{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1993:ERK4NFAR52U5SANJLUQNKWPZHN","short_pith_number":"pith:ERK4NFAR","schema_version":"1.0","canonical_sha256":"2455c69411eea9d901a95d20d559f93b694f80735c2f2b832120dfcf294abc18","source":{"kind":"arxiv","id":"hep-ph/9307316","version":2},"attestation_state":"computed","paper":{"title":"A New Class of Majoron-Emitting Double-Beta Decays","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C.P. Burgess, J.M. Cline","submitted_at":"1993-07-21T23:17:33Z","abstract_excerpt":"Motivated by the excess events that have recently been found near the endpoints of the double beta decay spectra of several elements, we re-examine models in which double beta decay can proceed through the neutrinoless emission of massless Nambu-Goldstone bosons (majorons). Noting that models proposed to date for this process must fine-tune either a scalar mass or a VEV to be less than 10 keV, we introduce a new kind of majoron which avoids this difficulty by carrying lepton number $L=-2$. We analyze in detail the requirements that models of both the conventional and our new type must satisfy "},"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":"hep-ph/9307316","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1993-07-21T23:17:33Z","cross_cats_sorted":[],"title_canon_sha256":"86bfaac4f666c67919546ee61772517b96aa8fb55b15fbb0ee0ef6711d63fa45","abstract_canon_sha256":"019a57bc2f4b22f4a4fa750376c13b903ecfb761cb61b3dacf682bf25b707ae4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:55:49.487218Z","signature_b64":"3sYwD2Z2fs+6trLP0WJFfZ9StDhbWlq5ys9nzog5dYAYyOF3K9803LeM0Z7txYMTjYOMpZwTY2FK3SAASGcjBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2455c69411eea9d901a95d20d559f93b694f80735c2f2b832120dfcf294abc18","last_reissued_at":"2026-07-04T15:55:49.486879Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:55:49.486879Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A New Class of Majoron-Emitting Double-Beta Decays","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C.P. Burgess, J.M. Cline","submitted_at":"1993-07-21T23:17:33Z","abstract_excerpt":"Motivated by the excess events that have recently been found near the endpoints of the double beta decay spectra of several elements, we re-examine models in which double beta decay can proceed through the neutrinoless emission of massless Nambu-Goldstone bosons (majorons). Noting that models proposed to date for this process must fine-tune either a scalar mass or a VEV to be less than 10 keV, we introduce a new kind of majoron which avoids this difficulty by carrying lepton number $L=-2$. We analyze in detail the requirements that models of both the conventional and our new type must satisfy "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9307316","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/9307316/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":"hep-ph/9307316","created_at":"2026-07-04T15:55:49.486937+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9307316v2","created_at":"2026-07-04T15:55:49.486937+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9307316","created_at":"2026-07-04T15:55:49.486937+00:00"},{"alias_kind":"pith_short_12","alias_value":"ERK4NFAR52U5","created_at":"2026-07-04T15:55:49.486937+00:00"},{"alias_kind":"pith_short_16","alias_value":"ERK4NFAR52U5SANJ","created_at":"2026-07-04T15:55:49.486937+00:00"},{"alias_kind":"pith_short_8","alias_value":"ERK4NFAR","created_at":"2026-07-04T15:55:49.486937+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.14160","citing_title":"$2\\nu\\beta\\beta$ Spectrum in Chiral Effective Field Theory","ref_index":15,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ERK4NFAR52U5SANJLUQNKWPZHN","json":"https://pith.science/pith/ERK4NFAR52U5SANJLUQNKWPZHN.json","graph_json":"https://pith.science/api/pith-number/ERK4NFAR52U5SANJLUQNKWPZHN/graph.json","events_json":"https://pith.science/api/pith-number/ERK4NFAR52U5SANJLUQNKWPZHN/events.json","paper":"https://pith.science/paper/ERK4NFAR"},"agent_actions":{"view_html":"https://pith.science/pith/ERK4NFAR52U5SANJLUQNKWPZHN","download_json":"https://pith.science/pith/ERK4NFAR52U5SANJLUQNKWPZHN.json","view_paper":"https://pith.science/paper/ERK4NFAR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9307316&json=true","fetch_graph":"https://pith.science/api/pith-number/ERK4NFAR52U5SANJLUQNKWPZHN/graph.json","fetch_events":"https://pith.science/api/pith-number/ERK4NFAR52U5SANJLUQNKWPZHN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ERK4NFAR52U5SANJLUQNKWPZHN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ERK4NFAR52U5SANJLUQNKWPZHN/action/storage_attestation","attest_author":"https://pith.science/pith/ERK4NFAR52U5SANJLUQNKWPZHN/action/author_attestation","sign_citation":"https://pith.science/pith/ERK4NFAR52U5SANJLUQNKWPZHN/action/citation_signature","submit_replication":"https://pith.science/pith/ERK4NFAR52U5SANJLUQNKWPZHN/action/replication_record"}},"created_at":"2026-07-04T15:55:49.486937+00:00","updated_at":"2026-07-04T15:55:49.486937+00:00"}