{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:WQFCZ6TN6CV4NLI52PIHNNPSJE","short_pith_number":"pith:WQFCZ6TN","schema_version":"1.0","canonical_sha256":"b40a2cfa6df0abc6ad1dd3d076b5f2490ef9d684bea06149f9b07f26da1fc4a1","source":{"kind":"arxiv","id":"1501.04109","version":1},"attestation_state":"computed","paper":{"title":"Effective response theory for zero energy Majorana bound states in three spatial dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.other","authors_text":"Jeffrey C. Y. Teo, Pedro L. S. Lopes, Shinsei Ryu","submitted_at":"2015-01-16T21:00:11Z","abstract_excerpt":"We propose a gravitational response theory for point defects (hedgehogs) binding Majorana zero modes in (3+1)-dimensional superconductors. Starting in 4+1 dimensions, where the point defect is extended into a line, a coupling of the bulk defect texture with the gravitational field is introduced. Diffeomorphism invariance then leads to an $SU(2)_2$ Kac-Moody current running along the defect line. The $SU(2)_2$ Kac-Moody algebra accounts for the non-Abelian nature of the zero modes in 3+1 dimensions. It is then shown to also encode the angular momentum density which permeates throughout the bulk"},"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":"1501.04109","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2015-01-16T21:00:11Z","cross_cats_sorted":[],"title_canon_sha256":"ebeef5152110202e5ad4a26e81825abf0f93ee8fe606034e279e11a3e2205cb6","abstract_canon_sha256":"b5b78939f68cd4202dbb6cf9ee9cce4b5a2fe8480d8c610f78d615fe9163935d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:37.806462Z","signature_b64":"wTITnaGA0/IKD+LsVA9ENH2KO1YUhFCXqU7RS+M3J8HQQfBxnP8cFIgEK+6omN+y4W4SeixWxcL9y6M1v3xmBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b40a2cfa6df0abc6ad1dd3d076b5f2490ef9d684bea06149f9b07f26da1fc4a1","last_reissued_at":"2026-05-18T01:59:37.805919Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:37.805919Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effective response theory for zero energy Majorana bound states in three spatial dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.other","authors_text":"Jeffrey C. Y. Teo, Pedro L. S. Lopes, Shinsei Ryu","submitted_at":"2015-01-16T21:00:11Z","abstract_excerpt":"We propose a gravitational response theory for point defects (hedgehogs) binding Majorana zero modes in (3+1)-dimensional superconductors. Starting in 4+1 dimensions, where the point defect is extended into a line, a coupling of the bulk defect texture with the gravitational field is introduced. Diffeomorphism invariance then leads to an $SU(2)_2$ Kac-Moody current running along the defect line. The $SU(2)_2$ Kac-Moody algebra accounts for the non-Abelian nature of the zero modes in 3+1 dimensions. It is then shown to also encode the angular momentum density which permeates throughout the bulk"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.04109","kind":"arxiv","version":1},"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":"1501.04109","created_at":"2026-05-18T01:59:37.805997+00:00"},{"alias_kind":"arxiv_version","alias_value":"1501.04109v1","created_at":"2026-05-18T01:59:37.805997+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.04109","created_at":"2026-05-18T01:59:37.805997+00:00"},{"alias_kind":"pith_short_12","alias_value":"WQFCZ6TN6CV4","created_at":"2026-05-18T12:29:47.479230+00:00"},{"alias_kind":"pith_short_16","alias_value":"WQFCZ6TN6CV4NLI5","created_at":"2026-05-18T12:29:47.479230+00:00"},{"alias_kind":"pith_short_8","alias_value":"WQFCZ6TN","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/WQFCZ6TN6CV4NLI52PIHNNPSJE","json":"https://pith.science/pith/WQFCZ6TN6CV4NLI52PIHNNPSJE.json","graph_json":"https://pith.science/api/pith-number/WQFCZ6TN6CV4NLI52PIHNNPSJE/graph.json","events_json":"https://pith.science/api/pith-number/WQFCZ6TN6CV4NLI52PIHNNPSJE/events.json","paper":"https://pith.science/paper/WQFCZ6TN"},"agent_actions":{"view_html":"https://pith.science/pith/WQFCZ6TN6CV4NLI52PIHNNPSJE","download_json":"https://pith.science/pith/WQFCZ6TN6CV4NLI52PIHNNPSJE.json","view_paper":"https://pith.science/paper/WQFCZ6TN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1501.04109&json=true","fetch_graph":"https://pith.science/api/pith-number/WQFCZ6TN6CV4NLI52PIHNNPSJE/graph.json","fetch_events":"https://pith.science/api/pith-number/WQFCZ6TN6CV4NLI52PIHNNPSJE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WQFCZ6TN6CV4NLI52PIHNNPSJE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WQFCZ6TN6CV4NLI52PIHNNPSJE/action/storage_attestation","attest_author":"https://pith.science/pith/WQFCZ6TN6CV4NLI52PIHNNPSJE/action/author_attestation","sign_citation":"https://pith.science/pith/WQFCZ6TN6CV4NLI52PIHNNPSJE/action/citation_signature","submit_replication":"https://pith.science/pith/WQFCZ6TN6CV4NLI52PIHNNPSJE/action/replication_record"}},"created_at":"2026-05-18T01:59:37.805997+00:00","updated_at":"2026-05-18T01:59:37.805997+00:00"}