{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:X5ANAHI6F5YHKIPVTH6DPFXDLT","short_pith_number":"pith:X5ANAHI6","schema_version":"1.0","canonical_sha256":"bf40d01d1e2f707521f599fc3796e35cc4cd32f666e562fbe440bdeb2a31a4bd","source":{"kind":"arxiv","id":"2506.08095","version":2},"attestation_state":"computed","paper":{"title":"Altermagnet-Superconductor Heterostructure: a Scalable Platform for Braiding of Majorana Modes","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.supr-con","quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Eric Mascot, Stephan Rachel, Themba Hodge","submitted_at":"2025-06-09T18:00:16Z","abstract_excerpt":"Topological quantum computation, featuring qubits built out of anyonic excitations known as Majorana zero modes (MZMs), have long presented an exciting pathway towards scalable quantum computation. Recently, the advent of altermagnetic materials has presented a new pathway towards localized MZMs on the boundary of two-dimensional materials, consisting of an altermagnetic film, subject to a superconducting proximity effect from a superconducting substrate. In this work, we demonstrate the possibility for an altermagnet-superconductor heterostructure, to not only harbor MZMs, but also freely man"},"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":"2506.08095","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-06-09T18:00:16Z","cross_cats_sorted":["cond-mat.supr-con","quant-ph"],"title_canon_sha256":"3a03a4ba918d350c3f0baf88812e20753a4f105bb6d16f2a82f1c1a9fb20361f","abstract_canon_sha256":"dc0391f043654ec6a5064f70491c20b42e69f44548704f800077fcaa73b92cb9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-24T01:14:57.470800Z","signature_b64":"AOPEv2rSXEGRYFb6wOrrFo+/l756GWnHU3fqM9cKDebmnlZ8/9cjEhlNRaiCY5JaJYtaUZqe/zpNJffh3qHYAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bf40d01d1e2f707521f599fc3796e35cc4cd32f666e562fbe440bdeb2a31a4bd","last_reissued_at":"2026-06-24T01:14:57.470333Z","signature_status":"signed_v1","first_computed_at":"2026-06-24T01:14:57.470333Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Altermagnet-Superconductor Heterostructure: a Scalable Platform for Braiding of Majorana Modes","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.supr-con","quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Eric Mascot, Stephan Rachel, Themba Hodge","submitted_at":"2025-06-09T18:00:16Z","abstract_excerpt":"Topological quantum computation, featuring qubits built out of anyonic excitations known as Majorana zero modes (MZMs), have long presented an exciting pathway towards scalable quantum computation. Recently, the advent of altermagnetic materials has presented a new pathway towards localized MZMs on the boundary of two-dimensional materials, consisting of an altermagnetic film, subject to a superconducting proximity effect from a superconducting substrate. In this work, we demonstrate the possibility for an altermagnet-superconductor heterostructure, to not only harbor MZMs, but also freely man"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.08095","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/2506.08095/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":"2506.08095","created_at":"2026-06-24T01:14:57.470391+00:00"},{"alias_kind":"arxiv_version","alias_value":"2506.08095v2","created_at":"2026-06-24T01:14:57.470391+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.08095","created_at":"2026-06-24T01:14:57.470391+00:00"},{"alias_kind":"pith_short_12","alias_value":"X5ANAHI6F5YH","created_at":"2026-06-24T01:14:57.470391+00:00"},{"alias_kind":"pith_short_16","alias_value":"X5ANAHI6F5YHKIPV","created_at":"2026-06-24T01:14:57.470391+00:00"},{"alias_kind":"pith_short_8","alias_value":"X5ANAHI6","created_at":"2026-06-24T01:14:57.470391+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.03364","citing_title":"Engineering subgap states in superconductors by the symmetry of altermagnetism","ref_index":97,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/X5ANAHI6F5YHKIPVTH6DPFXDLT","json":"https://pith.science/pith/X5ANAHI6F5YHKIPVTH6DPFXDLT.json","graph_json":"https://pith.science/api/pith-number/X5ANAHI6F5YHKIPVTH6DPFXDLT/graph.json","events_json":"https://pith.science/api/pith-number/X5ANAHI6F5YHKIPVTH6DPFXDLT/events.json","paper":"https://pith.science/paper/X5ANAHI6"},"agent_actions":{"view_html":"https://pith.science/pith/X5ANAHI6F5YHKIPVTH6DPFXDLT","download_json":"https://pith.science/pith/X5ANAHI6F5YHKIPVTH6DPFXDLT.json","view_paper":"https://pith.science/paper/X5ANAHI6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2506.08095&json=true","fetch_graph":"https://pith.science/api/pith-number/X5ANAHI6F5YHKIPVTH6DPFXDLT/graph.json","fetch_events":"https://pith.science/api/pith-number/X5ANAHI6F5YHKIPVTH6DPFXDLT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X5ANAHI6F5YHKIPVTH6DPFXDLT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X5ANAHI6F5YHKIPVTH6DPFXDLT/action/storage_attestation","attest_author":"https://pith.science/pith/X5ANAHI6F5YHKIPVTH6DPFXDLT/action/author_attestation","sign_citation":"https://pith.science/pith/X5ANAHI6F5YHKIPVTH6DPFXDLT/action/citation_signature","submit_replication":"https://pith.science/pith/X5ANAHI6F5YHKIPVTH6DPFXDLT/action/replication_record"}},"created_at":"2026-06-24T01:14:57.470391+00:00","updated_at":"2026-06-24T01:14:57.470391+00:00"}