{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:TUIDX22V2EUXQX4KLQ2UEQQSI4","short_pith_number":"pith:TUIDX22V","canonical_record":{"source":{"id":"1103.4033","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2011-03-21T14:29:00Z","cross_cats_sorted":["physics.atm-clus","physics.chem-ph"],"title_canon_sha256":"d581c838e37483831da6bf9a88f908cd0bd08a051b59e4590f2830094b3b8c85","abstract_canon_sha256":"516a9290f3f9316623debd4c72781960b0f4d4cc5e67029824755cd09a0c3bbc"},"schema_version":"1.0"},"canonical_sha256":"9d103beb55d129785f8a5c354242124721fb6518eb0bf727eb9c9554af3caf64","source":{"kind":"arxiv","id":"1103.4033","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1103.4033","created_at":"2026-05-18T02:02:48Z"},{"alias_kind":"arxiv_version","alias_value":"1103.4033v1","created_at":"2026-05-18T02:02:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1103.4033","created_at":"2026-05-18T02:02:48Z"},{"alias_kind":"pith_short_12","alias_value":"TUIDX22V2EUX","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"TUIDX22V2EUXQX4K","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"TUIDX22V","created_at":"2026-05-18T12:26:42Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:TUIDX22V2EUXQX4KLQ2UEQQSI4","target":"record","payload":{"canonical_record":{"source":{"id":"1103.4033","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2011-03-21T14:29:00Z","cross_cats_sorted":["physics.atm-clus","physics.chem-ph"],"title_canon_sha256":"d581c838e37483831da6bf9a88f908cd0bd08a051b59e4590f2830094b3b8c85","abstract_canon_sha256":"516a9290f3f9316623debd4c72781960b0f4d4cc5e67029824755cd09a0c3bbc"},"schema_version":"1.0"},"canonical_sha256":"9d103beb55d129785f8a5c354242124721fb6518eb0bf727eb9c9554af3caf64","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:02:48.797935Z","signature_b64":"suEI5Xn0Yez2zK3jZmuFIwM6VHgqTjf4kmVFf4r4SRbGJ5WzN676NuvP/sUOf4ixwS1TTZoydA0n/iCmRaKmDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9d103beb55d129785f8a5c354242124721fb6518eb0bf727eb9c9554af3caf64","last_reissued_at":"2026-05-18T02:02:48.797261Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:02:48.797261Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1103.4033","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":"2026-05-18T02:02:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FpHrJ7/lVIBG4PX2HdFyP88NdisdiRKyRgQsV15l58U26DKkBXxc6I/gVxBrIfMqgoFSYxn14Kb5IcDHWZ7qDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T05:20:39.355261Z"},"content_sha256":"99773f7ae0e6fe4f7c03c1416009d3163ab8af39ace4d33526b6cd56cd0f4035","schema_version":"1.0","event_id":"sha256:99773f7ae0e6fe4f7c03c1416009d3163ab8af39ace4d33526b6cd56cd0f4035"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:TUIDX22V2EUXQX4KLQ2UEQQSI4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Clusters of Exceptional Points for a Laser Control of Selective Vibrational Transfer","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atm-clus","physics.chem-ph"],"primary_cat":"quant-ph","authors_text":"Amine Jaouadi, Osman Atabek, Roland Lefebvre","submitted_at":"2011-03-21T14:29:00Z","abstract_excerpt":"When a molecule is exposed to a laser field, all field-free vibrational states become resonances, with complex quasi energies calculated using Floquet theory. There are many ways to produce the coalescences of pairs of such quasi energies, with appropriate wavelength-intensity choices which define Exceptional Points (EP) in the laser parameter plane. We dress for the molecular ion H$_2^+$ an exhaustive map of these exceptional points which appear in clusters. Such clusters can be used to define several vibrational transfer scenarios implying more than a single exceptional point, exchanging sin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1103.4033","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":"2026-05-18T02:02:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"poYHdq53nQ1MYoGvRFHrC5Ug8rG9G8dzniJ/BVMorE+oTpoC3CfCShtYyA/N4td1tOF3o86p18uch6MkqH9ACw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T05:20:39.355641Z"},"content_sha256":"52527f6f10c61f3972e8b3f63b529c56f33cc86317985b940366c50864487a78","schema_version":"1.0","event_id":"sha256:52527f6f10c61f3972e8b3f63b529c56f33cc86317985b940366c50864487a78"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TUIDX22V2EUXQX4KLQ2UEQQSI4/bundle.json","state_url":"https://pith.science/pith/TUIDX22V2EUXQX4KLQ2UEQQSI4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TUIDX22V2EUXQX4KLQ2UEQQSI4/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":"2026-06-24T05:20:39Z","links":{"resolver":"https://pith.science/pith/TUIDX22V2EUXQX4KLQ2UEQQSI4","bundle":"https://pith.science/pith/TUIDX22V2EUXQX4KLQ2UEQQSI4/bundle.json","state":"https://pith.science/pith/TUIDX22V2EUXQX4KLQ2UEQQSI4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TUIDX22V2EUXQX4KLQ2UEQQSI4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:TUIDX22V2EUXQX4KLQ2UEQQSI4","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":"516a9290f3f9316623debd4c72781960b0f4d4cc5e67029824755cd09a0c3bbc","cross_cats_sorted":["physics.atm-clus","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2011-03-21T14:29:00Z","title_canon_sha256":"d581c838e37483831da6bf9a88f908cd0bd08a051b59e4590f2830094b3b8c85"},"schema_version":"1.0","source":{"id":"1103.4033","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1103.4033","created_at":"2026-05-18T02:02:48Z"},{"alias_kind":"arxiv_version","alias_value":"1103.4033v1","created_at":"2026-05-18T02:02:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1103.4033","created_at":"2026-05-18T02:02:48Z"},{"alias_kind":"pith_short_12","alias_value":"TUIDX22V2EUX","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"TUIDX22V2EUXQX4K","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"TUIDX22V","created_at":"2026-05-18T12:26:42Z"}],"graph_snapshots":[{"event_id":"sha256:52527f6f10c61f3972e8b3f63b529c56f33cc86317985b940366c50864487a78","target":"graph","created_at":"2026-05-18T02:02:48Z","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":"When a molecule is exposed to a laser field, all field-free vibrational states become resonances, with complex quasi energies calculated using Floquet theory. There are many ways to produce the coalescences of pairs of such quasi energies, with appropriate wavelength-intensity choices which define Exceptional Points (EP) in the laser parameter plane. We dress for the molecular ion H$_2^+$ an exhaustive map of these exceptional points which appear in clusters. Such clusters can be used to define several vibrational transfer scenarios implying more than a single exceptional point, exchanging sin","authors_text":"Amine Jaouadi, Osman Atabek, Roland Lefebvre","cross_cats":["physics.atm-clus","physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2011-03-21T14:29:00Z","title":"Clusters of Exceptional Points for a Laser Control of Selective Vibrational Transfer"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1103.4033","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":"sha256:99773f7ae0e6fe4f7c03c1416009d3163ab8af39ace4d33526b6cd56cd0f4035","target":"record","created_at":"2026-05-18T02:02:48Z","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":"516a9290f3f9316623debd4c72781960b0f4d4cc5e67029824755cd09a0c3bbc","cross_cats_sorted":["physics.atm-clus","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2011-03-21T14:29:00Z","title_canon_sha256":"d581c838e37483831da6bf9a88f908cd0bd08a051b59e4590f2830094b3b8c85"},"schema_version":"1.0","source":{"id":"1103.4033","kind":"arxiv","version":1}},"canonical_sha256":"9d103beb55d129785f8a5c354242124721fb6518eb0bf727eb9c9554af3caf64","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9d103beb55d129785f8a5c354242124721fb6518eb0bf727eb9c9554af3caf64","first_computed_at":"2026-05-18T02:02:48.797261Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:02:48.797261Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"suEI5Xn0Yez2zK3jZmuFIwM6VHgqTjf4kmVFf4r4SRbGJ5WzN676NuvP/sUOf4ixwS1TTZoydA0n/iCmRaKmDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:02:48.797935Z","signed_message":"canonical_sha256_bytes"},"source_id":"1103.4033","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:99773f7ae0e6fe4f7c03c1416009d3163ab8af39ace4d33526b6cd56cd0f4035","sha256:52527f6f10c61f3972e8b3f63b529c56f33cc86317985b940366c50864487a78"],"state_sha256":"5d476e9aa2e1f74f798edfad6178202da12df01bc3b4245ed81e84d477e3d732"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ATxsBGdRkVUgDVOYMZcYne3NcwO7D1PJjqYeVcVo/qaqgNQ2Dni9Y+IzRyK6UGL7RBMybf5JBCAkTyIv2d7jAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T05:20:39.357630Z","bundle_sha256":"2e1ccb04e47c0d3d51c2c0816c44c955d76d55970630deb03f72a0eee32b6388"}}