{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:G3LLIHMU6MYO4WQY6JXBYIHRNJ","short_pith_number":"pith:G3LLIHMU","canonical_record":{"source":{"id":"1806.02707","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"hep-th","submitted_at":"2018-06-07T14:38:32Z","cross_cats_sorted":[],"title_canon_sha256":"488c03fd3fba61fe84ad4e5198a10b91953ab563efdf164e9d12c2c76377085c","abstract_canon_sha256":"a5229ea22ebddb94f8d796333805d7228657c4f1e5c15b2787f5667fd207f03c"},"schema_version":"1.0"},"canonical_sha256":"36d6b41d94f330ee5a18f26e1c20f16a40429c85ba93d573abf39c4179ebeee0","source":{"kind":"arxiv","id":"1806.02707","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1806.02707","created_at":"2026-05-18T00:06:39Z"},{"alias_kind":"arxiv_version","alias_value":"1806.02707v3","created_at":"2026-05-18T00:06:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.02707","created_at":"2026-05-18T00:06:39Z"},{"alias_kind":"pith_short_12","alias_value":"G3LLIHMU6MYO","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_16","alias_value":"G3LLIHMU6MYO4WQY","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_8","alias_value":"G3LLIHMU","created_at":"2026-05-18T12:32:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:G3LLIHMU6MYO4WQY6JXBYIHRNJ","target":"record","payload":{"canonical_record":{"source":{"id":"1806.02707","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"hep-th","submitted_at":"2018-06-07T14:38:32Z","cross_cats_sorted":[],"title_canon_sha256":"488c03fd3fba61fe84ad4e5198a10b91953ab563efdf164e9d12c2c76377085c","abstract_canon_sha256":"a5229ea22ebddb94f8d796333805d7228657c4f1e5c15b2787f5667fd207f03c"},"schema_version":"1.0"},"canonical_sha256":"36d6b41d94f330ee5a18f26e1c20f16a40429c85ba93d573abf39c4179ebeee0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:06:39.525574Z","signature_b64":"vWZbWOma60kY0zy3SvWho956mgUcwjcEwKQZYt+1UkmTFESvKjcAdQPDu8qeXaDt6CTRy77hf83ogrFUWe8GDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"36d6b41d94f330ee5a18f26e1c20f16a40429c85ba93d573abf39c4179ebeee0","last_reissued_at":"2026-05-18T00:06:39.525134Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:06:39.525134Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1806.02707","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":"2026-05-18T00:06:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XxYuI8o6xWBgckp3UlXMQdtrAvAHmUIDPBV6hHmPkVO9GXX6px4fD3OYCNjxRk4m16x7dnOtgoWQYprwVVBKDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T10:45:28.034494Z"},"content_sha256":"cb05e33af911d238dfd0309c7c7cf17471c0dd380acee498811541ed5640065a","schema_version":"1.0","event_id":"sha256:cb05e33af911d238dfd0309c7c7cf17471c0dd380acee498811541ed5640065a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:G3LLIHMU6MYO4WQY6JXBYIHRNJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"T-duality to Scattering Amplitude and Wilson Loop in Non-commutative Super Yang-Mills Theory","license":"http://creativecommons.org/licenses/by-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Hongfei Shu, Song He","submitted_at":"2018-06-07T14:38:32Z","abstract_excerpt":"We first perform bosonic T-duality transformation on one of the marginal TsT (T-duality, shift, T-duality)-deformed $AdS_5\\times S_5$ spacetime, which corresponds to 4D $\\mathcal{N}=4$ non-commutative super Yang-Mills theory (NCSYM). We then construct the solution to killing spinor equations of the resulting background, and perform the fermionic T-duality transformation. The final dual geometry becomes the usual $AdS_5\\times S_5$ but with the constant NS-NS B-field depending on the non-commutative parameter. As applications, we study the gluon scattering amplitude and open string (Wilson loop)"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.02707","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":"2026-05-18T00:06:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BQHK7wSL7jev1l0pBIftVXSosaSGzX6kzLa+oHkyPy4AIIKtGBpz49HsBvnhBV72/83T2kZT1vgdG7QfQW1KCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T10:45:28.035256Z"},"content_sha256":"e418e5422252645e15e71859261012c6a097a6fb6d3c1435b3ce36248ec0c805","schema_version":"1.0","event_id":"sha256:e418e5422252645e15e71859261012c6a097a6fb6d3c1435b3ce36248ec0c805"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/G3LLIHMU6MYO4WQY6JXBYIHRNJ/bundle.json","state_url":"https://pith.science/pith/G3LLIHMU6MYO4WQY6JXBYIHRNJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/G3LLIHMU6MYO4WQY6JXBYIHRNJ/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":"2026-05-30T10:45:28Z","links":{"resolver":"https://pith.science/pith/G3LLIHMU6MYO4WQY6JXBYIHRNJ","bundle":"https://pith.science/pith/G3LLIHMU6MYO4WQY6JXBYIHRNJ/bundle.json","state":"https://pith.science/pith/G3LLIHMU6MYO4WQY6JXBYIHRNJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/G3LLIHMU6MYO4WQY6JXBYIHRNJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:G3LLIHMU6MYO4WQY6JXBYIHRNJ","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":"a5229ea22ebddb94f8d796333805d7228657c4f1e5c15b2787f5667fd207f03c","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"hep-th","submitted_at":"2018-06-07T14:38:32Z","title_canon_sha256":"488c03fd3fba61fe84ad4e5198a10b91953ab563efdf164e9d12c2c76377085c"},"schema_version":"1.0","source":{"id":"1806.02707","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1806.02707","created_at":"2026-05-18T00:06:39Z"},{"alias_kind":"arxiv_version","alias_value":"1806.02707v3","created_at":"2026-05-18T00:06:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.02707","created_at":"2026-05-18T00:06:39Z"},{"alias_kind":"pith_short_12","alias_value":"G3LLIHMU6MYO","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_16","alias_value":"G3LLIHMU6MYO4WQY","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_8","alias_value":"G3LLIHMU","created_at":"2026-05-18T12:32:25Z"}],"graph_snapshots":[{"event_id":"sha256:e418e5422252645e15e71859261012c6a097a6fb6d3c1435b3ce36248ec0c805","target":"graph","created_at":"2026-05-18T00:06:39Z","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 first perform bosonic T-duality transformation on one of the marginal TsT (T-duality, shift, T-duality)-deformed $AdS_5\\times S_5$ spacetime, which corresponds to 4D $\\mathcal{N}=4$ non-commutative super Yang-Mills theory (NCSYM). We then construct the solution to killing spinor equations of the resulting background, and perform the fermionic T-duality transformation. The final dual geometry becomes the usual $AdS_5\\times S_5$ but with the constant NS-NS B-field depending on the non-commutative parameter. As applications, we study the gluon scattering amplitude and open string (Wilson loop)","authors_text":"Hongfei Shu, Song He","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"hep-th","submitted_at":"2018-06-07T14:38:32Z","title":"T-duality to Scattering Amplitude and Wilson Loop in Non-commutative Super Yang-Mills Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.02707","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:cb05e33af911d238dfd0309c7c7cf17471c0dd380acee498811541ed5640065a","target":"record","created_at":"2026-05-18T00:06:39Z","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":"a5229ea22ebddb94f8d796333805d7228657c4f1e5c15b2787f5667fd207f03c","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"hep-th","submitted_at":"2018-06-07T14:38:32Z","title_canon_sha256":"488c03fd3fba61fe84ad4e5198a10b91953ab563efdf164e9d12c2c76377085c"},"schema_version":"1.0","source":{"id":"1806.02707","kind":"arxiv","version":3}},"canonical_sha256":"36d6b41d94f330ee5a18f26e1c20f16a40429c85ba93d573abf39c4179ebeee0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"36d6b41d94f330ee5a18f26e1c20f16a40429c85ba93d573abf39c4179ebeee0","first_computed_at":"2026-05-18T00:06:39.525134Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:06:39.525134Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vWZbWOma60kY0zy3SvWho956mgUcwjcEwKQZYt+1UkmTFESvKjcAdQPDu8qeXaDt6CTRy77hf83ogrFUWe8GDg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:06:39.525574Z","signed_message":"canonical_sha256_bytes"},"source_id":"1806.02707","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cb05e33af911d238dfd0309c7c7cf17471c0dd380acee498811541ed5640065a","sha256:e418e5422252645e15e71859261012c6a097a6fb6d3c1435b3ce36248ec0c805"],"state_sha256":"ef67dbd411fb830109c5e7d62bd6240df0281d8de59832c30a03aa766202f9ef"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qlumw3AYRcdQSKB1dH3vk2GNAjA2TMLOCy39G+Tb8nanJ0K1LQ1cdG+2fVaEFkWa8PDV0zH2U+XlEeh6XnwVCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T10:45:28.038681Z","bundle_sha256":"4113f9232519ba01a1152829bd7c69868d39414fd1fac888d5f562dd533bca05"}}