{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:FGJMLQKB3K24ZDDNMF23X44LQE","short_pith_number":"pith:FGJMLQKB","canonical_record":{"source":{"id":"1302.5766","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-02-23T06:16:40Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"4f77e4723fe6e0dbf4eef17e6b9d2936b8af1e958c0357858a4f6c8e8722a92a","abstract_canon_sha256":"a974c76f2b066d5c9985e1ee2839d844e9fa3eb31b282aaf183fe5b261966272"},"schema_version":"1.0"},"canonical_sha256":"2992c5c141dab5cc8c6d6175bbf38b8100f45deb3f191056b70ddd1ddce3f3d9","source":{"kind":"arxiv","id":"1302.5766","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.5766","created_at":"2026-05-18T03:01:33Z"},{"alias_kind":"arxiv_version","alias_value":"1302.5766v1","created_at":"2026-05-18T03:01:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.5766","created_at":"2026-05-18T03:01:33Z"},{"alias_kind":"pith_short_12","alias_value":"FGJMLQKB3K24","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"FGJMLQKB3K24ZDDN","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"FGJMLQKB","created_at":"2026-05-18T12:27:45Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:FGJMLQKB3K24ZDDNMF23X44LQE","target":"record","payload":{"canonical_record":{"source":{"id":"1302.5766","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-02-23T06:16:40Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"4f77e4723fe6e0dbf4eef17e6b9d2936b8af1e958c0357858a4f6c8e8722a92a","abstract_canon_sha256":"a974c76f2b066d5c9985e1ee2839d844e9fa3eb31b282aaf183fe5b261966272"},"schema_version":"1.0"},"canonical_sha256":"2992c5c141dab5cc8c6d6175bbf38b8100f45deb3f191056b70ddd1ddce3f3d9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:01:33.444753Z","signature_b64":"32k9s+BgYgh20JQFc3OjyeojZs4Ce7tJ6Ja1eoZtECtS4FvNQMke/Z9f+YAc59pLK/taJ5oY4y7vkCmMCWDKBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2992c5c141dab5cc8c6d6175bbf38b8100f45deb3f191056b70ddd1ddce3f3d9","last_reissued_at":"2026-05-18T03:01:33.444287Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:01:33.444287Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1302.5766","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":"2026-05-18T03:01:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DncquxdShs2oKRUSqZB5bHIUji427rNolO5EFg9fpUlv3yVVPt7IJcl0yRZMEYwRPSkwOvXHaWBr2/0KX8nODw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T22:32:11.838565Z"},"content_sha256":"ef35e6e774be6c071e6fbb5bd5805b41ff96b0e91e07074f0100f4a76e8127b9","schema_version":"1.0","event_id":"sha256:ef35e6e774be6c071e6fbb5bd5805b41ff96b0e91e07074f0100f4a76e8127b9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:FGJMLQKB3K24ZDDNMF23X44LQE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Alternative Scenarios of Relativistic Heavy-Ion Collisions: I. Baryon Stopping","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Yu.B. Ivanov","submitted_at":"2013-02-23T06:16:40Z","abstract_excerpt":"Simulations of relativistic heavy-ion collisions within the three-fluid model employing a purely hadronic equation of state (EoS) and two versions of the EoS involving deconfinement transition are presented. The latter are an EoS with the first-order phase transition and that with a smooth crossover transition. The model setup is described in detail. The analysis is performed in a wide range of incident energies 2.7 GeV $< \\sqrt{s_{NN}} <$ 39 GeV in terms of the center-of-mass energy. Results on proton and net-proton rapidity distributions are reported. Comparison with available data indicate "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.5766","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":"2026-05-18T03:01:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"b4OB4bfupy9mHikmaJVYDNQimsTzZWR/muD3t0ftADggZxhXfR+1tyVGg0YHK0MykStVu3v11pfwibb6n/MODw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T22:32:11.839045Z"},"content_sha256":"c03ffbda0c5fa4ba43935e75a132856351303f9d5811a129e7278b21e7557fb1","schema_version":"1.0","event_id":"sha256:c03ffbda0c5fa4ba43935e75a132856351303f9d5811a129e7278b21e7557fb1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FGJMLQKB3K24ZDDNMF23X44LQE/bundle.json","state_url":"https://pith.science/pith/FGJMLQKB3K24ZDDNMF23X44LQE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FGJMLQKB3K24ZDDNMF23X44LQE/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":"2026-08-03T22:32:11Z","links":{"resolver":"https://pith.science/pith/FGJMLQKB3K24ZDDNMF23X44LQE","bundle":"https://pith.science/pith/FGJMLQKB3K24ZDDNMF23X44LQE/bundle.json","state":"https://pith.science/pith/FGJMLQKB3K24ZDDNMF23X44LQE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FGJMLQKB3K24ZDDNMF23X44LQE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:FGJMLQKB3K24ZDDNMF23X44LQE","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":"a974c76f2b066d5c9985e1ee2839d844e9fa3eb31b282aaf183fe5b261966272","cross_cats_sorted":["hep-ph","nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-02-23T06:16:40Z","title_canon_sha256":"4f77e4723fe6e0dbf4eef17e6b9d2936b8af1e958c0357858a4f6c8e8722a92a"},"schema_version":"1.0","source":{"id":"1302.5766","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.5766","created_at":"2026-05-18T03:01:33Z"},{"alias_kind":"arxiv_version","alias_value":"1302.5766v1","created_at":"2026-05-18T03:01:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.5766","created_at":"2026-05-18T03:01:33Z"},{"alias_kind":"pith_short_12","alias_value":"FGJMLQKB3K24","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"FGJMLQKB3K24ZDDN","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"FGJMLQKB","created_at":"2026-05-18T12:27:45Z"}],"graph_snapshots":[{"event_id":"sha256:c03ffbda0c5fa4ba43935e75a132856351303f9d5811a129e7278b21e7557fb1","target":"graph","created_at":"2026-05-18T03:01:33Z","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":"Simulations of relativistic heavy-ion collisions within the three-fluid model employing a purely hadronic equation of state (EoS) and two versions of the EoS involving deconfinement transition are presented. The latter are an EoS with the first-order phase transition and that with a smooth crossover transition. The model setup is described in detail. The analysis is performed in a wide range of incident energies 2.7 GeV $< \\sqrt{s_{NN}} <$ 39 GeV in terms of the center-of-mass energy. Results on proton and net-proton rapidity distributions are reported. Comparison with available data indicate ","authors_text":"Yu.B. Ivanov","cross_cats":["hep-ph","nucl-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-02-23T06:16:40Z","title":"Alternative Scenarios of Relativistic Heavy-Ion Collisions: I. Baryon Stopping"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.5766","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:ef35e6e774be6c071e6fbb5bd5805b41ff96b0e91e07074f0100f4a76e8127b9","target":"record","created_at":"2026-05-18T03:01:33Z","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":"a974c76f2b066d5c9985e1ee2839d844e9fa3eb31b282aaf183fe5b261966272","cross_cats_sorted":["hep-ph","nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-02-23T06:16:40Z","title_canon_sha256":"4f77e4723fe6e0dbf4eef17e6b9d2936b8af1e958c0357858a4f6c8e8722a92a"},"schema_version":"1.0","source":{"id":"1302.5766","kind":"arxiv","version":1}},"canonical_sha256":"2992c5c141dab5cc8c6d6175bbf38b8100f45deb3f191056b70ddd1ddce3f3d9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2992c5c141dab5cc8c6d6175bbf38b8100f45deb3f191056b70ddd1ddce3f3d9","first_computed_at":"2026-05-18T03:01:33.444287Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:01:33.444287Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"32k9s+BgYgh20JQFc3OjyeojZs4Ce7tJ6Ja1eoZtECtS4FvNQMke/Z9f+YAc59pLK/taJ5oY4y7vkCmMCWDKBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:01:33.444753Z","signed_message":"canonical_sha256_bytes"},"source_id":"1302.5766","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ef35e6e774be6c071e6fbb5bd5805b41ff96b0e91e07074f0100f4a76e8127b9","sha256:c03ffbda0c5fa4ba43935e75a132856351303f9d5811a129e7278b21e7557fb1"],"state_sha256":"2bc56547125e07295eaad00afddb29c2b1855154036c70a44caa4de1e910b0a5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JmQ7Cx/6GyFb03VbX3Jvqyo1e0zL3I/nFv5oYa3qyEJFkEPcVjGuBumUDeRQS73ZmtjBcuev4jxgfZf+sdKeBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T22:32:11.843083Z","bundle_sha256":"4a19a0af32a3105b25f4eaece2241ac00689a98fa0fda5ded04c146456c971fd"}}