias_kind":"pith_short_8","alias_value":"VXWT7M7X","created_at":"2026-05-18T12:32:59.047623+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/VXWT7M7XUWG66ZD7WIV5YUIRC3","json":"https://pith.science/pith/VXWT7M7XUWG66ZD7WIV5YUIRC3.json","graph_json":"https://pith.science/api/pith-number/VXWT7M7XUWG66ZD7WIV5YUIRC3/graph.json","events_json":"https://pith.science/api/pith-number/VXWT7M7XUWG66ZD7WIV5YUIRC3/events.json","paper":"https://pith.science/paper/VXWT7M7X"},"agent_actions":{"view_html":"https://pith.science/pith/VXWT7M7XUWG66ZD7WIV5YUIRC3","download_json":"https://pith.science/pith/VXWT7M7XUWG66ZD7WIV5YUIRC3.json","view_paper":"https://pith.science/paper/VXWT7M7X","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1802.01175&json=true","fetch_graph":"https://pith.science/api/pith-number/VXWT7M7XUWG66ZD7WIV5YUIRC3/graph.json","fetch_events":"https://pith.science/api/pith-number/VXWT7M7XUWG66ZD7WIV5YUIRC3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VXWT7M7XUWG66ZD7WIV5YUIRC3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VXWT7M7XUWG66ZD7WIV5YUIRC3/action/storage_attestation","attest_author":"https://pith.science/pith/VXWT7M7XUWG66ZD7WIV5YUIRC3/action/author_attestation","sign_citation":"https://pith.science/pith/VXWT7M7XUWG66ZD7WIV5YUIRC3/action/citation_signature","submit_replication":"https://pith.science/pith/VXWT7M7XUWG66ZD7WIV5YUIRC3/action/replication_record"}},"created_at":"2026-05-18T00:24:27.136923+00:00","updated_at":"2026-05-18T00:24:27.136923+00:00"}