{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:TXCV7N2HJMWZKDHFYVG5UOBFYY","short_pith_number":"pith:TXCV7N2H","schema_version":"1.0","canonical_sha256":"9dc55fb7474b2d950ce5c54dda3825c622b8192fad59a61b24f0cf13b2811b5b","source":{"kind":"arxiv","id":"1512.05332","version":4},"attestation_state":"computed","paper":{"title":"Interpreting a 750 GeV Diphoton Resonance","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Emmanuel Stamou, Gilad Perez, Rick S. Gupta, Sebastian J\\\"ager, Yevgeny Kats","submitted_at":"2015-12-16T20:55:11Z","abstract_excerpt":"We discuss the implications of the significant excesses in the diphoton final state observed by the LHC experiments ATLAS and CMS around a diphoton invariant mass of 750 GeV. The interpretation of the excess as a spin-zero s-channel resonance implies model-independent lower bounds on both its branching ratio and its coupling to photons, which stringently constrain dynamical models. We consider both the case where the excess is described by a narrow and a broad resonance. We also obtain model-independent constraints on the allowed couplings and branching fractions to final states other than dip"},"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":"1512.05332","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-12-16T20:55:11Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"9a3580f7dc7b5a7aa967b8ec0df6e40bf4196c740cccd197b6511c9a29570d68","abstract_canon_sha256":"632e4de7d100ca8acc2661ff1dd7e0982ec9b565e7ff1408abb2faa5bf0e695d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:10:14.823217Z","signature_b64":"qEgxaMfVcHDeBqw5qzLSCqTE+QzTPg/qoeIEtAgjxl/jah+n+UzTfux5DLQFyurRYH1DTOGieSGfavghzhajDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9dc55fb7474b2d950ce5c54dda3825c622b8192fad59a61b24f0cf13b2811b5b","last_reissued_at":"2026-05-18T01:10:14.822678Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:10:14.822678Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Interpreting a 750 GeV Diphoton Resonance","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Emmanuel Stamou, Gilad Perez, Rick S. Gupta, Sebastian J\\\"ager, Yevgeny Kats","submitted_at":"2015-12-16T20:55:11Z","abstract_excerpt":"We discuss the implications of the significant excesses in the diphoton final state observed by the LHC experiments ATLAS and CMS around a diphoton invariant mass of 750 GeV. The interpretation of the excess as a spin-zero s-channel resonance implies model-independent lower bounds on both its branching ratio and its coupling to photons, which stringently constrain dynamical models. We consider both the case where the excess is described by a narrow and a broad resonance. We also obtain model-independent constraints on the allowed couplings and branching fractions to final states other than dip"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.05332","kind":"arxiv","version":4},"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":"1512.05332","created_at":"2026-05-18T01:10:14.822763+00:00"},{"alias_kind":"arxiv_version","alias_value":"1512.05332v4","created_at":"2026-05-18T01:10:14.822763+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.05332","created_at":"2026-05-18T01:10:14.822763+00:00"},{"alias_kind":"pith_short_12","alias_value":"TXCV7N2HJMWZ","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_16","alias_value":"TXCV7N2HJMWZKDHF","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_8","alias_value":"TXCV7N2H","created_at":"2026-05-18T12:29:42.218222+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/TXCV7N2HJMWZKDHFYVG5UOBFYY","json":"https://pith.science/pith/TXCV7N2HJMWZKDHFYVG5UOBFYY.json","graph_json":"https://pith.science/api/pith-number/TXCV7N2HJMWZKDHFYVG5UOBFYY/graph.json","events_json":"https://pith.science/api/pith-number/TXCV7N2HJMWZKDHFYVG5UOBFYY/events.json","paper":"https://pith.science/paper/TXCV7N2H"},"agent_actions":{"view_html":"https://pith.science/pith/TXCV7N2HJMWZKDHFYVG5UOBFYY","download_json":"https://pith.science/pith/TXCV7N2HJMWZKDHFYVG5UOBFYY.json","view_paper":"https://pith.science/paper/TXCV7N2H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1512.05332&json=true","fetch_graph":"https://pith.science/api/pith-number/TXCV7N2HJMWZKDHFYVG5UOBFYY/graph.json","fetch_events":"https://pith.science/api/pith-number/TXCV7N2HJMWZKDHFYVG5UOBFYY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TXCV7N2HJMWZKDHFYVG5UOBFYY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TXCV7N2HJMWZKDHFYVG5UOBFYY/action/storage_attestation","attest_author":"https://pith.science/pith/TXCV7N2HJMWZKDHFYVG5UOBFYY/action/author_attestation","sign_citation":"https://pith.science/pith/TXCV7N2HJMWZKDHFYVG5UOBFYY/action/citation_signature","submit_replication":"https://pith.science/pith/TXCV7N2HJMWZKDHFYVG5UOBFYY/action/replication_record"}},"created_at":"2026-05-18T01:10:14.822763+00:00","updated_at":"2026-05-18T01:10:14.822763+00:00"}