{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:5UT6YL6HROXL4SE2T2YTDKA4U7","short_pith_number":"pith:5UT6YL6H","schema_version":"1.0","canonical_sha256":"ed27ec2fc78baebe489a9eb131a81ca7ea2e56e9bfc73272b921f528f1e2b2e1","source":{"kind":"arxiv","id":"2411.18205","version":1},"attestation_state":"computed","paper":{"title":"Nature of metallic and insulating domains in the CDW system 1T-TaSe2","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"A. Georges, A. Hunter, A. Tamai, C. Polley, C. Witteveen, F. Baumberger, F. B. Kugler, F.O. von Rohr, F. Petocchi, G. Carbone, G. Gatti, J. Osiecki, M. Straub, S. Mandloi, Y. Alexanian","submitted_at":"2024-11-27T10:30:08Z","abstract_excerpt":"We study the electronic structure of bulk 1T-TaSe$_2$ in the charge density wave phase at low temperature. Our spatially and angle resolved photoemission (ARPES) data show insulating areas coexisting with metallic regions characterized by a chiral Fermi surface and moderately correlated quasiparticle bands. Additionally, high-resolution laser ARPES reveals variations in the metallic regions, with series of low-energy states, whose energy, number and dispersion can be explained by the formation of quantum well states of different thicknesses. Dynamical mean field theory calculations show that t"},"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":"2411.18205","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-11-27T10:30:08Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"977b01c318ba4e3911230ac8c7c20abd9dfa31e821805656da692310c1b09593","abstract_canon_sha256":"18b667ccb035962f152754ff35e9ecc6114ac7711cdc625aa7942e903a18ba7b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:58:22.212040Z","signature_b64":"LRaWNOzFn3X8MaGtMoQGrmnjIqWNJ05yixPE8VpIUmdU2KSWkhbBfsrhnMsQ8pIp+WWaHgz+/jvMua+EoNH0BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ed27ec2fc78baebe489a9eb131a81ca7ea2e56e9bfc73272b921f528f1e2b2e1","last_reissued_at":"2026-07-05T11:58:22.211547Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:58:22.211547Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nature of metallic and insulating domains in the CDW system 1T-TaSe2","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"A. Georges, A. Hunter, A. Tamai, C. Polley, C. Witteveen, F. Baumberger, F. B. Kugler, F.O. von Rohr, F. Petocchi, G. Carbone, G. Gatti, J. Osiecki, M. Straub, S. Mandloi, Y. Alexanian","submitted_at":"2024-11-27T10:30:08Z","abstract_excerpt":"We study the electronic structure of bulk 1T-TaSe$_2$ in the charge density wave phase at low temperature. Our spatially and angle resolved photoemission (ARPES) data show insulating areas coexisting with metallic regions characterized by a chiral Fermi surface and moderately correlated quasiparticle bands. Additionally, high-resolution laser ARPES reveals variations in the metallic regions, with series of low-energy states, whose energy, number and dispersion can be explained by the formation of quantum well states of different thicknesses. Dynamical mean field theory calculations show that t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.18205","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2411.18205/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2411.18205","created_at":"2026-07-05T11:58:22.211607+00:00"},{"alias_kind":"arxiv_version","alias_value":"2411.18205v1","created_at":"2026-07-05T11:58:22.211607+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.18205","created_at":"2026-07-05T11:58:22.211607+00:00"},{"alias_kind":"pith_short_12","alias_value":"5UT6YL6HROXL","created_at":"2026-07-05T11:58:22.211607+00:00"},{"alias_kind":"pith_short_16","alias_value":"5UT6YL6HROXL4SE2","created_at":"2026-07-05T11:58:22.211607+00:00"},{"alias_kind":"pith_short_8","alias_value":"5UT6YL6H","created_at":"2026-07-05T11:58:22.211607+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.28259","citing_title":"Change in charge density wave order beyond the Lifshitz transition in 2H-Ta\\textsubscript{1$\\pm\\delta$}S\\textsubscript{2}","ref_index":4,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5UT6YL6HROXL4SE2T2YTDKA4U7","json":"https://pith.science/pith/5UT6YL6HROXL4SE2T2YTDKA4U7.json","graph_json":"https://pith.science/api/pith-number/5UT6YL6HROXL4SE2T2YTDKA4U7/graph.json","events_json":"https://pith.science/api/pith-number/5UT6YL6HROXL4SE2T2YTDKA4U7/events.json","paper":"https://pith.science/paper/5UT6YL6H"},"agent_actions":{"view_html":"https://pith.science/pith/5UT6YL6HROXL4SE2T2YTDKA4U7","download_json":"https://pith.science/pith/5UT6YL6HROXL4SE2T2YTDKA4U7.json","view_paper":"https://pith.science/paper/5UT6YL6H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2411.18205&json=true","fetch_graph":"https://pith.science/api/pith-number/5UT6YL6HROXL4SE2T2YTDKA4U7/graph.json","fetch_events":"https://pith.science/api/pith-number/5UT6YL6HROXL4SE2T2YTDKA4U7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5UT6YL6HROXL4SE2T2YTDKA4U7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5UT6YL6HROXL4SE2T2YTDKA4U7/action/storage_attestation","attest_author":"https://pith.science/pith/5UT6YL6HROXL4SE2T2YTDKA4U7/action/author_attestation","sign_citation":"https://pith.science/pith/5UT6YL6HROXL4SE2T2YTDKA4U7/action/citation_signature","submit_replication":"https://pith.science/pith/5UT6YL6HROXL4SE2T2YTDKA4U7/action/replication_record"}},"created_at":"2026-07-05T11:58:22.211607+00:00","updated_at":"2026-07-05T11:58:22.211607+00:00"}