{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:EMRUZZ4IZWNA3ZAIYIVPXGN6WK","short_pith_number":"pith:EMRUZZ4I","canonical_record":{"source":{"id":"1505.00978","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-05-05T12:19:41Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"f01995c8088a6713fd8068260cabe527832dd69dc4ff01ad313388e0e988b1fb","abstract_canon_sha256":"ee8da29d3e970d41d631e994d9dcee2e87e636ff8761bf87f5d97a8484f47541"},"schema_version":"1.0"},"canonical_sha256":"23234ce788cd9a0de408c22afb99beb292ab577ff2896bec2232129392621f5e","source":{"kind":"arxiv","id":"1505.00978","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.00978","created_at":"2026-05-18T01:34:23Z"},{"alias_kind":"arxiv_version","alias_value":"1505.00978v2","created_at":"2026-05-18T01:34:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.00978","created_at":"2026-05-18T01:34:23Z"},{"alias_kind":"pith_short_12","alias_value":"EMRUZZ4IZWNA","created_at":"2026-05-18T12:29:19Z"},{"alias_kind":"pith_short_16","alias_value":"EMRUZZ4IZWNA3ZAI","created_at":"2026-05-18T12:29:19Z"},{"alias_kind":"pith_short_8","alias_value":"EMRUZZ4I","created_at":"2026-05-18T12:29:19Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:EMRUZZ4IZWNA3ZAIYIVPXGN6WK","target":"record","payload":{"canonical_record":{"source":{"id":"1505.00978","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-05-05T12:19:41Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"f01995c8088a6713fd8068260cabe527832dd69dc4ff01ad313388e0e988b1fb","abstract_canon_sha256":"ee8da29d3e970d41d631e994d9dcee2e87e636ff8761bf87f5d97a8484f47541"},"schema_version":"1.0"},"canonical_sha256":"23234ce788cd9a0de408c22afb99beb292ab577ff2896bec2232129392621f5e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:34:23.088062Z","signature_b64":"CUMVsOGRMq2XcdUsXDHcARURErstbaL0tcegnJ87Gg3nb3YUDn0FUpGEgnpdAPWAFhGdUTrpyLC2mzx6VGUTCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"23234ce788cd9a0de408c22afb99beb292ab577ff2896bec2232129392621f5e","last_reissued_at":"2026-05-18T01:34:23.087430Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:34:23.087430Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1505.00978","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:34:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"i40Cc/jDvqMaPwiSBmLlbZUY3lV5rv8MJRje8Zr1Ww0CvexI2cLlhidWN3Z4ixwZhDJZZK4ouZ2JF8+o1V6qBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T11:53:46.460581Z"},"content_sha256":"3adf59c19a4291783d1a406caff4a4a131314344aac799211c323c707aaea7c4","schema_version":"1.0","event_id":"sha256:3adf59c19a4291783d1a406caff4a4a131314344aac799211c323c707aaea7c4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:EMRUZZ4IZWNA3ZAIYIVPXGN6WK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Predictions for Neutrinoless Double-Beta Decay in the 3+1 Sterile Neutrino Scenario","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"C. Giunti, E. M. Zavanin","submitted_at":"2015-05-05T12:19:41Z","abstract_excerpt":"We present accurate predictions of the effective Majorana mass $|m_{\\beta\\beta}|$ in neutrinoless double-$\\beta$ decay in the standard case of $3\\nu$ mixing and in the case of 3+1 neutrino mixing indicated by the reactor, Gallium and LSND anomalies. We have taken into account the uncertainties of the neutrino mixing parameters determined by oscillation experiments. It is shown that the predictions for $|m_{\\beta\\beta}|$ in the cases of $3\\nu$ and 3+1 mixing are quite different, in agreement with previous discussions in the literature, and that future measurements of neutrinoless double-$\\beta$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.00978","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":""},"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":"2026-05-18T01:34:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/5QMaIPp51sH7kA+O+7+cb9cDSLediBWXOYrjNIp/ucrQPfb4xNH4SJCL6X7z30zozaAJe1dm9BPKCBeOgRVCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T11:53:46.461043Z"},"content_sha256":"e6929c5803682b7ddf433bb31a33e7f3d11733104630e32d08db91986bb2a14e","schema_version":"1.0","event_id":"sha256:e6929c5803682b7ddf433bb31a33e7f3d11733104630e32d08db91986bb2a14e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EMRUZZ4IZWNA3ZAIYIVPXGN6WK/bundle.json","state_url":"https://pith.science/pith/EMRUZZ4IZWNA3ZAIYIVPXGN6WK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EMRUZZ4IZWNA3ZAIYIVPXGN6WK/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":"2026-08-12T11:53:46Z","links":{"resolver":"https://pith.science/pith/EMRUZZ4IZWNA3ZAIYIVPXGN6WK","bundle":"https://pith.science/pith/EMRUZZ4IZWNA3ZAIYIVPXGN6WK/bundle.json","state":"https://pith.science/pith/EMRUZZ4IZWNA3ZAIYIVPXGN6WK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EMRUZZ4IZWNA3ZAIYIVPXGN6WK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:EMRUZZ4IZWNA3ZAIYIVPXGN6WK","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":"ee8da29d3e970d41d631e994d9dcee2e87e636ff8761bf87f5d97a8484f47541","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-05-05T12:19:41Z","title_canon_sha256":"f01995c8088a6713fd8068260cabe527832dd69dc4ff01ad313388e0e988b1fb"},"schema_version":"1.0","source":{"id":"1505.00978","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.00978","created_at":"2026-05-18T01:34:23Z"},{"alias_kind":"arxiv_version","alias_value":"1505.00978v2","created_at":"2026-05-18T01:34:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.00978","created_at":"2026-05-18T01:34:23Z"},{"alias_kind":"pith_short_12","alias_value":"EMRUZZ4IZWNA","created_at":"2026-05-18T12:29:19Z"},{"alias_kind":"pith_short_16","alias_value":"EMRUZZ4IZWNA3ZAI","created_at":"2026-05-18T12:29:19Z"},{"alias_kind":"pith_short_8","alias_value":"EMRUZZ4I","created_at":"2026-05-18T12:29:19Z"}],"graph_snapshots":[{"event_id":"sha256:e6929c5803682b7ddf433bb31a33e7f3d11733104630e32d08db91986bb2a14e","target":"graph","created_at":"2026-05-18T01:34:23Z","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":"We present accurate predictions of the effective Majorana mass $|m_{\\beta\\beta}|$ in neutrinoless double-$\\beta$ decay in the standard case of $3\\nu$ mixing and in the case of 3+1 neutrino mixing indicated by the reactor, Gallium and LSND anomalies. We have taken into account the uncertainties of the neutrino mixing parameters determined by oscillation experiments. It is shown that the predictions for $|m_{\\beta\\beta}|$ in the cases of $3\\nu$ and 3+1 mixing are quite different, in agreement with previous discussions in the literature, and that future measurements of neutrinoless double-$\\beta$","authors_text":"C. Giunti, E. M. Zavanin","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-05-05T12:19:41Z","title":"Predictions for Neutrinoless Double-Beta Decay in the 3+1 Sterile Neutrino Scenario"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.00978","kind":"arxiv","version":2},"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":"sha256:3adf59c19a4291783d1a406caff4a4a131314344aac799211c323c707aaea7c4","target":"record","created_at":"2026-05-18T01:34:23Z","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":"ee8da29d3e970d41d631e994d9dcee2e87e636ff8761bf87f5d97a8484f47541","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-05-05T12:19:41Z","title_canon_sha256":"f01995c8088a6713fd8068260cabe527832dd69dc4ff01ad313388e0e988b1fb"},"schema_version":"1.0","source":{"id":"1505.00978","kind":"arxiv","version":2}},"canonical_sha256":"23234ce788cd9a0de408c22afb99beb292ab577ff2896bec2232129392621f5e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"23234ce788cd9a0de408c22afb99beb292ab577ff2896bec2232129392621f5e","first_computed_at":"2026-05-18T01:34:23.087430Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:34:23.087430Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"CUMVsOGRMq2XcdUsXDHcARURErstbaL0tcegnJ87Gg3nb3YUDn0FUpGEgnpdAPWAFhGdUTrpyLC2mzx6VGUTCg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:34:23.088062Z","signed_message":"canonical_sha256_bytes"},"source_id":"1505.00978","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3adf59c19a4291783d1a406caff4a4a131314344aac799211c323c707aaea7c4","sha256:e6929c5803682b7ddf433bb31a33e7f3d11733104630e32d08db91986bb2a14e"],"state_sha256":"0b64af1fe0c8ec2533069b81470ba8b1d9a24a4287383dc4f817c15498bfb427"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FD9UZQ0f4aJpkBpSdbwy/PAElDFLwLibzpPtJhcbXpzF6EpbxWHnwQZ8bh7dI1/RIGszGyJpv2fqPQaqsHTtBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-12T11:53:46.464870Z","bundle_sha256":"ba53df44ece27eb53ab8448fd6d4035a22b09bf9ea7ba2891669509495ec28d8"}}