{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:L3CYD2FY75XKDAEJEIOBCXGRXT","short_pith_number":"pith:L3CYD2FY","schema_version":"1.0","canonical_sha256":"5ec581e8b8ff6ea18089221c115cd1bcfad52365a79d8b04f520114b98c3ad1a","source":{"kind":"arxiv","id":"2606.28591","version":1},"attestation_state":"computed","paper":{"title":"Graphene as a Tunable Nonradiative Bath for Moir\\'e Excitons","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Katsunori Wakabayashi","submitted_at":"2026-06-26T20:36:14Z","abstract_excerpt":"A minimal theory for the nonradiative transfer of energy from a two-dimensional (2D) exciton -- especially a moir\\'e-localized exciton -- to a nearby graphene layer is presented. Starting from Fermi's golden rule, the transfer rate is written as the overlap between the exciton near-field spectrum and the long-wavelength electronic loss function of graphene, weighted by an exciton form factor. In the point-dipole limit the framework reproduces the established $\\GET\\propto z^{-4}$ law for energy transfer to graphene. Including the finite spatial extent of a moir\\'e exciton through a Gaussian for"},"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":"2606.28591","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-06-26T20:36:14Z","cross_cats_sorted":[],"title_canon_sha256":"52140a3bf0e04d9e5951bbb9befa0eeb00cef499b99dcc07f4c8eb5acdc3cc47","abstract_canon_sha256":"9858db814c54ae71035747db0a0773c7a4f09e860eba48a0bb7bcdbf1cb3375f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-30T00:15:20.067686Z","signature_b64":"a80AL+xnQ3SmisGNgAd/4jyntj53qAZk0Z4IMPZ3asxCTBxNd9UZvi35lrMUQ2kRzQMU3qctjWCA16qb/RgOBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5ec581e8b8ff6ea18089221c115cd1bcfad52365a79d8b04f520114b98c3ad1a","last_reissued_at":"2026-06-30T00:15:20.067180Z","signature_status":"signed_v1","first_computed_at":"2026-06-30T00:15:20.067180Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Graphene as a Tunable Nonradiative Bath for Moir\\'e Excitons","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Katsunori Wakabayashi","submitted_at":"2026-06-26T20:36:14Z","abstract_excerpt":"A minimal theory for the nonradiative transfer of energy from a two-dimensional (2D) exciton -- especially a moir\\'e-localized exciton -- to a nearby graphene layer is presented. Starting from Fermi's golden rule, the transfer rate is written as the overlap between the exciton near-field spectrum and the long-wavelength electronic loss function of graphene, weighted by an exciton form factor. In the point-dipole limit the framework reproduces the established $\\GET\\propto z^{-4}$ law for energy transfer to graphene. Including the finite spatial extent of a moir\\'e exciton through a Gaussian for"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.28591","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/2606.28591/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":"2606.28591","created_at":"2026-06-30T00:15:20.067256+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.28591v1","created_at":"2026-06-30T00:15:20.067256+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.28591","created_at":"2026-06-30T00:15:20.067256+00:00"},{"alias_kind":"pith_short_12","alias_value":"L3CYD2FY75XK","created_at":"2026-06-30T00:15:20.067256+00:00"},{"alias_kind":"pith_short_16","alias_value":"L3CYD2FY75XKDAEJ","created_at":"2026-06-30T00:15:20.067256+00:00"},{"alias_kind":"pith_short_8","alias_value":"L3CYD2FY","created_at":"2026-06-30T00:15:20.067256+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/L3CYD2FY75XKDAEJEIOBCXGRXT","json":"https://pith.science/pith/L3CYD2FY75XKDAEJEIOBCXGRXT.json","graph_json":"https://pith.science/api/pith-number/L3CYD2FY75XKDAEJEIOBCXGRXT/graph.json","events_json":"https://pith.science/api/pith-number/L3CYD2FY75XKDAEJEIOBCXGRXT/events.json","paper":"https://pith.science/paper/L3CYD2FY"},"agent_actions":{"view_html":"https://pith.science/pith/L3CYD2FY75XKDAEJEIOBCXGRXT","download_json":"https://pith.science/pith/L3CYD2FY75XKDAEJEIOBCXGRXT.json","view_paper":"https://pith.science/paper/L3CYD2FY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.28591&json=true","fetch_graph":"https://pith.science/api/pith-number/L3CYD2FY75XKDAEJEIOBCXGRXT/graph.json","fetch_events":"https://pith.science/api/pith-number/L3CYD2FY75XKDAEJEIOBCXGRXT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/L3CYD2FY75XKDAEJEIOBCXGRXT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/L3CYD2FY75XKDAEJEIOBCXGRXT/action/storage_attestation","attest_author":"https://pith.science/pith/L3CYD2FY75XKDAEJEIOBCXGRXT/action/author_attestation","sign_citation":"https://pith.science/pith/L3CYD2FY75XKDAEJEIOBCXGRXT/action/citation_signature","submit_replication":"https://pith.science/pith/L3CYD2FY75XKDAEJEIOBCXGRXT/action/replication_record"}},"created_at":"2026-06-30T00:15:20.067256+00:00","updated_at":"2026-06-30T00:15:20.067256+00:00"}