{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:EFK3WBOVSXLDX3MJHSJCIORAP6","short_pith_number":"pith:EFK3WBOV","canonical_record":{"source":{"id":"2504.02121","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-04-02T20:46:53Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"10aca7604d81f991551418158a2fb7f186d2841799074bdfb9382dd981ad45a0","abstract_canon_sha256":"6f86ddf5a3b291bd28b79f5d38867f229f53282ac5ae7b90cbb7a71017cc3f6d"},"schema_version":"1.0"},"canonical_sha256":"2155bb05d595d63bed893c92243a207f9de95073f60e7a2516e069eb5e07b1db","source":{"kind":"arxiv","id":"2504.02121","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2504.02121","created_at":"2026-07-05T10:43:50Z"},{"alias_kind":"arxiv_version","alias_value":"2504.02121v1","created_at":"2026-07-05T10:43:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2504.02121","created_at":"2026-07-05T10:43:50Z"},{"alias_kind":"pith_short_12","alias_value":"EFK3WBOVSXLD","created_at":"2026-07-05T10:43:50Z"},{"alias_kind":"pith_short_16","alias_value":"EFK3WBOVSXLDX3MJ","created_at":"2026-07-05T10:43:50Z"},{"alias_kind":"pith_short_8","alias_value":"EFK3WBOV","created_at":"2026-07-05T10:43:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:EFK3WBOVSXLDX3MJHSJCIORAP6","target":"record","payload":{"canonical_record":{"source":{"id":"2504.02121","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-04-02T20:46:53Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"10aca7604d81f991551418158a2fb7f186d2841799074bdfb9382dd981ad45a0","abstract_canon_sha256":"6f86ddf5a3b291bd28b79f5d38867f229f53282ac5ae7b90cbb7a71017cc3f6d"},"schema_version":"1.0"},"canonical_sha256":"2155bb05d595d63bed893c92243a207f9de95073f60e7a2516e069eb5e07b1db","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:43:50.903547Z","signature_b64":"jnnG6PBrijUl+1fn+Dr0O924o/Z/+qOqVREBOZTdlncrTVqnV9gUL+swRUABu4SkoT8gbrWOgwKUC9kuK719DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2155bb05d595d63bed893c92243a207f9de95073f60e7a2516e069eb5e07b1db","last_reissued_at":"2026-07-05T10:43:50.903161Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:43:50.903161Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2504.02121","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":"2026-07-05T10:43:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"svbLG7SGBmorM4EJG6vEK1cvBzavKSUyKJ8A5mSBaizaXVjuf0Csveh89Iea49S6u7fZIqc3rzqaKPMhOpBxDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T17:25:45.662748Z"},"content_sha256":"431ca426452e0b801b0405250e55085aba3d3304a64e0e0f89e4b68b832412ca","schema_version":"1.0","event_id":"sha256:431ca426452e0b801b0405250e55085aba3d3304a64e0e0f89e4b68b832412ca"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:EFK3WBOVSXLDX3MJHSJCIORAP6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"F-Term Hybrid Inflation and SUSY Breaking","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"C. Pallis","submitted_at":"2025-04-02T20:46:53Z","abstract_excerpt":"We consider F-term hybrid inflation and supersymmetry breaking in the context of a model which largely respects a global U(1) R symmetry. The Kaehler potential parameterizes the Kaehler manifold with an enhanced U(1)_Rx(SU(1,1)/U(1)) symmetry, where the scalar curvature of the second factor is determined by the achievement of a supersymmetry-breaking de Sitter vacuum without ugly tuning. The magnitude of the emergent soft tadpole term for the inflaton can be adjusted in the range (1.2-460) TeV -- increasing with the dimensionality of the representation of the waterfall fields -- so that the in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2504.02121","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/2504.02121/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":"2026-07-05T10:43:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ya/TzUn6HElYnBsRnWn3SiBB9DAUU8io1zPz20m6RBPOshWmuJdSycTHeGlnnI/7jqBGs9XWcB1kpTrLscNlAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T17:25:45.663280Z"},"content_sha256":"f18e2244c6c9875364a77513e5eb3b8f80277cf8e0ccec9a71dcc2ae91dcdada","schema_version":"1.0","event_id":"sha256:f18e2244c6c9875364a77513e5eb3b8f80277cf8e0ccec9a71dcc2ae91dcdada"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EFK3WBOVSXLDX3MJHSJCIORAP6/bundle.json","state_url":"https://pith.science/pith/EFK3WBOVSXLDX3MJHSJCIORAP6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EFK3WBOVSXLDX3MJHSJCIORAP6/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":"2026-08-03T17:25:45Z","links":{"resolver":"https://pith.science/pith/EFK3WBOVSXLDX3MJHSJCIORAP6","bundle":"https://pith.science/pith/EFK3WBOVSXLDX3MJHSJCIORAP6/bundle.json","state":"https://pith.science/pith/EFK3WBOVSXLDX3MJHSJCIORAP6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EFK3WBOVSXLDX3MJHSJCIORAP6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:EFK3WBOVSXLDX3MJHSJCIORAP6","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":"6f86ddf5a3b291bd28b79f5d38867f229f53282ac5ae7b90cbb7a71017cc3f6d","cross_cats_sorted":["astro-ph.CO","hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-04-02T20:46:53Z","title_canon_sha256":"10aca7604d81f991551418158a2fb7f186d2841799074bdfb9382dd981ad45a0"},"schema_version":"1.0","source":{"id":"2504.02121","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2504.02121","created_at":"2026-07-05T10:43:50Z"},{"alias_kind":"arxiv_version","alias_value":"2504.02121v1","created_at":"2026-07-05T10:43:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2504.02121","created_at":"2026-07-05T10:43:50Z"},{"alias_kind":"pith_short_12","alias_value":"EFK3WBOVSXLD","created_at":"2026-07-05T10:43:50Z"},{"alias_kind":"pith_short_16","alias_value":"EFK3WBOVSXLDX3MJ","created_at":"2026-07-05T10:43:50Z"},{"alias_kind":"pith_short_8","alias_value":"EFK3WBOV","created_at":"2026-07-05T10:43:50Z"}],"graph_snapshots":[{"event_id":"sha256:f18e2244c6c9875364a77513e5eb3b8f80277cf8e0ccec9a71dcc2ae91dcdada","target":"graph","created_at":"2026-07-05T10:43:50Z","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/2504.02121/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We consider F-term hybrid inflation and supersymmetry breaking in the context of a model which largely respects a global U(1) R symmetry. The Kaehler potential parameterizes the Kaehler manifold with an enhanced U(1)_Rx(SU(1,1)/U(1)) symmetry, where the scalar curvature of the second factor is determined by the achievement of a supersymmetry-breaking de Sitter vacuum without ugly tuning. The magnitude of the emergent soft tadpole term for the inflaton can be adjusted in the range (1.2-460) TeV -- increasing with the dimensionality of the representation of the waterfall fields -- so that the in","authors_text":"C. Pallis","cross_cats":["astro-ph.CO","hep-th"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-04-02T20:46:53Z","title":"F-Term Hybrid Inflation and SUSY Breaking"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2504.02121","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":"sha256:431ca426452e0b801b0405250e55085aba3d3304a64e0e0f89e4b68b832412ca","target":"record","created_at":"2026-07-05T10:43:50Z","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":"6f86ddf5a3b291bd28b79f5d38867f229f53282ac5ae7b90cbb7a71017cc3f6d","cross_cats_sorted":["astro-ph.CO","hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-04-02T20:46:53Z","title_canon_sha256":"10aca7604d81f991551418158a2fb7f186d2841799074bdfb9382dd981ad45a0"},"schema_version":"1.0","source":{"id":"2504.02121","kind":"arxiv","version":1}},"canonical_sha256":"2155bb05d595d63bed893c92243a207f9de95073f60e7a2516e069eb5e07b1db","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2155bb05d595d63bed893c92243a207f9de95073f60e7a2516e069eb5e07b1db","first_computed_at":"2026-07-05T10:43:50.903161Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:43:50.903161Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jnnG6PBrijUl+1fn+Dr0O924o/Z/+qOqVREBOZTdlncrTVqnV9gUL+swRUABu4SkoT8gbrWOgwKUC9kuK719DQ==","signature_status":"signed_v1","signed_at":"2026-07-05T10:43:50.903547Z","signed_message":"canonical_sha256_bytes"},"source_id":"2504.02121","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:431ca426452e0b801b0405250e55085aba3d3304a64e0e0f89e4b68b832412ca","sha256:f18e2244c6c9875364a77513e5eb3b8f80277cf8e0ccec9a71dcc2ae91dcdada"],"state_sha256":"79082752a4adb871fda60b45d51383667f727447adad06b6fd25788c24dd833f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4O3TrUf4CWiHNNjVwUP/GLc/2rRfYJ7k4sq+tKvJBBaZp3XuJo25vMsCclw5ZKXzlXsAkG4lRPBu/f8G2fiUBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T17:25:45.668677Z","bundle_sha256":"020d7acd75a948765264e1225e2ca8975b4edbab840ab5383efa0ee4653aa519"}}