{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:EHRBP24OQRO5U63MBKU3TZUQJW","short_pith_number":"pith:EHRBP24O","canonical_record":{"source":{"id":"1605.00188","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-05-01T00:32:44Z","cross_cats_sorted":["hep-th","nucl-ex","nucl-th"],"title_canon_sha256":"88d29634ff0b4b9a98910ce13154eadc1e42893cb6514ea9214eabc63decfb3f","abstract_canon_sha256":"2c1224d23090a9da8644997f3cd66f817c205b72d2803cded79413e4a2d77f9f"},"schema_version":"1.0"},"canonical_sha256":"21e217eb8e845dda7b6c0aa9b9e6904d882e8bcd764b143c5d41a8019ac28639","source":{"kind":"arxiv","id":"1605.00188","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.00188","created_at":"2026-05-18T01:01:15Z"},{"alias_kind":"arxiv_version","alias_value":"1605.00188v2","created_at":"2026-05-18T01:01:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.00188","created_at":"2026-05-18T01:01:15Z"},{"alias_kind":"pith_short_12","alias_value":"EHRBP24OQRO5","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_16","alias_value":"EHRBP24OQRO5U63M","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_8","alias_value":"EHRBP24O","created_at":"2026-05-18T12:30:12Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:EHRBP24OQRO5U63MBKU3TZUQJW","target":"record","payload":{"canonical_record":{"source":{"id":"1605.00188","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-05-01T00:32:44Z","cross_cats_sorted":["hep-th","nucl-ex","nucl-th"],"title_canon_sha256":"88d29634ff0b4b9a98910ce13154eadc1e42893cb6514ea9214eabc63decfb3f","abstract_canon_sha256":"2c1224d23090a9da8644997f3cd66f817c205b72d2803cded79413e4a2d77f9f"},"schema_version":"1.0"},"canonical_sha256":"21e217eb8e845dda7b6c0aa9b9e6904d882e8bcd764b143c5d41a8019ac28639","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:01:15.718417Z","signature_b64":"rvkeefJXGIVPl3IXQ0NsIEb+mUNw/OGisQjyfgyfOkSEaVhWQgEBqnPAkaBv3zV0xsdS9kkdt01M17u1JL+OAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"21e217eb8e845dda7b6c0aa9b9e6904d882e8bcd764b143c5d41a8019ac28639","last_reissued_at":"2026-05-18T01:01:15.717687Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:01:15.717687Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1605.00188","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":"2026-05-18T01:01:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Bin6NcESag+lN35Fp/IGGFoarQsbYefF1BD8VNjfVEvUXAcupmTYDONMnP4/+eFtBeWdCeOjGbXKso1uju+qDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T18:34:57.391659Z"},"content_sha256":"63990b7b339108e19cbf44511d09551cf5c22cedfc9fe97ab3afef3d9911890e","schema_version":"1.0","event_id":"sha256:63990b7b339108e19cbf44511d09551cf5c22cedfc9fe97ab3afef3d9911890e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:EHRBP24OQRO5U63MBKU3TZUQJW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Jet quenching parameter of quark-gluon plasma in strong magnetic field: Perturbative QCD and AdS/CFT correspondence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Ho-Ung Yee, Kiminad A. Mamo, Shiyong Li","submitted_at":"2016-05-01T00:32:44Z","abstract_excerpt":"We compute the jet quenching parameter $\\hat q$ of QCD plasma in the presence of strong magnetic field in both weakly and strongly coupled regimes. In weakly coupled regime, we compute $\\hat q$ in perturbative QCD at complete leading order (that is, leading log as well as the constant under the log) in QCD coupling constant $\\alpha_s$, assuming the hierarchy of scales $\\alpha_s eB\\ll T^2\\ll eB$. We consider two cases of jet orientations with respect to the magnetic field: 1) the case of jet moving parallel to the magnetic field, 2) the case jet moving perpendicular to the magnetic field. In th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.00188","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":"2026-05-18T01:01:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iffSQfTriWfNBhE/0FiRhesWB844Z9ovTyFgnbrVpyq8wSTZjt+AD7+wkIoXoOlLJDRFTzYLHNEB4YaVWZ3GAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T18:34:57.392390Z"},"content_sha256":"f1077d44e948f10d2f4209573ccc98a1138fe73deb90d7ddbeb614c9da07a610","schema_version":"1.0","event_id":"sha256:f1077d44e948f10d2f4209573ccc98a1138fe73deb90d7ddbeb614c9da07a610"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EHRBP24OQRO5U63MBKU3TZUQJW/bundle.json","state_url":"https://pith.science/pith/EHRBP24OQRO5U63MBKU3TZUQJW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EHRBP24OQRO5U63MBKU3TZUQJW/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":"2026-06-09T18:34:57Z","links":{"resolver":"https://pith.science/pith/EHRBP24OQRO5U63MBKU3TZUQJW","bundle":"https://pith.science/pith/EHRBP24OQRO5U63MBKU3TZUQJW/bundle.json","state":"https://pith.science/pith/EHRBP24OQRO5U63MBKU3TZUQJW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EHRBP24OQRO5U63MBKU3TZUQJW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:EHRBP24OQRO5U63MBKU3TZUQJW","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":"2c1224d23090a9da8644997f3cd66f817c205b72d2803cded79413e4a2d77f9f","cross_cats_sorted":["hep-th","nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-05-01T00:32:44Z","title_canon_sha256":"88d29634ff0b4b9a98910ce13154eadc1e42893cb6514ea9214eabc63decfb3f"},"schema_version":"1.0","source":{"id":"1605.00188","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.00188","created_at":"2026-05-18T01:01:15Z"},{"alias_kind":"arxiv_version","alias_value":"1605.00188v2","created_at":"2026-05-18T01:01:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.00188","created_at":"2026-05-18T01:01:15Z"},{"alias_kind":"pith_short_12","alias_value":"EHRBP24OQRO5","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_16","alias_value":"EHRBP24OQRO5U63M","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_8","alias_value":"EHRBP24O","created_at":"2026-05-18T12:30:12Z"}],"graph_snapshots":[{"event_id":"sha256:f1077d44e948f10d2f4209573ccc98a1138fe73deb90d7ddbeb614c9da07a610","target":"graph","created_at":"2026-05-18T01:01:15Z","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":"We compute the jet quenching parameter $\\hat q$ of QCD plasma in the presence of strong magnetic field in both weakly and strongly coupled regimes. In weakly coupled regime, we compute $\\hat q$ in perturbative QCD at complete leading order (that is, leading log as well as the constant under the log) in QCD coupling constant $\\alpha_s$, assuming the hierarchy of scales $\\alpha_s eB\\ll T^2\\ll eB$. We consider two cases of jet orientations with respect to the magnetic field: 1) the case of jet moving parallel to the magnetic field, 2) the case jet moving perpendicular to the magnetic field. In th","authors_text":"Ho-Ung Yee, Kiminad A. Mamo, Shiyong Li","cross_cats":["hep-th","nucl-ex","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-05-01T00:32:44Z","title":"Jet quenching parameter of quark-gluon plasma in strong magnetic field: Perturbative QCD and AdS/CFT correspondence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.00188","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":"sha256:63990b7b339108e19cbf44511d09551cf5c22cedfc9fe97ab3afef3d9911890e","target":"record","created_at":"2026-05-18T01:01:15Z","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":"2c1224d23090a9da8644997f3cd66f817c205b72d2803cded79413e4a2d77f9f","cross_cats_sorted":["hep-th","nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-05-01T00:32:44Z","title_canon_sha256":"88d29634ff0b4b9a98910ce13154eadc1e42893cb6514ea9214eabc63decfb3f"},"schema_version":"1.0","source":{"id":"1605.00188","kind":"arxiv","version":2}},"canonical_sha256":"21e217eb8e845dda7b6c0aa9b9e6904d882e8bcd764b143c5d41a8019ac28639","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"21e217eb8e845dda7b6c0aa9b9e6904d882e8bcd764b143c5d41a8019ac28639","first_computed_at":"2026-05-18T01:01:15.717687Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:01:15.717687Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rvkeefJXGIVPl3IXQ0NsIEb+mUNw/OGisQjyfgyfOkSEaVhWQgEBqnPAkaBv3zV0xsdS9kkdt01M17u1JL+OAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:01:15.718417Z","signed_message":"canonical_sha256_bytes"},"source_id":"1605.00188","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:63990b7b339108e19cbf44511d09551cf5c22cedfc9fe97ab3afef3d9911890e","sha256:f1077d44e948f10d2f4209573ccc98a1138fe73deb90d7ddbeb614c9da07a610"],"state_sha256":"3ab6e3fcc3a2496c041f6bc662ddbad7650d42de2a03c06df0a1b5f9371cfe05"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3EJB8hgT+TMCGB4I3Fh2PDUrdpc1iHL2OmnVnVTeY8xQVgLPYDn9XvO3M5qnQhlUZpIQM1QerPX+P2SRCzrIBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T18:34:57.396062Z","bundle_sha256":"299e6fbdb758956d21dee21827fef67e74d060ac61514006daeff7b196d53486"}}