{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:YROLPBNBIDQBEZLKOOYUPWXTEC","short_pith_number":"pith:YROLPBNB","canonical_record":{"source":{"id":"1407.6322","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-07-23T18:24:38Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"c866c6b71bbcd607d1eba7395aee88fa9861971a47f8a34107d40dc23852b0b3","abstract_canon_sha256":"58fd439823e4d46fcaec9e6cfbb45f3106394b3a098a445899a4e3e2e44c7932"},"schema_version":"1.0"},"canonical_sha256":"c45cb785a140e012656a73b147daf320bb76cf72c800ce151ebe23f0c8172ef8","source":{"kind":"arxiv","id":"1407.6322","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.6322","created_at":"2026-05-18T01:35:16Z"},{"alias_kind":"arxiv_version","alias_value":"1407.6322v2","created_at":"2026-05-18T01:35:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.6322","created_at":"2026-05-18T01:35:16Z"},{"alias_kind":"pith_short_12","alias_value":"YROLPBNBIDQB","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"YROLPBNBIDQBEZLK","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"YROLPBNB","created_at":"2026-05-18T12:28:57Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:YROLPBNBIDQBEZLKOOYUPWXTEC","target":"record","payload":{"canonical_record":{"source":{"id":"1407.6322","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-07-23T18:24:38Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"c866c6b71bbcd607d1eba7395aee88fa9861971a47f8a34107d40dc23852b0b3","abstract_canon_sha256":"58fd439823e4d46fcaec9e6cfbb45f3106394b3a098a445899a4e3e2e44c7932"},"schema_version":"1.0"},"canonical_sha256":"c45cb785a140e012656a73b147daf320bb76cf72c800ce151ebe23f0c8172ef8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:35:16.603613Z","signature_b64":"JZrnVJ74ck/4RaBaMQFyL5E0TsU5eQP9McJ+4kowG84JHVDhGT7SBHHaBDo4DMuqTB7K5YA0dwrFW0MWdR9sBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c45cb785a140e012656a73b147daf320bb76cf72c800ce151ebe23f0c8172ef8","last_reissued_at":"2026-05-18T01:35:16.602923Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:35:16.602923Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.6322","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:35:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aCp8vYma/D7KxKrUjKV3A09UBtYiOAvPMvybtFGQfEOPqpE4UEJmx1xf9fgkVbcJ3eXP3eEAsjTzWDI47d5gAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T14:17:15.558075Z"},"content_sha256":"e25c539a60e9b60c0602c4d6ff783b8cc7121c98f49ede1680c426f96d8c3bc7","schema_version":"1.0","event_id":"sha256:e25c539a60e9b60c0602c4d6ff783b8cc7121c98f49ede1680c426f96d8c3bc7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:YROLPBNBIDQBEZLKOOYUPWXTEC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Specific heat anomaly in a supercooled liquid with amorphous boundary conditions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"Andrea Cavagna, Daniel A. Martin, Tomas S. Grigera","submitted_at":"2014-07-23T18:24:38Z","abstract_excerpt":"We study the specific heat of a model supercooled liquid confined in a spherical cavity with amorphous boundary conditions. We find the equilibrium specific heat has a cavity-size-dependent peak as a function of temperature. The cavity allows us to perform a finite-size scaling (FSS) analysis, which indicates that the peak persists at a finite temperature in the thermodynamic limit. We attempt to collapse the data onto a FSS curve according to different theoretical scenarios, obtaining reasonable results in two cases: a \"not-so-simple\" liquid with nonstandard values of the exponents {\\alpha} a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.6322","kind":"arxiv","version":2},"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":"2026-05-18T01:35:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"E2H/ou6rMPPRu2gZMXfPkJT4vdA1h1YRlOeHNlYWXxwlLFhx4hIyKTy5mzuHFHh/DcaAJN2EvikTaGbH8DA7DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T14:17:15.558438Z"},"content_sha256":"501fb89221efd047d7cd751b319acb58e1eba8c02c3703c3942576736c95cdfe","schema_version":"1.0","event_id":"sha256:501fb89221efd047d7cd751b319acb58e1eba8c02c3703c3942576736c95cdfe"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YROLPBNBIDQBEZLKOOYUPWXTEC/bundle.json","state_url":"https://pith.science/pith/YROLPBNBIDQBEZLKOOYUPWXTEC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YROLPBNBIDQBEZLKOOYUPWXTEC/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":"2026-05-21T14:17:15Z","links":{"resolver":"https://pith.science/pith/YROLPBNBIDQBEZLKOOYUPWXTEC","bundle":"https://pith.science/pith/YROLPBNBIDQBEZLKOOYUPWXTEC/bundle.json","state":"https://pith.science/pith/YROLPBNBIDQBEZLKOOYUPWXTEC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YROLPBNBIDQBEZLKOOYUPWXTEC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:YROLPBNBIDQBEZLKOOYUPWXTEC","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":"58fd439823e4d46fcaec9e6cfbb45f3106394b3a098a445899a4e3e2e44c7932","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-07-23T18:24:38Z","title_canon_sha256":"c866c6b71bbcd607d1eba7395aee88fa9861971a47f8a34107d40dc23852b0b3"},"schema_version":"1.0","source":{"id":"1407.6322","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.6322","created_at":"2026-05-18T01:35:16Z"},{"alias_kind":"arxiv_version","alias_value":"1407.6322v2","created_at":"2026-05-18T01:35:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.6322","created_at":"2026-05-18T01:35:16Z"},{"alias_kind":"pith_short_12","alias_value":"YROLPBNBIDQB","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"YROLPBNBIDQBEZLK","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"YROLPBNB","created_at":"2026-05-18T12:28:57Z"}],"graph_snapshots":[{"event_id":"sha256:501fb89221efd047d7cd751b319acb58e1eba8c02c3703c3942576736c95cdfe","target":"graph","created_at":"2026-05-18T01:35:16Z","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 specific heat of a model supercooled liquid confined in a spherical cavity with amorphous boundary conditions. We find the equilibrium specific heat has a cavity-size-dependent peak as a function of temperature. The cavity allows us to perform a finite-size scaling (FSS) analysis, which indicates that the peak persists at a finite temperature in the thermodynamic limit. We attempt to collapse the data onto a FSS curve according to different theoretical scenarios, obtaining reasonable results in two cases: a \"not-so-simple\" liquid with nonstandard values of the exponents {\\alpha} a","authors_text":"Andrea Cavagna, Daniel A. Martin, Tomas S. Grigera","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-07-23T18:24:38Z","title":"Specific heat anomaly in a supercooled liquid with amorphous boundary conditions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.6322","kind":"arxiv","version":2},"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:e25c539a60e9b60c0602c4d6ff783b8cc7121c98f49ede1680c426f96d8c3bc7","target":"record","created_at":"2026-05-18T01:35:16Z","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":"58fd439823e4d46fcaec9e6cfbb45f3106394b3a098a445899a4e3e2e44c7932","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-07-23T18:24:38Z","title_canon_sha256":"c866c6b71bbcd607d1eba7395aee88fa9861971a47f8a34107d40dc23852b0b3"},"schema_version":"1.0","source":{"id":"1407.6322","kind":"arxiv","version":2}},"canonical_sha256":"c45cb785a140e012656a73b147daf320bb76cf72c800ce151ebe23f0c8172ef8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c45cb785a140e012656a73b147daf320bb76cf72c800ce151ebe23f0c8172ef8","first_computed_at":"2026-05-18T01:35:16.602923Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:35:16.602923Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"JZrnVJ74ck/4RaBaMQFyL5E0TsU5eQP9McJ+4kowG84JHVDhGT7SBHHaBDo4DMuqTB7K5YA0dwrFW0MWdR9sBw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:35:16.603613Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.6322","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e25c539a60e9b60c0602c4d6ff783b8cc7121c98f49ede1680c426f96d8c3bc7","sha256:501fb89221efd047d7cd751b319acb58e1eba8c02c3703c3942576736c95cdfe"],"state_sha256":"5e7ac25309289863522258ba063d018410fa033a8f4bfe8af010c8520a4fd819"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"b0MeHuZfh1MQfykRYccGSplbcxcFk5qZN4kILE3y4FirZHXSGr8YBTW2uq+xPsB2DNDWeguQ+Lxvp4ptxYrzAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-21T14:17:15.560417Z","bundle_sha256":"24a87a85100b4393fe4b0ceafe1e8a99b16ddf8a97dba7a6bf28e569de33e35f"}}