{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:BWPWBDDZ4BKHNNO3GGKJZQMY4C","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":"1c68f0518ec16186d5334e29cdaff8b3ad8dca10c15f1baabd784d097cd0b3f7","cross_cats_sorted":["cond-mat.stat-mech","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-03-04T08:32:28Z","title_canon_sha256":"28da5ff8c87e96c954816e7fb4ce4ab161c899459adb0bde1e69997552e1903b"},"schema_version":"1.0","source":{"id":"1503.01252","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1503.01252","created_at":"2026-05-18T02:17:11Z"},{"alias_kind":"arxiv_version","alias_value":"1503.01252v2","created_at":"2026-05-18T02:17:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.01252","created_at":"2026-05-18T02:17:11Z"},{"alias_kind":"pith_short_12","alias_value":"BWPWBDDZ4BKH","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_16","alias_value":"BWPWBDDZ4BKHNNO3","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_8","alias_value":"BWPWBDDZ","created_at":"2026-05-18T12:29:14Z"}],"graph_snapshots":[{"event_id":"sha256:08b40b8e29deaff6ec5b1862135f2f1f67c0cfd803a630c04ea0f985937b8ee8","target":"graph","created_at":"2026-05-18T02:17:11Z","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 electrostatic interaction in ionic fluids is well-known to give rise to a characteristic phase behavior and structure. Sometimes its long range is proposed to single out the electrostatic potential over other interactions with shorter ranges. Here the importance of the range for the phase behavior and the structure of ionic fluids is investigated by means of grandcanonical Monte Carlo simulations of the lattice restricted primitive model (LRPM). The long-ranged electrostatic interaction is compared to various types of short-ranged potentials obtained by sharp and/or smooth cut-off schemes.","authors_text":"Hendrik Bartsch, Markus Bier, Oliver Dannenmann","cross_cats":["cond-mat.stat-mech","physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-03-04T08:32:28Z","title":"Thermal and structural properties of ionic fluids"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.01252","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:c11a63fe561153924465cc2074a30d4707e831a5063fcd1e57deadbdd70eb4cb","target":"record","created_at":"2026-05-18T02:17:11Z","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":"1c68f0518ec16186d5334e29cdaff8b3ad8dca10c15f1baabd784d097cd0b3f7","cross_cats_sorted":["cond-mat.stat-mech","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-03-04T08:32:28Z","title_canon_sha256":"28da5ff8c87e96c954816e7fb4ce4ab161c899459adb0bde1e69997552e1903b"},"schema_version":"1.0","source":{"id":"1503.01252","kind":"arxiv","version":2}},"canonical_sha256":"0d9f608c79e05476b5db31949cc198e0b3089afa7894ba4a9b07d781b3f82fee","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0d9f608c79e05476b5db31949cc198e0b3089afa7894ba4a9b07d781b3f82fee","first_computed_at":"2026-05-18T02:17:11.095895Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:17:11.095895Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/x0ovgCdc+WwwKIRjtJY1bj1foBKX9yB4++rOQUjZek9eEz1GWELJvjkAzdFWnxlo1VT2krWPdc96nLCaC4/Dg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:17:11.096620Z","signed_message":"canonical_sha256_bytes"},"source_id":"1503.01252","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c11a63fe561153924465cc2074a30d4707e831a5063fcd1e57deadbdd70eb4cb","sha256:08b40b8e29deaff6ec5b1862135f2f1f67c0cfd803a630c04ea0f985937b8ee8"],"state_sha256":"789f3d0477218af8e3395833828459d90009e61291f8bb6f805a064c441b58ad"}