{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:NGFJ5J6LDDVYF3UTSKLJWMHWM3","short_pith_number":"pith:NGFJ5J6L","canonical_record":{"source":{"id":"1604.04507","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-04-15T13:53:13Z","cross_cats_sorted":[],"title_canon_sha256":"bada3d6356e12d5a6cbd3477621039fd8bddc2f38596b422c28b65075ce2e29f","abstract_canon_sha256":"f693339d98fd31b3e5fb4782853fb9495b086a0e3619005e0ab567bfa23c72bb"},"schema_version":"1.0"},"canonical_sha256":"698a9ea7cb18eb82ee9392969b30f666de93d845f81d1d4c4d0fe54bb0fd51bd","source":{"kind":"arxiv","id":"1604.04507","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.04507","created_at":"2026-05-18T00:45:49Z"},{"alias_kind":"arxiv_version","alias_value":"1604.04507v1","created_at":"2026-05-18T00:45:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.04507","created_at":"2026-05-18T00:45:49Z"},{"alias_kind":"pith_short_12","alias_value":"NGFJ5J6LDDVY","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"NGFJ5J6LDDVYF3UT","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"NGFJ5J6L","created_at":"2026-05-18T12:30:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:NGFJ5J6LDDVYF3UTSKLJWMHWM3","target":"record","payload":{"canonical_record":{"source":{"id":"1604.04507","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-04-15T13:53:13Z","cross_cats_sorted":[],"title_canon_sha256":"bada3d6356e12d5a6cbd3477621039fd8bddc2f38596b422c28b65075ce2e29f","abstract_canon_sha256":"f693339d98fd31b3e5fb4782853fb9495b086a0e3619005e0ab567bfa23c72bb"},"schema_version":"1.0"},"canonical_sha256":"698a9ea7cb18eb82ee9392969b30f666de93d845f81d1d4c4d0fe54bb0fd51bd","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:45:49.594566Z","signature_b64":"KBnGcbZkLHsdOfGFB+mCf3kSdwcxuq91ZjSEwo0C1l33Icl6tqN0a76JEzlsBu4RfESLfo6HyXc1DfjniVEyDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"698a9ea7cb18eb82ee9392969b30f666de93d845f81d1d4c4d0fe54bb0fd51bd","last_reissued_at":"2026-05-18T00:45:49.593832Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:45:49.593832Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1604.04507","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":"2026-05-18T00:45:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DO+NX7e6uogjxtehb2mP1HBP5KAj4s9QwPHFATXSFVx+vA36BU83Uw3p6YpkIa5lNTzQAo2nBm+oW7TDF5hLBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-20T08:41:33.403545Z"},"content_sha256":"c4b53bcf1ad06e24b8b884d6e42beec5064587d9b611eff70688396218e98668","schema_version":"1.0","event_id":"sha256:c4b53bcf1ad06e24b8b884d6e42beec5064587d9b611eff70688396218e98668"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:NGFJ5J6LDDVYF3UTSKLJWMHWM3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Correlations between the final momenta of electrons and their initial phase-space distribution in the process of tunnel ionization","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Karoly Tokesi, Peter Dombi, Peter Foldi, Viktor Ayadi","submitted_at":"2016-04-15T13:53:13Z","abstract_excerpt":"We present both full quantum mechanical and semiclassical calculations of above threshold ionization (ATI) of a hydrogen atom in the tunneling regime by a few-cycle linearly polarized infrared laser pulse. As a quantum treatment, we applied the direct integration of the time dependent Schr\\\"odinger equation (TDSE). In the semiclassical approximation (SCA), it is assumed that wavepacket propagation in the post-tunneling process can be well described within the classical framework. With these two methods, we analyze the similarities and deviations for ionization of the hydrogen atom. We found th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.04507","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":"2026-05-18T00:45:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aLJPU7oG3CIrdlF8EPklvVy6h5b+yPPPtUZZseGrp7F34rK6egb6FYiijlMxWuRmtcQEyRfO/DKuUvFLdhoqAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-20T08:41:33.403898Z"},"content_sha256":"accd695bc77b8eaf7c0ce35350bb2de08e4b84bb8742411a13d8e095d9007795","schema_version":"1.0","event_id":"sha256:accd695bc77b8eaf7c0ce35350bb2de08e4b84bb8742411a13d8e095d9007795"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NGFJ5J6LDDVYF3UTSKLJWMHWM3/bundle.json","state_url":"https://pith.science/pith/NGFJ5J6LDDVYF3UTSKLJWMHWM3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NGFJ5J6LDDVYF3UTSKLJWMHWM3/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":"2026-06-20T08:41:33Z","links":{"resolver":"https://pith.science/pith/NGFJ5J6LDDVYF3UTSKLJWMHWM3","bundle":"https://pith.science/pith/NGFJ5J6LDDVYF3UTSKLJWMHWM3/bundle.json","state":"https://pith.science/pith/NGFJ5J6LDDVYF3UTSKLJWMHWM3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NGFJ5J6LDDVYF3UTSKLJWMHWM3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:NGFJ5J6LDDVYF3UTSKLJWMHWM3","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":"f693339d98fd31b3e5fb4782853fb9495b086a0e3619005e0ab567bfa23c72bb","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-04-15T13:53:13Z","title_canon_sha256":"bada3d6356e12d5a6cbd3477621039fd8bddc2f38596b422c28b65075ce2e29f"},"schema_version":"1.0","source":{"id":"1604.04507","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.04507","created_at":"2026-05-18T00:45:49Z"},{"alias_kind":"arxiv_version","alias_value":"1604.04507v1","created_at":"2026-05-18T00:45:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.04507","created_at":"2026-05-18T00:45:49Z"},{"alias_kind":"pith_short_12","alias_value":"NGFJ5J6LDDVY","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"NGFJ5J6LDDVYF3UT","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"NGFJ5J6L","created_at":"2026-05-18T12:30:32Z"}],"graph_snapshots":[{"event_id":"sha256:accd695bc77b8eaf7c0ce35350bb2de08e4b84bb8742411a13d8e095d9007795","target":"graph","created_at":"2026-05-18T00:45:49Z","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 present both full quantum mechanical and semiclassical calculations of above threshold ionization (ATI) of a hydrogen atom in the tunneling regime by a few-cycle linearly polarized infrared laser pulse. As a quantum treatment, we applied the direct integration of the time dependent Schr\\\"odinger equation (TDSE). In the semiclassical approximation (SCA), it is assumed that wavepacket propagation in the post-tunneling process can be well described within the classical framework. With these two methods, we analyze the similarities and deviations for ionization of the hydrogen atom. We found th","authors_text":"Karoly Tokesi, Peter Dombi, Peter Foldi, Viktor Ayadi","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-04-15T13:53:13Z","title":"Correlations between the final momenta of electrons and their initial phase-space distribution in the process of tunnel ionization"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.04507","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:c4b53bcf1ad06e24b8b884d6e42beec5064587d9b611eff70688396218e98668","target":"record","created_at":"2026-05-18T00:45:49Z","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":"f693339d98fd31b3e5fb4782853fb9495b086a0e3619005e0ab567bfa23c72bb","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-04-15T13:53:13Z","title_canon_sha256":"bada3d6356e12d5a6cbd3477621039fd8bddc2f38596b422c28b65075ce2e29f"},"schema_version":"1.0","source":{"id":"1604.04507","kind":"arxiv","version":1}},"canonical_sha256":"698a9ea7cb18eb82ee9392969b30f666de93d845f81d1d4c4d0fe54bb0fd51bd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"698a9ea7cb18eb82ee9392969b30f666de93d845f81d1d4c4d0fe54bb0fd51bd","first_computed_at":"2026-05-18T00:45:49.593832Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:45:49.593832Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"KBnGcbZkLHsdOfGFB+mCf3kSdwcxuq91ZjSEwo0C1l33Icl6tqN0a76JEzlsBu4RfESLfo6HyXc1DfjniVEyDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:45:49.594566Z","signed_message":"canonical_sha256_bytes"},"source_id":"1604.04507","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c4b53bcf1ad06e24b8b884d6e42beec5064587d9b611eff70688396218e98668","sha256:accd695bc77b8eaf7c0ce35350bb2de08e4b84bb8742411a13d8e095d9007795"],"state_sha256":"cf6acc5758fea2bab751c25bbefcfa16e38b5af2c7da302ee852d1a54f0d0bb2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"B7bacZ5vNCWYRQ32ukyV0XUi6WjUh89+NQ9T7cBJ3Cp3ZnERshzTBgSzd15OC3P7AWCHIBvO+1pt/r7p/FNDBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-20T08:41:33.405866Z","bundle_sha256":"2b0a62ef2323e17cabbdf10dcea380b71fe28f08394c42618e5634667cab1513"}}