{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:EOE4DU3OB4UUA5IAH3DRUHM6LT","short_pith_number":"pith:EOE4DU3O","canonical_record":{"source":{"id":"1201.6081","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2012-01-29T20:57:28Z","cross_cats_sorted":["cond-mat.stat-mech","physics.bio-ph","physics.chem-ph"],"title_canon_sha256":"e8b45ae9ec04cef0375a76081799a5efa1c848d6b56f84d9e15f2add9e074c4f","abstract_canon_sha256":"ca6519507119773dee4d722f97050252c80f67f49db19df471a34776bf38bd22"},"schema_version":"1.0"},"canonical_sha256":"2389c1d36e0f294075003ec71a1d9e5cfab586e029ad353fa40dcaa4fc5e17bc","source":{"kind":"arxiv","id":"1201.6081","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.6081","created_at":"2026-05-18T03:51:47Z"},{"alias_kind":"arxiv_version","alias_value":"1201.6081v1","created_at":"2026-05-18T03:51:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.6081","created_at":"2026-05-18T03:51:47Z"},{"alias_kind":"pith_short_12","alias_value":"EOE4DU3OB4UU","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_16","alias_value":"EOE4DU3OB4UUA5IA","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_8","alias_value":"EOE4DU3O","created_at":"2026-05-18T12:27:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:EOE4DU3OB4UUA5IAH3DRUHM6LT","target":"record","payload":{"canonical_record":{"source":{"id":"1201.6081","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2012-01-29T20:57:28Z","cross_cats_sorted":["cond-mat.stat-mech","physics.bio-ph","physics.chem-ph"],"title_canon_sha256":"e8b45ae9ec04cef0375a76081799a5efa1c848d6b56f84d9e15f2add9e074c4f","abstract_canon_sha256":"ca6519507119773dee4d722f97050252c80f67f49db19df471a34776bf38bd22"},"schema_version":"1.0"},"canonical_sha256":"2389c1d36e0f294075003ec71a1d9e5cfab586e029ad353fa40dcaa4fc5e17bc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:51:47.142224Z","signature_b64":"R72qEkQRdi8MzlXl3K/XKjAkPQLOmhW++MYRqFNw8/gDyeYhjYyfgilv03Qxm0uTbfjbO7Gb1WQhbgQZ363IDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2389c1d36e0f294075003ec71a1d9e5cfab586e029ad353fa40dcaa4fc5e17bc","last_reissued_at":"2026-05-18T03:51:47.141648Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:51:47.141648Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1201.6081","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":"2026-05-18T03:51:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Nd7ypL/0jU6+i5bI32YFpQgYgRkIphsWiZ6Wy4cFryBrNdL91wYEUWU8CWBYW5dRl4lo0parXTaeNz+WFz3jCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T08:59:13.900283Z"},"content_sha256":"0de06f8a77dc0bd9045857f17e85ff7cdf474de35fcb938b2c2f1526a0d82980","schema_version":"1.0","event_id":"sha256:0de06f8a77dc0bd9045857f17e85ff7cdf474de35fcb938b2c2f1526a0d82980"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:EOE4DU3OB4UUA5IAH3DRUHM6LT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The Dielectric Constant of Ionic Solutions: A Field-Theory Approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","physics.bio-ph","physics.chem-ph"],"primary_cat":"cond-mat.soft","authors_text":"Amir Levy, David Andelman, Henri Orland","submitted_at":"2012-01-29T20:57:28Z","abstract_excerpt":"We study the variation of the dielectric response of a dielectric liquid (e.g. water) when a salt is added to the solution. Employing field-theoretical methods we expand the Gibbs free-energy to first order in a loop expansion and calculate self-consistently the dielectric constant. We predict analytically the dielectric decrement which depends on the ionic strength in a complex way. Furthermore, a qualitative description of the hydration shell is found and is characterized by a single length scale. Our prediction fits rather well a large range of concentrations for different salts using only "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.6081","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":"2026-05-18T03:51:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"n8W+5wYE5V/RWuj/bPED3Iq79fZuHBVfV7PmMPeDqlpt9X/DC9XI6tRr/BmjSHamS26LnUi1WEJvpsMQcsH7Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T08:59:13.900728Z"},"content_sha256":"ea33ec5cb695edb28cfa88d15caaa70767fe761e8a3fa787d4ec64d80c8d91db","schema_version":"1.0","event_id":"sha256:ea33ec5cb695edb28cfa88d15caaa70767fe761e8a3fa787d4ec64d80c8d91db"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EOE4DU3OB4UUA5IAH3DRUHM6LT/bundle.json","state_url":"https://pith.science/pith/EOE4DU3OB4UUA5IAH3DRUHM6LT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EOE4DU3OB4UUA5IAH3DRUHM6LT/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":"2026-06-11T08:59:13Z","links":{"resolver":"https://pith.science/pith/EOE4DU3OB4UUA5IAH3DRUHM6LT","bundle":"https://pith.science/pith/EOE4DU3OB4UUA5IAH3DRUHM6LT/bundle.json","state":"https://pith.science/pith/EOE4DU3OB4UUA5IAH3DRUHM6LT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EOE4DU3OB4UUA5IAH3DRUHM6LT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:EOE4DU3OB4UUA5IAH3DRUHM6LT","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":"ca6519507119773dee4d722f97050252c80f67f49db19df471a34776bf38bd22","cross_cats_sorted":["cond-mat.stat-mech","physics.bio-ph","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2012-01-29T20:57:28Z","title_canon_sha256":"e8b45ae9ec04cef0375a76081799a5efa1c848d6b56f84d9e15f2add9e074c4f"},"schema_version":"1.0","source":{"id":"1201.6081","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.6081","created_at":"2026-05-18T03:51:47Z"},{"alias_kind":"arxiv_version","alias_value":"1201.6081v1","created_at":"2026-05-18T03:51:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.6081","created_at":"2026-05-18T03:51:47Z"},{"alias_kind":"pith_short_12","alias_value":"EOE4DU3OB4UU","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_16","alias_value":"EOE4DU3OB4UUA5IA","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_8","alias_value":"EOE4DU3O","created_at":"2026-05-18T12:27:04Z"}],"graph_snapshots":[{"event_id":"sha256:ea33ec5cb695edb28cfa88d15caaa70767fe761e8a3fa787d4ec64d80c8d91db","target":"graph","created_at":"2026-05-18T03:51:47Z","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 study the variation of the dielectric response of a dielectric liquid (e.g. water) when a salt is added to the solution. Employing field-theoretical methods we expand the Gibbs free-energy to first order in a loop expansion and calculate self-consistently the dielectric constant. We predict analytically the dielectric decrement which depends on the ionic strength in a complex way. Furthermore, a qualitative description of the hydration shell is found and is characterized by a single length scale. Our prediction fits rather well a large range of concentrations for different salts using only ","authors_text":"Amir Levy, David Andelman, Henri Orland","cross_cats":["cond-mat.stat-mech","physics.bio-ph","physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2012-01-29T20:57:28Z","title":"The Dielectric Constant of Ionic Solutions: A Field-Theory Approach"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.6081","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":"sha256:0de06f8a77dc0bd9045857f17e85ff7cdf474de35fcb938b2c2f1526a0d82980","target":"record","created_at":"2026-05-18T03:51:47Z","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":"ca6519507119773dee4d722f97050252c80f67f49db19df471a34776bf38bd22","cross_cats_sorted":["cond-mat.stat-mech","physics.bio-ph","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2012-01-29T20:57:28Z","title_canon_sha256":"e8b45ae9ec04cef0375a76081799a5efa1c848d6b56f84d9e15f2add9e074c4f"},"schema_version":"1.0","source":{"id":"1201.6081","kind":"arxiv","version":1}},"canonical_sha256":"2389c1d36e0f294075003ec71a1d9e5cfab586e029ad353fa40dcaa4fc5e17bc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2389c1d36e0f294075003ec71a1d9e5cfab586e029ad353fa40dcaa4fc5e17bc","first_computed_at":"2026-05-18T03:51:47.141648Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:51:47.141648Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"R72qEkQRdi8MzlXl3K/XKjAkPQLOmhW++MYRqFNw8/gDyeYhjYyfgilv03Qxm0uTbfjbO7Gb1WQhbgQZ363IDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:51:47.142224Z","signed_message":"canonical_sha256_bytes"},"source_id":"1201.6081","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0de06f8a77dc0bd9045857f17e85ff7cdf474de35fcb938b2c2f1526a0d82980","sha256:ea33ec5cb695edb28cfa88d15caaa70767fe761e8a3fa787d4ec64d80c8d91db"],"state_sha256":"7b21d027a244cc3bf5ff791b8620e529bec98e9bd8d337cfbe1cdb5af92ef31d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4Oxms8h6nRqmnFprYvN4V+flJIJynZ/0qA+63UOfVmwAiOtnej0DYVmQL3Zv8yldMmfZBZRLHBdbuZN6sR2/CA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T08:59:13.902700Z","bundle_sha256":"b84d3f9d049cb100a2e16c011cbcb0119a1a9276960461e7099df396d9315f59"}}