{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:NVKLZJCTDLKI5OWVMSUSWNCHSY","short_pith_number":"pith:NVKLZJCT","schema_version":"1.0","canonical_sha256":"6d54bca4531ad48ebad564a92b34479616ed641cacbee58e8c3477487e241298","source":{"kind":"arxiv","id":"1707.04353","version":1},"attestation_state":"computed","paper":{"title":"Effective field theory for triaxially deformed nuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"J. Meng, N. Kaiser, Q. B. Chen, Ulf-G. Mei{\\ss}ner","submitted_at":"2017-07-13T23:19:49Z","abstract_excerpt":"Effective field theory (EFT) is generalized to investigate the rotational motion of triaxially deformed even-even nuclei. A Hamiltonian, called the triaxial rotor model (TRM), is obtained up to next-to-leading order (NLO) within the EFT formalism. Its applicability is examined by comparing with a five-dimensional collective Hamiltonian (5DCH) for the description of the energy spectra of the ground state and $\\gamma$ band in Ru isotopes. It is found that by taking into account the NLO corrections, the ground state band in the whole spin region and the $\\gamma$ band in the low spin region are we"},"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":"1707.04353","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-07-13T23:19:49Z","cross_cats_sorted":[],"title_canon_sha256":"87521c4d3b268e7cc5e451d17aadaff8a8237a1ae143d03afa997d83eee8992c","abstract_canon_sha256":"54423d1e80fea8788350e5ea9d850a43dc9affc449f13910e715f93fc7f27898"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:30:01.375846Z","signature_b64":"1LiGWgwakTSm2MbKAfStfvO3L85cYYM5p2LeuE8DtTLTz48u0vIKwluT5qaV31qK8rzgIVyznkxfpGtdEYqRAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6d54bca4531ad48ebad564a92b34479616ed641cacbee58e8c3477487e241298","last_reissued_at":"2026-05-18T00:30:01.375162Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:30:01.375162Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effective field theory for triaxially deformed nuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"J. Meng, N. Kaiser, Q. B. Chen, Ulf-G. Mei{\\ss}ner","submitted_at":"2017-07-13T23:19:49Z","abstract_excerpt":"Effective field theory (EFT) is generalized to investigate the rotational motion of triaxially deformed even-even nuclei. A Hamiltonian, called the triaxial rotor model (TRM), is obtained up to next-to-leading order (NLO) within the EFT formalism. Its applicability is examined by comparing with a five-dimensional collective Hamiltonian (5DCH) for the description of the energy spectra of the ground state and $\\gamma$ band in Ru isotopes. It is found that by taking into account the NLO corrections, the ground state band in the whole spin region and the $\\gamma$ band in the low spin region are we"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.04353","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":"1707.04353","created_at":"2026-05-18T00:30:01.375267+00:00"},{"alias_kind":"arxiv_version","alias_value":"1707.04353v1","created_at":"2026-05-18T00:30:01.375267+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.04353","created_at":"2026-05-18T00:30:01.375267+00:00"},{"alias_kind":"pith_short_12","alias_value":"NVKLZJCTDLKI","created_at":"2026-05-18T12:31:34.259226+00:00"},{"alias_kind":"pith_short_16","alias_value":"NVKLZJCTDLKI5OWV","created_at":"2026-05-18T12:31:34.259226+00:00"},{"alias_kind":"pith_short_8","alias_value":"NVKLZJCT","created_at":"2026-05-18T12:31:34.259226+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/NVKLZJCTDLKI5OWVMSUSWNCHSY","json":"https://pith.science/pith/NVKLZJCTDLKI5OWVMSUSWNCHSY.json","graph_json":"https://pith.science/api/pith-number/NVKLZJCTDLKI5OWVMSUSWNCHSY/graph.json","events_json":"https://pith.science/api/pith-number/NVKLZJCTDLKI5OWVMSUSWNCHSY/events.json","paper":"https://pith.science/paper/NVKLZJCT"},"agent_actions":{"view_html":"https://pith.science/pith/NVKLZJCTDLKI5OWVMSUSWNCHSY","download_json":"https://pith.science/pith/NVKLZJCTDLKI5OWVMSUSWNCHSY.json","view_paper":"https://pith.science/paper/NVKLZJCT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1707.04353&json=true","fetch_graph":"https://pith.science/api/pith-number/NVKLZJCTDLKI5OWVMSUSWNCHSY/graph.json","fetch_events":"https://pith.science/api/pith-number/NVKLZJCTDLKI5OWVMSUSWNCHSY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NVKLZJCTDLKI5OWVMSUSWNCHSY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NVKLZJCTDLKI5OWVMSUSWNCHSY/action/storage_attestation","attest_author":"https://pith.science/pith/NVKLZJCTDLKI5OWVMSUSWNCHSY/action/author_attestation","sign_citation":"https://pith.science/pith/NVKLZJCTDLKI5OWVMSUSWNCHSY/action/citation_signature","submit_replication":"https://pith.science/pith/NVKLZJCTDLKI5OWVMSUSWNCHSY/action/replication_record"}},"created_at":"2026-05-18T00:30:01.375267+00:00","updated_at":"2026-05-18T00:30:01.375267+00:00"}