{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:D446VRVO4IPMSO4LRCH6CRWEX5","short_pith_number":"pith:D446VRVO","schema_version":"1.0","canonical_sha256":"1f39eac6aee21ec93b8b888fe146c4bf755c2a1c0e4c963cefa0aad81e9a194c","source":{"kind":"arxiv","id":"2210.14236","version":2},"attestation_state":"computed","paper":{"title":"Bipolaronic superconductivity out of a Coulomb gas","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"A. J. Millis, B. V. Svistunov, C. Zhang, D. R. Reichman, J. Sous, M. Berciu, N. V. Prokof'ev","submitted_at":"2022-10-25T18:00:01Z","abstract_excerpt":"Employing unbiased sign-problem-free quantum Monte Carlo, we investigate the effects of long-range Coulomb forces on BEC of bipolarons using a model of bond phonon-modulated electron hopping. In absence of long-range repulsion, this model was recently shown to give rise to small-size, light-mass bipolarons that undergo a superfluid transition at high values of the critical transition temperature $T_\\mathrm{c}$. We find that $T_\\mathrm{c}$ in our model even with the long-range Coulomb repulsion remains much larger than that of Holstein bipolarons, and can be on the order of or greater than the "},"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":"2210.14236","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2022-10-25T18:00:01Z","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.str-el"],"title_canon_sha256":"aef90516d13da9cc48505a24be8879ab8f4d1385496f7f3421d58f44f554bd36","abstract_canon_sha256":"3cd05bd568a8076ca2e747889c0953498fa1ea59f3bb25a8f4890bddd9f53dd4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:24:46.823202Z","signature_b64":"EGM5vtIIKnZRjuA2p0pV5WYq7cRSBbHSAsho7Bi2Vtte38yB7Wuip5mbKM8cZA6n7NpV6cMFsO4YPnbVUeC/Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1f39eac6aee21ec93b8b888fe146c4bf755c2a1c0e4c963cefa0aad81e9a194c","last_reissued_at":"2026-07-05T07:24:46.822742Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:24:46.822742Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Bipolaronic superconductivity out of a Coulomb gas","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"A. J. Millis, B. V. Svistunov, C. Zhang, D. R. Reichman, J. Sous, M. Berciu, N. V. Prokof'ev","submitted_at":"2022-10-25T18:00:01Z","abstract_excerpt":"Employing unbiased sign-problem-free quantum Monte Carlo, we investigate the effects of long-range Coulomb forces on BEC of bipolarons using a model of bond phonon-modulated electron hopping. In absence of long-range repulsion, this model was recently shown to give rise to small-size, light-mass bipolarons that undergo a superfluid transition at high values of the critical transition temperature $T_\\mathrm{c}$. We find that $T_\\mathrm{c}$ in our model even with the long-range Coulomb repulsion remains much larger than that of Holstein bipolarons, and can be on the order of or greater than the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.14236","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2210.14236/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":"2210.14236","created_at":"2026-07-05T07:24:46.822801+00:00"},{"alias_kind":"arxiv_version","alias_value":"2210.14236v2","created_at":"2026-07-05T07:24:46.822801+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.14236","created_at":"2026-07-05T07:24:46.822801+00:00"},{"alias_kind":"pith_short_12","alias_value":"D446VRVO4IPM","created_at":"2026-07-05T07:24:46.822801+00:00"},{"alias_kind":"pith_short_16","alias_value":"D446VRVO4IPMSO4L","created_at":"2026-07-05T07:24:46.822801+00:00"},{"alias_kind":"pith_short_8","alias_value":"D446VRVO","created_at":"2026-07-05T07:24:46.822801+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/D446VRVO4IPMSO4LRCH6CRWEX5","json":"https://pith.science/pith/D446VRVO4IPMSO4LRCH6CRWEX5.json","graph_json":"https://pith.science/api/pith-number/D446VRVO4IPMSO4LRCH6CRWEX5/graph.json","events_json":"https://pith.science/api/pith-number/D446VRVO4IPMSO4LRCH6CRWEX5/events.json","paper":"https://pith.science/paper/D446VRVO"},"agent_actions":{"view_html":"https://pith.science/pith/D446VRVO4IPMSO4LRCH6CRWEX5","download_json":"https://pith.science/pith/D446VRVO4IPMSO4LRCH6CRWEX5.json","view_paper":"https://pith.science/paper/D446VRVO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2210.14236&json=true","fetch_graph":"https://pith.science/api/pith-number/D446VRVO4IPMSO4LRCH6CRWEX5/graph.json","fetch_events":"https://pith.science/api/pith-number/D446VRVO4IPMSO4LRCH6CRWEX5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/D446VRVO4IPMSO4LRCH6CRWEX5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/D446VRVO4IPMSO4LRCH6CRWEX5/action/storage_attestation","attest_author":"https://pith.science/pith/D446VRVO4IPMSO4LRCH6CRWEX5/action/author_attestation","sign_citation":"https://pith.science/pith/D446VRVO4IPMSO4LRCH6CRWEX5/action/citation_signature","submit_replication":"https://pith.science/pith/D446VRVO4IPMSO4LRCH6CRWEX5/action/replication_record"}},"created_at":"2026-07-05T07:24:46.822801+00:00","updated_at":"2026-07-05T07:24:46.822801+00:00"}