{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:IB22ZVH4JM5G5SKOCOMSQKOANJ","short_pith_number":"pith:IB22ZVH4","schema_version":"1.0","canonical_sha256":"4075acd4fc4b3a6ec94e13992829c06a5fac89937a84345c9348f567fdddce5d","source":{"kind":"arxiv","id":"2009.11825","version":2},"attestation_state":"computed","paper":{"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","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex","nucl-th"],"primary_cat":"hep-lat","authors_text":"Amy Nicholson, Andr\\'e Walker-Loud, Andrew Hanlon, Ben H\\\"orz, Chia Cheng Chang, Christopher K\\\"orber, Colin Morningstar, Dean Howarth, Enrico Rinaldi, Evan Berkowitz, John Bulava, M.A. Clark, Pavlos Vranas, Wayne Tai Lee","submitted_at":"2020-09-24T17:13:14Z","abstract_excerpt":"We report on the first application of the stochastic Laplacian Heaviside method for computing multi-particle interactions with lattice QCD to the two-nucleon system. Like the Laplacian Heaviside method, this method allows for the construction of interpolating operators which can be used to construct a positive definite set of two-nucleon correlation functions, unlike nearly all other applications of lattice QCD to two nucleons in the literature. It also allows for a variational analysis in which optimal linear combinations of the interpolating operators are formed that couple predominantly to "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2009.11825","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2020-09-24T17:13:14Z","cross_cats_sorted":["hep-ph","nucl-ex","nucl-th"],"title_canon_sha256":"10771571a83d3e0b791bcfa00689a18ac011eb1548922f1e307ca866682ee196","abstract_canon_sha256":"56d0b27018d939ea5e9ce89035995a3cd61a980fe165cc1a5e9964c7403087f7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:09:47.194325Z","signature_b64":"ksFzAh+tUguxtjVa1B94fABCeXAofQIfk1OrRPdXU0eBX/3yR/TacGXXKz2FuV1ECCN2n+oC0S9gd5YZnOLtDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4075acd4fc4b3a6ec94e13992829c06a5fac89937a84345c9348f567fdddce5d","last_reissued_at":"2026-07-05T02:09:47.193824Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:09:47.193824Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"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","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex","nucl-th"],"primary_cat":"hep-lat","authors_text":"Amy Nicholson, Andr\\'e Walker-Loud, Andrew Hanlon, Ben H\\\"orz, Chia Cheng Chang, Christopher K\\\"orber, Colin Morningstar, Dean Howarth, Enrico Rinaldi, Evan Berkowitz, John Bulava, M.A. Clark, Pavlos Vranas, Wayne Tai Lee","submitted_at":"2020-09-24T17:13:14Z","abstract_excerpt":"We report on the first application of the stochastic Laplacian Heaviside method for computing multi-particle interactions with lattice QCD to the two-nucleon system. Like the Laplacian Heaviside method, this method allows for the construction of interpolating operators which can be used to construct a positive definite set of two-nucleon correlation functions, unlike nearly all other applications of lattice QCD to two nucleons in the literature. It also allows for a variational analysis in which optimal linear combinations of the interpolating operators are formed that couple predominantly to "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2009.11825","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2009.11825/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2009.11825","created_at":"2026-07-05T02:09:47.193885+00:00"},{"alias_kind":"arxiv_version","alias_value":"2009.11825v2","created_at":"2026-07-05T02:09:47.193885+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2009.11825","created_at":"2026-07-05T02:09:47.193885+00:00"},{"alias_kind":"pith_short_12","alias_value":"IB22ZVH4JM5G","created_at":"2026-07-05T02:09:47.193885+00:00"},{"alias_kind":"pith_short_16","alias_value":"IB22ZVH4JM5G5SKO","created_at":"2026-07-05T02:09:47.193885+00:00"},{"alias_kind":"pith_short_8","alias_value":"IB22ZVH4","created_at":"2026-07-05T02:09:47.193885+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.16977","citing_title":"Two-nucleon systems at $m_{\\pi}\\approx292$ MeV from lattice QCD","ref_index":17,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IB22ZVH4JM5G5SKOCOMSQKOANJ","json":"https://pith.science/pith/IB22ZVH4JM5G5SKOCOMSQKOANJ.json","graph_json":"https://pith.science/api/pith-number/IB22ZVH4JM5G5SKOCOMSQKOANJ/graph.json","events_json":"https://pith.science/api/pith-number/IB22ZVH4JM5G5SKOCOMSQKOANJ/events.json","paper":"https://pith.science/paper/IB22ZVH4"},"agent_actions":{"view_html":"https://pith.science/pith/IB22ZVH4JM5G5SKOCOMSQKOANJ","download_json":"https://pith.science/pith/IB22ZVH4JM5G5SKOCOMSQKOANJ.json","view_paper":"https://pith.science/paper/IB22ZVH4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2009.11825&json=true","fetch_graph":"https://pith.science/api/pith-number/IB22ZVH4JM5G5SKOCOMSQKOANJ/graph.json","fetch_events":"https://pith.science/api/pith-number/IB22ZVH4JM5G5SKOCOMSQKOANJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IB22ZVH4JM5G5SKOCOMSQKOANJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IB22ZVH4JM5G5SKOCOMSQKOANJ/action/storage_attestation","attest_author":"https://pith.science/pith/IB22ZVH4JM5G5SKOCOMSQKOANJ/action/author_attestation","sign_citation":"https://pith.science/pith/IB22ZVH4JM5G5SKOCOMSQKOANJ/action/citation_signature","submit_replication":"https://pith.science/pith/IB22ZVH4JM5G5SKOCOMSQKOANJ/action/replication_record"}},"created_at":"2026-07-05T02:09:47.193885+00:00","updated_at":"2026-07-05T02:09:47.193885+00:00"}