{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:RVTDI33ZFK4HNB74GGHRXOZ3SO","short_pith_number":"pith:RVTDI33Z","schema_version":"1.0","canonical_sha256":"8d66346f792ab87687fc318f1bbb3b9394fb5453267167c989626e8b14c57aa9","source":{"kind":"arxiv","id":"2504.19569","version":1},"attestation_state":"computed","paper":{"title":"Fermionizing the ideal Bose gas via topological pumping","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Bruno Juli\\'a-D\\'iaz, Grigori E. Astrakharchik, Krzysztof Paw{\\l}owski, Maciej Marciniak","submitted_at":"2025-04-28T08:28:04Z","abstract_excerpt":"We investigate the coherence and correlations of many-body states appearing in topological pumping in a one-dimensional Bose gas. By analyzing the system at zero and infinite interaction strengths, we reveal a rescaling of momentum distributions accompanied by a self-similar behavior in first- and second-order correlation functions. In excited states of non-interacting bosons, the momentum distribution shows a comb-like structure similar to that of non-interacting fermions but at a higher density. This is mirrored by Friedel oscillations in the one-body density matrix. At the same time, the de"},"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":"2504.19569","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2025-04-28T08:28:04Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"b4cc0bbef15f2489038b5eacdfcb675bf9553a9dae38593eddf45064f7d7436a","abstract_canon_sha256":"7a456157d4cf1d5251e0dc4cce5c438fd866221a4eb2ced7ac0a1e592fa9c23e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:54:59.838159Z","signature_b64":"UdbS/Ao8MUEiozvAD4vKW3xOACHLHJYHf9J3Xt77F+ts8K87D7pDASX/8U+7s1M9VIIvP4U5DHt1BpSe5Tm9Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8d66346f792ab87687fc318f1bbb3b9394fb5453267167c989626e8b14c57aa9","last_reissued_at":"2026-07-05T10:54:59.837633Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:54:59.837633Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fermionizing the ideal Bose gas via topological pumping","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Bruno Juli\\'a-D\\'iaz, Grigori E. Astrakharchik, Krzysztof Paw{\\l}owski, Maciej Marciniak","submitted_at":"2025-04-28T08:28:04Z","abstract_excerpt":"We investigate the coherence and correlations of many-body states appearing in topological pumping in a one-dimensional Bose gas. By analyzing the system at zero and infinite interaction strengths, we reveal a rescaling of momentum distributions accompanied by a self-similar behavior in first- and second-order correlation functions. In excited states of non-interacting bosons, the momentum distribution shows a comb-like structure similar to that of non-interacting fermions but at a higher density. This is mirrored by Friedel oscillations in the one-body density matrix. At the same time, the de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2504.19569","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/2504.19569/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":"2504.19569","created_at":"2026-07-05T10:54:59.837699+00:00"},{"alias_kind":"arxiv_version","alias_value":"2504.19569v1","created_at":"2026-07-05T10:54:59.837699+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2504.19569","created_at":"2026-07-05T10:54:59.837699+00:00"},{"alias_kind":"pith_short_12","alias_value":"RVTDI33ZFK4H","created_at":"2026-07-05T10:54:59.837699+00:00"},{"alias_kind":"pith_short_16","alias_value":"RVTDI33ZFK4HNB74","created_at":"2026-07-05T10:54:59.837699+00:00"},{"alias_kind":"pith_short_8","alias_value":"RVTDI33Z","created_at":"2026-07-05T10:54:59.837699+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2602.17657","citing_title":"Realization of fractional Fermi seas","ref_index":27,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RVTDI33ZFK4HNB74GGHRXOZ3SO","json":"https://pith.science/pith/RVTDI33ZFK4HNB74GGHRXOZ3SO.json","graph_json":"https://pith.science/api/pith-number/RVTDI33ZFK4HNB74GGHRXOZ3SO/graph.json","events_json":"https://pith.science/api/pith-number/RVTDI33ZFK4HNB74GGHRXOZ3SO/events.json","paper":"https://pith.science/paper/RVTDI33Z"},"agent_actions":{"view_html":"https://pith.science/pith/RVTDI33ZFK4HNB74GGHRXOZ3SO","download_json":"https://pith.science/pith/RVTDI33ZFK4HNB74GGHRXOZ3SO.json","view_paper":"https://pith.science/paper/RVTDI33Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2504.19569&json=true","fetch_graph":"https://pith.science/api/pith-number/RVTDI33ZFK4HNB74GGHRXOZ3SO/graph.json","fetch_events":"https://pith.science/api/pith-number/RVTDI33ZFK4HNB74GGHRXOZ3SO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RVTDI33ZFK4HNB74GGHRXOZ3SO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RVTDI33ZFK4HNB74GGHRXOZ3SO/action/storage_attestation","attest_author":"https://pith.science/pith/RVTDI33ZFK4HNB74GGHRXOZ3SO/action/author_attestation","sign_citation":"https://pith.science/pith/RVTDI33ZFK4HNB74GGHRXOZ3SO/action/citation_signature","submit_replication":"https://pith.science/pith/RVTDI33ZFK4HNB74GGHRXOZ3SO/action/replication_record"}},"created_at":"2026-07-05T10:54:59.837699+00:00","updated_at":"2026-07-05T10:54:59.837699+00:00"}