{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:F4IEXR3P2KFUQ42SW76SWUK5ZC","short_pith_number":"pith:F4IEXR3P","canonical_record":{"source":{"id":"2509.14701","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-09-18T07:41:36Z","cross_cats_sorted":["astro-ph.CO","cond-mat.other","physics.atom-ph"],"title_canon_sha256":"cb459c1a00e90da8c03a743880b06d795be06a673a490decb1c5d71d360bfecd","abstract_canon_sha256":"c9ea8216e1887182369bf130204503e0b755024376f6c5f3fd8ed30bb4b082d5"},"schema_version":"1.0"},"canonical_sha256":"2f104bc76fd28b487352b7fd2b515dc88ccb169ce4f0a3ebd7a6037030218819","source":{"kind":"arxiv","id":"2509.14701","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2509.14701","created_at":"2026-07-29T01:24:25Z"},{"alias_kind":"arxiv_version","alias_value":"2509.14701v3","created_at":"2026-07-29T01:24:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2509.14701","created_at":"2026-07-29T01:24:25Z"},{"alias_kind":"pith_short_12","alias_value":"F4IEXR3P2KFU","created_at":"2026-07-29T01:24:25Z"},{"alias_kind":"pith_short_16","alias_value":"F4IEXR3P2KFUQ42S","created_at":"2026-07-29T01:24:25Z"},{"alias_kind":"pith_short_8","alias_value":"F4IEXR3P","created_at":"2026-07-29T01:24:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:F4IEXR3P2KFUQ42SW76SWUK5ZC","target":"record","payload":{"canonical_record":{"source":{"id":"2509.14701","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-09-18T07:41:36Z","cross_cats_sorted":["astro-ph.CO","cond-mat.other","physics.atom-ph"],"title_canon_sha256":"cb459c1a00e90da8c03a743880b06d795be06a673a490decb1c5d71d360bfecd","abstract_canon_sha256":"c9ea8216e1887182369bf130204503e0b755024376f6c5f3fd8ed30bb4b082d5"},"schema_version":"1.0"},"canonical_sha256":"2f104bc76fd28b487352b7fd2b515dc88ccb169ce4f0a3ebd7a6037030218819","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-29T01:24:25.331432Z","signature_b64":"LrS7iq7X/XJIHvIPAvJpWM93Ij1JYakrjcCp/7zeY2IAnYuKpiETWr5Je9WqZ8Og+93OLvCKP4ZJEaRgaJ4aDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2f104bc76fd28b487352b7fd2b515dc88ccb169ce4f0a3ebd7a6037030218819","last_reissued_at":"2026-07-29T01:24:25.330521Z","signature_status":"signed_v1","first_computed_at":"2026-07-29T01:24:25.330521Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2509.14701","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-29T01:24:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7nx7BJKcKXqJYDQv/Yoh0JytS9pN9rULX0EIzlBIUNAE/Fe9ADJrWjC5wVmzaKnzfboeSYlsxXTB45JAfkCeCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-20T09:26:32.858686Z"},"content_sha256":"07de78d086bfbf50b81573355d14a449bfa03ce113f2abfee9961f963a133cac","schema_version":"1.0","event_id":"sha256:07de78d086bfbf50b81573355d14a449bfa03ce113f2abfee9961f963a133cac"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:F4IEXR3P2KFUQ42SW76SWUK5ZC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Enhancement of Weak Interactions in Phase Transitions in Condensed Matter and Early Universe","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO","cond-mat.other","physics.atom-ph"],"primary_cat":"hep-ph","authors_text":"V. V. Flambaum","submitted_at":"2025-09-18T07:41:36Z","abstract_excerpt":"Parity-violating weak interactions produce extremely small energy differences between left- and right-handed chiral systems. We show that these microscopic effects may be strongly amplified during collective phenomena such as phase transitions. The enhancement factor is proportional to the critical number of atoms, $N_c$, in the nucleus of the new phase. After the nucleus reaches its critical size, it grows until it fills the entire system. Measurement of the ratio of produced left and right chiral structures may provide a way to measure this critical number $N_c$. Experiments where definite s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2509.14701","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2509.14701/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-29T01:24:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6L4SWppXTJgDsO75bUTcMX2q8UHxYaiT2qXJjOPjMBgNe8eJ+kuw60DoamJ9sfDFmqru8PU/02mAe57CbBeqDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-20T09:26:32.859191Z"},"content_sha256":"1c35b375053c0c6bb42ef6f392d2073ecab3720297e489e9ec175361f27c2062","schema_version":"1.0","event_id":"sha256:1c35b375053c0c6bb42ef6f392d2073ecab3720297e489e9ec175361f27c2062"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/F4IEXR3P2KFUQ42SW76SWUK5ZC/bundle.json","state_url":"https://pith.science/pith/F4IEXR3P2KFUQ42SW76SWUK5ZC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/F4IEXR3P2KFUQ42SW76SWUK5ZC/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":"2026-08-20T09:26:32Z","links":{"resolver":"https://pith.science/pith/F4IEXR3P2KFUQ42SW76SWUK5ZC","bundle":"https://pith.science/pith/F4IEXR3P2KFUQ42SW76SWUK5ZC/bundle.json","state":"https://pith.science/pith/F4IEXR3P2KFUQ42SW76SWUK5ZC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/F4IEXR3P2KFUQ42SW76SWUK5ZC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:F4IEXR3P2KFUQ42SW76SWUK5ZC","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":"c9ea8216e1887182369bf130204503e0b755024376f6c5f3fd8ed30bb4b082d5","cross_cats_sorted":["astro-ph.CO","cond-mat.other","physics.atom-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-09-18T07:41:36Z","title_canon_sha256":"cb459c1a00e90da8c03a743880b06d795be06a673a490decb1c5d71d360bfecd"},"schema_version":"1.0","source":{"id":"2509.14701","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2509.14701","created_at":"2026-07-29T01:24:25Z"},{"alias_kind":"arxiv_version","alias_value":"2509.14701v3","created_at":"2026-07-29T01:24:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2509.14701","created_at":"2026-07-29T01:24:25Z"},{"alias_kind":"pith_short_12","alias_value":"F4IEXR3P2KFU","created_at":"2026-07-29T01:24:25Z"},{"alias_kind":"pith_short_16","alias_value":"F4IEXR3P2KFUQ42S","created_at":"2026-07-29T01:24:25Z"},{"alias_kind":"pith_short_8","alias_value":"F4IEXR3P","created_at":"2026-07-29T01:24:25Z"}],"graph_snapshots":[{"event_id":"sha256:1c35b375053c0c6bb42ef6f392d2073ecab3720297e489e9ec175361f27c2062","target":"graph","created_at":"2026-07-29T01:24:25Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2509.14701/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Parity-violating weak interactions produce extremely small energy differences between left- and right-handed chiral systems. We show that these microscopic effects may be strongly amplified during collective phenomena such as phase transitions. The enhancement factor is proportional to the critical number of atoms, $N_c$, in the nucleus of the new phase. After the nucleus reaches its critical size, it grows until it fills the entire system. Measurement of the ratio of produced left and right chiral structures may provide a way to measure this critical number $N_c$. Experiments where definite s","authors_text":"V. V. Flambaum","cross_cats":["astro-ph.CO","cond-mat.other","physics.atom-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-09-18T07:41:36Z","title":"Enhancement of Weak Interactions in Phase Transitions in Condensed Matter and Early Universe"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2509.14701","kind":"arxiv","version":3},"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":"sha256:07de78d086bfbf50b81573355d14a449bfa03ce113f2abfee9961f963a133cac","target":"record","created_at":"2026-07-29T01:24:25Z","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":"c9ea8216e1887182369bf130204503e0b755024376f6c5f3fd8ed30bb4b082d5","cross_cats_sorted":["astro-ph.CO","cond-mat.other","physics.atom-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-09-18T07:41:36Z","title_canon_sha256":"cb459c1a00e90da8c03a743880b06d795be06a673a490decb1c5d71d360bfecd"},"schema_version":"1.0","source":{"id":"2509.14701","kind":"arxiv","version":3}},"canonical_sha256":"2f104bc76fd28b487352b7fd2b515dc88ccb169ce4f0a3ebd7a6037030218819","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2f104bc76fd28b487352b7fd2b515dc88ccb169ce4f0a3ebd7a6037030218819","first_computed_at":"2026-07-29T01:24:25.330521Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-29T01:24:25.330521Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"LrS7iq7X/XJIHvIPAvJpWM93Ij1JYakrjcCp/7zeY2IAnYuKpiETWr5Je9WqZ8Og+93OLvCKP4ZJEaRgaJ4aDw==","signature_status":"signed_v1","signed_at":"2026-07-29T01:24:25.331432Z","signed_message":"canonical_sha256_bytes"},"source_id":"2509.14701","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:07de78d086bfbf50b81573355d14a449bfa03ce113f2abfee9961f963a133cac","sha256:1c35b375053c0c6bb42ef6f392d2073ecab3720297e489e9ec175361f27c2062"],"state_sha256":"c563801048bc516a9c6550002b44e22eb350e050719289018d6992678b3e2188"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5cpkTewjjpYzaOcCx/YpBKs6noriMgwcd5e20OhG2Rqog/j3jqxujGTU5mv+oZvDKri2NVjaIvJ1JYZBqaW6AA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-20T09:26:32.864380Z","bundle_sha256":"b926a5faf03cac835ec97f1172c7056e29aec45093a6ae7e1bffdc847649cc07"}}