{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:WMXHSRJLWIWOOGSNWIEDKJWRNF","short_pith_number":"pith:WMXHSRJL","canonical_record":{"source":{"id":"1112.1797","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-08T09:56:39Z","cross_cats_sorted":[],"title_canon_sha256":"a6ffef4efab4f2025164e1fbb22ecfaa10155f422121fabf754f0d56cf445d98","abstract_canon_sha256":"aecc323a01d63ff6fa606e6a2dfce0ce28d2a472cb39382e37a80b1c9b38cdf1"},"schema_version":"1.0"},"canonical_sha256":"b32e79452bb22ce71a4db2083526d1694ae2c1ee4f26ae88966273471b813752","source":{"kind":"arxiv","id":"1112.1797","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.1797","created_at":"2026-05-18T02:23:59Z"},{"alias_kind":"arxiv_version","alias_value":"1112.1797v1","created_at":"2026-05-18T02:23:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.1797","created_at":"2026-05-18T02:23:59Z"},{"alias_kind":"pith_short_12","alias_value":"WMXHSRJLWIWO","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"WMXHSRJLWIWOOGSN","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"WMXHSRJL","created_at":"2026-05-18T12:26:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:WMXHSRJLWIWOOGSNWIEDKJWRNF","target":"record","payload":{"canonical_record":{"source":{"id":"1112.1797","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-08T09:56:39Z","cross_cats_sorted":[],"title_canon_sha256":"a6ffef4efab4f2025164e1fbb22ecfaa10155f422121fabf754f0d56cf445d98","abstract_canon_sha256":"aecc323a01d63ff6fa606e6a2dfce0ce28d2a472cb39382e37a80b1c9b38cdf1"},"schema_version":"1.0"},"canonical_sha256":"b32e79452bb22ce71a4db2083526d1694ae2c1ee4f26ae88966273471b813752","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:23:59.076483Z","signature_b64":"nteIOpNUj+FKa/qp1/u6uqy5EhA9s3xkKmSEfxhSkV8n9n0vo5eyVuPItKcGnTrNysWagQY3CgFk1u3QALkvCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b32e79452bb22ce71a4db2083526d1694ae2c1ee4f26ae88966273471b813752","last_reissued_at":"2026-05-18T02:23:59.075839Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:23:59.075839Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1112.1797","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":"2026-05-18T02:23:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tc8Z88qxln2Kh2tIrksYgt4cLCe6j72yC48ZKRdUYj2zOjK1N9H53jOGKwUsH7Y5FYhgcc96rOK76M92QaWZDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-02T14:10:10.900663Z"},"content_sha256":"299610ac9c95f0c929d122ed37336969df421dc4beb4b5699e9a89f599ffb763","schema_version":"1.0","event_id":"sha256:299610ac9c95f0c929d122ed37336969df421dc4beb4b5699e9a89f599ffb763"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:WMXHSRJLWIWOOGSNWIEDKJWRNF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Gauge theory and SIM(2) superspace","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ji\\v{r}\\'i Voh\\'anka","submitted_at":"2011-12-08T09:56:39Z","abstract_excerpt":"In this paper the SIM(2) superspace formulation of the supersymmetric Yang-Mills gauge theory minimally coupled to chiral superfields is discussed. The super-Poincare invariant supersymmetric Yang-Mills theory is rewritten to SIM(2) superspace formalism and the effects of SIM(2) invariant but Lorentz breaking terms are discussed. Two approaches are investigated. The first is based on the gauge chiral representation of the supersymmetric gauge theory and the second is based on the covariant representation of the supersymmetric gauge theory."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.1797","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":"2026-05-18T02:23:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"T0cdj6nMRVQWmRlAGgCGVInP44bOCiAHP109uDBTQgeKpuaDvGq0PdmpZAHu1tj9LsJDjEJYrlnBR1M2wA0uDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-02T14:10:10.901013Z"},"content_sha256":"7311d7cae3d393ac4370647d7c5a167f2d994159fde9d2b90b7fc91c6cddd371","schema_version":"1.0","event_id":"sha256:7311d7cae3d393ac4370647d7c5a167f2d994159fde9d2b90b7fc91c6cddd371"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WMXHSRJLWIWOOGSNWIEDKJWRNF/bundle.json","state_url":"https://pith.science/pith/WMXHSRJLWIWOOGSNWIEDKJWRNF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WMXHSRJLWIWOOGSNWIEDKJWRNF/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":"2026-07-02T14:10:10Z","links":{"resolver":"https://pith.science/pith/WMXHSRJLWIWOOGSNWIEDKJWRNF","bundle":"https://pith.science/pith/WMXHSRJLWIWOOGSNWIEDKJWRNF/bundle.json","state":"https://pith.science/pith/WMXHSRJLWIWOOGSNWIEDKJWRNF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WMXHSRJLWIWOOGSNWIEDKJWRNF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:WMXHSRJLWIWOOGSNWIEDKJWRNF","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":"aecc323a01d63ff6fa606e6a2dfce0ce28d2a472cb39382e37a80b1c9b38cdf1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-08T09:56:39Z","title_canon_sha256":"a6ffef4efab4f2025164e1fbb22ecfaa10155f422121fabf754f0d56cf445d98"},"schema_version":"1.0","source":{"id":"1112.1797","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.1797","created_at":"2026-05-18T02:23:59Z"},{"alias_kind":"arxiv_version","alias_value":"1112.1797v1","created_at":"2026-05-18T02:23:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.1797","created_at":"2026-05-18T02:23:59Z"},{"alias_kind":"pith_short_12","alias_value":"WMXHSRJLWIWO","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"WMXHSRJLWIWOOGSN","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"WMXHSRJL","created_at":"2026-05-18T12:26:44Z"}],"graph_snapshots":[{"event_id":"sha256:7311d7cae3d393ac4370647d7c5a167f2d994159fde9d2b90b7fc91c6cddd371","target":"graph","created_at":"2026-05-18T02:23:59Z","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 the SIM(2) superspace formulation of the supersymmetric Yang-Mills gauge theory minimally coupled to chiral superfields is discussed. The super-Poincare invariant supersymmetric Yang-Mills theory is rewritten to SIM(2) superspace formalism and the effects of SIM(2) invariant but Lorentz breaking terms are discussed. Two approaches are investigated. The first is based on the gauge chiral representation of the supersymmetric gauge theory and the second is based on the covariant representation of the supersymmetric gauge theory.","authors_text":"Ji\\v{r}\\'i Voh\\'anka","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-08T09:56:39Z","title":"Gauge theory and SIM(2) superspace"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.1797","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":"sha256:299610ac9c95f0c929d122ed37336969df421dc4beb4b5699e9a89f599ffb763","target":"record","created_at":"2026-05-18T02:23:59Z","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":"aecc323a01d63ff6fa606e6a2dfce0ce28d2a472cb39382e37a80b1c9b38cdf1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-08T09:56:39Z","title_canon_sha256":"a6ffef4efab4f2025164e1fbb22ecfaa10155f422121fabf754f0d56cf445d98"},"schema_version":"1.0","source":{"id":"1112.1797","kind":"arxiv","version":1}},"canonical_sha256":"b32e79452bb22ce71a4db2083526d1694ae2c1ee4f26ae88966273471b813752","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b32e79452bb22ce71a4db2083526d1694ae2c1ee4f26ae88966273471b813752","first_computed_at":"2026-05-18T02:23:59.075839Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:23:59.075839Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nteIOpNUj+FKa/qp1/u6uqy5EhA9s3xkKmSEfxhSkV8n9n0vo5eyVuPItKcGnTrNysWagQY3CgFk1u3QALkvCw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:23:59.076483Z","signed_message":"canonical_sha256_bytes"},"source_id":"1112.1797","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:299610ac9c95f0c929d122ed37336969df421dc4beb4b5699e9a89f599ffb763","sha256:7311d7cae3d393ac4370647d7c5a167f2d994159fde9d2b90b7fc91c6cddd371"],"state_sha256":"7bc48db80c0e89bd862798af6d976c0c5f63aba2effa9d75ed92a7e5c6ae4fa6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hP4Kk2fO/awx7/GwKzCG8PpFJ3U81A980Y4ylGRx10VnKeHGmAaczmPov3GaFyzRzYZLuvMM1SrfW4Dh2xd2Dw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-02T14:10:10.902971Z","bundle_sha256":"5a9a6e472b78090f39a03e5818e0a1bcf60288a756524c2d77fde157062e4f5d"}}