{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:TUQWIP5RAYIKCVYKS4BAKRBKZA","short_pith_number":"pith:TUQWIP5R","canonical_record":{"source":{"id":"1706.05222","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-06-16T11:40:05Z","cross_cats_sorted":[],"title_canon_sha256":"937e8d5521d256eb50751967b5aabcda73121487fd8a7f3e16df111fd1c2a811","abstract_canon_sha256":"d25684f92aa4c358ee099fe49f1928aa155186bc9d60effdb3c0d8454909fa48"},"schema_version":"1.0"},"canonical_sha256":"9d21643fb10610a1570a970205442ac80233d905d6b80e315e9850ced8183532","source":{"kind":"arxiv","id":"1706.05222","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.05222","created_at":"2026-05-18T00:38:02Z"},{"alias_kind":"arxiv_version","alias_value":"1706.05222v1","created_at":"2026-05-18T00:38:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.05222","created_at":"2026-05-18T00:38:02Z"},{"alias_kind":"pith_short_12","alias_value":"TUQWIP5RAYIK","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_16","alias_value":"TUQWIP5RAYIKCVYK","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_8","alias_value":"TUQWIP5R","created_at":"2026-05-18T12:31:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:TUQWIP5RAYIKCVYKS4BAKRBKZA","target":"record","payload":{"canonical_record":{"source":{"id":"1706.05222","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-06-16T11:40:05Z","cross_cats_sorted":[],"title_canon_sha256":"937e8d5521d256eb50751967b5aabcda73121487fd8a7f3e16df111fd1c2a811","abstract_canon_sha256":"d25684f92aa4c358ee099fe49f1928aa155186bc9d60effdb3c0d8454909fa48"},"schema_version":"1.0"},"canonical_sha256":"9d21643fb10610a1570a970205442ac80233d905d6b80e315e9850ced8183532","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:02.188302Z","signature_b64":"r2KIuU9/XasT6d9u3IgkR1oAfUAWylSBolKVrNA5LpcpqLS2Akq3nk1m73GfGootkARlQcn3WCQ32DDA2HWsCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9d21643fb10610a1570a970205442ac80233d905d6b80e315e9850ced8183532","last_reissued_at":"2026-05-18T00:38:02.187805Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:02.187805Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1706.05222","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":"2026-05-18T00:38:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+y3miPKJmQoCqyGmtQ06per0q7fAQoEkytLb5+UKFtU5QE1jhAca56cpfk+5K2LWCEXaHY5miSLL0CjONf9qAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T21:52:33.557129Z"},"content_sha256":"e2c01228dda1e84fe74fbe281916d3900e0e5163f44ce2658b8f271c2b88b28b","schema_version":"1.0","event_id":"sha256:e2c01228dda1e84fe74fbe281916d3900e0e5163f44ce2658b8f271c2b88b28b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:TUQWIP5RAYIKCVYKS4BAKRBKZA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Supersymmetric QCD on the Lattice: An Exploratory Study","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"H. Panagopoulos, M. Costa","submitted_at":"2017-06-16T11:40:05Z","abstract_excerpt":"We perform a pilot study of the perturbative renormalization of a Supersymmetric gauge theory with matter fields on the lattice. As a specific example, we consider Supersymmetric ${\\cal N}{=}1$ QCD (SQCD). We study the self-energies of all particles which appear in this theory, as well as the renormalization of the coupling constant. To this end we compute, perturbatively to one-loop, the relevant two-point and three-point Green's functions using both dimensional and lattice regularizations. Our lattice formulation involves the Wilson discretization for the gluino and quark fields; for gluons "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.05222","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":"2026-05-18T00:38:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GQ1JUJXXrJl2BmkLS0MNVnDlffSQXGPxqCyiTJeaXZkw4T265zYaBaApZljlmelKVES59dWKx/yHYRGKuag4Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T21:52:33.557742Z"},"content_sha256":"4fc07d2179b404ec66ca6116d027439c7e5c43cf1b101b9f2cc73f381d011707","schema_version":"1.0","event_id":"sha256:4fc07d2179b404ec66ca6116d027439c7e5c43cf1b101b9f2cc73f381d011707"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TUQWIP5RAYIKCVYKS4BAKRBKZA/bundle.json","state_url":"https://pith.science/pith/TUQWIP5RAYIKCVYKS4BAKRBKZA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TUQWIP5RAYIKCVYKS4BAKRBKZA/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":"2026-08-09T21:52:33Z","links":{"resolver":"https://pith.science/pith/TUQWIP5RAYIKCVYKS4BAKRBKZA","bundle":"https://pith.science/pith/TUQWIP5RAYIKCVYKS4BAKRBKZA/bundle.json","state":"https://pith.science/pith/TUQWIP5RAYIKCVYKS4BAKRBKZA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TUQWIP5RAYIKCVYKS4BAKRBKZA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:TUQWIP5RAYIKCVYKS4BAKRBKZA","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":"d25684f92aa4c358ee099fe49f1928aa155186bc9d60effdb3c0d8454909fa48","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-06-16T11:40:05Z","title_canon_sha256":"937e8d5521d256eb50751967b5aabcda73121487fd8a7f3e16df111fd1c2a811"},"schema_version":"1.0","source":{"id":"1706.05222","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.05222","created_at":"2026-05-18T00:38:02Z"},{"alias_kind":"arxiv_version","alias_value":"1706.05222v1","created_at":"2026-05-18T00:38:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.05222","created_at":"2026-05-18T00:38:02Z"},{"alias_kind":"pith_short_12","alias_value":"TUQWIP5RAYIK","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_16","alias_value":"TUQWIP5RAYIKCVYK","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_8","alias_value":"TUQWIP5R","created_at":"2026-05-18T12:31:46Z"}],"graph_snapshots":[{"event_id":"sha256:4fc07d2179b404ec66ca6116d027439c7e5c43cf1b101b9f2cc73f381d011707","target":"graph","created_at":"2026-05-18T00:38:02Z","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 perform a pilot study of the perturbative renormalization of a Supersymmetric gauge theory with matter fields on the lattice. As a specific example, we consider Supersymmetric ${\\cal N}{=}1$ QCD (SQCD). We study the self-energies of all particles which appear in this theory, as well as the renormalization of the coupling constant. To this end we compute, perturbatively to one-loop, the relevant two-point and three-point Green's functions using both dimensional and lattice regularizations. Our lattice formulation involves the Wilson discretization for the gluino and quark fields; for gluons ","authors_text":"H. Panagopoulos, M. Costa","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-06-16T11:40:05Z","title":"Supersymmetric QCD on the Lattice: An Exploratory Study"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.05222","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:e2c01228dda1e84fe74fbe281916d3900e0e5163f44ce2658b8f271c2b88b28b","target":"record","created_at":"2026-05-18T00:38:02Z","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":"d25684f92aa4c358ee099fe49f1928aa155186bc9d60effdb3c0d8454909fa48","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-06-16T11:40:05Z","title_canon_sha256":"937e8d5521d256eb50751967b5aabcda73121487fd8a7f3e16df111fd1c2a811"},"schema_version":"1.0","source":{"id":"1706.05222","kind":"arxiv","version":1}},"canonical_sha256":"9d21643fb10610a1570a970205442ac80233d905d6b80e315e9850ced8183532","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9d21643fb10610a1570a970205442ac80233d905d6b80e315e9850ced8183532","first_computed_at":"2026-05-18T00:38:02.187805Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:38:02.187805Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"r2KIuU9/XasT6d9u3IgkR1oAfUAWylSBolKVrNA5LpcpqLS2Akq3nk1m73GfGootkARlQcn3WCQ32DDA2HWsCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:38:02.188302Z","signed_message":"canonical_sha256_bytes"},"source_id":"1706.05222","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e2c01228dda1e84fe74fbe281916d3900e0e5163f44ce2658b8f271c2b88b28b","sha256:4fc07d2179b404ec66ca6116d027439c7e5c43cf1b101b9f2cc73f381d011707"],"state_sha256":"326f6ebcadb04f33adf049b4dcf1a0d38f54fcb9827a55024625a096c1bb8431"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RadTFGQd3m5T2RbcZfYsMND1wM0WsShuVO8ONm0hv26TQmKwTuv+qxSytvrUbjPuAlV8WBOxvpqMfoEDeyblAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-09T21:52:33.563367Z","bundle_sha256":"4c56cd7c724e847a0a34eab2c861ce23659b95b1b3228066a3f52e2d6f13984e"}}