{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:I5HBZMES775DLDLNL6WKRFHPEO","short_pith_number":"pith:I5HBZMES","canonical_record":{"source":{"id":"1601.01583","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-01-07T16:22:53Z","cross_cats_sorted":["gr-qc","hep-ph","nucl-th"],"title_canon_sha256":"b94dd1f977aedf2d9f3e11438cbe2b07e24dd2d6901f086993778c99cdd36edf","abstract_canon_sha256":"f28e198df50ee6f726ec45fb58a8b98dbe200f048e063588fab6dacd0526d786"},"schema_version":"1.0"},"canonical_sha256":"474e1cb092fffa358d6d5faca894ef2397be2ed41c3239fdf30aabe796fd3bf4","source":{"kind":"arxiv","id":"1601.01583","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1601.01583","created_at":"2026-05-18T01:16:43Z"},{"alias_kind":"arxiv_version","alias_value":"1601.01583v2","created_at":"2026-05-18T01:16:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.01583","created_at":"2026-05-18T01:16:43Z"},{"alias_kind":"pith_short_12","alias_value":"I5HBZMES775D","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_16","alias_value":"I5HBZMES775DLDLN","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_8","alias_value":"I5HBZMES","created_at":"2026-05-18T12:30:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:I5HBZMES775DLDLNL6WKRFHPEO","target":"record","payload":{"canonical_record":{"source":{"id":"1601.01583","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-01-07T16:22:53Z","cross_cats_sorted":["gr-qc","hep-ph","nucl-th"],"title_canon_sha256":"b94dd1f977aedf2d9f3e11438cbe2b07e24dd2d6901f086993778c99cdd36edf","abstract_canon_sha256":"f28e198df50ee6f726ec45fb58a8b98dbe200f048e063588fab6dacd0526d786"},"schema_version":"1.0"},"canonical_sha256":"474e1cb092fffa358d6d5faca894ef2397be2ed41c3239fdf30aabe796fd3bf4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:16:43.719235Z","signature_b64":"iKeeJ8aLOcfoVxoiqRAf93fz9E1QET0EKks/KHEuBYr40LVduena9fzt8dICyKNbRZVEeGmhy9JGZD6jxXPIBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"474e1cb092fffa358d6d5faca894ef2397be2ed41c3239fdf30aabe796fd3bf4","last_reissued_at":"2026-05-18T01:16:43.718564Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:16:43.718564Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1601.01583","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":"2026-05-18T01:16:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"S2Br68hcLhCyd5o7o+tf3RDgwFVMTJ2PPiWhN0yTgxcX5GEGyFOy9dNWSFjgBuTv2aObveTbX1IeODgGs8fUBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T09:16:52.188792Z"},"content_sha256":"2074c09f50040800a29c5f89fbecd58bc6e796c7defa3a714f62074668798261","schema_version":"1.0","event_id":"sha256:2074c09f50040800a29c5f89fbecd58bc6e796c7defa3a714f62074668798261"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:I5HBZMES775DLDLNL6WKRFHPEO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"How big are the smallest drops of quark-gluon plasma?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"Paul M. Chesler","submitted_at":"2016-01-07T16:22:53Z","abstract_excerpt":"Using holographic duality, we present results for both head-on and off-center collisions of Gaussian shock waves in strongly coupled $\\mathcal N = 4$ supersymmetric Yang-Mills theory. The shock waves superficially resemble Lorentz contracted colliding protons. The collisions results in the formation of a plasma whose evolution is well described by viscous hydrodynamics. The size of the produced droplet is $R \\sim 1/T_{\\rm eff}$ where $T_{\\rm eff}$ is the effective temperature, which is the characteristic microscopic scale in strongly coupled plasma. These results demonstrate the applicability "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.01583","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":"2026-05-18T01:16:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KMk7oI2QeXV0MmkNyPS5eWlJaqs9F6JmsNhMEuyr43deVRyQ5tJ/4/JauBBQ+1NmLaEnzKOEZ7B1ISgnCGnrDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T09:16:52.189168Z"},"content_sha256":"a213fde62e91cebcff50178a304ba5e71134d69f1652011e3fd15ac9f09f0c98","schema_version":"1.0","event_id":"sha256:a213fde62e91cebcff50178a304ba5e71134d69f1652011e3fd15ac9f09f0c98"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/I5HBZMES775DLDLNL6WKRFHPEO/bundle.json","state_url":"https://pith.science/pith/I5HBZMES775DLDLNL6WKRFHPEO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/I5HBZMES775DLDLNL6WKRFHPEO/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":"2026-08-03T09:16:52Z","links":{"resolver":"https://pith.science/pith/I5HBZMES775DLDLNL6WKRFHPEO","bundle":"https://pith.science/pith/I5HBZMES775DLDLNL6WKRFHPEO/bundle.json","state":"https://pith.science/pith/I5HBZMES775DLDLNL6WKRFHPEO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/I5HBZMES775DLDLNL6WKRFHPEO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:I5HBZMES775DLDLNL6WKRFHPEO","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":"f28e198df50ee6f726ec45fb58a8b98dbe200f048e063588fab6dacd0526d786","cross_cats_sorted":["gr-qc","hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-01-07T16:22:53Z","title_canon_sha256":"b94dd1f977aedf2d9f3e11438cbe2b07e24dd2d6901f086993778c99cdd36edf"},"schema_version":"1.0","source":{"id":"1601.01583","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1601.01583","created_at":"2026-05-18T01:16:43Z"},{"alias_kind":"arxiv_version","alias_value":"1601.01583v2","created_at":"2026-05-18T01:16:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.01583","created_at":"2026-05-18T01:16:43Z"},{"alias_kind":"pith_short_12","alias_value":"I5HBZMES775D","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_16","alias_value":"I5HBZMES775DLDLN","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_8","alias_value":"I5HBZMES","created_at":"2026-05-18T12:30:22Z"}],"graph_snapshots":[{"event_id":"sha256:a213fde62e91cebcff50178a304ba5e71134d69f1652011e3fd15ac9f09f0c98","target":"graph","created_at":"2026-05-18T01:16:43Z","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":"Using holographic duality, we present results for both head-on and off-center collisions of Gaussian shock waves in strongly coupled $\\mathcal N = 4$ supersymmetric Yang-Mills theory. The shock waves superficially resemble Lorentz contracted colliding protons. The collisions results in the formation of a plasma whose evolution is well described by viscous hydrodynamics. The size of the produced droplet is $R \\sim 1/T_{\\rm eff}$ where $T_{\\rm eff}$ is the effective temperature, which is the characteristic microscopic scale in strongly coupled plasma. These results demonstrate the applicability ","authors_text":"Paul M. Chesler","cross_cats":["gr-qc","hep-ph","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-01-07T16:22:53Z","title":"How big are the smallest drops of quark-gluon plasma?"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.01583","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":"sha256:2074c09f50040800a29c5f89fbecd58bc6e796c7defa3a714f62074668798261","target":"record","created_at":"2026-05-18T01:16:43Z","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":"f28e198df50ee6f726ec45fb58a8b98dbe200f048e063588fab6dacd0526d786","cross_cats_sorted":["gr-qc","hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-01-07T16:22:53Z","title_canon_sha256":"b94dd1f977aedf2d9f3e11438cbe2b07e24dd2d6901f086993778c99cdd36edf"},"schema_version":"1.0","source":{"id":"1601.01583","kind":"arxiv","version":2}},"canonical_sha256":"474e1cb092fffa358d6d5faca894ef2397be2ed41c3239fdf30aabe796fd3bf4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"474e1cb092fffa358d6d5faca894ef2397be2ed41c3239fdf30aabe796fd3bf4","first_computed_at":"2026-05-18T01:16:43.718564Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:16:43.718564Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"iKeeJ8aLOcfoVxoiqRAf93fz9E1QET0EKks/KHEuBYr40LVduena9fzt8dICyKNbRZVEeGmhy9JGZD6jxXPIBA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:16:43.719235Z","signed_message":"canonical_sha256_bytes"},"source_id":"1601.01583","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2074c09f50040800a29c5f89fbecd58bc6e796c7defa3a714f62074668798261","sha256:a213fde62e91cebcff50178a304ba5e71134d69f1652011e3fd15ac9f09f0c98"],"state_sha256":"3bbd39f4188daa72ad5930e314f4ec1f9201c6d33981f5c75b3bd71f2e83ebb8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IsBM0Y1hoxR5Z/UCe+VcsBpThGa3LWLprTIitF+c0NY9/KJa1UqzbgPiAZudCQo9ENFQfkw+TAfZDewY843cBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T09:16:52.191977Z","bundle_sha256":"3be558410192437bf8f7e460018cc5988c02d7a352a2bdc347300cc6f52cf5c0"}}