{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:X4BNJT5Q5ZC6TOVSFSW23AOT4U","short_pith_number":"pith:X4BNJT5Q","schema_version":"1.0","canonical_sha256":"bf02d4cfb0ee45e9bab22cadad81d3e527e39c2393c30c68e2b5dde312a4caf2","source":{"kind":"arxiv","id":"1706.07668","version":2},"attestation_state":"computed","paper":{"title":"Quantum Monte Carlo calculations of light nuclei with local chiral two- and three-nucleon interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Gezerlis, A. Schwenk, I. Tews, J. Carlson, J. E. Lynn, K. E. Schmidt, S. Gandolfi","submitted_at":"2017-06-23T12:29:38Z","abstract_excerpt":"Local chiral effective field theory interactions have recently been developed and used in the context of quantum Monte Carlo few- and many-body methods for nuclear physics. In this work, we go over detailed features of local chiral nucleon-nucleon interactions and examine their effect on properties of the deuteron, paying special attention to the perturbativeness of the expansion. We then turn to three-nucleon interactions, focusing on operator ambiguities and their interplay with regulator effects. We then discuss the nuclear Green's function Monte Carlo method, going over both wave-function "},"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":"1706.07668","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-06-23T12:29:38Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"36d82287a3fa7306079dcabaf9a73edc0c3e375ea3981e538e173f33c3860629","abstract_canon_sha256":"eb81c2479e3ef26c1d9aa1b1b924397e56a1b64fac90872426ae82997933a9bc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:28:40.709903Z","signature_b64":"kJgh+tnZRTk3URrP5VoyWgwiA8ZWF00OuPO8rZlXeDUt1cXCxbgM1n54m9oqd1t08C+7/hBOeEz9xmwKWD04Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bf02d4cfb0ee45e9bab22cadad81d3e527e39c2393c30c68e2b5dde312a4caf2","last_reissued_at":"2026-05-18T00:28:40.709239Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:28:40.709239Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum Monte Carlo calculations of light nuclei with local chiral two- and three-nucleon interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Gezerlis, A. Schwenk, I. Tews, J. Carlson, J. E. Lynn, K. E. Schmidt, S. Gandolfi","submitted_at":"2017-06-23T12:29:38Z","abstract_excerpt":"Local chiral effective field theory interactions have recently been developed and used in the context of quantum Monte Carlo few- and many-body methods for nuclear physics. In this work, we go over detailed features of local chiral nucleon-nucleon interactions and examine their effect on properties of the deuteron, paying special attention to the perturbativeness of the expansion. We then turn to three-nucleon interactions, focusing on operator ambiguities and their interplay with regulator effects. We then discuss the nuclear Green's function Monte Carlo method, going over both wave-function "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.07668","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":"1706.07668","created_at":"2026-05-18T00:28:40.709354+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.07668v2","created_at":"2026-05-18T00:28:40.709354+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.07668","created_at":"2026-05-18T00:28:40.709354+00:00"},{"alias_kind":"pith_short_12","alias_value":"X4BNJT5Q5ZC6","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_16","alias_value":"X4BNJT5Q5ZC6TOVS","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_8","alias_value":"X4BNJT5Q","created_at":"2026-05-18T12:31:53.515858+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.26926","citing_title":"Challenging chiral EFT with tritium beta decay","ref_index":81,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/X4BNJT5Q5ZC6TOVSFSW23AOT4U","json":"https://pith.science/pith/X4BNJT5Q5ZC6TOVSFSW23AOT4U.json","graph_json":"https://pith.science/api/pith-number/X4BNJT5Q5ZC6TOVSFSW23AOT4U/graph.json","events_json":"https://pith.science/api/pith-number/X4BNJT5Q5ZC6TOVSFSW23AOT4U/events.json","paper":"https://pith.science/paper/X4BNJT5Q"},"agent_actions":{"view_html":"https://pith.science/pith/X4BNJT5Q5ZC6TOVSFSW23AOT4U","download_json":"https://pith.science/pith/X4BNJT5Q5ZC6TOVSFSW23AOT4U.json","view_paper":"https://pith.science/paper/X4BNJT5Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.07668&json=true","fetch_graph":"https://pith.science/api/pith-number/X4BNJT5Q5ZC6TOVSFSW23AOT4U/graph.json","fetch_events":"https://pith.science/api/pith-number/X4BNJT5Q5ZC6TOVSFSW23AOT4U/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X4BNJT5Q5ZC6TOVSFSW23AOT4U/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X4BNJT5Q5ZC6TOVSFSW23AOT4U/action/storage_attestation","attest_author":"https://pith.science/pith/X4BNJT5Q5ZC6TOVSFSW23AOT4U/action/author_attestation","sign_citation":"https://pith.science/pith/X4BNJT5Q5ZC6TOVSFSW23AOT4U/action/citation_signature","submit_replication":"https://pith.science/pith/X4BNJT5Q5ZC6TOVSFSW23AOT4U/action/replication_record"}},"created_at":"2026-05-18T00:28:40.709354+00:00","updated_at":"2026-05-18T00:28:40.709354+00:00"}