{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:QWXSQAUJPJQC3VAIAAGRMOHTQG","short_pith_number":"pith:QWXSQAUJ","canonical_record":{"source":{"id":"1201.5012","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-01-24T15:26:46Z","cross_cats_sorted":[],"title_canon_sha256":"6fc4ce15880d7093b16b5419892012d96a8a93e6396442d4522eb3a9707bcc72","abstract_canon_sha256":"6b613d623807721b92f1d186ed60cb3238e166995aa38fe6cde0b77fc6d78f09"},"schema_version":"1.0"},"canonical_sha256":"85af2802897a602dd408000d1638f3818dc1780736958efe5f0cf5b1de45af14","source":{"kind":"arxiv","id":"1201.5012","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.5012","created_at":"2026-05-18T01:58:42Z"},{"alias_kind":"arxiv_version","alias_value":"1201.5012v1","created_at":"2026-05-18T01:58:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.5012","created_at":"2026-05-18T01:58:42Z"},{"alias_kind":"pith_short_12","alias_value":"QWXSQAUJPJQC","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_16","alias_value":"QWXSQAUJPJQC3VAI","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_8","alias_value":"QWXSQAUJ","created_at":"2026-05-18T12:27:20Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:QWXSQAUJPJQC3VAIAAGRMOHTQG","target":"record","payload":{"canonical_record":{"source":{"id":"1201.5012","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-01-24T15:26:46Z","cross_cats_sorted":[],"title_canon_sha256":"6fc4ce15880d7093b16b5419892012d96a8a93e6396442d4522eb3a9707bcc72","abstract_canon_sha256":"6b613d623807721b92f1d186ed60cb3238e166995aa38fe6cde0b77fc6d78f09"},"schema_version":"1.0"},"canonical_sha256":"85af2802897a602dd408000d1638f3818dc1780736958efe5f0cf5b1de45af14","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:42.759549Z","signature_b64":"Qj+mxRK8kEgCweH3fijMSCKwaBZ0c7yZ/4A6Sn2cVENFJBmUBLBfOapwYr8ZqI+A/ukXoABYkU4tQO3W35NtBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"85af2802897a602dd408000d1638f3818dc1780736958efe5f0cf5b1de45af14","last_reissued_at":"2026-05-18T01:58:42.758769Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:42.758769Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1201.5012","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":"2026-05-18T01:58:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sIsH1VSEiBLmzJrBMtvzUGjMZapfb5MHDby7/Ux7KzJqS2TvG1LC2UG0mrCQR5sim6PW/VS3yoASC+Q7t5dOBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T08:36:54.531344Z"},"content_sha256":"3696832cdbfd6565d8501bf0430affbe85be326a4500d0ac9ce094fdfd804698","schema_version":"1.0","event_id":"sha256:3696832cdbfd6565d8501bf0430affbe85be326a4500d0ac9ce094fdfd804698"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:QWXSQAUJPJQC3VAIAAGRMOHTQG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the non-planar beta-deformed N=4 super-Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Q. Jin, R. Roiban","submitted_at":"2012-01-24T15:26:46Z","abstract_excerpt":"The beta-deformation is one of the two superconformal deformations of the N=4 super-Yang-Mills theory. At the planar level it shares all of its properties except for supersymmetry, which is broken to the minimal amount. The tree-level amplitudes of this theory exhibit new features which depart from the commonly assumed properties of gauge theories with fields in the adjoint representation.\n  We analyze in detail complete one-loop amplitudes and a nonplanar two-loop amplitude of this theory and show that, despite having only N=1 supersymmetry, two-loop amplitudes have a further-improved ultravi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.5012","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":"2026-05-18T01:58:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rgaWhkskoM62fm2qqhoa7Zls1pXe58mDpkSd7wKZ5x2PzWkSNR/+i3MZNmhUVG7dnOOPo//03V84K4G80739Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T08:36:54.532099Z"},"content_sha256":"edc9b575a5482c9532e0c0d86d4a13e703db723bc983ab7246f8632c2440901a","schema_version":"1.0","event_id":"sha256:edc9b575a5482c9532e0c0d86d4a13e703db723bc983ab7246f8632c2440901a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QWXSQAUJPJQC3VAIAAGRMOHTQG/bundle.json","state_url":"https://pith.science/pith/QWXSQAUJPJQC3VAIAAGRMOHTQG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QWXSQAUJPJQC3VAIAAGRMOHTQG/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":"2026-06-11T08:36:54Z","links":{"resolver":"https://pith.science/pith/QWXSQAUJPJQC3VAIAAGRMOHTQG","bundle":"https://pith.science/pith/QWXSQAUJPJQC3VAIAAGRMOHTQG/bundle.json","state":"https://pith.science/pith/QWXSQAUJPJQC3VAIAAGRMOHTQG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QWXSQAUJPJQC3VAIAAGRMOHTQG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:QWXSQAUJPJQC3VAIAAGRMOHTQG","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":"6b613d623807721b92f1d186ed60cb3238e166995aa38fe6cde0b77fc6d78f09","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-01-24T15:26:46Z","title_canon_sha256":"6fc4ce15880d7093b16b5419892012d96a8a93e6396442d4522eb3a9707bcc72"},"schema_version":"1.0","source":{"id":"1201.5012","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.5012","created_at":"2026-05-18T01:58:42Z"},{"alias_kind":"arxiv_version","alias_value":"1201.5012v1","created_at":"2026-05-18T01:58:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.5012","created_at":"2026-05-18T01:58:42Z"},{"alias_kind":"pith_short_12","alias_value":"QWXSQAUJPJQC","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_16","alias_value":"QWXSQAUJPJQC3VAI","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_8","alias_value":"QWXSQAUJ","created_at":"2026-05-18T12:27:20Z"}],"graph_snapshots":[{"event_id":"sha256:edc9b575a5482c9532e0c0d86d4a13e703db723bc983ab7246f8632c2440901a","target":"graph","created_at":"2026-05-18T01:58:42Z","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":"The beta-deformation is one of the two superconformal deformations of the N=4 super-Yang-Mills theory. At the planar level it shares all of its properties except for supersymmetry, which is broken to the minimal amount. The tree-level amplitudes of this theory exhibit new features which depart from the commonly assumed properties of gauge theories with fields in the adjoint representation.\n  We analyze in detail complete one-loop amplitudes and a nonplanar two-loop amplitude of this theory and show that, despite having only N=1 supersymmetry, two-loop amplitudes have a further-improved ultravi","authors_text":"Q. Jin, R. Roiban","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-01-24T15:26:46Z","title":"On the non-planar beta-deformed N=4 super-Yang-Mills theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.5012","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":"sha256:3696832cdbfd6565d8501bf0430affbe85be326a4500d0ac9ce094fdfd804698","target":"record","created_at":"2026-05-18T01:58:42Z","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":"6b613d623807721b92f1d186ed60cb3238e166995aa38fe6cde0b77fc6d78f09","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-01-24T15:26:46Z","title_canon_sha256":"6fc4ce15880d7093b16b5419892012d96a8a93e6396442d4522eb3a9707bcc72"},"schema_version":"1.0","source":{"id":"1201.5012","kind":"arxiv","version":1}},"canonical_sha256":"85af2802897a602dd408000d1638f3818dc1780736958efe5f0cf5b1de45af14","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"85af2802897a602dd408000d1638f3818dc1780736958efe5f0cf5b1de45af14","first_computed_at":"2026-05-18T01:58:42.758769Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:58:42.758769Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Qj+mxRK8kEgCweH3fijMSCKwaBZ0c7yZ/4A6Sn2cVENFJBmUBLBfOapwYr8ZqI+A/ukXoABYkU4tQO3W35NtBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:58:42.759549Z","signed_message":"canonical_sha256_bytes"},"source_id":"1201.5012","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3696832cdbfd6565d8501bf0430affbe85be326a4500d0ac9ce094fdfd804698","sha256:edc9b575a5482c9532e0c0d86d4a13e703db723bc983ab7246f8632c2440901a"],"state_sha256":"d4e9b687c2858b82a3836acf0067920f11d75e21a5960e7304216313b903b817"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"v1TIxkZQOV8KMc3bK8HaAMcZbdOGe86IkwNeA1U0uTQLCxlW/Z7/AdvAsCP+Yj5RILgefiHI7uFwLKqv/T0IDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T08:36:54.536067Z","bundle_sha256":"a2d252a897c5e2484c4c1f47872b748570c8c30130f82cf10ca982826c181aaa"}}