{"as_of":"2026-08-23T15:19:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:07de58bfe869d2ba9c4d12938f8ae3c5571264c816a3beb9d2e93dd1b49b6ed7","coverage":[{"denominator":79,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":79,"source":"paper_references, paper_reference_links","source_observed_at":"2026-07-31T09:15:14.066967Z","state":"measured"},{"denominator":79,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":79,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-23T06:30:58.430688+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/2607.24648/citation-record","integrity":"/paper/2607.24648/integrity","json":"/paper/2607.24648/citation-record.json","paper":"/paper/2607.24648"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-07-31T09:15:13.674893Z","title":"1 + ∞X n=0 [(i eB+iE)·i∆ 2 ·] niE ·i∆2 · # iW A df, /E A E=0","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.674893Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:83335bd73f085b4cab4e4acc784da7a12dda0d5973f27e351f13eec4018612fa","observation_id":"1632d2a0-c93b-40ee-99a3-8434079a900a","resolution":{"observed_at":"2026-07-31T09:15:13.674893Z","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":"2026-07-31T09:15:13.680896Z","title":"triangle-type","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.680896Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:4dc9893c83909991dae5ed62449adf79cece50147a1cb14db8acf1b931b4538b","observation_id":"096ff9bf-2a85-49a2-bb85-81bd0bcbe981","resolution":{"observed_at":"2026-07-31T09:15:13.680896Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2304.03762","last_updated":"2024-03-06T16:11:48Z","snapshot_observed_at":"2026-08-19T11:42:45.482239Z","submitted_at":"2023-04-07T17:57:04Z","title":"Determination of crossing-symmetric $\\pi\\pi$ scattering amplitudes and the quark mass evolution of the $\\sigma$ constrained by lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2304.03762","snapshot_observed_at":"2026-07-31T09:15:13.686355Z","title":"Rodas, J","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.686355Z"},"links":{"cited_paper":"/paper/2304.03762","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:8d0fc9b44e120a0db286daf79d59e08dcb32e90470fb99ebb2b5b0a3818c3fb8","observation_id":"0173d936-0068-4239-9785-369a1bcb093d","resolution":{"observed_at":"2026-07-31T09:15:13.686355Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1708.06667","last_updated":"2017-08-20T21:44:55Z","snapshot_observed_at":"2026-08-19T06:59:24.770664Z","submitted_at":"2017-08-20T21:44:55Z","title":"Isoscalar $\\pi\\pi, K\\overline{K}, \\eta\\eta$ scattering and the $\\sigma, f_0, f_2$ mesons from QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1708.06667","snapshot_observed_at":"2026-07-31T09:15:13.692020Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.692020Z"},"links":{"cited_paper":"/paper/1708.06667","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:dfdf75347a8c8443e3e9f4feafcf48c6b91c08637a4a4b81f26306bc9587c4ed","observation_id":"c42a5f63-7987-48c3-a28b-49c1084d74e7","resolution":{"observed_at":"2026-07-31T09:15:13.692020Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1602.05122","last_updated":"2016-02-16T18:26:21Z","snapshot_observed_at":"2026-08-20T16:58:56.610919Z","submitted_at":"2016-02-16T18:26:21Z","title":"An $a_0$ resonance in strongly coupled $\\pi \\eta$, $K\\overline{K}$ scattering from lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1602.05122","snapshot_observed_at":"2026-07-31T09:15:13.697362Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.697362Z"},"links":{"cited_paper":"/paper/1602.05122","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:472ab31c3bf4ce25ef45a526af81399cd12f4d3c37fc0ce6d34886277c677586","observation_id":"188acc5c-3da8-42fd-91b8-45d3d1b5ab1b","resolution":{"observed_at":"2026-07-31T09:15:13.697362Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.10034","last_updated":"2021-03-22T12:28:34Z","snapshot_observed_at":"2026-08-09T11:04:20.421324Z","submitted_at":"2020-09-21T17:14:25Z","title":"Decays of an exotic $1^{-+}$ hybrid meson resonance in QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.10034","snapshot_observed_at":"2026-07-31T09:15:13.703711Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.703711Z"},"links":{"cited_paper":"/paper/2009.10034","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:2b191dc52d7795d4a037cfebdaa3a5ecdc8bca7997ce1ab364d081b85906487f","observation_id":"7cd4ba91-d73f-4b4c-8e92-56663514b378","resolution":{"observed_at":"2026-07-31T09:15:13.703711Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.04528","last_updated":"2016-11-24T17:54:31Z","snapshot_observed_at":"2026-08-14T21:35:12.639106Z","submitted_at":"2016-10-14T16:43:55Z","title":"Heavy-Quark QCD Exotica","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.04528","snapshot_observed_at":"2026-07-31T09:15:13.709538Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.709538Z"},"links":{"cited_paper":"/paper/1610.04528","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:649085ebe620a9fffb2834928c8a35d967c68da1f2e8af8f2f8a926345806da7","observation_id":"6ca7e917-a358-40d4-85cf-0f512a4087af","resolution":{"observed_at":"2026-07-31T09:15:13.709538Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-20T09:24:49.701384Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-31T09:15:13.715061Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.715061Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:63e363b91ac31def4aab7a8e4c3dd6e96d7d65a0542247eadabec5479db44878","observation_id":"12c0cfae-de6c-4712-b5a8-d35cba23fd5a","resolution":{"observed_at":"2026-07-31T09:15:13.715061Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.04701","last_updated":"2025-02-07T07:11:58Z","snapshot_observed_at":"2026-08-20T09:20:35.335339Z","submitted_at":"2025-02-07T07:11:58Z","title":"Lattice perspectives on doubly heavy tetraquarks","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.04701","snapshot_observed_at":"2026-07-31T09:15:13.719866Z","title":"Francis, Prog","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.719866Z"},"links":{"cited_paper":"/paper/2502.04701","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:712f7fdbb1a54580def52931c64ea51455e1e6e0ff194fb7303f7b93ffd387a9","observation_id":"d4156af3-e922-4164-83d9-cc26a420bde1","resolution":{"observed_at":"2026-07-31T09:15:13.719866Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2202.10110","last_updated":"2022-06-25T13:56:19Z","snapshot_observed_at":"2026-08-18T20:16:49.054853Z","submitted_at":"2022-02-21T10:50:10Z","title":"Signature of a doubly charm tetraquark pole in $DD^*$ scattering on the lattice","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2202.10110","snapshot_observed_at":"2026-07-31T09:15:13.724634Z","title":"Padmanath and S","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.724634Z"},"links":{"cited_paper":"/paper/2202.10110","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:7c057f825f67e95d79192c7fbcc387b08982fd67024f1b5374bb32e6659d8b1d","observation_id":"b8294db2-b1ed-4954-9cb2-c34118358862","resolution":{"observed_at":"2026-07-31T09:15:13.724634Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.15741","last_updated":"2025-03-19T15:47:32Z","snapshot_observed_at":"2026-08-18T20:11:16.460727Z","submitted_at":"2024-05-24T17:36:34Z","title":"Near-threshold states in coupled $DD^{\\ast}-D^{\\ast}D^{\\ast}$ scattering from lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.15741","snapshot_observed_at":"2026-07-31T09:15:13.729592Z","title":"Whyte, D","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.729592Z"},"links":{"cited_paper":"/paper/2405.15741","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:821d96e2f9470461f7fa66e33451e92c7a27e01c07a1a117bf6997a1ba108746","observation_id":"6bf61633-0e08-4407-af32-c25c969e2567","resolution":{"observed_at":"2026-07-31T09:15:13.729592Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2302.04505","last_updated":"2023-10-17T08:29:08Z","snapshot_observed_at":"2026-08-18T20:17:29.844001Z","submitted_at":"2023-02-09T08:58:41Z","title":"Doubly Charmed Tetraquark $T^+_{cc}$ from Lattice QCD near Physical Point","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2302.04505","snapshot_observed_at":"2026-07-31T09:15:13.734129Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.734129Z"},"links":{"cited_paper":"/paper/2302.04505","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:6d12aacc82f109de3b58611855fef2800f285b62f600af26468ba81aa63d50df","observation_id":"df2b802a-e75b-42f0-8592-10c07bf7a4f6","resolution":{"observed_at":"2026-07-31T09:15:13.734129Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2607.19009","last_updated":"2026-07-21T11:49:59Z","snapshot_observed_at":"2026-08-18T00:12:23.231856Z","submitted_at":"2026-07-21T11:49:59Z","title":"Resolving the $T_{cc}^+$ with $\\pi$ Exchange from Lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2607.19009","snapshot_observed_at":"2026-07-31T09:15:13.738943Z","title":"Pitanga Lachini and R","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.738943Z"},"links":{"cited_paper":"/paper/2607.19009","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:44dd10ee9d0b8dfa8b64abf958a1aa2941fc17e90e0ed3c5f6f89af8d95bcc28","observation_id":"1513f1c4-b7ec-44ed-b4fd-d243a07dfc09","resolution":{"observed_at":"2026-07-31T09:15:13.738943Z","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":"2026-07-31T09:15:13.743506Z","title":"Nagatsuka and S","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.743506Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:e56ddcf47478e127cf42fc0e0fcdb5834e96bd785464f5e1cd29bd5d171a4c26","observation_id":"f4836dc6-fa4c-4408-814a-ce41d6b6f1e9","resolution":{"observed_at":"2026-07-31T09:15:13.743506Z","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":"2026-07-31T09:15:13.747859Z","title":"Aaijet al.(LHCb), Nature Commun.13, 3351 (2022), arXiv:2109.01056 [hep-ex]","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.747859Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:beb0339f3d115b0385d82628c4428163bae5ef70b3f34681da175a6c6c696def","observation_id":"1c5cac14-04bb-464c-945f-883e3f042077","resolution":{"observed_at":"2026-07-31T09:15:13.747859Z","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":"2026-07-31T09:15:13.752175Z","title":"Aaijet al.(LHCb), Nature Phys.18, 751 (2022), arXiv:2109.01038 [hep-ex]","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.752175Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:578b15d3e53cb50521d224e5b078bb951197d1a493f8eaf9654f26acfc7a1cbf","observation_id":"1a9165ec-a809-4264-9cbd-967affc35e6e","resolution":{"observed_at":"2026-07-31T09:15:13.752175Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.04649","last_updated":"2025-01-12T17:19:58Z","snapshot_observed_at":"2026-08-18T20:13:14.035953Z","submitted_at":"2024-07-05T17:05:00Z","title":"Internal structure of the $T_{cc}(3875)^+$ from its light-quark mass dependence","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.04649","snapshot_observed_at":"2026-07-31T09:15:13.756536Z","title":"Abolnikov, V","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.756536Z"},"links":{"cited_paper":"/paper/2407.04649","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:2bc37f7ce1defd53f5672da8f95fed94adf7296960c0c7ae83ca05175edaf313","observation_id":"56a854d3-fc13-4095-9fd1-bae4a9644581","resolution":{"observed_at":"2026-07-31T09:15:13.756536Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2510.17549","last_updated":"2026-04-29T14:32:34Z","snapshot_observed_at":"2026-08-13T20:24:21.594728Z","submitted_at":"2025-10-20T13:58:04Z","title":"Electromagnetic form factors and structure of the $T_{bb}$ tetraquark from lattice QCD","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2510.17549","snapshot_observed_at":"2026-07-31T09:15:13.760968Z","title":"Vujmilovic, S","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.760968Z"},"links":{"cited_paper":"/paper/2510.17549","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:e36e7b0c9d7226232ba22b52c8ac2dbd81587a9e8c3d768ca2083a93c95ddb9b","observation_id":"d170e5f0-8b95-4db8-ae40-58eb695173c3","resolution":{"observed_at":"2026-07-31T09:15:13.760968Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.08507","last_updated":"2015-09-28T21:05:01Z","snapshot_observed_at":"2026-08-18T20:15:33.251107Z","submitted_at":"2015-09-28T21:05:01Z","title":"Relativistic, model-independent, multichannel $2\\to2$ transition amplitudes in a finite volume","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.08507","snapshot_observed_at":"2026-07-31T09:15:13.765591Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.765591Z"},"links":{"cited_paper":"/paper/1509.08507","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:3847457ba2b7e039a88afb5df58351be20af01361ec5d596dafafca995c12c3c","observation_id":"590a2d41-e239-4a27-bf4d-6142fcca85b4","resolution":{"observed_at":"2026-07-31T09:15:13.765591Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.10504","last_updated":"2018-12-26T19:10:24Z","snapshot_observed_at":"2026-08-18T20:15:33.822543Z","submitted_at":"2018-12-26T19:10:24Z","title":"Form factors of two-hadron states from a covariant finite-volume formalism","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.10504","snapshot_observed_at":"2026-07-31T09:15:13.770049Z","title":"Baroni, R","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.770049Z"},"links":{"cited_paper":"/paper/1812.10504","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:1405ab73d22b85b1247f0dd0204b98c45bd98b317d337d313deffe5778e400e3","observation_id":"4db292e4-be0d-40e3-ac3f-d6c8a7056008","resolution":{"observed_at":"2026-07-31T09:15:13.770049Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.13338","last_updated":"2020-12-24T17:23:00Z","snapshot_observed_at":"2026-08-16T18:56:07.760523Z","submitted_at":"2020-12-24T17:23:00Z","title":"On-shell representations of two-body transition amplitudes: single external current","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.13338","snapshot_observed_at":"2026-07-31T09:15:13.774555Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.774555Z"},"links":{"cited_paper":"/paper/2012.13338","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:ccbb116daabe1cc5adb1f2ccca2d63ffe51960b67256af825b8819ed65f277f7","observation_id":"e02354e5-e6b4-4466-a76a-66ccb4b09dbb","resolution":{"observed_at":"2026-07-31T09:15:13.774555Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.08484","last_updated":"2024-06-23T17:05:35Z","snapshot_observed_at":"2026-08-19T23:43:15.525694Z","submitted_at":"2023-10-12T16:43:04Z","title":"Gravitational form factors of the proton from lattice QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.08484","snapshot_observed_at":"2026-07-31T09:15:13.779092Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.779092Z"},"links":{"cited_paper":"/paper/2310.08484","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:f1fb6d53c5722a416200b544aa7d1d1b33ea1976c7e1a4781d803d2169955048","observation_id":"8c959910-dac9-4c3c-8384-61481e8a53e9","resolution":{"observed_at":"2026-07-31T09:15:13.779092Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.01808","last_updated":"2021-11-02T18:00:06Z","snapshot_observed_at":"2026-08-16T17:44:31.690622Z","submitted_at":"2021-11-02T18:00:06Z","title":"The transversity parton distribution function of the nucleon using the pseudo-distribution approach","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.01808","snapshot_observed_at":"2026-07-31T09:15:13.784054Z","title":"Egereret al.(HadStruc), Phys","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.784054Z"},"links":{"cited_paper":"/paper/2111.01808","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:14dc13387e2a4944fa54b2a316aeb9c6bdae55688f58381ae24c0d4c3c99520b","observation_id":"203da982-6cca-433e-8684-e4734292926e","resolution":{"observed_at":"2026-07-31T09:15:13.784054Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.10304","last_updated":"2024-07-15T03:35:18Z","snapshot_observed_at":"2026-08-18T20:17:27.254002Z","submitted_at":"2024-05-16T17:56:22Z","title":"Towards Unpolarized GPDs from Pseudo-Distributions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.10304","snapshot_observed_at":"2026-07-31T09:15:13.788828Z","title":"Dutrieux, R","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.788828Z"},"links":{"cited_paper":"/paper/2405.10304","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:330ff00f03d40036562c829cb8c9d68e194d82aa6264bc13d4878925e6a5498b","observation_id":"8eb59de3-7295-498f-87aa-ac38269739d7","resolution":{"observed_at":"2026-07-31T09:15:13.788828Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.07519","last_updated":"2021-12-14T16:29:00Z","snapshot_observed_at":"2026-08-18T20:12:19.993348Z","submitted_at":"2021-12-14T16:29:00Z","title":"Nucleon Helicity Generalized Parton Distribution at Physical Pion Mass from Lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.07519","snapshot_observed_at":"2026-07-31T09:15:13.793439Z","title":"Lin, Phys","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.793439Z"},"links":{"cited_paper":"/paper/2112.07519","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:a5703f586b5b7e7a8518d8b90f23ab78353df5356d8dfc0d6c9a951f745126f8","observation_id":"3b976c26-030d-48cb-bdfe-ec7cb240baa0","resolution":{"observed_at":"2026-07-31T09:15:13.793439Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1908.10706","last_updated":"2020-03-02T18:48:58Z","snapshot_observed_at":"2026-08-16T00:33:55.712757Z","submitted_at":"2019-08-28T13:13:10Z","title":"Moments of nucleon generalized parton distributions from lattice QCD simulations at physical pion mass","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1908.10706","snapshot_observed_at":"2026-07-31T09:15:13.798517Z","title":"Alexandrouet al., Phys","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.798517Z"},"links":{"cited_paper":"/paper/1908.10706","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:cd2da3e9f39db53b511c130e951d8d85a244740452cea22c339bbd0421a42355","observation_id":"ae239fc0-5919-4bd8-96c8-c62fd7be9faf","resolution":{"observed_at":"2026-07-31T09:15:13.798517Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.11117","last_updated":"2023-05-18T16:58:26Z","snapshot_observed_at":"2026-08-20T15:13:31.507366Z","submitted_at":"2023-05-18T16:58:26Z","title":"Moments of proton GPDs from the OPE of nonlocal quark bilinears up to NNLO","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.11117","snapshot_observed_at":"2026-07-31T09:15:13.802993Z","title":"Bhattacharya, K","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.802993Z"},"links":{"cited_paper":"/paper/2305.11117","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:5ad6b0991709163a9ccaf5c2899fca7f3a8919f91859cc2f8def95966da11839","observation_id":"039882d2-294d-4240-81fa-8e502626352a","resolution":{"observed_at":"2026-07-31T09:15:13.802993Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.03539","last_updated":"2025-02-04T15:06:13Z","snapshot_observed_at":"2026-08-18T21:35:23.505829Z","submitted_at":"2024-10-04T15:55:00Z","title":"Moments of Axial-Vector GPD from Lattice QCD: Quark Helicity, Orbital Angular Momentum, and Spin-Orbit Correlation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.03539","snapshot_observed_at":"2026-07-31T09:15:13.808330Z","title":"Bhattacharya, K","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.808330Z"},"links":{"cited_paper":"/paper/2410.03539","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:25f9e4b57b02430af0676741db4ca7a75804562c8c1aff4a0130c4822b324a74","observation_id":"a35dab63-0f91-422b-81b8-fc1823dfe25f","resolution":{"observed_at":"2026-07-31T09:15:13.808330Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2508.17998","last_updated":"2025-10-28T19:49:56Z","snapshot_observed_at":"2026-08-20T13:00:07.226063Z","submitted_at":"2025-08-25T13:09:36Z","title":"Generalized Parton Distributions from Lattice QCD with Asymmetric Momentum Transfer: Unpolarized Quarks at Nonzero Skewness","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.17998","snapshot_observed_at":"2026-07-31T09:15:13.812930Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.812930Z"},"links":{"cited_paper":"/paper/2508.17998","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:20a65c2c10cdb05a3d12819d403c2ff07faef7a4a8ad7059273032c2cbf0244f","observation_id":"899dab57-c8de-496f-a458-c91cfef06fcc","resolution":{"observed_at":"2026-07-31T09:15:13.812930Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0003023","last_updated":"2000-03-28T15:40:08Z","snapshot_observed_at":"2026-08-14T12:34:37.716608Z","submitted_at":"2000-03-28T15:40:08Z","title":"Weak transition matrix elements from finite-volume correlation functions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0003023","snapshot_observed_at":"2026-07-31T09:15:13.817755Z","title":"Lellouch and M","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.817755Z"},"links":{"cited_paper":"/paper/hep-lat/0003023","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:16ff61348f1cf2e2d2553c97f82a29b58d23bcc6d04b55a9aa1a68021c69109d","observation_id":"c70131cf-97c9-4c6e-ab71-f89fdacb0153","resolution":{"observed_at":"2026-07-31T09:15:13.817755Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0507009","last_updated":"2005-07-11T19:40:42Z","snapshot_observed_at":"2026-08-14T12:28:44.860913Z","submitted_at":"2005-07-11T19:40:42Z","title":"Finite Volume Corrections to the Two-Particle Decay of States with Non-Zero Momentum","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0507009","snapshot_observed_at":"2026-07-31T09:15:13.823195Z","title":null,"venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.823195Z"},"links":{"cited_paper":"/paper/hep-lat/0507009","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:e705aff220af1a2d4127a3ad4ff1e00d547a07960744b982ee3648a0276f4c9a","observation_id":"a18b14d2-69bc-491c-b4ff-25314e15bed1","resolution":{"observed_at":"2026-07-31T09:15:13.823195Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1406.5965","last_updated":"2015-01-29T21:14:07Z","snapshot_observed_at":"2026-08-14T23:29:23.200398Z","submitted_at":"2014-06-23T16:20:53Z","title":"Multichannel one-to-two transition amplitudes in a finite volume","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1406.5965","snapshot_observed_at":"2026-07-31T09:15:13.828198Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.828198Z"},"links":{"cited_paper":"/paper/1406.5965","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:e011bbe6f50b0a1328f0f96138b5d2d451dc0a994568c362fe5cc18085361144","observation_id":"23c7b9d4-b491-4412-a3dc-ef9fac4ec46c","resolution":{"observed_at":"2026-07-31T09:15:13.828198Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1502.04314","last_updated":"2015-02-15T14:16:24Z","snapshot_observed_at":"2026-08-14T22:59:59.075164Z","submitted_at":"2015-02-15T14:16:24Z","title":"Multichannel 0-to-2 and 1-to-2 transition amplitudes for arbitrary spin particles in a finite volume","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1502.04314","snapshot_observed_at":"2026-07-31T09:15:13.833821Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.833821Z"},"links":{"cited_paper":"/paper/1502.04314","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:3c444239d142f45d5f699075c26abc45909d82af85548f2d29ea813b20e65ac3","observation_id":"c606606f-f52c-4d4a-9fdb-e76f57ff2cc6","resolution":{"observed_at":"2026-07-31T09:15:13.833821Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1605.03386","last_updated":"2016-05-11T11:36:54Z","snapshot_observed_at":"2026-08-14T21:57:52.191673Z","submitted_at":"2016-05-11T11:36:54Z","title":"The $B\\to K^*$ form factors on the lattice","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1605.03386","snapshot_observed_at":"2026-07-31T09:15:13.838567Z","title":"Agadjanov, V","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.838567Z"},"links":{"cited_paper":"/paper/1605.03386","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:c83592b02b4af6601d07515d95f232afd1883016d6df08b3a98e604f8ecc19e9","observation_id":"2c48594d-dee6-420a-a09f-572ab452e8f1","resolution":{"observed_at":"2026-07-31T09:15:13.838567Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1604.03530","last_updated":"2016-04-12T19:14:24Z","snapshot_observed_at":"2026-08-14T22:01:58.677021Z","submitted_at":"2016-04-12T19:14:24Z","title":"The $\\pi\\pi\\to\\pi\\gamma^\\star$ amplitude and the resonant $\\rho\\to\\pi\\gamma^\\star$ transition from lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1604.03530","snapshot_observed_at":"2026-07-31T09:15:13.843201Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.843201Z"},"links":{"cited_paper":"/paper/1604.03530","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:b40f6db330945f2f7b26a605e4f9644d258d7a2bc8a627128612efee8249af41","observation_id":"c9bbce9e-248a-4d49-8787-e2117811d6b2","resolution":{"observed_at":"2026-07-31T09:15:13.843201Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.08357","last_updated":"2022-01-05T17:35:26Z","snapshot_observed_at":"2026-08-14T18:49:03.544410Z","submitted_at":"2018-07-22T20:02:20Z","title":"The $\\pi\\gamma \\to \\pi\\pi$ transition and the $\\rho$ radiative decay width from lattice QCD","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.08357","snapshot_observed_at":"2026-07-31T09:15:13.848142Z","title":"Alexandrou, L","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.848142Z"},"links":{"cited_paper":"/paper/1807.08357","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:ba7e3dfbc0200bdf2361cd247fdc231c18bf8eea41e400a17f1595478908661d","observation_id":"6e00bd18-6ec9-48eb-aebe-db4baedebe0b","resolution":{"observed_at":"2026-07-31T09:15:13.848142Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.6319","last_updated":"2015-03-05T15:15:54Z","snapshot_observed_at":"2026-08-14T23:06:48.487020Z","submitted_at":"2014-12-19T12:55:10Z","title":"Timelike pion form factor in lattice QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.6319","snapshot_observed_at":"2026-07-31T09:15:13.853186Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.853186Z"},"links":{"cited_paper":"/paper/1412.6319","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:d0b0bf81370b4c1649f6e7c747fa7dcab325a5bf7f8e39711ffc70e356357de8","observation_id":"8ca875b1-0439-4bfa-9888-833c0b431ddc","resolution":{"observed_at":"2026-07-31T09:15:13.853186Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.05007","last_updated":"2018-12-17T10:19:50Z","snapshot_observed_at":"2026-08-14T18:40:58.174338Z","submitted_at":"2018-08-15T09:09:20Z","title":"The $I=1$ pion-pion scattering amplitude and timelike pion form factor from $N_{\\rm f} = 2+1$ lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.05007","snapshot_observed_at":"2026-07-31T09:15:13.857948Z","title":"Andersen, J","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.857948Z"},"links":{"cited_paper":"/paper/1808.05007","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:7b67ad54ac07c07f548f34f3711363204797e6f46ff0d6796c57da8ac0ae8674","observation_id":"db8b5eb7-99b9-4905-9635-896fc48c0b51","resolution":{"observed_at":"2026-07-31T09:15:13.857948Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.01083","last_updated":"2019-10-02T16:57:33Z","snapshot_observed_at":"2026-08-11T15:07:31.989132Z","submitted_at":"2019-10-02T16:57:33Z","title":"Rho resonance, timelike pion form factor, and implications for lattice studies of the hadronic vacuum polarisation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.01083","snapshot_observed_at":"2026-07-31T09:15:13.863701Z","title":"Erben, J","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.863701Z"},"links":{"cited_paper":"/paper/1910.01083","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:827fb25cec9748f5afee21fc856b5701a333cee5a1ff5cffee64b856ce35a5f1","observation_id":"22105d9b-00bc-4f89-abdb-9d3eef3bd999","resolution":{"observed_at":"2026-07-31T09:15:13.863701Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.13755","last_updated":"2022-08-29T17:40:37Z","snapshot_observed_at":"2026-08-17T17:58:03.885503Z","submitted_at":"2022-08-29T17:40:37Z","title":"Radiative decay of the resonant $K^*$ and the $\\gamma K \\to K \\pi$ amplitude from lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.13755","snapshot_observed_at":"2026-07-31T09:15:13.870701Z","title":"Radhakrishnan, J","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.870701Z"},"links":{"cited_paper":"/paper/2208.13755","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:a6fc9629deb987950a5cb65def1ee7167bb0d46821c7d2ab315832b1cbd7df8b","observation_id":"2aad5f98-be7a-4474-bf08-0bf6be831616","resolution":{"observed_at":"2026-07-31T09:15:13.870701Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.20617","last_updated":"2024-07-30T07:47:45Z","snapshot_observed_at":"2026-08-16T13:29:58.468815Z","submitted_at":"2024-07-30T07:47:45Z","title":"Timelike meson form-factors beyond the elastic region from lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.20617","snapshot_observed_at":"2026-07-31T09:15:13.875838Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.875838Z"},"links":{"cited_paper":"/paper/2407.20617","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:c52e7f043018aae7bdf8f8ac4c16c1513d56bbb1f1e4c6c99b5339bae81fb323","observation_id":"6edf7eb0-3dce-4488-ad34-dc738ffcad3c","resolution":{"observed_at":"2026-07-31T09:15:13.875838Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1909.10357","last_updated":"2019-09-23T13:21:04Z","snapshot_observed_at":"2026-08-18T20:12:19.449650Z","submitted_at":"2019-09-23T13:21:04Z","title":"Consistency checks for two-body finite-volume matrix elements: I. Conserved currents and bound states","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.10357","snapshot_observed_at":"2026-07-31T09:15:13.880600Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.880600Z"},"links":{"cited_paper":"/paper/1909.10357","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:0db9bddc65822ad2367bd45cca4be698c8276caa37d74a8d12f04fbaabd7cfa4","observation_id":"ab7625c7-72e9-45c8-b8aa-fe789242f02d","resolution":{"observed_at":"2026-07-31T09:15:13.880600Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2002.00023","last_updated":"2020-01-31T19:05:14Z","snapshot_observed_at":"2026-08-14T12:26:53.997620Z","submitted_at":"2020-01-31T19:05:14Z","title":"Consistency checks for two-body finite-volume matrix elements: II. Perturbative systems","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2002.00023","snapshot_observed_at":"2026-07-31T09:15:13.885711Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.885711Z"},"links":{"cited_paper":"/paper/2002.00023","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:030ba1c232ddee3924c8ae2a628d0b6e3a48902dffdb2809b137f4fd05729b95","observation_id":"5d5cca35-f986-426e-97bb-d7fdf9c45cce","resolution":{"observed_at":"2026-07-31T09:15:13.885711Z","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":"2026-07-31T09:15:13.890125Z","title":"Moscoso, F","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.890125Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:4ab44cf346e8c009470ef74d09176e66c382766161921bb16734e452e3ebfba7","observation_id":"cb595ece-e7a7-4821-95a1-7dd290e0bb4e","resolution":{"observed_at":"2026-07-31T09:15:13.890125Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2603.09554","last_updated":"2026-07-07T16:01:51Z","snapshot_observed_at":"2026-08-04T00:00:44.358001Z","submitted_at":"2026-03-10T12:02:20Z","title":"First-Principles Determination of the Proton-Proton Fusion Matrix Element from Lattice QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2603.09554","snapshot_observed_at":"2026-07-31T09:15:13.894452Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.894452Z"},"links":{"cited_paper":"/paper/2603.09554","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:03f852f258897ca9961ab0927bbcd06e9e88322d98ebf637c1cde41ab867a570","observation_id":"a4d4b4b1-8f45-43df-8194-55aa8bcbeb50","resolution":{"observed_at":"2026-07-31T09:15:13.894452Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.09441","last_updated":"2023-08-31T03:56:09Z","snapshot_observed_at":"2026-08-18T20:18:35.406002Z","submitted_at":"2023-03-16T16:15:49Z","title":"Role of left-hand cut contributions on pole extractions from lattice data: Case study for $T_{cc}(3875)^+$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.09441","snapshot_observed_at":"2026-07-31T09:15:13.899120Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.899120Z"},"links":{"cited_paper":"/paper/2303.09441","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:eabc64569865343ef0ad89cf520ddab3ff5f9f0c6fab8697b2dd8c046bd56842","observation_id":"b3d7d024-ca9a-4388-ad19-6c6ababe2e15","resolution":{"observed_at":"2026-07-31T09:15:13.899120Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.01054","last_updated":"2021-11-15T17:54:48Z","snapshot_observed_at":"2026-08-18T20:12:45.464815Z","submitted_at":"2021-03-01T14:57:03Z","title":"Weakly bound $H$ dibaryon from SU(3)-flavor-symmetric QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.01054","snapshot_observed_at":"2026-07-31T09:15:13.905273Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.905273Z"},"links":{"cited_paper":"/paper/2103.01054","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:265a1e16411e469be393384afc4ff7603d5268821bfe2ffc37ec33554acdb629","observation_id":"867627d2-b818-4ba3-9659-025071d5dfce","resolution":{"observed_at":"2026-07-31T09:15:13.905273Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2311.18793","last_updated":"2024-10-10T09:22:28Z","snapshot_observed_at":"2026-08-21T09:43:26.950792Z","submitted_at":"2023-11-30T18:41:30Z","title":"Finite-volume scattering on the left-hand cut","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.18793","snapshot_observed_at":"2026-07-31T09:15:13.910491Z","title":"Bai˜ ao Raposo and M","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.910491Z"},"links":{"cited_paper":"/paper/2311.18793","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:36cf7072ace96bae774886e7468b4b8066de3be5df9a2b070724d5f391b4167a","observation_id":"8db542f2-d83d-4940-989e-f34b36d2e385","resolution":{"observed_at":"2026-07-31T09:15:13.910491Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.19375","last_updated":"2025-02-26T18:16:26Z","snapshot_observed_at":"2026-08-18T20:18:07.025515Z","submitted_at":"2025-02-26T18:16:26Z","title":"Extracting scattering amplitudes for arbitrary two-particle systems with one-particle left-hand cuts via lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.19375","snapshot_observed_at":"2026-07-31T09:15:13.915563Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.915563Z"},"links":{"cited_paper":"/paper/2502.19375","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:69464ca534d629c7e4deb95bbf0b46db16581961551895c5d9bcbb9e155097eb","observation_id":"869301ab-988e-4657-bfd7-5edb850cf5a3","resolution":{"observed_at":"2026-07-31T09:15:13.915563Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.01930","last_updated":"2024-04-29T04:28:05Z","snapshot_observed_at":"2026-08-18T20:19:11.849627Z","submitted_at":"2023-12-04T14:38:46Z","title":"Solving the left-hand cut problem in lattice QCD: $T_{cc}(3875)^+$ from finite volume energy levels","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.01930","snapshot_observed_at":"2026-07-31T09:15:13.920636Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.920636Z"},"links":{"cited_paper":"/paper/2312.01930","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:23e4480744ea2b55fc4282b34201d0b81485e2632b6a477e0c0e73383eba8e1e","observation_id":"461006ec-6b85-4194-b7e0-ea601df8278a","resolution":{"observed_at":"2026-07-31T09:15:13.920636Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.12985","last_updated":"2024-04-24T14:42:34Z","snapshot_observed_at":"2026-08-18T20:13:16.673316Z","submitted_at":"2024-02-20T13:14:02Z","title":"L\\\"uscher equation with long-range forces","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.12985","snapshot_observed_at":"2026-07-31T09:15:13.925966Z","title":"Bubna, H.-W","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.925966Z"},"links":{"cited_paper":"/paper/2402.12985","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:f35d7183c2672a9d994e781497e583b44682122ec147b625abdebc47851d6d3b","observation_id":"e2650896-5b22-45fa-9118-4008deff7861","resolution":{"observed_at":"2026-07-31T09:15:13.925966Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.06609","last_updated":"2024-06-03T06:37:07Z","snapshot_observed_at":"2026-08-18T20:11:47.210419Z","submitted_at":"2024-01-12T14:55:48Z","title":"Incorporating $DD\\pi$ effects and left-hand cuts in lattice QCD studies of the $T_{cc}(3875)^+$","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.06609","snapshot_observed_at":"2026-07-31T09:15:13.931445Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.931445Z"},"links":{"cited_paper":"/paper/2401.06609","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:6a26fae915531aea900d4bd1635b01100761b57ffbb7ac1c6e0a4f0fb2fcc39e","observation_id":"08239ac3-bca6-4eaf-94ca-19ea9963f8d0","resolution":{"observed_at":"2026-07-31T09:15:13.931445Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.15730","last_updated":"2024-11-24T06:17:31Z","snapshot_observed_at":"2026-08-18T20:35:11.414367Z","submitted_at":"2024-11-24T06:17:31Z","title":"Finite-volume quantization condition from the $N/D$ representation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.15730","snapshot_observed_at":"2026-07-31T09:15:13.937044Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.937044Z"},"links":{"cited_paper":"/paper/2411.15730","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:2730cf802861c69558228b450ea3d705eb86f7897757939e8932cda7048423bb","observation_id":"ba04f7f7-167f-4e0b-95aa-572c74f04fed","resolution":{"observed_at":"2026-07-31T09:15:13.937044Z","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":"2026-07-31T09:15:13.942202Z","title":"Yu, G.-J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.942202Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:d7cc847dc1c261316630b8971a21cb2b4adcdcc5693836049c4813aa09461c62","observation_id":"483c3202-330b-4967-a210-c3df431bb811","resolution":{"observed_at":"2026-07-31T09:15:13.942202Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.06266","last_updated":"2025-03-06T10:08:16Z","snapshot_observed_at":"2026-08-16T13:01:30.641709Z","submitted_at":"2024-11-09T19:35:05Z","title":"Doubly charm tetraquark channel with isospin $1$ from lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.06266","snapshot_observed_at":"2026-07-31T09:15:13.946803Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.946803Z"},"links":{"cited_paper":"/paper/2411.06266","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:73ca765d2b45778418412affdccd4d717a0ee53e467bf20b464a3fcd47bde29c","observation_id":"968eeaac-2115-47c7-8f3e-ad4cca9a0ddd","resolution":{"observed_at":"2026-07-31T09:15:13.946803Z","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":"2026-08-16T13:15:26.266291Z","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":"2026-07-31T09:15:13.951443Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.951443Z"},"links":{"cited_paper":"/paper/2409.17059","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:d23343bc8b926a8198d7bcfca074bd7906509ccf75927c60831436558a5aee3c","observation_id":"1bb015db-e1bd-4a33-b2dc-1936797a4038","resolution":{"observed_at":"2026-07-31T09:15:13.951443Z","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":"2026-07-31T09:15:13.957157Z","title":"Abolnikov, L","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.957157Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:04fb7e9ea3f55224ba2e7bab9201f666afe0a6c978c048daef0ad3df7ae490b9","observation_id":"3b02c65c-ee34-410a-b4d6-57c538632d00","resolution":{"observed_at":"2026-07-31T09:15:13.957157Z","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":"2026-07-31T09:15:13.962136Z","title":"Alharazin, A","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.962136Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:8ed277fec769f0623a8bf4aa5d424c2030c9f692fbaf9542f01dcfa92ab0bb4c","observation_id":"16401711-5444-4a9b-b781-20ff6c69a1e8","resolution":{"observed_at":"2026-07-31T09:15:13.962136Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2605.22957","last_updated":"2026-05-21T18:43:53Z","snapshot_observed_at":"2026-08-19T04:56:44.202071Z","submitted_at":"2026-05-21T18:43:53Z","title":"Finite-volume analysis of the $H$-dibaryon including left-hand-cut effects","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2605.22957","snapshot_observed_at":"2026-07-31T09:15:13.966748Z","title":"Rodas, L","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.966748Z"},"links":{"cited_paper":"/paper/2605.22957","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:8cbec0ddd38fbc6f4b5df3b5d3cdb797273158b033d0b222e86d1d876946e467","observation_id":"b50a8055-e8ff-4e3b-8e75-a8f894ff846e","resolution":{"observed_at":"2026-07-31T09:15:13.966748Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1608.04793","last_updated":"2016-08-16T22:12:21Z","snapshot_observed_at":"2026-08-14T21:43:55.824382Z","submitted_at":"2016-08-16T22:12:21Z","title":"Neutrinoless double beta decay from lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1608.04793","snapshot_observed_at":"2026-07-31T09:15:13.971817Z","title":"Nicholson, E","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.971817Z"},"links":{"cited_paper":"/paper/1608.04793","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:d029ff11e8865e2e91f13e05067f8dd975686260a58918977e70087c80233277","observation_id":"d6e9d2b9-27c5-4030-b0fc-a3410a2daa08","resolution":{"observed_at":"2026-07-31T09:15:13.971817Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/9804032","last_updated":"1998-11-18T00:35:57Z","snapshot_observed_at":"2026-08-19T23:17:30.011518Z","submitted_at":"1998-04-16T23:54:18Z","title":"A Perturbative Calculation of the Electromagnetic Form Factors of the Deuteron","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/9804032","snapshot_observed_at":"2026-07-31T09:15:13.976977Z","title":null,"venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.976977Z"},"links":{"cited_paper":"/paper/nucl-th/9804032","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:8d958ba9826a6a49bf03f2771cf56bf585352e7ab5b61c691ed21c29ef625134","observation_id":"d4cbbd09-4c07-45c9-be5a-b050b90c7195","resolution":{"observed_at":"2026-07-31T09:15:13.976977Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/9505017","last_updated":"1995-05-12T06:39:04Z","snapshot_observed_at":"2026-08-11T14:19:12.397191Z","submitted_at":"1995-05-12T06:39:04Z","title":"Chiral Lagrangian Approach to Exchange Vector Currents in Nuclei","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/9505017","snapshot_observed_at":"2026-07-31T09:15:13.982594Z","title":"Park, D.-P","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.982594Z"},"links":{"cited_paper":"/paper/nucl-th/9505017","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:7009c8b70f262fbd0635936d5c4ab8fce1837b1f6f8e08497d18bf539d3f3e3e","observation_id":"db8e7622-88da-49eb-93c5-71e2117a1dbf","resolution":{"observed_at":"2026-07-31T09:15:13.982594Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1106.4539","last_updated":"2011-06-22T19:41:59Z","snapshot_observed_at":"2026-08-15T04:43:10.591191Z","submitted_at":"2011-06-22T19:41:59Z","title":"The two-nucleon electromagnetic charge operator in chiral effective field theory ($\\chi$EFT) up to one loop","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1106.4539","snapshot_observed_at":"2026-07-31T09:15:13.988107Z","title":"Pastore, L","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.988107Z"},"links":{"cited_paper":"/paper/1106.4539","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:8b773be7f361f23ab1e9be9b60236821f643ee2653997cfb0786b109450127b9","observation_id":"4fce0657-e362-4c27-9012-ed67ec3cda48","resolution":{"observed_at":"2026-07-31T09:15:13.988107Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1107.0602","last_updated":"2011-07-04T11:59:39Z","snapshot_observed_at":"2026-08-17T21:20:35.123723Z","submitted_at":"2011-07-04T11:59:39Z","title":"Two-nucleon electromagnetic current in chiral effective field theory: one-pion exchange and short-range contributions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1107.0602","snapshot_observed_at":"2026-07-31T09:15:13.993636Z","title":"Kolling, E","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.993636Z"},"links":{"cited_paper":"/paper/1107.0602","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:5ec97a1739a30cac13ce2b046d03a366dd5f7424a7e1691d77eab36cd3882474","observation_id":"a5797908-4ad3-4167-a7c3-f6aeee414466","resolution":{"observed_at":"2026-07-31T09:15:13.993636Z","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":"2026-08-18T20:16:09.861290Z","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":"2026-07-31T09:15:13.998731Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.998731Z"},"links":{"cited_paper":"/paper/2010.09820","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:4551f59e14452a5c6f782dcda727cc64efa464ab142483f20cf3e002ddf0365f","observation_id":"33b6da3b-b2cb-40ac-b180-a862a9a26a1b","resolution":{"observed_at":"2026-07-31T09:15:13.998731Z","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":"2026-08-18T20:11:19.890690Z","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":"2026-07-31T09:15:14.003775Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.003775Z"},"links":{"cited_paper":"/paper/2303.04394","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:39ef1339a74c221457bf14a5aa836be9e7528841b108853e4f5e75006044e0e8","observation_id":"e1799192-89f5-409b-b776-68421901ed85","resolution":{"observed_at":"2026-07-31T09:15:14.003775Z","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":"2026-08-18T20:19:10.781031Z","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":"2026-07-31T09:15:14.008874Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.008874Z"},"links":{"cited_paper":"/paper/2312.00625","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:cc9984fad58ddf8f78526ba7c844816c863592ee7079375c5f57de7b541e8243","observation_id":"bf90c37f-83c6-4ada-8a17-3b699c09a31f","resolution":{"observed_at":"2026-07-31T09:15:14.008874Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1205.4642","last_updated":"2012-05-21T15:54:19Z","snapshot_observed_at":"2026-08-18T20:10:36.611679Z","submitted_at":"2012-05-21T15:54:19Z","title":"Matrix elements of unstable states","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1205.4642","snapshot_observed_at":"2026-07-31T09:15:14.014330Z","title":"Bernard, D","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.014330Z"},"links":{"cited_paper":"/paper/1205.4642","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:dada3c40ba6295820136e011b4debd14093b12b3110680c3a0f531bbdd749c18","observation_id":"41e6ebb5-603b-48a8-9501-5fb72cebe780","resolution":{"observed_at":"2026-07-31T09:15:14.014330Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2602.23044","last_updated":"2026-04-20T12:40:57Z","snapshot_observed_at":"2026-08-18T20:12:49.676114Z","submitted_at":"2026-02-26T14:27:52Z","title":"Form factors of the $\\rho$ meson from effective field theory and the lattice","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2602.23044","snapshot_observed_at":"2026-07-31T09:15:14.019138Z","title":"Meißner, A","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.019138Z"},"links":{"cited_paper":"/paper/2602.23044","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:0e0c504bca8ca9968ff82cc7a3821db1d80e9a509757518439c66962f575e44a","observation_id":"7e1a62ad-7cf4-4fd1-b74d-48fa194776a4","resolution":{"observed_at":"2026-07-31T09:15:14.019138Z","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":"2026-07-31T09:15:14.024054Z","title":"Bulavaet al.(Baryon Scattering), Phys","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.024054Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:161700dcbd9a4a430f6af687c0fd4b5b676290cc813f80418ec7bf8ab9d9c9a4","observation_id":"0ea5430f-dea9-45f6-94c5-d002ed988529","resolution":{"observed_at":"2026-07-31T09:15:14.024054Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.11825","last_updated":"2021-01-05T18:56:36Z","snapshot_observed_at":"2026-08-18T20:14:59.264640Z","submitted_at":"2020-09-24T17:13:14Z","title":"Two-nucleon S-wave interactions at the $SU(3)$ flavor-symmetric point with $m_{ud}\\simeq m_s^{\\rm phys}$: a first lattice QCD calculation with the stochastic Laplacian Heaviside method","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.11825","snapshot_observed_at":"2026-07-31T09:15:14.028759Z","title":"H¨ orzet al., Phys","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.028759Z"},"links":{"cited_paper":"/paper/2009.11825","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:62a2a6ff471a83cc7cd8bcf4918b90e05b5b46a5915dfb5317b6df6897dc1fe7","observation_id":"d017a194-dd44-4fb4-868a-87c915a7ab29","resolution":{"observed_at":"2026-07-31T09:15:14.028759Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.10835","last_updated":"2024-10-01T16:28:07Z","snapshot_observed_at":"2026-08-20T17:58:13.149570Z","submitted_at":"2021-08-24T16:46:52Z","title":"A variational study of two-nucleon systems with lattice QCD","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.10835","snapshot_observed_at":"2026-07-31T09:15:14.033275Z","title":"Amarasinghe, R","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.033275Z"},"links":{"cited_paper":"/paper/2108.10835","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:595be143cd69a439eabe9a39c2c8044eb450ef01fb8e7b454db5184d41d37da1","observation_id":"2b71254a-6cd9-4869-ba02-797376f1a72e","resolution":{"observed_at":"2026-07-31T09:15:14.033275Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.12039","last_updated":"2024-10-01T14:11:55Z","snapshot_observed_at":"2026-08-18T20:14:14.441870Z","submitted_at":"2024-04-18T09:46:44Z","title":"Constraints on the finite volume two-nucleon spectrum at $m_\\pi \\approx 806$ MeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.12039","snapshot_observed_at":"2026-07-31T09:15:14.037898Z","title":"Detmold, M","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.037898Z"},"links":{"cited_paper":"/paper/2404.12039","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:f9eaf760bf9ba36d74c539e8683942b49c4b4774de60276287b11c96c94eee36","observation_id":"181aede3-5d7d-40ec-8ab0-0e2d0a2d5e06","resolution":{"observed_at":"2026-07-31T09:15:14.037898Z","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":"2026-07-31T09:15:14.042359Z","title":"qeFaSx5y5nmUhSDJgoCpOR9oLGI=","venue":null,"work_id":null,"year":1960},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.042359Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:39bed0efb9dd12e856f2ce7d94f43a564be99d8896a4a0d505ce41cf81c95800","observation_id":"bbe89501-f771-41ea-ab71-932c1b32ba43","resolution":{"observed_at":"2026-07-31T09:15:14.042359Z","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":"2026-07-31T09:15:14.047049Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.047049Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:4af6c97e573e8d20e39b2276d62250ce795233ffdbaf67b09e440541daf25a0b","observation_id":"d7470dbd-64a6-48ad-8e51-23c96a36bf38","resolution":{"observed_at":"2026-07-31T09:15:14.047049Z","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":"2026-07-31T09:15:14.052281Z","title":"Furthermore, we will assume that the current is a Lorentz scalar that does not introduce any angular dependence","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.052281Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:464ec41c892c8bc54f968e377d826c8b98933c731c613f7336a401fd08fcef54","observation_id":"b845a715-404b-4472-ad6e-950fcf121dee","resolution":{"observed_at":"2026-07-31T09:15:14.052281Z","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":"2026-07-31T09:15:14.057384Z","title":"That implies that the singularities in the scalar S-wave amplitude will in general also occur in other partial-wave projections and for currents with different Lorentz structures","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.057384Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:fcdc88a2692a710a8919a9552002954e8c4d5182d01e9b6a9d7534fa83762ef7","observation_id":"48b5667a-8d6a-4034-b477-78854b27dd32","resolution":{"observed_at":"2026-07-31T09:15:14.057384Z","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":"2026-07-31T09:15:14.062117Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.062117Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:01a3de418f03e24509e32b70e8939fc1d55c427ea099dfe33ec9292538b11eec","observation_id":"8e947d78-75ff-4743-ad46-4dfa2ce7d71a","resolution":{"observed_at":"2026-07-31T09:15:14.062117Z","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":"2026-07-31T09:15:14.066967Z","title":"Note that our integrands are periodic in Φ such that there is no end-point condition in this variable","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:14.066967Z"},"links":{"citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:d58c279d31618723dfc7bbff4ca0dcaa6a7b7b8ec579b471f4f6cfde2f4e8580","observation_id":"363ad362-985f-4874-b1fa-3ebee0e18ca1","resolution":{"observed_at":"2026-07-31T09:15:14.066967Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","latest_version":1,"primary_category":"hep-lat","snapshot_observed_at":"2026-08-18T22:20:18.666925Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts"},"reference_resolution":{"displayed":79,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":79,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":79},"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":"2026-08-23T06:30:58.430688+00:00","source":"crossref"},{"observed_at":"2026-08-23T06:30:53.778098+00:00","source":"retraction_watch"}],"thesis":"As of 23 August 2026, this Paper Citation Record lists 79 of 79 outbound references and 0 inbound Pith citation observations for arXiv:2607.24648."}