{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:LJGICBDGLJHGA2GJORFKJLWGB4","short_pith_number":"pith:LJGICBDG","schema_version":"1.0","canonical_sha256":"5a4c8104665a4e6068c9744aa4aec60f37d8ede9a0ab198a91a3d45778557d63","source":{"kind":"arxiv","id":"2208.13175","version":1},"attestation_state":"computed","paper":{"title":"Neutron-proton differential transverse flow in $^{132}$Sn + $^{124}$Sn collisions at 270 MeV/nucleon","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Gao-Feng Wei, Qi-jun Zhi, Xin Huang, You-chang Yang, Zheng-Wen Long","submitted_at":"2022-08-28T08:45:15Z","abstract_excerpt":"Within a transport model, we study the neutron-proton differential transverse flow and its excitation function in central $^{132}$Sn + $^{124}$Sn collisions at 270 MeV/nucleon. To more accurately evaluate effects of the high-density behavior of symmetry energy \\esym on this observable, we also consider the uncertainties of \\esym around the saturation density $\\rho_{0}$. It is shown that the neutron-proton differential transverse flow and its excitation function are mainly sensitive to the slope $L$ of \\esym at $\\rho_{0}$. However, the effects of low-density behavior of \\esym on this observable"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2208.13175","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2022-08-28T08:45:15Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"cd29ed80e761b8fd62eebf2a047e718b3a4426f54adaaa70c8a6e7cf9dcf64b2","abstract_canon_sha256":"5bbff9237fb2f49db86bb44515648f2c8d86251d84edd2eb4c4c3dbf41b0d241"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:52:04.570163Z","signature_b64":"FXo9z17jj9nby53SuGS3OHfSr9An8H3oM9Rw4m3cO/VH/JIvh0evG2Wbu4YRYRmM4XYSz1EwJ71rE+4GBVkwAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5a4c8104665a4e6068c9744aa4aec60f37d8ede9a0ab198a91a3d45778557d63","last_reissued_at":"2026-07-05T04:52:04.569538Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:52:04.569538Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Neutron-proton differential transverse flow in $^{132}$Sn + $^{124}$Sn collisions at 270 MeV/nucleon","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Gao-Feng Wei, Qi-jun Zhi, Xin Huang, You-chang Yang, Zheng-Wen Long","submitted_at":"2022-08-28T08:45:15Z","abstract_excerpt":"Within a transport model, we study the neutron-proton differential transverse flow and its excitation function in central $^{132}$Sn + $^{124}$Sn collisions at 270 MeV/nucleon. To more accurately evaluate effects of the high-density behavior of symmetry energy \\esym on this observable, we also consider the uncertainties of \\esym around the saturation density $\\rho_{0}$. It is shown that the neutron-proton differential transverse flow and its excitation function are mainly sensitive to the slope $L$ of \\esym at $\\rho_{0}$. However, the effects of low-density behavior of \\esym on this observable"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2208.13175","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2208.13175/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2208.13175","created_at":"2026-07-05T04:52:04.569605+00:00"},{"alias_kind":"arxiv_version","alias_value":"2208.13175v1","created_at":"2026-07-05T04:52:04.569605+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2208.13175","created_at":"2026-07-05T04:52:04.569605+00:00"},{"alias_kind":"pith_short_12","alias_value":"LJGICBDGLJHG","created_at":"2026-07-05T04:52:04.569605+00:00"},{"alias_kind":"pith_short_16","alias_value":"LJGICBDGLJHGA2GJ","created_at":"2026-07-05T04:52:04.569605+00:00"},{"alias_kind":"pith_short_8","alias_value":"LJGICBDG","created_at":"2026-07-05T04:52:04.569605+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.23476","citing_title":"In-medium effects of nucleon-nucleon cross sections in heavy-ion collisions","ref_index":43,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LJGICBDGLJHGA2GJORFKJLWGB4","json":"https://pith.science/pith/LJGICBDGLJHGA2GJORFKJLWGB4.json","graph_json":"https://pith.science/api/pith-number/LJGICBDGLJHGA2GJORFKJLWGB4/graph.json","events_json":"https://pith.science/api/pith-number/LJGICBDGLJHGA2GJORFKJLWGB4/events.json","paper":"https://pith.science/paper/LJGICBDG"},"agent_actions":{"view_html":"https://pith.science/pith/LJGICBDGLJHGA2GJORFKJLWGB4","download_json":"https://pith.science/pith/LJGICBDGLJHGA2GJORFKJLWGB4.json","view_paper":"https://pith.science/paper/LJGICBDG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2208.13175&json=true","fetch_graph":"https://pith.science/api/pith-number/LJGICBDGLJHGA2GJORFKJLWGB4/graph.json","fetch_events":"https://pith.science/api/pith-number/LJGICBDGLJHGA2GJORFKJLWGB4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LJGICBDGLJHGA2GJORFKJLWGB4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LJGICBDGLJHGA2GJORFKJLWGB4/action/storage_attestation","attest_author":"https://pith.science/pith/LJGICBDGLJHGA2GJORFKJLWGB4/action/author_attestation","sign_citation":"https://pith.science/pith/LJGICBDGLJHGA2GJORFKJLWGB4/action/citation_signature","submit_replication":"https://pith.science/pith/LJGICBDGLJHGA2GJORFKJLWGB4/action/replication_record"}},"created_at":"2026-07-05T04:52:04.569605+00:00","updated_at":"2026-07-05T04:52:04.569605+00:00"}