{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:WUHQ3YJODQDMCZ5RZFONC2OVWI","short_pith_number":"pith:WUHQ3YJO","canonical_record":{"source":{"id":"1208.4190","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-08-21T04:46:25Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"d59511580a7b021a8243b927de6892c4e09b8871f5975ed1df046be0dc4bfe21","abstract_canon_sha256":"d8f1b3ca95abdc016dc3a54e52f62355d916275a9fb2b4d91ebc00ddbe2a7b79"},"schema_version":"1.0"},"canonical_sha256":"b50f0de12e1c06c167b1c95cd169d5b217e2392e21015ee5534ac9e5914b10c7","source":{"kind":"arxiv","id":"1208.4190","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1208.4190","created_at":"2026-05-18T01:55:08Z"},{"alias_kind":"arxiv_version","alias_value":"1208.4190v1","created_at":"2026-05-18T01:55:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1208.4190","created_at":"2026-05-18T01:55:08Z"},{"alias_kind":"pith_short_12","alias_value":"WUHQ3YJODQDM","created_at":"2026-05-18T12:27:27Z"},{"alias_kind":"pith_short_16","alias_value":"WUHQ3YJODQDMCZ5R","created_at":"2026-05-18T12:27:27Z"},{"alias_kind":"pith_short_8","alias_value":"WUHQ3YJO","created_at":"2026-05-18T12:27:27Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:WUHQ3YJODQDMCZ5RZFONC2OVWI","target":"record","payload":{"canonical_record":{"source":{"id":"1208.4190","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-08-21T04:46:25Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"d59511580a7b021a8243b927de6892c4e09b8871f5975ed1df046be0dc4bfe21","abstract_canon_sha256":"d8f1b3ca95abdc016dc3a54e52f62355d916275a9fb2b4d91ebc00ddbe2a7b79"},"schema_version":"1.0"},"canonical_sha256":"b50f0de12e1c06c167b1c95cd169d5b217e2392e21015ee5534ac9e5914b10c7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:55:08.923690Z","signature_b64":"3UsC6o0HbMn2CEeQrdct5ppNTCH+HwLJEuO0afRqMTVWB5tpvaQXtOZYg+PEweEQ7D0Z4iGqIpJafHjyR2ZNBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b50f0de12e1c06c167b1c95cd169d5b217e2392e21015ee5534ac9e5914b10c7","last_reissued_at":"2026-05-18T01:55:08.923035Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:55:08.923035Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1208.4190","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":"2026-05-18T01:55:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FIupTblJgrjsKRkNN53qxig+41JxH/jVp5/AV/9pazfHbtpFN2E9LVfmyDb9CJ5q+p1NoAftDaWDMy9TqB2iAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T19:41:49.198787Z"},"content_sha256":"a1a912784bb49d8180ae1c36b555e7765264518114c68a4f0ee5cee336ecc5ae","schema_version":"1.0","event_id":"sha256:a1a912784bb49d8180ae1c36b555e7765264518114c68a4f0ee5cee336ecc5ae"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:WUHQ3YJODQDMCZ5RZFONC2OVWI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Harmonic-seeded remote laser emissions in N2-Ar, N2-Xe and N2-Ne mixtures: a comparative study","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"physics.optics","authors_text":"Bin Zeng, Chaojin Zhang, Chenrui Jing, Guihua Li, Haisu Zhang, Huailiang Xu, Jielei Ni, Jinping Yao, See Leang Chin, Wei Chu, Ya Cheng, Zhizhan Xu","submitted_at":"2012-08-21T04:46:25Z","abstract_excerpt":"We report on the investigation on harmonic-seeded remote laser emissions at 391 nm wavelength from strong-field ionized nitrogen molecules in three different gas mixtures, i.e., N2-Ar, N2-Xe and N2-Ne. We observed a decrease in the remote laser intensity in the N2-Xe mixture because of the decreased clamped intensity in the filament; whereas in the N2-Ne mixture, the remote laser intensity slightly increases because of the increased clamped intensity within the filament. Remarkably, although the clamped intensity in the filament remains nearly unchanged in the N2-Ar mixture because of the simi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.4190","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":"2026-05-18T01:55:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9gxt+tU6EGkY643I/NP/FQg4IOwTY1aEmSqH8FQQzJQ+fH4dlS//YRF1O4VRe9huIFy7gTwyUQPx9EAgF6sGBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T19:41:49.199465Z"},"content_sha256":"af565b24504b91eb05b76ded5f83dab937ed6ec76b76acb4f12fcd210912a1d9","schema_version":"1.0","event_id":"sha256:af565b24504b91eb05b76ded5f83dab937ed6ec76b76acb4f12fcd210912a1d9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WUHQ3YJODQDMCZ5RZFONC2OVWI/bundle.json","state_url":"https://pith.science/pith/WUHQ3YJODQDMCZ5RZFONC2OVWI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WUHQ3YJODQDMCZ5RZFONC2OVWI/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":"2026-05-25T19:41:49Z","links":{"resolver":"https://pith.science/pith/WUHQ3YJODQDMCZ5RZFONC2OVWI","bundle":"https://pith.science/pith/WUHQ3YJODQDMCZ5RZFONC2OVWI/bundle.json","state":"https://pith.science/pith/WUHQ3YJODQDMCZ5RZFONC2OVWI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WUHQ3YJODQDMCZ5RZFONC2OVWI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:WUHQ3YJODQDMCZ5RZFONC2OVWI","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":"d8f1b3ca95abdc016dc3a54e52f62355d916275a9fb2b4d91ebc00ddbe2a7b79","cross_cats_sorted":["physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-08-21T04:46:25Z","title_canon_sha256":"d59511580a7b021a8243b927de6892c4e09b8871f5975ed1df046be0dc4bfe21"},"schema_version":"1.0","source":{"id":"1208.4190","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1208.4190","created_at":"2026-05-18T01:55:08Z"},{"alias_kind":"arxiv_version","alias_value":"1208.4190v1","created_at":"2026-05-18T01:55:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1208.4190","created_at":"2026-05-18T01:55:08Z"},{"alias_kind":"pith_short_12","alias_value":"WUHQ3YJODQDM","created_at":"2026-05-18T12:27:27Z"},{"alias_kind":"pith_short_16","alias_value":"WUHQ3YJODQDMCZ5R","created_at":"2026-05-18T12:27:27Z"},{"alias_kind":"pith_short_8","alias_value":"WUHQ3YJO","created_at":"2026-05-18T12:27:27Z"}],"graph_snapshots":[{"event_id":"sha256:af565b24504b91eb05b76ded5f83dab937ed6ec76b76acb4f12fcd210912a1d9","target":"graph","created_at":"2026-05-18T01:55:08Z","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 report on the investigation on harmonic-seeded remote laser emissions at 391 nm wavelength from strong-field ionized nitrogen molecules in three different gas mixtures, i.e., N2-Ar, N2-Xe and N2-Ne. We observed a decrease in the remote laser intensity in the N2-Xe mixture because of the decreased clamped intensity in the filament; whereas in the N2-Ne mixture, the remote laser intensity slightly increases because of the increased clamped intensity within the filament. Remarkably, although the clamped intensity in the filament remains nearly unchanged in the N2-Ar mixture because of the simi","authors_text":"Bin Zeng, Chaojin Zhang, Chenrui Jing, Guihua Li, Haisu Zhang, Huailiang Xu, Jielei Ni, Jinping Yao, See Leang Chin, Wei Chu, Ya Cheng, Zhizhan Xu","cross_cats":["physics.atom-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-08-21T04:46:25Z","title":"Harmonic-seeded remote laser emissions in N2-Ar, N2-Xe and N2-Ne mixtures: a comparative study"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.4190","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:a1a912784bb49d8180ae1c36b555e7765264518114c68a4f0ee5cee336ecc5ae","target":"record","created_at":"2026-05-18T01:55:08Z","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":"d8f1b3ca95abdc016dc3a54e52f62355d916275a9fb2b4d91ebc00ddbe2a7b79","cross_cats_sorted":["physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-08-21T04:46:25Z","title_canon_sha256":"d59511580a7b021a8243b927de6892c4e09b8871f5975ed1df046be0dc4bfe21"},"schema_version":"1.0","source":{"id":"1208.4190","kind":"arxiv","version":1}},"canonical_sha256":"b50f0de12e1c06c167b1c95cd169d5b217e2392e21015ee5534ac9e5914b10c7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b50f0de12e1c06c167b1c95cd169d5b217e2392e21015ee5534ac9e5914b10c7","first_computed_at":"2026-05-18T01:55:08.923035Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:55:08.923035Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"3UsC6o0HbMn2CEeQrdct5ppNTCH+HwLJEuO0afRqMTVWB5tpvaQXtOZYg+PEweEQ7D0Z4iGqIpJafHjyR2ZNBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:55:08.923690Z","signed_message":"canonical_sha256_bytes"},"source_id":"1208.4190","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a1a912784bb49d8180ae1c36b555e7765264518114c68a4f0ee5cee336ecc5ae","sha256:af565b24504b91eb05b76ded5f83dab937ed6ec76b76acb4f12fcd210912a1d9"],"state_sha256":"01bc98df508e488384f6c64fa82c18743735ef90ba4e9561a93c8d4a8b304c80"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MwxpnnJO4E0oAy108ZU8UeeH8tSl4yzLp1WqeRCY33V6720kHB91OQ1vY5fT+wqr0BaYQ9s+rw8rot+vppwYAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T19:41:49.203044Z","bundle_sha256":"6139b430a3eb4e1b06c10be5cb060e92ca723d35835413f12a15cc4b42834630"}}