{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:RHC42STGB42NCWMF3CH7XE5AD3","short_pith_number":"pith:RHC42STG","schema_version":"1.0","canonical_sha256":"89c5cd4a660f34d15985d88ffb93a01edaeb25733b3ba1cd827a2957ebf49830","source":{"kind":"arxiv","id":"physics/0308063","version":2},"attestation_state":"computed","paper":{"title":"Sensitivity of searches for new signals and its optimization","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"physics.data-an","authors_text":"Giovanni Punzi","submitted_at":"2003-08-15T16:05:00Z","abstract_excerpt":"A frequentist definition of sensitivity of a search for new phenomena is discussed, that has several useful properties. It is based on completely standard concepts, is generally applicable, and has a very clear interpretation. It is particularly suitable for optimization, being independent of a-priori expectations about the presence of a signal, thus allowing the determination of a single set of cuts that is optimal both for setting limits and for making a discovery. Simple approximate formulas are given for the common problem of Poisson counts with background."},"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":"physics/0308063","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"physics.data-an","submitted_at":"2003-08-15T16:05:00Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"cf72d09fda2b23144e4ccf040904cc773e957e52ce02c7293b1f345069a48720","abstract_canon_sha256":"af65042158e05c2d8d59f7cf0fd369cd4a889fb6e032d4f0b8e2dc8bc86d9142"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:44:00.757608Z","signature_b64":"2Nd58cMbYlhg3KesYbQDhVZ63W/CiXUaTQXmRPAu2uuOswXHIdV3wynYWgzM7udyY41yxiECrOSf4dKzexbPDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89c5cd4a660f34d15985d88ffb93a01edaeb25733b3ba1cd827a2957ebf49830","last_reissued_at":"2026-07-04T14:44:00.757220Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:44:00.757220Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Sensitivity of searches for new signals and its optimization","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"physics.data-an","authors_text":"Giovanni Punzi","submitted_at":"2003-08-15T16:05:00Z","abstract_excerpt":"A frequentist definition of sensitivity of a search for new phenomena is discussed, that has several useful properties. It is based on completely standard concepts, is generally applicable, and has a very clear interpretation. It is particularly suitable for optimization, being independent of a-priori expectations about the presence of a signal, thus allowing the determination of a single set of cuts that is optimal both for setting limits and for making a discovery. Simple approximate formulas are given for the common problem of Poisson counts with background."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0308063","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/physics/0308063/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"physics/0308063","created_at":"2026-07-04T14:44:00.757274+00:00"},{"alias_kind":"arxiv_version","alias_value":"physics/0308063v2","created_at":"2026-07-04T14:44:00.757274+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0308063","created_at":"2026-07-04T14:44:00.757274+00:00"},{"alias_kind":"pith_short_12","alias_value":"RHC42STGB42N","created_at":"2026-07-04T14:44:00.757274+00:00"},{"alias_kind":"pith_short_16","alias_value":"RHC42STGB42NCWMF","created_at":"2026-07-04T14:44:00.757274+00:00"},{"alias_kind":"pith_short_8","alias_value":"RHC42STG","created_at":"2026-07-04T14:44:00.757274+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":15,"internal_anchor_count":10,"sample":[{"citing_arxiv_id":"2607.07800","citing_title":"Search for axion-like particles decaying to two photons at Belle II","ref_index":31,"is_internal_anchor":true},{"citing_arxiv_id":"2606.24578","citing_title":"First evidence of $X(3872)\\to\\pi^0\\chi_{c0}(1P)$ and search for $X(3915)\\to\\pi^0\\chi_{c1}(1P)$","ref_index":44,"is_internal_anchor":true},{"citing_arxiv_id":"2605.21452","citing_title":"Sensitivity of the FCC-ee to axion-like particles at different center-of-mass energies","ref_index":26,"is_internal_anchor":true},{"citing_arxiv_id":"2605.21452","citing_title":"Sensitivity of the FCC-ee to axion-like particles at different center-of-mass energies","ref_index":26,"is_internal_anchor":true},{"citing_arxiv_id":"2510.13716","citing_title":"Searches for $B^0\\to K^+\\pi^-\\tau^+\\tau^-$ and $B_s^0\\to K^+K^-\\tau^+\\tau^-$ decays","ref_index":57,"is_internal_anchor":true},{"citing_arxiv_id":"2512.09288","citing_title":"Precision measurement of CP violation and branching fractions in $B^{\\pm} \\to K^0_{\\mathrm{S}} h^{\\pm}$ $(h = \\pi, K)$ decays and search for the rare decay $B_c^{\\pm} \\to K^0_{\\mathrm{S}} K^{\\pm}$","ref_index":46,"is_internal_anchor":true},{"citing_arxiv_id":"2601.03083","citing_title":"First evidence of the $B_s^0\\rightarrow K^-\\pi^+\\gamma$ decay","ref_index":51,"is_internal_anchor":true},{"citing_arxiv_id":"2601.10597","citing_title":"Search for sub-GeV dark particles in $\\eta\\to\\pi^0+\\rm{invisible}$ decay","ref_index":43,"is_internal_anchor":true},{"citing_arxiv_id":"2605.13649","citing_title":"Search for single vector-like quark production in opposite-sign dilepton final states in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","ref_index":45,"is_internal_anchor":true},{"citing_arxiv_id":"2604.02933","citing_title":"Search for the decays $B_{(s)}^0\\to J/\\psi\\gamma$ at LHCb","ref_index":30,"is_internal_anchor":true},{"citing_arxiv_id":"2605.04348","citing_title":"Observation of the charmless purely baryonic decay $\\mathinner{\\mathit{\\Lambda}^0_b\\!\\to \\mathit{\\Lambda} p \\overline{p}}$","ref_index":35,"is_internal_anchor":false},{"citing_arxiv_id":"2604.08396","citing_title":"Search for the lepton-flavour violating decays $B^+ \\to \\pi^+ \\mu^\\pm e^\\mp$","ref_index":36,"is_internal_anchor":false},{"citing_arxiv_id":"2605.07586","citing_title":"Evidence for the decay $B^0_s\\to\\phi\\eta'$","ref_index":30,"is_internal_anchor":false},{"citing_arxiv_id":"2604.10732","citing_title":"A search for microscopic black holes, string balls, and sphalerons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","ref_index":76,"is_internal_anchor":false},{"citing_arxiv_id":"2604.14359","citing_title":"Expected Sensitivity of the Light Dark Matter eXperiment to Long-Lived Dark Photons and Axion-Like Particles","ref_index":12,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RHC42STGB42NCWMF3CH7XE5AD3","json":"https://pith.science/pith/RHC42STGB42NCWMF3CH7XE5AD3.json","graph_json":"https://pith.science/api/pith-number/RHC42STGB42NCWMF3CH7XE5AD3/graph.json","events_json":"https://pith.science/api/pith-number/RHC42STGB42NCWMF3CH7XE5AD3/events.json","paper":"https://pith.science/paper/RHC42STG"},"agent_actions":{"view_html":"https://pith.science/pith/RHC42STGB42NCWMF3CH7XE5AD3","download_json":"https://pith.science/pith/RHC42STGB42NCWMF3CH7XE5AD3.json","view_paper":"https://pith.science/paper/RHC42STG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=physics/0308063&json=true","fetch_graph":"https://pith.science/api/pith-number/RHC42STGB42NCWMF3CH7XE5AD3/graph.json","fetch_events":"https://pith.science/api/pith-number/RHC42STGB42NCWMF3CH7XE5AD3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RHC42STGB42NCWMF3CH7XE5AD3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RHC42STGB42NCWMF3CH7XE5AD3/action/storage_attestation","attest_author":"https://pith.science/pith/RHC42STGB42NCWMF3CH7XE5AD3/action/author_attestation","sign_citation":"https://pith.science/pith/RHC42STGB42NCWMF3CH7XE5AD3/action/citation_signature","submit_replication":"https://pith.science/pith/RHC42STGB42NCWMF3CH7XE5AD3/action/replication_record"}},"created_at":"2026-07-04T14:44:00.757274+00:00","updated_at":"2026-07-04T14:44:00.757274+00:00"}