{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:MGETTEKI26QSFETNV7YOZHS5VD","short_pith_number":"pith:MGETTEKI","canonical_record":{"source":{"id":"1604.05513","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.data-an","submitted_at":"2016-04-19T10:50:03Z","cross_cats_sorted":["hep-ex","hep-ph","nucl-ex","nucl-th"],"title_canon_sha256":"e9c5decea034d07d26a15087969085911a22211c7e439110bcb6ef1f63aa82c3","abstract_canon_sha256":"a138ca35a5d21d18745196d5f44c1dd68c4bcd3ddafe2c2843aaf9120893074a"},"schema_version":"1.0"},"canonical_sha256":"6189399148d7a122926daff0ec9e5da8d2ab9f4f24d526afa4bb34b2a3342bf9","source":{"kind":"arxiv","id":"1604.05513","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.05513","created_at":"2026-05-18T01:16:12Z"},{"alias_kind":"arxiv_version","alias_value":"1604.05513v1","created_at":"2026-05-18T01:16:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.05513","created_at":"2026-05-18T01:16:12Z"},{"alias_kind":"pith_short_12","alias_value":"MGETTEKI26QS","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"MGETTEKI26QSFETN","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"MGETTEKI","created_at":"2026-05-18T12:30:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:MGETTEKI26QSFETNV7YOZHS5VD","target":"record","payload":{"canonical_record":{"source":{"id":"1604.05513","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.data-an","submitted_at":"2016-04-19T10:50:03Z","cross_cats_sorted":["hep-ex","hep-ph","nucl-ex","nucl-th"],"title_canon_sha256":"e9c5decea034d07d26a15087969085911a22211c7e439110bcb6ef1f63aa82c3","abstract_canon_sha256":"a138ca35a5d21d18745196d5f44c1dd68c4bcd3ddafe2c2843aaf9120893074a"},"schema_version":"1.0"},"canonical_sha256":"6189399148d7a122926daff0ec9e5da8d2ab9f4f24d526afa4bb34b2a3342bf9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:16:12.705478Z","signature_b64":"fZDcFaeVGf6JENa0t/cX8Iea8GMaXX+2t+JMiUiZTPNEfOt4geN4LSN9Tf8iaFwWEN4xL7GXmv/fuYgID0ZPCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6189399148d7a122926daff0ec9e5da8d2ab9f4f24d526afa4bb34b2a3342bf9","last_reissued_at":"2026-05-18T01:16:12.704821Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:16:12.704821Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1604.05513","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:16:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HAeGFpbZWga8I9CyjLsrOrp2LXQcXarm+oTZqF6PmQWhHPRAww3avYV/JcZGn7sjjFvFTNuFDheibgmbBGDmAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T15:38:45.703960Z"},"content_sha256":"f25a1d4edd30207549293e196fd2ae48b5a636915236dda911d66ab2563a0c0f","schema_version":"1.0","event_id":"sha256:f25a1d4edd30207549293e196fd2ae48b5a636915236dda911d66ab2563a0c0f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:MGETTEKI26QSFETNV7YOZHS5VD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Model independent analysis of nearly L\\'evy correlations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-ph","nucl-ex","nucl-th"],"primary_cat":"physics.data-an","authors_text":"H. C. Eggers, M. de Kock, T. Cs\\\"org\\H{o}, T. Nov\\'ak","submitted_at":"2016-04-19T10:50:03Z","abstract_excerpt":"A model-independent method for the analysis of the two-particle short-range correlations is presented, that can be utilized to describe e.g. Bose-Einstein (HBT), dynamical (ridge) or other correlation functions, that have a nearly L\\'evy or streched exponential shape. For the special case of L\\'evy exponent alpha = 1, the earlier Laguerre expansions are recovered, for the alpha = 2 special case, a new expansion method is obtained for nearly Gaussian correlation functions. Multi-dimensional L\\'evy expansions are also introduced and their potential application to analyze rigde correlation data i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.05513","kind":"arxiv","version":1},"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":"2026-05-18T01:16:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"42FFSeh4T7qQIZ81rmCAA4EdLVZbs2u0srdhHg2pdRB+PUMK8xgi+IjlvXjQJZZZPPMBbbwUwxbPdntW5OKVAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T15:38:45.704636Z"},"content_sha256":"50327be4389dde0e221eff45f10acf049d44f57d381c3fb1176a2d5acf77d87a","schema_version":"1.0","event_id":"sha256:50327be4389dde0e221eff45f10acf049d44f57d381c3fb1176a2d5acf77d87a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MGETTEKI26QSFETNV7YOZHS5VD/bundle.json","state_url":"https://pith.science/pith/MGETTEKI26QSFETNV7YOZHS5VD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MGETTEKI26QSFETNV7YOZHS5VD/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":"2026-06-06T15:38:45Z","links":{"resolver":"https://pith.science/pith/MGETTEKI26QSFETNV7YOZHS5VD","bundle":"https://pith.science/pith/MGETTEKI26QSFETNV7YOZHS5VD/bundle.json","state":"https://pith.science/pith/MGETTEKI26QSFETNV7YOZHS5VD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MGETTEKI26QSFETNV7YOZHS5VD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:MGETTEKI26QSFETNV7YOZHS5VD","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":"a138ca35a5d21d18745196d5f44c1dd68c4bcd3ddafe2c2843aaf9120893074a","cross_cats_sorted":["hep-ex","hep-ph","nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.data-an","submitted_at":"2016-04-19T10:50:03Z","title_canon_sha256":"e9c5decea034d07d26a15087969085911a22211c7e439110bcb6ef1f63aa82c3"},"schema_version":"1.0","source":{"id":"1604.05513","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.05513","created_at":"2026-05-18T01:16:12Z"},{"alias_kind":"arxiv_version","alias_value":"1604.05513v1","created_at":"2026-05-18T01:16:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.05513","created_at":"2026-05-18T01:16:12Z"},{"alias_kind":"pith_short_12","alias_value":"MGETTEKI26QS","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"MGETTEKI26QSFETN","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"MGETTEKI","created_at":"2026-05-18T12:30:32Z"}],"graph_snapshots":[{"event_id":"sha256:50327be4389dde0e221eff45f10acf049d44f57d381c3fb1176a2d5acf77d87a","target":"graph","created_at":"2026-05-18T01:16:12Z","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":"A model-independent method for the analysis of the two-particle short-range correlations is presented, that can be utilized to describe e.g. Bose-Einstein (HBT), dynamical (ridge) or other correlation functions, that have a nearly L\\'evy or streched exponential shape. For the special case of L\\'evy exponent alpha = 1, the earlier Laguerre expansions are recovered, for the alpha = 2 special case, a new expansion method is obtained for nearly Gaussian correlation functions. Multi-dimensional L\\'evy expansions are also introduced and their potential application to analyze rigde correlation data i","authors_text":"H. C. Eggers, M. de Kock, T. Cs\\\"org\\H{o}, T. Nov\\'ak","cross_cats":["hep-ex","hep-ph","nucl-ex","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.data-an","submitted_at":"2016-04-19T10:50:03Z","title":"Model independent analysis of nearly L\\'evy correlations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.05513","kind":"arxiv","version":1},"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:f25a1d4edd30207549293e196fd2ae48b5a636915236dda911d66ab2563a0c0f","target":"record","created_at":"2026-05-18T01:16:12Z","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":"a138ca35a5d21d18745196d5f44c1dd68c4bcd3ddafe2c2843aaf9120893074a","cross_cats_sorted":["hep-ex","hep-ph","nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.data-an","submitted_at":"2016-04-19T10:50:03Z","title_canon_sha256":"e9c5decea034d07d26a15087969085911a22211c7e439110bcb6ef1f63aa82c3"},"schema_version":"1.0","source":{"id":"1604.05513","kind":"arxiv","version":1}},"canonical_sha256":"6189399148d7a122926daff0ec9e5da8d2ab9f4f24d526afa4bb34b2a3342bf9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6189399148d7a122926daff0ec9e5da8d2ab9f4f24d526afa4bb34b2a3342bf9","first_computed_at":"2026-05-18T01:16:12.704821Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:16:12.704821Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"fZDcFaeVGf6JENa0t/cX8Iea8GMaXX+2t+JMiUiZTPNEfOt4geN4LSN9Tf8iaFwWEN4xL7GXmv/fuYgID0ZPCA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:16:12.705478Z","signed_message":"canonical_sha256_bytes"},"source_id":"1604.05513","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f25a1d4edd30207549293e196fd2ae48b5a636915236dda911d66ab2563a0c0f","sha256:50327be4389dde0e221eff45f10acf049d44f57d381c3fb1176a2d5acf77d87a"],"state_sha256":"3076187dd6725805062ee037671f03adb3e3161a6494df37af92aa66fe470ef2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cx76lfAkgsU6mFNYkcdHxmLcScgz6Nd4b1saCdbo1zqmATPeDnJwosxpdUu3hrxAokCFiSpc12PeCM+FxmM4Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T15:38:45.708044Z","bundle_sha256":"9cc1e99d0f85a637baace15d468c1ac734093415b2618084499e46d14b6470a1"}}