{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:J74YC2CYCQPYQZSRSJPOTORGDE","short_pith_number":"pith:J74YC2CY","schema_version":"1.0","canonical_sha256":"4ff9816858141f886651925ee9ba261930f830814046560db42acbe9549da2b6","source":{"kind":"arxiv","id":"2606.31610","version":1},"attestation_state":"computed","paper":{"title":"Nonequilibrium Casimir-Polder Force: Magnus-like Effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Francesco Intravaia, Kurt Busch, Maria Vittoria Gurrieri","submitted_at":"2026-06-30T12:58:28Z","abstract_excerpt":"The motion of a particle in vacuum near macroscopic bodies gives rise to a Magnus-like contribution to the nonequilibrium Casimir-Polder force. This effect originates from the interplay between particle dynamics and material-modified electromagnetic quantum fluctuations, inducing in the particle a direction-dependent angular momentum coupled to the electromagnetic field spin. The resulting drift force is proportional to the cross product of the particle's angular and translational velocities, revealing a rotational transport component in the nonequilibrium Casimir-Polder interaction. Our resul"},"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":"2606.31610","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2026-06-30T12:58:28Z","cross_cats_sorted":[],"title_canon_sha256":"226ae0b9134ea13fead8cdebd6fe2137e1f52a8bc084948c0a4187ac0901396f","abstract_canon_sha256":"34127ba70aca009fea240023596d1cd6a0452fc6116b512b939fab7eac8fb3ff"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-01T01:18:09.124476Z","signature_b64":"gLrng4Y8Lm6tLSWoQxYrF4O7cDvygV8QamqUfTtBZC/XvJD3P69VHYTW9t2Sgp2K2S9USf5JhJzYn3hXREJhAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4ff9816858141f886651925ee9ba261930f830814046560db42acbe9549da2b6","last_reissued_at":"2026-07-01T01:18:09.124055Z","signature_status":"signed_v1","first_computed_at":"2026-07-01T01:18:09.124055Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonequilibrium Casimir-Polder Force: Magnus-like Effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Francesco Intravaia, Kurt Busch, Maria Vittoria Gurrieri","submitted_at":"2026-06-30T12:58:28Z","abstract_excerpt":"The motion of a particle in vacuum near macroscopic bodies gives rise to a Magnus-like contribution to the nonequilibrium Casimir-Polder force. This effect originates from the interplay between particle dynamics and material-modified electromagnetic quantum fluctuations, inducing in the particle a direction-dependent angular momentum coupled to the electromagnetic field spin. The resulting drift force is proportional to the cross product of the particle's angular and translational velocities, revealing a rotational transport component in the nonequilibrium Casimir-Polder interaction. Our resul"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.31610","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/2606.31610/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":"2606.31610","created_at":"2026-07-01T01:18:09.124115+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.31610v1","created_at":"2026-07-01T01:18:09.124115+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.31610","created_at":"2026-07-01T01:18:09.124115+00:00"},{"alias_kind":"pith_short_12","alias_value":"J74YC2CYCQPY","created_at":"2026-07-01T01:18:09.124115+00:00"},{"alias_kind":"pith_short_16","alias_value":"J74YC2CYCQPYQZSR","created_at":"2026-07-01T01:18:09.124115+00:00"},{"alias_kind":"pith_short_8","alias_value":"J74YC2CY","created_at":"2026-07-01T01:18:09.124115+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/J74YC2CYCQPYQZSRSJPOTORGDE","json":"https://pith.science/pith/J74YC2CYCQPYQZSRSJPOTORGDE.json","graph_json":"https://pith.science/api/pith-number/J74YC2CYCQPYQZSRSJPOTORGDE/graph.json","events_json":"https://pith.science/api/pith-number/J74YC2CYCQPYQZSRSJPOTORGDE/events.json","paper":"https://pith.science/paper/J74YC2CY"},"agent_actions":{"view_html":"https://pith.science/pith/J74YC2CYCQPYQZSRSJPOTORGDE","download_json":"https://pith.science/pith/J74YC2CYCQPYQZSRSJPOTORGDE.json","view_paper":"https://pith.science/paper/J74YC2CY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.31610&json=true","fetch_graph":"https://pith.science/api/pith-number/J74YC2CYCQPYQZSRSJPOTORGDE/graph.json","fetch_events":"https://pith.science/api/pith-number/J74YC2CYCQPYQZSRSJPOTORGDE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J74YC2CYCQPYQZSRSJPOTORGDE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J74YC2CYCQPYQZSRSJPOTORGDE/action/storage_attestation","attest_author":"https://pith.science/pith/J74YC2CYCQPYQZSRSJPOTORGDE/action/author_attestation","sign_citation":"https://pith.science/pith/J74YC2CYCQPYQZSRSJPOTORGDE/action/citation_signature","submit_replication":"https://pith.science/pith/J74YC2CYCQPYQZSRSJPOTORGDE/action/replication_record"}},"created_at":"2026-07-01T01:18:09.124115+00:00","updated_at":"2026-07-01T01:18:09.124115+00:00"}