{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:GLLV3FZPBFAXPXSHSK6XJNIHPU","short_pith_number":"pith:GLLV3FZP","canonical_record":{"source":{"id":"1310.5678","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-21T19:07:17Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"e0b86ed60c2861b0ceaffba90240c171e069a0f4d362ff3f9d015ec423ec4ee6","abstract_canon_sha256":"3f24e3b182e90ac4aa496673cbe6547d3d81edc674b6b5fecfc99bba1502395c"},"schema_version":"1.0"},"canonical_sha256":"32d75d972f094177de4792bd74b5077d1a7a71c70fe8f5e594a6141559b8b820","source":{"kind":"arxiv","id":"1310.5678","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.5678","created_at":"2026-05-18T03:09:34Z"},{"alias_kind":"arxiv_version","alias_value":"1310.5678v1","created_at":"2026-05-18T03:09:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.5678","created_at":"2026-05-18T03:09:34Z"},{"alias_kind":"pith_short_12","alias_value":"GLLV3FZPBFAX","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"GLLV3FZPBFAXPXSH","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"GLLV3FZP","created_at":"2026-05-18T12:27:45Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:GLLV3FZPBFAXPXSHSK6XJNIHPU","target":"record","payload":{"canonical_record":{"source":{"id":"1310.5678","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-21T19:07:17Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"e0b86ed60c2861b0ceaffba90240c171e069a0f4d362ff3f9d015ec423ec4ee6","abstract_canon_sha256":"3f24e3b182e90ac4aa496673cbe6547d3d81edc674b6b5fecfc99bba1502395c"},"schema_version":"1.0"},"canonical_sha256":"32d75d972f094177de4792bd74b5077d1a7a71c70fe8f5e594a6141559b8b820","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:09:34.535469Z","signature_b64":"W71H/UdBE61ew5jV+IXjSNDFMqJLq1ksoR48SbAoKCSWkoqzOtDjgvRL8ohN3/WGA1aEG0RgwIdQQfhg98igCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"32d75d972f094177de4792bd74b5077d1a7a71c70fe8f5e594a6141559b8b820","last_reissued_at":"2026-05-18T03:09:34.534667Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:09:34.534667Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1310.5678","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:09:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O/E9F8ugJ/nSlhGU3nDFSLwXfOji+VMstSCi+DXQAZTOztfY2XfBRQZDDI3n5KOr3y9+Gi91zm1RwvhIrcniCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T10:39:51.058161Z"},"content_sha256":"a878e4af00f40d6f5166e87d073382e4fdd16165377e6f975d769255566d072e","schema_version":"1.0","event_id":"sha256:a878e4af00f40d6f5166e87d073382e4fdd16165377e6f975d769255566d072e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:GLLV3FZPBFAXPXSHSK6XJNIHPU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Numerical calculations of radiative and non-radiative relaxation of molecules near metal particles","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"Abraham Nitzan, Maxim Sukharev","submitted_at":"2013-10-21T19:07:17Z","abstract_excerpt":"The dependence of the radiative emission and the non-radiative (energy transfer to the metal) relaxation rates of a molecule near a small metal particle on the molecule-to-particle distance and on the molecular orientation is calculated using a numerical solution of the Maxwell equations for a model that described the metal as a dispersive dielectric particle and the molecule as an oscillating point dipole. The emission rate is obtained by evaluating the total oscillating dipole in the system, while the non-radiative rate is inferred from the rate of heat production on the particle. For the di"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.5678","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:09:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"n5JS7Q3dpTaZfWIEuaP8MjL0WifCG2DkvhqS2OxdldNDxRypWoj+CJqdlGgIRFBGpbqSIvqpQKOVXYAwAPNSDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T10:39:51.058519Z"},"content_sha256":"91aff4096e94a22091b5d0564be33530f7bd5787fd196b444ea388e755232d34","schema_version":"1.0","event_id":"sha256:91aff4096e94a22091b5d0564be33530f7bd5787fd196b444ea388e755232d34"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GLLV3FZPBFAXPXSHSK6XJNIHPU/bundle.json","state_url":"https://pith.science/pith/GLLV3FZPBFAXPXSHSK6XJNIHPU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GLLV3FZPBFAXPXSHSK6XJNIHPU/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-22T10:39:51Z","links":{"resolver":"https://pith.science/pith/GLLV3FZPBFAXPXSHSK6XJNIHPU","bundle":"https://pith.science/pith/GLLV3FZPBFAXPXSHSK6XJNIHPU/bundle.json","state":"https://pith.science/pith/GLLV3FZPBFAXPXSHSK6XJNIHPU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GLLV3FZPBFAXPXSHSK6XJNIHPU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:GLLV3FZPBFAXPXSHSK6XJNIHPU","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":"3f24e3b182e90ac4aa496673cbe6547d3d81edc674b6b5fecfc99bba1502395c","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-21T19:07:17Z","title_canon_sha256":"e0b86ed60c2861b0ceaffba90240c171e069a0f4d362ff3f9d015ec423ec4ee6"},"schema_version":"1.0","source":{"id":"1310.5678","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.5678","created_at":"2026-05-18T03:09:34Z"},{"alias_kind":"arxiv_version","alias_value":"1310.5678v1","created_at":"2026-05-18T03:09:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.5678","created_at":"2026-05-18T03:09:34Z"},{"alias_kind":"pith_short_12","alias_value":"GLLV3FZPBFAX","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"GLLV3FZPBFAXPXSH","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"GLLV3FZP","created_at":"2026-05-18T12:27:45Z"}],"graph_snapshots":[{"event_id":"sha256:91aff4096e94a22091b5d0564be33530f7bd5787fd196b444ea388e755232d34","target":"graph","created_at":"2026-05-18T03:09:34Z","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":"The dependence of the radiative emission and the non-radiative (energy transfer to the metal) relaxation rates of a molecule near a small metal particle on the molecule-to-particle distance and on the molecular orientation is calculated using a numerical solution of the Maxwell equations for a model that described the metal as a dispersive dielectric particle and the molecule as an oscillating point dipole. The emission rate is obtained by evaluating the total oscillating dipole in the system, while the non-radiative rate is inferred from the rate of heat production on the particle. For the di","authors_text":"Abraham Nitzan, Maxim Sukharev","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-21T19:07:17Z","title":"Numerical calculations of radiative and non-radiative relaxation of molecules near metal particles"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.5678","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:a878e4af00f40d6f5166e87d073382e4fdd16165377e6f975d769255566d072e","target":"record","created_at":"2026-05-18T03:09:34Z","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":"3f24e3b182e90ac4aa496673cbe6547d3d81edc674b6b5fecfc99bba1502395c","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-21T19:07:17Z","title_canon_sha256":"e0b86ed60c2861b0ceaffba90240c171e069a0f4d362ff3f9d015ec423ec4ee6"},"schema_version":"1.0","source":{"id":"1310.5678","kind":"arxiv","version":1}},"canonical_sha256":"32d75d972f094177de4792bd74b5077d1a7a71c70fe8f5e594a6141559b8b820","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"32d75d972f094177de4792bd74b5077d1a7a71c70fe8f5e594a6141559b8b820","first_computed_at":"2026-05-18T03:09:34.534667Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:09:34.534667Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"W71H/UdBE61ew5jV+IXjSNDFMqJLq1ksoR48SbAoKCSWkoqzOtDjgvRL8ohN3/WGA1aEG0RgwIdQQfhg98igCg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:09:34.535469Z","signed_message":"canonical_sha256_bytes"},"source_id":"1310.5678","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a878e4af00f40d6f5166e87d073382e4fdd16165377e6f975d769255566d072e","sha256:91aff4096e94a22091b5d0564be33530f7bd5787fd196b444ea388e755232d34"],"state_sha256":"14977711b55b30ec25dffa8f158bd3db4f14e30503b810916237ee89c3f8514c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LMMHAtbrBZF2dPxszN/O2jxoWUxxLNhTxQuI1egCuMFllAxYdPSnsqpitgfVINm5h3a4vRCPtZssDyHrjGdkBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-22T10:39:51.060765Z","bundle_sha256":"c6626adc1b87f018e7f7cca37d2399bd6566addc61379c8a4ad0e2349a599b70"}}