{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:XZE5QFF7SZOV7HXPZNJXIOLVBY","short_pith_number":"pith:XZE5QFF7","canonical_record":{"source":{"id":"1708.01299","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2017-08-03T20:28:29Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"354e90635ca16a85d077cc7de9ec91d037eee9a2f30341e9a66ec425562e3333","abstract_canon_sha256":"b7a36ae1fdbbc3ddb47c994ec51f64a2d677c7aa93f17471fee263137a4eb279"},"schema_version":"1.0"},"canonical_sha256":"be49d814bf965d5f9eefcb537439750e11545b50422519168eb5108495dc0de4","source":{"kind":"arxiv","id":"1708.01299","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.01299","created_at":"2026-05-18T00:33:48Z"},{"alias_kind":"arxiv_version","alias_value":"1708.01299v2","created_at":"2026-05-18T00:33:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.01299","created_at":"2026-05-18T00:33:48Z"},{"alias_kind":"pith_short_12","alias_value":"XZE5QFF7SZOV","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_16","alias_value":"XZE5QFF7SZOV7HXP","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_8","alias_value":"XZE5QFF7","created_at":"2026-05-18T12:31:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:XZE5QFF7SZOV7HXPZNJXIOLVBY","target":"record","payload":{"canonical_record":{"source":{"id":"1708.01299","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2017-08-03T20:28:29Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"354e90635ca16a85d077cc7de9ec91d037eee9a2f30341e9a66ec425562e3333","abstract_canon_sha256":"b7a36ae1fdbbc3ddb47c994ec51f64a2d677c7aa93f17471fee263137a4eb279"},"schema_version":"1.0"},"canonical_sha256":"be49d814bf965d5f9eefcb537439750e11545b50422519168eb5108495dc0de4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:48.898141Z","signature_b64":"ZxA7aLd1nB6UWxn2BLCIhS4ht0xVWQhdIUeGT46LXVrf5gAXh8CD4pGFMkwdI6ekfLRcdKCUv8cZdM3bt83dBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"be49d814bf965d5f9eefcb537439750e11545b50422519168eb5108495dc0de4","last_reissued_at":"2026-05-18T00:33:48.897596Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:48.897596Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1708.01299","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":"2026-05-18T00:33:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SsFSuWLRED7cTpdn6CGqPIsfbk7EFSjb4sQ8JwR9XbdhwcQ7w5oIYg7z0xPqqSoxKQsJGerAuLgwDJnRdmuhCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T13:12:53.695561Z"},"content_sha256":"15d3b666a038c52ae7f7f9854efb72cd2038e4e8392c2112cf25004bd340e949","schema_version":"1.0","event_id":"sha256:15d3b666a038c52ae7f7f9854efb72cd2038e4e8392c2112cf25004bd340e949"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:XZE5QFF7SZOV7HXPZNJXIOLVBY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Solvation in atomic liquids: connection between Gaussian field theory and density functional theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"physics.chem-ph","authors_text":"B. Rotenberg, D. Borgis, M. Levesque, V. Sergiievskyi","submitted_at":"2017-08-03T20:28:29Z","abstract_excerpt":"For the problem of molecular solvation, formulated as a liquid submitted to the external potential field created by a molecular solute of arbitrary shape dissolved in that solvent, we draw a connection between the Gaussian field theory derived by David Chandler [Phys. Rev. E, 1993, 48, 2898] and classical density functional theory. We show that Chandler's results concerning the solvation of a hard core of arbitrary shape can be recovered by either minimising a linearised HNC functional using an auxiliary Lagrange multiplier field to impose a vanishing density inside the core, or by minimising "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.01299","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":"2026-05-18T00:33:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LWzDzSyyMxqo0pCAuw8uw/P3Pq1lFjFSxHsmbAh41LTHmkHA+MXeDxIwC7ix1rR6Ul2sesahYkXaLkgH81saBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T13:12:53.695910Z"},"content_sha256":"a88a872ff9541a917aa466049543e348e81dac5220b1b57bb0773c1f9fc2fc9c","schema_version":"1.0","event_id":"sha256:a88a872ff9541a917aa466049543e348e81dac5220b1b57bb0773c1f9fc2fc9c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XZE5QFF7SZOV7HXPZNJXIOLVBY/bundle.json","state_url":"https://pith.science/pith/XZE5QFF7SZOV7HXPZNJXIOLVBY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XZE5QFF7SZOV7HXPZNJXIOLVBY/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":"2026-05-28T13:12:53Z","links":{"resolver":"https://pith.science/pith/XZE5QFF7SZOV7HXPZNJXIOLVBY","bundle":"https://pith.science/pith/XZE5QFF7SZOV7HXPZNJXIOLVBY/bundle.json","state":"https://pith.science/pith/XZE5QFF7SZOV7HXPZNJXIOLVBY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XZE5QFF7SZOV7HXPZNJXIOLVBY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:XZE5QFF7SZOV7HXPZNJXIOLVBY","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":"b7a36ae1fdbbc3ddb47c994ec51f64a2d677c7aa93f17471fee263137a4eb279","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2017-08-03T20:28:29Z","title_canon_sha256":"354e90635ca16a85d077cc7de9ec91d037eee9a2f30341e9a66ec425562e3333"},"schema_version":"1.0","source":{"id":"1708.01299","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.01299","created_at":"2026-05-18T00:33:48Z"},{"alias_kind":"arxiv_version","alias_value":"1708.01299v2","created_at":"2026-05-18T00:33:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.01299","created_at":"2026-05-18T00:33:48Z"},{"alias_kind":"pith_short_12","alias_value":"XZE5QFF7SZOV","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_16","alias_value":"XZE5QFF7SZOV7HXP","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_8","alias_value":"XZE5QFF7","created_at":"2026-05-18T12:31:56Z"}],"graph_snapshots":[{"event_id":"sha256:a88a872ff9541a917aa466049543e348e81dac5220b1b57bb0773c1f9fc2fc9c","target":"graph","created_at":"2026-05-18T00:33:48Z","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":"For the problem of molecular solvation, formulated as a liquid submitted to the external potential field created by a molecular solute of arbitrary shape dissolved in that solvent, we draw a connection between the Gaussian field theory derived by David Chandler [Phys. Rev. E, 1993, 48, 2898] and classical density functional theory. We show that Chandler's results concerning the solvation of a hard core of arbitrary shape can be recovered by either minimising a linearised HNC functional using an auxiliary Lagrange multiplier field to impose a vanishing density inside the core, or by minimising ","authors_text":"B. Rotenberg, D. Borgis, M. Levesque, V. Sergiievskyi","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2017-08-03T20:28:29Z","title":"Solvation in atomic liquids: connection between Gaussian field theory and density functional theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.01299","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":"sha256:15d3b666a038c52ae7f7f9854efb72cd2038e4e8392c2112cf25004bd340e949","target":"record","created_at":"2026-05-18T00:33:48Z","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":"b7a36ae1fdbbc3ddb47c994ec51f64a2d677c7aa93f17471fee263137a4eb279","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2017-08-03T20:28:29Z","title_canon_sha256":"354e90635ca16a85d077cc7de9ec91d037eee9a2f30341e9a66ec425562e3333"},"schema_version":"1.0","source":{"id":"1708.01299","kind":"arxiv","version":2}},"canonical_sha256":"be49d814bf965d5f9eefcb537439750e11545b50422519168eb5108495dc0de4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"be49d814bf965d5f9eefcb537439750e11545b50422519168eb5108495dc0de4","first_computed_at":"2026-05-18T00:33:48.897596Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:33:48.897596Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZxA7aLd1nB6UWxn2BLCIhS4ht0xVWQhdIUeGT46LXVrf5gAXh8CD4pGFMkwdI6ekfLRcdKCUv8cZdM3bt83dBA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:33:48.898141Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.01299","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:15d3b666a038c52ae7f7f9854efb72cd2038e4e8392c2112cf25004bd340e949","sha256:a88a872ff9541a917aa466049543e348e81dac5220b1b57bb0773c1f9fc2fc9c"],"state_sha256":"aa991fc7ba901f30e32cbdfa457daa1aaab0d4d66497a628178fe32c3aa9abac"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lqSJtFqevXi5MFCzeROfp4Eds8AzLYcscU4c0itbpFSxHx9hIo8/kSYvO5l5STfiArV6py8c/AsM/VLKT7FKAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T13:12:53.698046Z","bundle_sha256":"bfd3f5c01f98a5a2ed636bf4995a5acf8066f5e487d5802faee221c7097966c1"}}