{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:YT6IVAFKNUNJYM5LA6EGYQSUR3","short_pith_number":"pith:YT6IVAFK","canonical_record":{"source":{"id":"1205.7038","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-05-31T16:34:11Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"b1e4c21b2acd99789f2b8d13ce211595c0959d237f93d6c9aa0e837f95d1cb5b","abstract_canon_sha256":"c6af00f613b9297ec193edc9393ef04d0669b114e23e9323c3298c6c78bed3fc"},"schema_version":"1.0"},"canonical_sha256":"c4fc8a80aa6d1a9c33ab07886c42548ed950138598bb430dd2a88e31f3efdba2","source":{"kind":"arxiv","id":"1205.7038","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1205.7038","created_at":"2026-05-18T01:57:09Z"},{"alias_kind":"arxiv_version","alias_value":"1205.7038v3","created_at":"2026-05-18T01:57:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.7038","created_at":"2026-05-18T01:57:09Z"},{"alias_kind":"pith_short_12","alias_value":"YT6IVAFKNUNJ","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"YT6IVAFKNUNJYM5L","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"YT6IVAFK","created_at":"2026-05-18T12:27:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:YT6IVAFKNUNJYM5LA6EGYQSUR3","target":"record","payload":{"canonical_record":{"source":{"id":"1205.7038","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-05-31T16:34:11Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"b1e4c21b2acd99789f2b8d13ce211595c0959d237f93d6c9aa0e837f95d1cb5b","abstract_canon_sha256":"c6af00f613b9297ec193edc9393ef04d0669b114e23e9323c3298c6c78bed3fc"},"schema_version":"1.0"},"canonical_sha256":"c4fc8a80aa6d1a9c33ab07886c42548ed950138598bb430dd2a88e31f3efdba2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:57:09.300686Z","signature_b64":"wMSSU501Gvf/zZUkZavSF6jAZP3bnxMhJjRdnibJz/kt+XKE7RTEYcAvggzjvcpkd5IZLZ2RwH9xUAPCLrPHCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c4fc8a80aa6d1a9c33ab07886c42548ed950138598bb430dd2a88e31f3efdba2","last_reissued_at":"2026-05-18T01:57:09.300233Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:57:09.300233Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1205.7038","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":"2026-05-18T01:57:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4hgOKWDQ36uSP7ZOD+Pt5ki51oLQt5LHufU4dDC3m6pt3heSiSAew3h9qwaP5+zC9Csha9rqDhSqHBH2FcIlAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T04:01:39.138983Z"},"content_sha256":"73c96c538ca7dfc36cc02d79ae06a049cdcfeee9c5d872c2525d7cf886e73adc","schema_version":"1.0","event_id":"sha256:73c96c538ca7dfc36cc02d79ae06a049cdcfeee9c5d872c2525d7cf886e73adc"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:YT6IVAFKNUNJYM5LA6EGYQSUR3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"An anisotropic hybrid non-perturbative formulation for 4D N = 2 supersymmetric Yang-Mills theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-lat","authors_text":"Tomohisa Takimi","submitted_at":"2012-05-31T16:34:11Z","abstract_excerpt":"We provide a simple non-perturbative formulation for non-commutative four-dimensional N = 2 supersymmetric Yang-Mills theories. The formulation is constructed by a combination of deconstruction (orbifold projection), momentum cut-off and matrix model techniques. We also propose a moduli fixing term that preserves lattice supersymmetry on the deconstruction formulation. Although the analogous formulation for four-dimensional N = 2 supersymmetric Yang-Mills theories is proposed also in Nucl.Phys.B857(2012), our action is simpler and better suited for computer simulations. Moreover, not only for "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.7038","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":"2026-05-18T01:57:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nnu1eBdYqYL1yM4fgHqVRxi/cn+2gweLO/6by/hC2QL/YFGX6mI0gvoXMOWL6EWbM7Bn869FUqJogllMR8cxCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T04:01:39.139588Z"},"content_sha256":"41fdd708238270275a92a2dc99920dc0c7f91df886156b63b7688415ac77fd03","schema_version":"1.0","event_id":"sha256:41fdd708238270275a92a2dc99920dc0c7f91df886156b63b7688415ac77fd03"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YT6IVAFKNUNJYM5LA6EGYQSUR3/bundle.json","state_url":"https://pith.science/pith/YT6IVAFKNUNJYM5LA6EGYQSUR3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YT6IVAFKNUNJYM5LA6EGYQSUR3/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":"2026-06-01T04:01:39Z","links":{"resolver":"https://pith.science/pith/YT6IVAFKNUNJYM5LA6EGYQSUR3","bundle":"https://pith.science/pith/YT6IVAFKNUNJYM5LA6EGYQSUR3/bundle.json","state":"https://pith.science/pith/YT6IVAFKNUNJYM5LA6EGYQSUR3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YT6IVAFKNUNJYM5LA6EGYQSUR3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:YT6IVAFKNUNJYM5LA6EGYQSUR3","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":"c6af00f613b9297ec193edc9393ef04d0669b114e23e9323c3298c6c78bed3fc","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-05-31T16:34:11Z","title_canon_sha256":"b1e4c21b2acd99789f2b8d13ce211595c0959d237f93d6c9aa0e837f95d1cb5b"},"schema_version":"1.0","source":{"id":"1205.7038","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1205.7038","created_at":"2026-05-18T01:57:09Z"},{"alias_kind":"arxiv_version","alias_value":"1205.7038v3","created_at":"2026-05-18T01:57:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.7038","created_at":"2026-05-18T01:57:09Z"},{"alias_kind":"pith_short_12","alias_value":"YT6IVAFKNUNJ","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"YT6IVAFKNUNJYM5L","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"YT6IVAFK","created_at":"2026-05-18T12:27:30Z"}],"graph_snapshots":[{"event_id":"sha256:41fdd708238270275a92a2dc99920dc0c7f91df886156b63b7688415ac77fd03","target":"graph","created_at":"2026-05-18T01:57:09Z","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 provide a simple non-perturbative formulation for non-commutative four-dimensional N = 2 supersymmetric Yang-Mills theories. The formulation is constructed by a combination of deconstruction (orbifold projection), momentum cut-off and matrix model techniques. We also propose a moduli fixing term that preserves lattice supersymmetry on the deconstruction formulation. Although the analogous formulation for four-dimensional N = 2 supersymmetric Yang-Mills theories is proposed also in Nucl.Phys.B857(2012), our action is simpler and better suited for computer simulations. Moreover, not only for ","authors_text":"Tomohisa Takimi","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-05-31T16:34:11Z","title":"An anisotropic hybrid non-perturbative formulation for 4D N = 2 supersymmetric Yang-Mills theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.7038","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":"sha256:73c96c538ca7dfc36cc02d79ae06a049cdcfeee9c5d872c2525d7cf886e73adc","target":"record","created_at":"2026-05-18T01:57:09Z","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":"c6af00f613b9297ec193edc9393ef04d0669b114e23e9323c3298c6c78bed3fc","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-05-31T16:34:11Z","title_canon_sha256":"b1e4c21b2acd99789f2b8d13ce211595c0959d237f93d6c9aa0e837f95d1cb5b"},"schema_version":"1.0","source":{"id":"1205.7038","kind":"arxiv","version":3}},"canonical_sha256":"c4fc8a80aa6d1a9c33ab07886c42548ed950138598bb430dd2a88e31f3efdba2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c4fc8a80aa6d1a9c33ab07886c42548ed950138598bb430dd2a88e31f3efdba2","first_computed_at":"2026-05-18T01:57:09.300233Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:57:09.300233Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wMSSU501Gvf/zZUkZavSF6jAZP3bnxMhJjRdnibJz/kt+XKE7RTEYcAvggzjvcpkd5IZLZ2RwH9xUAPCLrPHCg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:57:09.300686Z","signed_message":"canonical_sha256_bytes"},"source_id":"1205.7038","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:73c96c538ca7dfc36cc02d79ae06a049cdcfeee9c5d872c2525d7cf886e73adc","sha256:41fdd708238270275a92a2dc99920dc0c7f91df886156b63b7688415ac77fd03"],"state_sha256":"1cd45efac0121553afd5545fe9d6f88a35a65566508d63b6bf204ed7877fc89e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ouZr8Uc6UvcbQyQ1pPdaeGBDQESJEO4OhGjiOGBzke8ve+OtKKxhcnrLW7SdRh76zNDrTtgbGpsheBb+d7PjAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T04:01:39.142490Z","bundle_sha256":"cb0f57b485544bd82c99a59e1dde2b2e1ea918d3b6c0655c15eb7c3680b6bef3"}}