{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:J3KOIYPOESB4Y5ST3MRG42KFPG","short_pith_number":"pith:J3KOIYPO","canonical_record":{"source":{"id":"1707.05403","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-07-17T22:09:05Z","cross_cats_sorted":["physics.chem-ph","physics.comp-ph"],"title_canon_sha256":"182bdbfa864ecea2ae5dcf7b16329f215105aa3c75016150a65ae89fa934feee","abstract_canon_sha256":"237a3f800581a2480318ca4a8d110b61b00b8c0b0ed02facb8c65b36ac8702f6"},"schema_version":"1.0"},"canonical_sha256":"4ed4e461ee2483cc7653db226e694579aa4f22e58eca62c4edc60b5674423625","source":{"kind":"arxiv","id":"1707.05403","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.05403","created_at":"2026-05-18T00:39:17Z"},{"alias_kind":"arxiv_version","alias_value":"1707.05403v1","created_at":"2026-05-18T00:39:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.05403","created_at":"2026-05-18T00:39:17Z"},{"alias_kind":"pith_short_12","alias_value":"J3KOIYPOESB4","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"J3KOIYPOESB4Y5ST","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"J3KOIYPO","created_at":"2026-05-18T12:31:21Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:J3KOIYPOESB4Y5ST3MRG42KFPG","target":"record","payload":{"canonical_record":{"source":{"id":"1707.05403","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-07-17T22:09:05Z","cross_cats_sorted":["physics.chem-ph","physics.comp-ph"],"title_canon_sha256":"182bdbfa864ecea2ae5dcf7b16329f215105aa3c75016150a65ae89fa934feee","abstract_canon_sha256":"237a3f800581a2480318ca4a8d110b61b00b8c0b0ed02facb8c65b36ac8702f6"},"schema_version":"1.0"},"canonical_sha256":"4ed4e461ee2483cc7653db226e694579aa4f22e58eca62c4edc60b5674423625","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:39:17.599679Z","signature_b64":"O0FOYi/JrW/LSk4/OPkpAQN4b8otWIT95tLniU1vBKOGgjuIehoFFgXGnmtSL0j0RJ2fr8Gfd2VORZ07xS5rDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4ed4e461ee2483cc7653db226e694579aa4f22e58eca62c4edc60b5674423625","last_reissued_at":"2026-05-18T00:39:17.599084Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:39:17.599084Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1707.05403","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":"2026-05-18T00:39:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xLUyTzYYcrR0JeolJq1dcRV9DRbjeH5b5zflkc4XiIOAcbu0SN6YW7oL2Yp5vUOxlp+zunRn7sBbJx8+o2AHCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T00:39:13.974537Z"},"content_sha256":"f2ea85fafbffe9c69ff1be380b2b82f7e8fc61a2e856f9cb88c1483f17b23129","schema_version":"1.0","event_id":"sha256:f2ea85fafbffe9c69ff1be380b2b82f7e8fc61a2e856f9cb88c1483f17b23129"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:J3KOIYPOESB4Y5ST3MRG42KFPG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A comparison of classical interatomic potentials applied to highly concentrated aqueous lithium chloride solutions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.chem-ph","physics.comp-ph"],"primary_cat":"cond-mat.soft","authors_text":"Ildik\\'o Pethes","submitted_at":"2017-07-17T22:09:05Z","abstract_excerpt":"Aqueous lithium chloride solutions up to very high concentrations were investigated in classical molecular dynamics simulations. Various force fields based on the 12-6 Lennard-Jones model, parametrized for non-polarizable water solvent molecules (SPC/E, TIP4P, TIP4PEw), were inspected. Twenty-nine combinations of ion-water interaction models were examined at four different salt concentrations. Densities, static dielectric constants and self-diffusion coefficients were calculated. Results derived from the different force fields scatter over a wide range of values. Neutron and X-ray weighted str"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.05403","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":"2026-05-18T00:39:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"J/dEoPtT7pAiskyvkCM30tIKKZVjkavlL0yTYebNmvVFZJygcCvTZOxfg/vx+pd7OZXceExiYvIA1eUzUO7bAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T00:39:13.975282Z"},"content_sha256":"792fc2969c3fe6f67dea51277947302764bd9f2e7885bf9fa5b3a9e74221b737","schema_version":"1.0","event_id":"sha256:792fc2969c3fe6f67dea51277947302764bd9f2e7885bf9fa5b3a9e74221b737"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/J3KOIYPOESB4Y5ST3MRG42KFPG/bundle.json","state_url":"https://pith.science/pith/J3KOIYPOESB4Y5ST3MRG42KFPG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/J3KOIYPOESB4Y5ST3MRG42KFPG/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":"2026-06-01T00:39:13Z","links":{"resolver":"https://pith.science/pith/J3KOIYPOESB4Y5ST3MRG42KFPG","bundle":"https://pith.science/pith/J3KOIYPOESB4Y5ST3MRG42KFPG/bundle.json","state":"https://pith.science/pith/J3KOIYPOESB4Y5ST3MRG42KFPG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/J3KOIYPOESB4Y5ST3MRG42KFPG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:J3KOIYPOESB4Y5ST3MRG42KFPG","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":"237a3f800581a2480318ca4a8d110b61b00b8c0b0ed02facb8c65b36ac8702f6","cross_cats_sorted":["physics.chem-ph","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-07-17T22:09:05Z","title_canon_sha256":"182bdbfa864ecea2ae5dcf7b16329f215105aa3c75016150a65ae89fa934feee"},"schema_version":"1.0","source":{"id":"1707.05403","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.05403","created_at":"2026-05-18T00:39:17Z"},{"alias_kind":"arxiv_version","alias_value":"1707.05403v1","created_at":"2026-05-18T00:39:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.05403","created_at":"2026-05-18T00:39:17Z"},{"alias_kind":"pith_short_12","alias_value":"J3KOIYPOESB4","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"J3KOIYPOESB4Y5ST","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"J3KOIYPO","created_at":"2026-05-18T12:31:21Z"}],"graph_snapshots":[{"event_id":"sha256:792fc2969c3fe6f67dea51277947302764bd9f2e7885bf9fa5b3a9e74221b737","target":"graph","created_at":"2026-05-18T00:39:17Z","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":"Aqueous lithium chloride solutions up to very high concentrations were investigated in classical molecular dynamics simulations. Various force fields based on the 12-6 Lennard-Jones model, parametrized for non-polarizable water solvent molecules (SPC/E, TIP4P, TIP4PEw), were inspected. Twenty-nine combinations of ion-water interaction models were examined at four different salt concentrations. Densities, static dielectric constants and self-diffusion coefficients were calculated. Results derived from the different force fields scatter over a wide range of values. Neutron and X-ray weighted str","authors_text":"Ildik\\'o Pethes","cross_cats":["physics.chem-ph","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-07-17T22:09:05Z","title":"A comparison of classical interatomic potentials applied to highly concentrated aqueous lithium chloride solutions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.05403","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:f2ea85fafbffe9c69ff1be380b2b82f7e8fc61a2e856f9cb88c1483f17b23129","target":"record","created_at":"2026-05-18T00:39:17Z","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":"237a3f800581a2480318ca4a8d110b61b00b8c0b0ed02facb8c65b36ac8702f6","cross_cats_sorted":["physics.chem-ph","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-07-17T22:09:05Z","title_canon_sha256":"182bdbfa864ecea2ae5dcf7b16329f215105aa3c75016150a65ae89fa934feee"},"schema_version":"1.0","source":{"id":"1707.05403","kind":"arxiv","version":1}},"canonical_sha256":"4ed4e461ee2483cc7653db226e694579aa4f22e58eca62c4edc60b5674423625","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4ed4e461ee2483cc7653db226e694579aa4f22e58eca62c4edc60b5674423625","first_computed_at":"2026-05-18T00:39:17.599084Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:39:17.599084Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"O0FOYi/JrW/LSk4/OPkpAQN4b8otWIT95tLniU1vBKOGgjuIehoFFgXGnmtSL0j0RJ2fr8Gfd2VORZ07xS5rDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:39:17.599679Z","signed_message":"canonical_sha256_bytes"},"source_id":"1707.05403","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f2ea85fafbffe9c69ff1be380b2b82f7e8fc61a2e856f9cb88c1483f17b23129","sha256:792fc2969c3fe6f67dea51277947302764bd9f2e7885bf9fa5b3a9e74221b737"],"state_sha256":"0fcaab63a5d30a12b44253e0891d0f459b9d2ae7b6b33daec77fcca8d46904e2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"u85ZE5/F8k2rbUR69OINo8lUGp3YKoJBCtbmBjGhWyyitGUY4xqEtBkFdDzXexEJZwBpzCDoJHvKTOMJAZOzCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T00:39:13.979495Z","bundle_sha256":"cd97bc88da4bfb69bc6e17e8554c3e0b102a6f2870ef187467432d2075f1a98b"}}