{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:KMAAOQRDZU2XVENP4YVC3Y5UFQ","short_pith_number":"pith:KMAAOQRD","canonical_record":{"source":{"id":"1509.08286","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-28T12:04:12Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"120a5c6f944b8e0187a525353f2c796ef0296a215263dad3fdba619afe34ac5e","abstract_canon_sha256":"980973e64417cd1c7281a37577008f984029460cb8b5c0aa3fb2fc3d387ae825"},"schema_version":"1.0"},"canonical_sha256":"5300074223cd357a91afe62a2de3b42c1ef94ea31ef59a9d3ea983d29c3dd2b9","source":{"kind":"arxiv","id":"1509.08286","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.08286","created_at":"2026-05-18T01:15:44Z"},{"alias_kind":"arxiv_version","alias_value":"1509.08286v1","created_at":"2026-05-18T01:15:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.08286","created_at":"2026-05-18T01:15:44Z"},{"alias_kind":"pith_short_12","alias_value":"KMAAOQRDZU2X","created_at":"2026-05-18T12:29:29Z"},{"alias_kind":"pith_short_16","alias_value":"KMAAOQRDZU2XVENP","created_at":"2026-05-18T12:29:29Z"},{"alias_kind":"pith_short_8","alias_value":"KMAAOQRD","created_at":"2026-05-18T12:29:29Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:KMAAOQRDZU2XVENP4YVC3Y5UFQ","target":"record","payload":{"canonical_record":{"source":{"id":"1509.08286","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-28T12:04:12Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"120a5c6f944b8e0187a525353f2c796ef0296a215263dad3fdba619afe34ac5e","abstract_canon_sha256":"980973e64417cd1c7281a37577008f984029460cb8b5c0aa3fb2fc3d387ae825"},"schema_version":"1.0"},"canonical_sha256":"5300074223cd357a91afe62a2de3b42c1ef94ea31ef59a9d3ea983d29c3dd2b9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:15:44.515501Z","signature_b64":"TiC2CoidsOYPsqEMLCJpLMUxoXj2o00R4hgXY6Ig5ZMO6N9/Jf6W2U5XzsZnU1CoKEGiT3Ye4jy91EVnOKB2AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5300074223cd357a91afe62a2de3b42c1ef94ea31ef59a9d3ea983d29c3dd2b9","last_reissued_at":"2026-05-18T01:15:44.514956Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:15:44.514956Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1509.08286","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":"2026-05-18T01:15:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QH8693GS3forL6g+n9IsRbx0p75jLWpPp4jAd6FvkR3RrO6ZUoptP0Kn1EdAGDKALJ291iZ9yubV2yxa2zJ1Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T14:17:27.181842Z"},"content_sha256":"7edc45a05629ffcd287d31cf0640b43f76570ae033a885fc4a28ed55d7fdf2bc","schema_version":"1.0","event_id":"sha256:7edc45a05629ffcd287d31cf0640b43f76570ae033a885fc4a28ed55d7fdf2bc"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:KMAAOQRDZU2XVENP4YVC3Y5UFQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Holographic entropy and real-time dynamics of quarkonium dissociation in non-Abelian plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Dmitri E. Kharzeev, Ioannis Iatrakis","submitted_at":"2015-09-28T12:04:12Z","abstract_excerpt":"The peak of the heavy quark pair entropy at the deconfinement transition, observed in lattice QCD, suggests that the transition is effectively driven by the increase of the entropy of bound states. The growth of the entropy with the inter-quark distance leads to the emergent entropic force that induces dissociation of quarkonium states. Since the quark-gluon plasma around the transition point is a strongly coupled system, we use the gauge-gravity duality to study the entropy of heavy quarkonium and the real-time dynamics of its dissociation. In particular, we employ the Improved Holographic QC"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.08286","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":"2026-05-18T01:15:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TxgChBlZ2GcxNMk7vAmWMtI64nQzi4ER5lbrDt0N7ZFBYtO+80TkZXolKkV1MwO8E73LgJ41c1GY9dgIYAdVDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T14:17:27.182233Z"},"content_sha256":"1a0105e33537b1dacbaa36a76c852e4779e8dcbd155c9add92bb1f3a8f4e03b1","schema_version":"1.0","event_id":"sha256:1a0105e33537b1dacbaa36a76c852e4779e8dcbd155c9add92bb1f3a8f4e03b1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KMAAOQRDZU2XVENP4YVC3Y5UFQ/bundle.json","state_url":"https://pith.science/pith/KMAAOQRDZU2XVENP4YVC3Y5UFQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KMAAOQRDZU2XVENP4YVC3Y5UFQ/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":"2026-05-30T14:17:27Z","links":{"resolver":"https://pith.science/pith/KMAAOQRDZU2XVENP4YVC3Y5UFQ","bundle":"https://pith.science/pith/KMAAOQRDZU2XVENP4YVC3Y5UFQ/bundle.json","state":"https://pith.science/pith/KMAAOQRDZU2XVENP4YVC3Y5UFQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KMAAOQRDZU2XVENP4YVC3Y5UFQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:KMAAOQRDZU2XVENP4YVC3Y5UFQ","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":"980973e64417cd1c7281a37577008f984029460cb8b5c0aa3fb2fc3d387ae825","cross_cats_sorted":["hep-th","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-28T12:04:12Z","title_canon_sha256":"120a5c6f944b8e0187a525353f2c796ef0296a215263dad3fdba619afe34ac5e"},"schema_version":"1.0","source":{"id":"1509.08286","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.08286","created_at":"2026-05-18T01:15:44Z"},{"alias_kind":"arxiv_version","alias_value":"1509.08286v1","created_at":"2026-05-18T01:15:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.08286","created_at":"2026-05-18T01:15:44Z"},{"alias_kind":"pith_short_12","alias_value":"KMAAOQRDZU2X","created_at":"2026-05-18T12:29:29Z"},{"alias_kind":"pith_short_16","alias_value":"KMAAOQRDZU2XVENP","created_at":"2026-05-18T12:29:29Z"},{"alias_kind":"pith_short_8","alias_value":"KMAAOQRD","created_at":"2026-05-18T12:29:29Z"}],"graph_snapshots":[{"event_id":"sha256:1a0105e33537b1dacbaa36a76c852e4779e8dcbd155c9add92bb1f3a8f4e03b1","target":"graph","created_at":"2026-05-18T01:15:44Z","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":"The peak of the heavy quark pair entropy at the deconfinement transition, observed in lattice QCD, suggests that the transition is effectively driven by the increase of the entropy of bound states. The growth of the entropy with the inter-quark distance leads to the emergent entropic force that induces dissociation of quarkonium states. Since the quark-gluon plasma around the transition point is a strongly coupled system, we use the gauge-gravity duality to study the entropy of heavy quarkonium and the real-time dynamics of its dissociation. In particular, we employ the Improved Holographic QC","authors_text":"Dmitri E. Kharzeev, Ioannis Iatrakis","cross_cats":["hep-th","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-28T12:04:12Z","title":"Holographic entropy and real-time dynamics of quarkonium dissociation in non-Abelian plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.08286","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":"sha256:7edc45a05629ffcd287d31cf0640b43f76570ae033a885fc4a28ed55d7fdf2bc","target":"record","created_at":"2026-05-18T01:15:44Z","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":"980973e64417cd1c7281a37577008f984029460cb8b5c0aa3fb2fc3d387ae825","cross_cats_sorted":["hep-th","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-28T12:04:12Z","title_canon_sha256":"120a5c6f944b8e0187a525353f2c796ef0296a215263dad3fdba619afe34ac5e"},"schema_version":"1.0","source":{"id":"1509.08286","kind":"arxiv","version":1}},"canonical_sha256":"5300074223cd357a91afe62a2de3b42c1ef94ea31ef59a9d3ea983d29c3dd2b9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5300074223cd357a91afe62a2de3b42c1ef94ea31ef59a9d3ea983d29c3dd2b9","first_computed_at":"2026-05-18T01:15:44.514956Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:15:44.514956Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TiC2CoidsOYPsqEMLCJpLMUxoXj2o00R4hgXY6Ig5ZMO6N9/Jf6W2U5XzsZnU1CoKEGiT3Ye4jy91EVnOKB2AA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:15:44.515501Z","signed_message":"canonical_sha256_bytes"},"source_id":"1509.08286","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7edc45a05629ffcd287d31cf0640b43f76570ae033a885fc4a28ed55d7fdf2bc","sha256:1a0105e33537b1dacbaa36a76c852e4779e8dcbd155c9add92bb1f3a8f4e03b1"],"state_sha256":"81509da91fabd20ebbaae44324068da18dfac4a5667e1f0fa1e926d3e078bb8c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NXLk2mNXKhNkUi4xQM2ubDR1g7GErxyWC1hop4MsLvyEWGxTC3RjiHLU5QBNTOClduusp7EIWZkSM4iSci3eAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T14:17:27.184414Z","bundle_sha256":"bd3b3b5fc362861f8a3ac480e092a9284d4a9e221014f8ef1271c903a9a3c163"}}