{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:WDCTR37NKT6LN6OZT5RJQJRLSQ","short_pith_number":"pith:WDCTR37N","schema_version":"1.0","canonical_sha256":"b0c538efed54fcb6f9d99f6298262b9433b4cb5cfcd79f4be2c85722f6dc8558","source":{"kind":"arxiv","id":"1503.00624","version":2},"attestation_state":"computed","paper":{"title":"Anisotropy and Strong-Coupling Effects on the Collective Mode Spectrum of Chiral Superconductors: Application to Sr$_2$RuO$_4$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Hao Wu, J. A. Sauls, Suk Bum Chung","submitted_at":"2015-03-02T17:22:34Z","abstract_excerpt":"Recent theories of Sr$_2$RuO$_4$ based on the interplay of strong interactions, spin-orbit coupling and multi-band anisotropy predict chiral or helical ground states with strong anisotropy of the pairing states, with deep minima in the excitation gap, as well as strong phase anisotropy for the chiral ground state. We develop time-dependent mean field theory to calculate the Bosonic spectrum for the class of 2D chiral superconductors spanning $^3$He-A to chiral superconductors with strong anisotropy. Chiral superconductors support a pair of massive Bosonic excitations of the time-reversed pairs"},"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":"1503.00624","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2015-03-02T17:22:34Z","cross_cats_sorted":[],"title_canon_sha256":"22e8bdf8d021133bc5f13691879f87fb0707598b8db25910addae347880e4a69","abstract_canon_sha256":"0613ee42084359e16cdbf4d03c8f61eb7d2408ab25f4b5e56e6bdfbf533d153f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:03:48.033345Z","signature_b64":"gXt8y2XvZ0kesLzFQ8GXfe2Xl0TMZyd2gyVpm0dhyCwA+Njnmb8BLIkyVv1xY+lxVX1eGsTUjGlK+BTv63uZCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b0c538efed54fcb6f9d99f6298262b9433b4cb5cfcd79f4be2c85722f6dc8558","last_reissued_at":"2026-05-18T02:03:48.032925Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:03:48.032925Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anisotropy and Strong-Coupling Effects on the Collective Mode Spectrum of Chiral Superconductors: Application to Sr$_2$RuO$_4$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Hao Wu, J. A. Sauls, Suk Bum Chung","submitted_at":"2015-03-02T17:22:34Z","abstract_excerpt":"Recent theories of Sr$_2$RuO$_4$ based on the interplay of strong interactions, spin-orbit coupling and multi-band anisotropy predict chiral or helical ground states with strong anisotropy of the pairing states, with deep minima in the excitation gap, as well as strong phase anisotropy for the chiral ground state. We develop time-dependent mean field theory to calculate the Bosonic spectrum for the class of 2D chiral superconductors spanning $^3$He-A to chiral superconductors with strong anisotropy. Chiral superconductors support a pair of massive Bosonic excitations of the time-reversed pairs"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.00624","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":""},"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":"1503.00624","created_at":"2026-05-18T02:03:48.032985+00:00"},{"alias_kind":"arxiv_version","alias_value":"1503.00624v2","created_at":"2026-05-18T02:03:48.032985+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.00624","created_at":"2026-05-18T02:03:48.032985+00:00"},{"alias_kind":"pith_short_12","alias_value":"WDCTR37NKT6L","created_at":"2026-05-18T12:29:47.479230+00:00"},{"alias_kind":"pith_short_16","alias_value":"WDCTR37NKT6LN6OZ","created_at":"2026-05-18T12:29:47.479230+00:00"},{"alias_kind":"pith_short_8","alias_value":"WDCTR37N","created_at":"2026-05-18T12:29:47.479230+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/WDCTR37NKT6LN6OZT5RJQJRLSQ","json":"https://pith.science/pith/WDCTR37NKT6LN6OZT5RJQJRLSQ.json","graph_json":"https://pith.science/api/pith-number/WDCTR37NKT6LN6OZT5RJQJRLSQ/graph.json","events_json":"https://pith.science/api/pith-number/WDCTR37NKT6LN6OZT5RJQJRLSQ/events.json","paper":"https://pith.science/paper/WDCTR37N"},"agent_actions":{"view_html":"https://pith.science/pith/WDCTR37NKT6LN6OZT5RJQJRLSQ","download_json":"https://pith.science/pith/WDCTR37NKT6LN6OZT5RJQJRLSQ.json","view_paper":"https://pith.science/paper/WDCTR37N","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1503.00624&json=true","fetch_graph":"https://pith.science/api/pith-number/WDCTR37NKT6LN6OZT5RJQJRLSQ/graph.json","fetch_events":"https://pith.science/api/pith-number/WDCTR37NKT6LN6OZT5RJQJRLSQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WDCTR37NKT6LN6OZT5RJQJRLSQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WDCTR37NKT6LN6OZT5RJQJRLSQ/action/storage_attestation","attest_author":"https://pith.science/pith/WDCTR37NKT6LN6OZT5RJQJRLSQ/action/author_attestation","sign_citation":"https://pith.science/pith/WDCTR37NKT6LN6OZT5RJQJRLSQ/action/citation_signature","submit_replication":"https://pith.science/pith/WDCTR37NKT6LN6OZT5RJQJRLSQ/action/replication_record"}},"created_at":"2026-05-18T02:03:48.032985+00:00","updated_at":"2026-05-18T02:03:48.032985+00:00"}