{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:LMGDEZG4SSY22AQASGA3ZYZVAL","short_pith_number":"pith:LMGDEZG4","schema_version":"1.0","canonical_sha256":"5b0c3264dc94b1ad02009181bce33502fb5900c5e036083063431a8aee81fda5","source":{"kind":"arxiv","id":"0811.2762","version":2},"attestation_state":"computed","paper":{"title":"Effective string theory constraints on the long distance behavior of the subleading potentials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"Guillem Perez-Nadal, Joan Soto","submitted_at":"2008-11-17T17:40:25Z","abstract_excerpt":"The dynamics of heavy quarkonium systems in the strong coupling regime reduces to a quantum mechanical problem with a number of potentials which may be organized in powers of 1/m, m being the heavy quark mass. The potentials must be calculated non-perturbatively, for instance in lattice QCD. It is well known that the long distance behavior of the static (1/m^0) potential is well reproduced by an effective string theory. We show that this effective string theory, if correct, should also reproduce the long distance behavior of all 1/m suppressed potentials. We demonstrate the practical usefulnes"},"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":"0811.2762","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2008-11-17T17:40:25Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"76a86f05f9eda24e7ef9d351071fe702e541e2b695837bea938c4bd615d98fa2","abstract_canon_sha256":"4ff212432a524dd47a9cee6d1ec4658fb92ad72848e8ec13e0cf60158c7ccfe1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:27:21.188793Z","signature_b64":"Vp4PnFjpXAK8KUTJizRWeZlbIT7Jle8m51DweHfXOTKl/ZW/35jb7Gla/K94hufgEBD4vPABxdObVpx4Hf6JDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5b0c3264dc94b1ad02009181bce33502fb5900c5e036083063431a8aee81fda5","last_reissued_at":"2026-07-04T17:27:21.188408Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:27:21.188408Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effective string theory constraints on the long distance behavior of the subleading potentials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"Guillem Perez-Nadal, Joan Soto","submitted_at":"2008-11-17T17:40:25Z","abstract_excerpt":"The dynamics of heavy quarkonium systems in the strong coupling regime reduces to a quantum mechanical problem with a number of potentials which may be organized in powers of 1/m, m being the heavy quark mass. The potentials must be calculated non-perturbatively, for instance in lattice QCD. It is well known that the long distance behavior of the static (1/m^0) potential is well reproduced by an effective string theory. We show that this effective string theory, if correct, should also reproduce the long distance behavior of all 1/m suppressed potentials. We demonstrate the practical usefulnes"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0811.2762","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/0811.2762/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":"0811.2762","created_at":"2026-07-04T17:27:21.188466+00:00"},{"alias_kind":"arxiv_version","alias_value":"0811.2762v2","created_at":"2026-07-04T17:27:21.188466+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0811.2762","created_at":"2026-07-04T17:27:21.188466+00:00"},{"alias_kind":"pith_short_12","alias_value":"LMGDEZG4SSY2","created_at":"2026-07-04T17:27:21.188466+00:00"},{"alias_kind":"pith_short_16","alias_value":"LMGDEZG4SSY22AQA","created_at":"2026-07-04T17:27:21.188466+00:00"},{"alias_kind":"pith_short_8","alias_value":"LMGDEZG4","created_at":"2026-07-04T17:27:21.188466+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.05179","citing_title":"Spin Structure of heavy-quark hybrids","ref_index":10,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LMGDEZG4SSY22AQASGA3ZYZVAL","json":"https://pith.science/pith/LMGDEZG4SSY22AQASGA3ZYZVAL.json","graph_json":"https://pith.science/api/pith-number/LMGDEZG4SSY22AQASGA3ZYZVAL/graph.json","events_json":"https://pith.science/api/pith-number/LMGDEZG4SSY22AQASGA3ZYZVAL/events.json","paper":"https://pith.science/paper/LMGDEZG4"},"agent_actions":{"view_html":"https://pith.science/pith/LMGDEZG4SSY22AQASGA3ZYZVAL","download_json":"https://pith.science/pith/LMGDEZG4SSY22AQASGA3ZYZVAL.json","view_paper":"https://pith.science/paper/LMGDEZG4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0811.2762&json=true","fetch_graph":"https://pith.science/api/pith-number/LMGDEZG4SSY22AQASGA3ZYZVAL/graph.json","fetch_events":"https://pith.science/api/pith-number/LMGDEZG4SSY22AQASGA3ZYZVAL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LMGDEZG4SSY22AQASGA3ZYZVAL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LMGDEZG4SSY22AQASGA3ZYZVAL/action/storage_attestation","attest_author":"https://pith.science/pith/LMGDEZG4SSY22AQASGA3ZYZVAL/action/author_attestation","sign_citation":"https://pith.science/pith/LMGDEZG4SSY22AQASGA3ZYZVAL/action/citation_signature","submit_replication":"https://pith.science/pith/LMGDEZG4SSY22AQASGA3ZYZVAL/action/replication_record"}},"created_at":"2026-07-04T17:27:21.188466+00:00","updated_at":"2026-07-04T17:27:21.188466+00:00"}