{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:IJJ4MAQNJ3XBBAKKQMJHPCNFHF","short_pith_number":"pith:IJJ4MAQN","canonical_record":{"source":{"id":"1811.10332","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-11-26T12:44:59Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"d88c23e6538eecb81bc66ba30da30a97a8eba537a79b52703bd9342141cc1f11","abstract_canon_sha256":"54fa749dd229665b73ba3c1c67462c8f7994d6618e3ba363323803299096da8b"},"schema_version":"1.0"},"canonical_sha256":"4253c6020d4eee10814a83127789a5397b35cf18d6de574208dcd1bfb487dc0c","source":{"kind":"arxiv","id":"1811.10332","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1811.10332","created_at":"2026-05-17T23:59:56Z"},{"alias_kind":"arxiv_version","alias_value":"1811.10332v1","created_at":"2026-05-17T23:59:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.10332","created_at":"2026-05-17T23:59:56Z"},{"alias_kind":"pith_short_12","alias_value":"IJJ4MAQNJ3XB","created_at":"2026-05-18T12:32:31Z"},{"alias_kind":"pith_short_16","alias_value":"IJJ4MAQNJ3XBBAKK","created_at":"2026-05-18T12:32:31Z"},{"alias_kind":"pith_short_8","alias_value":"IJJ4MAQN","created_at":"2026-05-18T12:32:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:IJJ4MAQNJ3XBBAKKQMJHPCNFHF","target":"record","payload":{"canonical_record":{"source":{"id":"1811.10332","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-11-26T12:44:59Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"d88c23e6538eecb81bc66ba30da30a97a8eba537a79b52703bd9342141cc1f11","abstract_canon_sha256":"54fa749dd229665b73ba3c1c67462c8f7994d6618e3ba363323803299096da8b"},"schema_version":"1.0"},"canonical_sha256":"4253c6020d4eee10814a83127789a5397b35cf18d6de574208dcd1bfb487dc0c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:56.753001Z","signature_b64":"9bJkas0wGx3Q8DdABCW8WIJSzZUwrOzV73jKh+N6ejH/9U+q84eB3+FZse9dyq2JtW3IGWEEU+0Pe5XcSqBlBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4253c6020d4eee10814a83127789a5397b35cf18d6de574208dcd1bfb487dc0c","last_reissued_at":"2026-05-17T23:59:56.752405Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:56.752405Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1811.10332","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":"2026-05-17T23:59:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cX/07RW7Yp+PKs4I7j9ifq6LOY+5/ZU413FSOCp6rBdxXnRkJnjGPD5PoviEcaer2JIn23I0YrTNDecZch/3Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T12:19:33.710587Z"},"content_sha256":"383ab5c3f8d7fbef742b966ed73ce4c72ba3192b4bf2734d2a6408bf4e30995d","schema_version":"1.0","event_id":"sha256:383ab5c3f8d7fbef742b966ed73ce4c72ba3192b4bf2734d2a6408bf4e30995d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:IJJ4MAQNJ3XBBAKKQMJHPCNFHF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Unexpected composition dependence of the first sharp diffraction peak in an alcohol-aldehyde liquid mixture: n-pentanol and pentanal","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft"],"primary_cat":"physics.chem-ph","authors_text":"Andrej Jamnik, Ildik\\'o Pethes, L\\'aszl\\'o Pusztai, L\\'aszl\\'o Temleitner, Matija Tom\\v{s}i\\v{c}","submitted_at":"2018-11-26T12:44:59Z","abstract_excerpt":"The total scattering structure factors of pure liquid n-pentanol, pentanal, and 5 of their mixtures, as determined by high energy synchrotron X-ray diffraction experiments, are presented. For the interpretation of measured data, molecular dynamics computer simulations are performed, utilizing 'all-atom' type force fields. The diffraction signals in general resemble each other over most of the monitored Q range above 1 ${\\AA}^{-1}$, but the absolute values of the intensities of the small-angle scattering maximum ('pre-peak', 'first sharp diffraction peak'), around 0.6 ${\\AA}^{-1}$, change in an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.10332","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":"2026-05-17T23:59:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"u2NiqEpkKVzzJOVFCGssjXddJTUh6EeagGlibRAuWKIlL3eDJCcP++6iDMjQNzBpNXgvW66FG8tZs3FIfMfYAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T12:19:33.710922Z"},"content_sha256":"84d7286f57eea3170faebf5b9ddd5bc0b2b8fae51442d2ebeceb6d2913e8c064","schema_version":"1.0","event_id":"sha256:84d7286f57eea3170faebf5b9ddd5bc0b2b8fae51442d2ebeceb6d2913e8c064"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IJJ4MAQNJ3XBBAKKQMJHPCNFHF/bundle.json","state_url":"https://pith.science/pith/IJJ4MAQNJ3XBBAKKQMJHPCNFHF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IJJ4MAQNJ3XBBAKKQMJHPCNFHF/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":"2026-05-31T12:19:33Z","links":{"resolver":"https://pith.science/pith/IJJ4MAQNJ3XBBAKKQMJHPCNFHF","bundle":"https://pith.science/pith/IJJ4MAQNJ3XBBAKKQMJHPCNFHF/bundle.json","state":"https://pith.science/pith/IJJ4MAQNJ3XBBAKKQMJHPCNFHF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IJJ4MAQNJ3XBBAKKQMJHPCNFHF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:IJJ4MAQNJ3XBBAKKQMJHPCNFHF","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":"54fa749dd229665b73ba3c1c67462c8f7994d6618e3ba363323803299096da8b","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-11-26T12:44:59Z","title_canon_sha256":"d88c23e6538eecb81bc66ba30da30a97a8eba537a79b52703bd9342141cc1f11"},"schema_version":"1.0","source":{"id":"1811.10332","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1811.10332","created_at":"2026-05-17T23:59:56Z"},{"alias_kind":"arxiv_version","alias_value":"1811.10332v1","created_at":"2026-05-17T23:59:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.10332","created_at":"2026-05-17T23:59:56Z"},{"alias_kind":"pith_short_12","alias_value":"IJJ4MAQNJ3XB","created_at":"2026-05-18T12:32:31Z"},{"alias_kind":"pith_short_16","alias_value":"IJJ4MAQNJ3XBBAKK","created_at":"2026-05-18T12:32:31Z"},{"alias_kind":"pith_short_8","alias_value":"IJJ4MAQN","created_at":"2026-05-18T12:32:31Z"}],"graph_snapshots":[{"event_id":"sha256:84d7286f57eea3170faebf5b9ddd5bc0b2b8fae51442d2ebeceb6d2913e8c064","target":"graph","created_at":"2026-05-17T23:59:56Z","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":"The total scattering structure factors of pure liquid n-pentanol, pentanal, and 5 of their mixtures, as determined by high energy synchrotron X-ray diffraction experiments, are presented. For the interpretation of measured data, molecular dynamics computer simulations are performed, utilizing 'all-atom' type force fields. The diffraction signals in general resemble each other over most of the monitored Q range above 1 ${\\AA}^{-1}$, but the absolute values of the intensities of the small-angle scattering maximum ('pre-peak', 'first sharp diffraction peak'), around 0.6 ${\\AA}^{-1}$, change in an","authors_text":"Andrej Jamnik, Ildik\\'o Pethes, L\\'aszl\\'o Pusztai, L\\'aszl\\'o Temleitner, Matija Tom\\v{s}i\\v{c}","cross_cats":["cond-mat.soft"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-11-26T12:44:59Z","title":"Unexpected composition dependence of the first sharp diffraction peak in an alcohol-aldehyde liquid mixture: n-pentanol and pentanal"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.10332","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":"sha256:383ab5c3f8d7fbef742b966ed73ce4c72ba3192b4bf2734d2a6408bf4e30995d","target":"record","created_at":"2026-05-17T23:59:56Z","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":"54fa749dd229665b73ba3c1c67462c8f7994d6618e3ba363323803299096da8b","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-11-26T12:44:59Z","title_canon_sha256":"d88c23e6538eecb81bc66ba30da30a97a8eba537a79b52703bd9342141cc1f11"},"schema_version":"1.0","source":{"id":"1811.10332","kind":"arxiv","version":1}},"canonical_sha256":"4253c6020d4eee10814a83127789a5397b35cf18d6de574208dcd1bfb487dc0c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4253c6020d4eee10814a83127789a5397b35cf18d6de574208dcd1bfb487dc0c","first_computed_at":"2026-05-17T23:59:56.752405Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:59:56.752405Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9bJkas0wGx3Q8DdABCW8WIJSzZUwrOzV73jKh+N6ejH/9U+q84eB3+FZse9dyq2JtW3IGWEEU+0Pe5XcSqBlBQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:59:56.753001Z","signed_message":"canonical_sha256_bytes"},"source_id":"1811.10332","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:383ab5c3f8d7fbef742b966ed73ce4c72ba3192b4bf2734d2a6408bf4e30995d","sha256:84d7286f57eea3170faebf5b9ddd5bc0b2b8fae51442d2ebeceb6d2913e8c064"],"state_sha256":"f1a83971bb5ee1af4215b643015635f54badca964b8632a6aafcf1ce57f074ea"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"i17KMoyEiDT6P6/t2BZWyjZ79Tw+Xnrs4WX4QFpDYlZYnE9wbyF31DT1T8qHrlOX+oYWcfC20uEtAg9D3FadDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T12:19:33.713185Z","bundle_sha256":"9e872691e008edd74d4bb8865ce70c4327096254f82e210ad26b0fbecb25a87b"}}