{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:WDGIL3PXEUB3YQH7ZM3MGDZARU","short_pith_number":"pith:WDGIL3PX","canonical_record":{"source":{"id":"1705.10996","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-05-31T09:05:12Z","cross_cats_sorted":[],"title_canon_sha256":"677f196fa2fb2b6a223f83cdf1506d0d2b29150cb726a1237227e1a861551aaf","abstract_canon_sha256":"92fff364964eff2d782e892d453a3e0ef47dc0d73d8d95a19575c22b514a8133"},"schema_version":"1.0"},"canonical_sha256":"b0cc85edf72503bc40ffcb36c30f208d0a32dd7fa02f65d3f822304894c4b657","source":{"kind":"arxiv","id":"1705.10996","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.10996","created_at":"2026-05-18T00:40:57Z"},{"alias_kind":"arxiv_version","alias_value":"1705.10996v1","created_at":"2026-05-18T00:40:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.10996","created_at":"2026-05-18T00:40:57Z"},{"alias_kind":"pith_short_12","alias_value":"WDGIL3PXEUB3","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_16","alias_value":"WDGIL3PXEUB3YQH7","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_8","alias_value":"WDGIL3PX","created_at":"2026-05-18T12:31:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:WDGIL3PXEUB3YQH7ZM3MGDZARU","target":"record","payload":{"canonical_record":{"source":{"id":"1705.10996","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-05-31T09:05:12Z","cross_cats_sorted":[],"title_canon_sha256":"677f196fa2fb2b6a223f83cdf1506d0d2b29150cb726a1237227e1a861551aaf","abstract_canon_sha256":"92fff364964eff2d782e892d453a3e0ef47dc0d73d8d95a19575c22b514a8133"},"schema_version":"1.0"},"canonical_sha256":"b0cc85edf72503bc40ffcb36c30f208d0a32dd7fa02f65d3f822304894c4b657","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:40:57.493815Z","signature_b64":"C5xZArWsAaT7WuLDtyPqp6TF3ByBn843Htnisp7JSltsQljiuyIKVeSzANUhhJkA0nuMnub5tupQbeRDK/DkBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b0cc85edf72503bc40ffcb36c30f208d0a32dd7fa02f65d3f822304894c4b657","last_reissued_at":"2026-05-18T00:40:57.493369Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:40:57.493369Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1705.10996","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":"2026-05-18T00:40:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jb9yINAPirRJhd5SVHosyJQSpaoGidC9gBqunsV3p6Majr/4Nei2M4jpJ9DZNGqTRAhkE4jkUixhSO9OwKUTBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T11:42:03.661256Z"},"content_sha256":"ab716411529d7b46c53209da60dc0dbdf0caca483f2009fbd2d90974707fffcd","schema_version":"1.0","event_id":"sha256:ab716411529d7b46c53209da60dc0dbdf0caca483f2009fbd2d90974707fffcd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:WDGIL3PXEUB3YQH7ZM3MGDZARU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Structural interactions in ionic liquids linked to higher order Poisson-Boltzmann equations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"A. C. Maggs, R. Blossey, R. Podgornik","submitted_at":"2017-05-31T09:05:12Z","abstract_excerpt":"We present a derivation of generalized Poisson-Boltzmann equations starting {from} classical theories of binary fluid mixtures, employing an approach based on the Legendre transform as recently applied to the case of local descriptions of the fluid free energy. Under specific symmetry assumptions, and in the linearized regime, the Poisson-Boltzmann equation reduces to a phenomenological equation introduced by (Bazant et al., 2011), whereby the structuring near the surface is determined by bulk coefficients."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.10996","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":"2026-05-18T00:40:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vw9i7rxp3lrpSkGclnR3MNlxKbObCUd3YKhtmUHHahGmALIY+Mb9B6PPo0tjkD/Yvns7Jeq17kGe038Ro8YcAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T11:42:03.661617Z"},"content_sha256":"0d18193158a8269a230b1b8d692fb2e90e12fdbd548f2d964223e81c653326d2","schema_version":"1.0","event_id":"sha256:0d18193158a8269a230b1b8d692fb2e90e12fdbd548f2d964223e81c653326d2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WDGIL3PXEUB3YQH7ZM3MGDZARU/bundle.json","state_url":"https://pith.science/pith/WDGIL3PXEUB3YQH7ZM3MGDZARU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WDGIL3PXEUB3YQH7ZM3MGDZARU/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":"2026-06-05T11:42:03Z","links":{"resolver":"https://pith.science/pith/WDGIL3PXEUB3YQH7ZM3MGDZARU","bundle":"https://pith.science/pith/WDGIL3PXEUB3YQH7ZM3MGDZARU/bundle.json","state":"https://pith.science/pith/WDGIL3PXEUB3YQH7ZM3MGDZARU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WDGIL3PXEUB3YQH7ZM3MGDZARU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:WDGIL3PXEUB3YQH7ZM3MGDZARU","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":"92fff364964eff2d782e892d453a3e0ef47dc0d73d8d95a19575c22b514a8133","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-05-31T09:05:12Z","title_canon_sha256":"677f196fa2fb2b6a223f83cdf1506d0d2b29150cb726a1237227e1a861551aaf"},"schema_version":"1.0","source":{"id":"1705.10996","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.10996","created_at":"2026-05-18T00:40:57Z"},{"alias_kind":"arxiv_version","alias_value":"1705.10996v1","created_at":"2026-05-18T00:40:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.10996","created_at":"2026-05-18T00:40:57Z"},{"alias_kind":"pith_short_12","alias_value":"WDGIL3PXEUB3","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_16","alias_value":"WDGIL3PXEUB3YQH7","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_8","alias_value":"WDGIL3PX","created_at":"2026-05-18T12:31:53Z"}],"graph_snapshots":[{"event_id":"sha256:0d18193158a8269a230b1b8d692fb2e90e12fdbd548f2d964223e81c653326d2","target":"graph","created_at":"2026-05-18T00:40:57Z","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":"We present a derivation of generalized Poisson-Boltzmann equations starting {from} classical theories of binary fluid mixtures, employing an approach based on the Legendre transform as recently applied to the case of local descriptions of the fluid free energy. Under specific symmetry assumptions, and in the linearized regime, the Poisson-Boltzmann equation reduces to a phenomenological equation introduced by (Bazant et al., 2011), whereby the structuring near the surface is determined by bulk coefficients.","authors_text":"A. C. Maggs, R. Blossey, R. Podgornik","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-05-31T09:05:12Z","title":"Structural interactions in ionic liquids linked to higher order Poisson-Boltzmann equations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.10996","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:ab716411529d7b46c53209da60dc0dbdf0caca483f2009fbd2d90974707fffcd","target":"record","created_at":"2026-05-18T00:40:57Z","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":"92fff364964eff2d782e892d453a3e0ef47dc0d73d8d95a19575c22b514a8133","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-05-31T09:05:12Z","title_canon_sha256":"677f196fa2fb2b6a223f83cdf1506d0d2b29150cb726a1237227e1a861551aaf"},"schema_version":"1.0","source":{"id":"1705.10996","kind":"arxiv","version":1}},"canonical_sha256":"b0cc85edf72503bc40ffcb36c30f208d0a32dd7fa02f65d3f822304894c4b657","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b0cc85edf72503bc40ffcb36c30f208d0a32dd7fa02f65d3f822304894c4b657","first_computed_at":"2026-05-18T00:40:57.493369Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:40:57.493369Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"C5xZArWsAaT7WuLDtyPqp6TF3ByBn843Htnisp7JSltsQljiuyIKVeSzANUhhJkA0nuMnub5tupQbeRDK/DkBg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:40:57.493815Z","signed_message":"canonical_sha256_bytes"},"source_id":"1705.10996","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ab716411529d7b46c53209da60dc0dbdf0caca483f2009fbd2d90974707fffcd","sha256:0d18193158a8269a230b1b8d692fb2e90e12fdbd548f2d964223e81c653326d2"],"state_sha256":"6739657d9de62129c9b177a1e024e080ba6a79f92962cd90331b84735b067192"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GRcHo3P+J4o7gF+cV8RtuotS2id7GYavgJYxzBPBv1JKuJf+OYIfQmztRvMjbxfKbSXBVjrJxh/QJsYNepqtBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T11:42:03.663621Z","bundle_sha256":"ef4bb96759991cb4900039774c6d5ba469790801ca05f82c6381d2fa837e42ca"}}