{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:O5CKAAXIX4VIZGRQ5SVA6IBPX2","short_pith_number":"pith:O5CKAAXI","canonical_record":{"source":{"id":"1107.2710","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-07-14T02:04:29Z","cross_cats_sorted":[],"title_canon_sha256":"e0d2b7aaef7397f5cf314851c805c815e120d8643617836aa19284628d54a52f","abstract_canon_sha256":"ccd5f1d97e997f8ac33d412a33342c5912791a112ad0921783fc766d4004a9e2"},"schema_version":"1.0"},"canonical_sha256":"7744a002e8bf2a8c9a30ecaa0f202fbe91aceb198ae55bc19cee73c73677e52e","source":{"kind":"arxiv","id":"1107.2710","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1107.2710","created_at":"2026-05-18T02:01:18Z"},{"alias_kind":"arxiv_version","alias_value":"1107.2710v3","created_at":"2026-05-18T02:01:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.2710","created_at":"2026-05-18T02:01:18Z"},{"alias_kind":"pith_short_12","alias_value":"O5CKAAXIX4VI","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_16","alias_value":"O5CKAAXIX4VIZGRQ","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_8","alias_value":"O5CKAAXI","created_at":"2026-05-18T12:26:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:O5CKAAXIX4VIZGRQ5SVA6IBPX2","target":"record","payload":{"canonical_record":{"source":{"id":"1107.2710","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-07-14T02:04:29Z","cross_cats_sorted":[],"title_canon_sha256":"e0d2b7aaef7397f5cf314851c805c815e120d8643617836aa19284628d54a52f","abstract_canon_sha256":"ccd5f1d97e997f8ac33d412a33342c5912791a112ad0921783fc766d4004a9e2"},"schema_version":"1.0"},"canonical_sha256":"7744a002e8bf2a8c9a30ecaa0f202fbe91aceb198ae55bc19cee73c73677e52e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:18.779648Z","signature_b64":"HV6nTfEcA+GjdUfbeJt7bL1eWA9u2gzJdeeLc8+Y+S39IhNfLhDvBkcBPGHQWJcntZGt5TsdFxj7/3GGJvgyDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7744a002e8bf2a8c9a30ecaa0f202fbe91aceb198ae55bc19cee73c73677e52e","last_reissued_at":"2026-05-18T02:01:18.779102Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:18.779102Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1107.2710","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:01:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5iRvDe053WGzdQ6zdXrbVB5zqEeJHr7NZkXHdK1+HClwBsarUh12GaUpq/laGvdp3YuYRBNzPtvRFW/8tmFyDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T15:43:28.920159Z"},"content_sha256":"8bba90fc82143e4060bceaebbf2aa3be7be5370849b2febf08641679141ec42b","schema_version":"1.0","event_id":"sha256:8bba90fc82143e4060bceaebbf2aa3be7be5370849b2febf08641679141ec42b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:O5CKAAXIX4VIZGRQ5SVA6IBPX2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dualities for Loop Amplitudes of N=6 Chern-Simons Matter Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Wei-Ming Chen, Yu-tin Huang","submitted_at":"2011-07-14T02:04:29Z","abstract_excerpt":"In this paper we study the one- and two-loop corrections to the four-point amplitude of N=6 Chern-Simons matter theory. Using generalized unitarity methods we express the one- and two-loop amplitudes in terms of dual-conformal integrals. Explicit integration by using dimensional reduction gives vanishing one-loop result as expected, while the two-loop result is non-vanishing and matches with the Wilson loop computation. Furthermore, the two-loop correction takes the same form as the one-loop correction to the four-point amplitude of N=4 super Yang-Mills. We discuss possible higher loop extensi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.2710","kind":"arxiv","version":3},"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":"2026-05-18T02:01:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+PnSfYqlD7GPGhONppsXJ+Mgb2bm/50CpbGZ6VO23Zo2/6x/3A9JTdVv5tnD1p0MEUEp23TvWWxDRlOoh6/GAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T15:43:28.920807Z"},"content_sha256":"2d46e83c92776db36106d123f231e7b03634e0b99d9a3fa4488b1a78594c8a55","schema_version":"1.0","event_id":"sha256:2d46e83c92776db36106d123f231e7b03634e0b99d9a3fa4488b1a78594c8a55"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/O5CKAAXIX4VIZGRQ5SVA6IBPX2/bundle.json","state_url":"https://pith.science/pith/O5CKAAXIX4VIZGRQ5SVA6IBPX2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/O5CKAAXIX4VIZGRQ5SVA6IBPX2/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":"2026-06-02T15:43:28Z","links":{"resolver":"https://pith.science/pith/O5CKAAXIX4VIZGRQ5SVA6IBPX2","bundle":"https://pith.science/pith/O5CKAAXIX4VIZGRQ5SVA6IBPX2/bundle.json","state":"https://pith.science/pith/O5CKAAXIX4VIZGRQ5SVA6IBPX2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/O5CKAAXIX4VIZGRQ5SVA6IBPX2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:O5CKAAXIX4VIZGRQ5SVA6IBPX2","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":"ccd5f1d97e997f8ac33d412a33342c5912791a112ad0921783fc766d4004a9e2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-07-14T02:04:29Z","title_canon_sha256":"e0d2b7aaef7397f5cf314851c805c815e120d8643617836aa19284628d54a52f"},"schema_version":"1.0","source":{"id":"1107.2710","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1107.2710","created_at":"2026-05-18T02:01:18Z"},{"alias_kind":"arxiv_version","alias_value":"1107.2710v3","created_at":"2026-05-18T02:01:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.2710","created_at":"2026-05-18T02:01:18Z"},{"alias_kind":"pith_short_12","alias_value":"O5CKAAXIX4VI","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_16","alias_value":"O5CKAAXIX4VIZGRQ","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_8","alias_value":"O5CKAAXI","created_at":"2026-05-18T12:26:37Z"}],"graph_snapshots":[{"event_id":"sha256:2d46e83c92776db36106d123f231e7b03634e0b99d9a3fa4488b1a78594c8a55","target":"graph","created_at":"2026-05-18T02:01:18Z","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":"In this paper we study the one- and two-loop corrections to the four-point amplitude of N=6 Chern-Simons matter theory. Using generalized unitarity methods we express the one- and two-loop amplitudes in terms of dual-conformal integrals. Explicit integration by using dimensional reduction gives vanishing one-loop result as expected, while the two-loop result is non-vanishing and matches with the Wilson loop computation. Furthermore, the two-loop correction takes the same form as the one-loop correction to the four-point amplitude of N=4 super Yang-Mills. We discuss possible higher loop extensi","authors_text":"Wei-Ming Chen, Yu-tin Huang","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-07-14T02:04:29Z","title":"Dualities for Loop Amplitudes of N=6 Chern-Simons Matter Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.2710","kind":"arxiv","version":3},"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":"sha256:8bba90fc82143e4060bceaebbf2aa3be7be5370849b2febf08641679141ec42b","target":"record","created_at":"2026-05-18T02:01:18Z","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":"ccd5f1d97e997f8ac33d412a33342c5912791a112ad0921783fc766d4004a9e2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-07-14T02:04:29Z","title_canon_sha256":"e0d2b7aaef7397f5cf314851c805c815e120d8643617836aa19284628d54a52f"},"schema_version":"1.0","source":{"id":"1107.2710","kind":"arxiv","version":3}},"canonical_sha256":"7744a002e8bf2a8c9a30ecaa0f202fbe91aceb198ae55bc19cee73c73677e52e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7744a002e8bf2a8c9a30ecaa0f202fbe91aceb198ae55bc19cee73c73677e52e","first_computed_at":"2026-05-18T02:01:18.779102Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:01:18.779102Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HV6nTfEcA+GjdUfbeJt7bL1eWA9u2gzJdeeLc8+Y+S39IhNfLhDvBkcBPGHQWJcntZGt5TsdFxj7/3GGJvgyDA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:01:18.779648Z","signed_message":"canonical_sha256_bytes"},"source_id":"1107.2710","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8bba90fc82143e4060bceaebbf2aa3be7be5370849b2febf08641679141ec42b","sha256:2d46e83c92776db36106d123f231e7b03634e0b99d9a3fa4488b1a78594c8a55"],"state_sha256":"a7787a7cf114469dfae3470d6e87c9885364f21e2583c7b2a774930ce28f5f20"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0r2ZtPBjYAncxqlKTJ/AGMPFXGsF/A94BuC8D+rEQ++bYsVVYp6SMrBHrVbTiVtHO9BzYAwLr12L4YUSUhyxAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T15:43:28.924428Z","bundle_sha256":"5182165af22d2544cdfbb1880882ef95bcc7563aa17e9f96fcb272d3cf4b81f0"}}