{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:UMSMSPW5FEH3NILVY4VWHWDSPD","short_pith_number":"pith:UMSMSPW5","canonical_record":{"source":{"id":"1808.09553","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2018-08-28T21:46:38Z","cross_cats_sorted":["physics.chem-ph","physics.comp-ph"],"title_canon_sha256":"e7ac2417154eca9d755dc73a84741b92673b87665582857d9136fdf2b354d8f8","abstract_canon_sha256":"9fdcf1b877089e60231667f98e276f7d22e7d99c7963b421856d0c0190b52253"},"schema_version":"1.0"},"canonical_sha256":"a324c93edd290fb6a175c72b63d87278c8dd91cb840dad77173ededadecc1393","source":{"kind":"arxiv","id":"1808.09553","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1808.09553","created_at":"2026-05-18T00:06:55Z"},{"alias_kind":"arxiv_version","alias_value":"1808.09553v1","created_at":"2026-05-18T00:06:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1808.09553","created_at":"2026-05-18T00:06:55Z"},{"alias_kind":"pith_short_12","alias_value":"UMSMSPW5FEH3","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_16","alias_value":"UMSMSPW5FEH3NILV","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_8","alias_value":"UMSMSPW5","created_at":"2026-05-18T12:32:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:UMSMSPW5FEH3NILVY4VWHWDSPD","target":"record","payload":{"canonical_record":{"source":{"id":"1808.09553","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2018-08-28T21:46:38Z","cross_cats_sorted":["physics.chem-ph","physics.comp-ph"],"title_canon_sha256":"e7ac2417154eca9d755dc73a84741b92673b87665582857d9136fdf2b354d8f8","abstract_canon_sha256":"9fdcf1b877089e60231667f98e276f7d22e7d99c7963b421856d0c0190b52253"},"schema_version":"1.0"},"canonical_sha256":"a324c93edd290fb6a175c72b63d87278c8dd91cb840dad77173ededadecc1393","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:06:55.223897Z","signature_b64":"KHmID3IfYEeFWZAVOQqir17ofHMzpVE20AGt8IRg3owRFWyFFZLTb/Fmz9XJNvPVzaRIugssInQGWvjcTbHiBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a324c93edd290fb6a175c72b63d87278c8dd91cb840dad77173ededadecc1393","last_reissued_at":"2026-05-18T00:06:55.223451Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:06:55.223451Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1808.09553","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":"2026-05-18T00:06:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rHZFQo+JeqHJeP9SpMZ/kxJgT9eq5BoB0xrwZ0To7Ex3xoE+Csf2EMPiacvMmkmJ1NxgZf0oBMx/h9jP4OhQBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T17:38:50.498280Z"},"content_sha256":"b069a0c90abfbabcb94aaae9c75ac0e108bac9b76082d66d2e3b3951902e84a8","schema_version":"1.0","event_id":"sha256:b069a0c90abfbabcb94aaae9c75ac0e108bac9b76082d66d2e3b3951902e84a8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:UMSMSPW5FEH3NILVY4VWHWDSPD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nonadiabatic electron dynamics effects on high-harmonic generation spectrum of H$_2^+$: minima and oscillatory pattern","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.chem-ph","physics.comp-ph"],"primary_cat":"physics.atom-ph","authors_text":"Mohsen Vafaee, Sajad Taghipour","submitted_at":"2018-08-28T21:46:38Z","abstract_excerpt":"We numerically solved the full-dimensional electronic time-dependent Schr\\\"{o}dinger equation for H$_2^+$ with Born-Oppenheimer approximation under different sin$^2$-shaped and trapezoidal laser pulses at some different wavelengths, with $I=$1 $\\times 10^{13}$ Wcm$^{-2}$, 3 $\\times 10^{13}$ Wcm$^{-2}$, and 6 $\\times 10^{13}$ Wcm$^{-2}$ intensity at 4.73 a.u. and 7.0 a.u. internuclear distances. Some structures such as complexity, minima, and oscillatory patterns appeared in the high-order harmonic generation (HHG) spectra are investigated in this work by considering the electron localization, "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.09553","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":"2026-05-18T00:06:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"n0FtPCncUzRxlisoKPATUf+B3qU84/yzaLk+1aLr6rpFxywq5gN6vrwcUO0LjAHkAnf1s3Fjv21RsmHSddv+Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T17:38:50.499041Z"},"content_sha256":"d96871cf8a3fa3789366e99a9654b9bc0043a5ba54a7e92d99fef406d5e1af31","schema_version":"1.0","event_id":"sha256:d96871cf8a3fa3789366e99a9654b9bc0043a5ba54a7e92d99fef406d5e1af31"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UMSMSPW5FEH3NILVY4VWHWDSPD/bundle.json","state_url":"https://pith.science/pith/UMSMSPW5FEH3NILVY4VWHWDSPD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UMSMSPW5FEH3NILVY4VWHWDSPD/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":"2026-05-26T17:38:50Z","links":{"resolver":"https://pith.science/pith/UMSMSPW5FEH3NILVY4VWHWDSPD","bundle":"https://pith.science/pith/UMSMSPW5FEH3NILVY4VWHWDSPD/bundle.json","state":"https://pith.science/pith/UMSMSPW5FEH3NILVY4VWHWDSPD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UMSMSPW5FEH3NILVY4VWHWDSPD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:UMSMSPW5FEH3NILVY4VWHWDSPD","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":"9fdcf1b877089e60231667f98e276f7d22e7d99c7963b421856d0c0190b52253","cross_cats_sorted":["physics.chem-ph","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2018-08-28T21:46:38Z","title_canon_sha256":"e7ac2417154eca9d755dc73a84741b92673b87665582857d9136fdf2b354d8f8"},"schema_version":"1.0","source":{"id":"1808.09553","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1808.09553","created_at":"2026-05-18T00:06:55Z"},{"alias_kind":"arxiv_version","alias_value":"1808.09553v1","created_at":"2026-05-18T00:06:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1808.09553","created_at":"2026-05-18T00:06:55Z"},{"alias_kind":"pith_short_12","alias_value":"UMSMSPW5FEH3","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_16","alias_value":"UMSMSPW5FEH3NILV","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_8","alias_value":"UMSMSPW5","created_at":"2026-05-18T12:32:56Z"}],"graph_snapshots":[{"event_id":"sha256:d96871cf8a3fa3789366e99a9654b9bc0043a5ba54a7e92d99fef406d5e1af31","target":"graph","created_at":"2026-05-18T00:06:55Z","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 numerically solved the full-dimensional electronic time-dependent Schr\\\"{o}dinger equation for H$_2^+$ with Born-Oppenheimer approximation under different sin$^2$-shaped and trapezoidal laser pulses at some different wavelengths, with $I=$1 $\\times 10^{13}$ Wcm$^{-2}$, 3 $\\times 10^{13}$ Wcm$^{-2}$, and 6 $\\times 10^{13}$ Wcm$^{-2}$ intensity at 4.73 a.u. and 7.0 a.u. internuclear distances. Some structures such as complexity, minima, and oscillatory patterns appeared in the high-order harmonic generation (HHG) spectra are investigated in this work by considering the electron localization, ","authors_text":"Mohsen Vafaee, Sajad Taghipour","cross_cats":["physics.chem-ph","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2018-08-28T21:46:38Z","title":"Nonadiabatic electron dynamics effects on high-harmonic generation spectrum of H$_2^+$: minima and oscillatory pattern"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.09553","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:b069a0c90abfbabcb94aaae9c75ac0e108bac9b76082d66d2e3b3951902e84a8","target":"record","created_at":"2026-05-18T00:06:55Z","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":"9fdcf1b877089e60231667f98e276f7d22e7d99c7963b421856d0c0190b52253","cross_cats_sorted":["physics.chem-ph","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2018-08-28T21:46:38Z","title_canon_sha256":"e7ac2417154eca9d755dc73a84741b92673b87665582857d9136fdf2b354d8f8"},"schema_version":"1.0","source":{"id":"1808.09553","kind":"arxiv","version":1}},"canonical_sha256":"a324c93edd290fb6a175c72b63d87278c8dd91cb840dad77173ededadecc1393","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a324c93edd290fb6a175c72b63d87278c8dd91cb840dad77173ededadecc1393","first_computed_at":"2026-05-18T00:06:55.223451Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:06:55.223451Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"KHmID3IfYEeFWZAVOQqir17ofHMzpVE20AGt8IRg3owRFWyFFZLTb/Fmz9XJNvPVzaRIugssInQGWvjcTbHiBw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:06:55.223897Z","signed_message":"canonical_sha256_bytes"},"source_id":"1808.09553","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b069a0c90abfbabcb94aaae9c75ac0e108bac9b76082d66d2e3b3951902e84a8","sha256:d96871cf8a3fa3789366e99a9654b9bc0043a5ba54a7e92d99fef406d5e1af31"],"state_sha256":"44c27aed607e4d0be02641ba05cde9785392bf2e29d645848b3b142f90280b4c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UPUmlw3dHVjux5xgL4lN6iKPJhUoPxJEWB9XMkjstrPZu/uzbZj1zI7rWtSjI0hQZhD76fv+ye+j3WRC+3BSCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T17:38:50.503007Z","bundle_sha256":"d0b372e40cca33d20a6b7a14c5df7e9b060215d6413a2c17073ef02000003b87"}}