{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:QGYGU3QHPIZZ6HR5D2EYLPZEDO","short_pith_number":"pith:QGYGU3QH","schema_version":"1.0","canonical_sha256":"81b06a6e077a339f1e3d1e8985bf241b81e6b7b7eb906437de51cdf7c904e354","source":{"kind":"arxiv","id":"1705.07973","version":2},"attestation_state":"computed","paper":{"title":"Probing the No-Scale ${\\cal F}$-$SU(5)$ One-Parameter Model via Gluino Searches at the LHC2","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dimitri V. Nanopoulos, James A. Maxin, Tianjun Li","submitted_at":"2017-05-22T20:00:02Z","abstract_excerpt":"In our recent paper entitled \"The return of the King: No-Scale ${\\cal F}$-$SU(5)$\", we showed that the model space supporting the most favorable phenomenology should have been probed in 2016 at the LHC2, with an even further reach into this region of the model in 2017-18. This ideal realm of the one-parameter version of No-Scale ${\\cal F}$-$SU(5)$ yields a 1.9-2.3 TeV gluino mass at the very same point where the light Higgs boson mass enters its rather narrow experimentally determined range of $m_h = 125.09 \\pm 0.24$ GeV. Given the recent results reported at Moriond 2017 for 36 ${\\rm fb}^{-1}$"},"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":"1705.07973","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-05-22T20:00:02Z","cross_cats_sorted":[],"title_canon_sha256":"bd90ab61a7cac51411508a91168d08c23e646ee47e54b0349875be97191c7bfe","abstract_canon_sha256":"f4462a17ba5d0813ea25294b9893dd88478dc1dce96d3f158d1d1b992f64c5e6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:36:43.180200Z","signature_b64":"YPFM0Stb73sI5/RC9QQTN1+xH9/JC+/QiPxBC0lTlfMSxSVhLxwK6JDoYM9SJwPU4d7oPHDvpFfW8SY3ThmDBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"81b06a6e077a339f1e3d1e8985bf241b81e6b7b7eb906437de51cdf7c904e354","last_reissued_at":"2026-05-18T00:36:43.179521Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:36:43.179521Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Probing the No-Scale ${\\cal F}$-$SU(5)$ One-Parameter Model via Gluino Searches at the LHC2","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dimitri V. Nanopoulos, James A. Maxin, Tianjun Li","submitted_at":"2017-05-22T20:00:02Z","abstract_excerpt":"In our recent paper entitled \"The return of the King: No-Scale ${\\cal F}$-$SU(5)$\", we showed that the model space supporting the most favorable phenomenology should have been probed in 2016 at the LHC2, with an even further reach into this region of the model in 2017-18. This ideal realm of the one-parameter version of No-Scale ${\\cal F}$-$SU(5)$ yields a 1.9-2.3 TeV gluino mass at the very same point where the light Higgs boson mass enters its rather narrow experimentally determined range of $m_h = 125.09 \\pm 0.24$ GeV. Given the recent results reported at Moriond 2017 for 36 ${\\rm fb}^{-1}$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.07973","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":"1705.07973","created_at":"2026-05-18T00:36:43.179633+00:00"},{"alias_kind":"arxiv_version","alias_value":"1705.07973v2","created_at":"2026-05-18T00:36:43.179633+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.07973","created_at":"2026-05-18T00:36:43.179633+00:00"},{"alias_kind":"pith_short_12","alias_value":"QGYGU3QHPIZZ","created_at":"2026-05-18T12:31:37.085036+00:00"},{"alias_kind":"pith_short_16","alias_value":"QGYGU3QHPIZZ6HR5","created_at":"2026-05-18T12:31:37.085036+00:00"},{"alias_kind":"pith_short_8","alias_value":"QGYGU3QH","created_at":"2026-05-18T12:31:37.085036+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/QGYGU3QHPIZZ6HR5D2EYLPZEDO","json":"https://pith.science/pith/QGYGU3QHPIZZ6HR5D2EYLPZEDO.json","graph_json":"https://pith.science/api/pith-number/QGYGU3QHPIZZ6HR5D2EYLPZEDO/graph.json","events_json":"https://pith.science/api/pith-number/QGYGU3QHPIZZ6HR5D2EYLPZEDO/events.json","paper":"https://pith.science/paper/QGYGU3QH"},"agent_actions":{"view_html":"https://pith.science/pith/QGYGU3QHPIZZ6HR5D2EYLPZEDO","download_json":"https://pith.science/pith/QGYGU3QHPIZZ6HR5D2EYLPZEDO.json","view_paper":"https://pith.science/paper/QGYGU3QH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1705.07973&json=true","fetch_graph":"https://pith.science/api/pith-number/QGYGU3QHPIZZ6HR5D2EYLPZEDO/graph.json","fetch_events":"https://pith.science/api/pith-number/QGYGU3QHPIZZ6HR5D2EYLPZEDO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QGYGU3QHPIZZ6HR5D2EYLPZEDO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QGYGU3QHPIZZ6HR5D2EYLPZEDO/action/storage_attestation","attest_author":"https://pith.science/pith/QGYGU3QHPIZZ6HR5D2EYLPZEDO/action/author_attestation","sign_citation":"https://pith.science/pith/QGYGU3QHPIZZ6HR5D2EYLPZEDO/action/citation_signature","submit_replication":"https://pith.science/pith/QGYGU3QHPIZZ6HR5D2EYLPZEDO/action/replication_record"}},"created_at":"2026-05-18T00:36:43.179633+00:00","updated_at":"2026-05-18T00:36:43.179633+00:00"}