{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:ZJE4HFAE6AT37OOGGSJPLG34DY","short_pith_number":"pith:ZJE4HFAE","schema_version":"1.0","canonical_sha256":"ca49c39404f027bfb9c63492f59b7c1e184ed7cde3fb1e4c769f02a972a83eda","source":{"kind":"arxiv","id":"nucl-th/9801034","version":2},"attestation_state":"computed","paper":{"title":"A New Expansion for Nucleon-Nucleon Interactions","license":"","headline":"","cross_cats":["cond-mat","hep-ph"],"primary_cat":"nucl-th","authors_text":"David B. Kaplan, Mark B. Wise, Martin J. Savage","submitted_at":"1998-01-19T18:54:19Z","abstract_excerpt":"We introduce a new and well defined power counting for the effective field theory describing nucleon-nucleon interactions. Because of the large NN scattering lengths it differs from other applications of chiral perturbation theory and is facilitated by introducing an unusual subtraction scheme and renormalization group analysis. Calculation to subleading order in the expansion can be done analytically, and we present the results for both the 1S0 and 3S1-3D1 channels."},"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":"nucl-th/9801034","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1998-01-19T18:54:19Z","cross_cats_sorted":["cond-mat","hep-ph"],"title_canon_sha256":"2ee265cec6e9272d7df94405aaf4bf92aa9cc5ae19c343af8af6b2c25a65cffd","abstract_canon_sha256":"f9a81b88a011d95af1931e4ba0df971f2e3b9136efcf5422f30d3dea112860f0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:10:12.900978Z","signature_b64":"PLdN41EALTrHB1l/I1UmOcSoxOp9pKH7vrgtEx9vtLmk33tsKar8zXaSedtEuNrZ8y2BRyzcHghRvcNfDirlAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ca49c39404f027bfb9c63492f59b7c1e184ed7cde3fb1e4c769f02a972a83eda","last_reissued_at":"2026-07-04T16:10:12.900610Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:10:12.900610Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A New Expansion for Nucleon-Nucleon Interactions","license":"","headline":"","cross_cats":["cond-mat","hep-ph"],"primary_cat":"nucl-th","authors_text":"David B. Kaplan, Mark B. Wise, Martin J. Savage","submitted_at":"1998-01-19T18:54:19Z","abstract_excerpt":"We introduce a new and well defined power counting for the effective field theory describing nucleon-nucleon interactions. Because of the large NN scattering lengths it differs from other applications of chiral perturbation theory and is facilitated by introducing an unusual subtraction scheme and renormalization group analysis. Calculation to subleading order in the expansion can be done analytically, and we present the results for both the 1S0 and 3S1-3D1 channels."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9801034","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/nucl-th/9801034/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":"nucl-th/9801034","created_at":"2026-07-04T16:10:12.900664+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9801034v2","created_at":"2026-07-04T16:10:12.900664+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9801034","created_at":"2026-07-04T16:10:12.900664+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZJE4HFAE6AT3","created_at":"2026-07-04T16:10:12.900664+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZJE4HFAE6AT37OOG","created_at":"2026-07-04T16:10:12.900664+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZJE4HFAE","created_at":"2026-07-04T16:10:12.900664+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":15,"internal_anchor_count":11,"sample":[{"citing_arxiv_id":"2606.21547","citing_title":"A short-range effective theory for single-neutron halo nuclei with a deformed core","ref_index":15,"is_internal_anchor":true},{"citing_arxiv_id":"2607.01443","citing_title":"The theory of electric dipole moments: the view from below","ref_index":163,"is_internal_anchor":true},{"citing_arxiv_id":"2606.17148","citing_title":"Quantum Resources and Wigner Symmetry in Nucleon-Nucleon Scattering from Effective Field Theory","ref_index":8,"is_internal_anchor":true},{"citing_arxiv_id":"2606.10128","citing_title":"Determining universal spectra from probability distributions","ref_index":19,"is_internal_anchor":true},{"citing_arxiv_id":"2606.29539","citing_title":"Observables in Schr\\\"odinger CFTs: How Aliens Built the Pyramids","ref_index":19,"is_internal_anchor":true},{"citing_arxiv_id":"2605.22134","citing_title":"Bootstrapping Two-Nucleon Effective Field Theories","ref_index":7,"is_internal_anchor":true},{"citing_arxiv_id":"2605.19062","citing_title":"Coulomb Corrections to Three-Nucleon Moments","ref_index":49,"is_internal_anchor":true},{"citing_arxiv_id":"2511.22590","citing_title":"Short-range production of three bottom mesons","ref_index":38,"is_internal_anchor":true},{"citing_arxiv_id":"2512.14117","citing_title":"Scrutiny of the new class of three-nucleon forces","ref_index":30,"is_internal_anchor":true},{"citing_arxiv_id":"2603.01561","citing_title":"Auxiliary counterterms and their role in effective field theory","ref_index":16,"is_internal_anchor":true},{"citing_arxiv_id":"2603.28842","citing_title":"Dimer Effective Field Theory","ref_index":11,"is_internal_anchor":true},{"citing_arxiv_id":"2604.26207","citing_title":"Functional Dimensional Regularization for O(N) Models","ref_index":6,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25221","citing_title":"Coulomb Effects and Wigner-SU(4) Symmetry in He-3 Charge and Magnetic Properties","ref_index":56,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25103","citing_title":"Rethinking Dimensional Regularization in Critical Phenomena","ref_index":21,"is_internal_anchor":false},{"citing_arxiv_id":"2604.23526","citing_title":"Smooth Threshold Effects from Dimensional Regularization","ref_index":33,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZJE4HFAE6AT37OOGGSJPLG34DY","json":"https://pith.science/pith/ZJE4HFAE6AT37OOGGSJPLG34DY.json","graph_json":"https://pith.science/api/pith-number/ZJE4HFAE6AT37OOGGSJPLG34DY/graph.json","events_json":"https://pith.science/api/pith-number/ZJE4HFAE6AT37OOGGSJPLG34DY/events.json","paper":"https://pith.science/paper/ZJE4HFAE"},"agent_actions":{"view_html":"https://pith.science/pith/ZJE4HFAE6AT37OOGGSJPLG34DY","download_json":"https://pith.science/pith/ZJE4HFAE6AT37OOGGSJPLG34DY.json","view_paper":"https://pith.science/paper/ZJE4HFAE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/9801034&json=true","fetch_graph":"https://pith.science/api/pith-number/ZJE4HFAE6AT37OOGGSJPLG34DY/graph.json","fetch_events":"https://pith.science/api/pith-number/ZJE4HFAE6AT37OOGGSJPLG34DY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZJE4HFAE6AT37OOGGSJPLG34DY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZJE4HFAE6AT37OOGGSJPLG34DY/action/storage_attestation","attest_author":"https://pith.science/pith/ZJE4HFAE6AT37OOGGSJPLG34DY/action/author_attestation","sign_citation":"https://pith.science/pith/ZJE4HFAE6AT37OOGGSJPLG34DY/action/citation_signature","submit_replication":"https://pith.science/pith/ZJE4HFAE6AT37OOGGSJPLG34DY/action/replication_record"}},"created_at":"2026-07-04T16:10:12.900664+00:00","updated_at":"2026-07-04T16:10:12.900664+00:00"}