{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:4R67O5E46E3GSNXAUDFXS26OIK","short_pith_number":"pith:4R67O5E4","canonical_record":{"source":{"id":"1202.3846","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-02-17T06:26:23Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"ad25a4ad8eef78accd3c230e1ac0dc6cdc2ae352c54e0ca73b63ab45240217dd","abstract_canon_sha256":"9cb950e648bf1dc5055ee08fd2213a6546f2c62122c5fedf960566d72325af21"},"schema_version":"1.0"},"canonical_sha256":"e47df7749cf1366936e0a0cb796bce42a2b60c267123a19c6dfe2c5b84cec05b","source":{"kind":"arxiv","id":"1202.3846","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1202.3846","created_at":"2026-05-18T01:58:24Z"},{"alias_kind":"arxiv_version","alias_value":"1202.3846v2","created_at":"2026-05-18T01:58:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.3846","created_at":"2026-05-18T01:58:24Z"},{"alias_kind":"pith_short_12","alias_value":"4R67O5E46E3G","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_16","alias_value":"4R67O5E46E3GSNXA","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_8","alias_value":"4R67O5E4","created_at":"2026-05-18T12:26:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:4R67O5E46E3GSNXAUDFXS26OIK","target":"record","payload":{"canonical_record":{"source":{"id":"1202.3846","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-02-17T06:26:23Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"ad25a4ad8eef78accd3c230e1ac0dc6cdc2ae352c54e0ca73b63ab45240217dd","abstract_canon_sha256":"9cb950e648bf1dc5055ee08fd2213a6546f2c62122c5fedf960566d72325af21"},"schema_version":"1.0"},"canonical_sha256":"e47df7749cf1366936e0a0cb796bce42a2b60c267123a19c6dfe2c5b84cec05b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:24.193766Z","signature_b64":"g5+ovodMuJOq8O2zsi4Of9jOPkYF7f+e5WFUC9Omgs5njtCVEAvn1hzQHzouzSZzDj7Bl823/IdlKwMdZYFGAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e47df7749cf1366936e0a0cb796bce42a2b60c267123a19c6dfe2c5b84cec05b","last_reissued_at":"2026-05-18T01:58:24.193364Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:24.193364Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1202.3846","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":"2026-05-18T01:58:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"K7I+/YUJ286IOdd/23jLI7bduJGkkl92KxskEruP5p9KSNGdIfb2PwT2MdzeJmZ4rpplw9LnQumLXc/vYXKkCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-20T13:05:05.855919Z"},"content_sha256":"744ccbb9cb4d55fdc3f30677e65f50043d6d62503f73791050cbe3fa8d145c0e","schema_version":"1.0","event_id":"sha256:744ccbb9cb4d55fdc3f30677e65f50043d6d62503f73791050cbe3fa8d145c0e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:4R67O5E46E3GSNXAUDFXS26OIK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Multiscale non-adiabatic dynamics with radiative decay, case study on the post-ionization fragmentation of rare-gas tetramers","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"physics.chem-ph","authors_text":"Florent X. Gad\\'ea, Frederic Renard, Ivan Jane\\v{c}ek, Pavel Naar, Ren\\'e Kalus, Tom\\'a\\v{s} Jan\\v{c}a","submitted_at":"2012-02-17T06:26:23Z","abstract_excerpt":"In this supplementary material, we recollect, for reader's convenience, the general scheme of suggested multiscale model (Sec. 1), and basic informations about approaches used for pilot study: a detailed description of the interaction model (Sec. 2) and dynamical methods used for the dark dynamics step (Sec. 3) reported previously in two preceding studies [1, 2]. In addition, a detailed description of the treatment of radiative processes is also given (Sec. 4)."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.3846","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":"2026-05-18T01:58:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yeWYjsq3OugnVXIkH596Xrax8LtiQASsTdoUe7aHRifNFPTY3Ub3+dn33gqTx0f8P/+YVbWOy1Vkp5w62sBfCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-20T13:05:05.856658Z"},"content_sha256":"f13909ee89a9d9fec5d7c6075e4018dbf492305f44b65c781ef04215e03b9f40","schema_version":"1.0","event_id":"sha256:f13909ee89a9d9fec5d7c6075e4018dbf492305f44b65c781ef04215e03b9f40"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4R67O5E46E3GSNXAUDFXS26OIK/bundle.json","state_url":"https://pith.science/pith/4R67O5E46E3GSNXAUDFXS26OIK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4R67O5E46E3GSNXAUDFXS26OIK/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":"2026-08-20T13:05:05Z","links":{"resolver":"https://pith.science/pith/4R67O5E46E3GSNXAUDFXS26OIK","bundle":"https://pith.science/pith/4R67O5E46E3GSNXAUDFXS26OIK/bundle.json","state":"https://pith.science/pith/4R67O5E46E3GSNXAUDFXS26OIK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4R67O5E46E3GSNXAUDFXS26OIK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:4R67O5E46E3GSNXAUDFXS26OIK","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":"9cb950e648bf1dc5055ee08fd2213a6546f2c62122c5fedf960566d72325af21","cross_cats_sorted":["quant-ph"],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-02-17T06:26:23Z","title_canon_sha256":"ad25a4ad8eef78accd3c230e1ac0dc6cdc2ae352c54e0ca73b63ab45240217dd"},"schema_version":"1.0","source":{"id":"1202.3846","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1202.3846","created_at":"2026-05-18T01:58:24Z"},{"alias_kind":"arxiv_version","alias_value":"1202.3846v2","created_at":"2026-05-18T01:58:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.3846","created_at":"2026-05-18T01:58:24Z"},{"alias_kind":"pith_short_12","alias_value":"4R67O5E46E3G","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_16","alias_value":"4R67O5E46E3GSNXA","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_8","alias_value":"4R67O5E4","created_at":"2026-05-18T12:26:53Z"}],"graph_snapshots":[{"event_id":"sha256:f13909ee89a9d9fec5d7c6075e4018dbf492305f44b65c781ef04215e03b9f40","target":"graph","created_at":"2026-05-18T01:58:24Z","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 this supplementary material, we recollect, for reader's convenience, the general scheme of suggested multiscale model (Sec. 1), and basic informations about approaches used for pilot study: a detailed description of the interaction model (Sec. 2) and dynamical methods used for the dark dynamics step (Sec. 3) reported previously in two preceding studies [1, 2]. In addition, a detailed description of the treatment of radiative processes is also given (Sec. 4).","authors_text":"Florent X. Gad\\'ea, Frederic Renard, Ivan Jane\\v{c}ek, Pavel Naar, Ren\\'e Kalus, Tom\\'a\\v{s} Jan\\v{c}a","cross_cats":["quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-02-17T06:26:23Z","title":"Multiscale non-adiabatic dynamics with radiative decay, case study on the post-ionization fragmentation of rare-gas tetramers"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.3846","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":"sha256:744ccbb9cb4d55fdc3f30677e65f50043d6d62503f73791050cbe3fa8d145c0e","target":"record","created_at":"2026-05-18T01:58:24Z","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":"9cb950e648bf1dc5055ee08fd2213a6546f2c62122c5fedf960566d72325af21","cross_cats_sorted":["quant-ph"],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-02-17T06:26:23Z","title_canon_sha256":"ad25a4ad8eef78accd3c230e1ac0dc6cdc2ae352c54e0ca73b63ab45240217dd"},"schema_version":"1.0","source":{"id":"1202.3846","kind":"arxiv","version":2}},"canonical_sha256":"e47df7749cf1366936e0a0cb796bce42a2b60c267123a19c6dfe2c5b84cec05b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e47df7749cf1366936e0a0cb796bce42a2b60c267123a19c6dfe2c5b84cec05b","first_computed_at":"2026-05-18T01:58:24.193364Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:58:24.193364Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"g5+ovodMuJOq8O2zsi4Of9jOPkYF7f+e5WFUC9Omgs5njtCVEAvn1hzQHzouzSZzDj7Bl823/IdlKwMdZYFGAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:58:24.193766Z","signed_message":"canonical_sha256_bytes"},"source_id":"1202.3846","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:744ccbb9cb4d55fdc3f30677e65f50043d6d62503f73791050cbe3fa8d145c0e","sha256:f13909ee89a9d9fec5d7c6075e4018dbf492305f44b65c781ef04215e03b9f40"],"state_sha256":"70e7163dc0bdc54655ef3787c0be7de064ac8e5312f2a0b2a02372a754d12543"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+f3VU7x7oZqu3DwL1VZTY6qevFfxCL6AfXOO3kEvnbiJV53lWet7RM4Pn1vj0D8aPCskNeP7wDWnIi40WWlNAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-20T13:05:05.870615Z","bundle_sha256":"6de0ce692bc061946adbb007367b16696efd07664b6f8d87ed2911d67ed8c00e"}}