{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:JDZFN3U6AFGGL7XPBNZMYELCG7","short_pith_number":"pith:JDZFN3U6","schema_version":"1.0","canonical_sha256":"48f256ee9e014c65feef0b72cc116237ff5bceb270e3abb0609ead29f17f51dd","source":{"kind":"arxiv","id":"1705.05511","version":2},"attestation_state":"computed","paper":{"title":"Ab initio electromagnetic observables with the in-medium similarity renormalization group","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"H. Hergert, N. M. Parzuchowski, P. Navr\\'atil, S. K. Bogner, S. R. Stroberg","submitted_at":"2017-05-16T03:04:25Z","abstract_excerpt":"We present the formalism for consistently transforming transition operators within the in-medium similarity renormalization group framework. We implement the operator transformation in both the equations-of-motion and valence-space variants, and present first results for electromagnetic transitions and moments in medium-mass nuclei using consistently-evolved operators, including the induced two-body parts. These results are compared to experimental values, and--where possible--the results of no-core shell model calculations using the same input chiral interaction. We find good agreement betwee"},"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":"1705.05511","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-05-16T03:04:25Z","cross_cats_sorted":[],"title_canon_sha256":"818875b617f09f71a5f7194c139fe153958f630431593c0ab3495a058e08322c","abstract_canon_sha256":"34de0e38a99761e005a20f5bd376b109e669132c665030a67b6b914bdf32271a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:49.831665Z","signature_b64":"DhfBASzcehOqzK7WNph1CTAQT9h4oThAoD1Gf3YRPwB20Jsn9uOsfpCKRhRH6/Odya8Ue8LAlqEawLlWTiyhAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"48f256ee9e014c65feef0b72cc116237ff5bceb270e3abb0609ead29f17f51dd","last_reissued_at":"2026-05-18T00:33:49.831117Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:49.831117Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Ab initio electromagnetic observables with the in-medium similarity renormalization group","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"H. Hergert, N. M. Parzuchowski, P. Navr\\'atil, S. K. Bogner, S. R. Stroberg","submitted_at":"2017-05-16T03:04:25Z","abstract_excerpt":"We present the formalism for consistently transforming transition operators within the in-medium similarity renormalization group framework. We implement the operator transformation in both the equations-of-motion and valence-space variants, and present first results for electromagnetic transitions and moments in medium-mass nuclei using consistently-evolved operators, including the induced two-body parts. These results are compared to experimental values, and--where possible--the results of no-core shell model calculations using the same input chiral interaction. We find good agreement betwee"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.05511","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":"1705.05511","created_at":"2026-05-18T00:33:49.831199+00:00"},{"alias_kind":"arxiv_version","alias_value":"1705.05511v2","created_at":"2026-05-18T00:33:49.831199+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.05511","created_at":"2026-05-18T00:33:49.831199+00:00"},{"alias_kind":"pith_short_12","alias_value":"JDZFN3U6AFGG","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_16","alias_value":"JDZFN3U6AFGGL7XP","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_8","alias_value":"JDZFN3U6","created_at":"2026-05-18T12:31:24.725408+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JDZFN3U6AFGGL7XPBNZMYELCG7","json":"https://pith.science/pith/JDZFN3U6AFGGL7XPBNZMYELCG7.json","graph_json":"https://pith.science/api/pith-number/JDZFN3U6AFGGL7XPBNZMYELCG7/graph.json","events_json":"https://pith.science/api/pith-number/JDZFN3U6AFGGL7XPBNZMYELCG7/events.json","paper":"https://pith.science/paper/JDZFN3U6"},"agent_actions":{"view_html":"https://pith.science/pith/JDZFN3U6AFGGL7XPBNZMYELCG7","download_json":"https://pith.science/pith/JDZFN3U6AFGGL7XPBNZMYELCG7.json","view_paper":"https://pith.science/paper/JDZFN3U6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1705.05511&json=true","fetch_graph":"https://pith.science/api/pith-number/JDZFN3U6AFGGL7XPBNZMYELCG7/graph.json","fetch_events":"https://pith.science/api/pith-number/JDZFN3U6AFGGL7XPBNZMYELCG7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JDZFN3U6AFGGL7XPBNZMYELCG7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JDZFN3U6AFGGL7XPBNZMYELCG7/action/storage_attestation","attest_author":"https://pith.science/pith/JDZFN3U6AFGGL7XPBNZMYELCG7/action/author_attestation","sign_citation":"https://pith.science/pith/JDZFN3U6AFGGL7XPBNZMYELCG7/action/citation_signature","submit_replication":"https://pith.science/pith/JDZFN3U6AFGGL7XPBNZMYELCG7/action/replication_record"}},"created_at":"2026-05-18T00:33:49.831199+00:00","updated_at":"2026-05-18T00:33:49.831199+00:00"}