{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:RDL5CV3KYLVTXNAQI2CQCWK5II","short_pith_number":"pith:RDL5CV3K","schema_version":"1.0","canonical_sha256":"88d7d1576ac2eb3bb410468501595d423af81bd6ae394e544537cae2e46bfe46","source":{"kind":"arxiv","id":"1310.1066","version":2},"attestation_state":"computed","paper":{"title":"Computation of the correlated metal-insulator transition in vanadium dioxide from first principles","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"Huihuo Zheng, Lucas K. Wagner","submitted_at":"2013-10-03T19:01:36Z","abstract_excerpt":"Vanadium dioxide(VO$_2$) is a paradigmatic example of a strongly correlated system that undergoes a metal-insulator transition at a structural phase transition. To date, this transition has necessitated significant post-hoc adjustments to theory in order to be described properly. Here we report standard state-of-the-art first principles quantum Monte Carlo (QMC) calculations of the structural dependence of the properties of VO$_2$. Using this technique, we simulate the interactions between electrons explicitly, which allows for the metal-insulator transition to naturally emerge, importantly wi"},"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":"1310.1066","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-10-03T19:01:36Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"27bf44f056fa10f4166c1d823c802af3d2fb0fac1ed809ceec3f5d62c79a0ac9","abstract_canon_sha256":"aa71c64061f1ba73167fec3dc65ccf911688931616eec121b77940f94e501b14"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:27:47.511688Z","signature_b64":"kJafYhDXCMN+hlc7k95NN+B1crMWa80nyBoK89pDXC9PO7DftEBw6L1dlJ1apYcylWEdh8abEYdDZ3FdcQwbCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"88d7d1576ac2eb3bb410468501595d423af81bd6ae394e544537cae2e46bfe46","last_reissued_at":"2026-05-18T00:27:47.511245Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:27:47.511245Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Computation of the correlated metal-insulator transition in vanadium dioxide from first principles","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"Huihuo Zheng, Lucas K. Wagner","submitted_at":"2013-10-03T19:01:36Z","abstract_excerpt":"Vanadium dioxide(VO$_2$) is a paradigmatic example of a strongly correlated system that undergoes a metal-insulator transition at a structural phase transition. To date, this transition has necessitated significant post-hoc adjustments to theory in order to be described properly. Here we report standard state-of-the-art first principles quantum Monte Carlo (QMC) calculations of the structural dependence of the properties of VO$_2$. Using this technique, we simulate the interactions between electrons explicitly, which allows for the metal-insulator transition to naturally emerge, importantly wi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.1066","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":"1310.1066","created_at":"2026-05-18T00:27:47.511330+00:00"},{"alias_kind":"arxiv_version","alias_value":"1310.1066v2","created_at":"2026-05-18T00:27:47.511330+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.1066","created_at":"2026-05-18T00:27:47.511330+00:00"},{"alias_kind":"pith_short_12","alias_value":"RDL5CV3KYLVT","created_at":"2026-05-18T12:27:57.521954+00:00"},{"alias_kind":"pith_short_16","alias_value":"RDL5CV3KYLVTXNAQ","created_at":"2026-05-18T12:27:57.521954+00:00"},{"alias_kind":"pith_short_8","alias_value":"RDL5CV3K","created_at":"2026-05-18T12:27:57.521954+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/RDL5CV3KYLVTXNAQI2CQCWK5II","json":"https://pith.science/pith/RDL5CV3KYLVTXNAQI2CQCWK5II.json","graph_json":"https://pith.science/api/pith-number/RDL5CV3KYLVTXNAQI2CQCWK5II/graph.json","events_json":"https://pith.science/api/pith-number/RDL5CV3KYLVTXNAQI2CQCWK5II/events.json","paper":"https://pith.science/paper/RDL5CV3K"},"agent_actions":{"view_html":"https://pith.science/pith/RDL5CV3KYLVTXNAQI2CQCWK5II","download_json":"https://pith.science/pith/RDL5CV3KYLVTXNAQI2CQCWK5II.json","view_paper":"https://pith.science/paper/RDL5CV3K","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1310.1066&json=true","fetch_graph":"https://pith.science/api/pith-number/RDL5CV3KYLVTXNAQI2CQCWK5II/graph.json","fetch_events":"https://pith.science/api/pith-number/RDL5CV3KYLVTXNAQI2CQCWK5II/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RDL5CV3KYLVTXNAQI2CQCWK5II/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RDL5CV3KYLVTXNAQI2CQCWK5II/action/storage_attestation","attest_author":"https://pith.science/pith/RDL5CV3KYLVTXNAQI2CQCWK5II/action/author_attestation","sign_citation":"https://pith.science/pith/RDL5CV3KYLVTXNAQI2CQCWK5II/action/citation_signature","submit_replication":"https://pith.science/pith/RDL5CV3KYLVTXNAQI2CQCWK5II/action/replication_record"}},"created_at":"2026-05-18T00:27:47.511330+00:00","updated_at":"2026-05-18T00:27:47.511330+00:00"}