{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:GUSNSVU5OH64CNAFQGTEO6VOJ4","short_pith_number":"pith:GUSNSVU5","canonical_record":{"source":{"id":"1806.09196","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-06-24T18:50:04Z","cross_cats_sorted":[],"title_canon_sha256":"9d4744a7522f2d07050ee9a3445eefe0f605529f9cb90f8c1509fe5a94caafe1","abstract_canon_sha256":"9341bc678e8fb2bf7208dc03bb6369bf411099155d4562b37a9c1bf163bc1d99"},"schema_version":"1.0"},"canonical_sha256":"3524d9569d71fdc1340581a6477aae4f0b6416f6a5814e7bc133621d61e533eb","source":{"kind":"arxiv","id":"1806.09196","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1806.09196","created_at":"2026-05-18T00:05:30Z"},{"alias_kind":"arxiv_version","alias_value":"1806.09196v1","created_at":"2026-05-18T00:05:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.09196","created_at":"2026-05-18T00:05:30Z"},{"alias_kind":"pith_short_12","alias_value":"GUSNSVU5OH64","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_16","alias_value":"GUSNSVU5OH64CNAF","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_8","alias_value":"GUSNSVU5","created_at":"2026-05-18T12:32:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:GUSNSVU5OH64CNAFQGTEO6VOJ4","target":"record","payload":{"canonical_record":{"source":{"id":"1806.09196","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-06-24T18:50:04Z","cross_cats_sorted":[],"title_canon_sha256":"9d4744a7522f2d07050ee9a3445eefe0f605529f9cb90f8c1509fe5a94caafe1","abstract_canon_sha256":"9341bc678e8fb2bf7208dc03bb6369bf411099155d4562b37a9c1bf163bc1d99"},"schema_version":"1.0"},"canonical_sha256":"3524d9569d71fdc1340581a6477aae4f0b6416f6a5814e7bc133621d61e533eb","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:05:30.670199Z","signature_b64":"U9jeX+o5JXkblA4HoNLPYvf0YdUnsLl87HliWG9jmgOUeKd6dL7AB42So6FLriW5A/bkGNwUcMEcW9rYZDd5Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3524d9569d71fdc1340581a6477aae4f0b6416f6a5814e7bc133621d61e533eb","last_reissued_at":"2026-05-18T00:05:30.669683Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:05:30.669683Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1806.09196","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":"2026-05-18T00:05:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0jQhKbYXwyI19fhR7ktsJuNAlVxG1xsREo4/HVZsK0Oz0CtpNdCGCAJ5ufkcDWYBmdXbg/lZhx60UFuVLS4HBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T17:39:09.624537Z"},"content_sha256":"829dc2e7c082b55de5d3ac08032759ca4d5133e59d7e443a18012b6333bc557c","schema_version":"1.0","event_id":"sha256:829dc2e7c082b55de5d3ac08032759ca4d5133e59d7e443a18012b6333bc557c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:GUSNSVU5OH64CNAFQGTEO6VOJ4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Compactification of 6d minimal SCFTs on Riemann surfaces","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Gabi Zafrir, Shlomo S. Razamat","submitted_at":"2018-06-24T18:50:04Z","abstract_excerpt":"We study compactifications on Riemann surfaces with punctures of N=(1,0) 6d SCFTs with a one dimensional tensor branch and no continuous global symmetries. The effective description of such models on the tensor branch is in terms of pure gauge theories with decoupled tensor. For generic Riemann surfaces, the resulting theories in four dimensions are expected to have N=1 supersymmetry. We compute the anomalies expected from the resulting 4d theories by integrating the anomaly polynomial of the 6d theory on the Riemann surface. For the cases with 6d gauge models with gauge groups SU(3) and SO(8)"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.09196","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":""},"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":"2026-05-18T00:05:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uO3byS85GUi3Wz1dZ0B6Cam2df+N3BObVlb+ihb0cuPVg56SO3iLIlAQOdENgWNzNgsV+em8nUFnB0X/lFNbDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T17:39:09.624871Z"},"content_sha256":"c6e30aefcbf63c40e9d541f271113135ea7f125271abd9abc0e50453fa452bd2","schema_version":"1.0","event_id":"sha256:c6e30aefcbf63c40e9d541f271113135ea7f125271abd9abc0e50453fa452bd2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GUSNSVU5OH64CNAFQGTEO6VOJ4/bundle.json","state_url":"https://pith.science/pith/GUSNSVU5OH64CNAFQGTEO6VOJ4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GUSNSVU5OH64CNAFQGTEO6VOJ4/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":"2026-06-01T17:39:09Z","links":{"resolver":"https://pith.science/pith/GUSNSVU5OH64CNAFQGTEO6VOJ4","bundle":"https://pith.science/pith/GUSNSVU5OH64CNAFQGTEO6VOJ4/bundle.json","state":"https://pith.science/pith/GUSNSVU5OH64CNAFQGTEO6VOJ4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GUSNSVU5OH64CNAFQGTEO6VOJ4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:GUSNSVU5OH64CNAFQGTEO6VOJ4","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":"9341bc678e8fb2bf7208dc03bb6369bf411099155d4562b37a9c1bf163bc1d99","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-06-24T18:50:04Z","title_canon_sha256":"9d4744a7522f2d07050ee9a3445eefe0f605529f9cb90f8c1509fe5a94caafe1"},"schema_version":"1.0","source":{"id":"1806.09196","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1806.09196","created_at":"2026-05-18T00:05:30Z"},{"alias_kind":"arxiv_version","alias_value":"1806.09196v1","created_at":"2026-05-18T00:05:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.09196","created_at":"2026-05-18T00:05:30Z"},{"alias_kind":"pith_short_12","alias_value":"GUSNSVU5OH64","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_16","alias_value":"GUSNSVU5OH64CNAF","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_8","alias_value":"GUSNSVU5","created_at":"2026-05-18T12:32:25Z"}],"graph_snapshots":[{"event_id":"sha256:c6e30aefcbf63c40e9d541f271113135ea7f125271abd9abc0e50453fa452bd2","target":"graph","created_at":"2026-05-18T00:05:30Z","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":"We study compactifications on Riemann surfaces with punctures of N=(1,0) 6d SCFTs with a one dimensional tensor branch and no continuous global symmetries. The effective description of such models on the tensor branch is in terms of pure gauge theories with decoupled tensor. For generic Riemann surfaces, the resulting theories in four dimensions are expected to have N=1 supersymmetry. We compute the anomalies expected from the resulting 4d theories by integrating the anomaly polynomial of the 6d theory on the Riemann surface. For the cases with 6d gauge models with gauge groups SU(3) and SO(8)","authors_text":"Gabi Zafrir, Shlomo S. Razamat","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-06-24T18:50:04Z","title":"Compactification of 6d minimal SCFTs on Riemann surfaces"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.09196","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":"sha256:829dc2e7c082b55de5d3ac08032759ca4d5133e59d7e443a18012b6333bc557c","target":"record","created_at":"2026-05-18T00:05:30Z","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":"9341bc678e8fb2bf7208dc03bb6369bf411099155d4562b37a9c1bf163bc1d99","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-06-24T18:50:04Z","title_canon_sha256":"9d4744a7522f2d07050ee9a3445eefe0f605529f9cb90f8c1509fe5a94caafe1"},"schema_version":"1.0","source":{"id":"1806.09196","kind":"arxiv","version":1}},"canonical_sha256":"3524d9569d71fdc1340581a6477aae4f0b6416f6a5814e7bc133621d61e533eb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3524d9569d71fdc1340581a6477aae4f0b6416f6a5814e7bc133621d61e533eb","first_computed_at":"2026-05-18T00:05:30.669683Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:05:30.669683Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"U9jeX+o5JXkblA4HoNLPYvf0YdUnsLl87HliWG9jmgOUeKd6dL7AB42So6FLriW5A/bkGNwUcMEcW9rYZDd5Cg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:05:30.670199Z","signed_message":"canonical_sha256_bytes"},"source_id":"1806.09196","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:829dc2e7c082b55de5d3ac08032759ca4d5133e59d7e443a18012b6333bc557c","sha256:c6e30aefcbf63c40e9d541f271113135ea7f125271abd9abc0e50453fa452bd2"],"state_sha256":"2af1c8352a95aa41821f397f235fe83a85b0786f7ffbaa707397ddcde347b530"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CZSeyXBvk0/AZfTzOFcajIwpntSjVzuG2sEVI0IIh8+a3vBvYUWmibLlIZR3jbdqHDuhjz2wdfUCMB3pR+euBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T17:39:09.626770Z","bundle_sha256":"99195554e3e95337e31f7a5df714756fa24398619eab34f75e1abc343e072411"}}