{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:DW25KDFAQXQFZ7ALUBWSWKXWY2","short_pith_number":"pith:DW25KDFA","canonical_record":{"source":{"id":"1405.2632","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-05-12T05:45:33Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"ee3d48d9db1c6afd152cb3e99987542b69fecb79c4662b6180b805e912c4fc05","abstract_canon_sha256":"be8c3d754c2178b59a009e25f60fc9317c761d6ecbb44da0d46258553b29c241"},"schema_version":"1.0"},"canonical_sha256":"1db5d50ca085e05cfc0ba06d2b2af6c690a99e7c1c4da1fb10d4422e72dd792e","source":{"kind":"arxiv","id":"1405.2632","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1405.2632","created_at":"2026-05-18T02:38:29Z"},{"alias_kind":"arxiv_version","alias_value":"1405.2632v2","created_at":"2026-05-18T02:38:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.2632","created_at":"2026-05-18T02:38:29Z"},{"alias_kind":"pith_short_12","alias_value":"DW25KDFAQXQF","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"DW25KDFAQXQFZ7AL","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"DW25KDFA","created_at":"2026-05-18T12:28:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:DW25KDFAQXQFZ7ALUBWSWKXWY2","target":"record","payload":{"canonical_record":{"source":{"id":"1405.2632","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-05-12T05:45:33Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"ee3d48d9db1c6afd152cb3e99987542b69fecb79c4662b6180b805e912c4fc05","abstract_canon_sha256":"be8c3d754c2178b59a009e25f60fc9317c761d6ecbb44da0d46258553b29c241"},"schema_version":"1.0"},"canonical_sha256":"1db5d50ca085e05cfc0ba06d2b2af6c690a99e7c1c4da1fb10d4422e72dd792e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:38:29.573064Z","signature_b64":"osIYRuB2M9zjS6Qs/oAN671TevUdjoVxxO/jH5qs+7zhWzWfZEvgVenvkoQJQAlk0DZsV3eur/83dPR8Y3QYBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1db5d50ca085e05cfc0ba06d2b2af6c690a99e7c1c4da1fb10d4422e72dd792e","last_reissued_at":"2026-05-18T02:38:29.572417Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:38:29.572417Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1405.2632","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":"2026-05-18T02:38:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"e3ZmMG/wo2a8Os0VVZDbaOUxOOZ0cqs6If83TvYH7VGkDYnX9u/Hk9dJk5q4DIoIr7tkvqTaJnuKYw1Uy+aeDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-18T23:48:07.240175Z"},"content_sha256":"e114642c293a2f530c3d24a05af7f811923623bb0fcb5076a09134c2d0e9c199","schema_version":"1.0","event_id":"sha256:e114642c293a2f530c3d24a05af7f811923623bb0fcb5076a09134c2d0e9c199"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:DW25KDFAQXQFZ7ALUBWSWKXWY2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Production of Light Nuclei in Heavy Ion Collisions Within Multiple Freezeout Scenario","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Bedangadas Mohanty, Sandeep Chatterjee","submitted_at":"2014-05-12T05:45:33Z","abstract_excerpt":"We discuss the production of light nuclei in heavy ion collisions within a multiple freezeout scenario. Thermal parameters extracted from the fits to the observed hadron yields are used to predict the multiplicities of light nuclei. Ratios of strange to non strange nuclei are found to be most sensitive to the details of the chemical freezeout. The well known disagreement between data of $^3_\\Lambda\\text{H/}^3\\text{He}$ and $\\overline{^3_\\Lambda\\text{H/}^3\\text{He}}$ at $\\sqrt{s_{NN}}=200$ GeV and models based on thermal as well as simple coalescence using a single chemical freezeout surface go"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.2632","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":"2026-05-18T02:38:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dgOaw9qSJbqQdM50mEY+Z9tCulea+/LmCnKPsxWIF0mce8PguZr0EdnPEk3MXkGR3oYZiHS70P1qZsqIdk52CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-18T23:48:07.240547Z"},"content_sha256":"53d7d2c3b7668fd5639e7da88f7d078ea01eb0bb0083e7e0640a72eaac5a3099","schema_version":"1.0","event_id":"sha256:53d7d2c3b7668fd5639e7da88f7d078ea01eb0bb0083e7e0640a72eaac5a3099"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DW25KDFAQXQFZ7ALUBWSWKXWY2/bundle.json","state_url":"https://pith.science/pith/DW25KDFAQXQFZ7ALUBWSWKXWY2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DW25KDFAQXQFZ7ALUBWSWKXWY2/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":"2026-05-18T23:48:07Z","links":{"resolver":"https://pith.science/pith/DW25KDFAQXQFZ7ALUBWSWKXWY2","bundle":"https://pith.science/pith/DW25KDFAQXQFZ7ALUBWSWKXWY2/bundle.json","state":"https://pith.science/pith/DW25KDFAQXQFZ7ALUBWSWKXWY2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DW25KDFAQXQFZ7ALUBWSWKXWY2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:DW25KDFAQXQFZ7ALUBWSWKXWY2","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":"be8c3d754c2178b59a009e25f60fc9317c761d6ecbb44da0d46258553b29c241","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-05-12T05:45:33Z","title_canon_sha256":"ee3d48d9db1c6afd152cb3e99987542b69fecb79c4662b6180b805e912c4fc05"},"schema_version":"1.0","source":{"id":"1405.2632","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1405.2632","created_at":"2026-05-18T02:38:29Z"},{"alias_kind":"arxiv_version","alias_value":"1405.2632v2","created_at":"2026-05-18T02:38:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.2632","created_at":"2026-05-18T02:38:29Z"},{"alias_kind":"pith_short_12","alias_value":"DW25KDFAQXQF","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"DW25KDFAQXQFZ7AL","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"DW25KDFA","created_at":"2026-05-18T12:28:25Z"}],"graph_snapshots":[{"event_id":"sha256:53d7d2c3b7668fd5639e7da88f7d078ea01eb0bb0083e7e0640a72eaac5a3099","target":"graph","created_at":"2026-05-18T02:38:29Z","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":"We discuss the production of light nuclei in heavy ion collisions within a multiple freezeout scenario. Thermal parameters extracted from the fits to the observed hadron yields are used to predict the multiplicities of light nuclei. Ratios of strange to non strange nuclei are found to be most sensitive to the details of the chemical freezeout. The well known disagreement between data of $^3_\\Lambda\\text{H/}^3\\text{He}$ and $\\overline{^3_\\Lambda\\text{H/}^3\\text{He}}$ at $\\sqrt{s_{NN}}=200$ GeV and models based on thermal as well as simple coalescence using a single chemical freezeout surface go","authors_text":"Bedangadas Mohanty, Sandeep Chatterjee","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-05-12T05:45:33Z","title":"Production of Light Nuclei in Heavy Ion Collisions Within Multiple Freezeout Scenario"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.2632","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:e114642c293a2f530c3d24a05af7f811923623bb0fcb5076a09134c2d0e9c199","target":"record","created_at":"2026-05-18T02:38:29Z","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":"be8c3d754c2178b59a009e25f60fc9317c761d6ecbb44da0d46258553b29c241","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-05-12T05:45:33Z","title_canon_sha256":"ee3d48d9db1c6afd152cb3e99987542b69fecb79c4662b6180b805e912c4fc05"},"schema_version":"1.0","source":{"id":"1405.2632","kind":"arxiv","version":2}},"canonical_sha256":"1db5d50ca085e05cfc0ba06d2b2af6c690a99e7c1c4da1fb10d4422e72dd792e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1db5d50ca085e05cfc0ba06d2b2af6c690a99e7c1c4da1fb10d4422e72dd792e","first_computed_at":"2026-05-18T02:38:29.572417Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:38:29.572417Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"osIYRuB2M9zjS6Qs/oAN671TevUdjoVxxO/jH5qs+7zhWzWfZEvgVenvkoQJQAlk0DZsV3eur/83dPR8Y3QYBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:38:29.573064Z","signed_message":"canonical_sha256_bytes"},"source_id":"1405.2632","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e114642c293a2f530c3d24a05af7f811923623bb0fcb5076a09134c2d0e9c199","sha256:53d7d2c3b7668fd5639e7da88f7d078ea01eb0bb0083e7e0640a72eaac5a3099"],"state_sha256":"4cbb0a8f81faf07e6ce5056107f3ddcb30c78f410630ad0b146a68bfa83b8f6c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rffqp1Q0Wdak7YHieUYzmMtT+isYvzDeDEdq4s+9qp2j9Eko8El6m3EGABAr4JmzpS+6iZ5koNCIaqfbNpShDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-18T23:48:07.242186Z","bundle_sha256":"cf2623283019d0acfd098d90da0fa5553d399f93eadfb099e66fdd68e954bd31"}}