{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:XNXDVFM46AXRXUPMIXD4WPDERA","short_pith_number":"pith:XNXDVFM4","schema_version":"1.0","canonical_sha256":"bb6e3a959cf02f1bd1ec45c7cb3c648823de886cfec76dfdfbd07fa9f825572d","source":{"kind":"arxiv","id":"2505.12799","version":1},"attestation_state":"computed","paper":{"title":"Resolving self-cavity effects in two-dimensional quantum materials","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"Alexander M. Potts, Guido Meier, Gunda Kipp, Hope M. Bretscher, James W. McIver, Marios H. Michael, Matthew W. Day, Toru Matsuyama","submitted_at":"2025-05-19T07:31:30Z","abstract_excerpt":"Two-dimensional materials and van der Waals (vdW) heterostructures host many strongly correlated and topological quantum phases on the $\\sim$ meV energy scale. Direct electrodynamical signatures of such states are thus expected to appear in the terahertz (THz) frequency range (1 THz $\\sim$ 4 meV). Because the typical size of vdW heterostructures ($\\sim$10 $\\mu m$) is much smaller than the diffraction limit of THz light, probing THz optical conductivities necessitates the use of near-field optical probes. However, interpreting the response of such near-field probes is complicated by finite-size"},"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":"2505.12799","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-05-19T07:31:30Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"48977345efb21cd3671868479d02a13e90c5fc37a54f1b44e60bb9d2a5a0d0f3","abstract_canon_sha256":"6c9db1b657f26b49066e7b65c76b317229cf0018658705735930517b4cae3ebc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:05:09.874911Z","signature_b64":"TYUbx6J9KWZp/8nnsiT8EMzn6gq3/5q6/X8/68seaSXsBBas/fxSgF/1nDZByZf0EZlF2O3U9bHSGudA0YtyBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bb6e3a959cf02f1bd1ec45c7cb3c648823de886cfec76dfdfbd07fa9f825572d","last_reissued_at":"2026-07-05T11:05:09.874412Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:05:09.874412Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Resolving self-cavity effects in two-dimensional quantum materials","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"Alexander M. Potts, Guido Meier, Gunda Kipp, Hope M. Bretscher, James W. McIver, Marios H. Michael, Matthew W. Day, Toru Matsuyama","submitted_at":"2025-05-19T07:31:30Z","abstract_excerpt":"Two-dimensional materials and van der Waals (vdW) heterostructures host many strongly correlated and topological quantum phases on the $\\sim$ meV energy scale. Direct electrodynamical signatures of such states are thus expected to appear in the terahertz (THz) frequency range (1 THz $\\sim$ 4 meV). Because the typical size of vdW heterostructures ($\\sim$10 $\\mu m$) is much smaller than the diffraction limit of THz light, probing THz optical conductivities necessitates the use of near-field optical probes. However, interpreting the response of such near-field probes is complicated by finite-size"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.12799","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/2505.12799/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":"2505.12799","created_at":"2026-07-05T11:05:09.874475+00:00"},{"alias_kind":"arxiv_version","alias_value":"2505.12799v1","created_at":"2026-07-05T11:05:09.874475+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.12799","created_at":"2026-07-05T11:05:09.874475+00:00"},{"alias_kind":"pith_short_12","alias_value":"XNXDVFM46AXR","created_at":"2026-07-05T11:05:09.874475+00:00"},{"alias_kind":"pith_short_16","alias_value":"XNXDVFM46AXRXUPM","created_at":"2026-07-05T11:05:09.874475+00:00"},{"alias_kind":"pith_short_8","alias_value":"XNXDVFM4","created_at":"2026-07-05T11:05:09.874475+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.10624","citing_title":"Terahertz electrodynamics in a zero-field Wigner crystal","ref_index":32,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XNXDVFM46AXRXUPMIXD4WPDERA","json":"https://pith.science/pith/XNXDVFM46AXRXUPMIXD4WPDERA.json","graph_json":"https://pith.science/api/pith-number/XNXDVFM46AXRXUPMIXD4WPDERA/graph.json","events_json":"https://pith.science/api/pith-number/XNXDVFM46AXRXUPMIXD4WPDERA/events.json","paper":"https://pith.science/paper/XNXDVFM4"},"agent_actions":{"view_html":"https://pith.science/pith/XNXDVFM46AXRXUPMIXD4WPDERA","download_json":"https://pith.science/pith/XNXDVFM46AXRXUPMIXD4WPDERA.json","view_paper":"https://pith.science/paper/XNXDVFM4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2505.12799&json=true","fetch_graph":"https://pith.science/api/pith-number/XNXDVFM46AXRXUPMIXD4WPDERA/graph.json","fetch_events":"https://pith.science/api/pith-number/XNXDVFM46AXRXUPMIXD4WPDERA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XNXDVFM46AXRXUPMIXD4WPDERA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XNXDVFM46AXRXUPMIXD4WPDERA/action/storage_attestation","attest_author":"https://pith.science/pith/XNXDVFM46AXRXUPMIXD4WPDERA/action/author_attestation","sign_citation":"https://pith.science/pith/XNXDVFM46AXRXUPMIXD4WPDERA/action/citation_signature","submit_replication":"https://pith.science/pith/XNXDVFM46AXRXUPMIXD4WPDERA/action/replication_record"}},"created_at":"2026-07-05T11:05:09.874475+00:00","updated_at":"2026-07-05T11:05:09.874475+00:00"}