{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:V5CYA3FCEIAP6CVHDDUIIZBH4W","short_pith_number":"pith:V5CYA3FC","schema_version":"1.0","canonical_sha256":"af45806ca22200ff0aa718e8846427e58f84bd834047f6f65efbbce4b9fa2e0b","source":{"kind":"arxiv","id":"2211.07742","version":1},"attestation_state":"computed","paper":{"title":"Aligning a Majorana fermion's anapole moment with an external current through photon emission mediated by the fermion's generalized polarizabilities","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"David C. Latimer, Kiana Walter, Kobi Hall","submitted_at":"2022-11-14T20:40:09Z","abstract_excerpt":"The sole static electromagnetic property of a spin-$\\frac{1}{2}$ Majorana fermion is its anapole moment. Though they cannot couple to single real photons, these particles can interact with electric currents through virtual photons. If a Majorana fermion is immersed in a background current, there is an energy difference between the spin states of the fermion; the higher energy state has its anapole moment antialigned with the current. In this paper, we address the ability of a system of initially unpolarized Majorana fermions to achieve some degree of polarization relative to a static backgroun"},"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":"2211.07742","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-11-14T20:40:09Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"718f09cb62d4a67249f80c97f6b0606f5a98863b1fc2ceeb6525844a62d3fce9","abstract_canon_sha256":"851e9af9467e4eca6fc00173fd9e564064b17066fcfdf84740a12fa204083492"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:23:00.209472Z","signature_b64":"ggAnTFumoKCal7Gotun4DrHFs+aBP/Qq8EDoT9k2ka//CF/RWS3Hf6knd6ZENYcRCaKLiUspfM2Zpm3SpNpwDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"af45806ca22200ff0aa718e8846427e58f84bd834047f6f65efbbce4b9fa2e0b","last_reissued_at":"2026-07-05T05:23:00.209044Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:23:00.209044Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Aligning a Majorana fermion's anapole moment with an external current through photon emission mediated by the fermion's generalized polarizabilities","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"David C. Latimer, Kiana Walter, Kobi Hall","submitted_at":"2022-11-14T20:40:09Z","abstract_excerpt":"The sole static electromagnetic property of a spin-$\\frac{1}{2}$ Majorana fermion is its anapole moment. Though they cannot couple to single real photons, these particles can interact with electric currents through virtual photons. If a Majorana fermion is immersed in a background current, there is an energy difference between the spin states of the fermion; the higher energy state has its anapole moment antialigned with the current. In this paper, we address the ability of a system of initially unpolarized Majorana fermions to achieve some degree of polarization relative to a static backgroun"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.07742","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2211.07742/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":"2211.07742","created_at":"2026-07-05T05:23:00.209109+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.07742v1","created_at":"2026-07-05T05:23:00.209109+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.07742","created_at":"2026-07-05T05:23:00.209109+00:00"},{"alias_kind":"pith_short_12","alias_value":"V5CYA3FCEIAP","created_at":"2026-07-05T05:23:00.209109+00:00"},{"alias_kind":"pith_short_16","alias_value":"V5CYA3FCEIAP6CVH","created_at":"2026-07-05T05:23:00.209109+00:00"},{"alias_kind":"pith_short_8","alias_value":"V5CYA3FC","created_at":"2026-07-05T05:23:00.209109+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/V5CYA3FCEIAP6CVHDDUIIZBH4W","json":"https://pith.science/pith/V5CYA3FCEIAP6CVHDDUIIZBH4W.json","graph_json":"https://pith.science/api/pith-number/V5CYA3FCEIAP6CVHDDUIIZBH4W/graph.json","events_json":"https://pith.science/api/pith-number/V5CYA3FCEIAP6CVHDDUIIZBH4W/events.json","paper":"https://pith.science/paper/V5CYA3FC"},"agent_actions":{"view_html":"https://pith.science/pith/V5CYA3FCEIAP6CVHDDUIIZBH4W","download_json":"https://pith.science/pith/V5CYA3FCEIAP6CVHDDUIIZBH4W.json","view_paper":"https://pith.science/paper/V5CYA3FC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.07742&json=true","fetch_graph":"https://pith.science/api/pith-number/V5CYA3FCEIAP6CVHDDUIIZBH4W/graph.json","fetch_events":"https://pith.science/api/pith-number/V5CYA3FCEIAP6CVHDDUIIZBH4W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V5CYA3FCEIAP6CVHDDUIIZBH4W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V5CYA3FCEIAP6CVHDDUIIZBH4W/action/storage_attestation","attest_author":"https://pith.science/pith/V5CYA3FCEIAP6CVHDDUIIZBH4W/action/author_attestation","sign_citation":"https://pith.science/pith/V5CYA3FCEIAP6CVHDDUIIZBH4W/action/citation_signature","submit_replication":"https://pith.science/pith/V5CYA3FCEIAP6CVHDDUIIZBH4W/action/replication_record"}},"created_at":"2026-07-05T05:23:00.209109+00:00","updated_at":"2026-07-05T05:23:00.209109+00:00"}