{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:TZ6LMXAP7S5FLH5S3HR75VVWTN","short_pith_number":"pith:TZ6LMXAP","canonical_record":{"source":{"id":"1103.1565","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atm-clus","submitted_at":"2011-03-08T15:48:04Z","cross_cats_sorted":["physics.atom-ph","physics.chem-ph"],"title_canon_sha256":"7706b15108c65ca978f1d04d826212db1454438560c1c47a0adba107717b6d6a","abstract_canon_sha256":"7f143db102d6153314d2253676c245c1bd204ab757a499749d507fa1b2fa39cf"},"schema_version":"1.0"},"canonical_sha256":"9e7cb65c0ffcba559fb2d9e3fed6b69b7e271e010fba744df1d9a448455a4dc5","source":{"kind":"arxiv","id":"1103.1565","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1103.1565","created_at":"2026-05-18T04:16:01Z"},{"alias_kind":"arxiv_version","alias_value":"1103.1565v2","created_at":"2026-05-18T04:16:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1103.1565","created_at":"2026-05-18T04:16:01Z"},{"alias_kind":"pith_short_12","alias_value":"TZ6LMXAP7S5F","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"TZ6LMXAP7S5FLH5S","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"TZ6LMXAP","created_at":"2026-05-18T12:26:42Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:TZ6LMXAP7S5FLH5S3HR75VVWTN","target":"record","payload":{"canonical_record":{"source":{"id":"1103.1565","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atm-clus","submitted_at":"2011-03-08T15:48:04Z","cross_cats_sorted":["physics.atom-ph","physics.chem-ph"],"title_canon_sha256":"7706b15108c65ca978f1d04d826212db1454438560c1c47a0adba107717b6d6a","abstract_canon_sha256":"7f143db102d6153314d2253676c245c1bd204ab757a499749d507fa1b2fa39cf"},"schema_version":"1.0"},"canonical_sha256":"9e7cb65c0ffcba559fb2d9e3fed6b69b7e271e010fba744df1d9a448455a4dc5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:16:01.899284Z","signature_b64":"ZE8K31sWREx3NOKubTChrNWJDGLtpIfkujRg5oDGSDTmXX5B62RGJVWWqWps2hvROERoe1GmMNNEiaEYAEJRDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9e7cb65c0ffcba559fb2d9e3fed6b69b7e271e010fba744df1d9a448455a4dc5","last_reissued_at":"2026-05-18T04:16:01.898529Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:16:01.898529Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1103.1565","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:16:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ntNinYMyjPB0ILZwfqcZtPPvIp60V4BpMi0f89WIw8i/q1CxalNgD+20LoLTBYVAlF37Fr9MmLHWky+RO3nACw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T13:50:47.973929Z"},"content_sha256":"08951d286aa7df901032e501bd5ec3dd41e6b298b030492e7f8050c322f7c7dd","schema_version":"1.0","event_id":"sha256:08951d286aa7df901032e501bd5ec3dd41e6b298b030492e7f8050c322f7c7dd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:TZ6LMXAP7S5FLH5S3HR75VVWTN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Complete dynamics of H2+ in strong laser fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","physics.chem-ph"],"primary_cat":"physics.atm-clus","authors_text":"F. Grossmann, J. Handt, J. M. Rost, M. Fischer, R. Schmidt, S. M. Krause","submitted_at":"2011-03-08T15:48:04Z","abstract_excerpt":"Based on a combined quantum-classical treatment, a complete study of the strong field dynamics of H2+, i.e. including all nuclear and electronic DOF as well as dissociation and ionization, is presented. We find that the ro-vibrational nuclear dynamics enhances dissociation and, at the same time, suppresses ionization, confirming experimental observations by I. Ben-Itzhak et al. [Phys. Rev. Lett. 95, 073002 (2005)]. In addition and counter-intuitively, it is shown that for large initial vibrational excitation ionization takes place favorably at large angles between the laser polarization and mo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1103.1565","kind":"arxiv","version":2},"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":"2026-05-18T04:16:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Jqlt93htUoe6SZZm8aWfoAuV7iiP5xNg804dRTRUPuy+itWtdTYvj6HNJFR3wdHl+JLfHDLnJ7CYXzpE8/SOCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T13:50:47.974278Z"},"content_sha256":"3d50e662c3a2c08459827648f9f6b14e3aa52d6e68790fad3dfc39e3bc4fd050","schema_version":"1.0","event_id":"sha256:3d50e662c3a2c08459827648f9f6b14e3aa52d6e68790fad3dfc39e3bc4fd050"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TZ6LMXAP7S5FLH5S3HR75VVWTN/bundle.json","state_url":"https://pith.science/pith/TZ6LMXAP7S5FLH5S3HR75VVWTN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TZ6LMXAP7S5FLH5S3HR75VVWTN/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":"2026-06-27T13:50:47Z","links":{"resolver":"https://pith.science/pith/TZ6LMXAP7S5FLH5S3HR75VVWTN","bundle":"https://pith.science/pith/TZ6LMXAP7S5FLH5S3HR75VVWTN/bundle.json","state":"https://pith.science/pith/TZ6LMXAP7S5FLH5S3HR75VVWTN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TZ6LMXAP7S5FLH5S3HR75VVWTN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:TZ6LMXAP7S5FLH5S3HR75VVWTN","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":"7f143db102d6153314d2253676c245c1bd204ab757a499749d507fa1b2fa39cf","cross_cats_sorted":["physics.atom-ph","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atm-clus","submitted_at":"2011-03-08T15:48:04Z","title_canon_sha256":"7706b15108c65ca978f1d04d826212db1454438560c1c47a0adba107717b6d6a"},"schema_version":"1.0","source":{"id":"1103.1565","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1103.1565","created_at":"2026-05-18T04:16:01Z"},{"alias_kind":"arxiv_version","alias_value":"1103.1565v2","created_at":"2026-05-18T04:16:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1103.1565","created_at":"2026-05-18T04:16:01Z"},{"alias_kind":"pith_short_12","alias_value":"TZ6LMXAP7S5F","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"TZ6LMXAP7S5FLH5S","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"TZ6LMXAP","created_at":"2026-05-18T12:26:42Z"}],"graph_snapshots":[{"event_id":"sha256:3d50e662c3a2c08459827648f9f6b14e3aa52d6e68790fad3dfc39e3bc4fd050","target":"graph","created_at":"2026-05-18T04:16:01Z","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":"Based on a combined quantum-classical treatment, a complete study of the strong field dynamics of H2+, i.e. including all nuclear and electronic DOF as well as dissociation and ionization, is presented. We find that the ro-vibrational nuclear dynamics enhances dissociation and, at the same time, suppresses ionization, confirming experimental observations by I. Ben-Itzhak et al. [Phys. Rev. Lett. 95, 073002 (2005)]. In addition and counter-intuitively, it is shown that for large initial vibrational excitation ionization takes place favorably at large angles between the laser polarization and mo","authors_text":"F. Grossmann, J. Handt, J. M. Rost, M. Fischer, R. Schmidt, S. M. Krause","cross_cats":["physics.atom-ph","physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atm-clus","submitted_at":"2011-03-08T15:48:04Z","title":"Complete dynamics of H2+ in strong laser fields"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1103.1565","kind":"arxiv","version":2},"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":"sha256:08951d286aa7df901032e501bd5ec3dd41e6b298b030492e7f8050c322f7c7dd","target":"record","created_at":"2026-05-18T04:16:01Z","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":"7f143db102d6153314d2253676c245c1bd204ab757a499749d507fa1b2fa39cf","cross_cats_sorted":["physics.atom-ph","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atm-clus","submitted_at":"2011-03-08T15:48:04Z","title_canon_sha256":"7706b15108c65ca978f1d04d826212db1454438560c1c47a0adba107717b6d6a"},"schema_version":"1.0","source":{"id":"1103.1565","kind":"arxiv","version":2}},"canonical_sha256":"9e7cb65c0ffcba559fb2d9e3fed6b69b7e271e010fba744df1d9a448455a4dc5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9e7cb65c0ffcba559fb2d9e3fed6b69b7e271e010fba744df1d9a448455a4dc5","first_computed_at":"2026-05-18T04:16:01.898529Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:16:01.898529Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZE8K31sWREx3NOKubTChrNWJDGLtpIfkujRg5oDGSDTmXX5B62RGJVWWqWps2hvROERoe1GmMNNEiaEYAEJRDA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:16:01.899284Z","signed_message":"canonical_sha256_bytes"},"source_id":"1103.1565","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:08951d286aa7df901032e501bd5ec3dd41e6b298b030492e7f8050c322f7c7dd","sha256:3d50e662c3a2c08459827648f9f6b14e3aa52d6e68790fad3dfc39e3bc4fd050"],"state_sha256":"6af1753e7f50405a51043db484444acb79f1a4d211ccf3de8c3fe9f8835de601"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dv/NwQvuky1VLaxmi37T62CrN4veSK4Q6U4jNesaHCnZNfpBbAVHFPv91i8e3BFBHI4h+AUzZ/5rcM06fanJAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-27T13:50:47.976161Z","bundle_sha256":"11e59daf0013cba8c64074496d571bae12ebbd17d3c9efc2a268310368ea1517"}}