{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:MWNLK2ECLB7ZIU6WXBPEEEYXCC","short_pith_number":"pith:MWNLK2EC","schema_version":"1.0","canonical_sha256":"659ab56882587f9453d6b85e42131710911e90ea501a5b4bcdc9b5a146fe57f1","source":{"kind":"arxiv","id":"1506.01410","version":2},"attestation_state":"computed","paper":{"title":"$\\mu$-Term Hybrid Inflation and Split Supersymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Nobuchika Okada, Qaisar Shafi","submitted_at":"2015-06-03T21:13:38Z","abstract_excerpt":"We consider $\\mu$-term hybrid inflation which, in its minimal format with gravity mediated supersymmetry breaking, leads to split supersymmetry. The MSSM $\\mu$-term in this framework is larger than the gravitino mass $m_G$, and successful inflation requires $m_G$ (and hence also $|\\mu|$) $\\gtrsim 5 \\times 10^7$ GeV, such that the gravitino decays before the LSP neutralino freezes out. Assuming universal scalar masses of the same order as $m_G$, this leads to split supersymmetry. The LSP wino with mass $\\simeq$ 2 TeV is a plausible dark matter candidate, the gluino may be accessible at the LHC,"},"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":"1506.01410","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-06-03T21:13:38Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"6456166059baacf9dde1be26e763444b319176bd440948b2b21057e05dcacaf7","abstract_canon_sha256":"76d1e88e874eb056ebaa10f614ed1b2828974c910ec6f0c2dee8288936de6478"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:24:45.577276Z","signature_b64":"IfnnxaAh4jXpP1PHpSHuOez2YWV5HKtJw/xt4wx86Jl0Shm8EoCrzou0OJLsCDP6HKuYh3N8wzHeELoZXRhpAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"659ab56882587f9453d6b85e42131710911e90ea501a5b4bcdc9b5a146fe57f1","last_reissued_at":"2026-05-18T00:24:45.576554Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:24:45.576554Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$\\mu$-Term Hybrid Inflation and Split Supersymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Nobuchika Okada, Qaisar Shafi","submitted_at":"2015-06-03T21:13:38Z","abstract_excerpt":"We consider $\\mu$-term hybrid inflation which, in its minimal format with gravity mediated supersymmetry breaking, leads to split supersymmetry. The MSSM $\\mu$-term in this framework is larger than the gravitino mass $m_G$, and successful inflation requires $m_G$ (and hence also $|\\mu|$) $\\gtrsim 5 \\times 10^7$ GeV, such that the gravitino decays before the LSP neutralino freezes out. Assuming universal scalar masses of the same order as $m_G$, this leads to split supersymmetry. The LSP wino with mass $\\simeq$ 2 TeV is a plausible dark matter candidate, the gluino may be accessible at the LHC,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.01410","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":"1506.01410","created_at":"2026-05-18T00:24:45.576683+00:00"},{"alias_kind":"arxiv_version","alias_value":"1506.01410v2","created_at":"2026-05-18T00:24:45.576683+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.01410","created_at":"2026-05-18T00:24:45.576683+00:00"},{"alias_kind":"pith_short_12","alias_value":"MWNLK2ECLB7Z","created_at":"2026-05-18T12:29:32.376354+00:00"},{"alias_kind":"pith_short_16","alias_value":"MWNLK2ECLB7ZIU6W","created_at":"2026-05-18T12:29:32.376354+00:00"},{"alias_kind":"pith_short_8","alias_value":"MWNLK2EC","created_at":"2026-05-18T12:29:32.376354+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/MWNLK2ECLB7ZIU6WXBPEEEYXCC","json":"https://pith.science/pith/MWNLK2ECLB7ZIU6WXBPEEEYXCC.json","graph_json":"https://pith.science/api/pith-number/MWNLK2ECLB7ZIU6WXBPEEEYXCC/graph.json","events_json":"https://pith.science/api/pith-number/MWNLK2ECLB7ZIU6WXBPEEEYXCC/events.json","paper":"https://pith.science/paper/MWNLK2EC"},"agent_actions":{"view_html":"https://pith.science/pith/MWNLK2ECLB7ZIU6WXBPEEEYXCC","download_json":"https://pith.science/pith/MWNLK2ECLB7ZIU6WXBPEEEYXCC.json","view_paper":"https://pith.science/paper/MWNLK2EC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1506.01410&json=true","fetch_graph":"https://pith.science/api/pith-number/MWNLK2ECLB7ZIU6WXBPEEEYXCC/graph.json","fetch_events":"https://pith.science/api/pith-number/MWNLK2ECLB7ZIU6WXBPEEEYXCC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MWNLK2ECLB7ZIU6WXBPEEEYXCC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MWNLK2ECLB7ZIU6WXBPEEEYXCC/action/storage_attestation","attest_author":"https://pith.science/pith/MWNLK2ECLB7ZIU6WXBPEEEYXCC/action/author_attestation","sign_citation":"https://pith.science/pith/MWNLK2ECLB7ZIU6WXBPEEEYXCC/action/citation_signature","submit_replication":"https://pith.science/pith/MWNLK2ECLB7ZIU6WXBPEEEYXCC/action/replication_record"}},"created_at":"2026-05-18T00:24:45.576683+00:00","updated_at":"2026-05-18T00:24:45.576683+00:00"}