{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:VPE7MBKSCAUWVPVHCQGQFUHXCF","short_pith_number":"pith:VPE7MBKS","canonical_record":{"source":{"id":"1804.04227","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-04-11T21:20:44Z","cross_cats_sorted":[],"title_canon_sha256":"0f2f0f1c6b0781f682eb9d15f446e2a03af5d674fa44530af392a9ea9725d451","abstract_canon_sha256":"5ff4d2cb479414eef898004947a67433d1deeee5629f649aed3d6e380ee2f2f1"},"schema_version":"1.0"},"canonical_sha256":"abc9f6055210296abea7140d02d0f7114d3a11698ba2c5720337a6f667fe6170","source":{"kind":"arxiv","id":"1804.04227","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1804.04227","created_at":"2026-05-18T00:18:40Z"},{"alias_kind":"arxiv_version","alias_value":"1804.04227v1","created_at":"2026-05-18T00:18:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1804.04227","created_at":"2026-05-18T00:18:40Z"},{"alias_kind":"pith_short_12","alias_value":"VPE7MBKSCAUW","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_16","alias_value":"VPE7MBKSCAUWVPVH","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_8","alias_value":"VPE7MBKS","created_at":"2026-05-18T12:32:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:VPE7MBKSCAUWVPVHCQGQFUHXCF","target":"record","payload":{"canonical_record":{"source":{"id":"1804.04227","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-04-11T21:20:44Z","cross_cats_sorted":[],"title_canon_sha256":"0f2f0f1c6b0781f682eb9d15f446e2a03af5d674fa44530af392a9ea9725d451","abstract_canon_sha256":"5ff4d2cb479414eef898004947a67433d1deeee5629f649aed3d6e380ee2f2f1"},"schema_version":"1.0"},"canonical_sha256":"abc9f6055210296abea7140d02d0f7114d3a11698ba2c5720337a6f667fe6170","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:18:40.313586Z","signature_b64":"yJwQOsBqUPmhLvaUa/5kveb5MhKKRrYh5UPf944PKInF6FBSOmzfnRnAoIQ7IIjFcTrRznu3khf9fQq529HECQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"abc9f6055210296abea7140d02d0f7114d3a11698ba2c5720337a6f667fe6170","last_reissued_at":"2026-05-18T00:18:40.313112Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:18:40.313112Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1804.04227","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:18:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"llynJTLPezcmLLqx5NXKoAzCr20KG53+LixrgPOvHnf8QdJEKKP4ZCtOu/PwNZ0VD98PNEWUVjxgOewEuW+0Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-19T23:28:05.703615Z"},"content_sha256":"63dd6390973e2b723ea5b7640cc297e37a24c73da3b414010aac603521907f70","schema_version":"1.0","event_id":"sha256:63dd6390973e2b723ea5b7640cc297e37a24c73da3b414010aac603521907f70"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:VPE7MBKSCAUWVPVHCQGQFUHXCF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Improved description of the $2\\nu\\beta\\beta$-decay and a possibility to determine the effective axial-vector coupling constant","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Amand Faessler, Du\\v{s}an \\v{S}tef\\'anik, Fedor \\v{S}imkovic, Rastislav Dvornick\\'y","submitted_at":"2018-04-11T21:20:44Z","abstract_excerpt":"An improved formalism of the two-neutrino double-beta decay ($2\\nu\\beta\\beta$-decay) rate is presented, which takes into account the dependence of energy denominators on lepton energies via the Taylor expansion. Till now, only the leading term in this expansion has been considered. The revised $2\\nu\\beta\\beta$-decay rate and differential characteristics depend on additional phase-space factors weighted by the ratios of $2\\nu\\beta\\beta$-decay nuclear matrix elements with different powers of the energy denominator. For nuclei of experimental interest all phase-space factors are calculated by usi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1804.04227","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:18:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RFVdpKFatVXuUJhBxi2EuQ5mctpfgPa0FAWT83wsyQzsXy67d5Y5QSRaXBeqJ0/yiE//6RKYavADr2APlt12DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-19T23:28:05.704387Z"},"content_sha256":"079ed7c7765d29a5d48f47d099ca68b70a2baf47b72fd1fa5e9034b42025b081","schema_version":"1.0","event_id":"sha256:079ed7c7765d29a5d48f47d099ca68b70a2baf47b72fd1fa5e9034b42025b081"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VPE7MBKSCAUWVPVHCQGQFUHXCF/bundle.json","state_url":"https://pith.science/pith/VPE7MBKSCAUWVPVHCQGQFUHXCF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VPE7MBKSCAUWVPVHCQGQFUHXCF/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-19T23:28:05Z","links":{"resolver":"https://pith.science/pith/VPE7MBKSCAUWVPVHCQGQFUHXCF","bundle":"https://pith.science/pith/VPE7MBKSCAUWVPVHCQGQFUHXCF/bundle.json","state":"https://pith.science/pith/VPE7MBKSCAUWVPVHCQGQFUHXCF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VPE7MBKSCAUWVPVHCQGQFUHXCF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:VPE7MBKSCAUWVPVHCQGQFUHXCF","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"5ff4d2cb479414eef898004947a67433d1deeee5629f649aed3d6e380ee2f2f1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-04-11T21:20:44Z","title_canon_sha256":"0f2f0f1c6b0781f682eb9d15f446e2a03af5d674fa44530af392a9ea9725d451"},"schema_version":"1.0","source":{"id":"1804.04227","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1804.04227","created_at":"2026-05-18T00:18:40Z"},{"alias_kind":"arxiv_version","alias_value":"1804.04227v1","created_at":"2026-05-18T00:18:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1804.04227","created_at":"2026-05-18T00:18:40Z"},{"alias_kind":"pith_short_12","alias_value":"VPE7MBKSCAUW","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_16","alias_value":"VPE7MBKSCAUWVPVH","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_8","alias_value":"VPE7MBKS","created_at":"2026-05-18T12:32:59Z"}],"graph_snapshots":[{"event_id":"sha256:079ed7c7765d29a5d48f47d099ca68b70a2baf47b72fd1fa5e9034b42025b081","target":"graph","created_at":"2026-05-18T00:18:40Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"An improved formalism of the two-neutrino double-beta decay ($2\\nu\\beta\\beta$-decay) rate is presented, which takes into account the dependence of energy denominators on lepton energies via the Taylor expansion. Till now, only the leading term in this expansion has been considered. The revised $2\\nu\\beta\\beta$-decay rate and differential characteristics depend on additional phase-space factors weighted by the ratios of $2\\nu\\beta\\beta$-decay nuclear matrix elements with different powers of the energy denominator. For nuclei of experimental interest all phase-space factors are calculated by usi","authors_text":"Amand Faessler, Du\\v{s}an \\v{S}tef\\'anik, Fedor \\v{S}imkovic, Rastislav Dvornick\\'y","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-04-11T21:20:44Z","title":"Improved description of the $2\\nu\\beta\\beta$-decay and a possibility to determine the effective axial-vector coupling constant"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1804.04227","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:63dd6390973e2b723ea5b7640cc297e37a24c73da3b414010aac603521907f70","target":"record","created_at":"2026-05-18T00:18:40Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"5ff4d2cb479414eef898004947a67433d1deeee5629f649aed3d6e380ee2f2f1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-04-11T21:20:44Z","title_canon_sha256":"0f2f0f1c6b0781f682eb9d15f446e2a03af5d674fa44530af392a9ea9725d451"},"schema_version":"1.0","source":{"id":"1804.04227","kind":"arxiv","version":1}},"canonical_sha256":"abc9f6055210296abea7140d02d0f7114d3a11698ba2c5720337a6f667fe6170","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"abc9f6055210296abea7140d02d0f7114d3a11698ba2c5720337a6f667fe6170","first_computed_at":"2026-05-18T00:18:40.313112Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:18:40.313112Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yJwQOsBqUPmhLvaUa/5kveb5MhKKRrYh5UPf944PKInF6FBSOmzfnRnAoIQ7IIjFcTrRznu3khf9fQq529HECQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:18:40.313586Z","signed_message":"canonical_sha256_bytes"},"source_id":"1804.04227","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:63dd6390973e2b723ea5b7640cc297e37a24c73da3b414010aac603521907f70","sha256:079ed7c7765d29a5d48f47d099ca68b70a2baf47b72fd1fa5e9034b42025b081"],"state_sha256":"1b1292fe900ccdfd0854b37e8bee30e995d0860f7dd6891a44bd840058601f59"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"N+umsxD6TLeksIejcv3F7d0w/OuTSqQuBkVrWxZoAWPeUgRLtY7UuPwSebCaxcKABJR9c+mHhSPdG782iD7bCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-19T23:28:05.707736Z","bundle_sha256":"391c51565213cfd39aa4c537dfae39969e303223b2f8f5ad5b777dd558dc4a70"}}