{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:I5A5BFF7ITVCNEOB5PINX7YLB7","short_pith_number":"pith:I5A5BFF7","schema_version":"1.0","canonical_sha256":"4741d094bf44ea2691c1ebd0dbff0b0ff72fc2fb8d04bb244f0bf5a4e0e52f63","source":{"kind":"arxiv","id":"1711.01162","version":1},"attestation_state":"computed","paper":{"title":"Resolved Power Corrections to the Inclusive Decay $\\bar B \\to X_s \\ell^+\\ell^-$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Michael Benzke, Michael Fickinger, Sascha Turczyk, Tobias Hurth","submitted_at":"2017-11-03T13:59:48Z","abstract_excerpt":"We identify the correct power counting of all the variables in the low-$q^2$ window of the inclusive decay $\\bar B \\to X_s \\ell^+\\ell^-$ within the effective theory SCET if a hadronic mass cut is imposed. Furthermore we analyse the resolved power corrections at the order $1/m_b$ in a systematic way. As a special feature, the resolved contributions stay nonlocal when the hadronic mass cut is released. Therefore they represent an irreducible uncertainty independent of the hadronic mass cut."},"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":"1711.01162","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-03T13:59:48Z","cross_cats_sorted":[],"title_canon_sha256":"2ae712e651e81bc4f0141a76f3f010fa87566eea6d7e9ae82ae5ad9c31d2e701","abstract_canon_sha256":"2269e720b9ecb0ec3341cb01fdfa594c3220da02b0da3b34cb27bf310f665a8b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:31:23.272071Z","signature_b64":"FRFQ8sqePPsC11zgpixzgFlPEnuRm3B4+O51rCl2b7Po/6Qs0gZEKuI+FcCuo9y737pmxoaXwApSTm8pgtWaCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4741d094bf44ea2691c1ebd0dbff0b0ff72fc2fb8d04bb244f0bf5a4e0e52f63","last_reissued_at":"2026-05-18T00:31:23.271635Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:31:23.271635Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Resolved Power Corrections to the Inclusive Decay $\\bar B \\to X_s \\ell^+\\ell^-$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Michael Benzke, Michael Fickinger, Sascha Turczyk, Tobias Hurth","submitted_at":"2017-11-03T13:59:48Z","abstract_excerpt":"We identify the correct power counting of all the variables in the low-$q^2$ window of the inclusive decay $\\bar B \\to X_s \\ell^+\\ell^-$ within the effective theory SCET if a hadronic mass cut is imposed. Furthermore we analyse the resolved power corrections at the order $1/m_b$ in a systematic way. As a special feature, the resolved contributions stay nonlocal when the hadronic mass cut is released. Therefore they represent an irreducible uncertainty independent of the hadronic mass cut."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.01162","kind":"arxiv","version":1},"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":"1711.01162","created_at":"2026-05-18T00:31:23.271700+00:00"},{"alias_kind":"arxiv_version","alias_value":"1711.01162v1","created_at":"2026-05-18T00:31:23.271700+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.01162","created_at":"2026-05-18T00:31:23.271700+00:00"},{"alias_kind":"pith_short_12","alias_value":"I5A5BFF7ITVC","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_16","alias_value":"I5A5BFF7ITVCNEOB","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_8","alias_value":"I5A5BFF7","created_at":"2026-05-18T12:31:21.493067+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.08902","citing_title":"Update of the nonlocal sub-leading ${O}_1$-${O}_7$ contribution to $\\bar B \\to X_s \\gamma$ at LO","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2605.06567","citing_title":"Probing unknown nonperturbative effects in $b \\to s \\ell\\ell$ with inclusive and exclusive observables","ref_index":34,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/I5A5BFF7ITVCNEOB5PINX7YLB7","json":"https://pith.science/pith/I5A5BFF7ITVCNEOB5PINX7YLB7.json","graph_json":"https://pith.science/api/pith-number/I5A5BFF7ITVCNEOB5PINX7YLB7/graph.json","events_json":"https://pith.science/api/pith-number/I5A5BFF7ITVCNEOB5PINX7YLB7/events.json","paper":"https://pith.science/paper/I5A5BFF7"},"agent_actions":{"view_html":"https://pith.science/pith/I5A5BFF7ITVCNEOB5PINX7YLB7","download_json":"https://pith.science/pith/I5A5BFF7ITVCNEOB5PINX7YLB7.json","view_paper":"https://pith.science/paper/I5A5BFF7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1711.01162&json=true","fetch_graph":"https://pith.science/api/pith-number/I5A5BFF7ITVCNEOB5PINX7YLB7/graph.json","fetch_events":"https://pith.science/api/pith-number/I5A5BFF7ITVCNEOB5PINX7YLB7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/I5A5BFF7ITVCNEOB5PINX7YLB7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/I5A5BFF7ITVCNEOB5PINX7YLB7/action/storage_attestation","attest_author":"https://pith.science/pith/I5A5BFF7ITVCNEOB5PINX7YLB7/action/author_attestation","sign_citation":"https://pith.science/pith/I5A5BFF7ITVCNEOB5PINX7YLB7/action/citation_signature","submit_replication":"https://pith.science/pith/I5A5BFF7ITVCNEOB5PINX7YLB7/action/replication_record"}},"created_at":"2026-05-18T00:31:23.271700+00:00","updated_at":"2026-05-18T00:31:23.271700+00:00"}