{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:XLSRHUCBTMP6VRKDF5WN47CDSB","short_pith_number":"pith:XLSRHUCB","canonical_record":{"source":{"id":"0903.4703","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-03-26T21:28:30Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"2d6401040fa83b4140203081216c7172f268334d2095b24d454d51c06b4f0c50","abstract_canon_sha256":"c43093b345913b8464c637086fbf528e8fb27ed0dbad0940722f9d3f2c59d7eb"},"schema_version":"1.0"},"canonical_sha256":"bae513d0419b1feac5432f6cde7c439071ffa1ad31e66d1e782710d9269254e7","source":{"kind":"arxiv","id":"0903.4703","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0903.4703","created_at":"2026-07-04T15:45:15Z"},{"alias_kind":"arxiv_version","alias_value":"0903.4703v2","created_at":"2026-07-04T15:45:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0903.4703","created_at":"2026-07-04T15:45:15Z"},{"alias_kind":"pith_short_12","alias_value":"XLSRHUCBTMP6","created_at":"2026-07-04T15:45:15Z"},{"alias_kind":"pith_short_16","alias_value":"XLSRHUCBTMP6VRKD","created_at":"2026-07-04T15:45:15Z"},{"alias_kind":"pith_short_8","alias_value":"XLSRHUCB","created_at":"2026-07-04T15:45:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:XLSRHUCBTMP6VRKDF5WN47CDSB","target":"record","payload":{"canonical_record":{"source":{"id":"0903.4703","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-03-26T21:28:30Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"2d6401040fa83b4140203081216c7172f268334d2095b24d454d51c06b4f0c50","abstract_canon_sha256":"c43093b345913b8464c637086fbf528e8fb27ed0dbad0940722f9d3f2c59d7eb"},"schema_version":"1.0"},"canonical_sha256":"bae513d0419b1feac5432f6cde7c439071ffa1ad31e66d1e782710d9269254e7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:45:15.240820Z","signature_b64":"GejJXPToM+Wxw4iAZAPtNOKbPOJ7P7YpyJeBoIHajNtDG563UBIVRcdy77d2oNnSLbCM3bsSCi/th5I2nrYzDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bae513d0419b1feac5432f6cde7c439071ffa1ad31e66d1e782710d9269254e7","last_reissued_at":"2026-07-04T15:45:15.240387Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:45:15.240387Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0903.4703","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":"2026-07-04T15:45:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SBGPrUpD3usHccMYCmZXJ7dhfU5NE7DNPfK2XOovnt2Fn3VgYMZWAl3U3tGFoYDn9R+xOUbpnbR4iBiN/QO1BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-10T17:24:51.821634Z"},"content_sha256":"0e7c229ca2272cd615b7c9b439b99c84b99d3daf23944ed087ec36f54386b539","schema_version":"1.0","event_id":"sha256:0e7c229ca2272cd615b7c9b439b99c84b99d3daf23944ed087ec36f54386b539"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:XLSRHUCBTMP6VRKDF5WN47CDSB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The imaginary part of the static gluon propagator in an anisotropic (viscous) QCD plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Adrian Dumitru, Michael Strickland, Yun Guo","submitted_at":"2009-03-26T21:28:30Z","abstract_excerpt":"We determine viscosity corrections to the retarded, advanced and symmetric gluon self energies and to the static propagator in the weak-coupling \"hard loop\" approximation to high-temperature QCD. We apply these results to calculate the imaginary part of the heavy-quark potential which is found to be smaller (in magnitude) than at vanishing viscosity. This implies a smaller decay width of quarkonium bound states in an anisotropic plasma."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0903.4703","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/0903.4703/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":"2026-07-04T15:45:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XoCNyFO3JU6xK2ywVEVrhkXcybVi3WAX4A1NU5mgksobQWSjrVmNH9f1i7RIDiQlx92WRgiiYMTkAu1eE0rcDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-10T17:24:51.822134Z"},"content_sha256":"15da722d6a2df0bf0adebf8b166ac146c39d9be8e2d4269b161b039d030670a9","schema_version":"1.0","event_id":"sha256:15da722d6a2df0bf0adebf8b166ac146c39d9be8e2d4269b161b039d030670a9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XLSRHUCBTMP6VRKDF5WN47CDSB/bundle.json","state_url":"https://pith.science/pith/XLSRHUCBTMP6VRKDF5WN47CDSB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XLSRHUCBTMP6VRKDF5WN47CDSB/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":"2026-08-10T17:24:51Z","links":{"resolver":"https://pith.science/pith/XLSRHUCBTMP6VRKDF5WN47CDSB","bundle":"https://pith.science/pith/XLSRHUCBTMP6VRKDF5WN47CDSB/bundle.json","state":"https://pith.science/pith/XLSRHUCBTMP6VRKDF5WN47CDSB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XLSRHUCBTMP6VRKDF5WN47CDSB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:XLSRHUCBTMP6VRKDF5WN47CDSB","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":"c43093b345913b8464c637086fbf528e8fb27ed0dbad0940722f9d3f2c59d7eb","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-03-26T21:28:30Z","title_canon_sha256":"2d6401040fa83b4140203081216c7172f268334d2095b24d454d51c06b4f0c50"},"schema_version":"1.0","source":{"id":"0903.4703","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0903.4703","created_at":"2026-07-04T15:45:15Z"},{"alias_kind":"arxiv_version","alias_value":"0903.4703v2","created_at":"2026-07-04T15:45:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0903.4703","created_at":"2026-07-04T15:45:15Z"},{"alias_kind":"pith_short_12","alias_value":"XLSRHUCBTMP6","created_at":"2026-07-04T15:45:15Z"},{"alias_kind":"pith_short_16","alias_value":"XLSRHUCBTMP6VRKD","created_at":"2026-07-04T15:45:15Z"},{"alias_kind":"pith_short_8","alias_value":"XLSRHUCB","created_at":"2026-07-04T15:45:15Z"}],"graph_snapshots":[{"event_id":"sha256:15da722d6a2df0bf0adebf8b166ac146c39d9be8e2d4269b161b039d030670a9","target":"graph","created_at":"2026-07-04T15:45:15Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/0903.4703/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We determine viscosity corrections to the retarded, advanced and symmetric gluon self energies and to the static propagator in the weak-coupling \"hard loop\" approximation to high-temperature QCD. We apply these results to calculate the imaginary part of the heavy-quark potential which is found to be smaller (in magnitude) than at vanishing viscosity. This implies a smaller decay width of quarkonium bound states in an anisotropic plasma.","authors_text":"Adrian Dumitru, Michael Strickland, Yun Guo","cross_cats":["nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-03-26T21:28:30Z","title":"The imaginary part of the static gluon propagator in an anisotropic (viscous) QCD plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0903.4703","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":"sha256:0e7c229ca2272cd615b7c9b439b99c84b99d3daf23944ed087ec36f54386b539","target":"record","created_at":"2026-07-04T15:45:15Z","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":"c43093b345913b8464c637086fbf528e8fb27ed0dbad0940722f9d3f2c59d7eb","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-03-26T21:28:30Z","title_canon_sha256":"2d6401040fa83b4140203081216c7172f268334d2095b24d454d51c06b4f0c50"},"schema_version":"1.0","source":{"id":"0903.4703","kind":"arxiv","version":2}},"canonical_sha256":"bae513d0419b1feac5432f6cde7c439071ffa1ad31e66d1e782710d9269254e7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bae513d0419b1feac5432f6cde7c439071ffa1ad31e66d1e782710d9269254e7","first_computed_at":"2026-07-04T15:45:15.240387Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:45:15.240387Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"GejJXPToM+Wxw4iAZAPtNOKbPOJ7P7YpyJeBoIHajNtDG563UBIVRcdy77d2oNnSLbCM3bsSCi/th5I2nrYzDg==","signature_status":"signed_v1","signed_at":"2026-07-04T15:45:15.240820Z","signed_message":"canonical_sha256_bytes"},"source_id":"0903.4703","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0e7c229ca2272cd615b7c9b439b99c84b99d3daf23944ed087ec36f54386b539","sha256:15da722d6a2df0bf0adebf8b166ac146c39d9be8e2d4269b161b039d030670a9"],"state_sha256":"523f190f35db8020f96117a508d926f521564aeb2a1a763a9a1975160bd5b3ef"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"teySekdbwjO2holI420cLeqvyCdZxuhUTwHw2Utt8DQlpPudFSGZcJi92Qcl++cTzk7BW1uozGBY+ET50oidCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-10T17:24:51.828482Z","bundle_sha256":"fcd64f73be9020b81b7e0edde10a4437a59ed089daed518f8fa46cde5ad6837d"}}