{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2019:SNADJ57JAM6G6I6WKD7YEVV6DY","short_pith_number":"pith:SNADJ57J","canonical_record":{"source":{"id":"1909.00784","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-09-02T16:15:13Z","cross_cats_sorted":[],"title_canon_sha256":"608375616e4b09664e92f2b392adbdab91dd1779f8f8cf8ab8a8757a98b7fabf","abstract_canon_sha256":"87c87280199ac087b9440679eebf9792f01214f289045e36104764257cac17a4"},"schema_version":"1.0"},"canonical_sha256":"934034f7e9033c6f23d650ff8256be1e29523857f9d3f5faff696a7837c56f41","source":{"kind":"arxiv","id":"1909.00784","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1909.00784","created_at":"2026-07-05T00:01:13Z"},{"alias_kind":"arxiv_version","alias_value":"1909.00784v1","created_at":"2026-07-05T00:01:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1909.00784","created_at":"2026-07-05T00:01:13Z"},{"alias_kind":"pith_short_12","alias_value":"SNADJ57JAM6G","created_at":"2026-07-05T00:01:13Z"},{"alias_kind":"pith_short_16","alias_value":"SNADJ57JAM6G6I6W","created_at":"2026-07-05T00:01:13Z"},{"alias_kind":"pith_short_8","alias_value":"SNADJ57J","created_at":"2026-07-05T00:01:13Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2019:SNADJ57JAM6G6I6WKD7YEVV6DY","target":"record","payload":{"canonical_record":{"source":{"id":"1909.00784","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-09-02T16:15:13Z","cross_cats_sorted":[],"title_canon_sha256":"608375616e4b09664e92f2b392adbdab91dd1779f8f8cf8ab8a8757a98b7fabf","abstract_canon_sha256":"87c87280199ac087b9440679eebf9792f01214f289045e36104764257cac17a4"},"schema_version":"1.0"},"canonical_sha256":"934034f7e9033c6f23d650ff8256be1e29523857f9d3f5faff696a7837c56f41","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:01:13.032339Z","signature_b64":"RLcKxNelOfSi4SxrRZ8qT1CCKTXcJ2fHoBq6pn0PtToqJQLJtzAwPeRcRJ88npn3uRh7ltu+ysu0cGKfJbvrAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"934034f7e9033c6f23d650ff8256be1e29523857f9d3f5faff696a7837c56f41","last_reissued_at":"2026-07-05T00:01:13.031999Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:01:13.031999Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1909.00784","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":"2026-07-05T00:01:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gvbbMuOX6sPqb+t3LopLxwU9iyzh3WyuFS8DxxEet9lCLp1AAsABTfqpfd93i8fRDPRub00RIg/XH2Zioyo9Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T18:40:51.303996Z"},"content_sha256":"efa93a6e4d4bd28d23871bb7978d90f6bf67d7cd5b5beeb1388099b1d5158a99","schema_version":"1.0","event_id":"sha256:efa93a6e4d4bd28d23871bb7978d90f6bf67d7cd5b5beeb1388099b1d5158a99"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2019:SNADJ57JAM6G6I6WKD7YEVV6DY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Higgs masses and couplings in the general 2HDM with unitarity bounds","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D. Jur\\v{c}iukonis, L. Lavoura","submitted_at":"2019-09-02T16:15:13Z","abstract_excerpt":"We investigate the general two Higgs doublet model imposing both the unitarity conditions and the bounded-from-below conditions. Both types of conditions restrict the ranges of the parameters of the scalar potential. We study the model in the Higgs basis, i.e. in the basis for the scalar doublets where only one doublet has vacuum expectation value. We use the experimental bounds on the oblique parameter T, to produce scalar particles with masses and cubic and quartic couplings of the Higgs in agreement with the phenomenology. The numerical calculations show that the cubic coupling may be up to"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1909.00784","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1909.00784/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T00:01:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2B/+j5Y62zAoJCOh3bJAK9B6TTWhBoODdr17NEz016insUD6XXbGVXl8g4CzDrx20opzKFhxHfLeRiDCZqIJAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T18:40:51.304495Z"},"content_sha256":"423d2f8658367a1ec3e46e5f7f86bd02f87a10d8cefc2dd8cbf3b5640d0b14ca","schema_version":"1.0","event_id":"sha256:423d2f8658367a1ec3e46e5f7f86bd02f87a10d8cefc2dd8cbf3b5640d0b14ca"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SNADJ57JAM6G6I6WKD7YEVV6DY/bundle.json","state_url":"https://pith.science/pith/SNADJ57JAM6G6I6WKD7YEVV6DY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SNADJ57JAM6G6I6WKD7YEVV6DY/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":"2026-08-15T18:40:51Z","links":{"resolver":"https://pith.science/pith/SNADJ57JAM6G6I6WKD7YEVV6DY","bundle":"https://pith.science/pith/SNADJ57JAM6G6I6WKD7YEVV6DY/bundle.json","state":"https://pith.science/pith/SNADJ57JAM6G6I6WKD7YEVV6DY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SNADJ57JAM6G6I6WKD7YEVV6DY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:SNADJ57JAM6G6I6WKD7YEVV6DY","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":"87c87280199ac087b9440679eebf9792f01214f289045e36104764257cac17a4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-09-02T16:15:13Z","title_canon_sha256":"608375616e4b09664e92f2b392adbdab91dd1779f8f8cf8ab8a8757a98b7fabf"},"schema_version":"1.0","source":{"id":"1909.00784","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1909.00784","created_at":"2026-07-05T00:01:13Z"},{"alias_kind":"arxiv_version","alias_value":"1909.00784v1","created_at":"2026-07-05T00:01:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1909.00784","created_at":"2026-07-05T00:01:13Z"},{"alias_kind":"pith_short_12","alias_value":"SNADJ57JAM6G","created_at":"2026-07-05T00:01:13Z"},{"alias_kind":"pith_short_16","alias_value":"SNADJ57JAM6G6I6W","created_at":"2026-07-05T00:01:13Z"},{"alias_kind":"pith_short_8","alias_value":"SNADJ57J","created_at":"2026-07-05T00:01:13Z"}],"graph_snapshots":[{"event_id":"sha256:423d2f8658367a1ec3e46e5f7f86bd02f87a10d8cefc2dd8cbf3b5640d0b14ca","target":"graph","created_at":"2026-07-05T00:01:13Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/1909.00784/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate the general two Higgs doublet model imposing both the unitarity conditions and the bounded-from-below conditions. Both types of conditions restrict the ranges of the parameters of the scalar potential. We study the model in the Higgs basis, i.e. in the basis for the scalar doublets where only one doublet has vacuum expectation value. We use the experimental bounds on the oblique parameter T, to produce scalar particles with masses and cubic and quartic couplings of the Higgs in agreement with the phenomenology. The numerical calculations show that the cubic coupling may be up to","authors_text":"D. Jur\\v{c}iukonis, L. Lavoura","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-09-02T16:15:13Z","title":"Higgs masses and couplings in the general 2HDM with unitarity bounds"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1909.00784","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:efa93a6e4d4bd28d23871bb7978d90f6bf67d7cd5b5beeb1388099b1d5158a99","target":"record","created_at":"2026-07-05T00:01:13Z","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":"87c87280199ac087b9440679eebf9792f01214f289045e36104764257cac17a4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-09-02T16:15:13Z","title_canon_sha256":"608375616e4b09664e92f2b392adbdab91dd1779f8f8cf8ab8a8757a98b7fabf"},"schema_version":"1.0","source":{"id":"1909.00784","kind":"arxiv","version":1}},"canonical_sha256":"934034f7e9033c6f23d650ff8256be1e29523857f9d3f5faff696a7837c56f41","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"934034f7e9033c6f23d650ff8256be1e29523857f9d3f5faff696a7837c56f41","first_computed_at":"2026-07-05T00:01:13.031999Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:01:13.031999Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"RLcKxNelOfSi4SxrRZ8qT1CCKTXcJ2fHoBq6pn0PtToqJQLJtzAwPeRcRJ88npn3uRh7ltu+ysu0cGKfJbvrAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T00:01:13.032339Z","signed_message":"canonical_sha256_bytes"},"source_id":"1909.00784","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:efa93a6e4d4bd28d23871bb7978d90f6bf67d7cd5b5beeb1388099b1d5158a99","sha256:423d2f8658367a1ec3e46e5f7f86bd02f87a10d8cefc2dd8cbf3b5640d0b14ca"],"state_sha256":"492e55a029d226e74367ea161335993476a31299af6f0a93675f7ce01512c27f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oCj7/XZCI6c+2Zdn0toOKcYTVMaZQH2k0s842l2EbR1sihAmV+BidqSP2yLUh6IsG/LCfI6SXPe2B4RmoJpCAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-15T18:40:51.308474Z","bundle_sha256":"6f8e3c00aeb0045fa2862ccece6637e58bf747f78f1a20247907e90d91764f79"}}