{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2005:HLJVDVIYYWJAMMJV4H763THEV3","short_pith_number":"pith:HLJVDVIY","canonical_record":{"source":{"id":"nucl-th/0512060","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2005-12-15T22:58:01Z","cross_cats_sorted":[],"title_canon_sha256":"f455deff221f0fed20fb3a6ee22d10639729471a6e85992cc6326706562ad265","abstract_canon_sha256":"21a15288fb0cddf0eba1aa370d3a661b86178a0b8ed4dbf5fb1f07408873d735"},"schema_version":"1.0"},"canonical_sha256":"3ad351d518c592063135e1ffedcce4aeda45fc53486c78e213d62f20841cfcb7","source":{"kind":"arxiv","id":"nucl-th/0512060","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0512060","created_at":"2026-05-18T00:37:06Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0512060v1","created_at":"2026-05-18T00:37:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0512060","created_at":"2026-05-18T00:37:06Z"},{"alias_kind":"pith_short_12","alias_value":"HLJVDVIYYWJA","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"HLJVDVIYYWJAMMJV","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"HLJVDVIY","created_at":"2026-05-18T12:25:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2005:HLJVDVIYYWJAMMJV4H763THEV3","target":"record","payload":{"canonical_record":{"source":{"id":"nucl-th/0512060","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2005-12-15T22:58:01Z","cross_cats_sorted":[],"title_canon_sha256":"f455deff221f0fed20fb3a6ee22d10639729471a6e85992cc6326706562ad265","abstract_canon_sha256":"21a15288fb0cddf0eba1aa370d3a661b86178a0b8ed4dbf5fb1f07408873d735"},"schema_version":"1.0"},"canonical_sha256":"3ad351d518c592063135e1ffedcce4aeda45fc53486c78e213d62f20841cfcb7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:37:06.943939Z","signature_b64":"sAEWvI6fhqX3r/w4QVT/TwAeRGi3TwMdKn0K0S+jSCNmSraQQz6Q5t+N5iRV+nfrn03Y0NUgVf6xaC+oL138AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3ad351d518c592063135e1ffedcce4aeda45fc53486c78e213d62f20841cfcb7","last_reissued_at":"2026-05-18T00:37:06.943393Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:37:06.943393Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"nucl-th/0512060","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":"2026-05-18T00:37:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FVFp41uyr/3yUTbmNcaMWy6UC3MLNejnfIqwIqPCWTvoLIQgl58q+vJSHkbcpsy4YC71iqgNCb82nGscsVEkBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T23:27:14.670061Z"},"content_sha256":"471b5bc157a5de8c7855cd7c3568de901076d06336c4d75379b77e1c49e09993","schema_version":"1.0","event_id":"sha256:471b5bc157a5de8c7855cd7c3568de901076d06336c4d75379b77e1c49e09993"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2005:HLJVDVIYYWJAMMJV4H763THEV3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Bose-Einstein or HBT correlation signature of a second order QCD phase transition","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"S. Hegyi, T. Csorgo, T. Novak, W. A. Zajc","submitted_at":"2005-12-15T22:58:01Z","abstract_excerpt":"For particles emerging from a second order QCD phase transition, we show that a recently introduced shape parameter of the Bose-Einstein correlation function, the Levy index of stability equals to the correlation exponent - one of the critical exponents that characterize the behavior of the matter in the vicinity of the second order phase transition point. Hence the shape of the Bose-Einstein / HBT correlation functions, when measured as a function of bombarding energy and centrality in various heavy ion reactions, can be utilized to locate experimentally the second order phase transition and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0512060","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":"2026-05-18T00:37:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2mYjAveFhNR1GqcC+PcLHoho44603OdSU3Z13UhXJfStvvhIGcYVXZzGHFQ4i5GYhJOjuYHIw/SCT08QJia7DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T23:27:14.670747Z"},"content_sha256":"29579d0de2f57fb6181faff6027bb39a58e33caced094ab7401a29f5bc4e8c18","schema_version":"1.0","event_id":"sha256:29579d0de2f57fb6181faff6027bb39a58e33caced094ab7401a29f5bc4e8c18"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HLJVDVIYYWJAMMJV4H763THEV3/bundle.json","state_url":"https://pith.science/pith/HLJVDVIYYWJAMMJV4H763THEV3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HLJVDVIYYWJAMMJV4H763THEV3/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":"2026-05-26T23:27:14Z","links":{"resolver":"https://pith.science/pith/HLJVDVIYYWJAMMJV4H763THEV3","bundle":"https://pith.science/pith/HLJVDVIYYWJAMMJV4H763THEV3/bundle.json","state":"https://pith.science/pith/HLJVDVIYYWJAMMJV4H763THEV3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HLJVDVIYYWJAMMJV4H763THEV3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2005:HLJVDVIYYWJAMMJV4H763THEV3","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":"21a15288fb0cddf0eba1aa370d3a661b86178a0b8ed4dbf5fb1f07408873d735","cross_cats_sorted":[],"license":"","primary_cat":"nucl-th","submitted_at":"2005-12-15T22:58:01Z","title_canon_sha256":"f455deff221f0fed20fb3a6ee22d10639729471a6e85992cc6326706562ad265"},"schema_version":"1.0","source":{"id":"nucl-th/0512060","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0512060","created_at":"2026-05-18T00:37:06Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0512060v1","created_at":"2026-05-18T00:37:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0512060","created_at":"2026-05-18T00:37:06Z"},{"alias_kind":"pith_short_12","alias_value":"HLJVDVIYYWJA","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"HLJVDVIYYWJAMMJV","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"HLJVDVIY","created_at":"2026-05-18T12:25:53Z"}],"graph_snapshots":[{"event_id":"sha256:29579d0de2f57fb6181faff6027bb39a58e33caced094ab7401a29f5bc4e8c18","target":"graph","created_at":"2026-05-18T00:37:06Z","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":"For particles emerging from a second order QCD phase transition, we show that a recently introduced shape parameter of the Bose-Einstein correlation function, the Levy index of stability equals to the correlation exponent - one of the critical exponents that characterize the behavior of the matter in the vicinity of the second order phase transition point. Hence the shape of the Bose-Einstein / HBT correlation functions, when measured as a function of bombarding energy and centrality in various heavy ion reactions, can be utilized to locate experimentally the second order phase transition and ","authors_text":"S. Hegyi, T. Csorgo, T. Novak, W. A. Zajc","cross_cats":[],"headline":"","license":"","primary_cat":"nucl-th","submitted_at":"2005-12-15T22:58:01Z","title":"Bose-Einstein or HBT correlation signature of a second order QCD phase transition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0512060","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":"sha256:471b5bc157a5de8c7855cd7c3568de901076d06336c4d75379b77e1c49e09993","target":"record","created_at":"2026-05-18T00:37:06Z","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":"21a15288fb0cddf0eba1aa370d3a661b86178a0b8ed4dbf5fb1f07408873d735","cross_cats_sorted":[],"license":"","primary_cat":"nucl-th","submitted_at":"2005-12-15T22:58:01Z","title_canon_sha256":"f455deff221f0fed20fb3a6ee22d10639729471a6e85992cc6326706562ad265"},"schema_version":"1.0","source":{"id":"nucl-th/0512060","kind":"arxiv","version":1}},"canonical_sha256":"3ad351d518c592063135e1ffedcce4aeda45fc53486c78e213d62f20841cfcb7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3ad351d518c592063135e1ffedcce4aeda45fc53486c78e213d62f20841cfcb7","first_computed_at":"2026-05-18T00:37:06.943393Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:37:06.943393Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"sAEWvI6fhqX3r/w4QVT/TwAeRGi3TwMdKn0K0S+jSCNmSraQQz6Q5t+N5iRV+nfrn03Y0NUgVf6xaC+oL138AA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:37:06.943939Z","signed_message":"canonical_sha256_bytes"},"source_id":"nucl-th/0512060","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:471b5bc157a5de8c7855cd7c3568de901076d06336c4d75379b77e1c49e09993","sha256:29579d0de2f57fb6181faff6027bb39a58e33caced094ab7401a29f5bc4e8c18"],"state_sha256":"851debff52271a0ba3827a26259ee7b5dad352c6d26e6dcefcfdd193d88b5680"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"V+3V5Ik8odz5Qgdls1OHysfSAqjp0/KZlazqOWnWcYAu9HI69Eiukm8dF8RQqUjOBJ1wW21bO4OPtm5GQt2yCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T23:27:14.674218Z","bundle_sha256":"5949f68798eb8ca87a3a78f0f4896926ecc6d12e28bc21aaa4372e3ab5eca9a4"}}