{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:Y5HCRBONI6I756DT3VWBAP7QGW","short_pith_number":"pith:Y5HCRBON","schema_version":"1.0","canonical_sha256":"c74e2885cd4791fef873dd6c103ff0359dec2eede66ea51073047a7870d4f3ed","source":{"kind":"arxiv","id":"0910.4534","version":1},"attestation_state":"computed","paper":{"title":"Finite temperature phase transition for disordered weakly interacting bosons in one dimension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas"],"primary_cat":"cond-mat.dis-nn","authors_text":"B.L. Altshuler, G.V. Shlyapnikov, I.L. Aleiner","submitted_at":"2009-10-23T16:50:03Z","abstract_excerpt":"It is commonly accepted that there are no phase transitions in one-dimensional (1D) systems at a finite temperature, because long-range correlations are destroyed by thermal fluctuations. Here we demonstrate that the 1D gas of short-range interacting bosons in the presence of disorder can undergo a finite temperature phase transition between two distinct states: fluid and insulator. None of these states has long-range spatial correlations, but this is a true albeit non-conventional phase transition because transport properties are singular at the transition point. In the fluid phase the mass t"},"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":"0910.4534","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2009-10-23T16:50:03Z","cross_cats_sorted":["cond-mat.quant-gas"],"title_canon_sha256":"efe535083b842989d494ea620f91dde6efbe13da1d790fa863e084da8e5e13b9","abstract_canon_sha256":"d02579800387d282b6803c1a95dc81e8ec75832f0b995b149893149d74210f8a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:11:12.126261Z","signature_b64":"Mc+GaNiHWTs4fK3XK7NJSeEa+AJ8wzUXLZpUDXw+J5XXuQ02P3vT+H3GeGpdEOXxynKa9f60I1XpBnlgbaQqCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c74e2885cd4791fef873dd6c103ff0359dec2eede66ea51073047a7870d4f3ed","last_reissued_at":"2026-05-18T02:11:12.125367Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:11:12.125367Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite temperature phase transition for disordered weakly interacting bosons in one dimension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas"],"primary_cat":"cond-mat.dis-nn","authors_text":"B.L. Altshuler, G.V. Shlyapnikov, I.L. Aleiner","submitted_at":"2009-10-23T16:50:03Z","abstract_excerpt":"It is commonly accepted that there are no phase transitions in one-dimensional (1D) systems at a finite temperature, because long-range correlations are destroyed by thermal fluctuations. Here we demonstrate that the 1D gas of short-range interacting bosons in the presence of disorder can undergo a finite temperature phase transition between two distinct states: fluid and insulator. None of these states has long-range spatial correlations, but this is a true albeit non-conventional phase transition because transport properties are singular at the transition point. In the fluid phase the mass t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0910.4534","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":"0910.4534","created_at":"2026-05-18T02:11:12.125534+00:00"},{"alias_kind":"arxiv_version","alias_value":"0910.4534v1","created_at":"2026-05-18T02:11:12.125534+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0910.4534","created_at":"2026-05-18T02:11:12.125534+00:00"},{"alias_kind":"pith_short_12","alias_value":"Y5HCRBONI6I7","created_at":"2026-05-18T12:26:02.257875+00:00"},{"alias_kind":"pith_short_16","alias_value":"Y5HCRBONI6I756DT","created_at":"2026-05-18T12:26:02.257875+00:00"},{"alias_kind":"pith_short_8","alias_value":"Y5HCRBON","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/Y5HCRBONI6I756DT3VWBAP7QGW","json":"https://pith.science/pith/Y5HCRBONI6I756DT3VWBAP7QGW.json","graph_json":"https://pith.science/api/pith-number/Y5HCRBONI6I756DT3VWBAP7QGW/graph.json","events_json":"https://pith.science/api/pith-number/Y5HCRBONI6I756DT3VWBAP7QGW/events.json","paper":"https://pith.science/paper/Y5HCRBON"},"agent_actions":{"view_html":"https://pith.science/pith/Y5HCRBONI6I756DT3VWBAP7QGW","download_json":"https://pith.science/pith/Y5HCRBONI6I756DT3VWBAP7QGW.json","view_paper":"https://pith.science/paper/Y5HCRBON","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0910.4534&json=true","fetch_graph":"https://pith.science/api/pith-number/Y5HCRBONI6I756DT3VWBAP7QGW/graph.json","fetch_events":"https://pith.science/api/pith-number/Y5HCRBONI6I756DT3VWBAP7QGW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Y5HCRBONI6I756DT3VWBAP7QGW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Y5HCRBONI6I756DT3VWBAP7QGW/action/storage_attestation","attest_author":"https://pith.science/pith/Y5HCRBONI6I756DT3VWBAP7QGW/action/author_attestation","sign_citation":"https://pith.science/pith/Y5HCRBONI6I756DT3VWBAP7QGW/action/citation_signature","submit_replication":"https://pith.science/pith/Y5HCRBONI6I756DT3VWBAP7QGW/action/replication_record"}},"created_at":"2026-05-18T02:11:12.125534+00:00","updated_at":"2026-05-18T02:11:12.125534+00:00"}