{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:WKMCO64FZHF2B2WI7XFZ77WKWJ","short_pith_number":"pith:WKMCO64F","schema_version":"1.0","canonical_sha256":"b298277b85c9cba0eac8fdcb9ffecab26b2f33d3c59679ab30d7e9cf6e6c61f8","source":{"kind":"arxiv","id":"1201.4722","version":3},"attestation_state":"computed","paper":{"title":"Techni-dilaton at 125 GeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Koichi Yamawaki, Shinya Matsuzaki","submitted_at":"2012-01-23T14:12:32Z","abstract_excerpt":"Walking technicolor predicts a light composite scalar, techni-dilaton, arising as a pseudo Nambu-Goldstone boson for the approximate scale symmetry spontaneously broken by techni-fermion condensation. We show that a light techni-dilaton with mass of around 125 GeV can explain presently observed excesses particularly in the di-photon decay channel at LHC."},"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":"1201.4722","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-01-23T14:12:32Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"d711c734cdd1e5e0f4ff70040fa270c5a718f5c9ca75808e5c9e617c5773512b","abstract_canon_sha256":"51340e4002dfae49dc334f7f0eb562a527ba95edec989bbf8ba7cc5df60048f0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:43.456516Z","signature_b64":"dHUbw37VNEJpeKRe6D59ExVdyocFlem3D5kkVv0K1xsPN5c8RT0XZ6VQdnTiF3CJGW3Dw6l9f6p5ZN1NzYPSCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b298277b85c9cba0eac8fdcb9ffecab26b2f33d3c59679ab30d7e9cf6e6c61f8","last_reissued_at":"2026-05-18T01:58:43.455743Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:43.455743Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Techni-dilaton at 125 GeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Koichi Yamawaki, Shinya Matsuzaki","submitted_at":"2012-01-23T14:12:32Z","abstract_excerpt":"Walking technicolor predicts a light composite scalar, techni-dilaton, arising as a pseudo Nambu-Goldstone boson for the approximate scale symmetry spontaneously broken by techni-fermion condensation. We show that a light techni-dilaton with mass of around 125 GeV can explain presently observed excesses particularly in the di-photon decay channel at LHC."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.4722","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":"1201.4722","created_at":"2026-05-18T01:58:43.455864+00:00"},{"alias_kind":"arxiv_version","alias_value":"1201.4722v3","created_at":"2026-05-18T01:58:43.455864+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.4722","created_at":"2026-05-18T01:58:43.455864+00:00"},{"alias_kind":"pith_short_12","alias_value":"WKMCO64FZHF2","created_at":"2026-05-18T12:27:25.539911+00:00"},{"alias_kind":"pith_short_16","alias_value":"WKMCO64FZHF2B2WI","created_at":"2026-05-18T12:27:25.539911+00:00"},{"alias_kind":"pith_short_8","alias_value":"WKMCO64F","created_at":"2026-05-18T12:27:25.539911+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/WKMCO64FZHF2B2WI7XFZ77WKWJ","json":"https://pith.science/pith/WKMCO64FZHF2B2WI7XFZ77WKWJ.json","graph_json":"https://pith.science/api/pith-number/WKMCO64FZHF2B2WI7XFZ77WKWJ/graph.json","events_json":"https://pith.science/api/pith-number/WKMCO64FZHF2B2WI7XFZ77WKWJ/events.json","paper":"https://pith.science/paper/WKMCO64F"},"agent_actions":{"view_html":"https://pith.science/pith/WKMCO64FZHF2B2WI7XFZ77WKWJ","download_json":"https://pith.science/pith/WKMCO64FZHF2B2WI7XFZ77WKWJ.json","view_paper":"https://pith.science/paper/WKMCO64F","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1201.4722&json=true","fetch_graph":"https://pith.science/api/pith-number/WKMCO64FZHF2B2WI7XFZ77WKWJ/graph.json","fetch_events":"https://pith.science/api/pith-number/WKMCO64FZHF2B2WI7XFZ77WKWJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WKMCO64FZHF2B2WI7XFZ77WKWJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WKMCO64FZHF2B2WI7XFZ77WKWJ/action/storage_attestation","attest_author":"https://pith.science/pith/WKMCO64FZHF2B2WI7XFZ77WKWJ/action/author_attestation","sign_citation":"https://pith.science/pith/WKMCO64FZHF2B2WI7XFZ77WKWJ/action/citation_signature","submit_replication":"https://pith.science/pith/WKMCO64FZHF2B2WI7XFZ77WKWJ/action/replication_record"}},"created_at":"2026-05-18T01:58:43.455864+00:00","updated_at":"2026-05-18T01:58:43.455864+00:00"}