{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:ONRU6FNF5REV4YYU2Q2UJD7EIR","short_pith_number":"pith:ONRU6FNF","schema_version":"1.0","canonical_sha256":"73634f15a5ec495e6314d435448fe44450582f4f548dc68ce5b840076198739a","source":{"kind":"arxiv","id":"2206.03476","version":3},"attestation_state":"computed","paper":{"title":"Many-body bound states and induced interactions of charged impurities in a bosonic bath","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"A. Negretti, G. E. Astrakharchik, K. Jachymski, L. A. Pe\\~na Ardila","submitted_at":"2022-06-07T17:50:12Z","abstract_excerpt":"Induced interactions and bound states of charge carriers immersed in a quantum medium are crucial for the investigation of quantum transport. Ultracold atom-ion systems can provide a convenient platform for studying this problem. Here, we investigate the static properties of one and two ionic impurities in a bosonic bath using quantum Monte Carlo methods. We identify three bipolaronic regimes depending on the strength of the atom-ion potential and the number of its two-body bound states: a perturbative regime resembling the situation of a pair of neutral impurities, a non-perturbative regime 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":"2206.03476","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2022-06-07T17:50:12Z","cross_cats_sorted":["physics.atom-ph","quant-ph"],"title_canon_sha256":"e04aff6458c07215eced1426eb9a102161e37a707fa5c888a7341c652012f92f","abstract_canon_sha256":"c59af06fbee797c2270f33ec550317872ae66245f1361d53db5b6506431d1da9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:55:09.324240Z","signature_b64":"5eirgbOXsasZeebD0jiNFWfLbYr1LrgJ2jZ+fKBBCWCn/uIcechOX2p8McdMVJz1lyXFikbY4ATk6dgKx6JPDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"73634f15a5ec495e6314d435448fe44450582f4f548dc68ce5b840076198739a","last_reissued_at":"2026-07-05T05:55:09.323667Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:55:09.323667Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Many-body bound states and induced interactions of charged impurities in a bosonic bath","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"A. Negretti, G. E. Astrakharchik, K. Jachymski, L. A. Pe\\~na Ardila","submitted_at":"2022-06-07T17:50:12Z","abstract_excerpt":"Induced interactions and bound states of charge carriers immersed in a quantum medium are crucial for the investigation of quantum transport. Ultracold atom-ion systems can provide a convenient platform for studying this problem. Here, we investigate the static properties of one and two ionic impurities in a bosonic bath using quantum Monte Carlo methods. We identify three bipolaronic regimes depending on the strength of the atom-ion potential and the number of its two-body bound states: a perturbative regime resembling the situation of a pair of neutral impurities, a non-perturbative regime t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.03476","kind":"arxiv","version":3},"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/2206.03476/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":"2206.03476","created_at":"2026-07-05T05:55:09.323755+00:00"},{"alias_kind":"arxiv_version","alias_value":"2206.03476v3","created_at":"2026-07-05T05:55:09.323755+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.03476","created_at":"2026-07-05T05:55:09.323755+00:00"},{"alias_kind":"pith_short_12","alias_value":"ONRU6FNF5REV","created_at":"2026-07-05T05:55:09.323755+00:00"},{"alias_kind":"pith_short_16","alias_value":"ONRU6FNF5REV4YYU","created_at":"2026-07-05T05:55:09.323755+00:00"},{"alias_kind":"pith_short_8","alias_value":"ONRU6FNF","created_at":"2026-07-05T05:55:09.323755+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.06520","citing_title":"Polaronic dressing of bound states","ref_index":39,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ONRU6FNF5REV4YYU2Q2UJD7EIR","json":"https://pith.science/pith/ONRU6FNF5REV4YYU2Q2UJD7EIR.json","graph_json":"https://pith.science/api/pith-number/ONRU6FNF5REV4YYU2Q2UJD7EIR/graph.json","events_json":"https://pith.science/api/pith-number/ONRU6FNF5REV4YYU2Q2UJD7EIR/events.json","paper":"https://pith.science/paper/ONRU6FNF"},"agent_actions":{"view_html":"https://pith.science/pith/ONRU6FNF5REV4YYU2Q2UJD7EIR","download_json":"https://pith.science/pith/ONRU6FNF5REV4YYU2Q2UJD7EIR.json","view_paper":"https://pith.science/paper/ONRU6FNF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2206.03476&json=true","fetch_graph":"https://pith.science/api/pith-number/ONRU6FNF5REV4YYU2Q2UJD7EIR/graph.json","fetch_events":"https://pith.science/api/pith-number/ONRU6FNF5REV4YYU2Q2UJD7EIR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ONRU6FNF5REV4YYU2Q2UJD7EIR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ONRU6FNF5REV4YYU2Q2UJD7EIR/action/storage_attestation","attest_author":"https://pith.science/pith/ONRU6FNF5REV4YYU2Q2UJD7EIR/action/author_attestation","sign_citation":"https://pith.science/pith/ONRU6FNF5REV4YYU2Q2UJD7EIR/action/citation_signature","submit_replication":"https://pith.science/pith/ONRU6FNF5REV4YYU2Q2UJD7EIR/action/replication_record"}},"created_at":"2026-07-05T05:55:09.323755+00:00","updated_at":"2026-07-05T05:55:09.323755+00:00"}