{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:C2YAG5XMYCHLC62XLHHPUHVVUB","short_pith_number":"pith:C2YAG5XM","canonical_record":{"source":{"id":"1106.1586","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2011-06-08T15:46:02Z","cross_cats_sorted":[],"title_canon_sha256":"a525b5a3bcdeb59ecd085cb1e63ed23bd34f625df5e059e0d95a9a9c2f5cc290","abstract_canon_sha256":"5777d20f78d08f6cf480b1b559eebf37f82a843a8b50181fdedf06ea0f86088b"},"schema_version":"1.0"},"canonical_sha256":"16b00376ecc08eb17b5759cefa1eb5a043624c2f1b8ef046896e96938b4bd5c4","source":{"kind":"arxiv","id":"1106.1586","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.1586","created_at":"2026-05-18T02:01:40Z"},{"alias_kind":"arxiv_version","alias_value":"1106.1586v1","created_at":"2026-05-18T02:01:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.1586","created_at":"2026-05-18T02:01:40Z"},{"alias_kind":"pith_short_12","alias_value":"C2YAG5XMYCHL","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"C2YAG5XMYCHLC62X","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"C2YAG5XM","created_at":"2026-05-18T12:26:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:C2YAG5XMYCHLC62XLHHPUHVVUB","target":"record","payload":{"canonical_record":{"source":{"id":"1106.1586","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2011-06-08T15:46:02Z","cross_cats_sorted":[],"title_canon_sha256":"a525b5a3bcdeb59ecd085cb1e63ed23bd34f625df5e059e0d95a9a9c2f5cc290","abstract_canon_sha256":"5777d20f78d08f6cf480b1b559eebf37f82a843a8b50181fdedf06ea0f86088b"},"schema_version":"1.0"},"canonical_sha256":"16b00376ecc08eb17b5759cefa1eb5a043624c2f1b8ef046896e96938b4bd5c4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:40.802311Z","signature_b64":"J08CnZehCagc8X1uegiR9TDQptX2Gl82XZZjRR1bT8tFeKUOgYywGf4XpUwCbjymiMOpPe1SVWfOfiulXh9CBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"16b00376ecc08eb17b5759cefa1eb5a043624c2f1b8ef046896e96938b4bd5c4","last_reissued_at":"2026-05-18T02:01:40.801759Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:40.801759Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1106.1586","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":"2026-05-18T02:01:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jEP/S8TAPY2rm/hLZmEDnLOZLOJGIPHMsHsfG9dPrK1wZNplHSZpbv+I5ecq+V7rvj2EDw1fS5qbrLwVS/i2AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T03:12:54.743074Z"},"content_sha256":"c4d1694f7959072ad7402cf3e7dee4c2c2f3d02a12d295601b50090ce668c5fe","schema_version":"1.0","event_id":"sha256:c4d1694f7959072ad7402cf3e7dee4c2c2f3d02a12d295601b50090ce668c5fe"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:C2YAG5XMYCHLC62XLHHPUHVVUB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Rotational spectrum of asymmetric top molecules in combined static and laser fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.chem-ph","authors_text":"J. J. Omiste, P. Schmelcher, R. Gonz\\'alez-F\\'erez","submitted_at":"2011-06-08T15:46:02Z","abstract_excerpt":"We examine the impact of the combination of a static electric field and a non resonant linearly polarized laser field on an asymmetric top molecule. Within the rigid rotor approximation, we analyze the symmetries of the Hamiltonian for all possible field configurations. For each irreducible representation, the Schr\\\"odinger equation is solved by a basis set expansion in terms of a linear combination of Wigner functions respecting the corresponding symmetries, which allows us to distinguish avoided crossings from genuine ones. Using the fluorobenzene and pyridazine molecules as prototypes, the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.1586","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":"2026-05-18T02:01:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DOcorDiFPrz/UAY+p+dBpi7batE/pO7IZMvEYi9RGJOK+z/CjtxgZEBQqKSDiqeC6LYNPYp8VkGyUoph6H16CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T03:12:54.743435Z"},"content_sha256":"622a4cf3a38f156e0318e9a251618abffb0e3b07aebc620aaaaf48c3c1a763ba","schema_version":"1.0","event_id":"sha256:622a4cf3a38f156e0318e9a251618abffb0e3b07aebc620aaaaf48c3c1a763ba"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/C2YAG5XMYCHLC62XLHHPUHVVUB/bundle.json","state_url":"https://pith.science/pith/C2YAG5XMYCHLC62XLHHPUHVVUB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/C2YAG5XMYCHLC62XLHHPUHVVUB/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":"2026-05-28T03:12:54Z","links":{"resolver":"https://pith.science/pith/C2YAG5XMYCHLC62XLHHPUHVVUB","bundle":"https://pith.science/pith/C2YAG5XMYCHLC62XLHHPUHVVUB/bundle.json","state":"https://pith.science/pith/C2YAG5XMYCHLC62XLHHPUHVVUB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/C2YAG5XMYCHLC62XLHHPUHVVUB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:C2YAG5XMYCHLC62XLHHPUHVVUB","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":"5777d20f78d08f6cf480b1b559eebf37f82a843a8b50181fdedf06ea0f86088b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2011-06-08T15:46:02Z","title_canon_sha256":"a525b5a3bcdeb59ecd085cb1e63ed23bd34f625df5e059e0d95a9a9c2f5cc290"},"schema_version":"1.0","source":{"id":"1106.1586","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.1586","created_at":"2026-05-18T02:01:40Z"},{"alias_kind":"arxiv_version","alias_value":"1106.1586v1","created_at":"2026-05-18T02:01:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.1586","created_at":"2026-05-18T02:01:40Z"},{"alias_kind":"pith_short_12","alias_value":"C2YAG5XMYCHL","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"C2YAG5XMYCHLC62X","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"C2YAG5XM","created_at":"2026-05-18T12:26:24Z"}],"graph_snapshots":[{"event_id":"sha256:622a4cf3a38f156e0318e9a251618abffb0e3b07aebc620aaaaf48c3c1a763ba","target":"graph","created_at":"2026-05-18T02:01:40Z","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 examine the impact of the combination of a static electric field and a non resonant linearly polarized laser field on an asymmetric top molecule. Within the rigid rotor approximation, we analyze the symmetries of the Hamiltonian for all possible field configurations. For each irreducible representation, the Schr\\\"odinger equation is solved by a basis set expansion in terms of a linear combination of Wigner functions respecting the corresponding symmetries, which allows us to distinguish avoided crossings from genuine ones. Using the fluorobenzene and pyridazine molecules as prototypes, the ","authors_text":"J. J. Omiste, P. Schmelcher, R. Gonz\\'alez-F\\'erez","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2011-06-08T15:46:02Z","title":"Rotational spectrum of asymmetric top molecules in combined static and laser fields"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.1586","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:c4d1694f7959072ad7402cf3e7dee4c2c2f3d02a12d295601b50090ce668c5fe","target":"record","created_at":"2026-05-18T02:01:40Z","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":"5777d20f78d08f6cf480b1b559eebf37f82a843a8b50181fdedf06ea0f86088b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2011-06-08T15:46:02Z","title_canon_sha256":"a525b5a3bcdeb59ecd085cb1e63ed23bd34f625df5e059e0d95a9a9c2f5cc290"},"schema_version":"1.0","source":{"id":"1106.1586","kind":"arxiv","version":1}},"canonical_sha256":"16b00376ecc08eb17b5759cefa1eb5a043624c2f1b8ef046896e96938b4bd5c4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"16b00376ecc08eb17b5759cefa1eb5a043624c2f1b8ef046896e96938b4bd5c4","first_computed_at":"2026-05-18T02:01:40.801759Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:01:40.801759Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"J08CnZehCagc8X1uegiR9TDQptX2Gl82XZZjRR1bT8tFeKUOgYywGf4XpUwCbjymiMOpPe1SVWfOfiulXh9CBA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:01:40.802311Z","signed_message":"canonical_sha256_bytes"},"source_id":"1106.1586","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c4d1694f7959072ad7402cf3e7dee4c2c2f3d02a12d295601b50090ce668c5fe","sha256:622a4cf3a38f156e0318e9a251618abffb0e3b07aebc620aaaaf48c3c1a763ba"],"state_sha256":"73e2ff29047a1eeb3426ea868e149db3c6efdb1398a73205eeca5aa8f5e150be"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Fnh3sPG8gMBNt5OvE2J1vUradBtm4E1sh4X9kU8MS9b7d4gfHz+NA8yDO4O2deHSrluwUYu+LEVwLJR0XbPdCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T03:12:54.745359Z","bundle_sha256":"6dd4ddce32bca1736ab153fe7b616b7a22547e573c8f787ce3b8c1404ee60415"}}