{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:AF2RZEWVU5KF5D3DR6AAQ4AXBE","short_pith_number":"pith:AF2RZEWV","canonical_record":{"source":{"id":"1709.04478","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-09-13T18:01:28Z","cross_cats_sorted":["cond-mat.stat-mech","physics.optics","quant-ph"],"title_canon_sha256":"390338c1f4af97017608d044ef94563afb787109d74dc72e8acb4a304c9c548a","abstract_canon_sha256":"125978ecf6a9079e7406c58f55063a7ba8570e57dcb9b67885bc213f29d173c0"},"schema_version":"1.0"},"canonical_sha256":"01751c92d5a7545e8f638f80087017091a01f182f48b3c8e588519b7ce2aaa1c","source":{"kind":"arxiv","id":"1709.04478","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.04478","created_at":"2026-05-18T00:35:03Z"},{"alias_kind":"arxiv_version","alias_value":"1709.04478v2","created_at":"2026-05-18T00:35:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.04478","created_at":"2026-05-18T00:35:03Z"},{"alias_kind":"pith_short_12","alias_value":"AF2RZEWVU5KF","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_16","alias_value":"AF2RZEWVU5KF5D3D","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_8","alias_value":"AF2RZEWV","created_at":"2026-05-18T12:31:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:AF2RZEWVU5KF5D3DR6AAQ4AXBE","target":"record","payload":{"canonical_record":{"source":{"id":"1709.04478","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-09-13T18:01:28Z","cross_cats_sorted":["cond-mat.stat-mech","physics.optics","quant-ph"],"title_canon_sha256":"390338c1f4af97017608d044ef94563afb787109d74dc72e8acb4a304c9c548a","abstract_canon_sha256":"125978ecf6a9079e7406c58f55063a7ba8570e57dcb9b67885bc213f29d173c0"},"schema_version":"1.0"},"canonical_sha256":"01751c92d5a7545e8f638f80087017091a01f182f48b3c8e588519b7ce2aaa1c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:03.378173Z","signature_b64":"uGsUpj91dui+2dXAXs0gFhPQdvT1PinMtK09RWG+JBbqHdeTeuZLwqSzgu78uVXbWaK52nqi6DAsUlvCYhtLAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"01751c92d5a7545e8f638f80087017091a01f182f48b3c8e588519b7ce2aaa1c","last_reissued_at":"2026-05-18T00:35:03.377408Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:03.377408Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1709.04478","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:35:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wf7UK7uAIxJt8QxaFbCxTnnhqQ0ov/z5TUsjVnNh9SB3lAGR4bHA/n0XZn6lx1qIbDs8nzFT+mYuAAaAGxf1Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T14:39:23.895127Z"},"content_sha256":"93f1f0511edeaa437724d0ad95ea8c157407f2fee276c4dea7de249eb0e4c210","schema_version":"1.0","event_id":"sha256:93f1f0511edeaa437724d0ad95ea8c157407f2fee276c4dea7de249eb0e4c210"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:AF2RZEWVU5KF5D3DR6AAQ4AXBE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fundamental efficiency bound for coherent energy transfer in nanophotonics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","physics.optics","quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Cristian L. Cortes, Zubin Jacob","submitted_at":"2017-09-13T18:01:28Z","abstract_excerpt":"We derive a unified quantum theory of coherent and incoherent energy transfer between two atoms (donor and acceptor) valid in arbitrary Markovian nanophotonic environments. Our theory predicts a fundamental bound $\\eta_{max} = \\frac{\\gamma_a}{\\gamma_d + \\gamma_a}$ for energy transfer efficiency arising from the spontaneous emission rates $\\gamma_{d}$ and $\\gamma_a$ of the donor and acceptor. We propose the control of the acceptor spontaneous emission rate as a new design principle for enhancing energy transfer efficiency. We predict an experiment using mirrors to enhance the efficiency bound b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.04478","kind":"arxiv","version":2},"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":"2026-05-18T00:35:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jUq8qg2FIAZxDtyaZDjQXFz/1/uhhP4aRCR90lkYMmn1Q9y/d0Lk2VNTevgZGMUgBOJEzkmlAc7Nv2CqiiSSBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T14:39:23.895867Z"},"content_sha256":"17e394f1ad439640ae06dc916b8d7bb5a1fc4dfa9e8c49b90eb4fe8504e54c03","schema_version":"1.0","event_id":"sha256:17e394f1ad439640ae06dc916b8d7bb5a1fc4dfa9e8c49b90eb4fe8504e54c03"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AF2RZEWVU5KF5D3DR6AAQ4AXBE/bundle.json","state_url":"https://pith.science/pith/AF2RZEWVU5KF5D3DR6AAQ4AXBE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AF2RZEWVU5KF5D3DR6AAQ4AXBE/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":"2026-05-27T14:39:23Z","links":{"resolver":"https://pith.science/pith/AF2RZEWVU5KF5D3DR6AAQ4AXBE","bundle":"https://pith.science/pith/AF2RZEWVU5KF5D3DR6AAQ4AXBE/bundle.json","state":"https://pith.science/pith/AF2RZEWVU5KF5D3DR6AAQ4AXBE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AF2RZEWVU5KF5D3DR6AAQ4AXBE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:AF2RZEWVU5KF5D3DR6AAQ4AXBE","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":"125978ecf6a9079e7406c58f55063a7ba8570e57dcb9b67885bc213f29d173c0","cross_cats_sorted":["cond-mat.stat-mech","physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-09-13T18:01:28Z","title_canon_sha256":"390338c1f4af97017608d044ef94563afb787109d74dc72e8acb4a304c9c548a"},"schema_version":"1.0","source":{"id":"1709.04478","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.04478","created_at":"2026-05-18T00:35:03Z"},{"alias_kind":"arxiv_version","alias_value":"1709.04478v2","created_at":"2026-05-18T00:35:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.04478","created_at":"2026-05-18T00:35:03Z"},{"alias_kind":"pith_short_12","alias_value":"AF2RZEWVU5KF","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_16","alias_value":"AF2RZEWVU5KF5D3D","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_8","alias_value":"AF2RZEWV","created_at":"2026-05-18T12:31:05Z"}],"graph_snapshots":[{"event_id":"sha256:17e394f1ad439640ae06dc916b8d7bb5a1fc4dfa9e8c49b90eb4fe8504e54c03","target":"graph","created_at":"2026-05-18T00:35:03Z","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":"We derive a unified quantum theory of coherent and incoherent energy transfer between two atoms (donor and acceptor) valid in arbitrary Markovian nanophotonic environments. Our theory predicts a fundamental bound $\\eta_{max} = \\frac{\\gamma_a}{\\gamma_d + \\gamma_a}$ for energy transfer efficiency arising from the spontaneous emission rates $\\gamma_{d}$ and $\\gamma_a$ of the donor and acceptor. We propose the control of the acceptor spontaneous emission rate as a new design principle for enhancing energy transfer efficiency. We predict an experiment using mirrors to enhance the efficiency bound b","authors_text":"Cristian L. Cortes, Zubin Jacob","cross_cats":["cond-mat.stat-mech","physics.optics","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-09-13T18:01:28Z","title":"Fundamental efficiency bound for coherent energy transfer in nanophotonics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.04478","kind":"arxiv","version":2},"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":"sha256:93f1f0511edeaa437724d0ad95ea8c157407f2fee276c4dea7de249eb0e4c210","target":"record","created_at":"2026-05-18T00:35:03Z","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":"125978ecf6a9079e7406c58f55063a7ba8570e57dcb9b67885bc213f29d173c0","cross_cats_sorted":["cond-mat.stat-mech","physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-09-13T18:01:28Z","title_canon_sha256":"390338c1f4af97017608d044ef94563afb787109d74dc72e8acb4a304c9c548a"},"schema_version":"1.0","source":{"id":"1709.04478","kind":"arxiv","version":2}},"canonical_sha256":"01751c92d5a7545e8f638f80087017091a01f182f48b3c8e588519b7ce2aaa1c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"01751c92d5a7545e8f638f80087017091a01f182f48b3c8e588519b7ce2aaa1c","first_computed_at":"2026-05-18T00:35:03.377408Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:35:03.377408Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"uGsUpj91dui+2dXAXs0gFhPQdvT1PinMtK09RWG+JBbqHdeTeuZLwqSzgu78uVXbWaK52nqi6DAsUlvCYhtLAw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:35:03.378173Z","signed_message":"canonical_sha256_bytes"},"source_id":"1709.04478","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:93f1f0511edeaa437724d0ad95ea8c157407f2fee276c4dea7de249eb0e4c210","sha256:17e394f1ad439640ae06dc916b8d7bb5a1fc4dfa9e8c49b90eb4fe8504e54c03"],"state_sha256":"ae58467dabea6f2c293ae405b2e127e54feb0253f3dab7a6d7713fad3c614613"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WyGW+aoeRNaRoKs986XPEtVKADgpsU4otT+H36pU6Jn+tM9XGbB11D6yvV+b2u38I9yU/YQxZPKZtHf4vuU8CA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T14:39:23.899639Z","bundle_sha256":"33a2ec8482c03a24142dd017e8967c0fbb9a44e575fbf6c5cc3d50c3d128a7b2"}}