{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:HIB7JK3QYNSHGYIGGLFPZ2QAFD","short_pith_number":"pith:HIB7JK3Q","schema_version":"1.0","canonical_sha256":"3a03f4ab70c36473610632cafcea0028c27ce05951e7ed13d4b7e187e661a9f8","source":{"kind":"arxiv","id":"1407.5620","version":2},"attestation_state":"computed","paper":{"title":"Scalable Tight-Binding Model for Graphene","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Christian Sch\\\"onenberger, Endre T\\'ov\\'ari, Fedor Tkatschenko, Klaus Richter, Markus Weiss, Ming-Hao Liu, P\\'eter Makk, Peter Rickhaus, Romain Maurand","submitted_at":"2014-07-21T14:43:56Z","abstract_excerpt":"Artificial graphene consisting of honeycomb lattices other than the atomic layer of carbon has been shown to exhibit electronic properties similar to real graphene. Here, we reverse the argument to show that transport properties of real graphene can be captured by simulations using \"theoretical artificial graphene.\" To prove this, we first derive a simple condition, along with its restrictions, to achieve band structure invariance for a scalable graphene lattice. We then present transport measurements for an ultraclean suspended single-layer graphene pn junction device, where ballistic transpo"},"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":"1407.5620","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-07-21T14:43:56Z","cross_cats_sorted":[],"title_canon_sha256":"71d23c2e8134dad38122f87d6cfbc0e38aaa7ff9e8b8b48a33d0f4e78a995529","abstract_canon_sha256":"a9de4e751ae4dba9623d206b05cd88212e014d3837e5172ac8e3645411d20ab1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:28:55.070887Z","signature_b64":"oE7WsNtxKBghqVqd5+yQYlw6yzZKEHnoBe1DFNcAcpwkLkERWyWqedYFwsdIfrked7ndqV3NeQ31AvDIl2ZEBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3a03f4ab70c36473610632cafcea0028c27ce05951e7ed13d4b7e187e661a9f8","last_reissued_at":"2026-05-18T02:28:55.070539Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:28:55.070539Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scalable Tight-Binding Model for Graphene","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Christian Sch\\\"onenberger, Endre T\\'ov\\'ari, Fedor Tkatschenko, Klaus Richter, Markus Weiss, Ming-Hao Liu, P\\'eter Makk, Peter Rickhaus, Romain Maurand","submitted_at":"2014-07-21T14:43:56Z","abstract_excerpt":"Artificial graphene consisting of honeycomb lattices other than the atomic layer of carbon has been shown to exhibit electronic properties similar to real graphene. Here, we reverse the argument to show that transport properties of real graphene can be captured by simulations using \"theoretical artificial graphene.\" To prove this, we first derive a simple condition, along with its restrictions, to achieve band structure invariance for a scalable graphene lattice. We then present transport measurements for an ultraclean suspended single-layer graphene pn junction device, where ballistic transpo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.5620","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":"1407.5620","created_at":"2026-05-18T02:28:55.070593+00:00"},{"alias_kind":"arxiv_version","alias_value":"1407.5620v2","created_at":"2026-05-18T02:28:55.070593+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.5620","created_at":"2026-05-18T02:28:55.070593+00:00"},{"alias_kind":"pith_short_12","alias_value":"HIB7JK3QYNSH","created_at":"2026-05-18T12:28:30.664211+00:00"},{"alias_kind":"pith_short_16","alias_value":"HIB7JK3QYNSHGYIG","created_at":"2026-05-18T12:28:30.664211+00:00"},{"alias_kind":"pith_short_8","alias_value":"HIB7JK3Q","created_at":"2026-05-18T12:28:30.664211+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/HIB7JK3QYNSHGYIGGLFPZ2QAFD","json":"https://pith.science/pith/HIB7JK3QYNSHGYIGGLFPZ2QAFD.json","graph_json":"https://pith.science/api/pith-number/HIB7JK3QYNSHGYIGGLFPZ2QAFD/graph.json","events_json":"https://pith.science/api/pith-number/HIB7JK3QYNSHGYIGGLFPZ2QAFD/events.json","paper":"https://pith.science/paper/HIB7JK3Q"},"agent_actions":{"view_html":"https://pith.science/pith/HIB7JK3QYNSHGYIGGLFPZ2QAFD","download_json":"https://pith.science/pith/HIB7JK3QYNSHGYIGGLFPZ2QAFD.json","view_paper":"https://pith.science/paper/HIB7JK3Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1407.5620&json=true","fetch_graph":"https://pith.science/api/pith-number/HIB7JK3QYNSHGYIGGLFPZ2QAFD/graph.json","fetch_events":"https://pith.science/api/pith-number/HIB7JK3QYNSHGYIGGLFPZ2QAFD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HIB7JK3QYNSHGYIGGLFPZ2QAFD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HIB7JK3QYNSHGYIGGLFPZ2QAFD/action/storage_attestation","attest_author":"https://pith.science/pith/HIB7JK3QYNSHGYIGGLFPZ2QAFD/action/author_attestation","sign_citation":"https://pith.science/pith/HIB7JK3QYNSHGYIGGLFPZ2QAFD/action/citation_signature","submit_replication":"https://pith.science/pith/HIB7JK3QYNSHGYIGGLFPZ2QAFD/action/replication_record"}},"created_at":"2026-05-18T02:28:55.070593+00:00","updated_at":"2026-05-18T02:28:55.070593+00:00"}