{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:BT2CSKLRI2EWQBXACKL4FDH7I5","short_pith_number":"pith:BT2CSKLR","canonical_record":{"source":{"id":"1011.2214","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-11-09T21:05:24Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"e3fd6ad19874cc7a85c55902e946f9cae23665dfb189b8e616aa20017f9c5351","abstract_canon_sha256":"c189d19d15553bce596f890d7791e267ca02250bd788f035101911608efa5888"},"schema_version":"1.0"},"canonical_sha256":"0cf429297146896806e01297c28cff47464ad87c7518bf487986992c14002c17","source":{"kind":"arxiv","id":"1011.2214","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1011.2214","created_at":"2026-05-18T04:28:39Z"},{"alias_kind":"arxiv_version","alias_value":"1011.2214v2","created_at":"2026-05-18T04:28:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.2214","created_at":"2026-05-18T04:28:39Z"},{"alias_kind":"pith_short_12","alias_value":"BT2CSKLRI2EW","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_16","alias_value":"BT2CSKLRI2EWQBXA","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_8","alias_value":"BT2CSKLR","created_at":"2026-05-18T12:26:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:BT2CSKLRI2EWQBXACKL4FDH7I5","target":"record","payload":{"canonical_record":{"source":{"id":"1011.2214","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-11-09T21:05:24Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"e3fd6ad19874cc7a85c55902e946f9cae23665dfb189b8e616aa20017f9c5351","abstract_canon_sha256":"c189d19d15553bce596f890d7791e267ca02250bd788f035101911608efa5888"},"schema_version":"1.0"},"canonical_sha256":"0cf429297146896806e01297c28cff47464ad87c7518bf487986992c14002c17","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:28:39.049364Z","signature_b64":"vdFrv35FVWzKRLU5OR1oAy/ZK9k7BQpmCueDmP4GVvBImFhwOMksKULawQLQa/6HLtrqJGv5oc2qGqegXCvFCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0cf429297146896806e01297c28cff47464ad87c7518bf487986992c14002c17","last_reissued_at":"2026-05-18T04:28:39.048980Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:28:39.048980Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1011.2214","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":"2026-05-18T04:28:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8tG+J3Cm8MNpbE8yhKjprMcXp31hUnZ+rOlPi55dI9mqY17ohiKtNTGVUU4Q82MO8C+OrmCwprDJMfILCLGuCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T22:06:01.150256Z"},"content_sha256":"acff627b1f22ebbc6e341d6330afb643e3b78fc49ecce8f958052e66a101c4d8","schema_version":"1.0","event_id":"sha256:acff627b1f22ebbc6e341d6330afb643e3b78fc49ecce8f958052e66a101c4d8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:BT2CSKLRI2EWQBXACKL4FDH7I5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamical R-parity Breaking at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Dilip Kumar Ghosh, Rabindra N. Mohapatra, Shao-Long Chen, Yue Zhang","submitted_at":"2010-11-09T21:05:24Z","abstract_excerpt":"In a class of extensions of the minimal supersymmetric standard model with (B-L)/left-right symmetry that explains the neutrino masses, breaking R-parity symmetry is an essential and dynamical requirement for successful gauge symmetry breaking. Two consequences of these models are: (i) a new kind of R-parity breaking interaction that protects proton stability but adds new contributions to neutrinoless double beta decay and (ii) an upper bound on the extra gauge and parity symmetry breaking scale which is within the large hadron collider (LHC) energy range. We point out that an important predic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.2214","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":"2026-05-18T04:28:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aZeniE6c7jHRVNN1lOlPOECVk86xN6WvJ6ck61rU3EZFQkme5KDui1jhejlWZVjcciAT2yI64awJEAQ+Vo9iDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T22:06:01.150898Z"},"content_sha256":"ee9402c29bbb05f6c09d30927aea6caaff8a41cdeba8d78600a1c0e6abe468ae","schema_version":"1.0","event_id":"sha256:ee9402c29bbb05f6c09d30927aea6caaff8a41cdeba8d78600a1c0e6abe468ae"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BT2CSKLRI2EWQBXACKL4FDH7I5/bundle.json","state_url":"https://pith.science/pith/BT2CSKLRI2EWQBXACKL4FDH7I5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BT2CSKLRI2EWQBXACKL4FDH7I5/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":"2026-06-03T22:06:01Z","links":{"resolver":"https://pith.science/pith/BT2CSKLRI2EWQBXACKL4FDH7I5","bundle":"https://pith.science/pith/BT2CSKLRI2EWQBXACKL4FDH7I5/bundle.json","state":"https://pith.science/pith/BT2CSKLRI2EWQBXACKL4FDH7I5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BT2CSKLRI2EWQBXACKL4FDH7I5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:BT2CSKLRI2EWQBXACKL4FDH7I5","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":"c189d19d15553bce596f890d7791e267ca02250bd788f035101911608efa5888","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-11-09T21:05:24Z","title_canon_sha256":"e3fd6ad19874cc7a85c55902e946f9cae23665dfb189b8e616aa20017f9c5351"},"schema_version":"1.0","source":{"id":"1011.2214","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1011.2214","created_at":"2026-05-18T04:28:39Z"},{"alias_kind":"arxiv_version","alias_value":"1011.2214v2","created_at":"2026-05-18T04:28:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.2214","created_at":"2026-05-18T04:28:39Z"},{"alias_kind":"pith_short_12","alias_value":"BT2CSKLRI2EW","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_16","alias_value":"BT2CSKLRI2EWQBXA","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_8","alias_value":"BT2CSKLR","created_at":"2026-05-18T12:26:05Z"}],"graph_snapshots":[{"event_id":"sha256:ee9402c29bbb05f6c09d30927aea6caaff8a41cdeba8d78600a1c0e6abe468ae","target":"graph","created_at":"2026-05-18T04:28:39Z","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":"In a class of extensions of the minimal supersymmetric standard model with (B-L)/left-right symmetry that explains the neutrino masses, breaking R-parity symmetry is an essential and dynamical requirement for successful gauge symmetry breaking. Two consequences of these models are: (i) a new kind of R-parity breaking interaction that protects proton stability but adds new contributions to neutrinoless double beta decay and (ii) an upper bound on the extra gauge and parity symmetry breaking scale which is within the large hadron collider (LHC) energy range. We point out that an important predic","authors_text":"Dilip Kumar Ghosh, Rabindra N. Mohapatra, Shao-Long Chen, Yue Zhang","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-11-09T21:05:24Z","title":"Dynamical R-parity Breaking at the LHC"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.2214","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:acff627b1f22ebbc6e341d6330afb643e3b78fc49ecce8f958052e66a101c4d8","target":"record","created_at":"2026-05-18T04:28:39Z","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":"c189d19d15553bce596f890d7791e267ca02250bd788f035101911608efa5888","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-11-09T21:05:24Z","title_canon_sha256":"e3fd6ad19874cc7a85c55902e946f9cae23665dfb189b8e616aa20017f9c5351"},"schema_version":"1.0","source":{"id":"1011.2214","kind":"arxiv","version":2}},"canonical_sha256":"0cf429297146896806e01297c28cff47464ad87c7518bf487986992c14002c17","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0cf429297146896806e01297c28cff47464ad87c7518bf487986992c14002c17","first_computed_at":"2026-05-18T04:28:39.048980Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:28:39.048980Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vdFrv35FVWzKRLU5OR1oAy/ZK9k7BQpmCueDmP4GVvBImFhwOMksKULawQLQa/6HLtrqJGv5oc2qGqegXCvFCw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:28:39.049364Z","signed_message":"canonical_sha256_bytes"},"source_id":"1011.2214","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:acff627b1f22ebbc6e341d6330afb643e3b78fc49ecce8f958052e66a101c4d8","sha256:ee9402c29bbb05f6c09d30927aea6caaff8a41cdeba8d78600a1c0e6abe468ae"],"state_sha256":"9b1c3711239e802fa9b05450eafe22b7616f0fd91a8be086f1a6ff7874fc5576"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yG+qDsopOTHU0MI6a3/PMMwqEDS+P0I4CS71NXYBv+aPHjXPFKxMKXq9mOwWGFUM61/IRPy3n0NoXpBpECqfDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T22:06:01.152968Z","bundle_sha256":"cc9dcc0c74af4d9b4a094bb926158f6e1d85e67e8423a47cd784a5ce073b6de7"}}