{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:MOE53Q6IPVSCXVZ3EF4FWCTR5C","short_pith_number":"pith:MOE53Q6I","schema_version":"1.0","canonical_sha256":"6389ddc3c87d642bd73b21785b0a71e8bfba90edd89ace01ad8ad4ba5b752c8f","source":{"kind":"arxiv","id":"1606.06335","version":1},"attestation_state":"computed","paper":{"title":"Local chiral potentials and the structure of light nuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Alejandro Kievsky, Alessandro Lovato, Laura E. Marcucci, Luca Girlanda, Maria Piarulli, Michele Viviani, Robert B. Wiringa, Rocco Schiavilla, Steven C. Pieper","submitted_at":"2016-06-20T21:08:57Z","abstract_excerpt":"We present fully local versions of the minimally non-local nucleon-nucleon potentials constructed in a previous paper [M.\\ Piarulli {\\it et al.}, Phys.\\ Rev.\\ C {\\bf 91}, 024003 (2015)], and use them in hypersperical-harmonics and quantum Monte Carlo calculations of ground and excited states of $^3$H, $^3$He, $^4$He, $^6$He, and $^6$Li nuclei. The long-range part of these local potentials includes one- and two-pion exchange contributions without and with $\\Delta$-isobars in the intermediate states up to order $Q^3$ ($Q$ denotes generically the low momentum scale) in the chiral expansion, while"},"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":"1606.06335","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-06-20T21:08:57Z","cross_cats_sorted":[],"title_canon_sha256":"e101aa2ea2dccc56bec8ca1e2850cb5e857a50a7870a8b4918a0d00ac417e74f","abstract_canon_sha256":"c7936d90cea302f927f6ecbf489ec93f78521d051d3e792e7ee5bd75aecf2e7f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:55:46.232499Z","signature_b64":"Vkc9J5BpMymLcArKanDhO34pj+V5Sd5McKBzRGyyTLEwFvX/BYv/OT0PMo9S4jvUZnXVJ23VUR2lyYsYxXs5AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6389ddc3c87d642bd73b21785b0a71e8bfba90edd89ace01ad8ad4ba5b752c8f","last_reissued_at":"2026-05-18T00:55:46.232041Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:55:46.232041Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Local chiral potentials and the structure of light nuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Alejandro Kievsky, Alessandro Lovato, Laura E. Marcucci, Luca Girlanda, Maria Piarulli, Michele Viviani, Robert B. Wiringa, Rocco Schiavilla, Steven C. Pieper","submitted_at":"2016-06-20T21:08:57Z","abstract_excerpt":"We present fully local versions of the minimally non-local nucleon-nucleon potentials constructed in a previous paper [M.\\ Piarulli {\\it et al.}, Phys.\\ Rev.\\ C {\\bf 91}, 024003 (2015)], and use them in hypersperical-harmonics and quantum Monte Carlo calculations of ground and excited states of $^3$H, $^3$He, $^4$He, $^6$He, and $^6$Li nuclei. The long-range part of these local potentials includes one- and two-pion exchange contributions without and with $\\Delta$-isobars in the intermediate states up to order $Q^3$ ($Q$ denotes generically the low momentum scale) in the chiral expansion, while"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.06335","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":"1606.06335","created_at":"2026-05-18T00:55:46.232106+00:00"},{"alias_kind":"arxiv_version","alias_value":"1606.06335v1","created_at":"2026-05-18T00:55:46.232106+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.06335","created_at":"2026-05-18T00:55:46.232106+00:00"},{"alias_kind":"pith_short_12","alias_value":"MOE53Q6IPVSC","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_16","alias_value":"MOE53Q6IPVSCXVZ3","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_8","alias_value":"MOE53Q6I","created_at":"2026-05-18T12:30:32.724797+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.14006","citing_title":"Quantum Monte Carlo calculation of $\\delta_C$ in the superallowed beta decay of $^{10}$C","ref_index":27,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MOE53Q6IPVSCXVZ3EF4FWCTR5C","json":"https://pith.science/pith/MOE53Q6IPVSCXVZ3EF4FWCTR5C.json","graph_json":"https://pith.science/api/pith-number/MOE53Q6IPVSCXVZ3EF4FWCTR5C/graph.json","events_json":"https://pith.science/api/pith-number/MOE53Q6IPVSCXVZ3EF4FWCTR5C/events.json","paper":"https://pith.science/paper/MOE53Q6I"},"agent_actions":{"view_html":"https://pith.science/pith/MOE53Q6IPVSCXVZ3EF4FWCTR5C","download_json":"https://pith.science/pith/MOE53Q6IPVSCXVZ3EF4FWCTR5C.json","view_paper":"https://pith.science/paper/MOE53Q6I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1606.06335&json=true","fetch_graph":"https://pith.science/api/pith-number/MOE53Q6IPVSCXVZ3EF4FWCTR5C/graph.json","fetch_events":"https://pith.science/api/pith-number/MOE53Q6IPVSCXVZ3EF4FWCTR5C/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MOE53Q6IPVSCXVZ3EF4FWCTR5C/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MOE53Q6IPVSCXVZ3EF4FWCTR5C/action/storage_attestation","attest_author":"https://pith.science/pith/MOE53Q6IPVSCXVZ3EF4FWCTR5C/action/author_attestation","sign_citation":"https://pith.science/pith/MOE53Q6IPVSCXVZ3EF4FWCTR5C/action/citation_signature","submit_replication":"https://pith.science/pith/MOE53Q6IPVSCXVZ3EF4FWCTR5C/action/replication_record"}},"created_at":"2026-05-18T00:55:46.232106+00:00","updated_at":"2026-05-18T00:55:46.232106+00:00"}