{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2006:NVLVBP6W4FOWIRNNMIYPAT5AAJ","short_pith_number":"pith:NVLVBP6W","canonical_record":{"source":{"id":"nucl-th/0611017","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2006-11-07T08:33:53Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"7e74edb91dc4bed113553528efee8a95fbdfdfe2670c85179750891fb0ffc6a0","abstract_canon_sha256":"8ef1dbbcebe8504a5b2eeb0d9f277e3ad9f60a3703d9288979947a599e4a76a2"},"schema_version":"1.0"},"canonical_sha256":"6d5750bfd6e15d6445ad6230f04fa002691aac9db13efb8f0b70d6b6c9da9868","source":{"kind":"arxiv","id":"nucl-th/0611017","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0611017","created_at":"2026-07-04T15:22:13Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0611017v2","created_at":"2026-07-04T15:22:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0611017","created_at":"2026-07-04T15:22:13Z"},{"alias_kind":"pith_short_12","alias_value":"NVLVBP6W4FOW","created_at":"2026-07-04T15:22:13Z"},{"alias_kind":"pith_short_16","alias_value":"NVLVBP6W4FOWIRNN","created_at":"2026-07-04T15:22:13Z"},{"alias_kind":"pith_short_8","alias_value":"NVLVBP6W","created_at":"2026-07-04T15:22:13Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2006:NVLVBP6W4FOWIRNNMIYPAT5AAJ","target":"record","payload":{"canonical_record":{"source":{"id":"nucl-th/0611017","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2006-11-07T08:33:53Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"7e74edb91dc4bed113553528efee8a95fbdfdfe2670c85179750891fb0ffc6a0","abstract_canon_sha256":"8ef1dbbcebe8504a5b2eeb0d9f277e3ad9f60a3703d9288979947a599e4a76a2"},"schema_version":"1.0"},"canonical_sha256":"6d5750bfd6e15d6445ad6230f04fa002691aac9db13efb8f0b70d6b6c9da9868","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:22:13.861669Z","signature_b64":"6s0zN9lXVcZM1zKEhLynoENbhfDlpqxfU6HVPeXfBjxHku8v82+gfeeHMSSEYXWfNTqb/ROKdFQYYqiejBV+Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6d5750bfd6e15d6445ad6230f04fa002691aac9db13efb8f0b70d6b6c9da9868","last_reissued_at":"2026-07-04T15:22:13.861235Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:22:13.861235Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"nucl-th/0611017","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":"2026-07-04T15:22:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3bOi7GXJNkyrD509dcwFTrH0JZa37NuyT+kR65BkyC2cNF2QtxslYCxHf6dDyKabdEUWVaxwj3FcUvlcE4ybCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T15:10:41.140140Z"},"content_sha256":"4a0187fdd9ee178af40c82784df1eca120ac6ef208469ce9e91f8c58da0f3aba","schema_version":"1.0","event_id":"sha256:4a0187fdd9ee178af40c82784df1eca120ac6ef208469ce9e91f8c58da0f3aba"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2006:NVLVBP6W4FOWIRNNMIYPAT5AAJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Effects of fluctuations on the initial eccentricity from the Color Glass Condensate in heavy ion collisions","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"H.-J. Drescher, Y. Nara","submitted_at":"2006-11-07T08:33:53Z","abstract_excerpt":"We introduce a modified form of the Kharzeev-Levin-Nardi (KLN) approach for nuclear collisions. The new ansatz for the unintegrated gluon distribution function preserves factorization, and the saturation scale is bound from below by that for a single nucleon. It also reproduces the correct scaling with the number of collisions at high transverse momentum. The corresponding Monte Carlo implementation allows us to account for fluctuations of the hard sources (nucleons) in the transverse plane. We compute various definitions of the eccentricity within the new approach, which are relevant for the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0611017","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/nucl-th/0611017/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":"2026-07-04T15:22:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YXKSHxHEG+edP3UpLVB147eu13hVgaMiMB0+GI5QDEsUfUF/VgSElUbDoDi+KCy4TcpnFUsVmv5A8yeSEnbvDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T15:10:41.140729Z"},"content_sha256":"76f8ddaea0a12e0d04f539a2a8d46a51a1bdbed7203ff490c3140382482cab7a","schema_version":"1.0","event_id":"sha256:76f8ddaea0a12e0d04f539a2a8d46a51a1bdbed7203ff490c3140382482cab7a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NVLVBP6W4FOWIRNNMIYPAT5AAJ/bundle.json","state_url":"https://pith.science/pith/NVLVBP6W4FOWIRNNMIYPAT5AAJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NVLVBP6W4FOWIRNNMIYPAT5AAJ/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":"2026-08-04T15:10:41Z","links":{"resolver":"https://pith.science/pith/NVLVBP6W4FOWIRNNMIYPAT5AAJ","bundle":"https://pith.science/pith/NVLVBP6W4FOWIRNNMIYPAT5AAJ/bundle.json","state":"https://pith.science/pith/NVLVBP6W4FOWIRNNMIYPAT5AAJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NVLVBP6W4FOWIRNNMIYPAT5AAJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2006:NVLVBP6W4FOWIRNNMIYPAT5AAJ","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":"8ef1dbbcebe8504a5b2eeb0d9f277e3ad9f60a3703d9288979947a599e4a76a2","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"nucl-th","submitted_at":"2006-11-07T08:33:53Z","title_canon_sha256":"7e74edb91dc4bed113553528efee8a95fbdfdfe2670c85179750891fb0ffc6a0"},"schema_version":"1.0","source":{"id":"nucl-th/0611017","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0611017","created_at":"2026-07-04T15:22:13Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0611017v2","created_at":"2026-07-04T15:22:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0611017","created_at":"2026-07-04T15:22:13Z"},{"alias_kind":"pith_short_12","alias_value":"NVLVBP6W4FOW","created_at":"2026-07-04T15:22:13Z"},{"alias_kind":"pith_short_16","alias_value":"NVLVBP6W4FOWIRNN","created_at":"2026-07-04T15:22:13Z"},{"alias_kind":"pith_short_8","alias_value":"NVLVBP6W","created_at":"2026-07-04T15:22:13Z"}],"graph_snapshots":[{"event_id":"sha256:76f8ddaea0a12e0d04f539a2a8d46a51a1bdbed7203ff490c3140382482cab7a","target":"graph","created_at":"2026-07-04T15:22:13Z","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/nucl-th/0611017/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We introduce a modified form of the Kharzeev-Levin-Nardi (KLN) approach for nuclear collisions. The new ansatz for the unintegrated gluon distribution function preserves factorization, and the saturation scale is bound from below by that for a single nucleon. It also reproduces the correct scaling with the number of collisions at high transverse momentum. The corresponding Monte Carlo implementation allows us to account for fluctuations of the hard sources (nucleons) in the transverse plane. We compute various definitions of the eccentricity within the new approach, which are relevant for the ","authors_text":"H.-J. Drescher, Y. Nara","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"nucl-th","submitted_at":"2006-11-07T08:33:53Z","title":"Effects of fluctuations on the initial eccentricity from the Color Glass Condensate in heavy ion collisions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0611017","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":"sha256:4a0187fdd9ee178af40c82784df1eca120ac6ef208469ce9e91f8c58da0f3aba","target":"record","created_at":"2026-07-04T15:22:13Z","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":"8ef1dbbcebe8504a5b2eeb0d9f277e3ad9f60a3703d9288979947a599e4a76a2","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"nucl-th","submitted_at":"2006-11-07T08:33:53Z","title_canon_sha256":"7e74edb91dc4bed113553528efee8a95fbdfdfe2670c85179750891fb0ffc6a0"},"schema_version":"1.0","source":{"id":"nucl-th/0611017","kind":"arxiv","version":2}},"canonical_sha256":"6d5750bfd6e15d6445ad6230f04fa002691aac9db13efb8f0b70d6b6c9da9868","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6d5750bfd6e15d6445ad6230f04fa002691aac9db13efb8f0b70d6b6c9da9868","first_computed_at":"2026-07-04T15:22:13.861235Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:22:13.861235Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6s0zN9lXVcZM1zKEhLynoENbhfDlpqxfU6HVPeXfBjxHku8v82+gfeeHMSSEYXWfNTqb/ROKdFQYYqiejBV+Aw==","signature_status":"signed_v1","signed_at":"2026-07-04T15:22:13.861669Z","signed_message":"canonical_sha256_bytes"},"source_id":"nucl-th/0611017","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4a0187fdd9ee178af40c82784df1eca120ac6ef208469ce9e91f8c58da0f3aba","sha256:76f8ddaea0a12e0d04f539a2a8d46a51a1bdbed7203ff490c3140382482cab7a"],"state_sha256":"59efcb84810059b82bf1925150b65da89d81a4530a34bf4420e6ae0ddbec4617"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AWM8RAzLAwndWgeM82zPyZE5586oi4kKMzKvI3Ld7vH+6lJS6/DOFLNwJ+dfM6YpoSla0yLsKHQ7GYX1ntB4Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T15:10:41.169728Z","bundle_sha256":"1cfb3e20b48ff7faf48f635268c8761a283f7a9313a5e01187abac7785e3cdc4"}}