{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:3Y235XRRFNGMDS6MF6H43GQGHV","short_pith_number":"pith:3Y235XRR","canonical_record":{"source":{"id":"1610.05585","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2016-10-18T12:53:44Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"99c4935886c21b08b1d7063c821537023c421e8f916d9a3f8fa9249ec92b3feb","abstract_canon_sha256":"1161d00ee7115cfd3a78e790855daa2e9d98e9bc7555679515f40e7dfe2c1624"},"schema_version":"1.0"},"canonical_sha256":"de35bede312b4cc1cbcc2f8fcd9a063d7740e6d19921f8cc1512a8b0e7abf075","source":{"kind":"arxiv","id":"1610.05585","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.05585","created_at":"2026-05-18T01:01:58Z"},{"alias_kind":"arxiv_version","alias_value":"1610.05585v1","created_at":"2026-05-18T01:01:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.05585","created_at":"2026-05-18T01:01:58Z"},{"alias_kind":"pith_short_12","alias_value":"3Y235XRRFNGM","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_16","alias_value":"3Y235XRRFNGMDS6M","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_8","alias_value":"3Y235XRR","created_at":"2026-05-18T12:29:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:3Y235XRRFNGMDS6MF6H43GQGHV","target":"record","payload":{"canonical_record":{"source":{"id":"1610.05585","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2016-10-18T12:53:44Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"99c4935886c21b08b1d7063c821537023c421e8f916d9a3f8fa9249ec92b3feb","abstract_canon_sha256":"1161d00ee7115cfd3a78e790855daa2e9d98e9bc7555679515f40e7dfe2c1624"},"schema_version":"1.0"},"canonical_sha256":"de35bede312b4cc1cbcc2f8fcd9a063d7740e6d19921f8cc1512a8b0e7abf075","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:01:58.912094Z","signature_b64":"6i0qjN4yJAwBD61yZzBVamB8NoEF985QOVrfUPDJkvSHmBmXnrAGhYq6Zm/6yfGvtBmE5Kouk7kf4G/gYmWJBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"de35bede312b4cc1cbcc2f8fcd9a063d7740e6d19921f8cc1512a8b0e7abf075","last_reissued_at":"2026-05-18T01:01:58.911490Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:01:58.911490Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1610.05585","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":"2026-05-18T01:01:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NnWV4QecVKUXy/oi/nI3UKJV7tR/IrYH3NMJ74Ha6nQ21NFmOMGsPbJ0jT29KYvkqU5RfZNEWEWOgivbZs+8Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T16:59:10.984153Z"},"content_sha256":"6c8147dda0bd1c6184ec2b4deb6eb90f9bae43630d258b3527278baa44e6a3d7","schema_version":"1.0","event_id":"sha256:6c8147dda0bd1c6184ec2b4deb6eb90f9bae43630d258b3527278baa44e6a3d7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:3Y235XRRFNGMDS6MF6H43GQGHV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Effect of entropy on the nucleation of cavitation bubbles in water under tension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft"],"primary_cat":"physics.chem-ph","authors_text":"Christoph Dellago, Georg Menzl","submitted_at":"2016-10-18T12:53:44Z","abstract_excerpt":"Water can exist in a metastable liquid state under tension for long times before the system relaxes into the vapor via cavitation, i.e., bubble nucleation. Microscopic information on the cavitation process can be extracted from experimental data by use of the nucleation theorem, which relates measured cavitation rates to the size of the critical bubble. To apply the nucleation theorem to experiments performed along an isochoric path, for instance, in cavitation experiments in mineral inclusions, knowledge of the bubble entropy is required. Using computer simulations, we compute the entropy of "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.05585","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":"2026-05-18T01:01:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fzoCJqS3I/+pQ4NvZdA8kZlUbGRV1RuY6BOtrNXJdqlbyxAswrguTvQb6UG2g7rcwQfnbDgoN1PXuTlvXHfCDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T16:59:10.984537Z"},"content_sha256":"8b82c899882053414a7df19bf4e4bc86487ceb2290b37f43eb65d32b383f3fa9","schema_version":"1.0","event_id":"sha256:8b82c899882053414a7df19bf4e4bc86487ceb2290b37f43eb65d32b383f3fa9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3Y235XRRFNGMDS6MF6H43GQGHV/bundle.json","state_url":"https://pith.science/pith/3Y235XRRFNGMDS6MF6H43GQGHV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3Y235XRRFNGMDS6MF6H43GQGHV/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":"2026-05-27T16:59:10Z","links":{"resolver":"https://pith.science/pith/3Y235XRRFNGMDS6MF6H43GQGHV","bundle":"https://pith.science/pith/3Y235XRRFNGMDS6MF6H43GQGHV/bundle.json","state":"https://pith.science/pith/3Y235XRRFNGMDS6MF6H43GQGHV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3Y235XRRFNGMDS6MF6H43GQGHV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:3Y235XRRFNGMDS6MF6H43GQGHV","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":"1161d00ee7115cfd3a78e790855daa2e9d98e9bc7555679515f40e7dfe2c1624","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2016-10-18T12:53:44Z","title_canon_sha256":"99c4935886c21b08b1d7063c821537023c421e8f916d9a3f8fa9249ec92b3feb"},"schema_version":"1.0","source":{"id":"1610.05585","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.05585","created_at":"2026-05-18T01:01:58Z"},{"alias_kind":"arxiv_version","alias_value":"1610.05585v1","created_at":"2026-05-18T01:01:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.05585","created_at":"2026-05-18T01:01:58Z"},{"alias_kind":"pith_short_12","alias_value":"3Y235XRRFNGM","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_16","alias_value":"3Y235XRRFNGMDS6M","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_8","alias_value":"3Y235XRR","created_at":"2026-05-18T12:29:58Z"}],"graph_snapshots":[{"event_id":"sha256:8b82c899882053414a7df19bf4e4bc86487ceb2290b37f43eb65d32b383f3fa9","target":"graph","created_at":"2026-05-18T01:01:58Z","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":"Water can exist in a metastable liquid state under tension for long times before the system relaxes into the vapor via cavitation, i.e., bubble nucleation. Microscopic information on the cavitation process can be extracted from experimental data by use of the nucleation theorem, which relates measured cavitation rates to the size of the critical bubble. To apply the nucleation theorem to experiments performed along an isochoric path, for instance, in cavitation experiments in mineral inclusions, knowledge of the bubble entropy is required. Using computer simulations, we compute the entropy of ","authors_text":"Christoph Dellago, Georg Menzl","cross_cats":["cond-mat.soft"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2016-10-18T12:53:44Z","title":"Effect of entropy on the nucleation of cavitation bubbles in water under tension"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.05585","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":"sha256:6c8147dda0bd1c6184ec2b4deb6eb90f9bae43630d258b3527278baa44e6a3d7","target":"record","created_at":"2026-05-18T01:01:58Z","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":"1161d00ee7115cfd3a78e790855daa2e9d98e9bc7555679515f40e7dfe2c1624","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2016-10-18T12:53:44Z","title_canon_sha256":"99c4935886c21b08b1d7063c821537023c421e8f916d9a3f8fa9249ec92b3feb"},"schema_version":"1.0","source":{"id":"1610.05585","kind":"arxiv","version":1}},"canonical_sha256":"de35bede312b4cc1cbcc2f8fcd9a063d7740e6d19921f8cc1512a8b0e7abf075","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"de35bede312b4cc1cbcc2f8fcd9a063d7740e6d19921f8cc1512a8b0e7abf075","first_computed_at":"2026-05-18T01:01:58.911490Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:01:58.911490Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6i0qjN4yJAwBD61yZzBVamB8NoEF985QOVrfUPDJkvSHmBmXnrAGhYq6Zm/6yfGvtBmE5Kouk7kf4G/gYmWJBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:01:58.912094Z","signed_message":"canonical_sha256_bytes"},"source_id":"1610.05585","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6c8147dda0bd1c6184ec2b4deb6eb90f9bae43630d258b3527278baa44e6a3d7","sha256:8b82c899882053414a7df19bf4e4bc86487ceb2290b37f43eb65d32b383f3fa9"],"state_sha256":"685c9d7f6deacc451ee0d1d391af5c23a91b45a656012e009e02d5b9c96f8bd5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZLjg1Fkr0HKBQZiEhlWv5IzLMNo+Jp8lBwYgdJnFE5glvaGd9yrhSsXtVqp/YcnNDl6E9p7bprDvFzPDxm7rAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T16:59:10.986667Z","bundle_sha256":"1082d10e41c6831630bfc2f060232238f2cb38652148a5bdabff2d8dc750e65a"}}