{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:YXN4HAZLLJPYOZQVF62HJRBAQ4","short_pith_number":"pith:YXN4HAZL","schema_version":"1.0","canonical_sha256":"c5dbc3832b5a5f8766152fb474c420873a6ad529f7d7c3eb420d319aed9b6039","source":{"kind":"arxiv","id":"1501.07615","version":3},"attestation_state":"computed","paper":{"title":"S-Wave Superconductivity in Anisotropic Holographic Insulators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","cond-mat.supr-con"],"primary_cat":"hep-th","authors_text":"Benedikt Herwerth, Johanna Erdmenger, Koenraad Schalm, Rene Meyer, Steffen Klug","submitted_at":"2015-01-29T21:11:31Z","abstract_excerpt":"Within gauge/gravity duality, we consider finite density systems in a helical lattice dual to asymptotically anti-de Sitter space-times with Bianchi VII symmetry. These systems can become an anisotropic insulator in one direction while retaining metallic behavior in others. To this model, we add a $U(1)$ charged scalar and show that below a critical temperature, it forms a spatially homogeneous condensate that restores isotropy in a new superconducting ground state. We determine the phase diagram in terms of the helix parameters and perform a stability analysis on its IR fixed point correspond"},"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":"1501.07615","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-01-29T21:11:31Z","cross_cats_sorted":["cond-mat.str-el","cond-mat.supr-con"],"title_canon_sha256":"0b758dc138631a546ee65d38b5acea2581339f56f837b8e186a16ad82ef9f282","abstract_canon_sha256":"a58020f0c388120b3887d1c553f61eabbd173356162eeecdeb956ec7ade4bb28"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:17:51.296843Z","signature_b64":"n4CuxYjHeQFQ8j6jQlYjKQrRZgwB80w2S6G3zRIxMd4c8hOvZuLBO6UaRRiqXe0XG2cBEd0/DcVo3N7J1ju3BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c5dbc3832b5a5f8766152fb474c420873a6ad529f7d7c3eb420d319aed9b6039","last_reissued_at":"2026-05-18T02:17:51.296280Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:17:51.296280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"S-Wave Superconductivity in Anisotropic Holographic Insulators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","cond-mat.supr-con"],"primary_cat":"hep-th","authors_text":"Benedikt Herwerth, Johanna Erdmenger, Koenraad Schalm, Rene Meyer, Steffen Klug","submitted_at":"2015-01-29T21:11:31Z","abstract_excerpt":"Within gauge/gravity duality, we consider finite density systems in a helical lattice dual to asymptotically anti-de Sitter space-times with Bianchi VII symmetry. These systems can become an anisotropic insulator in one direction while retaining metallic behavior in others. To this model, we add a $U(1)$ charged scalar and show that below a critical temperature, it forms a spatially homogeneous condensate that restores isotropy in a new superconducting ground state. We determine the phase diagram in terms of the helix parameters and perform a stability analysis on its IR fixed point correspond"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.07615","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":""},"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":"1501.07615","created_at":"2026-05-18T02:17:51.296388+00:00"},{"alias_kind":"arxiv_version","alias_value":"1501.07615v3","created_at":"2026-05-18T02:17:51.296388+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.07615","created_at":"2026-05-18T02:17:51.296388+00:00"},{"alias_kind":"pith_short_12","alias_value":"YXN4HAZLLJPY","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_16","alias_value":"YXN4HAZLLJPYOZQV","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_8","alias_value":"YXN4HAZL","created_at":"2026-05-18T12:29:52.810259+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.20321","citing_title":"Poles-zeros duality in semi-holographic Mott insulators","ref_index":79,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YXN4HAZLLJPYOZQVF62HJRBAQ4","json":"https://pith.science/pith/YXN4HAZLLJPYOZQVF62HJRBAQ4.json","graph_json":"https://pith.science/api/pith-number/YXN4HAZLLJPYOZQVF62HJRBAQ4/graph.json","events_json":"https://pith.science/api/pith-number/YXN4HAZLLJPYOZQVF62HJRBAQ4/events.json","paper":"https://pith.science/paper/YXN4HAZL"},"agent_actions":{"view_html":"https://pith.science/pith/YXN4HAZLLJPYOZQVF62HJRBAQ4","download_json":"https://pith.science/pith/YXN4HAZLLJPYOZQVF62HJRBAQ4.json","view_paper":"https://pith.science/paper/YXN4HAZL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1501.07615&json=true","fetch_graph":"https://pith.science/api/pith-number/YXN4HAZLLJPYOZQVF62HJRBAQ4/graph.json","fetch_events":"https://pith.science/api/pith-number/YXN4HAZLLJPYOZQVF62HJRBAQ4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YXN4HAZLLJPYOZQVF62HJRBAQ4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YXN4HAZLLJPYOZQVF62HJRBAQ4/action/storage_attestation","attest_author":"https://pith.science/pith/YXN4HAZLLJPYOZQVF62HJRBAQ4/action/author_attestation","sign_citation":"https://pith.science/pith/YXN4HAZLLJPYOZQVF62HJRBAQ4/action/citation_signature","submit_replication":"https://pith.science/pith/YXN4HAZLLJPYOZQVF62HJRBAQ4/action/replication_record"}},"created_at":"2026-05-18T02:17:51.296388+00:00","updated_at":"2026-05-18T02:17:51.296388+00:00"}