{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:HJ6B3Q4EYMMIW3FCYTKCWNTQU2","short_pith_number":"pith:HJ6B3Q4E","canonical_record":{"source":{"id":"1112.3688","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-12-15T23:13:44Z","cross_cats_sorted":["physics.chem-ph"],"title_canon_sha256":"46c92631703107f4a5ad14e6a10afaf1d06842c0ff797ff483403fff4d53f09d","abstract_canon_sha256":"f978ff4639736f2fae4147d7005560123a78061c71b87322b88e9925d2f77db3"},"schema_version":"1.0"},"canonical_sha256":"3a7c1dc384c3188b6ca2c4d42b3670a6b3edd1867ae72f138e8b9623b0bf2127","source":{"kind":"arxiv","id":"1112.3688","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.3688","created_at":"2026-05-18T01:59:08Z"},{"alias_kind":"arxiv_version","alias_value":"1112.3688v1","created_at":"2026-05-18T01:59:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.3688","created_at":"2026-05-18T01:59:08Z"},{"alias_kind":"pith_short_12","alias_value":"HJ6B3Q4EYMMI","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_16","alias_value":"HJ6B3Q4EYMMIW3FC","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_8","alias_value":"HJ6B3Q4E","created_at":"2026-05-18T12:26:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:HJ6B3Q4EYMMIW3FCYTKCWNTQU2","target":"record","payload":{"canonical_record":{"source":{"id":"1112.3688","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-12-15T23:13:44Z","cross_cats_sorted":["physics.chem-ph"],"title_canon_sha256":"46c92631703107f4a5ad14e6a10afaf1d06842c0ff797ff483403fff4d53f09d","abstract_canon_sha256":"f978ff4639736f2fae4147d7005560123a78061c71b87322b88e9925d2f77db3"},"schema_version":"1.0"},"canonical_sha256":"3a7c1dc384c3188b6ca2c4d42b3670a6b3edd1867ae72f138e8b9623b0bf2127","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:08.878785Z","signature_b64":"NeAsTkRvLOC0cDlbWKqeJ4xaqK+LWfC2eHh1Dc1Q6KUk7h7lb/pfnxekdwEJmUMpZvrmLZ4IyahIvkykzWQmAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3a7c1dc384c3188b6ca2c4d42b3670a6b3edd1867ae72f138e8b9623b0bf2127","last_reissued_at":"2026-05-18T01:59:08.878046Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:08.878046Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1112.3688","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":"2026-05-18T01:59:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"t9wVrdqAy6uLhuzPfFZGg/G8OfkuIC6da4DPWozpSuqpDt8DThyFSlg/ao65vseaniYZSHYS5KRhUkJ1+QnTCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T20:48:59.695230Z"},"content_sha256":"e3a8b045e80449cda1365a611231c45f23d9f04980c7ab3a5cdd5d8deac5e991","schema_version":"1.0","event_id":"sha256:e3a8b045e80449cda1365a611231c45f23d9f04980c7ab3a5cdd5d8deac5e991"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:HJ6B3Q4EYMMIW3FCYTKCWNTQU2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Multiphoton Dissociation of HeH+ below the He+(1s) + H(1s) Threshold","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.chem-ph"],"primary_cat":"physics.atom-ph","authors_text":"B. D. Esry, D. Ursrey, F. Anis","submitted_at":"2011-12-15T23:13:44Z","abstract_excerpt":"We discuss the strong-field dynamics of HeH+, the simplest stable heteronuclear molecule, focusing on identifying a laser regime for which there is a sufficient dissociation signal for experimental measurement. We numerically solve the time-dependent Schr\\\"odinger equation to obtain total dissociation probabilities, kinetic energy release spectra, and momentum distributions for wavelengths from 800 nm to 2400 nm. The suitability of this simple system as a prototype for understanding the strong-field nuclear dynamics of heteronuclear dissociation is discussed."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.3688","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":"2026-05-18T01:59:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fTp65hoAPYXQ1fWLtfoPN745yOOe8MNSvZK35q/dzngF6x7+ug8ml5Wc4+g9nZPMhiuLMgVH/qWbXd9AE8fiCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T20:48:59.695942Z"},"content_sha256":"5a29e95d10092f20dad6569cfe93678c55d56bf2613487f5390b1d4682354304","schema_version":"1.0","event_id":"sha256:5a29e95d10092f20dad6569cfe93678c55d56bf2613487f5390b1d4682354304"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HJ6B3Q4EYMMIW3FCYTKCWNTQU2/bundle.json","state_url":"https://pith.science/pith/HJ6B3Q4EYMMIW3FCYTKCWNTQU2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HJ6B3Q4EYMMIW3FCYTKCWNTQU2/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":"2026-06-07T20:48:59Z","links":{"resolver":"https://pith.science/pith/HJ6B3Q4EYMMIW3FCYTKCWNTQU2","bundle":"https://pith.science/pith/HJ6B3Q4EYMMIW3FCYTKCWNTQU2/bundle.json","state":"https://pith.science/pith/HJ6B3Q4EYMMIW3FCYTKCWNTQU2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HJ6B3Q4EYMMIW3FCYTKCWNTQU2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:HJ6B3Q4EYMMIW3FCYTKCWNTQU2","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":"f978ff4639736f2fae4147d7005560123a78061c71b87322b88e9925d2f77db3","cross_cats_sorted":["physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-12-15T23:13:44Z","title_canon_sha256":"46c92631703107f4a5ad14e6a10afaf1d06842c0ff797ff483403fff4d53f09d"},"schema_version":"1.0","source":{"id":"1112.3688","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.3688","created_at":"2026-05-18T01:59:08Z"},{"alias_kind":"arxiv_version","alias_value":"1112.3688v1","created_at":"2026-05-18T01:59:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.3688","created_at":"2026-05-18T01:59:08Z"},{"alias_kind":"pith_short_12","alias_value":"HJ6B3Q4EYMMI","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_16","alias_value":"HJ6B3Q4EYMMIW3FC","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_8","alias_value":"HJ6B3Q4E","created_at":"2026-05-18T12:26:30Z"}],"graph_snapshots":[{"event_id":"sha256:5a29e95d10092f20dad6569cfe93678c55d56bf2613487f5390b1d4682354304","target":"graph","created_at":"2026-05-18T01:59:08Z","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 discuss the strong-field dynamics of HeH+, the simplest stable heteronuclear molecule, focusing on identifying a laser regime for which there is a sufficient dissociation signal for experimental measurement. We numerically solve the time-dependent Schr\\\"odinger equation to obtain total dissociation probabilities, kinetic energy release spectra, and momentum distributions for wavelengths from 800 nm to 2400 nm. The suitability of this simple system as a prototype for understanding the strong-field nuclear dynamics of heteronuclear dissociation is discussed.","authors_text":"B. D. Esry, D. Ursrey, F. Anis","cross_cats":["physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-12-15T23:13:44Z","title":"Multiphoton Dissociation of HeH+ below the He+(1s) + H(1s) Threshold"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.3688","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:e3a8b045e80449cda1365a611231c45f23d9f04980c7ab3a5cdd5d8deac5e991","target":"record","created_at":"2026-05-18T01:59:08Z","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":"f978ff4639736f2fae4147d7005560123a78061c71b87322b88e9925d2f77db3","cross_cats_sorted":["physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-12-15T23:13:44Z","title_canon_sha256":"46c92631703107f4a5ad14e6a10afaf1d06842c0ff797ff483403fff4d53f09d"},"schema_version":"1.0","source":{"id":"1112.3688","kind":"arxiv","version":1}},"canonical_sha256":"3a7c1dc384c3188b6ca2c4d42b3670a6b3edd1867ae72f138e8b9623b0bf2127","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3a7c1dc384c3188b6ca2c4d42b3670a6b3edd1867ae72f138e8b9623b0bf2127","first_computed_at":"2026-05-18T01:59:08.878046Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:59:08.878046Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NeAsTkRvLOC0cDlbWKqeJ4xaqK+LWfC2eHh1Dc1Q6KUk7h7lb/pfnxekdwEJmUMpZvrmLZ4IyahIvkykzWQmAA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:59:08.878785Z","signed_message":"canonical_sha256_bytes"},"source_id":"1112.3688","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e3a8b045e80449cda1365a611231c45f23d9f04980c7ab3a5cdd5d8deac5e991","sha256:5a29e95d10092f20dad6569cfe93678c55d56bf2613487f5390b1d4682354304"],"state_sha256":"8e8398ba64decf27b3d2472cc72bc97856a8f61b13f8d5412bf422cdaa09e145"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0yLCOZziQgENnYGtx1FWyL6OLBa6yVXrUpFC0TaxjRlfsqyMNkWq8IYcSxUchIA1vJcu59WI9KZzx1eEwkItCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T20:48:59.699137Z","bundle_sha256":"0285234748aa08114f03bacb7c128d789664fe928f39f764dd2c4928b978df56"}}