{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:2TUPGT4VPBBBTUTQIRSTWWHLX7","short_pith_number":"pith:2TUPGT4V","schema_version":"1.0","canonical_sha256":"d4e8f34f95784219d27044653b58ebbfc7e37b36b9e19c7da0c4828aad0b6ecf","source":{"kind":"arxiv","id":"1606.04028","version":1},"attestation_state":"computed","paper":{"title":"Change of nuclear configurations in the neutrinoless double-$\\beta$ decay of $^{130}$Te $\\rightarrow$ $^{130}$Xe and $^{136}$Xe $\\rightarrow$ $^{136}$Ba","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"nucl-ex","authors_text":"A. Tamii, B. Liu, B. P. Kay, C. Iwamoto, C. R. Hoffman, D. K. Sharp, E. Ideguchi, G. S\\\"usoy, H. Fujita, H. J. Ong, J. A. Clark, J. P. Entwisle, J. P. Schiffer, M. Miura, M. Takaki, M. Tsumura, N. Aoi, S. Adachi, S. J. Freeman, S. V. Szwec, T. Furuno, T. Hashimoto, T. Ito, T. Kawabata, T. Suzuki, T. Yamamoto, Y. Fujita","submitted_at":"2016-06-13T16:54:28Z","abstract_excerpt":"The change in the configuration of valence protons between the initial and final states in the neutrinoless double-$\\beta$ decay of $^{130}$Te $\\rightarrow$ $^{130}$Xe and of $^{136}$Xe $\\rightarrow$ $^{136}$Ba has been determined by measuring the cross sections of the ($d$,$^3$He) reaction with 101-MeV deuterons. Together with our recent determination of the relevant neutron configurations involved in the process, a quantitative comparison with the latest shell-model and interacting-boson-model calculations reveals significant discrepancies. These are the same calculations used to determine t"},"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":"1606.04028","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2016-06-13T16:54:28Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"2d9bc4da007a53e4c139563d6a12a131d8c6bcab7cac383e9e1b8424677874d6","abstract_canon_sha256":"f5ce423264bc1a20381e57fd77864289f9e76fe9e6866ae8c4115dd51f7f7533"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:09:51.152741Z","signature_b64":"Ms/f8MP3ZUcR+C5PdpXWXHymKyojc4jb/M9cYmMrffs/OQ/XezZ2o23wfZztrFeHIhLl0I0LOtoy/8o8n0wWCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d4e8f34f95784219d27044653b58ebbfc7e37b36b9e19c7da0c4828aad0b6ecf","last_reissued_at":"2026-05-18T01:09:51.152164Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:09:51.152164Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Change of nuclear configurations in the neutrinoless double-$\\beta$ decay of $^{130}$Te $\\rightarrow$ $^{130}$Xe and $^{136}$Xe $\\rightarrow$ $^{136}$Ba","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"nucl-ex","authors_text":"A. Tamii, B. Liu, B. P. Kay, C. Iwamoto, C. R. Hoffman, D. K. Sharp, E. Ideguchi, G. S\\\"usoy, H. Fujita, H. J. Ong, J. A. Clark, J. P. Entwisle, J. P. Schiffer, M. Miura, M. Takaki, M. Tsumura, N. Aoi, S. Adachi, S. J. Freeman, S. V. Szwec, T. Furuno, T. Hashimoto, T. Ito, T. Kawabata, T. Suzuki, T. Yamamoto, Y. Fujita","submitted_at":"2016-06-13T16:54:28Z","abstract_excerpt":"The change in the configuration of valence protons between the initial and final states in the neutrinoless double-$\\beta$ decay of $^{130}$Te $\\rightarrow$ $^{130}$Xe and of $^{136}$Xe $\\rightarrow$ $^{136}$Ba has been determined by measuring the cross sections of the ($d$,$^3$He) reaction with 101-MeV deuterons. Together with our recent determination of the relevant neutron configurations involved in the process, a quantitative comparison with the latest shell-model and interacting-boson-model calculations reveals significant discrepancies. These are the same calculations used to determine t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.04028","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":"1606.04028","created_at":"2026-05-18T01:09:51.152254+00:00"},{"alias_kind":"arxiv_version","alias_value":"1606.04028v1","created_at":"2026-05-18T01:09:51.152254+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.04028","created_at":"2026-05-18T01:09:51.152254+00:00"},{"alias_kind":"pith_short_12","alias_value":"2TUPGT4VPBBB","created_at":"2026-05-18T12:29:55.572404+00:00"},{"alias_kind":"pith_short_16","alias_value":"2TUPGT4VPBBBTUTQ","created_at":"2026-05-18T12:29:55.572404+00:00"},{"alias_kind":"pith_short_8","alias_value":"2TUPGT4V","created_at":"2026-05-18T12:29:55.572404+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/2TUPGT4VPBBBTUTQIRSTWWHLX7","json":"https://pith.science/pith/2TUPGT4VPBBBTUTQIRSTWWHLX7.json","graph_json":"https://pith.science/api/pith-number/2TUPGT4VPBBBTUTQIRSTWWHLX7/graph.json","events_json":"https://pith.science/api/pith-number/2TUPGT4VPBBBTUTQIRSTWWHLX7/events.json","paper":"https://pith.science/paper/2TUPGT4V"},"agent_actions":{"view_html":"https://pith.science/pith/2TUPGT4VPBBBTUTQIRSTWWHLX7","download_json":"https://pith.science/pith/2TUPGT4VPBBBTUTQIRSTWWHLX7.json","view_paper":"https://pith.science/paper/2TUPGT4V","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1606.04028&json=true","fetch_graph":"https://pith.science/api/pith-number/2TUPGT4VPBBBTUTQIRSTWWHLX7/graph.json","fetch_events":"https://pith.science/api/pith-number/2TUPGT4VPBBBTUTQIRSTWWHLX7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2TUPGT4VPBBBTUTQIRSTWWHLX7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2TUPGT4VPBBBTUTQIRSTWWHLX7/action/storage_attestation","attest_author":"https://pith.science/pith/2TUPGT4VPBBBTUTQIRSTWWHLX7/action/author_attestation","sign_citation":"https://pith.science/pith/2TUPGT4VPBBBTUTQIRSTWWHLX7/action/citation_signature","submit_replication":"https://pith.science/pith/2TUPGT4VPBBBTUTQIRSTWWHLX7/action/replication_record"}},"created_at":"2026-05-18T01:09:51.152254+00:00","updated_at":"2026-05-18T01:09:51.152254+00:00"}