{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:RPCD62ZFEPCLC6B34UYBKGKZ5W","short_pith_number":"pith:RPCD62ZF","canonical_record":{"source":{"id":"1803.06421","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-03-16T22:49:21Z","cross_cats_sorted":[],"title_canon_sha256":"0e88f0d7670edc6c4b6a6baaa56727b3ac2e31df005d23043308f89f0382bac9","abstract_canon_sha256":"42840cdad581530a7a3977055e3f30a2f05dd5eee93d894e209cb996f546ac59"},"schema_version":"1.0"},"canonical_sha256":"8bc43f6b2523c4b1783be530151959eda9dab8a0b2cf8071417977cbb519a09f","source":{"kind":"arxiv","id":"1803.06421","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1803.06421","created_at":"2026-05-17T23:40:14Z"},{"alias_kind":"arxiv_version","alias_value":"1803.06421v1","created_at":"2026-05-17T23:40:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.06421","created_at":"2026-05-17T23:40:14Z"},{"alias_kind":"pith_short_12","alias_value":"RPCD62ZFEPCL","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_16","alias_value":"RPCD62ZFEPCLC6B3","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_8","alias_value":"RPCD62ZF","created_at":"2026-05-18T12:32:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:RPCD62ZFEPCLC6B34UYBKGKZ5W","target":"record","payload":{"canonical_record":{"source":{"id":"1803.06421","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-03-16T22:49:21Z","cross_cats_sorted":[],"title_canon_sha256":"0e88f0d7670edc6c4b6a6baaa56727b3ac2e31df005d23043308f89f0382bac9","abstract_canon_sha256":"42840cdad581530a7a3977055e3f30a2f05dd5eee93d894e209cb996f546ac59"},"schema_version":"1.0"},"canonical_sha256":"8bc43f6b2523c4b1783be530151959eda9dab8a0b2cf8071417977cbb519a09f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:40:14.248351Z","signature_b64":"garpgrlu8DM/cUJ1ymODp3mScyHuts8JEQx7mT6RSlvzcuJSwXfgj+q3JfzdTt6Gmi6yURE8FyjU1qQt8dOqDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8bc43f6b2523c4b1783be530151959eda9dab8a0b2cf8071417977cbb519a09f","last_reissued_at":"2026-05-17T23:40:14.247453Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:40:14.247453Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1803.06421","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":"2026-05-17T23:40:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iXOVFNeOyQX+0cDU8u4vHdVIUXPbA1AHQXAJc6P0t+DCF5nEfxJlHcM6cVwEAwDyChZ9T+EmmnYKzS+DMCK+CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T21:29:10.830053Z"},"content_sha256":"048a0bf95b295616e4cb2ecdb2bff01f478b233512106183818a4a27f7209182","schema_version":"1.0","event_id":"sha256:048a0bf95b295616e4cb2ecdb2bff01f478b233512106183818a4a27f7209182"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:RPCD62ZFEPCLC6B34UYBKGKZ5W","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Uncertainties in permittivities computed from molecular dynamics simulations and temperature correction of dielectric properties of condensed polar systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.chem-ph","authors_text":"C. Manuel Carlevaro, Hern\\'an R. S\\'anchez, Ramiro M. Irastorza","submitted_at":"2018-03-16T22:49:21Z","abstract_excerpt":"A robust, simple and fast procedure for the calculation of uncertainties in relative static dielectric permittivity ($\\varepsilon_s$) computed via molecular dynamics (MD) is proposed. It arises as a direct application of well founded statistical methods for auto-correlated variables. Also, in order to deal with the lack of experimental data about $\\varepsilon_s$ and relaxation times ($\\tau$) at different temperatures, a method for their prediction is suggested. It requires one experimental value and at least two MD simulations. In the case of relaxation times, a theoretical justification is pr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.06421","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":"2026-05-17T23:40:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lEq8Ah7fSIvbe+hMKAEPA67kN9s2jIPNWn4TGyu7iQIUQuyybp6sWmlEllfIjwjoq3UW6r1L2phqxImJ7j4FDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T21:29:10.830448Z"},"content_sha256":"eea97db665cb58c4cd5c41fd1ff00ef14ee54be0fd520bd883d428249a2af2bb","schema_version":"1.0","event_id":"sha256:eea97db665cb58c4cd5c41fd1ff00ef14ee54be0fd520bd883d428249a2af2bb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RPCD62ZFEPCLC6B34UYBKGKZ5W/bundle.json","state_url":"https://pith.science/pith/RPCD62ZFEPCLC6B34UYBKGKZ5W/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RPCD62ZFEPCLC6B34UYBKGKZ5W/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":"2026-06-06T21:29:10Z","links":{"resolver":"https://pith.science/pith/RPCD62ZFEPCLC6B34UYBKGKZ5W","bundle":"https://pith.science/pith/RPCD62ZFEPCLC6B34UYBKGKZ5W/bundle.json","state":"https://pith.science/pith/RPCD62ZFEPCLC6B34UYBKGKZ5W/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RPCD62ZFEPCLC6B34UYBKGKZ5W/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:RPCD62ZFEPCLC6B34UYBKGKZ5W","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":"42840cdad581530a7a3977055e3f30a2f05dd5eee93d894e209cb996f546ac59","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-03-16T22:49:21Z","title_canon_sha256":"0e88f0d7670edc6c4b6a6baaa56727b3ac2e31df005d23043308f89f0382bac9"},"schema_version":"1.0","source":{"id":"1803.06421","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1803.06421","created_at":"2026-05-17T23:40:14Z"},{"alias_kind":"arxiv_version","alias_value":"1803.06421v1","created_at":"2026-05-17T23:40:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.06421","created_at":"2026-05-17T23:40:14Z"},{"alias_kind":"pith_short_12","alias_value":"RPCD62ZFEPCL","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_16","alias_value":"RPCD62ZFEPCLC6B3","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_8","alias_value":"RPCD62ZF","created_at":"2026-05-18T12:32:50Z"}],"graph_snapshots":[{"event_id":"sha256:eea97db665cb58c4cd5c41fd1ff00ef14ee54be0fd520bd883d428249a2af2bb","target":"graph","created_at":"2026-05-17T23:40:14Z","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":"A robust, simple and fast procedure for the calculation of uncertainties in relative static dielectric permittivity ($\\varepsilon_s$) computed via molecular dynamics (MD) is proposed. It arises as a direct application of well founded statistical methods for auto-correlated variables. Also, in order to deal with the lack of experimental data about $\\varepsilon_s$ and relaxation times ($\\tau$) at different temperatures, a method for their prediction is suggested. It requires one experimental value and at least two MD simulations. In the case of relaxation times, a theoretical justification is pr","authors_text":"C. Manuel Carlevaro, Hern\\'an R. S\\'anchez, Ramiro M. Irastorza","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-03-16T22:49:21Z","title":"Uncertainties in permittivities computed from molecular dynamics simulations and temperature correction of dielectric properties of condensed polar systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.06421","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":"sha256:048a0bf95b295616e4cb2ecdb2bff01f478b233512106183818a4a27f7209182","target":"record","created_at":"2026-05-17T23:40:14Z","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":"42840cdad581530a7a3977055e3f30a2f05dd5eee93d894e209cb996f546ac59","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-03-16T22:49:21Z","title_canon_sha256":"0e88f0d7670edc6c4b6a6baaa56727b3ac2e31df005d23043308f89f0382bac9"},"schema_version":"1.0","source":{"id":"1803.06421","kind":"arxiv","version":1}},"canonical_sha256":"8bc43f6b2523c4b1783be530151959eda9dab8a0b2cf8071417977cbb519a09f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8bc43f6b2523c4b1783be530151959eda9dab8a0b2cf8071417977cbb519a09f","first_computed_at":"2026-05-17T23:40:14.247453Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:40:14.247453Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"garpgrlu8DM/cUJ1ymODp3mScyHuts8JEQx7mT6RSlvzcuJSwXfgj+q3JfzdTt6Gmi6yURE8FyjU1qQt8dOqDw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:40:14.248351Z","signed_message":"canonical_sha256_bytes"},"source_id":"1803.06421","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:048a0bf95b295616e4cb2ecdb2bff01f478b233512106183818a4a27f7209182","sha256:eea97db665cb58c4cd5c41fd1ff00ef14ee54be0fd520bd883d428249a2af2bb"],"state_sha256":"c8b8a20847597e32246b26aa2a0d809e005341b5482a5278836d08ce71236a0e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Gs6HDZlQzFkmZGZ6fjz4ye0N9HKGwrlPZjKSpdMHYfhpdZUMhWV7hzuehKhaBqYjoD4AOQkv3GmH7N1wyRpfAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T21:29:10.833704Z","bundle_sha256":"5a21a626b2fb3911b0955494825ee8e533c335b4ea89ffb28efeb41db3c095bf"}}