{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:GYBKQOE4FDQI25GYILUSVWA3AV","short_pith_number":"pith:GYBKQOE4","schema_version":"1.0","canonical_sha256":"3602a8389c28e08d74d842e92ad81b0551aa3aa4694cf94b4a158ca634e946a7","source":{"kind":"arxiv","id":"1111.2830","version":2},"attestation_state":"computed","paper":{"title":"Constraints on supersymmetry with light third family from LHC data","license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Biswarup Mukhopadhyaya (Harish-Chandra Research Institute), Nishita Desai","submitted_at":"2011-11-11T19:35:28Z","abstract_excerpt":"We present a re-interpretation of the recent ATLAS limits on supersymmetry in channels with jets (with and without b-tags) and missing energy, in the context of light third family squarks, while the first two squark families are inaccessible at the 7 TeV run of the Large Hadron Collider (LHC). In contrast to interpretations in terms of the high-scale based constrained minimal supersymmetric standard model (CMSSM), we primarily use the low-scale parametrisation of the phenomenological MSSM (pMSSM), and translate the limits in terms of physical masses of the third family squarks. Side by side, w"},"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":"1111.2830","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"hep-ph","submitted_at":"2011-11-11T19:35:28Z","cross_cats_sorted":[],"title_canon_sha256":"5938760be7edffa5e6cb752816972199860168469e69305e2cd7a12380e3d2dd","abstract_canon_sha256":"bc42141930db9c219c549dc4ce9360d6d9d5a0f54f78789669bd8381d4bcaddf"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:44:13.642654Z","signature_b64":"4E4zQ1182yKHDMQ98jBMTJHGXOSL4jQhudYFHMfXugONtp2vfkyI117C0kPqW4PICCaCNk2aIMl6xdrXoSHcCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3602a8389c28e08d74d842e92ad81b0551aa3aa4694cf94b4a158ca634e946a7","last_reissued_at":"2026-05-18T03:44:13.642160Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:44:13.642160Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Constraints on supersymmetry with light third family from LHC data","license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Biswarup Mukhopadhyaya (Harish-Chandra Research Institute), Nishita Desai","submitted_at":"2011-11-11T19:35:28Z","abstract_excerpt":"We present a re-interpretation of the recent ATLAS limits on supersymmetry in channels with jets (with and without b-tags) and missing energy, in the context of light third family squarks, while the first two squark families are inaccessible at the 7 TeV run of the Large Hadron Collider (LHC). In contrast to interpretations in terms of the high-scale based constrained minimal supersymmetric standard model (CMSSM), we primarily use the low-scale parametrisation of the phenomenological MSSM (pMSSM), and translate the limits in terms of physical masses of the third family squarks. Side by side, w"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.2830","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":"1111.2830","created_at":"2026-05-18T03:44:13.642241+00:00"},{"alias_kind":"arxiv_version","alias_value":"1111.2830v2","created_at":"2026-05-18T03:44:13.642241+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.2830","created_at":"2026-05-18T03:44:13.642241+00:00"},{"alias_kind":"pith_short_12","alias_value":"GYBKQOE4FDQI","created_at":"2026-05-18T12:26:30.835961+00:00"},{"alias_kind":"pith_short_16","alias_value":"GYBKQOE4FDQI25GY","created_at":"2026-05-18T12:26:30.835961+00:00"},{"alias_kind":"pith_short_8","alias_value":"GYBKQOE4","created_at":"2026-05-18T12:26:30.835961+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/GYBKQOE4FDQI25GYILUSVWA3AV","json":"https://pith.science/pith/GYBKQOE4FDQI25GYILUSVWA3AV.json","graph_json":"https://pith.science/api/pith-number/GYBKQOE4FDQI25GYILUSVWA3AV/graph.json","events_json":"https://pith.science/api/pith-number/GYBKQOE4FDQI25GYILUSVWA3AV/events.json","paper":"https://pith.science/paper/GYBKQOE4"},"agent_actions":{"view_html":"https://pith.science/pith/GYBKQOE4FDQI25GYILUSVWA3AV","download_json":"https://pith.science/pith/GYBKQOE4FDQI25GYILUSVWA3AV.json","view_paper":"https://pith.science/paper/GYBKQOE4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1111.2830&json=true","fetch_graph":"https://pith.science/api/pith-number/GYBKQOE4FDQI25GYILUSVWA3AV/graph.json","fetch_events":"https://pith.science/api/pith-number/GYBKQOE4FDQI25GYILUSVWA3AV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GYBKQOE4FDQI25GYILUSVWA3AV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GYBKQOE4FDQI25GYILUSVWA3AV/action/storage_attestation","attest_author":"https://pith.science/pith/GYBKQOE4FDQI25GYILUSVWA3AV/action/author_attestation","sign_citation":"https://pith.science/pith/GYBKQOE4FDQI25GYILUSVWA3AV/action/citation_signature","submit_replication":"https://pith.science/pith/GYBKQOE4FDQI25GYILUSVWA3AV/action/replication_record"}},"created_at":"2026-05-18T03:44:13.642241+00:00","updated_at":"2026-05-18T03:44:13.642241+00:00"}