{"as_of":"2026-08-11T11:03:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:fbe5ac3ed96c3bee16dff4f78d7439c37fec8df71aba8c8d80363cfff902e499","coverage":[{"denominator":128,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-03T08:29:47.892947Z","state":"measured"},{"denominator":103,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":103,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-11T06:34:44.6726+00:00","state":"measured"},{"denominator":3,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":3,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-02T22:11:05.199313Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-07-04T17:50:00.886776Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2601.16916","snapshot_observed_at":"2026-08-02T22:11:05.199313Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2602.17924","last_updated":"2026-07-10T19:52:20Z","snapshot_observed_at":"2026-08-06T22:08:46.924975Z","submitted_at":"2026-02-20T01:06:17Z","title":"Higher order quantization conditions for two-body scattering with spin","version":2},"reference_index":56,"source":"arxiv_source","source_observed_at":"2026-08-02T22:11:05.199313Z"},"links":{"cited_paper":"/paper/2601.16916","citing_paper":"/paper/2602.17924"},"observation_digest":"sha256:865b53b2f7ebcc426d219e9e3eac505a97379a7cef63b2949be9bd4890eccf00","observation_id":"ca4671c9-cc2b-40c6-a05f-4a50982f75fc","resolution":{"observed_at":"2026-08-02T22:11:05.199313Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"cited_work":{"arxiv_id":"2601.16916","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2601.16916","snapshot_observed_at":"2026-07-21T02:20:34.196291Z","title":"Coupled-channel approach to isotensorπππscattering from lattice QCD,","venue":null,"work_id":"f10b4dea-0c68-4dda-8840-3d65023a6a73","year":2026},"citing_paper":{"arxiv_id":"2606.19040","last_updated":"2026-06-17T13:08:52Z","snapshot_observed_at":"2026-07-06T23:54:23.090538Z","submitted_at":"2026-06-17T13:08:52Z","title":"Three-body unitary determination of the $f_1(1285)$ and $f_1(1420)$ pole positions","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-06-26T20:22:24.673041Z"},"links":{"cited_paper":"/paper/2601.16916","citing_paper":"/paper/2606.19040"},"observation_digest":"sha256:721fff3aac2837a3dce9cb90bc8ad054c736099b4682a05af3a1c407d4e43213","observation_id":"63512fee-4694-4dc6-aa59-c66787586593","resolution":{"observed_at":"2026-07-21T02:20:34.196291Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"cited_work":{"arxiv_id":"2601.16916","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2601.16916","snapshot_observed_at":"2026-07-21T02:20:34.196291Z","title":"Coupled-channel approach to isotensorπππscattering from lattice QCD,","venue":null,"work_id":"f10b4dea-0c68-4dda-8840-3d65023a6a73","year":2026},"citing_paper":{"arxiv_id":"2606.24709","last_updated":"2026-07-13T12:02:27Z","snapshot_observed_at":"2026-08-05T12:03:05.546432Z","submitted_at":"2026-06-23T15:32:59Z","title":"The $a_1(1420)$ in a Unitary Coupled-Channel Three-Body Approach","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-06-25T23:21:53.393768Z"},"links":{"cited_paper":"/paper/2601.16916","citing_paper":"/paper/2606.24709"},"observation_digest":"sha256:14e93bf9666fc5faebd2da52ecbf64040d4d96975da5fc4045ce1f42d59bfbf6","observation_id":"e192e6e9-ae44-4b82-ba20-0a8ba6c56458","resolution":{"observed_at":"2026-07-21T02:20:34.196291Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2601.16916/citation-record","integrity":"/paper/2601.16916/integrity","json":"/paper/2601.16916/citation-record.json","paper":"/paper/2601.16916"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T08:29:47.420690Z","title":"threshold","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.420690Z"},"links":{"citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:a9bd98aad02832c7595e1e6086c270e98a21b8d6ea1175aa1b2577501a62fdfd","observation_id":"821d4858-2913-493c-8b39-4be6cf588f94","resolution":{"observed_at":"2026-08-03T08:29:47.420690Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T08:29:47.426107Z","title":"washed out","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.426107Z"},"links":{"citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:4ac8724e209bdfe145f99dcb51adcad98a8f974382a547ef07641c24fc768e0d","observation_id":"fcdd8a79-710a-46c7-99cd-d1c54a46cc06","resolution":{"observed_at":"2026-08-03T08:29:47.426107Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2206.01477","last_updated":"2022-06-03T09:59:47Z","snapshot_observed_at":"2026-08-06T14:19:45.286561Z","submitted_at":"2022-06-03T09:59:47Z","title":"Towards a theory of hadron resonances","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.01477","snapshot_observed_at":"2026-08-03T08:29:47.430894Z","title":"Towards a theory of hadron resonances,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.430894Z"},"links":{"cited_paper":"/paper/2206.01477","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:bd5f4c8c00ff0bb00fb50cc0b16f7b3d5ef8b74f5eb4d222b2de64e41438da54","observation_id":"d9c6e2fd-ce1c-4076-9dc5-3e454475268f","resolution":{"observed_at":"2026-08-03T08:29:47.430894Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/9505040","last_updated":"1995-05-29T14:23:41Z","snapshot_observed_at":"2026-07-07T06:38:36.534226Z","submitted_at":"1995-05-29T14:23:41Z","title":"Updated analysis of $\\pi$N elastic scattering data to 2.1~GeV: The Baryon Spectrum","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/9505040","snapshot_observed_at":"2026-08-03T08:29:47.435485Z","title":"Updated analysis of pi N elastic scattering data to 2.1-GeV: The Baryon spectrum,","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.435485Z"},"links":{"cited_paper":"/paper/nucl-th/9505040","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:fd9503f708d347c80fe1e51ed4fd3c020378c4275bba293ac1d21ceff520eca5","observation_id":"7fa03c00-1ca7-4c14-8a46-cb0b890bad1d","resolution":{"observed_at":"2026-08-03T08:29:47.435485Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1011.0609","last_updated":"2010-11-02T13:17:11Z","snapshot_observed_at":"2026-07-06T02:18:35.213545Z","submitted_at":"2010-11-02T13:17:11Z","title":"On the nature of the Roper resonance","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1011.0609","snapshot_observed_at":"2026-08-03T08:29:47.440438Z","title":"On the nature of the Roper resonance,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.440438Z"},"links":{"cited_paper":"/paper/1011.0609","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:4b867d31eb86b85797b00b65e5449921d2674ac1a8209515fefa7030bc417491","observation_id":"f2792071-8b6a-4bab-8483-e43c35396908","resolution":{"observed_at":"2026-08-03T08:29:47.440438Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1211.6998","last_updated":"2013-04-26T14:53:25Z","snapshot_observed_at":"2026-07-06T03:00:55.840748Z","submitted_at":"2012-11-29T17:35:16Z","title":"Coupled-channel dynamics in the reactions piN --> piN, etaN, KLambda, KSigma","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1211.6998","snapshot_observed_at":"2026-08-03T08:29:47.445319Z","title":"Coupled-channel dynamics in the reactions piN –>piN, etaN, KLambda, KSigma,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.445319Z"},"links":{"cited_paper":"/paper/1211.6998","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:9951dbe70b297354f59a822aa0bfe5ae9212b0eb2a2e7656b68e1c6cc5e86beb","observation_id":"6c8cf47b-5e07-4327-b17b-120351bdfffc","resolution":{"observed_at":"2026-08-03T08:29:47.445319Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.01422","last_updated":"2017-01-31T11:36:38Z","snapshot_observed_at":"2026-08-09T11:01:13.279692Z","submitted_at":"2016-10-05T14:00:58Z","title":"Pion-nucleon scattering in the Roper channel from lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.01422","snapshot_observed_at":"2026-08-03T08:29:47.449787Z","title":"Pion-nucleon scattering in the Roper channel from lattice QCD,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.449787Z"},"links":{"cited_paper":"/paper/1610.01422","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:6f79013cd339145c211dc9f936764cac2dff797eef32185591793aff0fba66aa","observation_id":"f6346358-f33b-4855-a3e4-0f00affeae04","resolution":{"observed_at":"2026-08-03T08:29:47.449787Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1608.03051","last_updated":"2016-08-10T05:43:30Z","snapshot_observed_at":"2026-07-06T05:06:34.605569Z","submitted_at":"2016-08-10T05:43:30Z","title":"Search for low-lying lattice QCD eigenstates in the Roper regime","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1608.03051","snapshot_observed_at":"2026-08-03T08:29:47.454569Z","title":"Search for low-lying lattice QCD eigenstates in the Roper regime,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.454569Z"},"links":{"cited_paper":"/paper/1608.03051","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:14e2c16247b4a6db4fd9ae6b22a1c209de130875edb234633ed475fec7c6c33e","observation_id":"e98f4309-ec8f-4504-af4e-2538ea5b10e1","resolution":{"observed_at":"2026-08-03T08:29:47.454569Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.04536","last_updated":"2017-02-15T12:39:14Z","snapshot_observed_at":"2026-07-06T05:03:43.188549Z","submitted_at":"2016-07-15T14:46:14Z","title":"Hamiltonian effective field theory study of the $\\mathbf{N^*(1440)}$ resonance in lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.04536","snapshot_observed_at":"2026-08-03T08:29:47.459527Z","title":"Hamil- tonian effective field theory study of theN ∗(1440) resonance in lattice QCD,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.459527Z"},"links":{"cited_paper":"/paper/1607.04536","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:6cf61f173d0003e6c0c8907800b1b20186aaf9948b6370d315cfbd91c38e7c62","observation_id":"fa53c942-1407-4c27-a1d6-ee3de078dd73","resolution":{"observed_at":"2026-08-03T08:29:47.459527Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.04277","last_updated":"2019-10-07T17:28:31Z","snapshot_observed_at":"2026-07-06T07:52:13.448801Z","submitted_at":"2019-05-10T17:35:07Z","title":"Two- and three-pion finite-volume spectra at maximal isospin from lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.04277","snapshot_observed_at":"2026-08-03T08:29:47.463751Z","title":"Two- and three-pion finite-volume spectra at maximal isospin from lattice QCD,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.463751Z"},"links":{"cited_paper":"/paper/1905.04277","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:a809ebb6a133b2399c51392678bd7d88f9113da212f63f10f6ba106a3e4ebaac","observation_id":"a1d239fb-bf0f-4124-b572-16220910d530","resolution":{"observed_at":"2026-08-03T08:29:47.463751Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1911.09047","last_updated":"2020-09-23T15:10:02Z","snapshot_observed_at":"2026-08-09T21:38:17.876571Z","submitted_at":"2019-11-20T17:20:09Z","title":"Three pion spectrum in the $I=3$ channel from lattice QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1911.09047","snapshot_observed_at":"2026-08-03T08:29:47.468511Z","title":"Three pion spectrum in theI= 3 channel from lattice QCD,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.468511Z"},"links":{"cited_paper":"/paper/1911.09047","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:ede46c48c7f56ba8c780f0df9e6185d4b308af77e98b14805c15535ee6857201","observation_id":"5841f2d9-0991-47ee-9611-b8a943fe0dfe","resolution":{"observed_at":"2026-08-03T08:29:47.468511Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.03035","last_updated":"2021-05-25T08:17:48Z","snapshot_observed_at":"2026-08-10T06:41:14.613915Z","submitted_at":"2020-08-07T08:28:12Z","title":"Scattering of two and three physical pions at maximal isospin from lattice QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.03035","snapshot_observed_at":"2026-08-03T08:29:47.473469Z","title":"Scattering of two and three physical pions at maximal isospin from lattice QCD,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.473469Z"},"links":{"cited_paper":"/paper/2008.03035","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:c852dc037382e15f6df1a4dc2fe6c3afd31e05f5c0b152deb98549fe4253d9b3","observation_id":"db228812-a962-4e96-9a9a-67a9c5e84a2c","resolution":{"observed_at":"2026-08-03T08:29:47.473469Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.04931","last_updated":"2021-03-02T19:05:01Z","snapshot_observed_at":"2026-08-06T03:10:09.961729Z","submitted_at":"2020-09-10T15:18:27Z","title":"The energy-dependent $\\pi^+ \\pi^+ \\pi^+$ scattering amplitude from QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.04931","snapshot_observed_at":"2026-08-03T08:29:47.478604Z","title":"Energy-Dependentπ +π+π+ Scattering Amplitude from QCD,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.478604Z"},"links":{"cited_paper":"/paper/2009.04931","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:3a9c8b0ceb071f0c2d6706ca12b2f373f2a97f13100a4b63ec6c11993317c965","observation_id":"ff28d864-b38f-4730-a573-d7e93643c3f5","resolution":{"observed_at":"2026-08-03T08:29:47.478604Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.12358","last_updated":"2020-10-02T16:28:43Z","snapshot_observed_at":"2026-07-06T09:58:50.763747Z","submitted_at":"2020-09-25T17:47:13Z","title":"Finite-volume energy spectrum of the $K^-K^-K^-$ system","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.12358","snapshot_observed_at":"2026-08-03T08:29:47.483627Z","title":"Finite- volume energy spectrum of theK −K −K − system,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.483627Z"},"links":{"cited_paper":"/paper/2009.12358","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:7663e891bba28b51f5ac8284ddc27ed39fc8d4932338fd4b4b7f5b21d0cb3597","observation_id":"58d80b8f-a10d-4fcc-bdc0-a35f7f554f00","resolution":{"observed_at":"2026-08-03T08:29:47.483627Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.05590","last_updated":"2021-10-13T13:43:03Z","snapshot_observed_at":"2026-07-06T11:17:52.032348Z","submitted_at":"2021-06-10T08:45:59Z","title":"Interactions of two and three mesons including higher partial waves from lattice QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.05590","snapshot_observed_at":"2026-08-03T08:29:47.488694Z","title":"Interactions of two and three mesons including higher partial waves from lattice QCD,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.488694Z"},"links":{"cited_paper":"/paper/2106.05590","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:6ae8cec014db6e9bccd97735895d4e965610a56810b7bee63e82cc2272cb7b1e","observation_id":"d5fcfde9-63f3-4446-9924-f6d9a4b402aa","resolution":{"observed_at":"2026-08-03T08:29:47.488694Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2003.12130","last_updated":"2021-03-26T14:18:18Z","snapshot_observed_at":"2026-08-11T03:01:30.471073Z","submitted_at":"2020-03-26T19:55:15Z","title":"Charged multi-hadron systems in lattice QCD+QED","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2003.12130","snapshot_observed_at":"2026-08-03T08:29:47.493820Z","title":"Charged multihadron systems in lattice QCD+QED,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.493820Z"},"links":{"cited_paper":"/paper/2003.12130","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:62e8137b7c39f7230bd95339da14c1dbcea121b433c7b75ce312df2a901b3867","observation_id":"e8353724-6670-48a7-b331-6e137dae7cdb","resolution":{"observed_at":"2026-08-03T08:29:47.493820Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.15228","last_updated":"2021-12-30T22:34:16Z","snapshot_observed_at":"2026-08-11T02:58:46.949453Z","submitted_at":"2021-12-30T22:34:16Z","title":"Finite-volume effects and meson scattering in the 2-flavour Schwinger model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.15228","snapshot_observed_at":"2026-08-03T08:29:47.498364Z","title":"Finite-volume effects and meson scattering in the 2-flavour Schwinger model,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.498364Z"},"links":{"cited_paper":"/paper/2112.15228","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:10c34069a989b304219093f47b58c7c0df1401a5b8fa12cd7c6181c2823d3455","observation_id":"3010d72c-20aa-491a-8ed1-5f920a417e7b","resolution":{"observed_at":"2026-08-03T08:29:47.498364Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2107.03973","last_updated":"2021-07-08T16:59:13Z","snapshot_observed_at":"2026-08-09T15:06:09.093284Z","submitted_at":"2021-07-08T16:59:13Z","title":"Three-body dynamics of the $a_1(1260)$ resonance from lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2107.03973","snapshot_observed_at":"2026-08-03T08:29:47.503197Z","title":"Three-Body Dynamics of the a1(1260) Resonance from Lattice QCD,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.503197Z"},"links":{"cited_paper":"/paper/2107.03973","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:0e0814b7bd316b1a66d353b3432ab82ddfac977af831ee89a03d2da764b7859c","observation_id":"5a7bb140-ed1b-4979-895e-abd61fbf93d9","resolution":{"observed_at":"2026-08-03T08:29:47.503197Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.05605","last_updated":"2023-03-07T16:32:22Z","snapshot_observed_at":"2026-08-09T12:35:04.302713Z","submitted_at":"2022-11-10T14:27:12Z","title":"Three-body resonances in the $\\varphi^4$ theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.05605","snapshot_observed_at":"2026-08-03T08:29:47.507712Z","title":"Three-body resonances in theφ 4 theory,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.507712Z"},"links":{"cited_paper":"/paper/2211.05605","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:fef4d3ed6d092ed34c73bff4dd814d31899df4d61cd15605d7457cff3e404ce3","observation_id":"0b810b88-39f9-43e0-987a-6f2b57272122","resolution":{"observed_at":"2026-08-03T08:29:47.507712Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2302.13587","last_updated":"2023-04-26T19:26:11Z","snapshot_observed_at":"2026-07-06T14:56:08.467858Z","submitted_at":"2023-02-27T08:45:20Z","title":"Interactions of $\\pi K$, $\\pi \\pi K$ and $KK\\pi$ systems at maximal isospin from lattice QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2302.13587","snapshot_observed_at":"2026-08-03T08:29:47.512227Z","title":"Interactions ofπK,ππK and KKπsystems at maximal isospin from lattice QCD,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.512227Z"},"links":{"cited_paper":"/paper/2302.13587","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:6d1da439bb456ab12848426ad173bf65edd6fbafe37b99e1b5dbd6f83bc37aff","observation_id":"ee566862-af14-46a9-a958-00862b4320e8","resolution":{"observed_at":"2026-08-03T08:29:47.512227Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.16659","last_updated":"2024-11-23T10:12:34Z","snapshot_observed_at":"2026-07-06T18:50:48.181248Z","submitted_at":"2024-07-23T17:21:38Z","title":"$\\omega$ meson from lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.16659","snapshot_observed_at":"2026-08-03T08:29:47.517013Z","title":"ωMeson from Lattice QCD,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.517013Z"},"links":{"cited_paper":"/paper/2407.16659","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:f09d8441e521bf1510602fe8ca74021767d977ce99b27fbb077c90a951f396d0","observation_id":"fafb0f30-e539-4b9e-9315-75087c8b0d8b","resolution":{"observed_at":"2026-08-03T08:29:47.517013Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.17059","last_updated":"2025-02-10T23:55:29Z","snapshot_observed_at":"2026-08-05T12:36:23.502876Z","submitted_at":"2024-09-25T16:17:10Z","title":"Finite- and infinite-volume study of $DD\\pi$ scattering","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.17059","snapshot_observed_at":"2026-08-03T08:29:47.521507Z","title":"Finite- and infinite-volume study of DDπ scattering,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.521507Z"},"links":{"cited_paper":"/paper/2409.17059","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:1ecd85e83f38f0ed69fbdb6c56a793db239d01ce88b5fc2764d272f9b5bfdb30","observation_id":"a77898d0-f08a-4700-9927-509b956e9c66","resolution":{"observed_at":"2026-08-03T08:29:47.521507Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2510.09476","last_updated":"2026-06-25T17:39:31Z","snapshot_observed_at":"2026-08-08T14:31:14.402497Z","submitted_at":"2025-10-10T15:32:14Z","title":"Emergence of the $\\pi(1300)$ Resonance from Lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2510.09476","snapshot_observed_at":"2026-08-03T08:29:47.525870Z","title":"Emergence of theπ(1300) Resonance from Lattice QCD,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.525870Z"},"links":{"cited_paper":"/paper/2510.09476","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:d53a91e1ccc0d808e81f3d7bfc111bdce6940c31fa50b468a9650653322a0113","observation_id":"f0a4971a-a68b-4488-9467-2efcaaced910","resolution":{"observed_at":"2026-08-03T08:29:47.525870Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0710.1827","last_updated":"2007-10-09T17:30:43Z","snapshot_observed_at":"2026-07-06T01:31:37.791889Z","submitted_at":"2007-10-09T17:30:43Z","title":"Multi-Pion Systems in Lattice QCD and the Three-Pion Interaction","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0710.1827","snapshot_observed_at":"2026-08-03T08:29:47.530225Z","title":"Multi-Pion Systems in Lattice QCD and the Three-Pion Interaction,","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.530225Z"},"links":{"cited_paper":"/paper/0710.1827","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:bdb9a3f602348981ace63ed6af36d23bc0d6116bd4d0a87a28819c04a1fb8187","observation_id":"53f31f30-ac6c-451c-aee1-3707824570ba","resolution":{"observed_at":"2026-08-03T08:29:47.530225Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1203.1241","last_updated":"2012-04-24T13:19:45Z","snapshot_observed_at":"2026-08-06T19:15:17.203385Z","submitted_at":"2012-03-06T16:19:15Z","title":"Three particles in a finite volume","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1203.1241","snapshot_observed_at":"2026-08-03T08:29:47.534802Z","title":"Three particles in a finite volume,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.534802Z"},"links":{"cited_paper":"/paper/1203.1241","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:960a1d89b735cf0fbde68470fcd7a3cbb7d5b93858cf65d9323e4cb3a85bd426","observation_id":"c1d19ac1-13ea-4dcd-9b9b-498433411255","resolution":{"observed_at":"2026-08-03T08:29:47.534802Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1212.3398","last_updated":"2012-12-14T06:20:23Z","snapshot_observed_at":"2026-08-08T22:40:36.040734Z","submitted_at":"2012-12-14T06:20:23Z","title":"Three-particle scattering amplitudes from a finite volume formalism","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1212.3398","snapshot_observed_at":"2026-08-03T08:29:47.539308Z","title":"Three-particle scattering amplitudes from a finite volume formalism,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.539308Z"},"links":{"cited_paper":"/paper/1212.3398","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:51488e7f3a87303d82514cf6c63d47d79fd92abb433c48081e5d469f7210717a","observation_id":"3d99f524-eb2a-4440-bd8d-2d885b797f13","resolution":{"observed_at":"2026-08-03T08:29:47.539308Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.4969","last_updated":"2016-07-29T06:56:06Z","snapshot_observed_at":"2026-08-09T01:15:34.521846Z","submitted_at":"2014-12-16T12:09:20Z","title":"Spectrum of three-body bound states in a finite volume","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.4969","snapshot_observed_at":"2026-08-03T08:29:47.544343Z","title":"Spectrum of three-body bound states in a finite volume,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.544343Z"},"links":{"cited_paper":"/paper/1412.4969","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:92351df905ed2ea86a0d84de3c8da29f743c212efeb4eb0c038a35915ec8d4c8","observation_id":"5436088e-4f1e-4db8-bc8d-f7d0cc64d414","resolution":{"observed_at":"2026-08-03T08:29:47.544343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1408.5933","last_updated":"2014-11-19T04:41:14Z","snapshot_observed_at":"2026-08-10T09:11:35.166216Z","submitted_at":"2014-08-25T21:37:51Z","title":"A relativistic, model-independent, three-particle quantization condition","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.5933","snapshot_observed_at":"2026-08-03T08:29:47.548683Z","title":"Relativistic, model-independent, three-particle quantization condition,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.548683Z"},"links":{"cited_paper":"/paper/1408.5933","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:abc6c4a92ef981241cd78a22070bad064f44396a5786848364cafe3379f02bd8","observation_id":"a38deee6-144b-4ff5-ab90-a09336bde3c4","resolution":{"observed_at":"2026-08-03T08:29:47.548683Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1505.04099","last_updated":"2015-05-15T15:40:14Z","snapshot_observed_at":"2026-08-10T21:25:22.105508Z","submitted_at":"2015-05-15T15:40:14Z","title":"Finite volume corrections to the binding energy of the X(3872)","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1505.04099","snapshot_observed_at":"2026-08-03T08:29:47.553740Z","title":"Finite volume corrections to the binding energy of the X(3872),","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.553740Z"},"links":{"cited_paper":"/paper/1505.04099","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:3054ce4eb462d89a7bfe83965e7579118c7fae14c24b4a429bf4ed9edc39af06","observation_id":"82acc4e5-b2a4-4b78-a716-7aca29dfa2ee","resolution":{"observed_at":"2026-08-03T08:29:47.553740Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1504.04248","last_updated":"2016-01-04T23:41:27Z","snapshot_observed_at":"2026-07-06T04:15:10.918226Z","submitted_at":"2015-04-16T14:26:09Z","title":"Expressing the three-particle finite-volume spectrum in terms of the three-to-three scattering amplitude","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1504.04248","snapshot_observed_at":"2026-08-03T08:29:47.558166Z","title":"Expressing the three-particle finite-volume spectrum in terms of the three- to-three scattering amplitude,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.558166Z"},"links":{"cited_paper":"/paper/1504.04248","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:a058e282aeb5b13331896959fcbf955d503264ff735f912810ae753548b514e8","observation_id":"87b336fe-166b-45b1-a5e1-7cb2c875b867","resolution":{"observed_at":"2026-08-03T08:29:47.558166Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.07929","last_updated":"2015-09-26T00:50:11Z","snapshot_observed_at":"2026-07-06T04:31:09.282522Z","submitted_at":"2015-09-26T00:50:11Z","title":"Perturbative results for two and three particle threshold energies in finite volume","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.07929","snapshot_observed_at":"2026-08-03T08:29:47.562856Z","title":"Perturbative results for two and three particle threshold energies in finite volume,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.562856Z"},"links":{"cited_paper":"/paper/1509.07929","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:8379d40e613dc582ee13a0d3740d4e0340fb9312f7d9aaa82fad11e0f5fd9364","observation_id":"9da7d8fe-aa36-44f1-b0b5-7b15e16a4e04","resolution":{"observed_at":"2026-08-03T08:29:47.562856Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1602.00324","last_updated":"2017-08-02T10:23:43Z","snapshot_observed_at":"2026-07-06T04:44:39.683909Z","submitted_at":"2016-01-31T21:29:55Z","title":"Threshold expansion of the three-particle quantization condition","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1602.00324","snapshot_observed_at":"2026-08-03T08:29:47.567558Z","title":"Threshold expansion of the three-particle quantization condition,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.567558Z"},"links":{"cited_paper":"/paper/1602.00324","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:0be39fe4a823947409e5ee59721bf1bb495185bca0ef00692884ace3132d6a51","observation_id":"928f2987-a2fd-47e5-8b67-ccb14ea1ffb1","resolution":{"observed_at":"2026-08-03T08:29:47.567558Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.03184","last_updated":"2016-07-11T22:21:22Z","snapshot_observed_at":"2026-07-06T05:03:11.934242Z","submitted_at":"2016-07-11T22:21:22Z","title":"One spatial dimensional finite volume three-body interaction for a short-range potential","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.03184","snapshot_observed_at":"2026-08-03T08:29:47.571796Z","title":"One spatial dimensional finite volume three-body interaction for a short-range potential,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.571796Z"},"links":{"cited_paper":"/paper/1607.03184","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:7bbe85921844b5b76f784a23168e29a7fb0979159c45241f0ab2d039814534ba","observation_id":"acd30eab-e4e7-46d3-9e32-81b4ff1f7af5","resolution":{"observed_at":"2026-08-03T08:29:47.571796Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.08222","last_updated":"2017-11-19T15:25:34Z","snapshot_observed_at":"2026-07-06T06:01:05.478634Z","submitted_at":"2017-09-24T16:50:09Z","title":"Three-body Unitarity in the Finite Volume","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.08222","snapshot_observed_at":"2026-08-03T08:29:47.576372Z","title":"Three-body Unitarity in the Finite Volume,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.576372Z"},"links":{"cited_paper":"/paper/1709.08222","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:51c9ce463a953dea0f8df2a2a04989c00083313f31c9274e337bc167abc1cebe","observation_id":"27bcd3b7-d5ed-41fd-8f1c-d4542b008d69","resolution":{"observed_at":"2026-08-03T08:29:47.576372Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.00279","last_updated":"2018-02-01T14:49:12Z","snapshot_observed_at":"2026-08-09T18:42:36.982922Z","submitted_at":"2017-01-01T19:29:59Z","title":"Volume Dependence of N-Body Bound States","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.00279","snapshot_observed_at":"2026-08-03T08:29:47.580839Z","title":"Volume Dependence of N-Body Bound States,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.580839Z"},"links":{"cited_paper":"/paper/1701.00279","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:c7f167dfadfb837ff7b792d3f963afdb4b32242700e69ef2997809837f375f7b","observation_id":"9793faa2-fae7-4d06-a45c-074f363518f1","resolution":{"observed_at":"2026-08-03T08:29:47.580839Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1706.07700","last_updated":"2017-06-23T13:46:47Z","snapshot_observed_at":"2026-07-06T05:48:09.951143Z","submitted_at":"2017-06-23T13:46:47Z","title":"Three-particle quantization condition in a finite volume: 1. The role of the three-particle force","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.07700","snapshot_observed_at":"2026-08-03T08:29:47.585427Z","title":"Three-particle quantization condition in a finite volume: 1. The role of the three-particle force,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.585427Z"},"links":{"cited_paper":"/paper/1706.07700","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:d379475003159a5aca48fa4073f1507b0d92d8452dedc562f4d14d755b49092f","observation_id":"e7d73560-e51b-468a-a38d-c817e04c2da1","resolution":{"observed_at":"2026-08-03T08:29:47.585427Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.02176","last_updated":"2017-07-07T13:55:58Z","snapshot_observed_at":"2026-07-06T05:50:10.849445Z","submitted_at":"2017-07-07T13:55:58Z","title":"Three particle quantization condition in a finite volume: 2. general formalism and the analysis of data","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.02176","snapshot_observed_at":"2026-08-03T08:29:47.590019Z","title":"Three particle quantization condition in a finite volume: 2. general formalism and the analysis of data,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.590019Z"},"links":{"cited_paper":"/paper/1707.02176","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:82706e35851e9b6059c0200122e15ab1a02b3dd7278505de368cc1c017a96e1e","observation_id":"6e1ec93a-7874-425e-8b92-cb8ec928611d","resolution":{"observed_at":"2026-08-03T08:29:47.590019Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.07465","last_updated":"2017-04-30T18:27:38Z","snapshot_observed_at":"2026-07-06T05:27:34.280561Z","submitted_at":"2017-01-25T19:59:16Z","title":"Relating the finite-volume spectrum and the two-and-three-particle $S$ matrix for relativistic systems of identical scalar particles","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.07465","snapshot_observed_at":"2026-08-03T08:29:47.595614Z","title":"Relating the finite-volume spectrum and the two- and-three-particleSmatrix for relativistic systems of identical scalar particles,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.595614Z"},"links":{"cited_paper":"/paper/1701.07465","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:205e0a9e8ca579723d564f78382d67156519d3c6c83315f6212e506c546c8148","observation_id":"1553aa3b-f9ae-4929-90b9-38482894a332","resolution":{"observed_at":"2026-08-03T08:29:47.595614Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.04279","last_updated":"2018-10-20T08:01:11Z","snapshot_observed_at":"2026-08-05T11:47:34.345593Z","submitted_at":"2017-07-13T18:40:29Z","title":"Testing the threshold expansion for three-particle energies at fourth order in $\\phi^4$ theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.04279","snapshot_observed_at":"2026-08-03T08:29:47.600692Z","title":"Testing the threshold expansion for three-particle energies at fourth order inϕ 4 theory,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.600692Z"},"links":{"cited_paper":"/paper/1707.04279","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:0ca46080a1a4881212e7809993d2019a72a3f83e54e34304ceb6c7c9dd1cf4c7","observation_id":"2d7483e4-a937-4b50-938d-7d608a26fcea","resolution":{"observed_at":"2026-08-03T08:29:47.600692Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.08255","last_updated":"2017-09-24T21:05:14Z","snapshot_observed_at":"2026-08-11T10:08:44.050509Z","submitted_at":"2017-09-24T21:05:14Z","title":"An numerical approach for finite volume three-body interaction","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.08255","snapshot_observed_at":"2026-08-03T08:29:47.606085Z","title":"Numerical approach for finite volume three-body interaction,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.606085Z"},"links":{"cited_paper":"/paper/1709.08255","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:5c18eaec79abf2a0c45c9a073b356ef44cfc535474246f772f5a694029ac5c34","observation_id":"f214a051-755b-4894-a2f6-ecbaab223e55","resolution":{"observed_at":"2026-08-03T08:29:47.606085Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.00438","last_updated":"2017-10-06T00:58:34Z","snapshot_observed_at":"2026-08-05T14:41:13.041316Z","submitted_at":"2017-01-02T16:28:48Z","title":"An solvable three-body model in finite volume","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.00438","snapshot_observed_at":"2026-08-03T08:29:47.610720Z","title":"A solvable three-body model in finite volume,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.610720Z"},"links":{"cited_paper":"/paper/1701.00438","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:540238feea498a330133b115c9a2c070ab3c38b4b653cbae500b03925e8d9cc2","observation_id":"6694be96-93f7-46c1-8b72-db4464599632","resolution":{"observed_at":"2026-08-03T08:29:47.610720Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.08464","last_updated":"2018-06-29T12:14:21Z","snapshot_observed_at":"2026-07-06T06:15:46.123021Z","submitted_at":"2017-12-22T14:32:38Z","title":"Three-particle bound states in a finite volume: unequal masses and higher partial waves","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.08464","snapshot_observed_at":"2026-08-03T08:29:47.615949Z","title":"Three-particle bound states in a finite volume: unequal masses and higher partial waves,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.615949Z"},"links":{"cited_paper":"/paper/1712.08464","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:e93966868660615b43223fa8c43a3f581bbe28b4a72966a427e2ff31a531dedf","observation_id":"71b131c1-7cd8-4a3f-b668-87052efa738c","resolution":{"observed_at":"2026-08-03T08:29:47.615949Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.01261","last_updated":"2018-10-27T23:58:00Z","snapshot_observed_at":"2026-08-09T16:02:11.521029Z","submitted_at":"2018-10-02T14:02:28Z","title":"Variational approach to $N$-body interactions in finite volume","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.01261","snapshot_observed_at":"2026-08-03T08:29:47.620723Z","title":"Variational approach toN-body interactions in finite volume,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.620723Z"},"links":{"cited_paper":"/paper/1810.01261","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:493a2d36c420a4e9a0e01f3f3a288b173bb3b2659880e341f3536fc75fbbd7e1","observation_id":"80741a73-3ce0-4cef-aa9e-050c6391f466","resolution":{"observed_at":"2026-08-03T08:29:47.620723Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.07397","last_updated":"2018-08-22T14:56:35Z","snapshot_observed_at":"2026-08-08T08:49:38.150225Z","submitted_at":"2018-08-22T14:56:35Z","title":"Multiple-particle interaction in $1+1$ dimensional lattice model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.07397","snapshot_observed_at":"2026-08-03T08:29:47.625945Z","title":"Multiple-particle interaction in (1+1)-dimensional lattice model,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.625945Z"},"links":{"cited_paper":"/paper/1808.07397","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:6596e56e8cc359dba7c48393219f7c35fb988733f311c0f42d8834c385d78b43","observation_id":"7c30d39c-2621-4301-be6f-60c658a5c458","resolution":{"observed_at":"2026-08-03T08:29:47.625945Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.02029","last_updated":"2018-09-29T15:08:22Z","snapshot_observed_at":"2026-07-06T06:37:33.094941Z","submitted_at":"2018-05-05T09:35:30Z","title":"Signatures of few-body resonances in finite volume","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.02029","snapshot_observed_at":"2026-08-03T08:29:47.630851Z","title":"Signatures of few-body resonances in finite volume,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.630851Z"},"links":{"cited_paper":"/paper/1805.02029","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:d61f81228fc83570b397599c1b04bd1d2f4c4226f4b19868f1f3302024089368","observation_id":"42b272dc-53d5-4db4-b7dc-b62e26c5fc78","resolution":{"observed_at":"2026-08-03T08:29:47.630851Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.04169","last_updated":"2018-07-05T15:35:20Z","snapshot_observed_at":"2026-07-06T06:27:46.580255Z","submitted_at":"2018-03-12T10:13:46Z","title":"Numerical study of the relativistic three-body quantization condition in the isotropic approximation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.04169","snapshot_observed_at":"2026-08-03T08:29:47.635289Z","title":"Numerical study of the relativistic three-body quantization 27 condition in the isotropic approximation,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.635289Z"},"links":{"cited_paper":"/paper/1803.04169","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:dd8d73f69bb1958d36882cc2a8ab4ba05e0e3008f7a65d2d6db24a877870921c","observation_id":"57ba5dd7-5c8b-4e49-925d-0d1d97d2eb9e","resolution":{"observed_at":"2026-08-03T08:29:47.635289Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.01429","last_updated":"2018-10-02T18:00:45Z","snapshot_observed_at":"2026-08-10T07:11:58.476539Z","submitted_at":"2018-10-02T18:00:45Z","title":"Three-particle systems with resonant subprocesses in a finite volume","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.01429","snapshot_observed_at":"2026-08-03T08:29:47.639689Z","title":"Three-particle systems with resonant subprocesses in a finite volume,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.639689Z"},"links":{"cited_paper":"/paper/1810.01429","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:12701e1995556bfc6632ac7a5d9d0e5720ad33d3e7e7edf1b3dfbb022d9931a7","observation_id":"b14cd5e1-6c34-4d1a-9668-07ff481fe510","resolution":{"observed_at":"2026-08-03T08:29:47.639689Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.04746","last_updated":"2019-02-01T16:53:06Z","snapshot_observed_at":"2026-07-06T06:49:53.002704Z","submitted_at":"2018-07-12T17:55:21Z","title":"Finite-volume spectrum of $\\pi^+\\pi^+$ and $\\pi^+\\pi^+\\pi^+$ systems","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.04746","snapshot_observed_at":"2026-08-03T08:29:47.645174Z","title":"Finite-Volume Spectrum ofπ +π+ andπ +π+π+ Systems,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.645174Z"},"links":{"cited_paper":"/paper/1807.04746","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:20bddac70c851fb3b5704e38c266b507684be183d0fda8de7b4ae86dd7e353d3","observation_id":"93a89d15-34e4-4769-bc86-fdd9c258c60f","resolution":{"observed_at":"2026-08-03T08:29:47.645174Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.03362","last_updated":"2019-01-11T15:43:22Z","snapshot_observed_at":"2026-08-06T02:28:31.150991Z","submitted_at":"2018-02-09T17:33:53Z","title":"Three-body spectrum in a finite volume: the role of cubic symmetry","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.03362","snapshot_observed_at":"2026-08-03T08:29:47.649660Z","title":"Three-body spectrum in a finite volume: the role of cubic symmetry,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.649660Z"},"links":{"cited_paper":"/paper/1802.03362","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:0c3a12b984cf7d47ece658c084e9a6657cec31f10f56c6a5e587b9612d448906","observation_id":"a3da40a6-1d4c-4425-96e2-2160508232d7","resolution":{"observed_at":"2026-08-03T08:29:47.649660Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.12007","last_updated":"2019-05-28T18:14:39Z","snapshot_observed_at":"2026-08-09T18:11:13.110995Z","submitted_at":"2019-05-28T18:14:39Z","title":"On the Equivalence of Three-Particle Scattering Formalisms","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.12007","snapshot_observed_at":"2026-08-03T08:29:47.654730Z","title":"Equivalence of three-particle scattering formalisms,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.654730Z"},"links":{"cited_paper":"/paper/1905.12007","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:311227d81036241b4b1517c52b8b92a4415cc43d9772a76c5cfc14f089f71e2e","observation_id":"0c0f041c-81b3-438b-ad7a-f2816fc59b7e","resolution":{"observed_at":"2026-08-03T08:29:47.654730Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1909.05749","last_updated":"2019-09-12T15:25:07Z","snapshot_observed_at":"2026-08-05T19:30:06.224058Z","submitted_at":"2019-09-12T15:25:07Z","title":"Three-body unitarity versus finite-volume $\\pi^+\\pi^+\\pi^+$ spectrum from lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.05749","snapshot_observed_at":"2026-08-03T08:29:47.659299Z","title":"Three-body unitarity versus finite-volumeπ +π+π+ spectrum from lattice QCD,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.659299Z"},"links":{"cited_paper":"/paper/1909.05749","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:e04a85c2de7b1dd03b55a431ddd9a061433909a93e73762c589767a2f440c425","observation_id":"92c9f7df-8efc-4db9-aaa2-3600879884ad","resolution":{"observed_at":"2026-08-03T08:29:47.659299Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1908.08081","last_updated":"2020-02-27T15:29:00Z","snapshot_observed_at":"2026-08-10T23:30:45.936404Z","submitted_at":"2019-08-21T18:46:44Z","title":"Propagation of particles on a torus","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1908.08081","snapshot_observed_at":"2026-08-03T08:29:47.664410Z","title":"Propagation of particles on a torus,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.664410Z"},"links":{"cited_paper":"/paper/1908.08081","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:3b5b9225b64796927974c455ab76a6b9d09d0c2f1f7a6f4f9143d1ef2e9d98ac","observation_id":"00966274-3cd5-452b-86ad-0c5204a69b39","resolution":{"observed_at":"2026-08-03T08:29:47.664410Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1901.07095","last_updated":"2019-03-04T23:50:39Z","snapshot_observed_at":"2026-08-10T02:00:16.859697Z","submitted_at":"2019-01-21T22:00:55Z","title":"Implementing the three-particle quantization condition including higher partial waves","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1901.07095","snapshot_observed_at":"2026-08-03T08:29:47.669255Z","title":"Implementing the three-particle quantization condition including higher partial waves,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.669255Z"},"links":{"cited_paper":"/paper/1901.07095","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:55d47ce6b98677c816f170ab96eb892dcb6bd94de15f935a85986335cccb790a","observation_id":"e8fc1bb7-bb4f-404b-b408-4e8cb2e4d426","resolution":{"observed_at":"2026-08-03T08:29:47.669255Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.11188","last_updated":"2019-05-27T13:20:06Z","snapshot_observed_at":"2026-07-06T07:55:46.920800Z","submitted_at":"2019-05-27T13:20:06Z","title":"Unitarity of the infinite-volume three-particle scattering amplitude arising from a finite-volume formalism","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.11188","snapshot_observed_at":"2026-08-03T08:29:47.674701Z","title":"Unitarity of the infinite- volume three-particle scattering amplitude arising from a finite-volume formalism,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.674701Z"},"links":{"cited_paper":"/paper/1905.11188","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:14732cfcb4566a7ed48022b8012cf4dc33bad83fd1930485bb140e8ff5406717","observation_id":"44f6ab32-9081-4953-8812-0172f7c954b5","resolution":{"observed_at":"2026-08-03T08:29:47.674701Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1908.02411","last_updated":"2019-09-09T14:11:13Z","snapshot_observed_at":"2026-08-05T23:54:21.943658Z","submitted_at":"2019-08-07T01:05:44Z","title":"Numerical exploration of three relativistic particles in a finite volume including two-particle resonances and bound states","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1908.02411","snapshot_observed_at":"2026-08-03T08:29:47.679574Z","title":"Numerical exploration of three relativistic particles in a finite volume including two-particle resonances and bound states,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.679574Z"},"links":{"cited_paper":"/paper/1908.02411","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:8396b7cefd2e6e4e92d2c4bdcc916fa7e0c04ef548f927188a35a7549ce5e0ed","observation_id":"3ff99e9d-d33b-4472-ac5a-f6165f8285b3","resolution":{"observed_at":"2026-08-03T08:29:47.679574Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1902.01111","last_updated":"2019-08-09T18:01:09Z","snapshot_observed_at":"2026-08-03T17:34:47.327573Z","submitted_at":"2019-02-04T10:26:28Z","title":"Energy shift of the three-particle system in a finite volume","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1902.01111","snapshot_observed_at":"2026-08-03T08:29:47.684391Z","title":"Energy shift of the three-particle system in a finite volume,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.684391Z"},"links":{"cited_paper":"/paper/1902.01111","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:c8a07f5fc6d56d0f8b1f274584834a2cf37e2d09c1b50f1258f950953ac2c221","observation_id":"b5f359da-1bc4-4a75-8565-a372f8b68e34","resolution":{"observed_at":"2026-08-03T08:29:47.684391Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.08624","last_updated":"2020-01-12T23:40:04Z","snapshot_observed_at":"2026-08-08T13:26:03.753053Z","submitted_at":"2019-10-18T20:55:45Z","title":"A lattice model of heavy-light three-body system","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.08624","snapshot_observed_at":"2026-08-03T08:29:47.689001Z","title":"Lattice model of heavy-light three-body system,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.689001Z"},"links":{"cited_paper":"/paper/1910.08624","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:1628efca6387f54c50a398937d02275fc75e31b05f844da19074738f7da870f8","observation_id":"5d68473b-28ff-4c51-a23c-899de099db6f","resolution":{"observed_at":"2026-08-03T08:29:47.689001Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.05117","last_updated":"2019-05-13T16:13:12Z","snapshot_observed_at":"2026-08-09T14:12:29.415690Z","submitted_at":"2019-05-13T16:13:12Z","title":"$d$-dimensional L\\\"uscher's formula and the near-threshold three-body states in a finite volume","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.05117","snapshot_observed_at":"2026-08-03T08:29:47.693768Z","title":"d-dimensional L¨ uscher’s formula and the near-threshold three-body states in a finite volume,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.693768Z"},"links":{"cited_paper":"/paper/1905.05117","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:4d61678722f77f1e16af4375edb8c44e6da55088a95902f4c481d1ff1ba197fc","observation_id":"aa666b9c-d407-414d-b902-6bb880b9aef5","resolution":{"observed_at":"2026-08-03T08:29:47.693768Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.13014","last_updated":"2020-08-29T17:01:59Z","snapshot_observed_at":"2026-08-06T16:19:06.269019Z","submitted_at":"2020-08-29T17:01:59Z","title":"$DDK$ system in finite volume","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.13014","snapshot_observed_at":"2026-08-03T08:29:47.698764Z","title":"DDKsystem in finite volume,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.698764Z"},"links":{"cited_paper":"/paper/2008.13014","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:cab95f3aa534decfaf3fe706623c68dea1001889e6eaa523cffb0cccabb0efb3","observation_id":"2d88ad36-0bb6-4f3f-8812-2d81b2d2cfa8","resolution":{"observed_at":"2026-08-03T08:29:47.698764Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2003.10974","last_updated":"2020-12-30T15:40:48Z","snapshot_observed_at":"2026-08-03T16:25:55.258188Z","submitted_at":"2020-03-24T17:12:15Z","title":"Generalizing the relativistic quantization condition to include all three-pion isospin channels","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2003.10974","snapshot_observed_at":"2026-08-03T08:29:47.703763Z","title":"Generalizing the relativistic quantization condi- tion to include all three-pion isospin channels,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.703763Z"},"links":{"cited_paper":"/paper/2003.10974","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:61bc31c3d7a5643b81fb92b30297eb8753be860536c9588507cefee0fc5a4580","observation_id":"7800a5b4-ceb6-4fd8-b136-e2e2421471b2","resolution":{"observed_at":"2026-08-03T08:29:47.703763Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.12790","last_updated":"2020-09-08T22:11:33Z","snapshot_observed_at":"2026-08-10T06:21:20.276718Z","submitted_at":"2020-07-24T22:21:32Z","title":"Modeling few-body resonances in finite volume","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.12790","snapshot_observed_at":"2026-08-03T08:29:47.708763Z","title":"Modeling few-body resonances in finite volume,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.708763Z"},"links":{"cited_paper":"/paper/2007.12790","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:96521de90351373ecb73ef7a06f08c7e4f76e40969e459c74139d1a50e9d29f8","observation_id":"d27eabe8-cf49-4ea8-a8c6-b53dc68cbb35","resolution":{"observed_at":"2026-08-03T08:29:47.708763Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2002.04111","last_updated":"2020-02-10T22:13:02Z","snapshot_observed_at":"2026-08-03T13:19:56.218783Z","submitted_at":"2020-02-10T22:13:02Z","title":"Threshold expansion formula of $N$-boson in finite volume from variational approach","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2002.04111","snapshot_observed_at":"2026-08-03T08:29:47.713105Z","title":"Threshold expansion formula ofNbosons in a finite volume from a variational approach,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.713105Z"},"links":{"cited_paper":"/paper/2002.04111","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:05c7616f754ecb85dee7195be9197d802adafcf4cb7c965c23857a4f046bd1f6","observation_id":"29428477-b8bd-49c5-8112-79a16529067e","resolution":{"observed_at":"2026-08-03T08:29:47.713105Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.10895","last_updated":"2020-10-09T04:02:41Z","snapshot_observed_at":"2026-08-03T00:43:27.341973Z","submitted_at":"2020-07-21T15:37:10Z","title":"Visualizing resonances in finite volume","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.10895","snapshot_observed_at":"2026-08-03T08:29:47.717744Z","title":"Visualizing resonances in finite volume,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.717744Z"},"links":{"cited_paper":"/paper/2007.10895","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:555e6f9790272538f952e6d65e42aaf8c6a9a75d0d984f092b441b24dac3a29a","observation_id":"3b6f002c-2b51-4c25-bd32-91ed3a232e58","resolution":{"observed_at":"2026-08-03T08:29:47.717744Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2002.09266","last_updated":"2020-05-05T16:50:00Z","snapshot_observed_at":"2026-08-05T14:36:04.726069Z","submitted_at":"2020-02-21T13:24:15Z","title":"Multi-$\\pi^+$ systems in finite volume","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2002.09266","snapshot_observed_at":"2026-08-03T08:29:47.722074Z","title":"Multi-π + systems in a finite volume,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.722074Z"},"links":{"cited_paper":"/paper/2002.09266","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:e28147412f345555eeb8be3ba65886cd0e2ec096894337ced0447c49ecb22f0f","observation_id":"c4406518-630d-4e2c-b837-4d7778bb2f80","resolution":{"observed_at":"2026-08-03T08:29:47.722074Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.16188","last_updated":"2020-09-25T12:53:05Z","snapshot_observed_at":"2026-08-09T13:08:46.477021Z","submitted_at":"2020-07-31T17:33:03Z","title":"Alternative derivation of the relativistic three-particle quantization condition","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.16188","snapshot_observed_at":"2026-08-03T08:29:47.726543Z","title":"Alternative derivation of the relativistic three-particle quantization condition,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.726543Z"},"links":{"cited_paper":"/paper/2007.16188","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:45fe88c974b13c9f19d2db6a86f5633af09a7f34bd5aeced92161bc569bdcb5b","observation_id":"f7c030b4-5f2b-44e9-8c13-6ec57c6c23dc","resolution":{"observed_at":"2026-08-03T08:29:47.726543Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2011.05520","last_updated":"2021-03-10T16:45:09Z","snapshot_observed_at":"2026-08-10T22:36:05.705525Z","submitted_at":"2020-11-11T02:38:46Z","title":"Relativistic three-particle quantization condition for nondegenerate scalars","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2011.05520","snapshot_observed_at":"2026-08-03T08:29:47.730904Z","title":"Relativistic three-particle quantization condition for nondegenerate scalars,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.730904Z"},"links":{"cited_paper":"/paper/2011.05520","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:d71015991108ecf2f2775a731a8e8e32310f7be5e3b8617e579e1d8c3bfb900e","observation_id":"202f03e3-367a-4384-b5e8-40dc8faaece7","resolution":{"observed_at":"2026-08-03T08:29:47.730904Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T08:29:47.735219Z","title":"Finite-volume energy shift of the three-pion ground state,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.735219Z"},"links":{"citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:84c08a3283ae0e96695db6eaaae90866c26eaeec7df2fba312a857f8c81bec9b","observation_id":"37896768-1149-4f0b-98d5-1df0d456cab4","resolution":{"observed_at":"2026-08-03T08:29:47.735219Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.13957","last_updated":"2021-03-17T12:31:05Z","snapshot_observed_at":"2026-08-06T18:28:29.224674Z","submitted_at":"2020-12-27T14:58:36Z","title":"On the three-particle analog of the Lellouch-L\\\"uscher formula","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.13957","snapshot_observed_at":"2026-08-03T08:29:47.739536Z","title":"On the three-particle analog of the Lellouch-L¨ uscher formula,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.739536Z"},"links":{"cited_paper":"/paper/2012.13957","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:8a6b7bb30170f5619704ffce38664cf5f64e5628599e05ca914ce501798bd8e1","observation_id":"70f3d49b-395b-437c-9dd4-14f59e58c852","resolution":{"observed_at":"2026-08-03T08:29:47.739536Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.09820","last_updated":"2020-10-19T19:54:22Z","snapshot_observed_at":"2026-08-09T07:43:29.870562Z","submitted_at":"2020-10-19T19:54:22Z","title":"Solving relativistic three-body integral equations in the presence of bound states","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.09820","snapshot_observed_at":"2026-08-03T08:29:47.744606Z","title":"Solving relativistic three-body integral equations in the presence of bound states,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.744606Z"},"links":{"cited_paper":"/paper/2010.09820","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:99e96618f838ae335abe9f73782fc2d208625c1002efe50d1271a4a3f75e6e1c","observation_id":"fe1df860-32ec-4ea4-9b09-a3bb7c125d16","resolution":{"observed_at":"2026-08-03T08:29:47.744606Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2101.06144","last_updated":"2021-06-21T15:30:53Z","snapshot_observed_at":"2026-08-10T01:17:03.567674Z","submitted_at":"2021-01-15T14:42:23Z","title":"Three-body interactions from the finite-volume QCD spectrum","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2101.06144","snapshot_observed_at":"2026-08-03T08:29:47.749261Z","title":"Three-body interactions from the finite-volume QCD spectrum,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.749261Z"},"links":{"cited_paper":"/paper/2101.06144","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:f4477cdf081f19aaba26443224088dc595ff18461fbbed1375a6b269a4966d2b","observation_id":"00027519-77af-4553-80ff-b007c3905e53","resolution":{"observed_at":"2026-08-03T08:29:47.749261Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2110.09351","last_updated":"2022-02-10T10:13:42Z","snapshot_observed_at":"2026-08-08T09:04:44.445087Z","submitted_at":"2021-10-18T14:24:17Z","title":"Relativistic-invariant formulation of the NREFT three-particle quantization condition","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2110.09351","snapshot_observed_at":"2026-08-03T08:29:47.753909Z","title":"Relativistic-invariant formulation of the NREFT three- 28 particle quantization condition,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.753909Z"},"links":{"cited_paper":"/paper/2110.09351","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:b94e7cd0c55cb816f3c7ebadfda6f10874335158cfd926bde13c3cfbf23a9dec","observation_id":"b9df65c3-dd3c-4680-adbd-2cb618204b1f","resolution":{"observed_at":"2026-08-03T08:29:47.753909Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2101.10246","last_updated":"2021-04-23T16:44:37Z","snapshot_observed_at":"2026-08-09T18:09:24.498278Z","submitted_at":"2021-01-25T17:23:04Z","title":"Decay amplitudes to three hadrons from finite-volume matrix elements","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2101.10246","snapshot_observed_at":"2026-08-03T08:29:47.758527Z","title":"Decay amplitudes to three hadrons from finite- volume matrix elements,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.758527Z"},"links":{"cited_paper":"/paper/2101.10246","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:ae3b44d3d70ebf6fbed605b137c16eca41b7cade832880bca152074fb3b60caf","observation_id":"5c9c9bdc-8b39-4fec-b4b4-c960f32e6af5","resolution":{"observed_at":"2026-08-03T08:29:47.758527Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2105.12094","last_updated":"2021-08-21T17:15:20Z","snapshot_observed_at":"2026-08-08T13:42:41.661358Z","submitted_at":"2021-05-25T17:23:36Z","title":"Three-particle finite-volume formalism for $\\pi^+\\pi^+ K^+$ and related systems","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2105.12094","snapshot_observed_at":"2026-08-03T08:29:47.763249Z","title":"Three-particle finite-volume formalism forπ+π+K+ and related systems,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.763249Z"},"links":{"cited_paper":"/paper/2105.12094","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:601ceeedc37e3826d81d2deb9fe0afd26f9f039691fcb246a20c0be5a2191b7c","observation_id":"794f8783-62a3-4f83-b3a1-2fd9e9ff47b0","resolution":{"observed_at":"2026-08-03T08:29:47.763249Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.12734","last_updated":"2022-01-26T19:14:53Z","snapshot_observed_at":"2026-07-06T12:11:56.886534Z","submitted_at":"2021-11-24T19:00:10Z","title":"Implementing the three-particle quantization condition for $\\pi^+\\pi^+K^+$ and related systems","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.12734","snapshot_observed_at":"2026-08-03T08:29:47.768945Z","title":"Implementing the three-particle quantization condition forπ +π+K+ and related systems,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.768945Z"},"links":{"cited_paper":"/paper/2111.12734","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:2b3e3e98a447633bc3e9bdf2c355fc8ced0adc40416c524ffb2509104e3a20b5","observation_id":"21dae511-f1e4-40c6-a7cc-ccd1f30fb278","resolution":{"observed_at":"2026-08-03T08:29:47.768945Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.10126","last_updated":"2023-02-27T11:33:29Z","snapshot_observed_at":"2026-08-01T16:00:06.370264Z","submitted_at":"2022-11-18T10:04:39Z","title":"Three-particle Lellouch-L\\\"uscher formalism in moving frames","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.10126","snapshot_observed_at":"2026-08-03T08:29:47.774154Z","title":"Three-particle Lellouch-L¨ uscher formalism in moving frames,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.774154Z"},"links":{"cited_paper":"/paper/2211.10126","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:b7c8bdc38241ba94bebf335d8c688b42adf45c59dbd100b08c02dfc7dd3f9daa","observation_id":"2dec7d2d-41a8-4c18-a50d-435ef7029627","resolution":{"observed_at":"2026-08-03T08:29:47.774154Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2204.04807","last_updated":"2022-04-11T00:34:55Z","snapshot_observed_at":"2026-08-11T02:17:17.636263Z","submitted_at":"2022-04-11T00:34:55Z","title":"Spurious poles in a finite volume","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2204.04807","snapshot_observed_at":"2026-08-03T08:29:47.778838Z","title":"Spurious poles in a finite volume,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.778838Z"},"links":{"cited_paper":"/paper/2204.04807","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:bd355b6edabb472fe3ede2a2c9d4962cf4125054ae13fffed42c3f96c8c017bc","observation_id":"afe3efbc-4628-42ad-aeea-74b154d4754f","resolution":{"observed_at":"2026-08-03T08:29:47.778838Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.00625","last_updated":"2023-12-01T14:42:33Z","snapshot_observed_at":"2026-08-08T14:05:18.811803Z","submitted_at":"2023-12-01T14:42:33Z","title":"Partial-wave projection of the one-particle exchange in three-body scattering amplitudes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.00625","snapshot_observed_at":"2026-08-03T08:29:47.783801Z","title":"Partial-wave projection of the one-particle exchange in three-body scattering amplitudes,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.783801Z"},"links":{"cited_paper":"/paper/2312.00625","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:538c50f6a87fedad318e1bc32dfd4b3e04715574171e666cb636d7dc74c21cdd","observation_id":"0d995a0c-2d6c-4f9b-a256-531e5ded66af","resolution":{"observed_at":"2026-08-03T08:29:47.783801Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.04391","last_updated":"2024-04-26T04:42:00Z","snapshot_observed_at":"2026-08-05T01:57:28.831235Z","submitted_at":"2023-12-07T16:03:18Z","title":"Lellouch-L\\\"uscher factor for the $K\\to 3\\pi$ decays","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.04391","snapshot_observed_at":"2026-08-03T08:29:47.788545Z","title":"Lellouch-L¨ uscher factor for theK→3π decays,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.788545Z"},"links":{"cited_paper":"/paper/2312.04391","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:d428850a9f48b571721fca52854631436fb71f3d753c0a59aa1be3ef3a761511","observation_id":"7486e4ad-2a44-4117-aa30-7e43e1f8ba7e","resolution":{"observed_at":"2026-08-03T08:29:47.788545Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T08:29:47.793164Z","title":"Finite-volume energy shift of the three-nucleon ground state,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.793164Z"},"links":{"citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:8f16e139cecd56a050e77fd90b292df072294f23d70770dac9dbbd933b22883a","observation_id":"79c4bcdd-5ad2-4bbb-8d86-7d9c44c2c345","resolution":{"observed_at":"2026-08-03T08:29:47.793164Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.10219","last_updated":"2023-06-26T17:14:12Z","snapshot_observed_at":"2026-08-09T12:40:20.185047Z","submitted_at":"2023-03-17T19:30:26Z","title":"Three relativistic neutrons in a finite volume","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.10219","snapshot_observed_at":"2026-08-03T08:29:47.797348Z","title":"Three relativistic neutrons in a finite volume,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.797348Z"},"links":{"cited_paper":"/paper/2303.10219","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:2122c2d28cb248f93b5891b5b492110d08fa7f567aa8a8a0138346c77019f11b","observation_id":"6481af7a-cc41-4c7e-bd8f-1edd83a466fe","resolution":{"observed_at":"2026-08-03T08:29:47.797348Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T08:29:47.802041Z","title":"Finite-volume formalism forN ππat maximal isospin,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.802041Z"},"links":{"citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:6c7896d25b3bbe85c9cab82e80e44e9d86ad8b89e33899cf33fa9e1a74e74202","observation_id":"6cdbba11-897b-49d7-ac47-ac70c2395652","resolution":{"observed_at":"2026-08-03T08:29:47.802041Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T08:29:47.806644Z","title":"Implementing the three-neutron quantization condition,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.806644Z"},"links":{"citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:c399ed1f5d97a6b0e368651b80bef1341a5dd880942dc92e473788b0099cc061","observation_id":"fe3cfc47-bec8-4e7c-af66-135e75352656","resolution":{"observed_at":"2026-08-03T08:29:47.806644Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.10587","last_updated":"2022-08-22T20:38:56Z","snapshot_observed_at":"2026-07-06T13:44:22.049225Z","submitted_at":"2022-08-22T20:38:56Z","title":"Three-body scattering and quantization conditions from $S$ matrix unitarity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.10587","snapshot_observed_at":"2026-08-03T08:29:47.811043Z","title":"Three-body scattering and quantization conditions from S-matrix unitarity,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.811043Z"},"links":{"cited_paper":"/paper/2208.10587","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:6cf4eb92a138547058d128e3814ac6a0c27ece7aa73a7918b03cbe877e2ecda3","observation_id":"5ab746d9-1f65-4557-a1ae-a7eb791b4316","resolution":{"observed_at":"2026-08-03T08:29:47.811043Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.16190","last_updated":"2020-09-24T17:17:32Z","snapshot_observed_at":"2026-08-06T02:47:57.199735Z","submitted_at":"2020-07-31T17:33:50Z","title":"Equivalence of relativistic three-particle quantization conditions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.16190","snapshot_observed_at":"2026-08-03T08:29:47.816601Z","title":"Equivalence of relativistic three-particle quantization conditions,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.816601Z"},"links":{"cited_paper":"/paper/2007.16190","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:e9010bcd6a5b166897f90135428688e97017edf6b3b191ca9a363f1c0821d695","observation_id":"a6bed1a1-5674-4bb0-87f5-800d1f9e51d5","resolution":{"observed_at":"2026-08-03T08:29:47.816601Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1901.00483","last_updated":"2019-01-02T18:35:12Z","snapshot_observed_at":"2026-08-03T10:10:49.770207Z","submitted_at":"2019-01-02T18:35:12Z","title":"Lattice QCD and Three-particle Decays of Resonances","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1901.00483","snapshot_observed_at":"2026-08-03T08:29:47.822257Z","title":"Lattice QCD and Three-particle Decays of Resonances,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.822257Z"},"links":{"cited_paper":"/paper/1901.00483","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:8d9e0d60de05488195162fa28e46d791b800a53008ed027e29f01c482cf71fca","observation_id":"9d73cce9-50b4-46aa-b004-04c482634ea2","resolution":{"observed_at":"2026-08-03T08:29:47.822257Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.00577","last_updated":"2021-02-28T18:01:15Z","snapshot_observed_at":"2026-08-10T14:18:58.505855Z","submitted_at":"2021-02-28T18:01:15Z","title":"Multi-particle systems on the lattice and chiral extrapolations: a brief review","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.00577","snapshot_observed_at":"2026-08-03T08:29:47.826687Z","title":"Multi-particle systems on the lattice and chiral extrapolations: a brief review,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.826687Z"},"links":{"cited_paper":"/paper/2103.00577","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:052e679f30b84bde32748589763abcccaa8a67d45196e102fd231af4e8efc3ca","observation_id":"6a25020f-668a-4236-89da-cdfc3d288896","resolution":{"observed_at":"2026-08-03T08:29:47.826687Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T08:29:47.831262Z","title":"Three-particle scattering amplitudes from lattice QCD,","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.831262Z"},"links":{"citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:2dc7d3d71c5000f7494ee51672ab24a838c8c8f2d87471b03568a66d65569584","observation_id":"c68fe68e-7637-44d1-a198-1baa3a917445","resolution":{"observed_at":"2026-08-03T08:29:47.831262Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0903.4337","last_updated":"2009-09-18T22:51:05Z","snapshot_observed_at":"2026-07-06T01:55:39.201639Z","submitted_at":"2009-03-25T13:48:05Z","title":"Analytic properties of the scattering amplitude and resonances parameters in a meson exchange model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0903.4337","snapshot_observed_at":"2026-08-03T08:29:47.835771Z","title":"Analytic properties of the scattering amplitude and resonances parameters in a meson exchange model,","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.835771Z"},"links":{"cited_paper":"/paper/0903.4337","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:785180b991907b3f09296a1c4914588506b873540cefbd0e962a5168a8971a0b","observation_id":"20262db3-f032-4f83-80af-6a0a764ad44b","resolution":{"observed_at":"2026-08-03T08:29:47.835771Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0909.1356","last_updated":"2010-01-07T11:16:59Z","snapshot_observed_at":"2026-07-06T01:59:53.295097Z","submitted_at":"2009-09-07T23:15:59Z","title":"Disentangling the dynamical origin of P11 Nucleon Resonances","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0909.1356","snapshot_observed_at":"2026-08-03T08:29:47.840328Z","title":"Disentangling the Dynamical Origin of P-11 Nucleon Resonances,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.840328Z"},"links":{"cited_paper":"/paper/0909.1356","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:7fb0546ebbceb2463015db585d978bd65025e85fd1284d96e213af97035c1e84","observation_id":"d6b018a4-ef7b-41e7-9103-1e6f01ddf9f7","resolution":{"observed_at":"2026-08-03T08:29:47.840328Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.03355","last_updated":"2022-02-28T21:47:07Z","snapshot_observed_at":"2026-08-04T12:29:03.991476Z","submitted_at":"2021-12-06T21:01:36Z","title":"Pole position of the $a_1(1260)$ resonance in a three-body unitary framework","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.03355","snapshot_observed_at":"2026-08-03T08:29:47.845151Z","title":"Pole position of the a1(1260) resonance in a three-body unitary framework,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.845151Z"},"links":{"cited_paper":"/paper/2112.03355","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:f8e8a93b0c9001363280e42fece8abe53c01e56c4303d718adefc870edae8dd5","observation_id":"0c7eb441-6403-498c-af39-21a1dac4e3ce","resolution":{"observed_at":"2026-08-03T08:29:47.845151Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.04394","last_updated":"2023-03-08T05:55:24Z","snapshot_observed_at":"2026-08-09T09:42:38.596490Z","submitted_at":"2023-03-08T05:55:24Z","title":"Analytic continuation of the relativistic three-particle scattering amplitudes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.04394","snapshot_observed_at":"2026-08-03T08:29:47.850597Z","title":"Analytic continuation of the relativistic three-particle scattering amplitudes,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.850597Z"},"links":{"cited_paper":"/paper/2303.04394","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:1cbea63b6e502af605f7054433d208ecd5f5d0e11c47ce627031217e4ceec5ad","observation_id":"9303759f-31a6-4304-98fd-0c32edc00057","resolution":{"observed_at":"2026-08-03T08:29:47.850597Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T08:29:47.855614Z","title":"Dynamical coupled-channel models for hadron dynamics,","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.855614Z"},"links":{"citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:951dc2c52aa9a51e72868c0b95f537e95863c6b8a65d1bc4afc094f13fefdfb0","observation_id":"1b932309-0e4d-4714-9386-60e285bef036","resolution":{"observed_at":"2026-08-03T08:29:47.855614Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1909.02973","last_updated":"2021-03-15T09:16:33Z","snapshot_observed_at":"2026-08-05T07:00:28.553821Z","submitted_at":"2019-09-06T15:32:39Z","title":"$I = 3$ three-pion scattering amplitude from lattice QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.02973","snapshot_observed_at":"2026-08-03T08:29:47.860182Z","title":"I= 3 Three-Pion Scattering Amplitude from Lattice QCD,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.860182Z"},"links":{"cited_paper":"/paper/1909.02973","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:cac619a920a348496e5b41e09ed744924817eec10fd927bce8ea55b35fc6d858","observation_id":"b6cc9a0a-5859-4f9c-8181-02e889e3f529","resolution":{"observed_at":"2026-08-03T08:29:47.860182Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.17976","last_updated":"2025-07-15T15:01:45Z","snapshot_observed_at":"2026-08-07T17:50:50.330094Z","submitted_at":"2025-02-25T08:47:03Z","title":"Two- and three-meson scattering amplitudes with physical quark masses from lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.17976","snapshot_observed_at":"2026-08-03T08:29:47.864762Z","title":"Two- and three-meson scattering amplitudes with physical quark masses from lattice QCD,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.864762Z"},"links":{"cited_paper":"/paper/2502.17976","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:ce942162f1462a99f87eea66fadb7f6280870d5ec5c51af8ae0c97846806e21e","observation_id":"0fa17a44-7b2b-4fb0-abe5-efed40561186","resolution":{"observed_at":"2026-08-03T08:29:47.864762Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T08:29:47.869440Z","title":"Isotensor πππscattering with aρresonant subsystem from QCD,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.869440Z"},"links":{"citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:fc8f43a487d72b79f7d3a89c97ac4600b314cae419c59bbbbaf318e193e42dd4","observation_id":"aadbbf0e-4957-4672-b0b2-348b6bf2d26c","resolution":{"observed_at":"2026-08-03T08:29:47.869440Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.08721","last_updated":"2024-09-06T19:16:31Z","snapshot_observed_at":"2026-07-06T18:45:01.801741Z","submitted_at":"2024-07-11T17:55:30Z","title":"A unitary coupled-channel three-body amplitude with pions and kaons","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.08721","snapshot_observed_at":"2026-08-03T08:29:47.873718Z","title":"A unitary coupled-channel three-body amplitude with pions and kaons,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.873718Z"},"links":{"cited_paper":"/paper/2407.08721","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:1d5319a139b81417d92a54f3c94f737b0cec6dfa09a136e78a3f3e3f74b5d5e8","observation_id":"064d02a0-f571-443e-844b-d7b716f15d79","resolution":{"observed_at":"2026-08-03T08:29:47.873718Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T08:29:47.878470Z","title":"Revisiting the three-kaon interaction and its relation withK(1460),","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.878470Z"},"links":{"citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:c7377c8506f004f232fbbec6b01a33c18dfcd024e52cb50292fff9fffc84e7ad","observation_id":"7a9dc97b-0cc7-43a4-8454-70cfb5e149cb","resolution":{"observed_at":"2026-08-03T08:29:47.878470Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T08:29:47.883204Z","title":"Recent developments in chiral perturbation theory,","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.883204Z"},"links":{"citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:a7d3f7f0a7c5d35520dcac81b53a2c24ccaf432f785750a434eaecafab8cb420","observation_id":"5e175f24-c0f6-42c9-8b63-b6588c67d43b","resolution":{"observed_at":"2026-08-03T08:29:47.883204Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T08:29:47.888390Z","title":"Chiral perturbation theory: An effective field theory,","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.888390Z"},"links":{"citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:e77542ecf59cc41c0ea3507da110a4789d417a3345132e35394089116af62da1","observation_id":"e8b9afd9-8478-4b27-97e7-b604aacafab1","resolution":{"observed_at":"2026-08-03T08:29:47.888390Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1001.3229","last_updated":"2010-01-19T09:06:37Z","snapshot_observed_at":"2026-08-07T23:12:46.865082Z","submitted_at":"2010-01-19T09:06:37Z","title":"Nuclear forces from chiral effective field theory: a primer","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1001.3229","snapshot_observed_at":"2026-08-03T08:29:47.892947Z","title":"Nuclear Forces from Chiral Effective Field Theory: A Primer,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD","version":3},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-03T08:29:47.892947Z"},"links":{"cited_paper":"/paper/1001.3229","citing_paper":"/paper/2601.16916"},"observation_digest":"sha256:1b0ef2c3bad8316f2b978ddb14d5939015f6ec41ea9b5e75d3076700ca96e033","observation_id":"93a0d32a-778c-4391-88c4-18aaf057c978","resolution":{"observed_at":"2026-08-03T08:29:47.892947Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2601.16916","last_updated":"2026-07-31T16:21:13Z","latest_version":3,"primary_category":"hep-lat","snapshot_observed_at":"2026-08-09T21:53:29.015405Z","submitted_at":"2026-01-23T17:25:33Z","title":"Coupled-channel approach to isotensor $\\pi\\pi\\pi$ scattering from lattice QCD"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":100,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":128},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"thesis":"As of 11 August 2026, this Paper Citation Record lists 100 of 128 outbound references and 3 inbound Pith citation observations for arXiv:2601.16916."}