{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:KGIE7JXYEKMKNRL7MAMNMAPDTB","short_pith_number":"pith:KGIE7JXY","canonical_record":{"source":{"id":"1308.1291","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-08-06T14:57:21Z","cross_cats_sorted":[],"title_canon_sha256":"cf97dcaaeed1bd57aeb7f811cc0b3360b42650c4f5d8b2909e070e1e96bb4eb1","abstract_canon_sha256":"6e816318bb628cd6eda156d36ff708648ac6f44d05087b1c8cb080348e48f0ad"},"schema_version":"1.0"},"canonical_sha256":"51904fa6f82298a6c57f6018d601e398492f8abacb3a68dd57575ff41dc63613","source":{"kind":"arxiv","id":"1308.1291","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1308.1291","created_at":"2026-05-18T02:55:04Z"},{"alias_kind":"arxiv_version","alias_value":"1308.1291v2","created_at":"2026-05-18T02:55:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.1291","created_at":"2026-05-18T02:55:04Z"},{"alias_kind":"pith_short_12","alias_value":"KGIE7JXYEKMK","created_at":"2026-05-18T12:27:49Z"},{"alias_kind":"pith_short_16","alias_value":"KGIE7JXYEKMKNRL7","created_at":"2026-05-18T12:27:49Z"},{"alias_kind":"pith_short_8","alias_value":"KGIE7JXY","created_at":"2026-05-18T12:27:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:KGIE7JXYEKMKNRL7MAMNMAPDTB","target":"record","payload":{"canonical_record":{"source":{"id":"1308.1291","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-08-06T14:57:21Z","cross_cats_sorted":[],"title_canon_sha256":"cf97dcaaeed1bd57aeb7f811cc0b3360b42650c4f5d8b2909e070e1e96bb4eb1","abstract_canon_sha256":"6e816318bb628cd6eda156d36ff708648ac6f44d05087b1c8cb080348e48f0ad"},"schema_version":"1.0"},"canonical_sha256":"51904fa6f82298a6c57f6018d601e398492f8abacb3a68dd57575ff41dc63613","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:55:04.023244Z","signature_b64":"CwylyYEmetrox2Mdpt+hk69dMlp/+aOntjeBkvfELpYcb1V0Oys/p2ogIu+U0KNSBlyZp5RhGo8kLE1P+cf6AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"51904fa6f82298a6c57f6018d601e398492f8abacb3a68dd57575ff41dc63613","last_reissued_at":"2026-05-18T02:55:04.022801Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:55:04.022801Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1308.1291","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":"2026-05-18T02:55:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oeDxXadsWZ6ajNh9XP46kMDO5Oz1ikIC9iW7BcdGhU1VeuiaKWeVOwEs0HwDvlJ2h53Bq6tKyqdFDeof09PMBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T15:37:34.856522Z"},"content_sha256":"aad9aedd7e1f6e804c8f381ec858ab8c6caa9e25d979de5f7131aeef152b9ec9","schema_version":"1.0","event_id":"sha256:aad9aedd7e1f6e804c8f381ec858ab8c6caa9e25d979de5f7131aeef152b9ec9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:KGIE7JXYEKMKNRL7MAMNMAPDTB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Constraining a class of B-L extended models from vacuum stability and perturbativity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Joydeep Chakrabortty, Partha Konar, Tanmoy Mondal","submitted_at":"2013-08-06T14:57:21Z","abstract_excerpt":"The precise knowledge of the Standard Model Higgs boson and top quark masses and couplings are crucial to understand the physics beyond it. SM like Higgs boson having mass in the range of 123-127 GeV squeezes the parameters for beyond standard model. In recent LHC era many TeV scale neutrino mass models have earned much attention as they pose many interesting phenomenological aspects. We have contemplated B-L extended models which are theoretically well motivated and phenomenologically interesting, and successfully explain neutrino mass generation. In this article we have analysed the detailed"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.1291","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":"2026-05-18T02:55:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"21suKz6gBE7Ag2M7eShO8GyehJ8j/2VcbRnDpf5R/8ux64x+hj9Y7hZh7h1GHQjJIX0yuWWYs4RLWdmUJxX2Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T15:37:34.856919Z"},"content_sha256":"c5ece6c2853230aac47e5148cc1940e27c34a82a62d15ea19c4a300eb0327b72","schema_version":"1.0","event_id":"sha256:c5ece6c2853230aac47e5148cc1940e27c34a82a62d15ea19c4a300eb0327b72"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KGIE7JXYEKMKNRL7MAMNMAPDTB/bundle.json","state_url":"https://pith.science/pith/KGIE7JXYEKMKNRL7MAMNMAPDTB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KGIE7JXYEKMKNRL7MAMNMAPDTB/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":"2026-05-22T15:37:34Z","links":{"resolver":"https://pith.science/pith/KGIE7JXYEKMKNRL7MAMNMAPDTB","bundle":"https://pith.science/pith/KGIE7JXYEKMKNRL7MAMNMAPDTB/bundle.json","state":"https://pith.science/pith/KGIE7JXYEKMKNRL7MAMNMAPDTB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KGIE7JXYEKMKNRL7MAMNMAPDTB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:KGIE7JXYEKMKNRL7MAMNMAPDTB","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":"6e816318bb628cd6eda156d36ff708648ac6f44d05087b1c8cb080348e48f0ad","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-08-06T14:57:21Z","title_canon_sha256":"cf97dcaaeed1bd57aeb7f811cc0b3360b42650c4f5d8b2909e070e1e96bb4eb1"},"schema_version":"1.0","source":{"id":"1308.1291","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1308.1291","created_at":"2026-05-18T02:55:04Z"},{"alias_kind":"arxiv_version","alias_value":"1308.1291v2","created_at":"2026-05-18T02:55:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.1291","created_at":"2026-05-18T02:55:04Z"},{"alias_kind":"pith_short_12","alias_value":"KGIE7JXYEKMK","created_at":"2026-05-18T12:27:49Z"},{"alias_kind":"pith_short_16","alias_value":"KGIE7JXYEKMKNRL7","created_at":"2026-05-18T12:27:49Z"},{"alias_kind":"pith_short_8","alias_value":"KGIE7JXY","created_at":"2026-05-18T12:27:49Z"}],"graph_snapshots":[{"event_id":"sha256:c5ece6c2853230aac47e5148cc1940e27c34a82a62d15ea19c4a300eb0327b72","target":"graph","created_at":"2026-05-18T02:55:04Z","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":"The precise knowledge of the Standard Model Higgs boson and top quark masses and couplings are crucial to understand the physics beyond it. SM like Higgs boson having mass in the range of 123-127 GeV squeezes the parameters for beyond standard model. In recent LHC era many TeV scale neutrino mass models have earned much attention as they pose many interesting phenomenological aspects. We have contemplated B-L extended models which are theoretically well motivated and phenomenologically interesting, and successfully explain neutrino mass generation. In this article we have analysed the detailed","authors_text":"Joydeep Chakrabortty, Partha Konar, Tanmoy Mondal","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-08-06T14:57:21Z","title":"Constraining a class of B-L extended models from vacuum stability and perturbativity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.1291","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:aad9aedd7e1f6e804c8f381ec858ab8c6caa9e25d979de5f7131aeef152b9ec9","target":"record","created_at":"2026-05-18T02:55:04Z","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":"6e816318bb628cd6eda156d36ff708648ac6f44d05087b1c8cb080348e48f0ad","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-08-06T14:57:21Z","title_canon_sha256":"cf97dcaaeed1bd57aeb7f811cc0b3360b42650c4f5d8b2909e070e1e96bb4eb1"},"schema_version":"1.0","source":{"id":"1308.1291","kind":"arxiv","version":2}},"canonical_sha256":"51904fa6f82298a6c57f6018d601e398492f8abacb3a68dd57575ff41dc63613","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"51904fa6f82298a6c57f6018d601e398492f8abacb3a68dd57575ff41dc63613","first_computed_at":"2026-05-18T02:55:04.022801Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:55:04.022801Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"CwylyYEmetrox2Mdpt+hk69dMlp/+aOntjeBkvfELpYcb1V0Oys/p2ogIu+U0KNSBlyZp5RhGo8kLE1P+cf6AQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:55:04.023244Z","signed_message":"canonical_sha256_bytes"},"source_id":"1308.1291","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:aad9aedd7e1f6e804c8f381ec858ab8c6caa9e25d979de5f7131aeef152b9ec9","sha256:c5ece6c2853230aac47e5148cc1940e27c34a82a62d15ea19c4a300eb0327b72"],"state_sha256":"f5f81b834d179f862780e2a0d46120e6eed6bf88693d1fe41fed982f533676af"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qvp5ORaOLL3hb4zrN5g5ES4rlFWk9A1fxYB8IA4Meq4w2W4bw9BPMT7dqPmjWXEYhvZZ2Vd4ZMclwP1qZY6jBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-22T15:37:34.859898Z","bundle_sha256":"9b6848d8b2e72842ffc638ec5cfc5e7c4b9431c1300bb609ef2fe1ec361fe9a6"}}