{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:DSNO4C2PH5WP24LSGRIGZRFEHI","short_pith_number":"pith:DSNO4C2P","canonical_record":{"source":{"id":"2607.24914","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2026-07-27T18:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"a4f853315581918f2b88a4d5a2a7651a1fb224c7559636ca82626ef76d1038fd","abstract_canon_sha256":"b261c8fd789d3e42ac70f0ce9c892c366dc20a0efc1dc7a28854fd9355c7c56f"},"schema_version":"1.0"},"canonical_sha256":"1c9aee0b4f3f6cfd717234506cc4a43a10d5b4324f2d9936cb0c3406015fc466","source":{"kind":"arxiv","id":"2607.24914","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.24914","created_at":"2026-07-29T00:24:51Z"},{"alias_kind":"arxiv_version","alias_value":"2607.24914v1","created_at":"2026-07-29T00:24:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.24914","created_at":"2026-07-29T00:24:51Z"},{"alias_kind":"pith_short_12","alias_value":"DSNO4C2PH5WP","created_at":"2026-07-29T00:24:51Z"},{"alias_kind":"pith_short_16","alias_value":"DSNO4C2PH5WP24LS","created_at":"2026-07-29T00:24:51Z"},{"alias_kind":"pith_short_8","alias_value":"DSNO4C2P","created_at":"2026-07-29T00:24:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:DSNO4C2PH5WP24LSGRIGZRFEHI","target":"record","payload":{"canonical_record":{"source":{"id":"2607.24914","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2026-07-27T18:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"a4f853315581918f2b88a4d5a2a7651a1fb224c7559636ca82626ef76d1038fd","abstract_canon_sha256":"b261c8fd789d3e42ac70f0ce9c892c366dc20a0efc1dc7a28854fd9355c7c56f"},"schema_version":"1.0"},"canonical_sha256":"1c9aee0b4f3f6cfd717234506cc4a43a10d5b4324f2d9936cb0c3406015fc466","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-29T00:24:51.571583Z","signature_b64":"EaRWKqv9CkL1bmofpiwA2Et89rm77fYYMELA8zvt2gmJv9Io3ySVx1PN/msqA6vOKTcJ9UVrckV3zAPnBGsKDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1c9aee0b4f3f6cfd717234506cc4a43a10d5b4324f2d9936cb0c3406015fc466","last_reissued_at":"2026-07-29T00:24:51.570683Z","signature_status":"signed_v1","first_computed_at":"2026-07-29T00:24:51.570683Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2607.24914","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":"2026-07-29T00:24:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vP/bZJdVQCYt3g2eS0GAtJXrLY28VZsv4qWnzJOcDK09ePCTz1qn6wYi1CM18VtcC8H9+bvbbUjIXqyTfPTqAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-31T16:40:18.463107Z"},"content_sha256":"4f7f45df6bde2b1af213e2f774bb8a0cd857789b34657adcf7212eae03897f5e","schema_version":"1.0","event_id":"sha256:4f7f45df6bde2b1af213e2f774bb8a0cd857789b34657adcf7212eae03897f5e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:DSNO4C2PH5WP24LSGRIGZRFEHI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Kaluza-Klein Perturbation Theory from Exceptional Field Theory","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Camilla Lavino, Camille Eloy, Henning Samtleben, Olaf Hohm, Yehudi Simon","submitted_at":"2026-07-27T18:00:01Z","abstract_excerpt":"We develop the perturbation theory of ten and eleven-dimensional supergravities on a large class of Kaluza-Klein backgrounds including familiar AdS examples such as AdS$_5\\times S^5$, but also more general manifolds such as black hole geometries. Employing ${\\rm E}_{6(6)}$ exceptional field theory with the backgrounds characterized by a generalized Scherk-Schwarz ansatz, we determine the first order field equations for the fluctuations that are gauge invariant under linearized generalized diffeomorphisms. We then present the details of the Higgs mechanism for all fields including spin-2 for th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.24914","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/2607.24914/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":"2026-07-29T00:24:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZR/SiqGCcIOjDY593ynIihLrfiteAMUAfeDeXzgaWkyggZifm+VQ722xS5P2re9eKAkh+44G2aYLhqxghMeKDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-31T16:40:18.464083Z"},"content_sha256":"88bbe3fc8e0c77330d43a5533c48fc46938c618db4715e321877c2cbc32586a7","schema_version":"1.0","event_id":"sha256:88bbe3fc8e0c77330d43a5533c48fc46938c618db4715e321877c2cbc32586a7"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:DSNO4C2PH5WP24LSGRIGZRFEHI","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1103/PhysRevD.32.389 resolves to 'Mass spectrum of chiral ten-dimensional<i>N=2</i>supergravity on<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"'. A reader following the printed text alone cannot reach it.","snippet":"H. J. Kim, L. J. Romans and P. van Nieuwenhuizen,The mass spectrum of chiral ten- dimensionalN= 2supergravity onS 5, Phys. Rev.D32, 389 (1985), doi:10.1103/PhysRevD. 32.389","arxiv_id":"2607.24914","detector":"doi_compliance","evidence":{"ref_index":39,"verdict_class":"incontrovertible","resolved_title":"Mass spectrum of chiral ten-dimensional<i>N=2</i>supergravity on<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mi>S</mml:mi></mml:mrow><mml:mrow><mml:mn>5</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>","printed_excerpt":"10.1103/physrevd","reconstructed_doi":"10.1103/PhysRevD.32.389"},"severity":"advisory","ref_index":39,"audited_at":"2026-07-31T06:11:39.014960Z","event_type":"pith.integrity.v1","detected_doi":"10.1103/PhysRevD.32.389","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"c3dfb800fb79e3a6d86c925725a46495801b77b1c9673a378b2e10ac39c362ae","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"Mass spectrum of chiral ten-dimensional<i>N=2</i>supergravity on<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mi>S</mml:mi></mml:mrow><mml:mrow><mml:mn>5</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":14233,"payload_sha256":"74a155fafa09ee49b0214784104a7538796866ca25ccce1a51116d34438a9e3d","signature_b64":null,"signing_key_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-31T06:16:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TlZma7NcAkHLVZnayquAH+S8eyJylOBmZFnPzLrupOTThX/qA93d52V8nK6VqATqJsiKJpcRCcV4wrGs0YIUCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-31T16:40:18.469001Z"},"content_sha256":"89fc42694e8718a434dbaa8efff1b3628199133235ec20794e2d74e44131602f","schema_version":"1.0","event_id":"sha256:89fc42694e8718a434dbaa8efff1b3628199133235ec20794e2d74e44131602f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DSNO4C2PH5WP24LSGRIGZRFEHI/bundle.json","state_url":"https://pith.science/pith/DSNO4C2PH5WP24LSGRIGZRFEHI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DSNO4C2PH5WP24LSGRIGZRFEHI/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":"2026-07-31T16:40:18Z","links":{"resolver":"https://pith.science/pith/DSNO4C2PH5WP24LSGRIGZRFEHI","bundle":"https://pith.science/pith/DSNO4C2PH5WP24LSGRIGZRFEHI/bundle.json","state":"https://pith.science/pith/DSNO4C2PH5WP24LSGRIGZRFEHI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DSNO4C2PH5WP24LSGRIGZRFEHI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:DSNO4C2PH5WP24LSGRIGZRFEHI","merge_version":"pith-open-graph-merge-v1","event_count":3,"valid_event_count":3,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"b261c8fd789d3e42ac70f0ce9c892c366dc20a0efc1dc7a28854fd9355c7c56f","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2026-07-27T18:00:01Z","title_canon_sha256":"a4f853315581918f2b88a4d5a2a7651a1fb224c7559636ca82626ef76d1038fd"},"schema_version":"1.0","source":{"id":"2607.24914","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.24914","created_at":"2026-07-29T00:24:51Z"},{"alias_kind":"arxiv_version","alias_value":"2607.24914v1","created_at":"2026-07-29T00:24:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.24914","created_at":"2026-07-29T00:24:51Z"},{"alias_kind":"pith_short_12","alias_value":"DSNO4C2PH5WP","created_at":"2026-07-29T00:24:51Z"},{"alias_kind":"pith_short_16","alias_value":"DSNO4C2PH5WP24LS","created_at":"2026-07-29T00:24:51Z"},{"alias_kind":"pith_short_8","alias_value":"DSNO4C2P","created_at":"2026-07-29T00:24:51Z"}],"graph_snapshots":[{"event_id":"sha256:88bbe3fc8e0c77330d43a5533c48fc46938c618db4715e321877c2cbc32586a7","target":"graph","created_at":"2026-07-29T00:24:51Z","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/2607.24914/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We develop the perturbation theory of ten and eleven-dimensional supergravities on a large class of Kaluza-Klein backgrounds including familiar AdS examples such as AdS$_5\\times S^5$, but also more general manifolds such as black hole geometries. Employing ${\\rm E}_{6(6)}$ exceptional field theory with the backgrounds characterized by a generalized Scherk-Schwarz ansatz, we determine the first order field equations for the fluctuations that are gauge invariant under linearized generalized diffeomorphisms. We then present the details of the Higgs mechanism for all fields including spin-2 for th","authors_text":"Camilla Lavino, Camille Eloy, Henning Samtleben, Olaf Hohm, Yehudi Simon","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2026-07-27T18:00:01Z","title":"Kaluza-Klein Perturbation Theory from Exceptional Field Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.24914","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":"sha256:4f7f45df6bde2b1af213e2f774bb8a0cd857789b34657adcf7212eae03897f5e","target":"record","created_at":"2026-07-29T00:24:51Z","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":"b261c8fd789d3e42ac70f0ce9c892c366dc20a0efc1dc7a28854fd9355c7c56f","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2026-07-27T18:00:01Z","title_canon_sha256":"a4f853315581918f2b88a4d5a2a7651a1fb224c7559636ca82626ef76d1038fd"},"schema_version":"1.0","source":{"id":"2607.24914","kind":"arxiv","version":1}},"canonical_sha256":"1c9aee0b4f3f6cfd717234506cc4a43a10d5b4324f2d9936cb0c3406015fc466","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1c9aee0b4f3f6cfd717234506cc4a43a10d5b4324f2d9936cb0c3406015fc466","first_computed_at":"2026-07-29T00:24:51.570683Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-29T00:24:51.570683Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EaRWKqv9CkL1bmofpiwA2Et89rm77fYYMELA8zvt2gmJv9Io3ySVx1PN/msqA6vOKTcJ9UVrckV3zAPnBGsKDw==","signature_status":"signed_v1","signed_at":"2026-07-29T00:24:51.571583Z","signed_message":"canonical_sha256_bytes"},"source_id":"2607.24914","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4f7f45df6bde2b1af213e2f774bb8a0cd857789b34657adcf7212eae03897f5e","sha256:88bbe3fc8e0c77330d43a5533c48fc46938c618db4715e321877c2cbc32586a7","sha256:89fc42694e8718a434dbaa8efff1b3628199133235ec20794e2d74e44131602f"],"state_sha256":"58e0369b070a5e5a49d280c7166db35dbeba91e470f9c09157d856dca5e6898b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"V7VXz1R13Kvl+2W9ehPPRSaUn7DdnCF5WX69IoXJTUPY5RipEVcLf2rLYgETl6jjh2JUq/uafZQow1JAcfOxBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-31T16:40:18.471706Z","bundle_sha256":"76f186255b2895abd0814d991ecdc9bd5fc3df80a0ac15da8136ba0a101e88e4"}}