{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:BOSBX2JSUXZJ27YTVLOLG74K4G","short_pith_number":"pith:BOSBX2JS","schema_version":"1.0","canonical_sha256":"0ba41be932a5f29d7f13aadcb37f8ae19b29cf3a4367d92107e56b44b3db971c","source":{"kind":"arxiv","id":"2301.02007","version":1},"attestation_state":"computed","paper":{"title":"$0^+$ to $2^+$ neutrinoless double-$\\beta$ decay of $^{76}$Ge, $^{82}$Se, $^{130}$Te and $^{136}$Xe in the microscopic interacting boson model}","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"E. Santopinto, J. Ferretti, J. Kotila, R. Magana Vsevolodovna","submitted_at":"2023-01-05T11:14:25Z","abstract_excerpt":"Here, we study the neutrinoless double-$\\beta$ ($0\\nu\\beta\\beta$) decay between the ground state and the first $2^+$ state of $^{76}\\mbox{Ge} \\rightarrow {}^{76}\\mbox{Se}$, $^{82}\\mbox{Se} \\rightarrow{}^{82}\\mbox{Kr}$, $^{130}\\mbox{Te} \\rightarrow {}^{130}\\mbox{Xe}$ and $^{136}\\mbox{Xe} \\rightarrow {}^{136}\\mbox{Ba}$ systems. The relevant nuclear matrix elements (NMEs) involved in the process are calculated within the formalism of the microscopic interacting boson model (IBM-2). The IBM-2 has been widely used to obtain predictions for nuclear observables, such as the spectrum, but also to expl"},"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":"2301.02007","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2023-01-05T11:14:25Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"54b532c9f42699c3917a4cbe6ac6e276f11969d3f609b450d0ea059f6730235d","abstract_canon_sha256":"dd662299fad954a6a502a35fcc79ed6d80229709c94eddd6301183b9bd8a77e9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:30:48.888551Z","signature_b64":"W1XQL5ZI0Dz5x371KSL2WJvjkjpUQ7VT0aP3sc1CkBQkvJbv7hkpAwnNwNisRJbv0VgiZo4xChT37bMqCp6oBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0ba41be932a5f29d7f13aadcb37f8ae19b29cf3a4367d92107e56b44b3db971c","last_reissued_at":"2026-07-05T05:30:48.888102Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:30:48.888102Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$0^+$ to $2^+$ neutrinoless double-$\\beta$ decay of $^{76}$Ge, $^{82}$Se, $^{130}$Te and $^{136}$Xe in the microscopic interacting boson model}","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"E. Santopinto, J. Ferretti, J. Kotila, R. Magana Vsevolodovna","submitted_at":"2023-01-05T11:14:25Z","abstract_excerpt":"Here, we study the neutrinoless double-$\\beta$ ($0\\nu\\beta\\beta$) decay between the ground state and the first $2^+$ state of $^{76}\\mbox{Ge} \\rightarrow {}^{76}\\mbox{Se}$, $^{82}\\mbox{Se} \\rightarrow{}^{82}\\mbox{Kr}$, $^{130}\\mbox{Te} \\rightarrow {}^{130}\\mbox{Xe}$ and $^{136}\\mbox{Xe} \\rightarrow {}^{136}\\mbox{Ba}$ systems. The relevant nuclear matrix elements (NMEs) involved in the process are calculated within the formalism of the microscopic interacting boson model (IBM-2). The IBM-2 has been widely used to obtain predictions for nuclear observables, such as the spectrum, but also to expl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2301.02007","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2301.02007/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2301.02007","created_at":"2026-07-05T05:30:48.888175+00:00"},{"alias_kind":"arxiv_version","alias_value":"2301.02007v1","created_at":"2026-07-05T05:30:48.888175+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2301.02007","created_at":"2026-07-05T05:30:48.888175+00:00"},{"alias_kind":"pith_short_12","alias_value":"BOSBX2JSUXZJ","created_at":"2026-07-05T05:30:48.888175+00:00"},{"alias_kind":"pith_short_16","alias_value":"BOSBX2JSUXZJ27YT","created_at":"2026-07-05T05:30:48.888175+00:00"},{"alias_kind":"pith_short_8","alias_value":"BOSBX2JS","created_at":"2026-07-05T05:30:48.888175+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/BOSBX2JSUXZJ27YTVLOLG74K4G","json":"https://pith.science/pith/BOSBX2JSUXZJ27YTVLOLG74K4G.json","graph_json":"https://pith.science/api/pith-number/BOSBX2JSUXZJ27YTVLOLG74K4G/graph.json","events_json":"https://pith.science/api/pith-number/BOSBX2JSUXZJ27YTVLOLG74K4G/events.json","paper":"https://pith.science/paper/BOSBX2JS"},"agent_actions":{"view_html":"https://pith.science/pith/BOSBX2JSUXZJ27YTVLOLG74K4G","download_json":"https://pith.science/pith/BOSBX2JSUXZJ27YTVLOLG74K4G.json","view_paper":"https://pith.science/paper/BOSBX2JS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2301.02007&json=true","fetch_graph":"https://pith.science/api/pith-number/BOSBX2JSUXZJ27YTVLOLG74K4G/graph.json","fetch_events":"https://pith.science/api/pith-number/BOSBX2JSUXZJ27YTVLOLG74K4G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BOSBX2JSUXZJ27YTVLOLG74K4G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BOSBX2JSUXZJ27YTVLOLG74K4G/action/storage_attestation","attest_author":"https://pith.science/pith/BOSBX2JSUXZJ27YTVLOLG74K4G/action/author_attestation","sign_citation":"https://pith.science/pith/BOSBX2JSUXZJ27YTVLOLG74K4G/action/citation_signature","submit_replication":"https://pith.science/pith/BOSBX2JSUXZJ27YTVLOLG74K4G/action/replication_record"}},"created_at":"2026-07-05T05:30:48.888175+00:00","updated_at":"2026-07-05T05:30:48.888175+00:00"}