{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:DNU4R6ABZ4S7LEQG7RWZ3J7YUW","short_pith_number":"pith:DNU4R6AB","canonical_record":{"source":{"id":"1404.4031","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2014-04-15T19:35:09Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"3903f47682aecb69653349204aaa33e7831d96211b3ae91ca2c3c63c717181f9","abstract_canon_sha256":"4593d144cf64b60db45ef78afe05070a8effcf990f73f15b069a50d6cbae2913"},"schema_version":"1.0"},"canonical_sha256":"1b69c8f801cf25f59206fc6d9da7f8a5a7c5397cf2bb6de3cdc0d7f052706d0c","source":{"kind":"arxiv","id":"1404.4031","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.4031","created_at":"2026-05-18T02:54:13Z"},{"alias_kind":"arxiv_version","alias_value":"1404.4031v1","created_at":"2026-05-18T02:54:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.4031","created_at":"2026-05-18T02:54:13Z"},{"alias_kind":"pith_short_12","alias_value":"DNU4R6ABZ4S7","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"DNU4R6ABZ4S7LEQG","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"DNU4R6AB","created_at":"2026-05-18T12:28:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:DNU4R6ABZ4S7LEQG7RWZ3J7YUW","target":"record","payload":{"canonical_record":{"source":{"id":"1404.4031","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2014-04-15T19:35:09Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"3903f47682aecb69653349204aaa33e7831d96211b3ae91ca2c3c63c717181f9","abstract_canon_sha256":"4593d144cf64b60db45ef78afe05070a8effcf990f73f15b069a50d6cbae2913"},"schema_version":"1.0"},"canonical_sha256":"1b69c8f801cf25f59206fc6d9da7f8a5a7c5397cf2bb6de3cdc0d7f052706d0c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:54:13.128776Z","signature_b64":"DzqUyywhKckFbOFLuVMhFgTM5ePw5hDPj3f5xwrMlUt6Fe0ocdvruRZ6z5cHXRpideac0cQWJv4DvFrquZZMDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1b69c8f801cf25f59206fc6d9da7f8a5a7c5397cf2bb6de3cdc0d7f052706d0c","last_reissued_at":"2026-05-18T02:54:13.128182Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:54:13.128182Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1404.4031","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":"2026-05-18T02:54:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hpmnjmU+6hX3acZbK0XPdKvSMccR33a0smNmuE3IIQdw70IRz1OatQaBsrCMrH5vDXs/LbHBQaSmL1Ns4PnyCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T22:51:23.778528Z"},"content_sha256":"f902b17b1c6c22ec2c574c875cbe01f096de209a739fdcafb83155521def8b0e","schema_version":"1.0","event_id":"sha256:f902b17b1c6c22ec2c574c875cbe01f096de209a739fdcafb83155521def8b0e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:DNU4R6ABZ4S7LEQG7RWZ3J7YUW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Water and its relatives: the stable, supercooled and particularly the stretched, regimes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft"],"primary_cat":"physics.chem-ph","authors_text":"C. Austen Angell, Stacey L. Meadley","submitted_at":"2014-04-15T19:35:09Z","abstract_excerpt":"While the water molecule is simple, its condensed phase liquid behavior is so complex that no consensus description has emerged despite three centuries of effort. Here we identify features of its behavior that are the most peculiar, hence suggest ways forward. We examine the properties of water at the boundaries of common experience, including stable states at high pressure, the supercooled state at normal and elevated pressure, and the stretched (\"negative pressure\") state, out to the limits of mechanical stability. The familiar anomalies at moderate pressures (viscosity and density (TMD) beh"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.4031","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":"2026-05-18T02:54:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gDl9Pc2KJVqTlYNS/rdG8wLF2Emh+f4hiRYv2tTNyEonk+hihZRQ45fmJx2do9d4s+9uwIYBwwVXsX4PPPkxCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T22:51:23.778888Z"},"content_sha256":"af5002e35fa4f18b66e95ce5618449d36a7e697b1855c25f7d5415e5a6bc7d10","schema_version":"1.0","event_id":"sha256:af5002e35fa4f18b66e95ce5618449d36a7e697b1855c25f7d5415e5a6bc7d10"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DNU4R6ABZ4S7LEQG7RWZ3J7YUW/bundle.json","state_url":"https://pith.science/pith/DNU4R6ABZ4S7LEQG7RWZ3J7YUW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DNU4R6ABZ4S7LEQG7RWZ3J7YUW/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":"2026-06-25T22:51:23Z","links":{"resolver":"https://pith.science/pith/DNU4R6ABZ4S7LEQG7RWZ3J7YUW","bundle":"https://pith.science/pith/DNU4R6ABZ4S7LEQG7RWZ3J7YUW/bundle.json","state":"https://pith.science/pith/DNU4R6ABZ4S7LEQG7RWZ3J7YUW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DNU4R6ABZ4S7LEQG7RWZ3J7YUW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:DNU4R6ABZ4S7LEQG7RWZ3J7YUW","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":"4593d144cf64b60db45ef78afe05070a8effcf990f73f15b069a50d6cbae2913","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2014-04-15T19:35:09Z","title_canon_sha256":"3903f47682aecb69653349204aaa33e7831d96211b3ae91ca2c3c63c717181f9"},"schema_version":"1.0","source":{"id":"1404.4031","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.4031","created_at":"2026-05-18T02:54:13Z"},{"alias_kind":"arxiv_version","alias_value":"1404.4031v1","created_at":"2026-05-18T02:54:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.4031","created_at":"2026-05-18T02:54:13Z"},{"alias_kind":"pith_short_12","alias_value":"DNU4R6ABZ4S7","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"DNU4R6ABZ4S7LEQG","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"DNU4R6AB","created_at":"2026-05-18T12:28:25Z"}],"graph_snapshots":[{"event_id":"sha256:af5002e35fa4f18b66e95ce5618449d36a7e697b1855c25f7d5415e5a6bc7d10","target":"graph","created_at":"2026-05-18T02:54:13Z","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":"While the water molecule is simple, its condensed phase liquid behavior is so complex that no consensus description has emerged despite three centuries of effort. Here we identify features of its behavior that are the most peculiar, hence suggest ways forward. We examine the properties of water at the boundaries of common experience, including stable states at high pressure, the supercooled state at normal and elevated pressure, and the stretched (\"negative pressure\") state, out to the limits of mechanical stability. The familiar anomalies at moderate pressures (viscosity and density (TMD) beh","authors_text":"C. Austen Angell, Stacey L. Meadley","cross_cats":["cond-mat.soft"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2014-04-15T19:35:09Z","title":"Water and its relatives: the stable, supercooled and particularly the stretched, regimes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.4031","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:f902b17b1c6c22ec2c574c875cbe01f096de209a739fdcafb83155521def8b0e","target":"record","created_at":"2026-05-18T02:54:13Z","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":"4593d144cf64b60db45ef78afe05070a8effcf990f73f15b069a50d6cbae2913","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2014-04-15T19:35:09Z","title_canon_sha256":"3903f47682aecb69653349204aaa33e7831d96211b3ae91ca2c3c63c717181f9"},"schema_version":"1.0","source":{"id":"1404.4031","kind":"arxiv","version":1}},"canonical_sha256":"1b69c8f801cf25f59206fc6d9da7f8a5a7c5397cf2bb6de3cdc0d7f052706d0c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1b69c8f801cf25f59206fc6d9da7f8a5a7c5397cf2bb6de3cdc0d7f052706d0c","first_computed_at":"2026-05-18T02:54:13.128182Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:54:13.128182Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"DzqUyywhKckFbOFLuVMhFgTM5ePw5hDPj3f5xwrMlUt6Fe0ocdvruRZ6z5cHXRpideac0cQWJv4DvFrquZZMDw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:54:13.128776Z","signed_message":"canonical_sha256_bytes"},"source_id":"1404.4031","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f902b17b1c6c22ec2c574c875cbe01f096de209a739fdcafb83155521def8b0e","sha256:af5002e35fa4f18b66e95ce5618449d36a7e697b1855c25f7d5415e5a6bc7d10"],"state_sha256":"f4317a7d3988717df9cbcf54a2fecb9d510a1ab488991659959eaaf745b1c30a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dTSIM4z5TI5RJ8oHfqyC+rWeGvdAWAbq3EtYROXXlldOzQOpvbUnJB6Aa6w6vd4NqUuEbZXB3xOwwoKKBFjwCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-25T22:51:23.781130Z","bundle_sha256":"79328a19d847fdd31d7565520b86370fd41d1211c29a874e34985c575bac7535"}}