{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:CS3YGS765NFWV7VN26PWMPEXZ3","short_pith_number":"pith:CS3YGS76","schema_version":"1.0","canonical_sha256":"14b7834bfeeb4b6afeadd79f663c97cecd500681df6021785e51b0928ee952aa","source":{"kind":"arxiv","id":"1412.3107","version":2},"attestation_state":"computed","paper":{"title":"Precision Natural SUSY at CEPC, FCC-ee, and ILC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"JiJi Fan, Lian-Tao Wang, Matthew Reece","submitted_at":"2014-12-09T21:00:00Z","abstract_excerpt":"Testing the idea of naturalness is and will continue to be one of the most important goals of high energy physics experiments. It will play a central role in the physics program of future colliders. In this paper, we present projections of the reach of natural SUSY at future lepton colliders: CEPC, FCC-ee and ILC. We focus on the observables which give the strongest reach, the electroweak precision observables (for left-handed stops), and Higgs to gluon and photon decay rates (for both left- and right-handed stops). There is a \"blind spot\" when the stop mixing parameter Xt is approximately equ"},"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":"1412.3107","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-12-09T21:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"124cab3c893c86484535a86b6bb0b0c37aadfe673a861739d74b9233546c4efd","abstract_canon_sha256":"2ddfce9211fa45def0d548a4adcd3df31e76f9a1584ac545927da64b22479c11"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:33:48.955470Z","signature_b64":"iBQRx9wvyX1UqyuTFeRLPD/bL5HMJpeq26q1O4NaAeQrWKrKrM5um2Ad3TPu1fuKJwXJDnW9DlZvxaIRveYGCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"14b7834bfeeb4b6afeadd79f663c97cecd500681df6021785e51b0928ee952aa","last_reissued_at":"2026-05-18T01:33:48.954814Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:33:48.954814Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Precision Natural SUSY at CEPC, FCC-ee, and ILC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"JiJi Fan, Lian-Tao Wang, Matthew Reece","submitted_at":"2014-12-09T21:00:00Z","abstract_excerpt":"Testing the idea of naturalness is and will continue to be one of the most important goals of high energy physics experiments. It will play a central role in the physics program of future colliders. In this paper, we present projections of the reach of natural SUSY at future lepton colliders: CEPC, FCC-ee and ILC. We focus on the observables which give the strongest reach, the electroweak precision observables (for left-handed stops), and Higgs to gluon and photon decay rates (for both left- and right-handed stops). There is a \"blind spot\" when the stop mixing parameter Xt is approximately equ"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.3107","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":"1412.3107","created_at":"2026-05-18T01:33:48.954935+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.3107v2","created_at":"2026-05-18T01:33:48.954935+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.3107","created_at":"2026-05-18T01:33:48.954935+00:00"},{"alias_kind":"pith_short_12","alias_value":"CS3YGS765NFW","created_at":"2026-05-18T12:28:22.404517+00:00"},{"alias_kind":"pith_short_16","alias_value":"CS3YGS765NFWV7VN","created_at":"2026-05-18T12:28:22.404517+00:00"},{"alias_kind":"pith_short_8","alias_value":"CS3YGS76","created_at":"2026-05-18T12:28:22.404517+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.00272","citing_title":"Future Circular Collider Feasibility Study Report: Volume 1, Physics, Experiments, Detectors","ref_index":112,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CS3YGS765NFWV7VN26PWMPEXZ3","json":"https://pith.science/pith/CS3YGS765NFWV7VN26PWMPEXZ3.json","graph_json":"https://pith.science/api/pith-number/CS3YGS765NFWV7VN26PWMPEXZ3/graph.json","events_json":"https://pith.science/api/pith-number/CS3YGS765NFWV7VN26PWMPEXZ3/events.json","paper":"https://pith.science/paper/CS3YGS76"},"agent_actions":{"view_html":"https://pith.science/pith/CS3YGS765NFWV7VN26PWMPEXZ3","download_json":"https://pith.science/pith/CS3YGS765NFWV7VN26PWMPEXZ3.json","view_paper":"https://pith.science/paper/CS3YGS76","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.3107&json=true","fetch_graph":"https://pith.science/api/pith-number/CS3YGS765NFWV7VN26PWMPEXZ3/graph.json","fetch_events":"https://pith.science/api/pith-number/CS3YGS765NFWV7VN26PWMPEXZ3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CS3YGS765NFWV7VN26PWMPEXZ3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CS3YGS765NFWV7VN26PWMPEXZ3/action/storage_attestation","attest_author":"https://pith.science/pith/CS3YGS765NFWV7VN26PWMPEXZ3/action/author_attestation","sign_citation":"https://pith.science/pith/CS3YGS765NFWV7VN26PWMPEXZ3/action/citation_signature","submit_replication":"https://pith.science/pith/CS3YGS765NFWV7VN26PWMPEXZ3/action/replication_record"}},"created_at":"2026-05-18T01:33:48.954935+00:00","updated_at":"2026-05-18T01:33:48.954935+00:00"}