{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:6YZ2XYTIS7ROT7IPGRXTBV5EEQ","short_pith_number":"pith:6YZ2XYTI","schema_version":"1.0","canonical_sha256":"f633abe26897e2e9fd0f346f30d7a4240073ff5dd9ced82c447cd3a3c993c8fe","source":{"kind":"arxiv","id":"1506.06141","version":3},"attestation_state":"computed","paper":{"title":"Discovering Uncolored Naturalness in Exotic Higgs Decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Christopher B. Verhaaren, David Curtin","submitted_at":"2015-06-19T20:01:27Z","abstract_excerpt":"Solutions to the hierarchy problem usually require top partners. In standard SUSY or composite Higgs theories, the partners carry SM color and are becoming increasingly constrained by LHC searches. However, theories like Folded SUSY (FS), Twin Higgs (TH) and Quirky Little Higgs (QLH) introduce uncolored top partners, which can be SM singlets or carry electroweak charge. Their small production cross section left doubt as to whether the LHC can effectively probe such scenarios. Typically, these partners are charged under their own mirror color gauge group. In FS and QLH, the absence of light mir"},"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":"1506.06141","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-06-19T20:01:27Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"f882516cb7b1553ed47e8880320899743296deb606ce063d54a6da8f77e047cf","abstract_canon_sha256":"e8731950d88f7b593292fa1b5aded6f258edd034493945aaa0a1804c02373d5b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:16:18.622056Z","signature_b64":"DA9XmnCQChIA+fxNcAjehp35xqkjkzMTA/aY/Pivk+GB5Z6xj4Jm5TXiel2nJKdlFqyozDBe6c0xhkL0iKzJCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f633abe26897e2e9fd0f346f30d7a4240073ff5dd9ced82c447cd3a3c993c8fe","last_reissued_at":"2026-05-18T01:16:18.621291Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:16:18.621291Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Discovering Uncolored Naturalness in Exotic Higgs Decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Christopher B. Verhaaren, David Curtin","submitted_at":"2015-06-19T20:01:27Z","abstract_excerpt":"Solutions to the hierarchy problem usually require top partners. In standard SUSY or composite Higgs theories, the partners carry SM color and are becoming increasingly constrained by LHC searches. However, theories like Folded SUSY (FS), Twin Higgs (TH) and Quirky Little Higgs (QLH) introduce uncolored top partners, which can be SM singlets or carry electroweak charge. Their small production cross section left doubt as to whether the LHC can effectively probe such scenarios. Typically, these partners are charged under their own mirror color gauge group. In FS and QLH, the absence of light mir"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.06141","kind":"arxiv","version":3},"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":"1506.06141","created_at":"2026-05-18T01:16:18.621431+00:00"},{"alias_kind":"arxiv_version","alias_value":"1506.06141v3","created_at":"2026-05-18T01:16:18.621431+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.06141","created_at":"2026-05-18T01:16:18.621431+00:00"},{"alias_kind":"pith_short_12","alias_value":"6YZ2XYTIS7RO","created_at":"2026-05-18T12:29:07.941421+00:00"},{"alias_kind":"pith_short_16","alias_value":"6YZ2XYTIS7ROT7IP","created_at":"2026-05-18T12:29:07.941421+00:00"},{"alias_kind":"pith_short_8","alias_value":"6YZ2XYTI","created_at":"2026-05-18T12:29:07.941421+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2503.05463","citing_title":"Search for Higgs boson exotic decays into Lorentz-boosted light bosons in the four-$\\tau$ final state at $\\sqrt{s}=13$ TeV with the ATLAS detector","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2602.03235","citing_title":"Search for the production of dark Higgs in the framework of Mono-Z$^{\\prime}$ portal at the FCC-ee simulated electron-positron collisions at $\\sqrt{s} = 240$ GeV","ref_index":9,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6YZ2XYTIS7ROT7IPGRXTBV5EEQ","json":"https://pith.science/pith/6YZ2XYTIS7ROT7IPGRXTBV5EEQ.json","graph_json":"https://pith.science/api/pith-number/6YZ2XYTIS7ROT7IPGRXTBV5EEQ/graph.json","events_json":"https://pith.science/api/pith-number/6YZ2XYTIS7ROT7IPGRXTBV5EEQ/events.json","paper":"https://pith.science/paper/6YZ2XYTI"},"agent_actions":{"view_html":"https://pith.science/pith/6YZ2XYTIS7ROT7IPGRXTBV5EEQ","download_json":"https://pith.science/pith/6YZ2XYTIS7ROT7IPGRXTBV5EEQ.json","view_paper":"https://pith.science/paper/6YZ2XYTI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1506.06141&json=true","fetch_graph":"https://pith.science/api/pith-number/6YZ2XYTIS7ROT7IPGRXTBV5EEQ/graph.json","fetch_events":"https://pith.science/api/pith-number/6YZ2XYTIS7ROT7IPGRXTBV5EEQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6YZ2XYTIS7ROT7IPGRXTBV5EEQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6YZ2XYTIS7ROT7IPGRXTBV5EEQ/action/storage_attestation","attest_author":"https://pith.science/pith/6YZ2XYTIS7ROT7IPGRXTBV5EEQ/action/author_attestation","sign_citation":"https://pith.science/pith/6YZ2XYTIS7ROT7IPGRXTBV5EEQ/action/citation_signature","submit_replication":"https://pith.science/pith/6YZ2XYTIS7ROT7IPGRXTBV5EEQ/action/replication_record"}},"created_at":"2026-05-18T01:16:18.621431+00:00","updated_at":"2026-05-18T01:16:18.621431+00:00"}