{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:YCQMG6VFCWPKEDVOHFWWIZDRHK","short_pith_number":"pith:YCQMG6VF","schema_version":"1.0","canonical_sha256":"c0a0c37aa5159ea20eae396d6464713ab441d2158bdd7e285fc28e1ef36bb24f","source":{"kind":"arxiv","id":"1811.05585","version":1},"attestation_state":"computed","paper":{"title":"Towards a precise determination of the scattering amplitudes of the charmed and light-flavor pseudoscalar mesons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"A. Rusetsky, J. A. Oller, Liuming Liu, Ulf-G. Meissner, Zhi-Hui Guo","submitted_at":"2018-11-14T01:16:32Z","abstract_excerpt":"We study the scattering of the light-flavor pseudoscalar mesons ($\\pi, K, \\eta$) off the ground-state charmed mesons ($D,D_s$) within chiral effective field theory. The recent lattice simulation results on various scattering lengths and the finite-volume spectra both in the moving and center-of-mass frames, most of which are obtained at unphysical meson masses, are used to constrain the free parameters in our theory. Explicit formulas to include the $S$- and $P$-wave mixing to determine the finite-volume energy levels are provided. After a successful reproduction of the lattice data, we perfor"},"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":"1811.05585","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-11-14T01:16:32Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"a89ebf852d8b60efac2aa0e7f3b0a776bd394432c6e4cdd0bc4dfd7bc794a218","abstract_canon_sha256":"3a990c219503e04e9eba27bfd5e51fb0cf9f6843ef68379de1c89908d7b46fe2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:56:22.954525Z","signature_b64":"RmwxPNdnFw6k/uU+V1E8yWMzSzW3VEJO+OYMwKnRXdFDPlhLh4tKCqXqwehh41o9lBml+ZklM1EaCKw6qNHaAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c0a0c37aa5159ea20eae396d6464713ab441d2158bdd7e285fc28e1ef36bb24f","last_reissued_at":"2026-05-17T23:56:22.953845Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:56:22.953845Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Towards a precise determination of the scattering amplitudes of the charmed and light-flavor pseudoscalar mesons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"A. Rusetsky, J. A. Oller, Liuming Liu, Ulf-G. Meissner, Zhi-Hui Guo","submitted_at":"2018-11-14T01:16:32Z","abstract_excerpt":"We study the scattering of the light-flavor pseudoscalar mesons ($\\pi, K, \\eta$) off the ground-state charmed mesons ($D,D_s$) within chiral effective field theory. The recent lattice simulation results on various scattering lengths and the finite-volume spectra both in the moving and center-of-mass frames, most of which are obtained at unphysical meson masses, are used to constrain the free parameters in our theory. Explicit formulas to include the $S$- and $P$-wave mixing to determine the finite-volume energy levels are provided. After a successful reproduction of the lattice data, we perfor"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.05585","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":"1811.05585","created_at":"2026-05-17T23:56:22.953957+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.05585v1","created_at":"2026-05-17T23:56:22.953957+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.05585","created_at":"2026-05-17T23:56:22.953957+00:00"},{"alias_kind":"pith_short_12","alias_value":"YCQMG6VFCWPK","created_at":"2026-05-18T12:33:04.347982+00:00"},{"alias_kind":"pith_short_16","alias_value":"YCQMG6VFCWPKEDVO","created_at":"2026-05-18T12:33:04.347982+00:00"},{"alias_kind":"pith_short_8","alias_value":"YCQMG6VF","created_at":"2026-05-18T12:33:04.347982+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2607.02452","citing_title":"The $D_{s1}(2460)$ and other open-charm $1^+$ states in relativistic chiral effective field theory","ref_index":94,"is_internal_anchor":true},{"citing_arxiv_id":"2606.06180","citing_title":"Vector charmonium(-like) states in the energy range of 4.1-4.6 GeV","ref_index":155,"is_internal_anchor":true},{"citing_arxiv_id":"2606.03826","citing_title":"Revealing the $D_0^*(2300)$ two-pole structure from lattice data and the SU(3) limit","ref_index":55,"is_internal_anchor":true},{"citing_arxiv_id":"2604.18286","citing_title":"Analysis of the $D_0^*(2300)$ resonance from lattice QCD under chiral symmetry","ref_index":66,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YCQMG6VFCWPKEDVOHFWWIZDRHK","json":"https://pith.science/pith/YCQMG6VFCWPKEDVOHFWWIZDRHK.json","graph_json":"https://pith.science/api/pith-number/YCQMG6VFCWPKEDVOHFWWIZDRHK/graph.json","events_json":"https://pith.science/api/pith-number/YCQMG6VFCWPKEDVOHFWWIZDRHK/events.json","paper":"https://pith.science/paper/YCQMG6VF"},"agent_actions":{"view_html":"https://pith.science/pith/YCQMG6VFCWPKEDVOHFWWIZDRHK","download_json":"https://pith.science/pith/YCQMG6VFCWPKEDVOHFWWIZDRHK.json","view_paper":"https://pith.science/paper/YCQMG6VF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.05585&json=true","fetch_graph":"https://pith.science/api/pith-number/YCQMG6VFCWPKEDVOHFWWIZDRHK/graph.json","fetch_events":"https://pith.science/api/pith-number/YCQMG6VFCWPKEDVOHFWWIZDRHK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YCQMG6VFCWPKEDVOHFWWIZDRHK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YCQMG6VFCWPKEDVOHFWWIZDRHK/action/storage_attestation","attest_author":"https://pith.science/pith/YCQMG6VFCWPKEDVOHFWWIZDRHK/action/author_attestation","sign_citation":"https://pith.science/pith/YCQMG6VFCWPKEDVOHFWWIZDRHK/action/citation_signature","submit_replication":"https://pith.science/pith/YCQMG6VFCWPKEDVOHFWWIZDRHK/action/replication_record"}},"created_at":"2026-05-17T23:56:22.953957+00:00","updated_at":"2026-05-17T23:56:22.953957+00:00"}