{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:LRFV5QNW54MYXVDVQNEHZUKEHW","short_pith_number":"pith:LRFV5QNW","schema_version":"1.0","canonical_sha256":"5c4b5ec1b6ef198bd47583487cd1443d906178a666e34fbb7468ef6fc6395713","source":{"kind":"arxiv","id":"1008.2044","version":1},"attestation_state":"computed","paper":{"title":"Casimir effect of electromagnetic field in Randall-Sundrum spacetime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"L.P. Teo","submitted_at":"2010-08-12T04:44:57Z","abstract_excerpt":"We study the finite temperature Casimir effect on a pair of parallel perfectly conducting plates in Randall-Sundrum model without using scalar field analogy. Two different ways of interpreting perfectly conducting conditions are discussed. The conventional way that uses perfectly conducting condition induced from 5D leads to three discrete mode corrections. This is very different from the result obtained from imposing 4D perfectly conducting conditions on the 4D massless and massive vector fields obtained by decomposing the 5D electromagnetic field. The latter only contains two discrete mode c"},"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":"1008.2044","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-08-12T04:44:57Z","cross_cats_sorted":[],"title_canon_sha256":"03d0ac317f40bdba6de1f3e4a5e3afb2a5e3e9edece7b239fa2dbc08b8721fee","abstract_canon_sha256":"7ac765ef74d2e29d895dd0f738b24aaa133a099d3bdea243006a346ae39e5bb2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:33:08.409508Z","signature_b64":"pG7aDNA1nAYCSCBQ/1plBexonkzfQi7sp209A3vi9njS1vEY04uXK4wBfu4f2CECT+ILX9P3wErJaDDwS/gGBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5c4b5ec1b6ef198bd47583487cd1443d906178a666e34fbb7468ef6fc6395713","last_reissued_at":"2026-05-18T02:33:08.409093Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:33:08.409093Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Casimir effect of electromagnetic field in Randall-Sundrum spacetime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"L.P. Teo","submitted_at":"2010-08-12T04:44:57Z","abstract_excerpt":"We study the finite temperature Casimir effect on a pair of parallel perfectly conducting plates in Randall-Sundrum model without using scalar field analogy. Two different ways of interpreting perfectly conducting conditions are discussed. The conventional way that uses perfectly conducting condition induced from 5D leads to three discrete mode corrections. This is very different from the result obtained from imposing 4D perfectly conducting conditions on the 4D massless and massive vector fields obtained by decomposing the 5D electromagnetic field. The latter only contains two discrete mode c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1008.2044","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":""},"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":"1008.2044","created_at":"2026-05-18T02:33:08.409155+00:00"},{"alias_kind":"arxiv_version","alias_value":"1008.2044v1","created_at":"2026-05-18T02:33:08.409155+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1008.2044","created_at":"2026-05-18T02:33:08.409155+00:00"},{"alias_kind":"pith_short_12","alias_value":"LRFV5QNW54MY","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_16","alias_value":"LRFV5QNW54MYXVDV","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_8","alias_value":"LRFV5QNW","created_at":"2026-05-18T12:26:10.704358+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/LRFV5QNW54MYXVDVQNEHZUKEHW","json":"https://pith.science/pith/LRFV5QNW54MYXVDVQNEHZUKEHW.json","graph_json":"https://pith.science/api/pith-number/LRFV5QNW54MYXVDVQNEHZUKEHW/graph.json","events_json":"https://pith.science/api/pith-number/LRFV5QNW54MYXVDVQNEHZUKEHW/events.json","paper":"https://pith.science/paper/LRFV5QNW"},"agent_actions":{"view_html":"https://pith.science/pith/LRFV5QNW54MYXVDVQNEHZUKEHW","download_json":"https://pith.science/pith/LRFV5QNW54MYXVDVQNEHZUKEHW.json","view_paper":"https://pith.science/paper/LRFV5QNW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1008.2044&json=true","fetch_graph":"https://pith.science/api/pith-number/LRFV5QNW54MYXVDVQNEHZUKEHW/graph.json","fetch_events":"https://pith.science/api/pith-number/LRFV5QNW54MYXVDVQNEHZUKEHW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LRFV5QNW54MYXVDVQNEHZUKEHW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LRFV5QNW54MYXVDVQNEHZUKEHW/action/storage_attestation","attest_author":"https://pith.science/pith/LRFV5QNW54MYXVDVQNEHZUKEHW/action/author_attestation","sign_citation":"https://pith.science/pith/LRFV5QNW54MYXVDVQNEHZUKEHW/action/citation_signature","submit_replication":"https://pith.science/pith/LRFV5QNW54MYXVDVQNEHZUKEHW/action/replication_record"}},"created_at":"2026-05-18T02:33:08.409155+00:00","updated_at":"2026-05-18T02:33:08.409155+00:00"}