{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:GVEM2H4IEP4KHCUF4S3GMT3VIW","short_pith_number":"pith:GVEM2H4I","schema_version":"1.0","canonical_sha256":"3548cd1f8823f8a38a85e4b6664f75459c0f686db8eb14e8b1511a9d096fa5d8","source":{"kind":"arxiv","id":"0812.0557","version":1},"attestation_state":"computed","paper":{"title":"Computation of Casimir forces for dielectrics or intrinsic semiconductors based on the Boltzmann transport equation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Diego A. R. Dalvit, Steve K. Lamoreaux","submitted_at":"2008-12-02T17:41:00Z","abstract_excerpt":"The interaction between drifting carriers and traveling electromagnetic waves is considered within the context of the classical Boltzmann transport equation to compute the Casimir-Lifshitz force between media with small density of charge carriers, including dielectrics and intrinsic semiconductors. We expand upon our previous work [Phys. Rev. Lett. {\\bf 101}, 163203 (2008)] and derive in some detail the frequency-dependent reflection amplitudes in this theory and compute the corresponding Casimir free energy for a parallel plate configuration. We critically discuss the the issue of verificatio"},"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":"0812.0557","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2008-12-02T17:41:00Z","cross_cats_sorted":[],"title_canon_sha256":"b8294af7c831ea6d32ab43b10867ac7c161d0b8df922c6083af6ad36e213dbf4","abstract_canon_sha256":"792a256444f3b25e6537d631ca9d413cd0dc1f72a128f95e559275cf2702184f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:15:12.184615Z","signature_b64":"dYDJWpXDg4fwx/E8raeZ7Dkb7AhhB0RRHVbigzcHwqkGVdzXkKRAFzBkN7CW7ZBfjNg8WqwcUEcf+8BHCjgYDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3548cd1f8823f8a38a85e4b6664f75459c0f686db8eb14e8b1511a9d096fa5d8","last_reissued_at":"2026-05-18T02:15:12.183906Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:15:12.183906Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Computation of Casimir forces for dielectrics or intrinsic semiconductors based on the Boltzmann transport equation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Diego A. R. Dalvit, Steve K. Lamoreaux","submitted_at":"2008-12-02T17:41:00Z","abstract_excerpt":"The interaction between drifting carriers and traveling electromagnetic waves is considered within the context of the classical Boltzmann transport equation to compute the Casimir-Lifshitz force between media with small density of charge carriers, including dielectrics and intrinsic semiconductors. We expand upon our previous work [Phys. Rev. Lett. {\\bf 101}, 163203 (2008)] and derive in some detail the frequency-dependent reflection amplitudes in this theory and compute the corresponding Casimir free energy for a parallel plate configuration. We critically discuss the the issue of verificatio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0812.0557","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":"0812.0557","created_at":"2026-05-18T02:15:12.184012+00:00"},{"alias_kind":"arxiv_version","alias_value":"0812.0557v1","created_at":"2026-05-18T02:15:12.184012+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0812.0557","created_at":"2026-05-18T02:15:12.184012+00:00"},{"alias_kind":"pith_short_12","alias_value":"GVEM2H4IEP4K","created_at":"2026-05-18T12:25:57.157939+00:00"},{"alias_kind":"pith_short_16","alias_value":"GVEM2H4IEP4KHCUF","created_at":"2026-05-18T12:25:57.157939+00:00"},{"alias_kind":"pith_short_8","alias_value":"GVEM2H4I","created_at":"2026-05-18T12:25:57.157939+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/GVEM2H4IEP4KHCUF4S3GMT3VIW","json":"https://pith.science/pith/GVEM2H4IEP4KHCUF4S3GMT3VIW.json","graph_json":"https://pith.science/api/pith-number/GVEM2H4IEP4KHCUF4S3GMT3VIW/graph.json","events_json":"https://pith.science/api/pith-number/GVEM2H4IEP4KHCUF4S3GMT3VIW/events.json","paper":"https://pith.science/paper/GVEM2H4I"},"agent_actions":{"view_html":"https://pith.science/pith/GVEM2H4IEP4KHCUF4S3GMT3VIW","download_json":"https://pith.science/pith/GVEM2H4IEP4KHCUF4S3GMT3VIW.json","view_paper":"https://pith.science/paper/GVEM2H4I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0812.0557&json=true","fetch_graph":"https://pith.science/api/pith-number/GVEM2H4IEP4KHCUF4S3GMT3VIW/graph.json","fetch_events":"https://pith.science/api/pith-number/GVEM2H4IEP4KHCUF4S3GMT3VIW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GVEM2H4IEP4KHCUF4S3GMT3VIW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GVEM2H4IEP4KHCUF4S3GMT3VIW/action/storage_attestation","attest_author":"https://pith.science/pith/GVEM2H4IEP4KHCUF4S3GMT3VIW/action/author_attestation","sign_citation":"https://pith.science/pith/GVEM2H4IEP4KHCUF4S3GMT3VIW/action/citation_signature","submit_replication":"https://pith.science/pith/GVEM2H4IEP4KHCUF4S3GMT3VIW/action/replication_record"}},"created_at":"2026-05-18T02:15:12.184012+00:00","updated_at":"2026-05-18T02:15:12.184012+00:00"}