{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:UWOM6WSJDB4PGDDPNKZWXIOEEG","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"288657a6080fc1632fc65a6bf3eeac72472c34bf5dc76c4ff795e9652dc045f1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-01-30T10:23:38Z","title_canon_sha256":"0d46a1b39e8a3c595f6a4025fb171048499544ded16738b360bd57ad3b037c6f"},"schema_version":"1.0","source":{"id":"1201.6156","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.6156","created_at":"2026-05-18T04:03:33Z"},{"alias_kind":"arxiv_version","alias_value":"1201.6156v1","created_at":"2026-05-18T04:03:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.6156","created_at":"2026-05-18T04:03:33Z"},{"alias_kind":"pith_short_12","alias_value":"UWOM6WSJDB4P","created_at":"2026-05-18T12:27:25Z"},{"alias_kind":"pith_short_16","alias_value":"UWOM6WSJDB4PGDDP","created_at":"2026-05-18T12:27:25Z"},{"alias_kind":"pith_short_8","alias_value":"UWOM6WSJ","created_at":"2026-05-18T12:27:25Z"}],"graph_snapshots":[{"event_id":"sha256:7041e3375ceb860a80292f87ec154d6bd189d3da4cacb62a57107724c755f26b","target":"graph","created_at":"2026-05-18T04:03:33Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Electromagnetic sources, as e.g. lasers, antennas, diffusers or thermal sources, produce a wavefield that interacts with objects to transfer them its momentum. We show that the photonic force exerted on a small particle in the near field of a planar statistically homogeneous fluctuating source uniquely depends and acts along the coordinate perpendicular to its surface. The gradient part of this force is contributed by only the evanescent components of the emitted field, its sign being opposite to that of the real part of the particle polarizability. The non-conservative force part is uniquely ","authors_text":"Juan Miguel Aunon, Manuel Nieto-Vesperinas","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-01-30T10:23:38Z","title":"Photonic forces in the near field of statistically homogeneous fluctuating sources"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.6156","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:99711b36fe8f9f505e559febdde4a76f6a36640d99f62dba9b52a0315c10817f","target":"record","created_at":"2026-05-18T04:03:33Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"288657a6080fc1632fc65a6bf3eeac72472c34bf5dc76c4ff795e9652dc045f1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-01-30T10:23:38Z","title_canon_sha256":"0d46a1b39e8a3c595f6a4025fb171048499544ded16738b360bd57ad3b037c6f"},"schema_version":"1.0","source":{"id":"1201.6156","kind":"arxiv","version":1}},"canonical_sha256":"a59ccf5a491878f30c6f6ab36ba1c42190f9ade4c0792f03abe8d20fe0612aa6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a59ccf5a491878f30c6f6ab36ba1c42190f9ade4c0792f03abe8d20fe0612aa6","first_computed_at":"2026-05-18T04:03:33.580069Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:03:33.580069Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8Nq5c8Eae2bzfTEhTWfXFW/FZv610uExBO5I3PA/ShFFdwyk76boj17vRLxARmP53cuEEXGoCx6WnDSQApT0DQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:03:33.580678Z","signed_message":"canonical_sha256_bytes"},"source_id":"1201.6156","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:99711b36fe8f9f505e559febdde4a76f6a36640d99f62dba9b52a0315c10817f","sha256:7041e3375ceb860a80292f87ec154d6bd189d3da4cacb62a57107724c755f26b"],"state_sha256":"5e5a609d8f2a9db3621e2d406bf40856612a2f0e141e6a97463bf4e52256591b"}