{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:HA2FLJKTXT4QVQ6AB7F2C4D74D","short_pith_number":"pith:HA2FLJKT","schema_version":"1.0","canonical_sha256":"383455a553bcf90ac3c00fcba1707fe0d3da6fae9ac5370f4dee3b33f1d446e8","source":{"kind":"arxiv","id":"hep-th/0610114","version":1},"attestation_state":"computed","paper":{"title":"Casimir densities for two spherical branes in Rindler-like spacetimes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.A. Saharian, M.R. Setare","submitted_at":"2006-10-10T13:25:25Z","abstract_excerpt":"Wightman function, the vacuum expectation values of the field square and the energy-momentum tensor are evaluated for a scalar field obeying the Robin boundary conditions on two spherical branes in (D+1)-dimensional Rindler-like spacetime $Ri\\times S^{D-1}$, with a two-dimensional Rindler spacetime $Ri$. This spacetime approximates the near horizon geometry of (D+1)-dimensional black hole. By using the generalized Abel-Plana formula, the vacuum expectation values are presented as the sum of single brane and second brane induced parts. Various limiting cases are studied. The vacuum forces actin"},"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":"hep-th/0610114","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2006-10-10T13:25:25Z","cross_cats_sorted":[],"title_canon_sha256":"2e6990a2a7ccc2f8c5ca0e19f96f13273b0b498b76c724aa5ac06667bacfd470","abstract_canon_sha256":"75209c50c3812ffed55c49a19f66d4ff65330dc4fff66826bbc5bc37779150d2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:38:26.348934Z","signature_b64":"lEscPj7XdK+gpbHmqmnZ8OiXO5xNkodQfA5r77vYRN+Y3UsRQq/+WinSCpTPo7HehmnNs75WClylkMQd6iVLAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"383455a553bcf90ac3c00fcba1707fe0d3da6fae9ac5370f4dee3b33f1d446e8","last_reissued_at":"2026-05-18T04:38:26.348538Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:38:26.348538Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Casimir densities for two spherical branes in Rindler-like spacetimes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.A. Saharian, M.R. Setare","submitted_at":"2006-10-10T13:25:25Z","abstract_excerpt":"Wightman function, the vacuum expectation values of the field square and the energy-momentum tensor are evaluated for a scalar field obeying the Robin boundary conditions on two spherical branes in (D+1)-dimensional Rindler-like spacetime $Ri\\times S^{D-1}$, with a two-dimensional Rindler spacetime $Ri$. This spacetime approximates the near horizon geometry of (D+1)-dimensional black hole. By using the generalized Abel-Plana formula, the vacuum expectation values are presented as the sum of single brane and second brane induced parts. Various limiting cases are studied. The vacuum forces actin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0610114","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":"hep-th/0610114","created_at":"2026-05-18T04:38:26.348600+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0610114v1","created_at":"2026-05-18T04:38:26.348600+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0610114","created_at":"2026-05-18T04:38:26.348600+00:00"},{"alias_kind":"pith_short_12","alias_value":"HA2FLJKTXT4Q","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_16","alias_value":"HA2FLJKTXT4QVQ6A","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_8","alias_value":"HA2FLJKT","created_at":"2026-05-18T12:25:53.939244+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/HA2FLJKTXT4QVQ6AB7F2C4D74D","json":"https://pith.science/pith/HA2FLJKTXT4QVQ6AB7F2C4D74D.json","graph_json":"https://pith.science/api/pith-number/HA2FLJKTXT4QVQ6AB7F2C4D74D/graph.json","events_json":"https://pith.science/api/pith-number/HA2FLJKTXT4QVQ6AB7F2C4D74D/events.json","paper":"https://pith.science/paper/HA2FLJKT"},"agent_actions":{"view_html":"https://pith.science/pith/HA2FLJKTXT4QVQ6AB7F2C4D74D","download_json":"https://pith.science/pith/HA2FLJKTXT4QVQ6AB7F2C4D74D.json","view_paper":"https://pith.science/paper/HA2FLJKT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0610114&json=true","fetch_graph":"https://pith.science/api/pith-number/HA2FLJKTXT4QVQ6AB7F2C4D74D/graph.json","fetch_events":"https://pith.science/api/pith-number/HA2FLJKTXT4QVQ6AB7F2C4D74D/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HA2FLJKTXT4QVQ6AB7F2C4D74D/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HA2FLJKTXT4QVQ6AB7F2C4D74D/action/storage_attestation","attest_author":"https://pith.science/pith/HA2FLJKTXT4QVQ6AB7F2C4D74D/action/author_attestation","sign_citation":"https://pith.science/pith/HA2FLJKTXT4QVQ6AB7F2C4D74D/action/citation_signature","submit_replication":"https://pith.science/pith/HA2FLJKTXT4QVQ6AB7F2C4D74D/action/replication_record"}},"created_at":"2026-05-18T04:38:26.348600+00:00","updated_at":"2026-05-18T04:38:26.348600+00:00"}