{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:VK7DMKTIVM62XLTVUDUQAZ2XMZ","short_pith_number":"pith:VK7DMKTI","canonical_record":{"source":{"id":"1003.0822","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2010-03-03T14:34:23Z","cross_cats_sorted":["physics.class-ph"],"title_canon_sha256":"18619c230f7ee6e20f369240dce63f3f4b51cfdcd96433bc359d49f2929eb45a","abstract_canon_sha256":"889923e639fd3b9ec065f6548eb125a314892478dc04419620af66dc73fab9fa"},"schema_version":"1.0"},"canonical_sha256":"aabe362a68ab3dabae75a0e90067576676ac48b6d05e2fe48812e43f01d60c5a","source":{"kind":"arxiv","id":"1003.0822","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1003.0822","created_at":"2026-05-18T02:08:47Z"},{"alias_kind":"arxiv_version","alias_value":"1003.0822v1","created_at":"2026-05-18T02:08:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.0822","created_at":"2026-05-18T02:08:47Z"},{"alias_kind":"pith_short_12","alias_value":"VK7DMKTIVM62","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_16","alias_value":"VK7DMKTIVM62XLTV","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_8","alias_value":"VK7DMKTI","created_at":"2026-05-18T12:26:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:VK7DMKTIVM62XLTVUDUQAZ2XMZ","target":"record","payload":{"canonical_record":{"source":{"id":"1003.0822","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2010-03-03T14:34:23Z","cross_cats_sorted":["physics.class-ph"],"title_canon_sha256":"18619c230f7ee6e20f369240dce63f3f4b51cfdcd96433bc359d49f2929eb45a","abstract_canon_sha256":"889923e639fd3b9ec065f6548eb125a314892478dc04419620af66dc73fab9fa"},"schema_version":"1.0"},"canonical_sha256":"aabe362a68ab3dabae75a0e90067576676ac48b6d05e2fe48812e43f01d60c5a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:08:47.054952Z","signature_b64":"Qao/v65RJcnFvX/iB0LfutG2H4qYyJ30pxOgZxC6EzK+SI7s740Ll9lutNUwR4BdybaxCNk7bh1CBwd7m3uaAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aabe362a68ab3dabae75a0e90067576676ac48b6d05e2fe48812e43f01d60c5a","last_reissued_at":"2026-05-18T02:08:47.054046Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:08:47.054046Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1003.0822","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":"2026-05-18T02:08:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5v+9G3o+aZfzFZc35QowHQV9EH78gstzN8Rew4KGbd6UZbcJ/GpW7wLRKw60H+2hdjtDKgyn5z58saQz7zu1AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T10:18:38.921564Z"},"content_sha256":"862247ea7cf5405cbc87140cdca8b7ce03b8d78c1aca5790149eb2115789841b","schema_version":"1.0","event_id":"sha256:862247ea7cf5405cbc87140cdca8b7ce03b8d78c1aca5790149eb2115789841b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:VK7DMKTIVM62XLTVUDUQAZ2XMZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Double Resonance Nanolaser based on Coupled Slit-hole Resonator Structures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.class-ph"],"primary_cat":"physics.optics","authors_text":"H. Liu, S. M. Wang, S. N. Zhu, W. M. Ye, X. D. Yuan, Z. H. Zhu","submitted_at":"2010-03-03T14:34:23Z","abstract_excerpt":"This work investigates a kind of metallic magnetic cavity based on slit-hole resonators (SHRs). Two orthogonal hybrid magnetic resonance modes of the cavity with a large spatial overlap are predesigned at the wavelengths of 980 nm and 1550 nm. The Yb-Er co-doped material serving as a gain medium is set in the cavity; this enables the resonator to have high optical activity. The numerical result shows that the strong lasing at 1550 nm may be achieved when the cavity array is pumped at 980 nm. This double resonance nanolaser array has potential applications in future optical devices and quantum "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.0822","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":"2026-05-18T02:08:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ba6ZtJtW4iBd8hcgtb5aLPMCT9VvrrVJiY6kFb1C/d6XwMaufs3n7RYZh4vkkmKDiDXbSQbjn+shTWZ3VQdeDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T10:18:38.922234Z"},"content_sha256":"04729a3ca3e1ef723bf4caea07affa5340fde1a71ab9e3ccdf04116501bf3495","schema_version":"1.0","event_id":"sha256:04729a3ca3e1ef723bf4caea07affa5340fde1a71ab9e3ccdf04116501bf3495"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VK7DMKTIVM62XLTVUDUQAZ2XMZ/bundle.json","state_url":"https://pith.science/pith/VK7DMKTIVM62XLTVUDUQAZ2XMZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VK7DMKTIVM62XLTVUDUQAZ2XMZ/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":"2026-05-20T10:18:38Z","links":{"resolver":"https://pith.science/pith/VK7DMKTIVM62XLTVUDUQAZ2XMZ","bundle":"https://pith.science/pith/VK7DMKTIVM62XLTVUDUQAZ2XMZ/bundle.json","state":"https://pith.science/pith/VK7DMKTIVM62XLTVUDUQAZ2XMZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VK7DMKTIVM62XLTVUDUQAZ2XMZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:VK7DMKTIVM62XLTVUDUQAZ2XMZ","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":"889923e639fd3b9ec065f6548eb125a314892478dc04419620af66dc73fab9fa","cross_cats_sorted":["physics.class-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2010-03-03T14:34:23Z","title_canon_sha256":"18619c230f7ee6e20f369240dce63f3f4b51cfdcd96433bc359d49f2929eb45a"},"schema_version":"1.0","source":{"id":"1003.0822","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1003.0822","created_at":"2026-05-18T02:08:47Z"},{"alias_kind":"arxiv_version","alias_value":"1003.0822v1","created_at":"2026-05-18T02:08:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.0822","created_at":"2026-05-18T02:08:47Z"},{"alias_kind":"pith_short_12","alias_value":"VK7DMKTIVM62","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_16","alias_value":"VK7DMKTIVM62XLTV","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_8","alias_value":"VK7DMKTI","created_at":"2026-05-18T12:26:15Z"}],"graph_snapshots":[{"event_id":"sha256:04729a3ca3e1ef723bf4caea07affa5340fde1a71ab9e3ccdf04116501bf3495","target":"graph","created_at":"2026-05-18T02:08:47Z","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":"This work investigates a kind of metallic magnetic cavity based on slit-hole resonators (SHRs). Two orthogonal hybrid magnetic resonance modes of the cavity with a large spatial overlap are predesigned at the wavelengths of 980 nm and 1550 nm. The Yb-Er co-doped material serving as a gain medium is set in the cavity; this enables the resonator to have high optical activity. The numerical result shows that the strong lasing at 1550 nm may be achieved when the cavity array is pumped at 980 nm. This double resonance nanolaser array has potential applications in future optical devices and quantum ","authors_text":"H. Liu, S. M. Wang, S. N. Zhu, W. M. Ye, X. D. Yuan, Z. H. Zhu","cross_cats":["physics.class-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2010-03-03T14:34:23Z","title":"Double Resonance Nanolaser based on Coupled Slit-hole Resonator Structures"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.0822","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":"sha256:862247ea7cf5405cbc87140cdca8b7ce03b8d78c1aca5790149eb2115789841b","target":"record","created_at":"2026-05-18T02:08:47Z","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":"889923e639fd3b9ec065f6548eb125a314892478dc04419620af66dc73fab9fa","cross_cats_sorted":["physics.class-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2010-03-03T14:34:23Z","title_canon_sha256":"18619c230f7ee6e20f369240dce63f3f4b51cfdcd96433bc359d49f2929eb45a"},"schema_version":"1.0","source":{"id":"1003.0822","kind":"arxiv","version":1}},"canonical_sha256":"aabe362a68ab3dabae75a0e90067576676ac48b6d05e2fe48812e43f01d60c5a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"aabe362a68ab3dabae75a0e90067576676ac48b6d05e2fe48812e43f01d60c5a","first_computed_at":"2026-05-18T02:08:47.054046Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:08:47.054046Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Qao/v65RJcnFvX/iB0LfutG2H4qYyJ30pxOgZxC6EzK+SI7s740Ll9lutNUwR4BdybaxCNk7bh1CBwd7m3uaAA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:08:47.054952Z","signed_message":"canonical_sha256_bytes"},"source_id":"1003.0822","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:862247ea7cf5405cbc87140cdca8b7ce03b8d78c1aca5790149eb2115789841b","sha256:04729a3ca3e1ef723bf4caea07affa5340fde1a71ab9e3ccdf04116501bf3495"],"state_sha256":"6a273aa8f15b7603a42f81ab97b884b33ae25186bb500e57dc9143d2be3fee65"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uaUPMt0RAhPPw5xTpNVS84Rcd8sF2L53ypFtGnCpimSbIZUw7Ot7+mDWZg43Ly7sTsr/v3BF6wGyy0SpBUdnBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-20T10:18:38.925655Z","bundle_sha256":"b18600ab003a20f96086d149ddf08df77c8c916bc053c4fedf5eda0217950134"}}