{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:ZTL6JIKERFIQLIZIFMLNQ7VHNP","short_pith_number":"pith:ZTL6JIKE","canonical_record":{"source":{"id":"1303.3673","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2013-03-15T04:03:56Z","cross_cats_sorted":[],"title_canon_sha256":"00a7971ede3759df3876a99e109034ab077aabb78df8b6a42fdee4d5068a8191","abstract_canon_sha256":"c012e716953f3f409df5ffd2bf55bb3497abf952c0682200166d7ca5d9ecbea8"},"schema_version":"1.0"},"canonical_sha256":"ccd7e4a144895105a3282b16d87ea76bec4e47f86aed461e1b85611086eea8a2","source":{"kind":"arxiv","id":"1303.3673","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.3673","created_at":"2026-05-18T03:16:28Z"},{"alias_kind":"arxiv_version","alias_value":"1303.3673v1","created_at":"2026-05-18T03:16:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.3673","created_at":"2026-05-18T03:16:28Z"},{"alias_kind":"pith_short_12","alias_value":"ZTL6JIKERFIQ","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"ZTL6JIKERFIQLIZI","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"ZTL6JIKE","created_at":"2026-05-18T12:28:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:ZTL6JIKERFIQLIZIFMLNQ7VHNP","target":"record","payload":{"canonical_record":{"source":{"id":"1303.3673","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2013-03-15T04:03:56Z","cross_cats_sorted":[],"title_canon_sha256":"00a7971ede3759df3876a99e109034ab077aabb78df8b6a42fdee4d5068a8191","abstract_canon_sha256":"c012e716953f3f409df5ffd2bf55bb3497abf952c0682200166d7ca5d9ecbea8"},"schema_version":"1.0"},"canonical_sha256":"ccd7e4a144895105a3282b16d87ea76bec4e47f86aed461e1b85611086eea8a2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:16:28.664255Z","signature_b64":"bDOODYtxYl1vKFWNkFqwGn8Z/Y/GONEVI/L7My2iVbS7sg1YMkZi/Fcv8HQ5Lj4FtakcDL+8G2mA4MWS6vEZAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ccd7e4a144895105a3282b16d87ea76bec4e47f86aed461e1b85611086eea8a2","last_reissued_at":"2026-05-18T03:16:28.663478Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:16:28.663478Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1303.3673","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":"2026-05-18T03:16:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZIfpLr18MrAScJgm7B4aPf5jGydl99oJ4Obm1pRVytR5qfWG4Ceu3jXsPzy1X5DLEvEUbefhQWK/CequhhwrBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-16T12:51:21.047675Z"},"content_sha256":"d6116e72d12a710b36c312c3acbc0bf4dc3313af6e01f0189a6f26d4a50efbf8","schema_version":"1.0","event_id":"sha256:d6116e72d12a710b36c312c3acbc0bf4dc3313af6e01f0189a6f26d4a50efbf8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:ZTL6JIKERFIQLIZIFMLNQ7VHNP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"All-analytical semiclassical theory of spaser for plasmonic nanocavity","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Xiaolan Zhong, Zhiyuan Li","submitted_at":"2013-03-15T04:03:56Z","abstract_excerpt":"Experimental approaches to manipulate light-matter interaction at nanoscale have quickly advanced in recent years, leading to the demonstration of spaser (surface plasmon amplification by stimulated emission of radiation) in plasmonic nanocavities. Yet, a well-understood analytical theory to better understand and quantitatively explain the connotation of spaser system is urgently needed. Here we develop an all-analytical semiclassical theory to investigate the energy exchange between active materials and fields and the spaser performance in a plasmonic nanocavity. The theory can be commonly us"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.3673","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":"2026-05-18T03:16:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"N8G29msFfZDuXrw5wAAhzA5F0FGD7+vlXaNml5UN4tio82FtnDdzKbc0RlK5t5qvTw8SHbH7C/qvIUEZ/d/sCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-16T12:51:21.048030Z"},"content_sha256":"450054ed079a99a9aba7d7687b046ca5a188d921ded17a375aa3fef6ada21e65","schema_version":"1.0","event_id":"sha256:450054ed079a99a9aba7d7687b046ca5a188d921ded17a375aa3fef6ada21e65"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZTL6JIKERFIQLIZIFMLNQ7VHNP/bundle.json","state_url":"https://pith.science/pith/ZTL6JIKERFIQLIZIFMLNQ7VHNP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZTL6JIKERFIQLIZIFMLNQ7VHNP/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":"2026-07-16T12:51:21Z","links":{"resolver":"https://pith.science/pith/ZTL6JIKERFIQLIZIFMLNQ7VHNP","bundle":"https://pith.science/pith/ZTL6JIKERFIQLIZIFMLNQ7VHNP/bundle.json","state":"https://pith.science/pith/ZTL6JIKERFIQLIZIFMLNQ7VHNP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZTL6JIKERFIQLIZIFMLNQ7VHNP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:ZTL6JIKERFIQLIZIFMLNQ7VHNP","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":"c012e716953f3f409df5ffd2bf55bb3497abf952c0682200166d7ca5d9ecbea8","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2013-03-15T04:03:56Z","title_canon_sha256":"00a7971ede3759df3876a99e109034ab077aabb78df8b6a42fdee4d5068a8191"},"schema_version":"1.0","source":{"id":"1303.3673","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.3673","created_at":"2026-05-18T03:16:28Z"},{"alias_kind":"arxiv_version","alias_value":"1303.3673v1","created_at":"2026-05-18T03:16:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.3673","created_at":"2026-05-18T03:16:28Z"},{"alias_kind":"pith_short_12","alias_value":"ZTL6JIKERFIQ","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"ZTL6JIKERFIQLIZI","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"ZTL6JIKE","created_at":"2026-05-18T12:28:09Z"}],"graph_snapshots":[{"event_id":"sha256:450054ed079a99a9aba7d7687b046ca5a188d921ded17a375aa3fef6ada21e65","target":"graph","created_at":"2026-05-18T03:16:28Z","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":"Experimental approaches to manipulate light-matter interaction at nanoscale have quickly advanced in recent years, leading to the demonstration of spaser (surface plasmon amplification by stimulated emission of radiation) in plasmonic nanocavities. Yet, a well-understood analytical theory to better understand and quantitatively explain the connotation of spaser system is urgently needed. Here we develop an all-analytical semiclassical theory to investigate the energy exchange between active materials and fields and the spaser performance in a plasmonic nanocavity. The theory can be commonly us","authors_text":"Xiaolan Zhong, Zhiyuan Li","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2013-03-15T04:03:56Z","title":"All-analytical semiclassical theory of spaser for plasmonic nanocavity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.3673","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:d6116e72d12a710b36c312c3acbc0bf4dc3313af6e01f0189a6f26d4a50efbf8","target":"record","created_at":"2026-05-18T03:16:28Z","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":"c012e716953f3f409df5ffd2bf55bb3497abf952c0682200166d7ca5d9ecbea8","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2013-03-15T04:03:56Z","title_canon_sha256":"00a7971ede3759df3876a99e109034ab077aabb78df8b6a42fdee4d5068a8191"},"schema_version":"1.0","source":{"id":"1303.3673","kind":"arxiv","version":1}},"canonical_sha256":"ccd7e4a144895105a3282b16d87ea76bec4e47f86aed461e1b85611086eea8a2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ccd7e4a144895105a3282b16d87ea76bec4e47f86aed461e1b85611086eea8a2","first_computed_at":"2026-05-18T03:16:28.663478Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:16:28.663478Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bDOODYtxYl1vKFWNkFqwGn8Z/Y/GONEVI/L7My2iVbS7sg1YMkZi/Fcv8HQ5Lj4FtakcDL+8G2mA4MWS6vEZAA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:16:28.664255Z","signed_message":"canonical_sha256_bytes"},"source_id":"1303.3673","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d6116e72d12a710b36c312c3acbc0bf4dc3313af6e01f0189a6f26d4a50efbf8","sha256:450054ed079a99a9aba7d7687b046ca5a188d921ded17a375aa3fef6ada21e65"],"state_sha256":"e8b1802882d0ede93d96edc36b91f4ae3c498a4a3795f3fac4173b90937bf3a5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"n3vxIb3EEJCud0pIdCBeCSnmCgoSfcsfDICdVB8An+CJxflzFmzhkQA3rvv8frDFYXjajw74RATFdFRZWYuoBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-16T12:51:21.050603Z","bundle_sha256":"abe82674405224902689ec24460ff232d6f78c75fbd5aa90c88a6864dfe1289c"}}