{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:7IL3VIJG47QDJVT5EM67WXRTP6","short_pith_number":"pith:7IL3VIJG","canonical_record":{"source":{"id":"1602.00526","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-02-01T13:56:13Z","cross_cats_sorted":["cond-mat.other","physics.chem-ph"],"title_canon_sha256":"ad3b4aecbd8ac1d7a98b6adf859cd5c1e4cc6e296d3c874341a6b7cf564c0b0f","abstract_canon_sha256":"27d89b374c162bc31ce9d74805b36755b1b21e52bfde5f0885e95f8eeafd1cd8"},"schema_version":"1.0"},"canonical_sha256":"fa17baa126e7e034d67d233dfb5e337fa356773e14681645d14f4310a47ef730","source":{"kind":"arxiv","id":"1602.00526","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.00526","created_at":"2026-05-18T01:21:35Z"},{"alias_kind":"arxiv_version","alias_value":"1602.00526v1","created_at":"2026-05-18T01:21:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.00526","created_at":"2026-05-18T01:21:35Z"},{"alias_kind":"pith_short_12","alias_value":"7IL3VIJG47QD","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"7IL3VIJG47QDJVT5","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"7IL3VIJG","created_at":"2026-05-18T12:30:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:7IL3VIJG47QDJVT5EM67WXRTP6","target":"record","payload":{"canonical_record":{"source":{"id":"1602.00526","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-02-01T13:56:13Z","cross_cats_sorted":["cond-mat.other","physics.chem-ph"],"title_canon_sha256":"ad3b4aecbd8ac1d7a98b6adf859cd5c1e4cc6e296d3c874341a6b7cf564c0b0f","abstract_canon_sha256":"27d89b374c162bc31ce9d74805b36755b1b21e52bfde5f0885e95f8eeafd1cd8"},"schema_version":"1.0"},"canonical_sha256":"fa17baa126e7e034d67d233dfb5e337fa356773e14681645d14f4310a47ef730","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:21:35.184084Z","signature_b64":"oKExEIqkFlE5AcDueJText+tZhI1SfVAnlw5c1JSjHv9D/Ky7puSwzeWQUFfx5ORJSD/2yGturAYJoqpkA8NAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fa17baa126e7e034d67d233dfb5e337fa356773e14681645d14f4310a47ef730","last_reissued_at":"2026-05-18T01:21:35.183372Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:21:35.183372Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1602.00526","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":"2026-05-18T01:21:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"c9O+KidWhVR0UmmFvTIdmmPGXVm0RTOdsFSDJGMkycPQSj21U3C//kW9sjuzgb2hxuSn7BcjZFpKiN0EIqIJDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-02T08:13:12.477559Z"},"content_sha256":"f0e483ec9db798f7dabe80727c6014ee1ae81e0f9e023fe87a24a580ea1c7462","schema_version":"1.0","event_id":"sha256:f0e483ec9db798f7dabe80727c6014ee1ae81e0f9e023fe87a24a580ea1c7462"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:7IL3VIJG47QDJVT5EM67WXRTP6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Transition in fluctuation behaviour of normal liquids under high pressures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other","physics.chem-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Eugene B. Postnikov, Miros{\\l}aw Chor\\k{a}\\.zewski","submitted_at":"2016-02-01T13:56:13Z","abstract_excerpt":"We explore the behaviour of the inverse reduced density fluctuations and the isobaric expansion coefficient using {\\alpha},{\\omega}-dibromoalkanes as an example. Two different states are revealed far from the critical point: the region of exponentially decaying fluctuations near the coexistence curve and the state with longer correlations under sufficiently high pressures. The crossing of the isotherms of the isobaric expansion coefficient occurs within the PVT range of the mentioned transition. We discuss the interplay of this crossing with the changes in molecular packing structure connected"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.00526","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":"2026-05-18T01:21:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tBbyzKaYHFVDNIxHQOAk9Bq2kP0odEG+7zroer8b1dBbwv6DtJ1FaIgy6JJS07thEAqKhlp37xw8XwYnTsDUDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-02T08:13:12.477912Z"},"content_sha256":"7de76b237896c1037d20326049e71d6b3d4afa8e54376b5a339ed00f576dccd8","schema_version":"1.0","event_id":"sha256:7de76b237896c1037d20326049e71d6b3d4afa8e54376b5a339ed00f576dccd8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7IL3VIJG47QDJVT5EM67WXRTP6/bundle.json","state_url":"https://pith.science/pith/7IL3VIJG47QDJVT5EM67WXRTP6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7IL3VIJG47QDJVT5EM67WXRTP6/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":"2026-07-02T08:13:12Z","links":{"resolver":"https://pith.science/pith/7IL3VIJG47QDJVT5EM67WXRTP6","bundle":"https://pith.science/pith/7IL3VIJG47QDJVT5EM67WXRTP6/bundle.json","state":"https://pith.science/pith/7IL3VIJG47QDJVT5EM67WXRTP6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7IL3VIJG47QDJVT5EM67WXRTP6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:7IL3VIJG47QDJVT5EM67WXRTP6","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":"27d89b374c162bc31ce9d74805b36755b1b21e52bfde5f0885e95f8eeafd1cd8","cross_cats_sorted":["cond-mat.other","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-02-01T13:56:13Z","title_canon_sha256":"ad3b4aecbd8ac1d7a98b6adf859cd5c1e4cc6e296d3c874341a6b7cf564c0b0f"},"schema_version":"1.0","source":{"id":"1602.00526","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.00526","created_at":"2026-05-18T01:21:35Z"},{"alias_kind":"arxiv_version","alias_value":"1602.00526v1","created_at":"2026-05-18T01:21:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.00526","created_at":"2026-05-18T01:21:35Z"},{"alias_kind":"pith_short_12","alias_value":"7IL3VIJG47QD","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"7IL3VIJG47QDJVT5","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"7IL3VIJG","created_at":"2026-05-18T12:30:04Z"}],"graph_snapshots":[{"event_id":"sha256:7de76b237896c1037d20326049e71d6b3d4afa8e54376b5a339ed00f576dccd8","target":"graph","created_at":"2026-05-18T01:21:35Z","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 explore the behaviour of the inverse reduced density fluctuations and the isobaric expansion coefficient using {\\alpha},{\\omega}-dibromoalkanes as an example. Two different states are revealed far from the critical point: the region of exponentially decaying fluctuations near the coexistence curve and the state with longer correlations under sufficiently high pressures. The crossing of the isotherms of the isobaric expansion coefficient occurs within the PVT range of the mentioned transition. We discuss the interplay of this crossing with the changes in molecular packing structure connected","authors_text":"Eugene B. Postnikov, Miros{\\l}aw Chor\\k{a}\\.zewski","cross_cats":["cond-mat.other","physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-02-01T13:56:13Z","title":"Transition in fluctuation behaviour of normal liquids under high pressures"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.00526","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:f0e483ec9db798f7dabe80727c6014ee1ae81e0f9e023fe87a24a580ea1c7462","target":"record","created_at":"2026-05-18T01:21:35Z","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":"27d89b374c162bc31ce9d74805b36755b1b21e52bfde5f0885e95f8eeafd1cd8","cross_cats_sorted":["cond-mat.other","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-02-01T13:56:13Z","title_canon_sha256":"ad3b4aecbd8ac1d7a98b6adf859cd5c1e4cc6e296d3c874341a6b7cf564c0b0f"},"schema_version":"1.0","source":{"id":"1602.00526","kind":"arxiv","version":1}},"canonical_sha256":"fa17baa126e7e034d67d233dfb5e337fa356773e14681645d14f4310a47ef730","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fa17baa126e7e034d67d233dfb5e337fa356773e14681645d14f4310a47ef730","first_computed_at":"2026-05-18T01:21:35.183372Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:21:35.183372Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"oKExEIqkFlE5AcDueJText+tZhI1SfVAnlw5c1JSjHv9D/Ky7puSwzeWQUFfx5ORJSD/2yGturAYJoqpkA8NAw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:21:35.184084Z","signed_message":"canonical_sha256_bytes"},"source_id":"1602.00526","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f0e483ec9db798f7dabe80727c6014ee1ae81e0f9e023fe87a24a580ea1c7462","sha256:7de76b237896c1037d20326049e71d6b3d4afa8e54376b5a339ed00f576dccd8"],"state_sha256":"6dc28458fae5c4948728714b8abc84eb67902017d270137d2775acad6edcccbf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YaSQBuS4PFBPLkSrCZ/ME81jd4rhM+mzI1QoQHRGq7VUTmbBEXYU5yF1hiLPuCTTRyk+WxpYuVo9sRVQRus3Dw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-02T08:13:12.479820Z","bundle_sha256":"3a7b69474a5609eb5587ae2400677baab7eb09767a81934ddf4801252b2d7a66"}}