{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:RG23QAETJTPKQ3U7GLGSFMNSOW","short_pith_number":"pith:RG23QAET","canonical_record":{"source":{"id":"1810.07019","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-10-16T14:18:58Z","cross_cats_sorted":[],"title_canon_sha256":"a5b93b679722706d8d02a29aad152d5f7287ea9c2291c1dfc25d6a17faf822a2","abstract_canon_sha256":"99cb3a17e6940d04cd337e1ef6d11d1d501f8c968a182657eaff4e27e5615002"},"schema_version":"1.0"},"canonical_sha256":"89b5b800934cdea86e9f32cd22b1b275ac44e93efe620503fa1434bb31c4c88b","source":{"kind":"arxiv","id":"1810.07019","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.07019","created_at":"2026-05-17T23:53:25Z"},{"alias_kind":"arxiv_version","alias_value":"1810.07019v1","created_at":"2026-05-17T23:53:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.07019","created_at":"2026-05-17T23:53:25Z"},{"alias_kind":"pith_short_12","alias_value":"RG23QAETJTPK","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_16","alias_value":"RG23QAETJTPKQ3U7","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_8","alias_value":"RG23QAET","created_at":"2026-05-18T12:32:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:RG23QAETJTPKQ3U7GLGSFMNSOW","target":"record","payload":{"canonical_record":{"source":{"id":"1810.07019","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-10-16T14:18:58Z","cross_cats_sorted":[],"title_canon_sha256":"a5b93b679722706d8d02a29aad152d5f7287ea9c2291c1dfc25d6a17faf822a2","abstract_canon_sha256":"99cb3a17e6940d04cd337e1ef6d11d1d501f8c968a182657eaff4e27e5615002"},"schema_version":"1.0"},"canonical_sha256":"89b5b800934cdea86e9f32cd22b1b275ac44e93efe620503fa1434bb31c4c88b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:53:25.915739Z","signature_b64":"zp4IbT+1oHbdfsBCwoZjFfOi2/8ui5SNJ+s8I86m+Fsp9FdoxdmogNyoOdkmxmpPv3PatE0PeUf0ESfBaz5RBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89b5b800934cdea86e9f32cd22b1b275ac44e93efe620503fa1434bb31c4c88b","last_reissued_at":"2026-05-17T23:53:25.914633Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:53:25.914633Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1810.07019","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":"2026-05-17T23:53:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VHWLZJARJRyBHJQQLZPfID/F9qZ7RxOipApX0qQTsuTiuB6rfAbDFwHlLl5hDJ7Lxs8mMenx3IhsMusaxq0lDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T01:58:09.263327Z"},"content_sha256":"0b97021268e044df4b8e6dc739970cc9f2b0c936f793429330e3e59d97e3e5ca","schema_version":"1.0","event_id":"sha256:0b97021268e044df4b8e6dc739970cc9f2b0c936f793429330e3e59d97e3e5ca"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:RG23QAETJTPKQ3U7GLGSFMNSOW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Critical exponents of finite temperature chiral phase transition in soft-wall AdS/QCD models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Danning Li, Jianwei Chen, Mei Huang, Song He","submitted_at":"2018-10-16T14:18:58Z","abstract_excerpt":"Criticality of chiral phase transition at finite temperature is investigated in a soft-wall AdS/QCD model with $SU_L(N_f)\\times SU_R(N_f)$ symmetry, especially for $N_f=2,3$ and $N_f=2+1$. It is shown that in quark mass plane($m_{u/d}-m_s$) chiral phase transition is second order at a certain critical line, by which the whole plane is divided into first order and crossover regions. The critical exponents $\\beta$ and $\\delta$, describing critical behavior of chiral condensate along temperature axis and light quark mass axis, are extracted both numerically and analytically. The model gives the c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.07019","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":"2026-05-17T23:53:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iP/EupWD/o0uVMuXVDnkmgJPtv4fyQ7+rJQEUs/wukCRtWFNZDU2Fcjk1fY3GxHsjHuqOiXNVyzxva0EJIr1AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T01:58:09.263695Z"},"content_sha256":"911a73ad40ca8472dbb9727337921c2201e60853ba605eba3ce5ef3504914358","schema_version":"1.0","event_id":"sha256:911a73ad40ca8472dbb9727337921c2201e60853ba605eba3ce5ef3504914358"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RG23QAETJTPKQ3U7GLGSFMNSOW/bundle.json","state_url":"https://pith.science/pith/RG23QAETJTPKQ3U7GLGSFMNSOW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RG23QAETJTPKQ3U7GLGSFMNSOW/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":"2026-05-28T01:58:09Z","links":{"resolver":"https://pith.science/pith/RG23QAETJTPKQ3U7GLGSFMNSOW","bundle":"https://pith.science/pith/RG23QAETJTPKQ3U7GLGSFMNSOW/bundle.json","state":"https://pith.science/pith/RG23QAETJTPKQ3U7GLGSFMNSOW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RG23QAETJTPKQ3U7GLGSFMNSOW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:RG23QAETJTPKQ3U7GLGSFMNSOW","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":"99cb3a17e6940d04cd337e1ef6d11d1d501f8c968a182657eaff4e27e5615002","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-10-16T14:18:58Z","title_canon_sha256":"a5b93b679722706d8d02a29aad152d5f7287ea9c2291c1dfc25d6a17faf822a2"},"schema_version":"1.0","source":{"id":"1810.07019","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.07019","created_at":"2026-05-17T23:53:25Z"},{"alias_kind":"arxiv_version","alias_value":"1810.07019v1","created_at":"2026-05-17T23:53:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.07019","created_at":"2026-05-17T23:53:25Z"},{"alias_kind":"pith_short_12","alias_value":"RG23QAETJTPK","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_16","alias_value":"RG23QAETJTPKQ3U7","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_8","alias_value":"RG23QAET","created_at":"2026-05-18T12:32:50Z"}],"graph_snapshots":[{"event_id":"sha256:911a73ad40ca8472dbb9727337921c2201e60853ba605eba3ce5ef3504914358","target":"graph","created_at":"2026-05-17T23:53:25Z","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"},"paper":{"abstract_excerpt":"Criticality of chiral phase transition at finite temperature is investigated in a soft-wall AdS/QCD model with $SU_L(N_f)\\times SU_R(N_f)$ symmetry, especially for $N_f=2,3$ and $N_f=2+1$. It is shown that in quark mass plane($m_{u/d}-m_s$) chiral phase transition is second order at a certain critical line, by which the whole plane is divided into first order and crossover regions. The critical exponents $\\beta$ and $\\delta$, describing critical behavior of chiral condensate along temperature axis and light quark mass axis, are extracted both numerically and analytically. The model gives the c","authors_text":"Danning Li, Jianwei Chen, Mei Huang, Song He","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-10-16T14:18:58Z","title":"Critical exponents of finite temperature chiral phase transition in soft-wall AdS/QCD models"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.07019","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":"sha256:0b97021268e044df4b8e6dc739970cc9f2b0c936f793429330e3e59d97e3e5ca","target":"record","created_at":"2026-05-17T23:53:25Z","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":"99cb3a17e6940d04cd337e1ef6d11d1d501f8c968a182657eaff4e27e5615002","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-10-16T14:18:58Z","title_canon_sha256":"a5b93b679722706d8d02a29aad152d5f7287ea9c2291c1dfc25d6a17faf822a2"},"schema_version":"1.0","source":{"id":"1810.07019","kind":"arxiv","version":1}},"canonical_sha256":"89b5b800934cdea86e9f32cd22b1b275ac44e93efe620503fa1434bb31c4c88b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"89b5b800934cdea86e9f32cd22b1b275ac44e93efe620503fa1434bb31c4c88b","first_computed_at":"2026-05-17T23:53:25.914633Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:53:25.914633Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"zp4IbT+1oHbdfsBCwoZjFfOi2/8ui5SNJ+s8I86m+Fsp9FdoxdmogNyoOdkmxmpPv3PatE0PeUf0ESfBaz5RBw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:53:25.915739Z","signed_message":"canonical_sha256_bytes"},"source_id":"1810.07019","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0b97021268e044df4b8e6dc739970cc9f2b0c936f793429330e3e59d97e3e5ca","sha256:911a73ad40ca8472dbb9727337921c2201e60853ba605eba3ce5ef3504914358"],"state_sha256":"7c2d7f8dab141cfa3a5992b9f6c71ea1b2e34f18da044855dbe84f4af7979f9a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NB/FPIVho+cQX+3FjfgowCyo4xSqohtozL8MBdj3jul4OL97Fi0dgIWQyV6pr4tbFvXzl9D8KJfNpPIpkJxpAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T01:58:09.265713Z","bundle_sha256":"7b212a946f818758b5d3802c817a4c8f38aa69f1d24e4a12215b610169e9cf02"}}