{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:2OJDZCNOHYFFX7NTLWIDJWVL3I","short_pith_number":"pith:2OJDZCNO","schema_version":"1.0","canonical_sha256":"d3923c89ae3e0a5bfdb35d9034daabda27e19445d2a3edefe219eb7b8d2d52a6","source":{"kind":"arxiv","id":"1508.05396","version":2},"attestation_state":"computed","paper":{"title":"Folded Supersymmetry with a Twist","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"David Pinner, Hou Keong Lou, Nathaniel Craig, Timothy Cohen","submitted_at":"2015-08-21T20:09:38Z","abstract_excerpt":"Folded supersymmetry (f-SUSY) stabilizes the weak scale against radiative corrections from the top sector via scalar partners whose gauge quantum numbers differ from their Standard Model counterparts. This non-trivial pairing of states can be realized in extra-dimensional theories with appropriate supersymmetry-breaking boundary conditions. We present a class of calculable f-SUSY models that are parametrized by a non-trivial twist in 5D boundary conditions and can accommodate the observed Higgs mass and couplings. Although the distinctive phenomenology associated with the novel folded states s"},"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":"1508.05396","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-08-21T20:09:38Z","cross_cats_sorted":[],"title_canon_sha256":"ceb3c4b5dd9bfd464b847f2849cc85ffa232d36dd844ab6d2b664f7d99133000","abstract_canon_sha256":"44665e7411798779d99b34affd22203798b0fd6c69092649d286d6c5ed01bb38"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:17:30.619221Z","signature_b64":"feNRymh6epUUaurtyJCW14CvSmklhL76wipBAHrwD2BZca9SFSSXWRIllgTQuy+WykYpj94uZ1g/ZLYx//R5DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d3923c89ae3e0a5bfdb35d9034daabda27e19445d2a3edefe219eb7b8d2d52a6","last_reissued_at":"2026-05-18T01:17:30.618440Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:17:30.618440Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Folded Supersymmetry with a Twist","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"David Pinner, Hou Keong Lou, Nathaniel Craig, Timothy Cohen","submitted_at":"2015-08-21T20:09:38Z","abstract_excerpt":"Folded supersymmetry (f-SUSY) stabilizes the weak scale against radiative corrections from the top sector via scalar partners whose gauge quantum numbers differ from their Standard Model counterparts. This non-trivial pairing of states can be realized in extra-dimensional theories with appropriate supersymmetry-breaking boundary conditions. We present a class of calculable f-SUSY models that are parametrized by a non-trivial twist in 5D boundary conditions and can accommodate the observed Higgs mass and couplings. Although the distinctive phenomenology associated with the novel folded states s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.05396","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":"1508.05396","created_at":"2026-05-18T01:17:30.618573+00:00"},{"alias_kind":"arxiv_version","alias_value":"1508.05396v2","created_at":"2026-05-18T01:17:30.618573+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.05396","created_at":"2026-05-18T01:17:30.618573+00:00"},{"alias_kind":"pith_short_12","alias_value":"2OJDZCNOHYFF","created_at":"2026-05-18T12:29:02.477457+00:00"},{"alias_kind":"pith_short_16","alias_value":"2OJDZCNOHYFFX7NT","created_at":"2026-05-18T12:29:02.477457+00:00"},{"alias_kind":"pith_short_8","alias_value":"2OJDZCNO","created_at":"2026-05-18T12:29:02.477457+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.10141","citing_title":"Searching for long-lived dark scalars at the FCC-ee","ref_index":7,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2OJDZCNOHYFFX7NTLWIDJWVL3I","json":"https://pith.science/pith/2OJDZCNOHYFFX7NTLWIDJWVL3I.json","graph_json":"https://pith.science/api/pith-number/2OJDZCNOHYFFX7NTLWIDJWVL3I/graph.json","events_json":"https://pith.science/api/pith-number/2OJDZCNOHYFFX7NTLWIDJWVL3I/events.json","paper":"https://pith.science/paper/2OJDZCNO"},"agent_actions":{"view_html":"https://pith.science/pith/2OJDZCNOHYFFX7NTLWIDJWVL3I","download_json":"https://pith.science/pith/2OJDZCNOHYFFX7NTLWIDJWVL3I.json","view_paper":"https://pith.science/paper/2OJDZCNO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1508.05396&json=true","fetch_graph":"https://pith.science/api/pith-number/2OJDZCNOHYFFX7NTLWIDJWVL3I/graph.json","fetch_events":"https://pith.science/api/pith-number/2OJDZCNOHYFFX7NTLWIDJWVL3I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2OJDZCNOHYFFX7NTLWIDJWVL3I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2OJDZCNOHYFFX7NTLWIDJWVL3I/action/storage_attestation","attest_author":"https://pith.science/pith/2OJDZCNOHYFFX7NTLWIDJWVL3I/action/author_attestation","sign_citation":"https://pith.science/pith/2OJDZCNOHYFFX7NTLWIDJWVL3I/action/citation_signature","submit_replication":"https://pith.science/pith/2OJDZCNOHYFFX7NTLWIDJWVL3I/action/replication_record"}},"created_at":"2026-05-18T01:17:30.618573+00:00","updated_at":"2026-05-18T01:17:30.618573+00:00"}