{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:ZHE242L3MESVAVV2CNBQ2L3363","short_pith_number":"pith:ZHE242L3","canonical_record":{"source":{"id":"1801.08062","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-01-24T16:34:00Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"94a2efc7e2fdfef82f244e754c6f7ba9801131e66374f446ab0bb25d5a5646ec","abstract_canon_sha256":"59e3142acd408994f189be96df6aeab19859090c7f5c9c624789b9d9c6895e79"},"schema_version":"1.0"},"canonical_sha256":"c9c9ae697b61255056ba13430d2f7bf6f8b24e244ff64130fcfb9c1309263576","source":{"kind":"arxiv","id":"1801.08062","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.08062","created_at":"2026-05-18T00:18:11Z"},{"alias_kind":"arxiv_version","alias_value":"1801.08062v1","created_at":"2026-05-18T00:18:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.08062","created_at":"2026-05-18T00:18:11Z"},{"alias_kind":"pith_short_12","alias_value":"ZHE242L3MESV","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_16","alias_value":"ZHE242L3MESVAVV2","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_8","alias_value":"ZHE242L3","created_at":"2026-05-18T12:33:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:ZHE242L3MESVAVV2CNBQ2L3363","target":"record","payload":{"canonical_record":{"source":{"id":"1801.08062","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-01-24T16:34:00Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"94a2efc7e2fdfef82f244e754c6f7ba9801131e66374f446ab0bb25d5a5646ec","abstract_canon_sha256":"59e3142acd408994f189be96df6aeab19859090c7f5c9c624789b9d9c6895e79"},"schema_version":"1.0"},"canonical_sha256":"c9c9ae697b61255056ba13430d2f7bf6f8b24e244ff64130fcfb9c1309263576","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:18:11.501523Z","signature_b64":"XGIJlXipsaiEJM+HIXDGHFB4wfLOMdIyEgT6Ggap2FoidI4iOpybDy5unVykkpDcXMvDaua/LFd3YNOyJax1BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c9c9ae697b61255056ba13430d2f7bf6f8b24e244ff64130fcfb9c1309263576","last_reissued_at":"2026-05-18T00:18:11.500903Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:18:11.500903Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1801.08062","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":"2026-05-18T00:18:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fV7G4/sS5FOki9hk7AmjAIS1aywYxohvpKKdkdNAqatxkPVdg/EGXGz8gYvCSL0IDoXEunOpvwGBzo357K9CCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T23:00:35.525908Z"},"content_sha256":"1aa165ff9c02fcc85130445b06bc3de6123216bbe13b791eab9ce69f71aed6a3","schema_version":"1.0","event_id":"sha256:1aa165ff9c02fcc85130445b06bc3de6123216bbe13b791eab9ce69f71aed6a3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:ZHE242L3MESVAVV2CNBQ2L3363","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The light bound states of $\\mathcal{N}=1$ supersymmetric SU(3) Yang-Mills theory on the lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-lat","authors_text":"Georg Bergner, Gernot M\\\"unster, Henning Gerber, Istvan Montvay, Philipp Scior, Pietro Giudice, Sajid Ali, Stefano Piemonte","submitted_at":"2018-01-24T16:34:00Z","abstract_excerpt":"In this article we summarise our results from numerical simulations of $\\mathcal{N}=1$ supersymmetric Yang-Mills theory with gauge group SU(3). We use the formulation of Curci and Veneziano with clover-improved Wilson fermions. The masses of various bound states have been obtained at different values of the gluino mass and gauge coupling. Extrapolations to the limit of vanishing gluino mass indicate that the bound states form mass-degenerate supermultiplets."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.08062","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":"2026-05-18T00:18:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+6wK4imw7Nxf8aqz2qv62NrJS7K2I/s1epiSuWIPsq4RdRBpmcEPpODSdPBk9P4q/VqiK3Lv8FGTAaV6yK/1Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T23:00:35.526578Z"},"content_sha256":"43c2b4deff41acc6a5973c02ff72e2c286ccbc63713c730451b219c5d2617f2a","schema_version":"1.0","event_id":"sha256:43c2b4deff41acc6a5973c02ff72e2c286ccbc63713c730451b219c5d2617f2a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZHE242L3MESVAVV2CNBQ2L3363/bundle.json","state_url":"https://pith.science/pith/ZHE242L3MESVAVV2CNBQ2L3363/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZHE242L3MESVAVV2CNBQ2L3363/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":"2026-05-28T23:00:35Z","links":{"resolver":"https://pith.science/pith/ZHE242L3MESVAVV2CNBQ2L3363","bundle":"https://pith.science/pith/ZHE242L3MESVAVV2CNBQ2L3363/bundle.json","state":"https://pith.science/pith/ZHE242L3MESVAVV2CNBQ2L3363/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZHE242L3MESVAVV2CNBQ2L3363/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:ZHE242L3MESVAVV2CNBQ2L3363","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":"59e3142acd408994f189be96df6aeab19859090c7f5c9c624789b9d9c6895e79","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-01-24T16:34:00Z","title_canon_sha256":"94a2efc7e2fdfef82f244e754c6f7ba9801131e66374f446ab0bb25d5a5646ec"},"schema_version":"1.0","source":{"id":"1801.08062","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.08062","created_at":"2026-05-18T00:18:11Z"},{"alias_kind":"arxiv_version","alias_value":"1801.08062v1","created_at":"2026-05-18T00:18:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.08062","created_at":"2026-05-18T00:18:11Z"},{"alias_kind":"pith_short_12","alias_value":"ZHE242L3MESV","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_16","alias_value":"ZHE242L3MESVAVV2","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_8","alias_value":"ZHE242L3","created_at":"2026-05-18T12:33:07Z"}],"graph_snapshots":[{"event_id":"sha256:43c2b4deff41acc6a5973c02ff72e2c286ccbc63713c730451b219c5d2617f2a","target":"graph","created_at":"2026-05-18T00:18:11Z","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 article we summarise our results from numerical simulations of $\\mathcal{N}=1$ supersymmetric Yang-Mills theory with gauge group SU(3). We use the formulation of Curci and Veneziano with clover-improved Wilson fermions. The masses of various bound states have been obtained at different values of the gluino mass and gauge coupling. Extrapolations to the limit of vanishing gluino mass indicate that the bound states form mass-degenerate supermultiplets.","authors_text":"Georg Bergner, Gernot M\\\"unster, Henning Gerber, Istvan Montvay, Philipp Scior, Pietro Giudice, Sajid Ali, Stefano Piemonte","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-01-24T16:34:00Z","title":"The light bound states of $\\mathcal{N}=1$ supersymmetric SU(3) Yang-Mills theory on the lattice"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.08062","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":"sha256:1aa165ff9c02fcc85130445b06bc3de6123216bbe13b791eab9ce69f71aed6a3","target":"record","created_at":"2026-05-18T00:18:11Z","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":"59e3142acd408994f189be96df6aeab19859090c7f5c9c624789b9d9c6895e79","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-01-24T16:34:00Z","title_canon_sha256":"94a2efc7e2fdfef82f244e754c6f7ba9801131e66374f446ab0bb25d5a5646ec"},"schema_version":"1.0","source":{"id":"1801.08062","kind":"arxiv","version":1}},"canonical_sha256":"c9c9ae697b61255056ba13430d2f7bf6f8b24e244ff64130fcfb9c1309263576","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c9c9ae697b61255056ba13430d2f7bf6f8b24e244ff64130fcfb9c1309263576","first_computed_at":"2026-05-18T00:18:11.500903Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:18:11.500903Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"XGIJlXipsaiEJM+HIXDGHFB4wfLOMdIyEgT6Ggap2FoidI4iOpybDy5unVykkpDcXMvDaua/LFd3YNOyJax1BQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:18:11.501523Z","signed_message":"canonical_sha256_bytes"},"source_id":"1801.08062","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1aa165ff9c02fcc85130445b06bc3de6123216bbe13b791eab9ce69f71aed6a3","sha256:43c2b4deff41acc6a5973c02ff72e2c286ccbc63713c730451b219c5d2617f2a"],"state_sha256":"20aaa71cff4fa6dc35f29c3f5c01ec20c9c2e9b328c776a0fda058dcec879fe8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BTuwc8v3gF5cflb945QYsq4StSPcEp+7KLnuMOgTrAGNYI7Im94OX5wumNup4gU8aTEuc8V5Jyahvlcc0iKPAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T23:00:35.530156Z","bundle_sha256":"2dce23e4ad9540ab2157bd1fc0e0aa45ba650c78ab855c97431c8cfc740e9296"}}