{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:K3MLLL7SH4TPFAGBE4BRJDFCFK","short_pith_number":"pith:K3MLLL7S","canonical_record":{"source":{"id":"1006.0570","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-06-03T07:45:00Z","cross_cats_sorted":["astro-ph.HE","nucl-th"],"title_canon_sha256":"258e3f1c9917d5da5f11e3a65593d40825b5c353678550ac0a6b134dd64e4e37","abstract_canon_sha256":"18f8a93509a63c97a81c5d205677a74e6095851a588d8c900af2dfc4e30671e7"},"schema_version":"1.0"},"canonical_sha256":"56d8b5aff23f26f280c12703148ca22aad04edbf8a826ac55620ebfdc6f2b7b2","source":{"kind":"arxiv","id":"1006.0570","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1006.0570","created_at":"2026-05-18T04:25:03Z"},{"alias_kind":"arxiv_version","alias_value":"1006.0570v2","created_at":"2026-05-18T04:25:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1006.0570","created_at":"2026-05-18T04:25:03Z"},{"alias_kind":"pith_short_12","alias_value":"K3MLLL7SH4TP","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_16","alias_value":"K3MLLL7SH4TPFAGB","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_8","alias_value":"K3MLLL7S","created_at":"2026-05-18T12:26:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:K3MLLL7SH4TPFAGBE4BRJDFCFK","target":"record","payload":{"canonical_record":{"source":{"id":"1006.0570","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-06-03T07:45:00Z","cross_cats_sorted":["astro-ph.HE","nucl-th"],"title_canon_sha256":"258e3f1c9917d5da5f11e3a65593d40825b5c353678550ac0a6b134dd64e4e37","abstract_canon_sha256":"18f8a93509a63c97a81c5d205677a74e6095851a588d8c900af2dfc4e30671e7"},"schema_version":"1.0"},"canonical_sha256":"56d8b5aff23f26f280c12703148ca22aad04edbf8a826ac55620ebfdc6f2b7b2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:25:03.498770Z","signature_b64":"2NzOZloy88sUpe/Al1e+2hbHd0UUhym8p5D1k1umR3X8a/gwn5QiBroLhLUEtnbBsQbUfnnK8JWae/Qh4SDUBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"56d8b5aff23f26f280c12703148ca22aad04edbf8a826ac55620ebfdc6f2b7b2","last_reissued_at":"2026-05-18T04:25:03.498308Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:25:03.498308Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1006.0570","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:25:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ieYqKsg7SIign+twK5MrdQ7vMpfBRlw3cFzKUGG00WKawSukJgIzY9mLUQfO0MBkugz9PEAof0Jct5f1E2XWBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T02:38:39.349672Z"},"content_sha256":"6d0c885661c53538530687dcddfa8a51ba718eb9fe9b4ff9f90ad470ac7443e5","schema_version":"1.0","event_id":"sha256:6d0c885661c53538530687dcddfa8a51ba718eb9fe9b4ff9f90ad470ac7443e5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:K3MLLL7SH4TPFAGBE4BRJDFCFK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nuclear matter at high density: Phase transitions, multiquark states, and supernova outbursts","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE","nucl-th"],"primary_cat":"hep-ph","authors_text":"A. V. Yudin, D. K. Nadyozhin, M. A. Trusov, M. I. Krivoruchenko, T. L. Rasinkova, Yu. A. Simonov","submitted_at":"2010-06-03T07:45:00Z","abstract_excerpt":"Phase transition from hadronic matter to quark-gluon matter is discussed for various regimes of temperature and baryon number density. For small and medium densities, the phase transition is accurately described in the framework of the Field Correlation Method, whereas at high density predictions are less certain and leave room for the phenomenological models. We study formation of multiquark states (MQS) at zero temperature and high density. Relevant MQS components of the nuclear matter can be described using a previously developed formalism of the quark compound bags (QCB).\n  Partial-wave an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1006.0570","kind":"arxiv","version":2},"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":"2026-05-18T04:25:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nBEjSSaN0FInpKq5mJkOcAt7orIkiqyCbPbbNe86k3p+npU5dTz2ujzE58CL213eqoN7i7jyOMchnQ8kFKR5AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T02:38:39.350292Z"},"content_sha256":"50983c4064d8f36f429964844e1e6bb07c082febcbabb90f29ff558b1ebbbded","schema_version":"1.0","event_id":"sha256:50983c4064d8f36f429964844e1e6bb07c082febcbabb90f29ff558b1ebbbded"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/K3MLLL7SH4TPFAGBE4BRJDFCFK/bundle.json","state_url":"https://pith.science/pith/K3MLLL7SH4TPFAGBE4BRJDFCFK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/K3MLLL7SH4TPFAGBE4BRJDFCFK/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":"2026-06-01T02:38:39Z","links":{"resolver":"https://pith.science/pith/K3MLLL7SH4TPFAGBE4BRJDFCFK","bundle":"https://pith.science/pith/K3MLLL7SH4TPFAGBE4BRJDFCFK/bundle.json","state":"https://pith.science/pith/K3MLLL7SH4TPFAGBE4BRJDFCFK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/K3MLLL7SH4TPFAGBE4BRJDFCFK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:K3MLLL7SH4TPFAGBE4BRJDFCFK","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":"18f8a93509a63c97a81c5d205677a74e6095851a588d8c900af2dfc4e30671e7","cross_cats_sorted":["astro-ph.HE","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-06-03T07:45:00Z","title_canon_sha256":"258e3f1c9917d5da5f11e3a65593d40825b5c353678550ac0a6b134dd64e4e37"},"schema_version":"1.0","source":{"id":"1006.0570","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1006.0570","created_at":"2026-05-18T04:25:03Z"},{"alias_kind":"arxiv_version","alias_value":"1006.0570v2","created_at":"2026-05-18T04:25:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1006.0570","created_at":"2026-05-18T04:25:03Z"},{"alias_kind":"pith_short_12","alias_value":"K3MLLL7SH4TP","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_16","alias_value":"K3MLLL7SH4TPFAGB","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_8","alias_value":"K3MLLL7S","created_at":"2026-05-18T12:26:09Z"}],"graph_snapshots":[{"event_id":"sha256:50983c4064d8f36f429964844e1e6bb07c082febcbabb90f29ff558b1ebbbded","target":"graph","created_at":"2026-05-18T04:25:03Z","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":"Phase transition from hadronic matter to quark-gluon matter is discussed for various regimes of temperature and baryon number density. For small and medium densities, the phase transition is accurately described in the framework of the Field Correlation Method, whereas at high density predictions are less certain and leave room for the phenomenological models. We study formation of multiquark states (MQS) at zero temperature and high density. Relevant MQS components of the nuclear matter can be described using a previously developed formalism of the quark compound bags (QCB).\n  Partial-wave an","authors_text":"A. V. Yudin, D. K. Nadyozhin, M. A. Trusov, M. I. Krivoruchenko, T. L. Rasinkova, Yu. A. Simonov","cross_cats":["astro-ph.HE","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-06-03T07:45:00Z","title":"Nuclear matter at high density: Phase transitions, multiquark states, and supernova outbursts"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1006.0570","kind":"arxiv","version":2},"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":"sha256:6d0c885661c53538530687dcddfa8a51ba718eb9fe9b4ff9f90ad470ac7443e5","target":"record","created_at":"2026-05-18T04:25:03Z","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":"18f8a93509a63c97a81c5d205677a74e6095851a588d8c900af2dfc4e30671e7","cross_cats_sorted":["astro-ph.HE","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-06-03T07:45:00Z","title_canon_sha256":"258e3f1c9917d5da5f11e3a65593d40825b5c353678550ac0a6b134dd64e4e37"},"schema_version":"1.0","source":{"id":"1006.0570","kind":"arxiv","version":2}},"canonical_sha256":"56d8b5aff23f26f280c12703148ca22aad04edbf8a826ac55620ebfdc6f2b7b2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"56d8b5aff23f26f280c12703148ca22aad04edbf8a826ac55620ebfdc6f2b7b2","first_computed_at":"2026-05-18T04:25:03.498308Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:25:03.498308Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2NzOZloy88sUpe/Al1e+2hbHd0UUhym8p5D1k1umR3X8a/gwn5QiBroLhLUEtnbBsQbUfnnK8JWae/Qh4SDUBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:25:03.498770Z","signed_message":"canonical_sha256_bytes"},"source_id":"1006.0570","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6d0c885661c53538530687dcddfa8a51ba718eb9fe9b4ff9f90ad470ac7443e5","sha256:50983c4064d8f36f429964844e1e6bb07c082febcbabb90f29ff558b1ebbbded"],"state_sha256":"8ad45995c2c192a3df62b3334976f75005a4332187236a3497fb990d20e767c8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"a9h0m7bF0cP7kGBEVepDslyXDCyHr5ddF+ltlY5jGC2V6DUJTG/Di6IfYXP/Ox4CsCOGoiy9bLcoWFMZ1WiHBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T02:38:39.354008Z","bundle_sha256":"c423d02bb1510b816629a45628dcd33b45c97ed7b07bc319d6ce413a10c554a6"}}