{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2001:WH2XMX7DM2B6NZQ2VLBAQXPO2Z","short_pith_number":"pith:WH2XMX7D","canonical_record":{"source":{"id":"hep-th/0106219","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2001-06-25T10:33:28Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"48c4b8442363aac36671de2c0e7a78c3669677c83d76aad667d3560fc1b0cc8a","abstract_canon_sha256":"3d260effac609312719f5d4bf494e955374709662536429d966c09117fac7811"},"schema_version":"1.0"},"canonical_sha256":"b1f5765fe36683e6e61aaac2085deed6533c16b712583695262b2bb892422e24","source":{"kind":"arxiv","id":"hep-th/0106219","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0106219","created_at":"2026-07-04T16:27:55Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0106219v1","created_at":"2026-07-04T16:27:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0106219","created_at":"2026-07-04T16:27:55Z"},{"alias_kind":"pith_short_12","alias_value":"WH2XMX7DM2B6","created_at":"2026-07-04T16:27:55Z"},{"alias_kind":"pith_short_16","alias_value":"WH2XMX7DM2B6NZQ2","created_at":"2026-07-04T16:27:55Z"},{"alias_kind":"pith_short_8","alias_value":"WH2XMX7D","created_at":"2026-07-04T16:27:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2001:WH2XMX7DM2B6NZQ2VLBAQXPO2Z","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0106219","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2001-06-25T10:33:28Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"48c4b8442363aac36671de2c0e7a78c3669677c83d76aad667d3560fc1b0cc8a","abstract_canon_sha256":"3d260effac609312719f5d4bf494e955374709662536429d966c09117fac7811"},"schema_version":"1.0"},"canonical_sha256":"b1f5765fe36683e6e61aaac2085deed6533c16b712583695262b2bb892422e24","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:27:55.303671Z","signature_b64":"7WiSgWkrmY09chMSUrk45HZqS0R5RYUEWrMCoej06xJYt1FHscaAc2XpbBFZZEwVrLPfQbpAOBr7tqq6frKkAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b1f5765fe36683e6e61aaac2085deed6533c16b712583695262b2bb892422e24","last_reissued_at":"2026-07-04T16:27:55.303280Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:27:55.303280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0106219","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":"2026-07-04T16:27:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vIDxTslzz6xpYbKEFkmy52FaWZvafIudWhSiqdxUptWzMohSorvEJav7Ck72DHoVan1b7wL/LPUxehoDC/xMBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T21:22:36.534830Z"},"content_sha256":"19e81b09d5487d9090bdbdcb53b8ecbd70745cf96e71f1c0a06df0ddca1ed073","schema_version":"1.0","event_id":"sha256:19e81b09d5487d9090bdbdcb53b8ecbd70745cf96e71f1c0a06df0ddca1ed073"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2001:WH2XMX7DM2B6NZQ2VLBAQXPO2Z","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Three-quark clusters at finite temperatures and densities","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-th","authors_text":"H.J. Weber (U Virginia), Inst. Tech. Aeronautics), M. Beyer (U Rostock), S. Mattiello (U Rostock), T. Frederico (Sao Paulo","submitted_at":"2001-06-25T10:33:28Z","abstract_excerpt":"We present a relativistic three-body equation to study correlations in a medium of finite temperatures and densities. This equation is derived within a systematic Dyson equation approach and includes the dominant medium effects due to Pauli blocking and self energy corrections. Relativity is implemented utilizing the light front form. The equation is solved for a zero-range force for parameters close to the confinement-deconfinement transition of QCD. We present correlations between two- and three-particle binding energies and calculate the three-body Mott transition."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0106219","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-th/0106219/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":"2026-07-04T16:27:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JKHNoL0z8d+r5s2JFFtW8iqlDLbtmxlTZhLhx2+DyZ31UdfAtohDKxUZ6/3Frw1Yc5yml2E2crGUKylVmLcuAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T21:22:36.535359Z"},"content_sha256":"c3886f74e06e6928c1d57e21df9a21276a89c0618303da9cdf7a13c4745ca127","schema_version":"1.0","event_id":"sha256:c3886f74e06e6928c1d57e21df9a21276a89c0618303da9cdf7a13c4745ca127"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WH2XMX7DM2B6NZQ2VLBAQXPO2Z/bundle.json","state_url":"https://pith.science/pith/WH2XMX7DM2B6NZQ2VLBAQXPO2Z/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WH2XMX7DM2B6NZQ2VLBAQXPO2Z/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":"2026-08-04T21:22:36Z","links":{"resolver":"https://pith.science/pith/WH2XMX7DM2B6NZQ2VLBAQXPO2Z","bundle":"https://pith.science/pith/WH2XMX7DM2B6NZQ2VLBAQXPO2Z/bundle.json","state":"https://pith.science/pith/WH2XMX7DM2B6NZQ2VLBAQXPO2Z/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WH2XMX7DM2B6NZQ2VLBAQXPO2Z/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2001:WH2XMX7DM2B6NZQ2VLBAQXPO2Z","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":"3d260effac609312719f5d4bf494e955374709662536429d966c09117fac7811","cross_cats_sorted":["nucl-th"],"license":"","primary_cat":"hep-th","submitted_at":"2001-06-25T10:33:28Z","title_canon_sha256":"48c4b8442363aac36671de2c0e7a78c3669677c83d76aad667d3560fc1b0cc8a"},"schema_version":"1.0","source":{"id":"hep-th/0106219","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0106219","created_at":"2026-07-04T16:27:55Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0106219v1","created_at":"2026-07-04T16:27:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0106219","created_at":"2026-07-04T16:27:55Z"},{"alias_kind":"pith_short_12","alias_value":"WH2XMX7DM2B6","created_at":"2026-07-04T16:27:55Z"},{"alias_kind":"pith_short_16","alias_value":"WH2XMX7DM2B6NZQ2","created_at":"2026-07-04T16:27:55Z"},{"alias_kind":"pith_short_8","alias_value":"WH2XMX7D","created_at":"2026-07-04T16:27:55Z"}],"graph_snapshots":[{"event_id":"sha256:c3886f74e06e6928c1d57e21df9a21276a89c0618303da9cdf7a13c4745ca127","target":"graph","created_at":"2026-07-04T16:27:55Z","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-th/0106219/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present a relativistic three-body equation to study correlations in a medium of finite temperatures and densities. This equation is derived within a systematic Dyson equation approach and includes the dominant medium effects due to Pauli blocking and self energy corrections. Relativity is implemented utilizing the light front form. The equation is solved for a zero-range force for parameters close to the confinement-deconfinement transition of QCD. We present correlations between two- and three-particle binding energies and calculate the three-body Mott transition.","authors_text":"H.J. Weber (U Virginia), Inst. Tech. Aeronautics), M. Beyer (U Rostock), S. Mattiello (U Rostock), T. Frederico (Sao Paulo","cross_cats":["nucl-th"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2001-06-25T10:33:28Z","title":"Three-quark clusters at finite temperatures and densities"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0106219","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":"sha256:19e81b09d5487d9090bdbdcb53b8ecbd70745cf96e71f1c0a06df0ddca1ed073","target":"record","created_at":"2026-07-04T16:27:55Z","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":"3d260effac609312719f5d4bf494e955374709662536429d966c09117fac7811","cross_cats_sorted":["nucl-th"],"license":"","primary_cat":"hep-th","submitted_at":"2001-06-25T10:33:28Z","title_canon_sha256":"48c4b8442363aac36671de2c0e7a78c3669677c83d76aad667d3560fc1b0cc8a"},"schema_version":"1.0","source":{"id":"hep-th/0106219","kind":"arxiv","version":1}},"canonical_sha256":"b1f5765fe36683e6e61aaac2085deed6533c16b712583695262b2bb892422e24","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b1f5765fe36683e6e61aaac2085deed6533c16b712583695262b2bb892422e24","first_computed_at":"2026-07-04T16:27:55.303280Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:27:55.303280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7WiSgWkrmY09chMSUrk45HZqS0R5RYUEWrMCoej06xJYt1FHscaAc2XpbBFZZEwVrLPfQbpAOBr7tqq6frKkAw==","signature_status":"signed_v1","signed_at":"2026-07-04T16:27:55.303671Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0106219","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:19e81b09d5487d9090bdbdcb53b8ecbd70745cf96e71f1c0a06df0ddca1ed073","sha256:c3886f74e06e6928c1d57e21df9a21276a89c0618303da9cdf7a13c4745ca127"],"state_sha256":"21b343086e5c4761f5a27f39a8dfe23082873d82dde880b005da40f3421e3a49"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rrGjlMmrj+SzITiV8s7FEzq2075N85DzChO40ux94xY8iimVpjXCvIUIpww0SGJx4b3AqIJhqVNnJ9ErFhmmDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T21:22:36.540664Z","bundle_sha256":"65599a67086ecffb2504475eae06951abd3402f127332d8403feee7de129b820"}}