{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1995:5Z4QNR26TOVAC224HKDRXUCXQR","short_pith_number":"pith:5Z4QNR26","canonical_record":{"source":{"id":"hep-ph/9503469","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-03-30T15:35:09Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"a683f1da68ff012bc83eded19aef439f207954fb613ee23120284a10ec11fd00","abstract_canon_sha256":"1b0144736de8beb60e15d0b0bf0bb5ba1d360c8d06b44655066a7ebe5e9b5f55"},"schema_version":"1.0"},"canonical_sha256":"ee7906c75e9baa016b5c3a871bd057847c3197c7feedd8f880f544a7ec0dea40","source":{"kind":"arxiv","id":"hep-ph/9503469","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9503469","created_at":"2026-05-18T01:06:30Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9503469v1","created_at":"2026-05-18T01:06:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9503469","created_at":"2026-05-18T01:06:30Z"},{"alias_kind":"pith_short_12","alias_value":"5Z4QNR26TOVA","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"5Z4QNR26TOVAC224","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"5Z4QNR26","created_at":"2026-05-18T12:25:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1995:5Z4QNR26TOVAC224HKDRXUCXQR","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9503469","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-03-30T15:35:09Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"a683f1da68ff012bc83eded19aef439f207954fb613ee23120284a10ec11fd00","abstract_canon_sha256":"1b0144736de8beb60e15d0b0bf0bb5ba1d360c8d06b44655066a7ebe5e9b5f55"},"schema_version":"1.0"},"canonical_sha256":"ee7906c75e9baa016b5c3a871bd057847c3197c7feedd8f880f544a7ec0dea40","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:30.389909Z","signature_b64":"O1CXThSTncljt3qHWQ5M+Rbjhu4qOPl9d/87u+R9nEnEFRpT7H93ii/ZY+5qslNVwf9VpQLGjCugi3eglMnlBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ee7906c75e9baa016b5c3a871bd057847c3197c7feedd8f880f544a7ec0dea40","last_reissued_at":"2026-05-18T01:06:30.389252Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:30.389252Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9503469","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":"2026-05-18T01:06:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"utvmAoMzxIv73YzZyVrSiQ/VnK7wEj6X/KoMmvDfl793VEdS+faz6RaXggLxmb2BGfrVT95qyGOKpmx33DEbAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T01:01:26.111746Z"},"content_sha256":"7ed97020de2530bcea476e937cc77437439af069af57947eb97ec79a4b21ca43","schema_version":"1.0","event_id":"sha256:7ed97020de2530bcea476e937cc77437439af069af57947eb97ec79a4b21ca43"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1995:5Z4QNR26TOVAC224HKDRXUCXQR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Finite-Temperature Corrections in the Dilated Chiral Quark Model","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Hyun Kyu Lee, Mannque Rho, Youngman Kim","submitted_at":"1995-03-30T15:35:09Z","abstract_excerpt":"We calculate the finite-temperature corrections in the dilated chiral quark model using the effective potential formalism. Assuming that the dilaton limit is applicable at some short length scale, we interpret the results to represent the behavior of hadrons in dense {\\it and} hot matter. We obtain the scaling law, $\\frac{f_{\\pi}(T)}{f_{\\pi}} = \\frac{m_Q (T)}{m_Q}\n \\simeq \\frac{m_{\\sigma}(T)}{m_{\\sigma}}$ while we argue, using PCAC, that pion mass does not scale within the temperature range involved in our Lagrangian. It is found that the hadron masses and the pion decay constant drop faster w"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9503469","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":"2026-05-18T01:06:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zMBUD7G7qoYBu0GW8lb5PVgQvo3RA1g/jYn9n56d3L58U8CIP0/oyNNHcLcCXPBkUpyP2Mt2Xd1ypo4hmzn3Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T01:01:26.112282Z"},"content_sha256":"9926c5f35749738d80833bf2471b42d12e004488d23ae5b9e4d589087fae0f2f","schema_version":"1.0","event_id":"sha256:9926c5f35749738d80833bf2471b42d12e004488d23ae5b9e4d589087fae0f2f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5Z4QNR26TOVAC224HKDRXUCXQR/bundle.json","state_url":"https://pith.science/pith/5Z4QNR26TOVAC224HKDRXUCXQR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5Z4QNR26TOVAC224HKDRXUCXQR/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":"2026-06-06T01:01:26Z","links":{"resolver":"https://pith.science/pith/5Z4QNR26TOVAC224HKDRXUCXQR","bundle":"https://pith.science/pith/5Z4QNR26TOVAC224HKDRXUCXQR/bundle.json","state":"https://pith.science/pith/5Z4QNR26TOVAC224HKDRXUCXQR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5Z4QNR26TOVAC224HKDRXUCXQR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1995:5Z4QNR26TOVAC224HKDRXUCXQR","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":"1b0144736de8beb60e15d0b0bf0bb5ba1d360c8d06b44655066a7ebe5e9b5f55","cross_cats_sorted":["nucl-th"],"license":"","primary_cat":"hep-ph","submitted_at":"1995-03-30T15:35:09Z","title_canon_sha256":"a683f1da68ff012bc83eded19aef439f207954fb613ee23120284a10ec11fd00"},"schema_version":"1.0","source":{"id":"hep-ph/9503469","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9503469","created_at":"2026-05-18T01:06:30Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9503469v1","created_at":"2026-05-18T01:06:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9503469","created_at":"2026-05-18T01:06:30Z"},{"alias_kind":"pith_short_12","alias_value":"5Z4QNR26TOVA","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"5Z4QNR26TOVAC224","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"5Z4QNR26","created_at":"2026-05-18T12:25:47Z"}],"graph_snapshots":[{"event_id":"sha256:9926c5f35749738d80833bf2471b42d12e004488d23ae5b9e4d589087fae0f2f","target":"graph","created_at":"2026-05-18T01:06:30Z","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 calculate the finite-temperature corrections in the dilated chiral quark model using the effective potential formalism. Assuming that the dilaton limit is applicable at some short length scale, we interpret the results to represent the behavior of hadrons in dense {\\it and} hot matter. We obtain the scaling law, $\\frac{f_{\\pi}(T)}{f_{\\pi}} = \\frac{m_Q (T)}{m_Q}\n \\simeq \\frac{m_{\\sigma}(T)}{m_{\\sigma}}$ while we argue, using PCAC, that pion mass does not scale within the temperature range involved in our Lagrangian. It is found that the hadron masses and the pion decay constant drop faster w","authors_text":"Hyun Kyu Lee, Mannque Rho, Youngman Kim","cross_cats":["nucl-th"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1995-03-30T15:35:09Z","title":"Finite-Temperature Corrections in the Dilated Chiral Quark Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9503469","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":"sha256:7ed97020de2530bcea476e937cc77437439af069af57947eb97ec79a4b21ca43","target":"record","created_at":"2026-05-18T01:06:30Z","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":"1b0144736de8beb60e15d0b0bf0bb5ba1d360c8d06b44655066a7ebe5e9b5f55","cross_cats_sorted":["nucl-th"],"license":"","primary_cat":"hep-ph","submitted_at":"1995-03-30T15:35:09Z","title_canon_sha256":"a683f1da68ff012bc83eded19aef439f207954fb613ee23120284a10ec11fd00"},"schema_version":"1.0","source":{"id":"hep-ph/9503469","kind":"arxiv","version":1}},"canonical_sha256":"ee7906c75e9baa016b5c3a871bd057847c3197c7feedd8f880f544a7ec0dea40","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ee7906c75e9baa016b5c3a871bd057847c3197c7feedd8f880f544a7ec0dea40","first_computed_at":"2026-05-18T01:06:30.389252Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:06:30.389252Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"O1CXThSTncljt3qHWQ5M+Rbjhu4qOPl9d/87u+R9nEnEFRpT7H93ii/ZY+5qslNVwf9VpQLGjCugi3eglMnlBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:06:30.389909Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9503469","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7ed97020de2530bcea476e937cc77437439af069af57947eb97ec79a4b21ca43","sha256:9926c5f35749738d80833bf2471b42d12e004488d23ae5b9e4d589087fae0f2f"],"state_sha256":"05de3660c540b88b12b5746176f44a0e9115844e33e3582ca62853cd6ffb2f28"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WAdiVHi/HaXAmmJfN8CBA2kNVJuis9lu+a2hHqkeuQmfSw63dNidNPN4ac+ZBaBsXOfg5jidxmg53/EVWqWfDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T01:01:26.115589Z","bundle_sha256":"7885b345c049e4d89253e2710811b6d7d51b0ee6bc90e3ec1cde805b62f41e26"}}