{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:LQRNWYFMWQ2LJ2BGPIR5LRAN4P","short_pith_number":"pith:LQRNWYFM","schema_version":"1.0","canonical_sha256":"5c22db60acb434b4e8267a23d5c40de3c135e7c5a636f1fbc373fa819529102b","source":{"kind":"arxiv","id":"2207.09491","version":2},"attestation_state":"computed","paper":{"title":"Magnetic-field sensitive charge density wave orders in the superconducting phase of UTe2","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"Anuva Aishwarya, Arjun Raghavan, Eduardo Fradkin, Johnpierre Paglione, Julian May-Mann, Laimei Nie, Marisa Romanelli, Nicholas P. Butch, Shanta R. Saha, Sheng Ran, Vidya Madhavan","submitted_at":"2022-07-19T18:04:47Z","abstract_excerpt":"The intense interest in triplet superconductivity partly stems from theoretical predictions of exotic excitations such as non-abelian Majorana modes, chiral supercurrents, and half-quantum vortices. However, fundamentally new, and unexpected states may emerge when triplet superconductivity appears in a strongly correlated system. In this work we use scanning tunneling microscopy to reveal an unusual charge density wave (CDW) order in the heavy fermion triplet superconductor, UTe2. Our high-resolution maps reveal a multi-component incommensurate CDW whose intensity get weaker with increasing fi"},"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":"2207.09491","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2022-07-19T18:04:47Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"01cf1a84073abe8643a2db010e512508176050012f220efa482983f707ab6682","abstract_canon_sha256":"39898f0afaa1757139b5928fa35c3d858060045a8a5eee583b8cf36ce21ffcc1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:25:57.996357Z","signature_b64":"FdRdNoy4ew7W8/yIQIZl3+TyvtMPyv15b74YNshtYTSIRenQVhDh4LAhnUBcs5KkWMUBuxlCnhEQuejJEP7uAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5c22db60acb434b4e8267a23d5c40de3c135e7c5a636f1fbc373fa819529102b","last_reissued_at":"2026-07-05T06:25:57.995991Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:25:57.995991Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magnetic-field sensitive charge density wave orders in the superconducting phase of UTe2","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"Anuva Aishwarya, Arjun Raghavan, Eduardo Fradkin, Johnpierre Paglione, Julian May-Mann, Laimei Nie, Marisa Romanelli, Nicholas P. Butch, Shanta R. Saha, Sheng Ran, Vidya Madhavan","submitted_at":"2022-07-19T18:04:47Z","abstract_excerpt":"The intense interest in triplet superconductivity partly stems from theoretical predictions of exotic excitations such as non-abelian Majorana modes, chiral supercurrents, and half-quantum vortices. However, fundamentally new, and unexpected states may emerge when triplet superconductivity appears in a strongly correlated system. In this work we use scanning tunneling microscopy to reveal an unusual charge density wave (CDW) order in the heavy fermion triplet superconductor, UTe2. Our high-resolution maps reveal a multi-component incommensurate CDW whose intensity get weaker with increasing fi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2207.09491","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/2207.09491/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":"2207.09491","created_at":"2026-07-05T06:25:57.996044+00:00"},{"alias_kind":"arxiv_version","alias_value":"2207.09491v2","created_at":"2026-07-05T06:25:57.996044+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2207.09491","created_at":"2026-07-05T06:25:57.996044+00:00"},{"alias_kind":"pith_short_12","alias_value":"LQRNWYFMWQ2L","created_at":"2026-07-05T06:25:57.996044+00:00"},{"alias_kind":"pith_short_16","alias_value":"LQRNWYFMWQ2LJ2BG","created_at":"2026-07-05T06:25:57.996044+00:00"},{"alias_kind":"pith_short_8","alias_value":"LQRNWYFM","created_at":"2026-07-05T06:25:57.996044+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.21711","citing_title":"Symmetry-Enforced Pair-Density Wave and Chiral Interband Superconductivity in Strongly Correlated Kagome Systems","ref_index":17,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LQRNWYFMWQ2LJ2BGPIR5LRAN4P","json":"https://pith.science/pith/LQRNWYFMWQ2LJ2BGPIR5LRAN4P.json","graph_json":"https://pith.science/api/pith-number/LQRNWYFMWQ2LJ2BGPIR5LRAN4P/graph.json","events_json":"https://pith.science/api/pith-number/LQRNWYFMWQ2LJ2BGPIR5LRAN4P/events.json","paper":"https://pith.science/paper/LQRNWYFM"},"agent_actions":{"view_html":"https://pith.science/pith/LQRNWYFMWQ2LJ2BGPIR5LRAN4P","download_json":"https://pith.science/pith/LQRNWYFMWQ2LJ2BGPIR5LRAN4P.json","view_paper":"https://pith.science/paper/LQRNWYFM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2207.09491&json=true","fetch_graph":"https://pith.science/api/pith-number/LQRNWYFMWQ2LJ2BGPIR5LRAN4P/graph.json","fetch_events":"https://pith.science/api/pith-number/LQRNWYFMWQ2LJ2BGPIR5LRAN4P/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LQRNWYFMWQ2LJ2BGPIR5LRAN4P/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LQRNWYFMWQ2LJ2BGPIR5LRAN4P/action/storage_attestation","attest_author":"https://pith.science/pith/LQRNWYFMWQ2LJ2BGPIR5LRAN4P/action/author_attestation","sign_citation":"https://pith.science/pith/LQRNWYFMWQ2LJ2BGPIR5LRAN4P/action/citation_signature","submit_replication":"https://pith.science/pith/LQRNWYFMWQ2LJ2BGPIR5LRAN4P/action/replication_record"}},"created_at":"2026-07-05T06:25:57.996044+00:00","updated_at":"2026-07-05T06:25:57.996044+00:00"}