{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:NSUH432V73AIPA5I3S3NXGA6M2","short_pith_number":"pith:NSUH432V","schema_version":"1.0","canonical_sha256":"6ca87e6f55fec08783a8dcb6db981e66a21ed3fd5795dbd653dce09f455d9525","source":{"kind":"arxiv","id":"1405.2775","version":5},"attestation_state":"computed","paper":{"title":"Dynamical Generation of the Weak Scale and Inflation in High-Scale Supersymmetry","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"Sibo Zheng","submitted_at":"2014-05-12T14:20:56Z","abstract_excerpt":"Combination of Plank and BICEP2 data reported that tensor to scalar ratio $r\\simeq 0.16$ and scalar spectral index $n_{s}\\simeq 0.96$. In this short note, it is shown that chaotic inflation with quadratic potential, which perfectly accounts for present fit to $r$ and $n_s$, and relatively heavy Higgs mass for fine-tuned MSSM, are both suggested to be consequences of high-scale supersymmetry (SUSY) breaking. Following this idea, we find that inflaton mass is of same order as soft mass, flatness of inflation potential doesn't need a shift symmetry, and scale of inflation energy density automatic"},"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":"1405.2775","kind":"arxiv","version":5},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"hep-ph","submitted_at":"2014-05-12T14:20:56Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"4919d51c0ee5f34ddb4f9f65c79b1e6df64624a0df4f929769b93575662e9d1f","abstract_canon_sha256":"65deb983331422e4981e6e17c54c073e7e68575d6f32cef27f8fa6db3e528305"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:26:31.794356Z","signature_b64":"s0p9Px75qyCTWRLZbv4Q2K8n4NPxEVMyv1nDSNyczJOQUAx1YHpGYzzIEBf05NgB4XIl/OWhPogIo7o/nmzWAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6ca87e6f55fec08783a8dcb6db981e66a21ed3fd5795dbd653dce09f455d9525","last_reissued_at":"2026-05-18T02:26:31.793978Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:26:31.793978Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamical Generation of the Weak Scale and Inflation in High-Scale Supersymmetry","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"Sibo Zheng","submitted_at":"2014-05-12T14:20:56Z","abstract_excerpt":"Combination of Plank and BICEP2 data reported that tensor to scalar ratio $r\\simeq 0.16$ and scalar spectral index $n_{s}\\simeq 0.96$. In this short note, it is shown that chaotic inflation with quadratic potential, which perfectly accounts for present fit to $r$ and $n_s$, and relatively heavy Higgs mass for fine-tuned MSSM, are both suggested to be consequences of high-scale supersymmetry (SUSY) breaking. Following this idea, we find that inflaton mass is of same order as soft mass, flatness of inflation potential doesn't need a shift symmetry, and scale of inflation energy density automatic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.2775","kind":"arxiv","version":5},"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":"1405.2775","created_at":"2026-05-18T02:26:31.794033+00:00"},{"alias_kind":"arxiv_version","alias_value":"1405.2775v5","created_at":"2026-05-18T02:26:31.794033+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.2775","created_at":"2026-05-18T02:26:31.794033+00:00"},{"alias_kind":"pith_short_12","alias_value":"NSUH432V73AI","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_16","alias_value":"NSUH432V73AIPA5I","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_8","alias_value":"NSUH432V","created_at":"2026-05-18T12:28:41.024544+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/NSUH432V73AIPA5I3S3NXGA6M2","json":"https://pith.science/pith/NSUH432V73AIPA5I3S3NXGA6M2.json","graph_json":"https://pith.science/api/pith-number/NSUH432V73AIPA5I3S3NXGA6M2/graph.json","events_json":"https://pith.science/api/pith-number/NSUH432V73AIPA5I3S3NXGA6M2/events.json","paper":"https://pith.science/paper/NSUH432V"},"agent_actions":{"view_html":"https://pith.science/pith/NSUH432V73AIPA5I3S3NXGA6M2","download_json":"https://pith.science/pith/NSUH432V73AIPA5I3S3NXGA6M2.json","view_paper":"https://pith.science/paper/NSUH432V","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1405.2775&json=true","fetch_graph":"https://pith.science/api/pith-number/NSUH432V73AIPA5I3S3NXGA6M2/graph.json","fetch_events":"https://pith.science/api/pith-number/NSUH432V73AIPA5I3S3NXGA6M2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NSUH432V73AIPA5I3S3NXGA6M2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NSUH432V73AIPA5I3S3NXGA6M2/action/storage_attestation","attest_author":"https://pith.science/pith/NSUH432V73AIPA5I3S3NXGA6M2/action/author_attestation","sign_citation":"https://pith.science/pith/NSUH432V73AIPA5I3S3NXGA6M2/action/citation_signature","submit_replication":"https://pith.science/pith/NSUH432V73AIPA5I3S3NXGA6M2/action/replication_record"}},"created_at":"2026-05-18T02:26:31.794033+00:00","updated_at":"2026-05-18T02:26:31.794033+00:00"}