{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:CYDDC7MBQYVWVW42SAUOU3IR75","short_pith_number":"pith:CYDDC7MB","schema_version":"1.0","canonical_sha256":"1606317d81862b6adb9a9028ea6d11ff5bb8879065bf520246b9a23206281fbd","source":{"kind":"arxiv","id":"1403.2598","version":1},"attestation_state":"computed","paper":{"title":"Optical binding of cylinder photonic molecules in the near-field of partially coherent fluctuating Gaussian Schell model sources. A coherent mode representation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"F. J. Valvidia-Valero, Juan Miguel Au\\~n\\'on, Manuel Nieto-Vesperinas","submitted_at":"2014-03-11T14:56:54Z","abstract_excerpt":"We present a theory and computation method of radiation pressure from partially coherent light by establishing a coherent mode representation of the radiation forces. This is illustrated with the near field emitted from a Gaussian Schell model source, mechanically acting on a single cylinder with magnetodielectric behavior, or on a photonic molecule constituted by a pair of such cylinders. Thus after studying the force produced by a single particle, we address the effects of the spatial coherence on the bonding and anti-bonding states of two particles. The coherence length manifests the critic"},"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":"1403.2598","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-03-11T14:56:54Z","cross_cats_sorted":[],"title_canon_sha256":"e9f61789b2b7ef08f39c5ac31b0603a6a76b692a761326b5329c9f24797c6170","abstract_canon_sha256":"404ccb56d6d27f7e739a25de64a1fc53888689329a2324e97420e0c6a846783e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:56:42.978742Z","signature_b64":"auqFrQ1H9y36w2+83+O8L1QryQ/PhGf7NW3ofyrcIW0tUmrj+p8NQLc1d93p5TH8VS3MuMt5M97qjQb2AvzRBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1606317d81862b6adb9a9028ea6d11ff5bb8879065bf520246b9a23206281fbd","last_reissued_at":"2026-05-18T02:56:42.978310Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:56:42.978310Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Optical binding of cylinder photonic molecules in the near-field of partially coherent fluctuating Gaussian Schell model sources. A coherent mode representation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"F. J. Valvidia-Valero, Juan Miguel Au\\~n\\'on, Manuel Nieto-Vesperinas","submitted_at":"2014-03-11T14:56:54Z","abstract_excerpt":"We present a theory and computation method of radiation pressure from partially coherent light by establishing a coherent mode representation of the radiation forces. This is illustrated with the near field emitted from a Gaussian Schell model source, mechanically acting on a single cylinder with magnetodielectric behavior, or on a photonic molecule constituted by a pair of such cylinders. Thus after studying the force produced by a single particle, we address the effects of the spatial coherence on the bonding and anti-bonding states of two particles. The coherence length manifests the critic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.2598","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":"1403.2598","created_at":"2026-05-18T02:56:42.978384+00:00"},{"alias_kind":"arxiv_version","alias_value":"1403.2598v1","created_at":"2026-05-18T02:56:42.978384+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.2598","created_at":"2026-05-18T02:56:42.978384+00:00"},{"alias_kind":"pith_short_12","alias_value":"CYDDC7MBQYVW","created_at":"2026-05-18T12:28:25.294606+00:00"},{"alias_kind":"pith_short_16","alias_value":"CYDDC7MBQYVWVW42","created_at":"2026-05-18T12:28:25.294606+00:00"},{"alias_kind":"pith_short_8","alias_value":"CYDDC7MB","created_at":"2026-05-18T12:28:25.294606+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/CYDDC7MBQYVWVW42SAUOU3IR75","json":"https://pith.science/pith/CYDDC7MBQYVWVW42SAUOU3IR75.json","graph_json":"https://pith.science/api/pith-number/CYDDC7MBQYVWVW42SAUOU3IR75/graph.json","events_json":"https://pith.science/api/pith-number/CYDDC7MBQYVWVW42SAUOU3IR75/events.json","paper":"https://pith.science/paper/CYDDC7MB"},"agent_actions":{"view_html":"https://pith.science/pith/CYDDC7MBQYVWVW42SAUOU3IR75","download_json":"https://pith.science/pith/CYDDC7MBQYVWVW42SAUOU3IR75.json","view_paper":"https://pith.science/paper/CYDDC7MB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1403.2598&json=true","fetch_graph":"https://pith.science/api/pith-number/CYDDC7MBQYVWVW42SAUOU3IR75/graph.json","fetch_events":"https://pith.science/api/pith-number/CYDDC7MBQYVWVW42SAUOU3IR75/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CYDDC7MBQYVWVW42SAUOU3IR75/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CYDDC7MBQYVWVW42SAUOU3IR75/action/storage_attestation","attest_author":"https://pith.science/pith/CYDDC7MBQYVWVW42SAUOU3IR75/action/author_attestation","sign_citation":"https://pith.science/pith/CYDDC7MBQYVWVW42SAUOU3IR75/action/citation_signature","submit_replication":"https://pith.science/pith/CYDDC7MBQYVWVW42SAUOU3IR75/action/replication_record"}},"created_at":"2026-05-18T02:56:42.978384+00:00","updated_at":"2026-05-18T02:56:42.978384+00:00"}