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We study a similarly universal, Lorentz-breaking deformation of two-dimensional CFTs that posess a conserved $U(1)$ current, $J$. The deformation takes the schematic form $J \\bar T$ and is interesting because it preserves an $SL(2,\\mathbb{R}) \\times"},"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":"1710.08415","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-10-23T18:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"6b90e9040438d0dee1bdeb9be40462b8dd48c3e4d88ff09ed92037ae86f55590","abstract_canon_sha256":"703d1534d537bc4df5c9f9939bdc39d14362afa04d63df1e8695e90cadb2e289"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:55:23.174973Z","signature_b64":"kfGQa1gWzZzwYs0b9PlVKVFZFVIodbrWvVn/j5Dl/QvuBa9DDSdWeGz4FpneDntWPQrqQrhl0kLvRXUxNqTBBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3bf04e589e3d35da66d4e347e3beaeb61515f04ee65db55e8b72819c50a99d5e","last_reissued_at":"2026-05-17T23:55:23.174310Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:55:23.174310Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An integrable Lorentz-breaking deformation of two-dimensional CFTs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Monica Guica","submitted_at":"2017-10-23T18:00:00Z","abstract_excerpt":"It has been recently shown that the deformation of an arbitrary two-dimensional conformal field theory by the composite irrelevant operator $T \\bar T$, built from the components of the stress tensor, is solvable; in particular, the finite-size spectrum of the deformed theory can be obtained from that of the original CFT through a universal formula. We study a similarly universal, Lorentz-breaking deformation of two-dimensional CFTs that posess a conserved $U(1)$ current, $J$. 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