{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:MC6ZFEBGS5DABPCCHAD77R5P2S","short_pith_number":"pith:MC6ZFEBG","schema_version":"1.0","canonical_sha256":"60bd929026974600bc423807ffc7afd4b4b00ef356694cc25ff686bb644f64a0","source":{"kind":"arxiv","id":"2311.10817","version":2},"attestation_state":"computed","paper":{"title":"Small Kinetic Mixing in String Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Arthur Hebecker, Joerg Jaeckel, Ruben Kuespert","submitted_at":"2023-11-17T19:00:02Z","abstract_excerpt":"Kinetic mixing between gauge fields of different $U(1)$ factors is a well-studied phenomenon in 4d EFT. In string compactifications with $U(1)$s from sequestered D-brane sectors, kinetic mixing becomes a key target for the UV prediction of a phenomenologically important EFT operator. Surprisingly, in many cases kinetic mixing is absent due to a non-trivial cancellation. In particular, D3-D3 kinetic mixing in type-IIB vanishes while D3-anti-D3 mixing does not. This follows both from exact CFT calculations on tori as well as from a leading-order 10d supergravity analysis, where the key cancellat"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2311.10817","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-11-17T19:00:02Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"80ca4717a1cac66520a7bf61e939d5eb7b9e4a963f7fd1bf6d262cf82880cf7c","abstract_canon_sha256":"c8f4fe8ecb296960c7e0b53783884c55c6f3b72458f402ce67a915ce38954c75"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:46:26.756965Z","signature_b64":"pAgCc4Na5Nbhdni0gG6ge2XJ+iXB2lm5vAJUqRuPttYR0NFiviBDKD5XWBY3MnICPqxxbs7XlcUdoC+DjPQGDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"60bd929026974600bc423807ffc7afd4b4b00ef356694cc25ff686bb644f64a0","last_reissued_at":"2026-07-05T07:46:26.756330Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:46:26.756330Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Small Kinetic Mixing in String Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Arthur Hebecker, Joerg Jaeckel, Ruben Kuespert","submitted_at":"2023-11-17T19:00:02Z","abstract_excerpt":"Kinetic mixing between gauge fields of different $U(1)$ factors is a well-studied phenomenon in 4d EFT. In string compactifications with $U(1)$s from sequestered D-brane sectors, kinetic mixing becomes a key target for the UV prediction of a phenomenologically important EFT operator. Surprisingly, in many cases kinetic mixing is absent due to a non-trivial cancellation. In particular, D3-D3 kinetic mixing in type-IIB vanishes while D3-anti-D3 mixing does not. This follows both from exact CFT calculations on tori as well as from a leading-order 10d supergravity analysis, where the key cancellat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.10817","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2311.10817/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2311.10817","created_at":"2026-07-05T07:46:26.756415+00:00"},{"alias_kind":"arxiv_version","alias_value":"2311.10817v2","created_at":"2026-07-05T07:46:26.756415+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.10817","created_at":"2026-07-05T07:46:26.756415+00:00"},{"alias_kind":"pith_short_12","alias_value":"MC6ZFEBGS5DA","created_at":"2026-07-05T07:46:26.756415+00:00"},{"alias_kind":"pith_short_16","alias_value":"MC6ZFEBGS5DABPCC","created_at":"2026-07-05T07:46:26.756415+00:00"},{"alias_kind":"pith_short_8","alias_value":"MC6ZFEBG","created_at":"2026-07-05T07:46:26.756415+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2507.13432","citing_title":"INTEGRAL, eROSITA and Voyager Constraints on Light Bosonic Dark Matter: ALPs, Dark Photons, Scalars, $B-L$ and $L_{i}-L_{j}$ Vectors","ref_index":23,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MC6ZFEBGS5DABPCCHAD77R5P2S","json":"https://pith.science/pith/MC6ZFEBGS5DABPCCHAD77R5P2S.json","graph_json":"https://pith.science/api/pith-number/MC6ZFEBGS5DABPCCHAD77R5P2S/graph.json","events_json":"https://pith.science/api/pith-number/MC6ZFEBGS5DABPCCHAD77R5P2S/events.json","paper":"https://pith.science/paper/MC6ZFEBG"},"agent_actions":{"view_html":"https://pith.science/pith/MC6ZFEBGS5DABPCCHAD77R5P2S","download_json":"https://pith.science/pith/MC6ZFEBGS5DABPCCHAD77R5P2S.json","view_paper":"https://pith.science/paper/MC6ZFEBG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2311.10817&json=true","fetch_graph":"https://pith.science/api/pith-number/MC6ZFEBGS5DABPCCHAD77R5P2S/graph.json","fetch_events":"https://pith.science/api/pith-number/MC6ZFEBGS5DABPCCHAD77R5P2S/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MC6ZFEBGS5DABPCCHAD77R5P2S/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MC6ZFEBGS5DABPCCHAD77R5P2S/action/storage_attestation","attest_author":"https://pith.science/pith/MC6ZFEBGS5DABPCCHAD77R5P2S/action/author_attestation","sign_citation":"https://pith.science/pith/MC6ZFEBGS5DABPCCHAD77R5P2S/action/citation_signature","submit_replication":"https://pith.science/pith/MC6ZFEBGS5DABPCCHAD77R5P2S/action/replication_record"}},"created_at":"2026-07-05T07:46:26.756415+00:00","updated_at":"2026-07-05T07:46:26.756415+00:00"}