{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2002:XYGLFLZN5IPEES4WXXZFTX7WQ4","short_pith_number":"pith:XYGLFLZN","canonical_record":{"source":{"id":"hep-ph/0204132","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-04-11T20:58:39Z","cross_cats_sorted":["astro-ph","nucl-th"],"title_canon_sha256":"03ae3f8dec2769a4e4ba9517f31bdd00d2cd09b0f564eb30cc0f2d563a342e3b","abstract_canon_sha256":"03a9e980bcdb6977c887c0fcac821f32b6fa223d410cd548735ff7a0d5134c8b"},"schema_version":"1.0"},"canonical_sha256":"be0cb2af2dea1e424b96bdf259dff68731b7419cb008573116dcfe063cacd77c","source":{"kind":"arxiv","id":"hep-ph/0204132","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0204132","created_at":"2026-07-04T16:34:04Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0204132v3","created_at":"2026-07-04T16:34:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0204132","created_at":"2026-07-04T16:34:04Z"},{"alias_kind":"pith_short_12","alias_value":"XYGLFLZN5IPE","created_at":"2026-07-04T16:34:04Z"},{"alias_kind":"pith_short_16","alias_value":"XYGLFLZN5IPEES4W","created_at":"2026-07-04T16:34:04Z"},{"alias_kind":"pith_short_8","alias_value":"XYGLFLZN","created_at":"2026-07-04T16:34:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2002:XYGLFLZN5IPEES4WXXZFTX7WQ4","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0204132","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-04-11T20:58:39Z","cross_cats_sorted":["astro-ph","nucl-th"],"title_canon_sha256":"03ae3f8dec2769a4e4ba9517f31bdd00d2cd09b0f564eb30cc0f2d563a342e3b","abstract_canon_sha256":"03a9e980bcdb6977c887c0fcac821f32b6fa223d410cd548735ff7a0d5134c8b"},"schema_version":"1.0"},"canonical_sha256":"be0cb2af2dea1e424b96bdf259dff68731b7419cb008573116dcfe063cacd77c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:34:04.254766Z","signature_b64":"gIpOqAdVkyD2afsmbgaA1fWzYywCL4r4xglVHNV3GZCt9KIM44Rf6SsdH4NKQbtGWlt/SF5rl2kRZU64RsPZBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"be0cb2af2dea1e424b96bdf259dff68731b7419cb008573116dcfe063cacd77c","last_reissued_at":"2026-07-04T16:34:04.254430Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:34:04.254430Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0204132","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":"2026-07-04T16:34:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2+HvvbEA9YptFdsO7XwyhrSrhQxSKWXVE9FID6nkN7IsYxWMaImxZHWsSFC1hnF35V1MEts87sMZDio4EYKpAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-08T13:38:47.783504Z"},"content_sha256":"ad4440bb8d55e9df67f6f97009b2c7738e81dd63ee244e52ac5b050a037b4978","schema_version":"1.0","event_id":"sha256:ad4440bb8d55e9df67f6f97009b2c7738e81dd63ee244e52ac5b050a037b4978"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2002:XYGLFLZN5IPEES4WXXZFTX7WQ4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Thermal conductivity of dense quark matter and cooling of stars","license":"","headline":"","cross_cats":["astro-ph","nucl-th"],"primary_cat":"hep-ph","authors_text":"Igor A. Shovkovy, Paul J. Ellis","submitted_at":"2002-04-11T20:58:39Z","abstract_excerpt":"The thermal conductivity of the color-flavor locked phase of dense quark matter is calculated. The dominant contribution to the conductivity comes from photons and Nambu-Goldstone bosons associated with breaking of baryon number which are trapped in the quark core. Because of their very large mean free path the conductivity is also very large. The cooling of the quark core arises mostly from the heat flux across the surface of direct contact with the nuclear matter. As the thermal conductivity of the neighboring layer is also high, the whole interior of the star should be nearly isothermal. Ou"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0204132","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/hep-ph/0204132/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":"2026-07-04T16:34:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jEvTv6miWyNnhXpEJv8anGy8kzLCAVCyYlVWjFClRcE2cLqUn8tB/20CnAqmSIwUnfJmk0Rbma/dBKNET/p0CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-08T13:38:47.784457Z"},"content_sha256":"5c2f0c0c2a335606175a62ba49360d429762092ba0260ea2e5c43e5c1879c284","schema_version":"1.0","event_id":"sha256:5c2f0c0c2a335606175a62ba49360d429762092ba0260ea2e5c43e5c1879c284"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XYGLFLZN5IPEES4WXXZFTX7WQ4/bundle.json","state_url":"https://pith.science/pith/XYGLFLZN5IPEES4WXXZFTX7WQ4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XYGLFLZN5IPEES4WXXZFTX7WQ4/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":"2026-08-08T13:38:47Z","links":{"resolver":"https://pith.science/pith/XYGLFLZN5IPEES4WXXZFTX7WQ4","bundle":"https://pith.science/pith/XYGLFLZN5IPEES4WXXZFTX7WQ4/bundle.json","state":"https://pith.science/pith/XYGLFLZN5IPEES4WXXZFTX7WQ4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XYGLFLZN5IPEES4WXXZFTX7WQ4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:XYGLFLZN5IPEES4WXXZFTX7WQ4","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":"03a9e980bcdb6977c887c0fcac821f32b6fa223d410cd548735ff7a0d5134c8b","cross_cats_sorted":["astro-ph","nucl-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2002-04-11T20:58:39Z","title_canon_sha256":"03ae3f8dec2769a4e4ba9517f31bdd00d2cd09b0f564eb30cc0f2d563a342e3b"},"schema_version":"1.0","source":{"id":"hep-ph/0204132","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0204132","created_at":"2026-07-04T16:34:04Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0204132v3","created_at":"2026-07-04T16:34:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0204132","created_at":"2026-07-04T16:34:04Z"},{"alias_kind":"pith_short_12","alias_value":"XYGLFLZN5IPE","created_at":"2026-07-04T16:34:04Z"},{"alias_kind":"pith_short_16","alias_value":"XYGLFLZN5IPEES4W","created_at":"2026-07-04T16:34:04Z"},{"alias_kind":"pith_short_8","alias_value":"XYGLFLZN","created_at":"2026-07-04T16:34:04Z"}],"graph_snapshots":[{"event_id":"sha256:5c2f0c0c2a335606175a62ba49360d429762092ba0260ea2e5c43e5c1879c284","target":"graph","created_at":"2026-07-04T16:34:04Z","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/0204132/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The thermal conductivity of the color-flavor locked phase of dense quark matter is calculated. The dominant contribution to the conductivity comes from photons and Nambu-Goldstone bosons associated with breaking of baryon number which are trapped in the quark core. Because of their very large mean free path the conductivity is also very large. The cooling of the quark core arises mostly from the heat flux across the surface of direct contact with the nuclear matter. As the thermal conductivity of the neighboring layer is also high, the whole interior of the star should be nearly isothermal. Ou","authors_text":"Igor A. Shovkovy, Paul J. Ellis","cross_cats":["astro-ph","nucl-th"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2002-04-11T20:58:39Z","title":"Thermal conductivity of dense quark matter and cooling of stars"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0204132","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:ad4440bb8d55e9df67f6f97009b2c7738e81dd63ee244e52ac5b050a037b4978","target":"record","created_at":"2026-07-04T16:34:04Z","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":"03a9e980bcdb6977c887c0fcac821f32b6fa223d410cd548735ff7a0d5134c8b","cross_cats_sorted":["astro-ph","nucl-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2002-04-11T20:58:39Z","title_canon_sha256":"03ae3f8dec2769a4e4ba9517f31bdd00d2cd09b0f564eb30cc0f2d563a342e3b"},"schema_version":"1.0","source":{"id":"hep-ph/0204132","kind":"arxiv","version":3}},"canonical_sha256":"be0cb2af2dea1e424b96bdf259dff68731b7419cb008573116dcfe063cacd77c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"be0cb2af2dea1e424b96bdf259dff68731b7419cb008573116dcfe063cacd77c","first_computed_at":"2026-07-04T16:34:04.254430Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:34:04.254430Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gIpOqAdVkyD2afsmbgaA1fWzYywCL4r4xglVHNV3GZCt9KIM44Rf6SsdH4NKQbtGWlt/SF5rl2kRZU64RsPZBA==","signature_status":"signed_v1","signed_at":"2026-07-04T16:34:04.254766Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0204132","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ad4440bb8d55e9df67f6f97009b2c7738e81dd63ee244e52ac5b050a037b4978","sha256:5c2f0c0c2a335606175a62ba49360d429762092ba0260ea2e5c43e5c1879c284"],"state_sha256":"22bd59c0c62162878a6335a43d854d0bc52c20b9940dd00bcbff3dfbf88904e6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"P/RkokQBfmsdIBITwC+xHGBPB3KIcLThYAbCneeRjHEr6VBnxDL70HgN2rUS23NNjpFN3628qwUiwup2ZArSBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-08T13:38:47.790187Z","bundle_sha256":"53a82b916af88c01b98451c69b8d0fbf869055251a95951533d6f55146c42329"}}