{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:IAT22GALLCGIZJA4RADQSW64WN","short_pith_number":"pith:IAT22GAL","schema_version":"1.0","canonical_sha256":"4027ad180b588c8ca41c8807095bdcb34546c58d2a626822bcfb6cd06621fe3c","source":{"kind":"arxiv","id":"1810.02646","version":1},"attestation_state":"computed","paper":{"title":"How (not) to renormalize integral equations with singular potentials in effective field theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"nucl-th","authors_text":"A. M. Gasparyan, E. Epelbaum, J. Gegelia, Ulf-G. Mei{\\ss}ner","submitted_at":"2018-10-05T12:28:38Z","abstract_excerpt":"We discuss the connection between the perturbative and non-perturbative renormalization and related conceptual issues in the few-nucleon sector of the low-energy effective field theory of the strong interactions. General arguments are supported by examples from effective theories with and without pions as dynamical degrees of freedom. A quantum mechanical potential with explicitly specified short- and long-range parts is considered as an \"underlying fundamental theory\" and the corresponding effective field theory potential is constructed. Further, the problem of the effective field theoretical"},"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":"1810.02646","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-10-05T12:28:38Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"e4910eb2d5b7a1c0b5844edfa58d3a10ce0cb3c9cc2bbae64662fd233c95ab6d","abstract_canon_sha256":"401290eca8484ae56aafebf0eefcb899737cbef38ea2192cc0c9048f7788f42e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:00:47.566459Z","signature_b64":"btEGocG/NPBBzMYes6v+z/qi6IB7Rx0Rd1JToXgZ3D4hA1KefU/1RwKwWdoB1X8ZCpjsan93HKL60WbKTLNeAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4027ad180b588c8ca41c8807095bdcb34546c58d2a626822bcfb6cd06621fe3c","last_reissued_at":"2026-05-18T00:00:47.565848Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:00:47.565848Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"How (not) to renormalize integral equations with singular potentials in effective field theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"nucl-th","authors_text":"A. M. Gasparyan, E. Epelbaum, J. Gegelia, Ulf-G. Mei{\\ss}ner","submitted_at":"2018-10-05T12:28:38Z","abstract_excerpt":"We discuss the connection between the perturbative and non-perturbative renormalization and related conceptual issues in the few-nucleon sector of the low-energy effective field theory of the strong interactions. General arguments are supported by examples from effective theories with and without pions as dynamical degrees of freedom. A quantum mechanical potential with explicitly specified short- and long-range parts is considered as an \"underlying fundamental theory\" and the corresponding effective field theory potential is constructed. Further, the problem of the effective field theoretical"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.02646","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1810.02646","created_at":"2026-05-18T00:00:47.565946+00:00"},{"alias_kind":"arxiv_version","alias_value":"1810.02646v1","created_at":"2026-05-18T00:00:47.565946+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.02646","created_at":"2026-05-18T00:00:47.565946+00:00"},{"alias_kind":"pith_short_12","alias_value":"IAT22GALLCGI","created_at":"2026-05-18T12:32:28.185984+00:00"},{"alias_kind":"pith_short_16","alias_value":"IAT22GALLCGIZJA4","created_at":"2026-05-18T12:32:28.185984+00:00"},{"alias_kind":"pith_short_8","alias_value":"IAT22GAL","created_at":"2026-05-18T12:32:28.185984+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2605.22134","citing_title":"Bootstrapping Two-Nucleon Effective Field Theories","ref_index":23,"is_internal_anchor":true},{"citing_arxiv_id":"2512.14117","citing_title":"Scrutiny of the new class of three-nucleon forces","ref_index":56,"is_internal_anchor":true},{"citing_arxiv_id":"2603.01561","citing_title":"Auxiliary counterterms and their role in effective field theory","ref_index":21,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IAT22GALLCGIZJA4RADQSW64WN","json":"https://pith.science/pith/IAT22GALLCGIZJA4RADQSW64WN.json","graph_json":"https://pith.science/api/pith-number/IAT22GALLCGIZJA4RADQSW64WN/graph.json","events_json":"https://pith.science/api/pith-number/IAT22GALLCGIZJA4RADQSW64WN/events.json","paper":"https://pith.science/paper/IAT22GAL"},"agent_actions":{"view_html":"https://pith.science/pith/IAT22GALLCGIZJA4RADQSW64WN","download_json":"https://pith.science/pith/IAT22GALLCGIZJA4RADQSW64WN.json","view_paper":"https://pith.science/paper/IAT22GAL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1810.02646&json=true","fetch_graph":"https://pith.science/api/pith-number/IAT22GALLCGIZJA4RADQSW64WN/graph.json","fetch_events":"https://pith.science/api/pith-number/IAT22GALLCGIZJA4RADQSW64WN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IAT22GALLCGIZJA4RADQSW64WN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IAT22GALLCGIZJA4RADQSW64WN/action/storage_attestation","attest_author":"https://pith.science/pith/IAT22GALLCGIZJA4RADQSW64WN/action/author_attestation","sign_citation":"https://pith.science/pith/IAT22GALLCGIZJA4RADQSW64WN/action/citation_signature","submit_replication":"https://pith.science/pith/IAT22GALLCGIZJA4RADQSW64WN/action/replication_record"}},"created_at":"2026-05-18T00:00:47.565946+00:00","updated_at":"2026-05-18T00:00:47.565946+00:00"}