{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:JQ2SX4SDAB6VGGOMGAHI5RLRIG","short_pith_number":"pith:JQ2SX4SD","canonical_record":{"source":{"id":"1210.5367","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-10-19T10:14:12Z","cross_cats_sorted":[],"title_canon_sha256":"fdf6065f0d430b6629283ad6aab41ae7c9ce6b55a8c3f32a3069142cd8a26017","abstract_canon_sha256":"a429250388a6ae0b1fd64497266fd82db1816b296ef3e8ce7f85643ab5119056"},"schema_version":"1.0"},"canonical_sha256":"4c352bf243007d5319cc300e8ec5714188449928747959d74d9a2a1d3f3c4205","source":{"kind":"arxiv","id":"1210.5367","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.5367","created_at":"2026-05-18T01:53:45Z"},{"alias_kind":"arxiv_version","alias_value":"1210.5367v2","created_at":"2026-05-18T01:53:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.5367","created_at":"2026-05-18T01:53:45Z"},{"alias_kind":"pith_short_12","alias_value":"JQ2SX4SDAB6V","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"JQ2SX4SDAB6VGGOM","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"JQ2SX4SD","created_at":"2026-05-18T12:27:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:JQ2SX4SDAB6VGGOMGAHI5RLRIG","target":"record","payload":{"canonical_record":{"source":{"id":"1210.5367","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-10-19T10:14:12Z","cross_cats_sorted":[],"title_canon_sha256":"fdf6065f0d430b6629283ad6aab41ae7c9ce6b55a8c3f32a3069142cd8a26017","abstract_canon_sha256":"a429250388a6ae0b1fd64497266fd82db1816b296ef3e8ce7f85643ab5119056"},"schema_version":"1.0"},"canonical_sha256":"4c352bf243007d5319cc300e8ec5714188449928747959d74d9a2a1d3f3c4205","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:53:45.998850Z","signature_b64":"bdvF5yP83PlLFe7Cxp37Sa/X9A56qsOt+jcnfHGhfWG5q+mIZjhf37mOmnkH2dquoamqUNVDquTm+L1LlkHBCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4c352bf243007d5319cc300e8ec5714188449928747959d74d9a2a1d3f3c4205","last_reissued_at":"2026-05-18T01:53:45.998061Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:53:45.998061Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1210.5367","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":"2026-05-18T01:53:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SEKJJU4L+V366f4/sF/Rit1XyHldZHBp5ZIDc35OS6l7AW7UOOUb2aUZMZcCF/xC5cHITGdwM2DLEMWN2SaTDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T09:03:47.743270Z"},"content_sha256":"ba41d552a6ab95d9827a520545d5f9b890e3f51c978fe6cb6f343e9d0cd912d8","schema_version":"1.0","event_id":"sha256:ba41d552a6ab95d9827a520545d5f9b890e3f51c978fe6cb6f343e9d0cd912d8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:JQ2SX4SDAB6VGGOMGAHI5RLRIG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Uncertainties in nuclear transition matrix elements for $\\beta ^{+}\\beta ^{+}$ and $\\varepsilon \\beta ^{+}$ modes of neutrinoless positron double-$\\beta $ decay within PHFB model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"J. G. Hirsch, K. Chaturvedi, P. K. Raina, P. K. Rath, P. Lohani, R. Chandra","submitted_at":"2012-10-19T10:14:12Z","abstract_excerpt":"Uncertainties in the nuclear transition matrix elements $M^{(0\\nu)}$ and $M^{(0N)}$ of the double-positron emission $(\\beta ^{+}\\beta ^{+})_{0\\nu}$ and electron-positron conversion $(\\varepsilon \\beta ^{+})_{0\\nu}$ modes due to the exchange of light and heavy Majorana neutrinos, respectively, are calculated for $^{96}$Ru, $^{102}$Pd, $^{106}$Cd, $^{124}$Xe, $^{130}$Ba and $^{156}$Dy isotopes by employing the PHFB model with four different parameterization of the pairing plus multipolar two-body interactions and three different parameterizations of the Jastrow short range correlations. In all c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.5367","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":"2026-05-18T01:53:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lK5uYy6NeYYcaeqne4x+7A5LJEvhQDXiI/Y6rTzuswP42DhfVyBo70FcPVJfwTE1ATwzuVizPdDVnkCepBcEBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T09:03:47.743668Z"},"content_sha256":"2f2b44485da6ecdcbd581381a4242426555ac27315ee1e62fefaaf49f8408b8c","schema_version":"1.0","event_id":"sha256:2f2b44485da6ecdcbd581381a4242426555ac27315ee1e62fefaaf49f8408b8c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JQ2SX4SDAB6VGGOMGAHI5RLRIG/bundle.json","state_url":"https://pith.science/pith/JQ2SX4SDAB6VGGOMGAHI5RLRIG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JQ2SX4SDAB6VGGOMGAHI5RLRIG/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":"2026-05-30T09:03:47Z","links":{"resolver":"https://pith.science/pith/JQ2SX4SDAB6VGGOMGAHI5RLRIG","bundle":"https://pith.science/pith/JQ2SX4SDAB6VGGOMGAHI5RLRIG/bundle.json","state":"https://pith.science/pith/JQ2SX4SDAB6VGGOMGAHI5RLRIG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JQ2SX4SDAB6VGGOMGAHI5RLRIG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:JQ2SX4SDAB6VGGOMGAHI5RLRIG","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":"a429250388a6ae0b1fd64497266fd82db1816b296ef3e8ce7f85643ab5119056","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-10-19T10:14:12Z","title_canon_sha256":"fdf6065f0d430b6629283ad6aab41ae7c9ce6b55a8c3f32a3069142cd8a26017"},"schema_version":"1.0","source":{"id":"1210.5367","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.5367","created_at":"2026-05-18T01:53:45Z"},{"alias_kind":"arxiv_version","alias_value":"1210.5367v2","created_at":"2026-05-18T01:53:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.5367","created_at":"2026-05-18T01:53:45Z"},{"alias_kind":"pith_short_12","alias_value":"JQ2SX4SDAB6V","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"JQ2SX4SDAB6VGGOM","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"JQ2SX4SD","created_at":"2026-05-18T12:27:11Z"}],"graph_snapshots":[{"event_id":"sha256:2f2b44485da6ecdcbd581381a4242426555ac27315ee1e62fefaaf49f8408b8c","target":"graph","created_at":"2026-05-18T01:53:45Z","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":"Uncertainties in the nuclear transition matrix elements $M^{(0\\nu)}$ and $M^{(0N)}$ of the double-positron emission $(\\beta ^{+}\\beta ^{+})_{0\\nu}$ and electron-positron conversion $(\\varepsilon \\beta ^{+})_{0\\nu}$ modes due to the exchange of light and heavy Majorana neutrinos, respectively, are calculated for $^{96}$Ru, $^{102}$Pd, $^{106}$Cd, $^{124}$Xe, $^{130}$Ba and $^{156}$Dy isotopes by employing the PHFB model with four different parameterization of the pairing plus multipolar two-body interactions and three different parameterizations of the Jastrow short range correlations. In all c","authors_text":"J. G. Hirsch, K. Chaturvedi, P. K. Raina, P. K. Rath, P. Lohani, R. Chandra","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-10-19T10:14:12Z","title":"Uncertainties in nuclear transition matrix elements for $\\beta ^{+}\\beta ^{+}$ and $\\varepsilon \\beta ^{+}$ modes of neutrinoless positron double-$\\beta $ decay within PHFB model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.5367","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:ba41d552a6ab95d9827a520545d5f9b890e3f51c978fe6cb6f343e9d0cd912d8","target":"record","created_at":"2026-05-18T01:53:45Z","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":"a429250388a6ae0b1fd64497266fd82db1816b296ef3e8ce7f85643ab5119056","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-10-19T10:14:12Z","title_canon_sha256":"fdf6065f0d430b6629283ad6aab41ae7c9ce6b55a8c3f32a3069142cd8a26017"},"schema_version":"1.0","source":{"id":"1210.5367","kind":"arxiv","version":2}},"canonical_sha256":"4c352bf243007d5319cc300e8ec5714188449928747959d74d9a2a1d3f3c4205","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4c352bf243007d5319cc300e8ec5714188449928747959d74d9a2a1d3f3c4205","first_computed_at":"2026-05-18T01:53:45.998061Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:53:45.998061Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bdvF5yP83PlLFe7Cxp37Sa/X9A56qsOt+jcnfHGhfWG5q+mIZjhf37mOmnkH2dquoamqUNVDquTm+L1LlkHBCw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:53:45.998850Z","signed_message":"canonical_sha256_bytes"},"source_id":"1210.5367","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ba41d552a6ab95d9827a520545d5f9b890e3f51c978fe6cb6f343e9d0cd912d8","sha256:2f2b44485da6ecdcbd581381a4242426555ac27315ee1e62fefaaf49f8408b8c"],"state_sha256":"b4af3d1e99f5514ef0385af5a0bd39c32bf561d3086bdc757132f8e099551f26"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wxPlaogoM6ia6zNQOi58hY9snNhj1FhqaomWL77ig5v7fveYN3tuabDKhOiowD3XuXk/vvvAs6vdemeuiklkDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T09:03:47.745880Z","bundle_sha256":"a438bfb7b983e974ff0c44926c19b8c29add9abcaa0f2cf4d00eba775ba18326"}}