{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:VWJKUWAR4RSMEMOHRF5H5TZCFW","short_pith_number":"pith:VWJKUWAR","canonical_record":{"source":{"id":"1801.08591","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2018-01-25T21:01:19Z","cross_cats_sorted":[],"title_canon_sha256":"c7043ccef95c67814660ad3ec3dae9a9f4007a402b7e07edbf2b4f0db4e05e8e","abstract_canon_sha256":"10088cd695765c8a39472c6f3baf9a136ad409baaf1d68b9a1f6712651c5874b"},"schema_version":"1.0"},"canonical_sha256":"ad92aa5811e464c231c7897a7ecf222dba6bf5a6487bc0ebb39a1f83de047c70","source":{"kind":"arxiv","id":"1801.08591","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.08591","created_at":"2026-05-18T00:05:45Z"},{"alias_kind":"arxiv_version","alias_value":"1801.08591v1","created_at":"2026-05-18T00:05:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.08591","created_at":"2026-05-18T00:05:45Z"},{"alias_kind":"pith_short_12","alias_value":"VWJKUWAR4RSM","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_16","alias_value":"VWJKUWAR4RSMEMOH","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_8","alias_value":"VWJKUWAR","created_at":"2026-05-18T12:32:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:VWJKUWAR4RSMEMOHRF5H5TZCFW","target":"record","payload":{"canonical_record":{"source":{"id":"1801.08591","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2018-01-25T21:01:19Z","cross_cats_sorted":[],"title_canon_sha256":"c7043ccef95c67814660ad3ec3dae9a9f4007a402b7e07edbf2b4f0db4e05e8e","abstract_canon_sha256":"10088cd695765c8a39472c6f3baf9a136ad409baaf1d68b9a1f6712651c5874b"},"schema_version":"1.0"},"canonical_sha256":"ad92aa5811e464c231c7897a7ecf222dba6bf5a6487bc0ebb39a1f83de047c70","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:05:45.956207Z","signature_b64":"Zksbk7pqKWvEvsrsb57j6hJIXPOpYSWdKrlZ4x+fxd3VEwGtZMk3zBGxhk8haR23B0JRM7lTzbCEkB/yfc6lCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ad92aa5811e464c231c7897a7ecf222dba6bf5a6487bc0ebb39a1f83de047c70","last_reissued_at":"2026-05-18T00:05:45.955492Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:05:45.955492Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1801.08591","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":"2026-05-18T00:05:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GJv5csivgKZGsw7iN+ICuUJ+sNP481FNShtjBONboonNxYYhqaOeTF0d2CAUxYumNxrXfppWq0DfHHQHxHzQBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T18:52:41.451061Z"},"content_sha256":"600b148fd7cc764e0b24a68410e20a42c9854de6bebb2fe6431605aeff435513","schema_version":"1.0","event_id":"sha256:600b148fd7cc764e0b24a68410e20a42c9854de6bebb2fe6431605aeff435513"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:VWJKUWAR4RSMEMOHRF5H5TZCFW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum sensing of motion in colloids via time-dependent Purcell effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Alexander S. Shalin, Alexey S. Kadochkin, Ivan I. Shishkin, Pavel Ginzburg","submitted_at":"2018-01-25T21:01:19Z","abstract_excerpt":"Light-matter interaction dynamics is governed by the strength of local coupling constants, tailored by surrounding electromagnetic structures. Characteristic decay times in dipole-allowed fluorescent transitions are much faster than mechanical conformational changes within an environment and, as the result, the latter can be assumed static during the emission process. However, slow-decaying compounds can break this commonly accepted approximation and introduce new interaction regimes. Here, slow decaying phosphorescent compounds are proposed to perform quantum sensing of nearby structure's mot"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.08591","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":"2026-05-18T00:05:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Cba07njKF/XOhhBz+VV+JDcjuEM8hjprZNlAtn6xlJlh+H0EZAsXUKBrQ6+7TeLiS3zLKs4kO7kGrIBmxIkVAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T18:52:41.451421Z"},"content_sha256":"c8cd469f7c490375db74e6b530ae29ef1a5456845f5b7cd328c74aaaa98fcc36","schema_version":"1.0","event_id":"sha256:c8cd469f7c490375db74e6b530ae29ef1a5456845f5b7cd328c74aaaa98fcc36"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VWJKUWAR4RSMEMOHRF5H5TZCFW/bundle.json","state_url":"https://pith.science/pith/VWJKUWAR4RSMEMOHRF5H5TZCFW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VWJKUWAR4RSMEMOHRF5H5TZCFW/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":"2026-06-02T18:52:41Z","links":{"resolver":"https://pith.science/pith/VWJKUWAR4RSMEMOHRF5H5TZCFW","bundle":"https://pith.science/pith/VWJKUWAR4RSMEMOHRF5H5TZCFW/bundle.json","state":"https://pith.science/pith/VWJKUWAR4RSMEMOHRF5H5TZCFW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VWJKUWAR4RSMEMOHRF5H5TZCFW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:VWJKUWAR4RSMEMOHRF5H5TZCFW","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":"10088cd695765c8a39472c6f3baf9a136ad409baaf1d68b9a1f6712651c5874b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2018-01-25T21:01:19Z","title_canon_sha256":"c7043ccef95c67814660ad3ec3dae9a9f4007a402b7e07edbf2b4f0db4e05e8e"},"schema_version":"1.0","source":{"id":"1801.08591","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.08591","created_at":"2026-05-18T00:05:45Z"},{"alias_kind":"arxiv_version","alias_value":"1801.08591v1","created_at":"2026-05-18T00:05:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.08591","created_at":"2026-05-18T00:05:45Z"},{"alias_kind":"pith_short_12","alias_value":"VWJKUWAR4RSM","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_16","alias_value":"VWJKUWAR4RSMEMOH","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_8","alias_value":"VWJKUWAR","created_at":"2026-05-18T12:32:59Z"}],"graph_snapshots":[{"event_id":"sha256:c8cd469f7c490375db74e6b530ae29ef1a5456845f5b7cd328c74aaaa98fcc36","target":"graph","created_at":"2026-05-18T00:05:45Z","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":"Light-matter interaction dynamics is governed by the strength of local coupling constants, tailored by surrounding electromagnetic structures. Characteristic decay times in dipole-allowed fluorescent transitions are much faster than mechanical conformational changes within an environment and, as the result, the latter can be assumed static during the emission process. However, slow-decaying compounds can break this commonly accepted approximation and introduce new interaction regimes. Here, slow decaying phosphorescent compounds are proposed to perform quantum sensing of nearby structure's mot","authors_text":"Alexander S. Shalin, Alexey S. Kadochkin, Ivan I. Shishkin, Pavel Ginzburg","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2018-01-25T21:01:19Z","title":"Quantum sensing of motion in colloids via time-dependent Purcell effect"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.08591","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":"sha256:600b148fd7cc764e0b24a68410e20a42c9854de6bebb2fe6431605aeff435513","target":"record","created_at":"2026-05-18T00:05:45Z","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":"10088cd695765c8a39472c6f3baf9a136ad409baaf1d68b9a1f6712651c5874b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2018-01-25T21:01:19Z","title_canon_sha256":"c7043ccef95c67814660ad3ec3dae9a9f4007a402b7e07edbf2b4f0db4e05e8e"},"schema_version":"1.0","source":{"id":"1801.08591","kind":"arxiv","version":1}},"canonical_sha256":"ad92aa5811e464c231c7897a7ecf222dba6bf5a6487bc0ebb39a1f83de047c70","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ad92aa5811e464c231c7897a7ecf222dba6bf5a6487bc0ebb39a1f83de047c70","first_computed_at":"2026-05-18T00:05:45.955492Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:05:45.955492Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Zksbk7pqKWvEvsrsb57j6hJIXPOpYSWdKrlZ4x+fxd3VEwGtZMk3zBGxhk8haR23B0JRM7lTzbCEkB/yfc6lCA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:05:45.956207Z","signed_message":"canonical_sha256_bytes"},"source_id":"1801.08591","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:600b148fd7cc764e0b24a68410e20a42c9854de6bebb2fe6431605aeff435513","sha256:c8cd469f7c490375db74e6b530ae29ef1a5456845f5b7cd328c74aaaa98fcc36"],"state_sha256":"9c469cb22e8768c45734a54b23b4b5ca3357d4525694612c0f7e87dc7990aa2b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"E5MFMY4TvtEgjsbKX8odUSUyRiA1JdyX6T53WO9UTru4At8hw9dyQxt0exkDRFAEkieAKldAh8bOmFsdd0VuCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T18:52:41.453466Z","bundle_sha256":"f48bc5506d98fe66cc9f3447b9c1ab43cb3b5a7c1a3ed9086a142596b834d876"}}