{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2005:5WYD27M4HY5DOG3HTSBJVRUYFU","short_pith_number":"pith:5WYD27M4","canonical_record":{"source":{"id":"hep-ph/0504073","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-04-09T15:12:34Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"516580439d4c713bbae81e83c870a6855870666b74cf3efefde45d5ca989887a","abstract_canon_sha256":"e5c323bd22f958c44fd2b3b31de77885819cf875daee0905127bfa43e4cfb8b2"},"schema_version":"1.0"},"canonical_sha256":"edb03d7d9c3e3a371b679c829ac6982d041b32ed44fe270b4ac750e1bfa95bf8","source":{"kind":"arxiv","id":"hep-ph/0504073","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0504073","created_at":"2026-07-04T14:29:14Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0504073v1","created_at":"2026-07-04T14:29:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0504073","created_at":"2026-07-04T14:29:14Z"},{"alias_kind":"pith_short_12","alias_value":"5WYD27M4HY5D","created_at":"2026-07-04T14:29:14Z"},{"alias_kind":"pith_short_16","alias_value":"5WYD27M4HY5DOG3H","created_at":"2026-07-04T14:29:14Z"},{"alias_kind":"pith_short_8","alias_value":"5WYD27M4","created_at":"2026-07-04T14:29:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2005:5WYD27M4HY5DOG3HTSBJVRUYFU","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0504073","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-04-09T15:12:34Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"516580439d4c713bbae81e83c870a6855870666b74cf3efefde45d5ca989887a","abstract_canon_sha256":"e5c323bd22f958c44fd2b3b31de77885819cf875daee0905127bfa43e4cfb8b2"},"schema_version":"1.0"},"canonical_sha256":"edb03d7d9c3e3a371b679c829ac6982d041b32ed44fe270b4ac750e1bfa95bf8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:29:14.544169Z","signature_b64":"V/h+e9shleal2uLbV3r+gaVLEfT6s+aBpi9WF4JDly94hEemaWYM9M2UwHoaXJ3HxX2yitkgreOytvN9o8HsDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"edb03d7d9c3e3a371b679c829ac6982d041b32ed44fe270b4ac750e1bfa95bf8","last_reissued_at":"2026-07-04T14:29:14.543774Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:29:14.543774Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0504073","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":"2026-07-04T14:29:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Qxw08L9lxrznlUOAPlkcNgA2rL2epB57Q8LPL81e8VK+RiP1GoGYP5RjkC4Tih0vCuk1wD0zivNPOLFtRr8yCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T12:05:03.330520Z"},"content_sha256":"ca9f97d51491f2c2c12d431162ef7cefadc7904c081fbd0b0946c51daa4b4db8","schema_version":"1.0","event_id":"sha256:ca9f97d51491f2c2c12d431162ef7cefadc7904c081fbd0b0946c51daa4b4db8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2005:5WYD27M4HY5DOG3HTSBJVRUYFU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Chiral Phase Transition in QCD and Vector Manifestation","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Chihiro Sasaki","submitted_at":"2005-04-09T15:12:34Z","abstract_excerpt":"Spontaneous chiral symmetry breaking is one of the most important features in low-energy QCD. The chiral symmetry is expected to be restored at very high temperature and/or density. Accompanied by the chiral phase transition, properties of hadrons will be changed especially near the critical point. The study of the phenomena associated with the chiral phase transition will give us some clues on the connection between the chiral symmetry and the low-energy hadron dynamics.\n  We develop the theory based on the hidden local symmetry (HLS) at finite temperature, which is an effective field theory "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0504073","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0504073/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":"2026-07-04T14:29:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GJP5HWE3wSjOLR2N6ORqhDqTt08Is6Cw4lO/sQlEf5myLdiIPLIaEs534HivLgnJ3DiMuJqA40U/uobJeSUIBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T12:05:03.331101Z"},"content_sha256":"52c6c8d04c03cb3a291ac621e94957ddea260fc7f529859906f83a0214bd34e6","schema_version":"1.0","event_id":"sha256:52c6c8d04c03cb3a291ac621e94957ddea260fc7f529859906f83a0214bd34e6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5WYD27M4HY5DOG3HTSBJVRUYFU/bundle.json","state_url":"https://pith.science/pith/5WYD27M4HY5DOG3HTSBJVRUYFU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5WYD27M4HY5DOG3HTSBJVRUYFU/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":"2026-08-15T12:05:03Z","links":{"resolver":"https://pith.science/pith/5WYD27M4HY5DOG3HTSBJVRUYFU","bundle":"https://pith.science/pith/5WYD27M4HY5DOG3HTSBJVRUYFU/bundle.json","state":"https://pith.science/pith/5WYD27M4HY5DOG3HTSBJVRUYFU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5WYD27M4HY5DOG3HTSBJVRUYFU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2005:5WYD27M4HY5DOG3HTSBJVRUYFU","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":"e5c323bd22f958c44fd2b3b31de77885819cf875daee0905127bfa43e4cfb8b2","cross_cats_sorted":["nucl-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2005-04-09T15:12:34Z","title_canon_sha256":"516580439d4c713bbae81e83c870a6855870666b74cf3efefde45d5ca989887a"},"schema_version":"1.0","source":{"id":"hep-ph/0504073","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0504073","created_at":"2026-07-04T14:29:14Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0504073v1","created_at":"2026-07-04T14:29:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0504073","created_at":"2026-07-04T14:29:14Z"},{"alias_kind":"pith_short_12","alias_value":"5WYD27M4HY5D","created_at":"2026-07-04T14:29:14Z"},{"alias_kind":"pith_short_16","alias_value":"5WYD27M4HY5DOG3H","created_at":"2026-07-04T14:29:14Z"},{"alias_kind":"pith_short_8","alias_value":"5WYD27M4","created_at":"2026-07-04T14:29:14Z"}],"graph_snapshots":[{"event_id":"sha256:52c6c8d04c03cb3a291ac621e94957ddea260fc7f529859906f83a0214bd34e6","target":"graph","created_at":"2026-07-04T14:29:14Z","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/hep-ph/0504073/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Spontaneous chiral symmetry breaking is one of the most important features in low-energy QCD. The chiral symmetry is expected to be restored at very high temperature and/or density. Accompanied by the chiral phase transition, properties of hadrons will be changed especially near the critical point. The study of the phenomena associated with the chiral phase transition will give us some clues on the connection between the chiral symmetry and the low-energy hadron dynamics.\n  We develop the theory based on the hidden local symmetry (HLS) at finite temperature, which is an effective field theory ","authors_text":"Chihiro Sasaki","cross_cats":["nucl-th"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2005-04-09T15:12:34Z","title":"Chiral Phase Transition in QCD and Vector Manifestation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0504073","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:ca9f97d51491f2c2c12d431162ef7cefadc7904c081fbd0b0946c51daa4b4db8","target":"record","created_at":"2026-07-04T14:29:14Z","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":"e5c323bd22f958c44fd2b3b31de77885819cf875daee0905127bfa43e4cfb8b2","cross_cats_sorted":["nucl-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2005-04-09T15:12:34Z","title_canon_sha256":"516580439d4c713bbae81e83c870a6855870666b74cf3efefde45d5ca989887a"},"schema_version":"1.0","source":{"id":"hep-ph/0504073","kind":"arxiv","version":1}},"canonical_sha256":"edb03d7d9c3e3a371b679c829ac6982d041b32ed44fe270b4ac750e1bfa95bf8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"edb03d7d9c3e3a371b679c829ac6982d041b32ed44fe270b4ac750e1bfa95bf8","first_computed_at":"2026-07-04T14:29:14.543774Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T14:29:14.543774Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"V/h+e9shleal2uLbV3r+gaVLEfT6s+aBpi9WF4JDly94hEemaWYM9M2UwHoaXJ3HxX2yitkgreOytvN9o8HsDw==","signature_status":"signed_v1","signed_at":"2026-07-04T14:29:14.544169Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0504073","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ca9f97d51491f2c2c12d431162ef7cefadc7904c081fbd0b0946c51daa4b4db8","sha256:52c6c8d04c03cb3a291ac621e94957ddea260fc7f529859906f83a0214bd34e6"],"state_sha256":"5d8398716861805a99c18ca84766622b4e0dceef7fcf1684c28e99de0210f09f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"c99TOoRl4BEG5cKf+tV9nHu1YwN1tkTj5Vjvf5SSrjhypURdMeu+3uaUyQkTlWpPcOn3kPsro8ANJSsPl6nECQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-15T12:05:03.334589Z","bundle_sha256":"ef59f998c93f764ecfb60458e1b2c5e00a41c1cde9069d7bbe948e4d8082d75e"}}