{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:BXR6J6BFAQL7J5QSDYANGL3K3V","short_pith_number":"pith:BXR6J6BF","schema_version":"1.0","canonical_sha256":"0de3e4f8250417f4f6121e00d32f6add7611a49b677d1d497ab3c613f1352ef1","source":{"kind":"arxiv","id":"nucl-th/0107056","version":2},"attestation_state":"computed","paper":{"title":"Transition to meson-dominated matter at RHIC. Consequences for kaon flow","license":"","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"2), 2) ((1) Institute for Theoretical Physics, Amand Faessler (1), C. Fuchs (1), E. Zabrodin (1, Germany; (2) Institute for Nuclear Physics, L. Bravina (1, L. Csernai (3), Moscow State University, Norway), Russia; (3) Department of Physics, University of Bergen, University of Tuebingen","submitted_at":"2001-07-20T17:22:40Z","abstract_excerpt":"Anisotropic flow of kaons and antikaons is studied in heavy-ion collisions at CERN SPS and BNL RHIC energies within the microscopic quark-gluon string model. In the midrapidity range the directed flow of kaons v_1 differs considerably from that of antikaons at SPS energy (E_{lab} = 160 AGeV), while at RHIC energy (\\sqrt{s} = 130 AGeV) the excitation functions of both, kaon and antikaon, flows coincide within the statistical error bars. The change is attributed to formation of dense meson-dominated matter at RHIC, where the differences in interaction cross-sections of kaons and antikaons become"},"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":"nucl-th/0107056","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2001-07-20T17:22:40Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"e6a122f32be09d90f5ac61a8430de6e8c4e3c60e3d06a3b7eb539b45144756fd","abstract_canon_sha256":"e1cfc0d049bf46c037769bff3a437f2d0a9d1dcbdca65195c88706af985253e6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:16.485283Z","signature_b64":"nya7O3b04Zwvmbbg0cThyO3WBThc5xU6rZzpDrRfOxCkOqixScisuH6xfuMoyxK1M7j/pm8gKzr5hPzDzxNBBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0de3e4f8250417f4f6121e00d32f6add7611a49b677d1d497ab3c613f1352ef1","last_reissued_at":"2026-05-18T01:38:16.484607Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:16.484607Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Transition to meson-dominated matter at RHIC. Consequences for kaon flow","license":"","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"2), 2) ((1) Institute for Theoretical Physics, Amand Faessler (1), C. Fuchs (1), E. Zabrodin (1, Germany; (2) Institute for Nuclear Physics, L. Bravina (1, L. Csernai (3), Moscow State University, Norway), Russia; (3) Department of Physics, University of Bergen, University of Tuebingen","submitted_at":"2001-07-20T17:22:40Z","abstract_excerpt":"Anisotropic flow of kaons and antikaons is studied in heavy-ion collisions at CERN SPS and BNL RHIC energies within the microscopic quark-gluon string model. In the midrapidity range the directed flow of kaons v_1 differs considerably from that of antikaons at SPS energy (E_{lab} = 160 AGeV), while at RHIC energy (\\sqrt{s} = 130 AGeV) the excitation functions of both, kaon and antikaon, flows coincide within the statistical error bars. The change is attributed to formation of dense meson-dominated matter at RHIC, where the differences in interaction cross-sections of kaons and antikaons become"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0107056","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0107056","created_at":"2026-05-18T01:38:16.484714+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0107056v2","created_at":"2026-05-18T01:38:16.484714+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0107056","created_at":"2026-05-18T01:38:16.484714+00:00"},{"alias_kind":"pith_short_12","alias_value":"BXR6J6BFAQL7","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_16","alias_value":"BXR6J6BFAQL7J5QS","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_8","alias_value":"BXR6J6BF","created_at":"2026-05-18T12:25:50.254431+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BXR6J6BFAQL7J5QSDYANGL3K3V","json":"https://pith.science/pith/BXR6J6BFAQL7J5QSDYANGL3K3V.json","graph_json":"https://pith.science/api/pith-number/BXR6J6BFAQL7J5QSDYANGL3K3V/graph.json","events_json":"https://pith.science/api/pith-number/BXR6J6BFAQL7J5QSDYANGL3K3V/events.json","paper":"https://pith.science/paper/BXR6J6BF"},"agent_actions":{"view_html":"https://pith.science/pith/BXR6J6BFAQL7J5QSDYANGL3K3V","download_json":"https://pith.science/pith/BXR6J6BFAQL7J5QSDYANGL3K3V.json","view_paper":"https://pith.science/paper/BXR6J6BF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0107056&json=true","fetch_graph":"https://pith.science/api/pith-number/BXR6J6BFAQL7J5QSDYANGL3K3V/graph.json","fetch_events":"https://pith.science/api/pith-number/BXR6J6BFAQL7J5QSDYANGL3K3V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BXR6J6BFAQL7J5QSDYANGL3K3V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BXR6J6BFAQL7J5QSDYANGL3K3V/action/storage_attestation","attest_author":"https://pith.science/pith/BXR6J6BFAQL7J5QSDYANGL3K3V/action/author_attestation","sign_citation":"https://pith.science/pith/BXR6J6BFAQL7J5QSDYANGL3K3V/action/citation_signature","submit_replication":"https://pith.science/pith/BXR6J6BFAQL7J5QSDYANGL3K3V/action/replication_record"}},"created_at":"2026-05-18T01:38:16.484714+00:00","updated_at":"2026-05-18T01:38:16.484714+00:00"}