{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:7GUG3FUDOROAE3MY4TEJORAF4A","short_pith_number":"pith:7GUG3FUD","canonical_record":{"source":{"id":"1608.02747","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-08-09T10:11:37Z","cross_cats_sorted":["cond-mat.mes-hall","quant-ph"],"title_canon_sha256":"7b7847bbd0d5e871dfb21c38c3aa893fbde5221aeb1130d46ba9757cfc5c6e0e","abstract_canon_sha256":"0587f69d2934dc5ac337815d803080bd76d5e8c5b91219559a643e5699591ba5"},"schema_version":"1.0"},"canonical_sha256":"f9a86d9683745c026d98e4c8974405e03191ab8d3916c3079e71214bd929d17f","source":{"kind":"arxiv","id":"1608.02747","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.02747","created_at":"2026-05-18T00:59:19Z"},{"alias_kind":"arxiv_version","alias_value":"1608.02747v1","created_at":"2026-05-18T00:59:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.02747","created_at":"2026-05-18T00:59:19Z"},{"alias_kind":"pith_short_12","alias_value":"7GUG3FUDOROA","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"7GUG3FUDOROAE3MY","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"7GUG3FUD","created_at":"2026-05-18T12:30:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:7GUG3FUDOROAE3MY4TEJORAF4A","target":"record","payload":{"canonical_record":{"source":{"id":"1608.02747","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-08-09T10:11:37Z","cross_cats_sorted":["cond-mat.mes-hall","quant-ph"],"title_canon_sha256":"7b7847bbd0d5e871dfb21c38c3aa893fbde5221aeb1130d46ba9757cfc5c6e0e","abstract_canon_sha256":"0587f69d2934dc5ac337815d803080bd76d5e8c5b91219559a643e5699591ba5"},"schema_version":"1.0"},"canonical_sha256":"f9a86d9683745c026d98e4c8974405e03191ab8d3916c3079e71214bd929d17f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:59:19.859740Z","signature_b64":"9xa0JJdlotnoJDlTYmgGpcr5sLP8nKUMytQffub1zw34luN1yWkwjrSgbu4SmepUhaQbzYK/1P0b8KxaP2fNAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f9a86d9683745c026d98e4c8974405e03191ab8d3916c3079e71214bd929d17f","last_reissued_at":"2026-05-18T00:59:19.859026Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:59:19.859026Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1608.02747","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":"2026-05-18T00:59:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pSr7M2LaLvRdUuQCraUFp2H7SrHQRxvAE9Yq6uj5i1t2FnCLq6PLvtohZ3zgVDW7yXdnHkUb8oEo0cq+RbvWDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T21:57:15.516659Z"},"content_sha256":"a5cd44bfc4e4762b2b31d61938387c0c935d4881fccb2cedda26926b3f5b2154","schema_version":"1.0","event_id":"sha256:a5cd44bfc4e4762b2b31d61938387c0c935d4881fccb2cedda26926b3f5b2154"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:7GUG3FUDOROAE3MY4TEJORAF4A","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Near-field relaxation of a quantum emitter to 2D semiconductors: surface dissipation and exciton polaritons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","quant-ph"],"primary_cat":"physics.optics","authors_text":"A. Louise Bradley, Cristian A. Marocico, Paul R. Eastham, Vasilios D. Karanikolas","submitted_at":"2016-08-09T10:11:37Z","abstract_excerpt":"The total spontaneous emission rate of a quantum emitter in the presence of an infinite MoS\\textsubscript{2} monolayer is enhanced by several orders of magnitude, compared to its free-space value, due to the excitation of surface exciton polariton modes and lossy modes. The spectral and distance dependence of the spontaneous emission rate are analyzed and the lossy-surface-wave, surface exciton polariton mode and radiative contributions are identified. The transverse magnetic and transverse electric exciton polariton modes can be excited for different emission frequencies of the quantum emitte"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.02747","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":"2026-05-18T00:59:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"26qH55DiJ6I+3Swc2DXqzzx0kflbxCJ65hWqWlV+cEhxBl5WEDZHDfK2dj6JY35o2jskUiSR9NHixgyYcU92Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T21:57:15.517017Z"},"content_sha256":"43678c1f3b2ba537d191d3d2e0526047d9b92041168da1abbcb28baf90ce461e","schema_version":"1.0","event_id":"sha256:43678c1f3b2ba537d191d3d2e0526047d9b92041168da1abbcb28baf90ce461e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7GUG3FUDOROAE3MY4TEJORAF4A/bundle.json","state_url":"https://pith.science/pith/7GUG3FUDOROAE3MY4TEJORAF4A/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7GUG3FUDOROAE3MY4TEJORAF4A/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":"2026-05-30T21:57:15Z","links":{"resolver":"https://pith.science/pith/7GUG3FUDOROAE3MY4TEJORAF4A","bundle":"https://pith.science/pith/7GUG3FUDOROAE3MY4TEJORAF4A/bundle.json","state":"https://pith.science/pith/7GUG3FUDOROAE3MY4TEJORAF4A/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7GUG3FUDOROAE3MY4TEJORAF4A/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:7GUG3FUDOROAE3MY4TEJORAF4A","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":"0587f69d2934dc5ac337815d803080bd76d5e8c5b91219559a643e5699591ba5","cross_cats_sorted":["cond-mat.mes-hall","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-08-09T10:11:37Z","title_canon_sha256":"7b7847bbd0d5e871dfb21c38c3aa893fbde5221aeb1130d46ba9757cfc5c6e0e"},"schema_version":"1.0","source":{"id":"1608.02747","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.02747","created_at":"2026-05-18T00:59:19Z"},{"alias_kind":"arxiv_version","alias_value":"1608.02747v1","created_at":"2026-05-18T00:59:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.02747","created_at":"2026-05-18T00:59:19Z"},{"alias_kind":"pith_short_12","alias_value":"7GUG3FUDOROA","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"7GUG3FUDOROAE3MY","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"7GUG3FUD","created_at":"2026-05-18T12:30:04Z"}],"graph_snapshots":[{"event_id":"sha256:43678c1f3b2ba537d191d3d2e0526047d9b92041168da1abbcb28baf90ce461e","target":"graph","created_at":"2026-05-18T00:59:19Z","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 total spontaneous emission rate of a quantum emitter in the presence of an infinite MoS\\textsubscript{2} monolayer is enhanced by several orders of magnitude, compared to its free-space value, due to the excitation of surface exciton polariton modes and lossy modes. The spectral and distance dependence of the spontaneous emission rate are analyzed and the lossy-surface-wave, surface exciton polariton mode and radiative contributions are identified. The transverse magnetic and transverse electric exciton polariton modes can be excited for different emission frequencies of the quantum emitte","authors_text":"A. Louise Bradley, Cristian A. Marocico, Paul R. Eastham, Vasilios D. Karanikolas","cross_cats":["cond-mat.mes-hall","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-08-09T10:11:37Z","title":"Near-field relaxation of a quantum emitter to 2D semiconductors: surface dissipation and exciton polaritons"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.02747","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:a5cd44bfc4e4762b2b31d61938387c0c935d4881fccb2cedda26926b3f5b2154","target":"record","created_at":"2026-05-18T00:59:19Z","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":"0587f69d2934dc5ac337815d803080bd76d5e8c5b91219559a643e5699591ba5","cross_cats_sorted":["cond-mat.mes-hall","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-08-09T10:11:37Z","title_canon_sha256":"7b7847bbd0d5e871dfb21c38c3aa893fbde5221aeb1130d46ba9757cfc5c6e0e"},"schema_version":"1.0","source":{"id":"1608.02747","kind":"arxiv","version":1}},"canonical_sha256":"f9a86d9683745c026d98e4c8974405e03191ab8d3916c3079e71214bd929d17f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f9a86d9683745c026d98e4c8974405e03191ab8d3916c3079e71214bd929d17f","first_computed_at":"2026-05-18T00:59:19.859026Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:59:19.859026Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9xa0JJdlotnoJDlTYmgGpcr5sLP8nKUMytQffub1zw34luN1yWkwjrSgbu4SmepUhaQbzYK/1P0b8KxaP2fNAg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:59:19.859740Z","signed_message":"canonical_sha256_bytes"},"source_id":"1608.02747","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a5cd44bfc4e4762b2b31d61938387c0c935d4881fccb2cedda26926b3f5b2154","sha256:43678c1f3b2ba537d191d3d2e0526047d9b92041168da1abbcb28baf90ce461e"],"state_sha256":"d6e65d396302aa6def803687b768e91f27de59d61de507240dc1c67ef3b91b23"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FJ5iK3WYx7r+Dm+vZgzvOz697IjnlThwzXzB/uNrZTC5Mvl2I1L1ebaTTJ6iuHLBiBETPtwRSkn4xl/3oFteCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T21:57:15.519783Z","bundle_sha256":"38ea3ba7c6c171e7d76ac0b0778e12638df73d2b566ff5fdd0ef479743a46954"}}