{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:FMDIYTEV3MRNGGRNSATMFF4JMR","short_pith_number":"pith:FMDIYTEV","canonical_record":{"source":{"id":"1210.6583","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-24T15:53:51Z","cross_cats_sorted":["nucl-ex","nucl-th"],"title_canon_sha256":"c4f04ed421610721b76093cc10652527dfd42233beafb812f8e98a600d7b72ee","abstract_canon_sha256":"bfe689c6667aa2705aca9f50a99a2fbefbfe08da531d539af8d993a48fafd902"},"schema_version":"1.0"},"canonical_sha256":"2b068c4c95db22d31a2d9026c29789645b605a015c1c4ef6f08b098be0afbbaa","source":{"kind":"arxiv","id":"1210.6583","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.6583","created_at":"2026-05-18T01:53:43Z"},{"alias_kind":"arxiv_version","alias_value":"1210.6583v1","created_at":"2026-05-18T01:53:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.6583","created_at":"2026-05-18T01:53:43Z"},{"alias_kind":"pith_short_12","alias_value":"FMDIYTEV3MRN","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_16","alias_value":"FMDIYTEV3MRNGGRN","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_8","alias_value":"FMDIYTEV","created_at":"2026-05-18T12:27:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:FMDIYTEV3MRNGGRNSATMFF4JMR","target":"record","payload":{"canonical_record":{"source":{"id":"1210.6583","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-24T15:53:51Z","cross_cats_sorted":["nucl-ex","nucl-th"],"title_canon_sha256":"c4f04ed421610721b76093cc10652527dfd42233beafb812f8e98a600d7b72ee","abstract_canon_sha256":"bfe689c6667aa2705aca9f50a99a2fbefbfe08da531d539af8d993a48fafd902"},"schema_version":"1.0"},"canonical_sha256":"2b068c4c95db22d31a2d9026c29789645b605a015c1c4ef6f08b098be0afbbaa","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:53:43.639749Z","signature_b64":"YKuMFUH+SO1zLf82sk5fvzzk8j6tky+4kSu8QDpjPEXrxLyaZ5Yzg/G8krq5FLprp729Ye4awT7u1EghTUdvAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2b068c4c95db22d31a2d9026c29789645b605a015c1c4ef6f08b098be0afbbaa","last_reissued_at":"2026-05-18T01:53:43.639174Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:53:43.639174Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1210.6583","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":"2026-05-18T01:53:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"z71TUAbM8ld3t3OyBiPXqohifizpTKvBXql2wg3gEbZjU/mtyNrS/Z7Y+YvSSiMxH883kIaDkMkiyPoVffVdDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T09:30:03.772129Z"},"content_sha256":"34a05038c4ca74f4e83eb32ef412860c3866803fbba7499ff00f91b1668851ff","schema_version":"1.0","event_id":"sha256:34a05038c4ca74f4e83eb32ef412860c3866803fbba7499ff00f91b1668851ff"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:FMDIYTEV3MRNGGRNSATMFF4JMR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"In-Medium Quarkonia at SPS, RHIC and LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Andrew Emerick, Ralf Rapp, Xingbo Zhao","submitted_at":"2012-10-24T15:53:51Z","abstract_excerpt":"A kinetic-rate equation approach in a thermally expanding medium is employed to calculate the evolution of charmonium and bottomonium distributions in heavy-ion collisions. The equilibrium properties of the quarkonia are taken from in-medium spectral functions which are schematically constrained by euclidean correlators from lattice QCD. The initial conditions for the rate equation (heavy-flavor cross sections, nuclear absorption) and the thermal evolution are constrained by data as available. After fixing two free parameters to describe charmonium data at SPS and RHIC, the predictions for LHC"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.6583","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":"2026-05-18T01:53:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HTK4A8ebIn3D8E1Q2eMSMf5ri46qRhMMhlCG1oywdQ+HeE1j257JxXPXsF5/j3qmsicT5Spe67gXpo+84cfiBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T09:30:03.772814Z"},"content_sha256":"e3c5244381167d166b8a2ac7a0d10eead870321d71567ba69ddfe13233b1bc58","schema_version":"1.0","event_id":"sha256:e3c5244381167d166b8a2ac7a0d10eead870321d71567ba69ddfe13233b1bc58"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FMDIYTEV3MRNGGRNSATMFF4JMR/bundle.json","state_url":"https://pith.science/pith/FMDIYTEV3MRNGGRNSATMFF4JMR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FMDIYTEV3MRNGGRNSATMFF4JMR/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":"2026-06-09T09:30:03Z","links":{"resolver":"https://pith.science/pith/FMDIYTEV3MRNGGRNSATMFF4JMR","bundle":"https://pith.science/pith/FMDIYTEV3MRNGGRNSATMFF4JMR/bundle.json","state":"https://pith.science/pith/FMDIYTEV3MRNGGRNSATMFF4JMR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FMDIYTEV3MRNGGRNSATMFF4JMR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:FMDIYTEV3MRNGGRNSATMFF4JMR","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":"bfe689c6667aa2705aca9f50a99a2fbefbfe08da531d539af8d993a48fafd902","cross_cats_sorted":["nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-24T15:53:51Z","title_canon_sha256":"c4f04ed421610721b76093cc10652527dfd42233beafb812f8e98a600d7b72ee"},"schema_version":"1.0","source":{"id":"1210.6583","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.6583","created_at":"2026-05-18T01:53:43Z"},{"alias_kind":"arxiv_version","alias_value":"1210.6583v1","created_at":"2026-05-18T01:53:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.6583","created_at":"2026-05-18T01:53:43Z"},{"alias_kind":"pith_short_12","alias_value":"FMDIYTEV3MRN","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_16","alias_value":"FMDIYTEV3MRNGGRN","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_8","alias_value":"FMDIYTEV","created_at":"2026-05-18T12:27:06Z"}],"graph_snapshots":[{"event_id":"sha256:e3c5244381167d166b8a2ac7a0d10eead870321d71567ba69ddfe13233b1bc58","target":"graph","created_at":"2026-05-18T01:53:43Z","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":"A kinetic-rate equation approach in a thermally expanding medium is employed to calculate the evolution of charmonium and bottomonium distributions in heavy-ion collisions. The equilibrium properties of the quarkonia are taken from in-medium spectral functions which are schematically constrained by euclidean correlators from lattice QCD. The initial conditions for the rate equation (heavy-flavor cross sections, nuclear absorption) and the thermal evolution are constrained by data as available. After fixing two free parameters to describe charmonium data at SPS and RHIC, the predictions for LHC","authors_text":"Andrew Emerick, Ralf Rapp, Xingbo Zhao","cross_cats":["nucl-ex","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-24T15:53:51Z","title":"In-Medium Quarkonia at SPS, RHIC and LHC"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.6583","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":"sha256:34a05038c4ca74f4e83eb32ef412860c3866803fbba7499ff00f91b1668851ff","target":"record","created_at":"2026-05-18T01:53:43Z","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":"bfe689c6667aa2705aca9f50a99a2fbefbfe08da531d539af8d993a48fafd902","cross_cats_sorted":["nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-24T15:53:51Z","title_canon_sha256":"c4f04ed421610721b76093cc10652527dfd42233beafb812f8e98a600d7b72ee"},"schema_version":"1.0","source":{"id":"1210.6583","kind":"arxiv","version":1}},"canonical_sha256":"2b068c4c95db22d31a2d9026c29789645b605a015c1c4ef6f08b098be0afbbaa","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2b068c4c95db22d31a2d9026c29789645b605a015c1c4ef6f08b098be0afbbaa","first_computed_at":"2026-05-18T01:53:43.639174Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:53:43.639174Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"YKuMFUH+SO1zLf82sk5fvzzk8j6tky+4kSu8QDpjPEXrxLyaZ5Yzg/G8krq5FLprp729Ye4awT7u1EghTUdvAA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:53:43.639749Z","signed_message":"canonical_sha256_bytes"},"source_id":"1210.6583","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:34a05038c4ca74f4e83eb32ef412860c3866803fbba7499ff00f91b1668851ff","sha256:e3c5244381167d166b8a2ac7a0d10eead870321d71567ba69ddfe13233b1bc58"],"state_sha256":"e351b5a72f9a50c80c6d6202d710c376c9a9c121a9d97a6b877ab1ece36fa919"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oZUeW1kRkQ98mGgSEd/7KTtgf78in34SEQCqYZLCbVeL4SDMCPoDa11GOm8Kqw0ZTU2SRKttnSLRthdx2njKDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T09:30:03.776246Z","bundle_sha256":"f9371384a4c5672be45babacdbebe3b1a9fa7a2e7bb2ee7844b6448346d6e797"}}