{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:W4L5NHIU7BAZW5EJ4YTSFC74SP","short_pith_number":"pith:W4L5NHIU","canonical_record":{"source":{"id":"1307.1487","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-07-04T20:56:19Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"1d63dc26c5175b2e833a803f9d9f6750c6765be44d63b37922d2414570e60644","abstract_canon_sha256":"ade22ca1b987a93a817da8a6cb862f78c27d1dddaab8eeb23467220a67c417c8"},"schema_version":"1.0"},"canonical_sha256":"b717d69d14f8419b7489e627228bfc93c70abe518873d9edf50c4d3ecb91cbd2","source":{"kind":"arxiv","id":"1307.1487","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.1487","created_at":"2026-05-18T03:04:49Z"},{"alias_kind":"arxiv_version","alias_value":"1307.1487v2","created_at":"2026-05-18T03:04:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.1487","created_at":"2026-05-18T03:04:49Z"},{"alias_kind":"pith_short_12","alias_value":"W4L5NHIU7BAZ","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_16","alias_value":"W4L5NHIU7BAZW5EJ","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_8","alias_value":"W4L5NHIU","created_at":"2026-05-18T12:28:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:W4L5NHIU7BAZW5EJ4YTSFC74SP","target":"record","payload":{"canonical_record":{"source":{"id":"1307.1487","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-07-04T20:56:19Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"1d63dc26c5175b2e833a803f9d9f6750c6765be44d63b37922d2414570e60644","abstract_canon_sha256":"ade22ca1b987a93a817da8a6cb862f78c27d1dddaab8eeb23467220a67c417c8"},"schema_version":"1.0"},"canonical_sha256":"b717d69d14f8419b7489e627228bfc93c70abe518873d9edf50c4d3ecb91cbd2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:04:49.120080Z","signature_b64":"8/Djec7QumehTq+DeCz3v8mPCtmE/+Jn8jPP72mAMfrPsDIjd1EhfG/nJvyi0gCJYcFnCfnF2/milyKQtqASDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b717d69d14f8419b7489e627228bfc93c70abe518873d9edf50c4d3ecb91cbd2","last_reissued_at":"2026-05-18T03:04:49.119536Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:04:49.119536Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1307.1487","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":"2026-05-18T03:04:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YwWds2oOsisCsBeQ1SKF6crS1BERgGD6WurG8VO/rPJ/qMtmJSNSBxL4supIA5z0sJBXIiO2pJ62h4RzarPGDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T17:16:16.565692Z"},"content_sha256":"b44ffd6af64912305adac027dfc30b78c1157502bee19ac89e0e8a01b7ee538f","schema_version":"1.0","event_id":"sha256:b44ffd6af64912305adac027dfc30b78c1157502bee19ac89e0e8a01b7ee538f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:W4L5NHIU7BAZW5EJ4YTSFC74SP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Inhomogeneous Thermalization in Strongly Coupled Field Theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"A. Bernamonti, A. Sch\\\"afer, B. Craps, B. M\\\"uller, E. Keski-Vakkuri, F. Galli, J. de Boer, L. Franti, V. Balasubramanian","submitted_at":"2013-07-04T20:56:19Z","abstract_excerpt":"To describe theoretically the creation and evolution of the quark-gluon plasma, one typically employs three ingredients: a model for the initial state, non-hydrodynamic early time evolution, and hydrodynamics. In this paper we study the non-hydrodynamic early time evolution using the AdS/CFT correspondence in the presence of inhomogeneities. We find that the AdS description of the early time evolution is well-matched by free streaming. Near the end of the early time interval where our analytic computations are reliable, the stress tensor agrees with the second order hydrodynamic stress tensor "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.1487","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":"2026-05-18T03:04:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Qd/j/e+Wjaoq5Tw2MK/S/Bv+hlsmogZ6flbhU6L0ltaQhTEAbfEeptBc8LMr+3Te9q2adc3bU/PASgEDu0F8Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T17:16:16.566026Z"},"content_sha256":"588b1303a893bef0b0e82f663501e835826bda5445a296f79cab0ce94837dc22","schema_version":"1.0","event_id":"sha256:588b1303a893bef0b0e82f663501e835826bda5445a296f79cab0ce94837dc22"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/W4L5NHIU7BAZW5EJ4YTSFC74SP/bundle.json","state_url":"https://pith.science/pith/W4L5NHIU7BAZW5EJ4YTSFC74SP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/W4L5NHIU7BAZW5EJ4YTSFC74SP/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":"2026-06-01T17:16:16Z","links":{"resolver":"https://pith.science/pith/W4L5NHIU7BAZW5EJ4YTSFC74SP","bundle":"https://pith.science/pith/W4L5NHIU7BAZW5EJ4YTSFC74SP/bundle.json","state":"https://pith.science/pith/W4L5NHIU7BAZW5EJ4YTSFC74SP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/W4L5NHIU7BAZW5EJ4YTSFC74SP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:W4L5NHIU7BAZW5EJ4YTSFC74SP","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":"ade22ca1b987a93a817da8a6cb862f78c27d1dddaab8eeb23467220a67c417c8","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-07-04T20:56:19Z","title_canon_sha256":"1d63dc26c5175b2e833a803f9d9f6750c6765be44d63b37922d2414570e60644"},"schema_version":"1.0","source":{"id":"1307.1487","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.1487","created_at":"2026-05-18T03:04:49Z"},{"alias_kind":"arxiv_version","alias_value":"1307.1487v2","created_at":"2026-05-18T03:04:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.1487","created_at":"2026-05-18T03:04:49Z"},{"alias_kind":"pith_short_12","alias_value":"W4L5NHIU7BAZ","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_16","alias_value":"W4L5NHIU7BAZW5EJ","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_8","alias_value":"W4L5NHIU","created_at":"2026-05-18T12:28:04Z"}],"graph_snapshots":[{"event_id":"sha256:588b1303a893bef0b0e82f663501e835826bda5445a296f79cab0ce94837dc22","target":"graph","created_at":"2026-05-18T03:04:49Z","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":"To describe theoretically the creation and evolution of the quark-gluon plasma, one typically employs three ingredients: a model for the initial state, non-hydrodynamic early time evolution, and hydrodynamics. In this paper we study the non-hydrodynamic early time evolution using the AdS/CFT correspondence in the presence of inhomogeneities. We find that the AdS description of the early time evolution is well-matched by free streaming. Near the end of the early time interval where our analytic computations are reliable, the stress tensor agrees with the second order hydrodynamic stress tensor ","authors_text":"A. Bernamonti, A. Sch\\\"afer, B. Craps, B. M\\\"uller, E. Keski-Vakkuri, F. Galli, J. de Boer, L. Franti, V. Balasubramanian","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-07-04T20:56:19Z","title":"Inhomogeneous Thermalization in Strongly Coupled Field Theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.1487","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:b44ffd6af64912305adac027dfc30b78c1157502bee19ac89e0e8a01b7ee538f","target":"record","created_at":"2026-05-18T03:04:49Z","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":"ade22ca1b987a93a817da8a6cb862f78c27d1dddaab8eeb23467220a67c417c8","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-07-04T20:56:19Z","title_canon_sha256":"1d63dc26c5175b2e833a803f9d9f6750c6765be44d63b37922d2414570e60644"},"schema_version":"1.0","source":{"id":"1307.1487","kind":"arxiv","version":2}},"canonical_sha256":"b717d69d14f8419b7489e627228bfc93c70abe518873d9edf50c4d3ecb91cbd2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b717d69d14f8419b7489e627228bfc93c70abe518873d9edf50c4d3ecb91cbd2","first_computed_at":"2026-05-18T03:04:49.119536Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:04:49.119536Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8/Djec7QumehTq+DeCz3v8mPCtmE/+Jn8jPP72mAMfrPsDIjd1EhfG/nJvyi0gCJYcFnCfnF2/milyKQtqASDg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:04:49.120080Z","signed_message":"canonical_sha256_bytes"},"source_id":"1307.1487","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b44ffd6af64912305adac027dfc30b78c1157502bee19ac89e0e8a01b7ee538f","sha256:588b1303a893bef0b0e82f663501e835826bda5445a296f79cab0ce94837dc22"],"state_sha256":"d89c81807f8fa7470859874c62cab494aba0bfbe33a0144390b2cce950f1d7a2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xJfhiqC/gRxpxD/EYwQPp8fdihFIOs+xFvFrAkYDekNMjtGgRoEjJYtvOo1EiAKFisxnGcc/M/DctjzdM8X1Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T17:16:16.567925Z","bundle_sha256":"8e52a4f1b334db11c443db6ddecb6c9c3f7bf77f260bba08d2a7d2021d276480"}}