{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:6X44SB3K2AXP7Q4FLJ3HDEIWK5","short_pith_number":"pith:6X44SB3K","schema_version":"1.0","canonical_sha256":"f5f9c9076ad02effc3855a7671911657559ebacb10b2132c0f7cfb6ef685c42a","source":{"kind":"arxiv","id":"2005.00552","version":4},"attestation_state":"computed","paper":{"title":"Nonrelativistic effective field theory for heavy exotic hadrons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Jaume Tarr\\'us Castell\\`a, Joan Soto","submitted_at":"2020-05-01T18:02:07Z","abstract_excerpt":"We propose an effective field theory to describe hadrons with two heavy quarks without any assumption on the typical distance between the heavy quarks with respect to the typical hadronic scale. The construction is based on Non-Relativistic QCD and inspired in the strong coupling regime of Potential Non-Relativistic QCD. We construct the effective theory at leading and next-to-leading order in the inverse heavy-quark mass expansion for arbitrary quantum numbers of the light degrees of freedom. Hence our results hold for hybrids, tetraquarks, double heavy baryons and pentaquarks, for which we a"},"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":"2005.00552","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-05-01T18:02:07Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"ab01c7348574c1076cc5c85313400c9547e6ea81e8c908ca16cb123142415189","abstract_canon_sha256":"80456574c9227dfd04264ee8f80dfaa1088deafa2c11d1cc4e55dcd3e533c4f5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:32:37.769002Z","signature_b64":"19WjrXXsotQiRVCFdTYY/WBCkUyhxfd9tIlFMJyOgvGCWRejvC8a9a/Df5fPJOWnplZTpMYTv/OknYGMeV7KBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f5f9c9076ad02effc3855a7671911657559ebacb10b2132c0f7cfb6ef685c42a","last_reissued_at":"2026-07-05T09:32:37.768464Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:32:37.768464Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonrelativistic effective field theory for heavy exotic hadrons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Jaume Tarr\\'us Castell\\`a, Joan Soto","submitted_at":"2020-05-01T18:02:07Z","abstract_excerpt":"We propose an effective field theory to describe hadrons with two heavy quarks without any assumption on the typical distance between the heavy quarks with respect to the typical hadronic scale. The construction is based on Non-Relativistic QCD and inspired in the strong coupling regime of Potential Non-Relativistic QCD. We construct the effective theory at leading and next-to-leading order in the inverse heavy-quark mass expansion for arbitrary quantum numbers of the light degrees of freedom. Hence our results hold for hybrids, tetraquarks, double heavy baryons and pentaquarks, for which we a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2005.00552","kind":"arxiv","version":4},"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/2005.00552/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":"2005.00552","created_at":"2026-07-05T09:32:37.768518+00:00"},{"alias_kind":"arxiv_version","alias_value":"2005.00552v4","created_at":"2026-07-05T09:32:37.768518+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2005.00552","created_at":"2026-07-05T09:32:37.768518+00:00"},{"alias_kind":"pith_short_12","alias_value":"6X44SB3K2AXP","created_at":"2026-07-05T09:32:37.768518+00:00"},{"alias_kind":"pith_short_16","alias_value":"6X44SB3K2AXP7Q4F","created_at":"2026-07-05T09:32:37.768518+00:00"},{"alias_kind":"pith_short_8","alias_value":"6X44SB3K","created_at":"2026-07-05T09:32:37.768518+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.12309","citing_title":"$\\boldsymbol{\\chi_{c1}}(3872)$ and its Partners in the Diabatic Born-Oppenheimer Approximation for QCD","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2602.02436","citing_title":"Wilson loops with neural networks","ref_index":20,"is_internal_anchor":false},{"citing_arxiv_id":"2604.12603","citing_title":"Open-flavor threshold effects on quarkonium spectrum in the BOEFT","ref_index":95,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6X44SB3K2AXP7Q4FLJ3HDEIWK5","json":"https://pith.science/pith/6X44SB3K2AXP7Q4FLJ3HDEIWK5.json","graph_json":"https://pith.science/api/pith-number/6X44SB3K2AXP7Q4FLJ3HDEIWK5/graph.json","events_json":"https://pith.science/api/pith-number/6X44SB3K2AXP7Q4FLJ3HDEIWK5/events.json","paper":"https://pith.science/paper/6X44SB3K"},"agent_actions":{"view_html":"https://pith.science/pith/6X44SB3K2AXP7Q4FLJ3HDEIWK5","download_json":"https://pith.science/pith/6X44SB3K2AXP7Q4FLJ3HDEIWK5.json","view_paper":"https://pith.science/paper/6X44SB3K","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2005.00552&json=true","fetch_graph":"https://pith.science/api/pith-number/6X44SB3K2AXP7Q4FLJ3HDEIWK5/graph.json","fetch_events":"https://pith.science/api/pith-number/6X44SB3K2AXP7Q4FLJ3HDEIWK5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6X44SB3K2AXP7Q4FLJ3HDEIWK5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6X44SB3K2AXP7Q4FLJ3HDEIWK5/action/storage_attestation","attest_author":"https://pith.science/pith/6X44SB3K2AXP7Q4FLJ3HDEIWK5/action/author_attestation","sign_citation":"https://pith.science/pith/6X44SB3K2AXP7Q4FLJ3HDEIWK5/action/citation_signature","submit_replication":"https://pith.science/pith/6X44SB3K2AXP7Q4FLJ3HDEIWK5/action/replication_record"}},"created_at":"2026-07-05T09:32:37.768518+00:00","updated_at":"2026-07-05T09:32:37.768518+00:00"}