{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:UUGGCVH2Z4VMOZW4KY2GGSSMMU","short_pith_number":"pith:UUGGCVH2","schema_version":"1.0","canonical_sha256":"a50c6154facf2ac766dc5634634a4c65255130c9a12ead2fc155df6c2d526f99","source":{"kind":"arxiv","id":"1406.0454","version":2},"attestation_state":"computed","paper":{"title":"Local chiral effective field theory interactions and quantum Monte Carlo applications","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Gezerlis, A. Nogga, A. Schwenk, E. Epelbaum, I. Tews, K. Hebeler, M. Freunek, S. Gandolfi","submitted_at":"2014-06-02T17:44:27Z","abstract_excerpt":"We present details of the derivation of local chiral effective field theory interactions to next-to-next-to-leading order, and show results for nucleon-nucleon phase shifts and deuteron properties for these potentials. We then perform systematic auxiliary-field diffusion Monte Carlo calculations for neutron matter based on the developed local chiral potentials at different orders. This includes studies of the effects of the spectral-function regularization and of the local regulators. For all orders, we compare the quantum Monte Carlo results with perturbative many-body calculations and find e"},"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":"1406.0454","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-06-02T17:44:27Z","cross_cats_sorted":["cond-mat.quant-gas","hep-ph","nucl-ex"],"title_canon_sha256":"1a349a44cd592417de09cdf68e0d014229747f43181829e5bd115615fc349ab8","abstract_canon_sha256":"70ec502d58ac6299a66fa3c5de6726f7e28f4cc6194d3181c5668ba9e62483ee"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:32:46.029147Z","signature_b64":"XQ6M0iHviTYlK1L24LxitdXTg/vTP6SC0clkaESJrnEzcIDkFMNbtAzk2rPaa1n1dtKrjyzf0DGGW8wWBdpyAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a50c6154facf2ac766dc5634634a4c65255130c9a12ead2fc155df6c2d526f99","last_reissued_at":"2026-05-18T02:32:46.028740Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:32:46.028740Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Local chiral effective field theory interactions and quantum Monte Carlo applications","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Gezerlis, A. Nogga, A. Schwenk, E. Epelbaum, I. Tews, K. Hebeler, M. Freunek, S. Gandolfi","submitted_at":"2014-06-02T17:44:27Z","abstract_excerpt":"We present details of the derivation of local chiral effective field theory interactions to next-to-next-to-leading order, and show results for nucleon-nucleon phase shifts and deuteron properties for these potentials. We then perform systematic auxiliary-field diffusion Monte Carlo calculations for neutron matter based on the developed local chiral potentials at different orders. This includes studies of the effects of the spectral-function regularization and of the local regulators. For all orders, we compare the quantum Monte Carlo results with perturbative many-body calculations and find e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.0454","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":""},"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":"1406.0454","created_at":"2026-05-18T02:32:46.028798+00:00"},{"alias_kind":"arxiv_version","alias_value":"1406.0454v2","created_at":"2026-05-18T02:32:46.028798+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.0454","created_at":"2026-05-18T02:32:46.028798+00:00"},{"alias_kind":"pith_short_12","alias_value":"UUGGCVH2Z4VM","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_16","alias_value":"UUGGCVH2Z4VMOZW4","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_8","alias_value":"UUGGCVH2","created_at":"2026-05-18T12:28:52.271510+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2512.14117","citing_title":"Scrutiny of the new class of three-nucleon forces","ref_index":91,"is_internal_anchor":true},{"citing_arxiv_id":"2603.01561","citing_title":"Auxiliary counterterms and their role in effective field theory","ref_index":50,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UUGGCVH2Z4VMOZW4KY2GGSSMMU","json":"https://pith.science/pith/UUGGCVH2Z4VMOZW4KY2GGSSMMU.json","graph_json":"https://pith.science/api/pith-number/UUGGCVH2Z4VMOZW4KY2GGSSMMU/graph.json","events_json":"https://pith.science/api/pith-number/UUGGCVH2Z4VMOZW4KY2GGSSMMU/events.json","paper":"https://pith.science/paper/UUGGCVH2"},"agent_actions":{"view_html":"https://pith.science/pith/UUGGCVH2Z4VMOZW4KY2GGSSMMU","download_json":"https://pith.science/pith/UUGGCVH2Z4VMOZW4KY2GGSSMMU.json","view_paper":"https://pith.science/paper/UUGGCVH2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1406.0454&json=true","fetch_graph":"https://pith.science/api/pith-number/UUGGCVH2Z4VMOZW4KY2GGSSMMU/graph.json","fetch_events":"https://pith.science/api/pith-number/UUGGCVH2Z4VMOZW4KY2GGSSMMU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UUGGCVH2Z4VMOZW4KY2GGSSMMU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UUGGCVH2Z4VMOZW4KY2GGSSMMU/action/storage_attestation","attest_author":"https://pith.science/pith/UUGGCVH2Z4VMOZW4KY2GGSSMMU/action/author_attestation","sign_citation":"https://pith.science/pith/UUGGCVH2Z4VMOZW4KY2GGSSMMU/action/citation_signature","submit_replication":"https://pith.science/pith/UUGGCVH2Z4VMOZW4KY2GGSSMMU/action/replication_record"}},"created_at":"2026-05-18T02:32:46.028798+00:00","updated_at":"2026-05-18T02:32:46.028798+00:00"}