{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:5K5VU4TE73X6YILAYVNVA7NWUD","short_pith_number":"pith:5K5VU4TE","canonical_record":{"source":{"id":"1011.4605","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-11-20T19:55:15Z","cross_cats_sorted":["physics.chem-ph","physics.comp-ph","quant-ph"],"title_canon_sha256":"701e75269a58478fd450ec220e032e68d9c8eb8359c28ef7868fabcc03d25d87","abstract_canon_sha256":"65bc15cc65e9d9049c7c819dfe95c738e47fc81cfa01dd662c5bcf0062c8a597"},"schema_version":"1.0"},"canonical_sha256":"eabb5a7264feefec2160c55b507db6a0e51a5ea9f31914ae00d08dd14ebc1ca8","source":{"kind":"arxiv","id":"1011.4605","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1011.4605","created_at":"2026-05-18T04:17:03Z"},{"alias_kind":"arxiv_version","alias_value":"1011.4605v2","created_at":"2026-05-18T04:17:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.4605","created_at":"2026-05-18T04:17:03Z"},{"alias_kind":"pith_short_12","alias_value":"5K5VU4TE73X6","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"5K5VU4TE73X6YILA","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"5K5VU4TE","created_at":"2026-05-18T12:26:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:5K5VU4TE73X6YILAYVNVA7NWUD","target":"record","payload":{"canonical_record":{"source":{"id":"1011.4605","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-11-20T19:55:15Z","cross_cats_sorted":["physics.chem-ph","physics.comp-ph","quant-ph"],"title_canon_sha256":"701e75269a58478fd450ec220e032e68d9c8eb8359c28ef7868fabcc03d25d87","abstract_canon_sha256":"65bc15cc65e9d9049c7c819dfe95c738e47fc81cfa01dd662c5bcf0062c8a597"},"schema_version":"1.0"},"canonical_sha256":"eabb5a7264feefec2160c55b507db6a0e51a5ea9f31914ae00d08dd14ebc1ca8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:17:03.033447Z","signature_b64":"T28rwyMncF2MuatmAdrNioADKuBdKfZvLDt+0pncBHJFu5LJ23GzQuVSvkdcGLqYnu8cotjeg7dOHFf/YyOgCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eabb5a7264feefec2160c55b507db6a0e51a5ea9f31914ae00d08dd14ebc1ca8","last_reissued_at":"2026-05-18T04:17:03.032935Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:17:03.032935Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1011.4605","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":"2026-05-18T04:17:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"itxi6h8P3Gy3BN4BWy7TOTWt9go1ZCnR4f3ggdes3lbMahkU4svXvrO1ZbfNg4bgfKwSw4/CZ13BY21h1mdCCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T04:28:45.008113Z"},"content_sha256":"1b0dfc4ee812c8098c4271bf645d77d3c91cccaf4b4319a0e862be6db05ba59c","schema_version":"1.0","event_id":"sha256:1b0dfc4ee812c8098c4271bf645d77d3c91cccaf4b4319a0e862be6db05ba59c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:5K5VU4TE73X6YILAYVNVA7NWUD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nuclear classical dynamics of H$_2$ in intense laser field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.chem-ph","physics.comp-ph","quant-ph"],"primary_cat":"physics.atom-ph","authors_text":"Babak Shokri, Firoozeh Sami, Mohsen Vafaee","submitted_at":"2010-11-20T19:55:15Z","abstract_excerpt":"In the first part of this paper, the different distinguishable pathways and regions of the single and sequential double ionization are determined and discussed. It is shown that there are two distinguishable pathways for the single ionization and four distinct pathways for the sequential double ionization. It is also shown that there are two and three different regions of space which are related to the single and double ionization respectively. In the second part of the paper, the time dependent Schr\\\"{o}dinger and Newton equations are solved simultaneously for the electrons and the nuclei of "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.4605","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":"2026-05-18T04:17:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cowT9V0uJ/D3Oldftka32n/lo6lTKlFV0Cp5I5+KB10jsIKA3OwPZx6+lRbWM5v5LalpuQkxzJrUyR0hx6plAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T04:28:45.008733Z"},"content_sha256":"b1f3aa604622d8eff7380d3c365f1d929f1953da95438b5b6fa9623c59d6cd99","schema_version":"1.0","event_id":"sha256:b1f3aa604622d8eff7380d3c365f1d929f1953da95438b5b6fa9623c59d6cd99"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5K5VU4TE73X6YILAYVNVA7NWUD/bundle.json","state_url":"https://pith.science/pith/5K5VU4TE73X6YILAYVNVA7NWUD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5K5VU4TE73X6YILAYVNVA7NWUD/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":"2026-05-27T04:28:45Z","links":{"resolver":"https://pith.science/pith/5K5VU4TE73X6YILAYVNVA7NWUD","bundle":"https://pith.science/pith/5K5VU4TE73X6YILAYVNVA7NWUD/bundle.json","state":"https://pith.science/pith/5K5VU4TE73X6YILAYVNVA7NWUD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5K5VU4TE73X6YILAYVNVA7NWUD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:5K5VU4TE73X6YILAYVNVA7NWUD","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":"65bc15cc65e9d9049c7c819dfe95c738e47fc81cfa01dd662c5bcf0062c8a597","cross_cats_sorted":["physics.chem-ph","physics.comp-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-11-20T19:55:15Z","title_canon_sha256":"701e75269a58478fd450ec220e032e68d9c8eb8359c28ef7868fabcc03d25d87"},"schema_version":"1.0","source":{"id":"1011.4605","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1011.4605","created_at":"2026-05-18T04:17:03Z"},{"alias_kind":"arxiv_version","alias_value":"1011.4605v2","created_at":"2026-05-18T04:17:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.4605","created_at":"2026-05-18T04:17:03Z"},{"alias_kind":"pith_short_12","alias_value":"5K5VU4TE73X6","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"5K5VU4TE73X6YILA","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"5K5VU4TE","created_at":"2026-05-18T12:26:04Z"}],"graph_snapshots":[{"event_id":"sha256:b1f3aa604622d8eff7380d3c365f1d929f1953da95438b5b6fa9623c59d6cd99","target":"graph","created_at":"2026-05-18T04:17:03Z","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":"In the first part of this paper, the different distinguishable pathways and regions of the single and sequential double ionization are determined and discussed. It is shown that there are two distinguishable pathways for the single ionization and four distinct pathways for the sequential double ionization. It is also shown that there are two and three different regions of space which are related to the single and double ionization respectively. In the second part of the paper, the time dependent Schr\\\"{o}dinger and Newton equations are solved simultaneously for the electrons and the nuclei of ","authors_text":"Babak Shokri, Firoozeh Sami, Mohsen Vafaee","cross_cats":["physics.chem-ph","physics.comp-ph","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-11-20T19:55:15Z","title":"Nuclear classical dynamics of H$_2$ in intense laser field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.4605","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":"sha256:1b0dfc4ee812c8098c4271bf645d77d3c91cccaf4b4319a0e862be6db05ba59c","target":"record","created_at":"2026-05-18T04:17:03Z","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":"65bc15cc65e9d9049c7c819dfe95c738e47fc81cfa01dd662c5bcf0062c8a597","cross_cats_sorted":["physics.chem-ph","physics.comp-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-11-20T19:55:15Z","title_canon_sha256":"701e75269a58478fd450ec220e032e68d9c8eb8359c28ef7868fabcc03d25d87"},"schema_version":"1.0","source":{"id":"1011.4605","kind":"arxiv","version":2}},"canonical_sha256":"eabb5a7264feefec2160c55b507db6a0e51a5ea9f31914ae00d08dd14ebc1ca8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"eabb5a7264feefec2160c55b507db6a0e51a5ea9f31914ae00d08dd14ebc1ca8","first_computed_at":"2026-05-18T04:17:03.032935Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:17:03.032935Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"T28rwyMncF2MuatmAdrNioADKuBdKfZvLDt+0pncBHJFu5LJ23GzQuVSvkdcGLqYnu8cotjeg7dOHFf/YyOgCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:17:03.033447Z","signed_message":"canonical_sha256_bytes"},"source_id":"1011.4605","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1b0dfc4ee812c8098c4271bf645d77d3c91cccaf4b4319a0e862be6db05ba59c","sha256:b1f3aa604622d8eff7380d3c365f1d929f1953da95438b5b6fa9623c59d6cd99"],"state_sha256":"c31834e415faccde1b93c3b8762406018b1310dddb3698f037beaef74423aea0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"x18yUoU6Mxll6/c6Wb43P8pstL/zDrU86BmWIoQkGU7SQsOH7NjqCSPqTvRmdrVQPeGHU6mb5Vjx5Ff0eFokCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T04:28:45.012274Z","bundle_sha256":"e7413e4c11ca7a92eda56067186d36e5f89a4c245e8a8588ae6654b90bc41fea"}}