{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:UBY2UZTAM7SLS6OBMLI7SKHWBZ","short_pith_number":"pith:UBY2UZTA","schema_version":"1.0","canonical_sha256":"a071aa666067e4b979c162d1f928f60e617f799b32694e163d670714ea2e5f47","source":{"kind":"arxiv","id":"0906.0955","version":1},"attestation_state":"computed","paper":{"title":"Polarization Suppression and Nonmonotonic Local Two-Body Correlations in the Two-Component Bose Gas in One Dimension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"A. Klauser, J.-S. Caux, J. van den Brink","submitted_at":"2009-06-04T18:21:50Z","abstract_excerpt":"We study the interplay of quantum statistics, strong interactions and finite temperatures in the two-component (spinor) Bose gas with repulsive delta-function interactions in one dimension. Using the Thermodynamic Bethe Ansatz, we obtain the equation of state, population densities and local density correlation numerically as a function of all physical parameters (interaction, temperature and chemical potentials), quantifying the full crossover between low-temperature ferromagnetic and high-temperature unpolarized regimes. In contrast to the single-component, Lieb-Liniger gas, nonmonotonic beha"},"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":"0906.0955","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2009-06-04T18:21:50Z","cross_cats_sorted":[],"title_canon_sha256":"25397f80aa5d5a59cd2fb974dbd5143898b8ee62af11215cbbe9c1dc58331f1c","abstract_canon_sha256":"59696ab69b2dafb6e2200138e14459d089a214502e3e17252c216f1d9159378c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:59.625793Z","signature_b64":"WKIndg06FAPaTCpEoxzkD0Z9Wt0KTOO/PU70YWaqjll5OMcDmgACB5Y3C/7Vzlqy2mv3tjsmaEZ61HOYI+GQDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a071aa666067e4b979c162d1f928f60e617f799b32694e163d670714ea2e5f47","last_reissued_at":"2026-05-18T03:23:59.624948Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:59.624948Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Polarization Suppression and Nonmonotonic Local Two-Body Correlations in the Two-Component Bose Gas in One Dimension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"A. Klauser, J.-S. Caux, J. van den Brink","submitted_at":"2009-06-04T18:21:50Z","abstract_excerpt":"We study the interplay of quantum statistics, strong interactions and finite temperatures in the two-component (spinor) Bose gas with repulsive delta-function interactions in one dimension. Using the Thermodynamic Bethe Ansatz, we obtain the equation of state, population densities and local density correlation numerically as a function of all physical parameters (interaction, temperature and chemical potentials), quantifying the full crossover between low-temperature ferromagnetic and high-temperature unpolarized regimes. In contrast to the single-component, Lieb-Liniger gas, nonmonotonic beha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0906.0955","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"0906.0955","created_at":"2026-05-18T03:23:59.625071+00:00"},{"alias_kind":"arxiv_version","alias_value":"0906.0955v1","created_at":"2026-05-18T03:23:59.625071+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0906.0955","created_at":"2026-05-18T03:23:59.625071+00:00"},{"alias_kind":"pith_short_12","alias_value":"UBY2UZTAM7SL","created_at":"2026-05-18T12:26:02.257875+00:00"},{"alias_kind":"pith_short_16","alias_value":"UBY2UZTAM7SLS6OB","created_at":"2026-05-18T12:26:02.257875+00:00"},{"alias_kind":"pith_short_8","alias_value":"UBY2UZTA","created_at":"2026-05-18T12:26:02.257875+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/UBY2UZTAM7SLS6OBMLI7SKHWBZ","json":"https://pith.science/pith/UBY2UZTAM7SLS6OBMLI7SKHWBZ.json","graph_json":"https://pith.science/api/pith-number/UBY2UZTAM7SLS6OBMLI7SKHWBZ/graph.json","events_json":"https://pith.science/api/pith-number/UBY2UZTAM7SLS6OBMLI7SKHWBZ/events.json","paper":"https://pith.science/paper/UBY2UZTA"},"agent_actions":{"view_html":"https://pith.science/pith/UBY2UZTAM7SLS6OBMLI7SKHWBZ","download_json":"https://pith.science/pith/UBY2UZTAM7SLS6OBMLI7SKHWBZ.json","view_paper":"https://pith.science/paper/UBY2UZTA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0906.0955&json=true","fetch_graph":"https://pith.science/api/pith-number/UBY2UZTAM7SLS6OBMLI7SKHWBZ/graph.json","fetch_events":"https://pith.science/api/pith-number/UBY2UZTAM7SLS6OBMLI7SKHWBZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UBY2UZTAM7SLS6OBMLI7SKHWBZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UBY2UZTAM7SLS6OBMLI7SKHWBZ/action/storage_attestation","attest_author":"https://pith.science/pith/UBY2UZTAM7SLS6OBMLI7SKHWBZ/action/author_attestation","sign_citation":"https://pith.science/pith/UBY2UZTAM7SLS6OBMLI7SKHWBZ/action/citation_signature","submit_replication":"https://pith.science/pith/UBY2UZTAM7SLS6OBMLI7SKHWBZ/action/replication_record"}},"created_at":"2026-05-18T03:23:59.625071+00:00","updated_at":"2026-05-18T03:23:59.625071+00:00"}