{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:VKAA2IINQUL2BHMDBBQAT2LFUW","short_pith_number":"pith:VKAA2IIN","canonical_record":{"source":{"id":"1701.05064","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-01-18T14:00:05Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"f8501d22c53495c40d36751060c6800ff98f638083287fcbe85e7ea67644158c","abstract_canon_sha256":"fa15a2ebc4703d0b67a057d426f925547740ea36757d4e1eabbe55dac79daea2"},"schema_version":"1.0"},"canonical_sha256":"aa800d210d8517a09d83086009e965a5b16b943f397d2b79ddddf5d54983605e","source":{"kind":"arxiv","id":"1701.05064","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1701.05064","created_at":"2026-05-18T00:44:23Z"},{"alias_kind":"arxiv_version","alias_value":"1701.05064v2","created_at":"2026-05-18T00:44:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.05064","created_at":"2026-05-18T00:44:23Z"},{"alias_kind":"pith_short_12","alias_value":"VKAA2IINQUL2","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"VKAA2IINQUL2BHMD","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"VKAA2IIN","created_at":"2026-05-18T12:31:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:VKAA2IINQUL2BHMDBBQAT2LFUW","target":"record","payload":{"canonical_record":{"source":{"id":"1701.05064","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-01-18T14:00:05Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"f8501d22c53495c40d36751060c6800ff98f638083287fcbe85e7ea67644158c","abstract_canon_sha256":"fa15a2ebc4703d0b67a057d426f925547740ea36757d4e1eabbe55dac79daea2"},"schema_version":"1.0"},"canonical_sha256":"aa800d210d8517a09d83086009e965a5b16b943f397d2b79ddddf5d54983605e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:44:23.772195Z","signature_b64":"7V+yNmizNj+JpQcKR3VIi+XMmpLiMAc4+o3Z0Fve8cBGuNFK0qa1YNWx60OTxBarkC+Ln0GNQEoUL9EqvMM7Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aa800d210d8517a09d83086009e965a5b16b943f397d2b79ddddf5d54983605e","last_reissued_at":"2026-05-18T00:44:23.770390Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:44:23.770390Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1701.05064","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":"2026-05-18T00:44:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UIsS8wM/bFVBwc4jH/jvvfG8IqryOvg+BSxRviu/4sDNL/x9Dbvx8whKUsdqZ9C+zHB46HX5mdXIzVth8rz5Bw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-19T13:01:17.470886Z"},"content_sha256":"1494572b3a9257951b2cc10094786f4eaea637b4203c112e307fc67388db8fb3","schema_version":"1.0","event_id":"sha256:1494572b3a9257951b2cc10094786f4eaea637b4203c112e307fc67388db8fb3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:VKAA2IINQUL2BHMDBBQAT2LFUW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Parametric estimate of the relative photon yields from the Glasma and the Quark-Gluon Plasma in heavy-ion collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"J. Berges, K. Reygers, N. Tanji, R. Venugopalan","submitted_at":"2017-01-18T14:00:05Z","abstract_excerpt":"Recent classical-statistical numerical simulations have established the \"bottom-up\" thermalization scenario of Baier et al. as the correct weak coupling effective theory for thermalization in ultrarelativistic heavy-ion collisions. We perform a parametric study of photon production in the various stages of this bottom-up framework to ascertain the relative contribution of the off-equilibrium \"Glasma\" relative to that of a thermalized Quark-Gluon Plasma. Taking into account the constraints imposed by the measured charged hadron multiplicities at RHIC and the LHC, we find that Glasma contributio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.05064","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":"2026-05-18T00:44:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Oq9uAH3NmnZgOL1xgFhqFj9XW0NfTHAr0nDgbpOOxPsfmOwzPhlxpGZqHg98yT1iXXOJvQrt1ssW1bJq4ueKBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-19T13:01:17.471224Z"},"content_sha256":"9f99a14c4701bbf18a796fe493e37d78524021cdc2a7a4d4bdec9c31415b6aad","schema_version":"1.0","event_id":"sha256:9f99a14c4701bbf18a796fe493e37d78524021cdc2a7a4d4bdec9c31415b6aad"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VKAA2IINQUL2BHMDBBQAT2LFUW/bundle.json","state_url":"https://pith.science/pith/VKAA2IINQUL2BHMDBBQAT2LFUW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VKAA2IINQUL2BHMDBBQAT2LFUW/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":"2026-05-19T13:01:17Z","links":{"resolver":"https://pith.science/pith/VKAA2IINQUL2BHMDBBQAT2LFUW","bundle":"https://pith.science/pith/VKAA2IINQUL2BHMDBBQAT2LFUW/bundle.json","state":"https://pith.science/pith/VKAA2IINQUL2BHMDBBQAT2LFUW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VKAA2IINQUL2BHMDBBQAT2LFUW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:VKAA2IINQUL2BHMDBBQAT2LFUW","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":"fa15a2ebc4703d0b67a057d426f925547740ea36757d4e1eabbe55dac79daea2","cross_cats_sorted":["hep-ph","nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-01-18T14:00:05Z","title_canon_sha256":"f8501d22c53495c40d36751060c6800ff98f638083287fcbe85e7ea67644158c"},"schema_version":"1.0","source":{"id":"1701.05064","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1701.05064","created_at":"2026-05-18T00:44:23Z"},{"alias_kind":"arxiv_version","alias_value":"1701.05064v2","created_at":"2026-05-18T00:44:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.05064","created_at":"2026-05-18T00:44:23Z"},{"alias_kind":"pith_short_12","alias_value":"VKAA2IINQUL2","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"VKAA2IINQUL2BHMD","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"VKAA2IIN","created_at":"2026-05-18T12:31:49Z"}],"graph_snapshots":[{"event_id":"sha256:9f99a14c4701bbf18a796fe493e37d78524021cdc2a7a4d4bdec9c31415b6aad","target":"graph","created_at":"2026-05-18T00:44:23Z","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":"Recent classical-statistical numerical simulations have established the \"bottom-up\" thermalization scenario of Baier et al. as the correct weak coupling effective theory for thermalization in ultrarelativistic heavy-ion collisions. We perform a parametric study of photon production in the various stages of this bottom-up framework to ascertain the relative contribution of the off-equilibrium \"Glasma\" relative to that of a thermalized Quark-Gluon Plasma. Taking into account the constraints imposed by the measured charged hadron multiplicities at RHIC and the LHC, we find that Glasma contributio","authors_text":"J. Berges, K. Reygers, N. Tanji, R. Venugopalan","cross_cats":["hep-ph","nucl-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-01-18T14:00:05Z","title":"Parametric estimate of the relative photon yields from the Glasma and the Quark-Gluon Plasma in heavy-ion collisions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.05064","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":"sha256:1494572b3a9257951b2cc10094786f4eaea637b4203c112e307fc67388db8fb3","target":"record","created_at":"2026-05-18T00:44:23Z","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":"fa15a2ebc4703d0b67a057d426f925547740ea36757d4e1eabbe55dac79daea2","cross_cats_sorted":["hep-ph","nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-01-18T14:00:05Z","title_canon_sha256":"f8501d22c53495c40d36751060c6800ff98f638083287fcbe85e7ea67644158c"},"schema_version":"1.0","source":{"id":"1701.05064","kind":"arxiv","version":2}},"canonical_sha256":"aa800d210d8517a09d83086009e965a5b16b943f397d2b79ddddf5d54983605e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"aa800d210d8517a09d83086009e965a5b16b943f397d2b79ddddf5d54983605e","first_computed_at":"2026-05-18T00:44:23.770390Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:44:23.770390Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7V+yNmizNj+JpQcKR3VIi+XMmpLiMAc4+o3Z0Fve8cBGuNFK0qa1YNWx60OTxBarkC+Ln0GNQEoUL9EqvMM7Cw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:44:23.772195Z","signed_message":"canonical_sha256_bytes"},"source_id":"1701.05064","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1494572b3a9257951b2cc10094786f4eaea637b4203c112e307fc67388db8fb3","sha256:9f99a14c4701bbf18a796fe493e37d78524021cdc2a7a4d4bdec9c31415b6aad"],"state_sha256":"fff191e7de796b5b5d0e7e65e1914e178a53dcf6a74708ae4d3fc5e20cb8a425"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YSfFO7wNM5iNVIpM9XGHSxyb+QuznM7edgtdaJjodt72m+at+/yrzjrKbZUMpEQ0nJ+uSL1bu60Qno81R9vhDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-19T13:01:17.472815Z","bundle_sha256":"be06e030a83adf86a568d5b1121fdf5693f45dd2baa9df79c3eafd1e9831b077"}}