{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:GM7VTO35SSSUMFIC6QFBJVKJID","short_pith_number":"pith:GM7VTO35","canonical_record":{"source":{"id":"1303.2618","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2013-03-11T19:01:24Z","cross_cats_sorted":["gr-qc","hep-th"],"title_canon_sha256":"8bb0e501eba9e6bd76c080b7386c1ba4074063ad574daf9e2b765c02fbaea087","abstract_canon_sha256":"636b85535646785efeb174e281b0a77581f62fe20f8547ece701048e489fc5b6"},"schema_version":"1.0"},"canonical_sha256":"333f59bb7d94a5461502f40a14d54940d5a26fb36c9de282658cf44be40acdc5","source":{"kind":"arxiv","id":"1303.2618","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.2618","created_at":"2026-05-18T01:51:08Z"},{"alias_kind":"arxiv_version","alias_value":"1303.2618v2","created_at":"2026-05-18T01:51:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.2618","created_at":"2026-05-18T01:51:08Z"},{"alias_kind":"pith_short_12","alias_value":"GM7VTO35SSSU","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"GM7VTO35SSSUMFIC","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"GM7VTO35","created_at":"2026-05-18T12:27:45Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:GM7VTO35SSSUMFIC6QFBJVKJID","target":"record","payload":{"canonical_record":{"source":{"id":"1303.2618","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2013-03-11T19:01:24Z","cross_cats_sorted":["gr-qc","hep-th"],"title_canon_sha256":"8bb0e501eba9e6bd76c080b7386c1ba4074063ad574daf9e2b765c02fbaea087","abstract_canon_sha256":"636b85535646785efeb174e281b0a77581f62fe20f8547ece701048e489fc5b6"},"schema_version":"1.0"},"canonical_sha256":"333f59bb7d94a5461502f40a14d54940d5a26fb36c9de282658cf44be40acdc5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:51:08.736969Z","signature_b64":"nhi6fBgBLXhFl7heQ/pstWiatQeUdeEWTFTt0nfniu2uOZS2Bon5mRUfEvhOGKtrBuPPkEufIfJZ6AsLFBCbAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"333f59bb7d94a5461502f40a14d54940d5a26fb36c9de282658cf44be40acdc5","last_reissued_at":"2026-05-18T01:51:08.736261Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:51:08.736261Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1303.2618","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":"2026-05-18T01:51:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fUNTAWOKQmJtUnEenktBkMly0mbXKbeYFsAI+iFDlJu73RX/copfXJ5uzULL6aMBSuCwFMfvWuDSIcmEnZirCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T21:10:43.755595Z"},"content_sha256":"1c3f6547ece4020bafb77ba9cbb261721067339ea678feae0caf2897009288d4","schema_version":"1.0","event_id":"sha256:1c3f6547ece4020bafb77ba9cbb261721067339ea678feae0caf2897009288d4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:GM7VTO35SSSUMFIC6QFBJVKJID","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"DBI Galileon in the Effective Field Theory of Inflation: Orthogonal non-Gaussianities and constraints from the Trispectrum","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-th"],"primary_cat":"astro-ph.CO","authors_text":"Sebastien Renaux-Petel","submitted_at":"2013-03-11T19:01:24Z","abstract_excerpt":"Very few explicit inflationary scenarios are known to generate a large bispectrum of orthogonal shape. Dirac-Born-Infeld Galileon inflation, in which an induced gravity term is added to the DBI action, is one such model. We formulate it in the language of the effective field theory of inflation by identifying the unitary gauge operators that govern the behavior of its cosmological fluctuations. We show how to recover rather easily from this its power spectrum and bispectrum, which we calculated previously using standard cosmological perturbation theory. We push our calculations up to the deter"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.2618","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":"2026-05-18T01:51:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"z88AfVkfjNFsjffczINqS9M3stdoFZ7NWTUgj6aKULQa73NKSfSdnZwXTpnZxzPuTz73DJIPa/YlpVt0fZ63Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T21:10:43.756276Z"},"content_sha256":"6a55dfe4b57ec9525b97a307848d044757380dedc9f157e4a51a9e7616062eee","schema_version":"1.0","event_id":"sha256:6a55dfe4b57ec9525b97a307848d044757380dedc9f157e4a51a9e7616062eee"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GM7VTO35SSSUMFIC6QFBJVKJID/bundle.json","state_url":"https://pith.science/pith/GM7VTO35SSSUMFIC6QFBJVKJID/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GM7VTO35SSSUMFIC6QFBJVKJID/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":"2026-05-28T21:10:43Z","links":{"resolver":"https://pith.science/pith/GM7VTO35SSSUMFIC6QFBJVKJID","bundle":"https://pith.science/pith/GM7VTO35SSSUMFIC6QFBJVKJID/bundle.json","state":"https://pith.science/pith/GM7VTO35SSSUMFIC6QFBJVKJID/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GM7VTO35SSSUMFIC6QFBJVKJID/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:GM7VTO35SSSUMFIC6QFBJVKJID","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":"636b85535646785efeb174e281b0a77581f62fe20f8547ece701048e489fc5b6","cross_cats_sorted":["gr-qc","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2013-03-11T19:01:24Z","title_canon_sha256":"8bb0e501eba9e6bd76c080b7386c1ba4074063ad574daf9e2b765c02fbaea087"},"schema_version":"1.0","source":{"id":"1303.2618","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.2618","created_at":"2026-05-18T01:51:08Z"},{"alias_kind":"arxiv_version","alias_value":"1303.2618v2","created_at":"2026-05-18T01:51:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.2618","created_at":"2026-05-18T01:51:08Z"},{"alias_kind":"pith_short_12","alias_value":"GM7VTO35SSSU","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"GM7VTO35SSSUMFIC","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"GM7VTO35","created_at":"2026-05-18T12:27:45Z"}],"graph_snapshots":[{"event_id":"sha256:6a55dfe4b57ec9525b97a307848d044757380dedc9f157e4a51a9e7616062eee","target":"graph","created_at":"2026-05-18T01:51:08Z","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":"Very few explicit inflationary scenarios are known to generate a large bispectrum of orthogonal shape. Dirac-Born-Infeld Galileon inflation, in which an induced gravity term is added to the DBI action, is one such model. We formulate it in the language of the effective field theory of inflation by identifying the unitary gauge operators that govern the behavior of its cosmological fluctuations. We show how to recover rather easily from this its power spectrum and bispectrum, which we calculated previously using standard cosmological perturbation theory. We push our calculations up to the deter","authors_text":"Sebastien Renaux-Petel","cross_cats":["gr-qc","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2013-03-11T19:01:24Z","title":"DBI Galileon in the Effective Field Theory of Inflation: Orthogonal non-Gaussianities and constraints from the Trispectrum"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.2618","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":"sha256:1c3f6547ece4020bafb77ba9cbb261721067339ea678feae0caf2897009288d4","target":"record","created_at":"2026-05-18T01:51:08Z","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":"636b85535646785efeb174e281b0a77581f62fe20f8547ece701048e489fc5b6","cross_cats_sorted":["gr-qc","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2013-03-11T19:01:24Z","title_canon_sha256":"8bb0e501eba9e6bd76c080b7386c1ba4074063ad574daf9e2b765c02fbaea087"},"schema_version":"1.0","source":{"id":"1303.2618","kind":"arxiv","version":2}},"canonical_sha256":"333f59bb7d94a5461502f40a14d54940d5a26fb36c9de282658cf44be40acdc5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"333f59bb7d94a5461502f40a14d54940d5a26fb36c9de282658cf44be40acdc5","first_computed_at":"2026-05-18T01:51:08.736261Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:51:08.736261Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nhi6fBgBLXhFl7heQ/pstWiatQeUdeEWTFTt0nfniu2uOZS2Bon5mRUfEvhOGKtrBuPPkEufIfJZ6AsLFBCbAw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:51:08.736969Z","signed_message":"canonical_sha256_bytes"},"source_id":"1303.2618","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1c3f6547ece4020bafb77ba9cbb261721067339ea678feae0caf2897009288d4","sha256:6a55dfe4b57ec9525b97a307848d044757380dedc9f157e4a51a9e7616062eee"],"state_sha256":"1417a9de81acdeee6bf6fc372fe26c9804f79b2ccd20ad8f9db59975704c2373"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aYrooDGkOtY36fJA+ZiQ1Y43unVATiAzDKiLYRjKDuDhAcyPvY9ygNhiSeUZtYScZy6+pgCtun7jVDNp7Pl0DQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T21:10:43.759786Z","bundle_sha256":"13cddec95ff1d64fd19a7f4d966a5f293a92eac5ce5dd85c4d2fcc7a967376be"}}