{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:QNNQOU66YL7LHAZFPIQEZIIOBL","short_pith_number":"pith:QNNQOU66","schema_version":"1.0","canonical_sha256":"835b0753dec2feb383257a204ca10e0aeb95c347af2205dd1c3b78f26743b695","source":{"kind":"arxiv","id":"1707.02176","version":1},"attestation_state":"computed","paper":{"title":"Three particle quantization condition in a finite volume: 2. general formalism and the analysis of data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"A. Rusetsky, H.-W. Hammer, J.-Y. Pang","submitted_at":"2017-07-07T13:55:58Z","abstract_excerpt":"We derive the three-body quantization condition in a finite volume using an effective field theory in the particle-dimer picture. Moreover, we consider the extraction of physical observables from the lattice spectrum using the quantization condition. To illustrate the general framework, we calculate the volume-dependent three-particle spectrum in a simple model both below and above the three-particle threshold. The relation to existing approaches is discussed in detail."},"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":"1707.02176","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-07-07T13:55:58Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"e3f958d961a186ac93a24a3e09b546acaa4b66b2b7a1a1c0ac795523d914fac8","abstract_canon_sha256":"8a8869734536a547e0a515ec7ceadbf7f64c3399fe8cb156bf45b42397dfb20a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:30:01.562610Z","signature_b64":"HPHVJVitIiRFaf+DWE0V69v23S7TA7qRgwJA0ZzlONxcETcAGKv609g+3H3peylMXD1HXF7VUo64i1i6/R0uCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"835b0753dec2feb383257a204ca10e0aeb95c347af2205dd1c3b78f26743b695","last_reissued_at":"2026-05-18T00:30:01.561980Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:30:01.561980Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Three particle quantization condition in a finite volume: 2. general formalism and the analysis of data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"A. Rusetsky, H.-W. Hammer, J.-Y. Pang","submitted_at":"2017-07-07T13:55:58Z","abstract_excerpt":"We derive the three-body quantization condition in a finite volume using an effective field theory in the particle-dimer picture. Moreover, we consider the extraction of physical observables from the lattice spectrum using the quantization condition. To illustrate the general framework, we calculate the volume-dependent three-particle spectrum in a simple model both below and above the three-particle threshold. The relation to existing approaches is discussed in detail."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.02176","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":"1707.02176","created_at":"2026-05-18T00:30:01.562067+00:00"},{"alias_kind":"arxiv_version","alias_value":"1707.02176v1","created_at":"2026-05-18T00:30:01.562067+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.02176","created_at":"2026-05-18T00:30:01.562067+00:00"},{"alias_kind":"pith_short_12","alias_value":"QNNQOU66YL7L","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_16","alias_value":"QNNQOU66YL7LHAZF","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_8","alias_value":"QNNQOU66","created_at":"2026-05-18T12:31:39.905425+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2502.04232","citing_title":"$D_1$ and $D_2$ resonances in coupled-channel scattering amplitudes from lattice QCD","ref_index":77,"is_internal_anchor":true},{"citing_arxiv_id":"2604.19553","citing_title":"Exotic $T^*_{csJ}$ and $T^*_{c\\bar{s}J}$ states and coupled-channel scattering at the $SU(3)$ flavour symmetric point from lattice QCD","ref_index":53,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QNNQOU66YL7LHAZFPIQEZIIOBL","json":"https://pith.science/pith/QNNQOU66YL7LHAZFPIQEZIIOBL.json","graph_json":"https://pith.science/api/pith-number/QNNQOU66YL7LHAZFPIQEZIIOBL/graph.json","events_json":"https://pith.science/api/pith-number/QNNQOU66YL7LHAZFPIQEZIIOBL/events.json","paper":"https://pith.science/paper/QNNQOU66"},"agent_actions":{"view_html":"https://pith.science/pith/QNNQOU66YL7LHAZFPIQEZIIOBL","download_json":"https://pith.science/pith/QNNQOU66YL7LHAZFPIQEZIIOBL.json","view_paper":"https://pith.science/paper/QNNQOU66","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1707.02176&json=true","fetch_graph":"https://pith.science/api/pith-number/QNNQOU66YL7LHAZFPIQEZIIOBL/graph.json","fetch_events":"https://pith.science/api/pith-number/QNNQOU66YL7LHAZFPIQEZIIOBL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QNNQOU66YL7LHAZFPIQEZIIOBL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QNNQOU66YL7LHAZFPIQEZIIOBL/action/storage_attestation","attest_author":"https://pith.science/pith/QNNQOU66YL7LHAZFPIQEZIIOBL/action/author_attestation","sign_citation":"https://pith.science/pith/QNNQOU66YL7LHAZFPIQEZIIOBL/action/citation_signature","submit_replication":"https://pith.science/pith/QNNQOU66YL7LHAZFPIQEZIIOBL/action/replication_record"}},"created_at":"2026-05-18T00:30:01.562067+00:00","updated_at":"2026-05-18T00:30:01.562067+00:00"}