{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:VAX4AT5I3JGFNFFMCQJLG4NINS","short_pith_number":"pith:VAX4AT5I","canonical_record":{"source":{"id":"1302.1432","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-02-06T16:43:25Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"a2ba6e1824f9f26423293626295df99c519c8109782490d0e9647af087fe978b","abstract_canon_sha256":"a252776838a703ec687baceff7ea25200b9394ec42bb3a0d47e76078e2cc5e6c"},"schema_version":"1.0"},"canonical_sha256":"a82fc04fa8da4c5694ac1412b371a86c965a455dbfc7bc20a6a6f250b0d69b3e","source":{"kind":"arxiv","id":"1302.1432","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.1432","created_at":"2026-05-18T01:51:49Z"},{"alias_kind":"arxiv_version","alias_value":"1302.1432v2","created_at":"2026-05-18T01:51:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.1432","created_at":"2026-05-18T01:51:49Z"},{"alias_kind":"pith_short_12","alias_value":"VAX4AT5I3JGF","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_16","alias_value":"VAX4AT5I3JGFNFFM","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_8","alias_value":"VAX4AT5I","created_at":"2026-05-18T12:28:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:VAX4AT5I3JGFNFFMCQJLG4NINS","target":"record","payload":{"canonical_record":{"source":{"id":"1302.1432","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-02-06T16:43:25Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"a2ba6e1824f9f26423293626295df99c519c8109782490d0e9647af087fe978b","abstract_canon_sha256":"a252776838a703ec687baceff7ea25200b9394ec42bb3a0d47e76078e2cc5e6c"},"schema_version":"1.0"},"canonical_sha256":"a82fc04fa8da4c5694ac1412b371a86c965a455dbfc7bc20a6a6f250b0d69b3e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:51:49.732035Z","signature_b64":"LEgjXX5onPpPYNmL9/mxTu4NEc/x9Vr5osD2sNjk0GFyCLtG7eNKv5dZA55AtAM8vm2wM+eF/59ED8OmnchJAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a82fc04fa8da4c5694ac1412b371a86c965a455dbfc7bc20a6a6f250b0d69b3e","last_reissued_at":"2026-05-18T01:51:49.731509Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:51:49.731509Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1302.1432","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":"2026-05-18T01:51:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7JfnMQX4pRztdmLC02BCYv26DCybWgiaXPo5gzrVdKEWq84SZHW/qDlf7w/d+fxdsbOl9nDudbbjd+qKkiKsBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T21:57:46.606070Z"},"content_sha256":"e76e8e8d42752aa3ee06b1e585ed267b0b89953b6a5892c4286e8d7a2c10bf4c","schema_version":"1.0","event_id":"sha256:e76e8e8d42752aa3ee06b1e585ed267b0b89953b6a5892c4286e8d7a2c10bf4c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:VAX4AT5I3JGFNFFMCQJLG4NINS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Energy momentum tensor correlators in hot Yang-Mills theory: holography confronts lattice and perturbation theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Aleksi Vuorinen, K. Kajantie, Martin Krssak","submitted_at":"2013-02-06T16:43:25Z","abstract_excerpt":"We investigate the behavior of energy momentum tensor correlators in strongly coupled large-N_c Yang-Mills theory at nonzero temperature, working within the Improved Holographic QCD model. In particular, we determine the spectral functions and corresponding imaginary time correlators in the bulk and shear channels, and compare the results to recent perturbative and lattice calculations where available. For the bulk channel imaginary time correlator, for which all three results exist, lattice data is seen to favor the holographic prediction over the perturbative one over a wide range of tempera"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.1432","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":"2026-05-18T01:51:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yKRa+XH914P/wnl66Xw6KcTu+4e4C9F1oaCDpa9nTSEPoktjWHT50SfjqkprTL2j1eWZID6QBY02SL++BX0nBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T21:57:46.606420Z"},"content_sha256":"48d43bf610896e208e35db5f4a74b51f3357dbf85544267054b562c2ab36f7c4","schema_version":"1.0","event_id":"sha256:48d43bf610896e208e35db5f4a74b51f3357dbf85544267054b562c2ab36f7c4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VAX4AT5I3JGFNFFMCQJLG4NINS/bundle.json","state_url":"https://pith.science/pith/VAX4AT5I3JGFNFFMCQJLG4NINS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VAX4AT5I3JGFNFFMCQJLG4NINS/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":"2026-06-29T21:57:46Z","links":{"resolver":"https://pith.science/pith/VAX4AT5I3JGFNFFMCQJLG4NINS","bundle":"https://pith.science/pith/VAX4AT5I3JGFNFFMCQJLG4NINS/bundle.json","state":"https://pith.science/pith/VAX4AT5I3JGFNFFMCQJLG4NINS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VAX4AT5I3JGFNFFMCQJLG4NINS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:VAX4AT5I3JGFNFFMCQJLG4NINS","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":"a252776838a703ec687baceff7ea25200b9394ec42bb3a0d47e76078e2cc5e6c","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-02-06T16:43:25Z","title_canon_sha256":"a2ba6e1824f9f26423293626295df99c519c8109782490d0e9647af087fe978b"},"schema_version":"1.0","source":{"id":"1302.1432","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.1432","created_at":"2026-05-18T01:51:49Z"},{"alias_kind":"arxiv_version","alias_value":"1302.1432v2","created_at":"2026-05-18T01:51:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.1432","created_at":"2026-05-18T01:51:49Z"},{"alias_kind":"pith_short_12","alias_value":"VAX4AT5I3JGF","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_16","alias_value":"VAX4AT5I3JGFNFFM","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_8","alias_value":"VAX4AT5I","created_at":"2026-05-18T12:28:04Z"}],"graph_snapshots":[{"event_id":"sha256:48d43bf610896e208e35db5f4a74b51f3357dbf85544267054b562c2ab36f7c4","target":"graph","created_at":"2026-05-18T01:51:49Z","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 investigate the behavior of energy momentum tensor correlators in strongly coupled large-N_c Yang-Mills theory at nonzero temperature, working within the Improved Holographic QCD model. In particular, we determine the spectral functions and corresponding imaginary time correlators in the bulk and shear channels, and compare the results to recent perturbative and lattice calculations where available. For the bulk channel imaginary time correlator, for which all three results exist, lattice data is seen to favor the holographic prediction over the perturbative one over a wide range of tempera","authors_text":"Aleksi Vuorinen, K. Kajantie, Martin Krssak","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-02-06T16:43:25Z","title":"Energy momentum tensor correlators in hot Yang-Mills theory: holography confronts lattice and perturbation theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.1432","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:e76e8e8d42752aa3ee06b1e585ed267b0b89953b6a5892c4286e8d7a2c10bf4c","target":"record","created_at":"2026-05-18T01:51:49Z","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":"a252776838a703ec687baceff7ea25200b9394ec42bb3a0d47e76078e2cc5e6c","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-02-06T16:43:25Z","title_canon_sha256":"a2ba6e1824f9f26423293626295df99c519c8109782490d0e9647af087fe978b"},"schema_version":"1.0","source":{"id":"1302.1432","kind":"arxiv","version":2}},"canonical_sha256":"a82fc04fa8da4c5694ac1412b371a86c965a455dbfc7bc20a6a6f250b0d69b3e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a82fc04fa8da4c5694ac1412b371a86c965a455dbfc7bc20a6a6f250b0d69b3e","first_computed_at":"2026-05-18T01:51:49.731509Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:51:49.731509Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"LEgjXX5onPpPYNmL9/mxTu4NEc/x9Vr5osD2sNjk0GFyCLtG7eNKv5dZA55AtAM8vm2wM+eF/59ED8OmnchJAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:51:49.732035Z","signed_message":"canonical_sha256_bytes"},"source_id":"1302.1432","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e76e8e8d42752aa3ee06b1e585ed267b0b89953b6a5892c4286e8d7a2c10bf4c","sha256:48d43bf610896e208e35db5f4a74b51f3357dbf85544267054b562c2ab36f7c4"],"state_sha256":"f16fcda644cebedaa8da406b81d4140c59b1e807c8aef004a3c971c6539995d3"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5dhJFAOn/Cq4vpO9m2k7jzflJsFqZCO9L2kkPY0XiWV2iqjmsatHi1uCt9v+OYfoHCIs+YYUu003+MR1yum2Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-29T21:57:46.608284Z","bundle_sha256":"7ede3af7bd95339bf6c7f56ff6af4b3faef813ad47c20f199ba4ce3afc7d8800"}}