{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:C2YQECQ5WIDM6FLNNKHYTUFEF4","short_pith_number":"pith:C2YQECQ5","canonical_record":{"source":{"id":"2206.15471","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-06-30T17:58:36Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"title_canon_sha256":"9978caa9c8f41e79c1550d6b3b9e19231c1759c00f69c9b507982f4cfa366fff","abstract_canon_sha256":"25a99ec8609007545515b627c8ea95fce740af9017ead57e6d7d7aad7e143e15"},"schema_version":"1.0"},"canonical_sha256":"16b1020a1db206cf156d6a8f89d0a42f354c900e3621c114747c431987aac1c5","source":{"kind":"arxiv","id":"2206.15471","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2206.15471","created_at":"2026-07-05T06:38:26Z"},{"alias_kind":"arxiv_version","alias_value":"2206.15471v2","created_at":"2026-07-05T06:38:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.15471","created_at":"2026-07-05T06:38:26Z"},{"alias_kind":"pith_short_12","alias_value":"C2YQECQ5WIDM","created_at":"2026-07-05T06:38:26Z"},{"alias_kind":"pith_short_16","alias_value":"C2YQECQ5WIDM6FLN","created_at":"2026-07-05T06:38:26Z"},{"alias_kind":"pith_short_8","alias_value":"C2YQECQ5","created_at":"2026-07-05T06:38:26Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:C2YQECQ5WIDM6FLNNKHYTUFEF4","target":"record","payload":{"canonical_record":{"source":{"id":"2206.15471","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-06-30T17:58:36Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"title_canon_sha256":"9978caa9c8f41e79c1550d6b3b9e19231c1759c00f69c9b507982f4cfa366fff","abstract_canon_sha256":"25a99ec8609007545515b627c8ea95fce740af9017ead57e6d7d7aad7e143e15"},"schema_version":"1.0"},"canonical_sha256":"16b1020a1db206cf156d6a8f89d0a42f354c900e3621c114747c431987aac1c5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:38:26.423243Z","signature_b64":"YOge7BFSE3MZiEnhzkhzCZCfsdQv8FD+DQRgDUJutWwOX5NjayPlthEcps9kPJUT0kw4Xb7sdTVaSpVFHtEvDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"16b1020a1db206cf156d6a8f89d0a42f354c900e3621c114747c431987aac1c5","last_reissued_at":"2026-07-05T06:38:26.422760Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:38:26.422760Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2206.15471","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":"2026-07-05T06:38:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yj9NSVJwuOZCmnj6q4+Ufb/pXcCWKcRAzwLyW/iiIpkUpu/GfuV7ezXGesN+L4UpUNPPouNHdTlU/l4HOqxLDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T17:00:18.856944Z"},"content_sha256":"47a95bcb5255f247a3dc6be9b7d8536fdc3bbdd7061636542ea8a8da7e3d311e","schema_version":"1.0","event_id":"sha256:47a95bcb5255f247a3dc6be9b7d8536fdc3bbdd7061636542ea8a8da7e3d311e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:C2YQECQ5WIDM6FLNNKHYTUFEF4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Temperature dependence of the static quark diffusion coefficient","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Debasish Banerjee, Pushan Majumdar, Rajiv Gavai, Saumen Datta","submitted_at":"2022-06-30T17:58:36Z","abstract_excerpt":"The energy loss pattern of a low momentum heavy quark in a deconfined quark-gluon plasma can be understood in terms of a Langevin description. In thermal equilibrium, the motion can then be parametrized in terms of a single heavy quark momentum diffusion coefficient kappa, which needs to be determined nonperturbatively. In this work, we study the temperature dependence of kappa for a static quark in a gluonic plasma, with a particular emphasis on the temperature range of interest for heavy ion collision experiments."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.15471","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2206.15471/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":"2026-07-05T06:38:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZVgUdOOOCi7TZvJCLyuApMW1QDN2VBusMsXGxVQ1WJoIvxMt7VWFLtFnnY3mUYR1B/uCizOo0++G+6MTdFWJCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T17:00:18.857515Z"},"content_sha256":"77ecf495c4a33331fedbc6440f6bc565d603ccbaecf1d01aa9aaf88110831c6c","schema_version":"1.0","event_id":"sha256:77ecf495c4a33331fedbc6440f6bc565d603ccbaecf1d01aa9aaf88110831c6c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/C2YQECQ5WIDM6FLNNKHYTUFEF4/bundle.json","state_url":"https://pith.science/pith/C2YQECQ5WIDM6FLNNKHYTUFEF4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/C2YQECQ5WIDM6FLNNKHYTUFEF4/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":"2026-08-16T17:00:18Z","links":{"resolver":"https://pith.science/pith/C2YQECQ5WIDM6FLNNKHYTUFEF4","bundle":"https://pith.science/pith/C2YQECQ5WIDM6FLNNKHYTUFEF4/bundle.json","state":"https://pith.science/pith/C2YQECQ5WIDM6FLNNKHYTUFEF4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/C2YQECQ5WIDM6FLNNKHYTUFEF4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:C2YQECQ5WIDM6FLNNKHYTUFEF4","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":"25a99ec8609007545515b627c8ea95fce740af9017ead57e6d7d7aad7e143e15","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-06-30T17:58:36Z","title_canon_sha256":"9978caa9c8f41e79c1550d6b3b9e19231c1759c00f69c9b507982f4cfa366fff"},"schema_version":"1.0","source":{"id":"2206.15471","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2206.15471","created_at":"2026-07-05T06:38:26Z"},{"alias_kind":"arxiv_version","alias_value":"2206.15471v2","created_at":"2026-07-05T06:38:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.15471","created_at":"2026-07-05T06:38:26Z"},{"alias_kind":"pith_short_12","alias_value":"C2YQECQ5WIDM","created_at":"2026-07-05T06:38:26Z"},{"alias_kind":"pith_short_16","alias_value":"C2YQECQ5WIDM6FLN","created_at":"2026-07-05T06:38:26Z"},{"alias_kind":"pith_short_8","alias_value":"C2YQECQ5","created_at":"2026-07-05T06:38:26Z"}],"graph_snapshots":[{"event_id":"sha256:77ecf495c4a33331fedbc6440f6bc565d603ccbaecf1d01aa9aaf88110831c6c","target":"graph","created_at":"2026-07-05T06:38:26Z","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/2206.15471/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The energy loss pattern of a low momentum heavy quark in a deconfined quark-gluon plasma can be understood in terms of a Langevin description. In thermal equilibrium, the motion can then be parametrized in terms of a single heavy quark momentum diffusion coefficient kappa, which needs to be determined nonperturbatively. In this work, we study the temperature dependence of kappa for a static quark in a gluonic plasma, with a particular emphasis on the temperature range of interest for heavy ion collision experiments.","authors_text":"Debasish Banerjee, Pushan Majumdar, Rajiv Gavai, Saumen Datta","cross_cats":["hep-ex","hep-lat","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-06-30T17:58:36Z","title":"Temperature dependence of the static quark diffusion coefficient"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.15471","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":"sha256:47a95bcb5255f247a3dc6be9b7d8536fdc3bbdd7061636542ea8a8da7e3d311e","target":"record","created_at":"2026-07-05T06:38:26Z","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":"25a99ec8609007545515b627c8ea95fce740af9017ead57e6d7d7aad7e143e15","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-06-30T17:58:36Z","title_canon_sha256":"9978caa9c8f41e79c1550d6b3b9e19231c1759c00f69c9b507982f4cfa366fff"},"schema_version":"1.0","source":{"id":"2206.15471","kind":"arxiv","version":2}},"canonical_sha256":"16b1020a1db206cf156d6a8f89d0a42f354c900e3621c114747c431987aac1c5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"16b1020a1db206cf156d6a8f89d0a42f354c900e3621c114747c431987aac1c5","first_computed_at":"2026-07-05T06:38:26.422760Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:38:26.422760Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"YOge7BFSE3MZiEnhzkhzCZCfsdQv8FD+DQRgDUJutWwOX5NjayPlthEcps9kPJUT0kw4Xb7sdTVaSpVFHtEvDw==","signature_status":"signed_v1","signed_at":"2026-07-05T06:38:26.423243Z","signed_message":"canonical_sha256_bytes"},"source_id":"2206.15471","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:47a95bcb5255f247a3dc6be9b7d8536fdc3bbdd7061636542ea8a8da7e3d311e","sha256:77ecf495c4a33331fedbc6440f6bc565d603ccbaecf1d01aa9aaf88110831c6c"],"state_sha256":"7bfc70ed414dc6208edd079297ef8e81a84300a42368be860bac13bebbec65b6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YZz7OKl5pT+rTTJhdiIahvU5oD5f/7rvga+FqsXO8XFwkcHCA7XWkWOc17w8xbFxsiw7fQz1vATuzPHBvH3ACQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-16T17:00:18.863345Z","bundle_sha256":"c5b938b7a8e050e0301c48a0e85acc8a47252eaabc3e1d451b87d8d98da2bd38"}}