{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1995:2LSKRT3AUG33WMKTKX4D5FJ7FZ","short_pith_number":"pith:2LSKRT3A","canonical_record":{"source":{"id":"hep-ph/9512439","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-12-29T04:40:30Z","cross_cats_sorted":["astro-ph","hep-th"],"title_canon_sha256":"db22891bf24998fbf28f1c7b5f513355e634af1299df81d19aa4084e72e8564e","abstract_canon_sha256":"7c41d2109c4c2f876201b8643472ebd0bb7d9bcac6c5f42c4f58bfa3a3a34928"},"schema_version":"1.0"},"canonical_sha256":"d2e4a8cf60a1b7bb315355f83e953f2e7957302e565c7a2da4e6826e9cc9eb44","source":{"kind":"arxiv","id":"hep-ph/9512439","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9512439","created_at":"2026-07-04T15:49:39Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9512439v3","created_at":"2026-07-04T15:49:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9512439","created_at":"2026-07-04T15:49:39Z"},{"alias_kind":"pith_short_12","alias_value":"2LSKRT3AUG33","created_at":"2026-07-04T15:49:39Z"},{"alias_kind":"pith_short_16","alias_value":"2LSKRT3AUG33WMKT","created_at":"2026-07-04T15:49:39Z"},{"alias_kind":"pith_short_8","alias_value":"2LSKRT3A","created_at":"2026-07-04T15:49:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1995:2LSKRT3AUG33WMKTKX4D5FJ7FZ","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9512439","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-12-29T04:40:30Z","cross_cats_sorted":["astro-ph","hep-th"],"title_canon_sha256":"db22891bf24998fbf28f1c7b5f513355e634af1299df81d19aa4084e72e8564e","abstract_canon_sha256":"7c41d2109c4c2f876201b8643472ebd0bb7d9bcac6c5f42c4f58bfa3a3a34928"},"schema_version":"1.0"},"canonical_sha256":"d2e4a8cf60a1b7bb315355f83e953f2e7957302e565c7a2da4e6826e9cc9eb44","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:49:39.343002Z","signature_b64":"Cfiy0FCqc33ewyRWYCciVkOWoL08CZTfFAJRSPiYm5oqVbLghkC6g6/eMMnjpDMEQStKrExZ4UJJx8lr5CdzBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d2e4a8cf60a1b7bb315355f83e953f2e7957302e565c7a2da4e6826e9cc9eb44","last_reissued_at":"2026-07-04T15:49:39.342512Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:49:39.342512Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9512439","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T15:49:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"i8E3xckEQz91ev96mlE3Cg50sDu4yY9KMNywkRny6edC0UgmxCsOrMw8r+e2jXE1FXKj8hZk+CkrClL+Y/ScCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T23:25:38.437148Z"},"content_sha256":"f21958bd2b5134872374a950deec241b2300be5587844d44cedf7b819931df54","schema_version":"1.0","event_id":"sha256:f21958bd2b5134872374a950deec241b2300be5587844d44cedf7b819931df54"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1995:2LSKRT3AUG33WMKTKX4D5FJ7FZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Supernatural Inflation: Inflation from Supersymmetry with No (Very) Small Parameters","license":"","headline":"","cross_cats":["astro-ph","hep-th"],"primary_cat":"hep-ph","authors_text":"Alan Guth, Lisa Randall, Marin Soljacic","submitted_at":"1995-12-29T04:40:30Z","abstract_excerpt":"Most models of inflation have small parameters, either to guarantee sufficient inflation or the correct magnitude of the density perturbations. In this paper we show that, in supersymmetric theories with weak scale supersymmetry breaking, one can construct viable inflationary models in which the requisite parameters appear naturally in the form of the ratio of mass scales that are already present in the theory. Successful inflationary models can be constructed from the flat-direction fields of a renormalizable supersymmetric potential, and such models can be realized even in the context of a s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9512439","kind":"arxiv","version":3},"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/hep-ph/9512439/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":"2026-07-04T15:49:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"km6W1SqAc4jboYKLT7ViQmoSrNbKIlacQwPFg3VqII2s88beHb65mGk24lMjHxVKbJLZifLzMtTsdroJCpTKBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T23:25:38.437649Z"},"content_sha256":"9901e2f36987e652a51a8bb574bea09a71deb649b8784522774c5c709d6fbd84","schema_version":"1.0","event_id":"sha256:9901e2f36987e652a51a8bb574bea09a71deb649b8784522774c5c709d6fbd84"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2LSKRT3AUG33WMKTKX4D5FJ7FZ/bundle.json","state_url":"https://pith.science/pith/2LSKRT3AUG33WMKTKX4D5FJ7FZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2LSKRT3AUG33WMKTKX4D5FJ7FZ/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":"2026-08-05T23:25:38Z","links":{"resolver":"https://pith.science/pith/2LSKRT3AUG33WMKTKX4D5FJ7FZ","bundle":"https://pith.science/pith/2LSKRT3AUG33WMKTKX4D5FJ7FZ/bundle.json","state":"https://pith.science/pith/2LSKRT3AUG33WMKTKX4D5FJ7FZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2LSKRT3AUG33WMKTKX4D5FJ7FZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1995:2LSKRT3AUG33WMKTKX4D5FJ7FZ","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":"7c41d2109c4c2f876201b8643472ebd0bb7d9bcac6c5f42c4f58bfa3a3a34928","cross_cats_sorted":["astro-ph","hep-th"],"license":"","primary_cat":"hep-ph","submitted_at":"1995-12-29T04:40:30Z","title_canon_sha256":"db22891bf24998fbf28f1c7b5f513355e634af1299df81d19aa4084e72e8564e"},"schema_version":"1.0","source":{"id":"hep-ph/9512439","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9512439","created_at":"2026-07-04T15:49:39Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9512439v3","created_at":"2026-07-04T15:49:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9512439","created_at":"2026-07-04T15:49:39Z"},{"alias_kind":"pith_short_12","alias_value":"2LSKRT3AUG33","created_at":"2026-07-04T15:49:39Z"},{"alias_kind":"pith_short_16","alias_value":"2LSKRT3AUG33WMKT","created_at":"2026-07-04T15:49:39Z"},{"alias_kind":"pith_short_8","alias_value":"2LSKRT3A","created_at":"2026-07-04T15:49:39Z"}],"graph_snapshots":[{"event_id":"sha256:9901e2f36987e652a51a8bb574bea09a71deb649b8784522774c5c709d6fbd84","target":"graph","created_at":"2026-07-04T15:49:39Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-ph/9512439/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Most models of inflation have small parameters, either to guarantee sufficient inflation or the correct magnitude of the density perturbations. In this paper we show that, in supersymmetric theories with weak scale supersymmetry breaking, one can construct viable inflationary models in which the requisite parameters appear naturally in the form of the ratio of mass scales that are already present in the theory. Successful inflationary models can be constructed from the flat-direction fields of a renormalizable supersymmetric potential, and such models can be realized even in the context of a s","authors_text":"Alan Guth, Lisa Randall, Marin Soljacic","cross_cats":["astro-ph","hep-th"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1995-12-29T04:40:30Z","title":"Supernatural Inflation: Inflation from Supersymmetry with No (Very) Small Parameters"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9512439","kind":"arxiv","version":3},"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:f21958bd2b5134872374a950deec241b2300be5587844d44cedf7b819931df54","target":"record","created_at":"2026-07-04T15:49:39Z","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":"7c41d2109c4c2f876201b8643472ebd0bb7d9bcac6c5f42c4f58bfa3a3a34928","cross_cats_sorted":["astro-ph","hep-th"],"license":"","primary_cat":"hep-ph","submitted_at":"1995-12-29T04:40:30Z","title_canon_sha256":"db22891bf24998fbf28f1c7b5f513355e634af1299df81d19aa4084e72e8564e"},"schema_version":"1.0","source":{"id":"hep-ph/9512439","kind":"arxiv","version":3}},"canonical_sha256":"d2e4a8cf60a1b7bb315355f83e953f2e7957302e565c7a2da4e6826e9cc9eb44","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d2e4a8cf60a1b7bb315355f83e953f2e7957302e565c7a2da4e6826e9cc9eb44","first_computed_at":"2026-07-04T15:49:39.342512Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:49:39.342512Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Cfiy0FCqc33ewyRWYCciVkOWoL08CZTfFAJRSPiYm5oqVbLghkC6g6/eMMnjpDMEQStKrExZ4UJJx8lr5CdzBA==","signature_status":"signed_v1","signed_at":"2026-07-04T15:49:39.343002Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9512439","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f21958bd2b5134872374a950deec241b2300be5587844d44cedf7b819931df54","sha256:9901e2f36987e652a51a8bb574bea09a71deb649b8784522774c5c709d6fbd84"],"state_sha256":"1c9ba208bc444495cf7222b9e7b774519b597274b0cff8a4aa46a2e531ddb0f5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JMRoTALMBMvftpEUue5sKvqDdEeQLKNeF29auIvGw1imY9yJVsGdG96gdbyynbodfzrpNOrKYpfUj28hTiAgDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-05T23:25:38.440989Z","bundle_sha256":"32f23badea613cccb423218af3b9299435333e6095546807e7a9ac4fc6fc6ddb"}}