{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:JPJLPSIXGO62JUNGYYJ2H7ZZCE","short_pith_number":"pith:JPJLPSIX","canonical_record":{"source":{"id":"2205.11339","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-05-23T14:32:39Z","cross_cats_sorted":[],"title_canon_sha256":"dce49f460131329c6e329baf2f608176e0582da2f094e9c79844fc71befd11ce","abstract_canon_sha256":"39e2cc7a2ec2b5ad800eb76f1d8a42982dd473986fcdf5d411248d4750baa90f"},"schema_version":"1.0"},"canonical_sha256":"4bd2b7c91733bda4d1a6c613a3ff3911256a9790da98a6d9d54c1c4045ab405f","source":{"kind":"arxiv","id":"2205.11339","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2205.11339","created_at":"2026-07-05T04:45:59Z"},{"alias_kind":"arxiv_version","alias_value":"2205.11339v3","created_at":"2026-07-05T04:45:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2205.11339","created_at":"2026-07-05T04:45:59Z"},{"alias_kind":"pith_short_12","alias_value":"JPJLPSIXGO62","created_at":"2026-07-05T04:45:59Z"},{"alias_kind":"pith_short_16","alias_value":"JPJLPSIXGO62JUNG","created_at":"2026-07-05T04:45:59Z"},{"alias_kind":"pith_short_8","alias_value":"JPJLPSIX","created_at":"2026-07-05T04:45:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:JPJLPSIXGO62JUNGYYJ2H7ZZCE","target":"record","payload":{"canonical_record":{"source":{"id":"2205.11339","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-05-23T14:32:39Z","cross_cats_sorted":[],"title_canon_sha256":"dce49f460131329c6e329baf2f608176e0582da2f094e9c79844fc71befd11ce","abstract_canon_sha256":"39e2cc7a2ec2b5ad800eb76f1d8a42982dd473986fcdf5d411248d4750baa90f"},"schema_version":"1.0"},"canonical_sha256":"4bd2b7c91733bda4d1a6c613a3ff3911256a9790da98a6d9d54c1c4045ab405f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:45:59.793589Z","signature_b64":"COvF/xMFZNjjYczRw3JpT17xaf6gfQNr7sIVBJTqnRgV5YmaIaS3svOH1Kc2xjvM4h+HFeGkZKF9rTq/j7LuAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4bd2b7c91733bda4d1a6c613a3ff3911256a9790da98a6d9d54c1c4045ab405f","last_reissued_at":"2026-07-05T04:45:59.793064Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:45:59.793064Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2205.11339","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":"2026-07-05T04:45:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kGRX+RCOO4MgQ+2Qjoqw4TGIxaVgaLDN/fTwSaeETU0dUvzGINYg+DEWlW8UDfsmM7A6vdDigqXhdAXu5wUSCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-18T10:12:24.563099Z"},"content_sha256":"0ab22607d0227f007112459fc1284ac7b5189c857cc69ba855d18bcd30c75168","schema_version":"1.0","event_id":"sha256:0ab22607d0227f007112459fc1284ac7b5189c857cc69ba855d18bcd30c75168"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:JPJLPSIXGO62JUNGYYJ2H7ZZCE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Semiclassics with 't Hooft flux background for QCD with $2$-index quarks","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Mithat \\\"Unsal, Yuya Tanizaki","submitted_at":"2022-05-23T14:32:39Z","abstract_excerpt":"We study quantum chromodynamics including the two-index symmetric or anti-symmetric quark (QCD(Sym/ASym)) on small $\\mathbb{R}^2\\times T^2$ with a suitable magnetic flux. We first discuss the 't Hooft anomaly of these theories and claim that discrete chiral symmetry should be spontaneously broken completely to satisfy the anomaly matching condition. The $T^2$ compactification with the magnetic flux preserves the 't Hooft anomaly, and the $2$d effective theory is constrained by the same anomaly of $4$d QCD(Sym/ASym). We demonstrate the spontaneous breakdown of chiral symmetry using the dilute g"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2205.11339","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2205.11339/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T04:45:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LFFDwbaT3NlQ3poYoaPLUXPo8INyNUCxgcm19yseDJsEELwhWb6Win/0oaBFu4mxX4EY66lKk34gQCvoyZeADQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-18T10:12:24.564103Z"},"content_sha256":"2101c23e45b02a66e4fe44c4c1451a5be5eb0cc4ee3ea840a8a26be0dd571a61","schema_version":"1.0","event_id":"sha256:2101c23e45b02a66e4fe44c4c1451a5be5eb0cc4ee3ea840a8a26be0dd571a61"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JPJLPSIXGO62JUNGYYJ2H7ZZCE/bundle.json","state_url":"https://pith.science/pith/JPJLPSIXGO62JUNGYYJ2H7ZZCE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JPJLPSIXGO62JUNGYYJ2H7ZZCE/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":"2026-08-18T10:12:24Z","links":{"resolver":"https://pith.science/pith/JPJLPSIXGO62JUNGYYJ2H7ZZCE","bundle":"https://pith.science/pith/JPJLPSIXGO62JUNGYYJ2H7ZZCE/bundle.json","state":"https://pith.science/pith/JPJLPSIXGO62JUNGYYJ2H7ZZCE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JPJLPSIXGO62JUNGYYJ2H7ZZCE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:JPJLPSIXGO62JUNGYYJ2H7ZZCE","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":"39e2cc7a2ec2b5ad800eb76f1d8a42982dd473986fcdf5d411248d4750baa90f","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-05-23T14:32:39Z","title_canon_sha256":"dce49f460131329c6e329baf2f608176e0582da2f094e9c79844fc71befd11ce"},"schema_version":"1.0","source":{"id":"2205.11339","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2205.11339","created_at":"2026-07-05T04:45:59Z"},{"alias_kind":"arxiv_version","alias_value":"2205.11339v3","created_at":"2026-07-05T04:45:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2205.11339","created_at":"2026-07-05T04:45:59Z"},{"alias_kind":"pith_short_12","alias_value":"JPJLPSIXGO62","created_at":"2026-07-05T04:45:59Z"},{"alias_kind":"pith_short_16","alias_value":"JPJLPSIXGO62JUNG","created_at":"2026-07-05T04:45:59Z"},{"alias_kind":"pith_short_8","alias_value":"JPJLPSIX","created_at":"2026-07-05T04:45:59Z"}],"graph_snapshots":[{"event_id":"sha256:2101c23e45b02a66e4fe44c4c1451a5be5eb0cc4ee3ea840a8a26be0dd571a61","target":"graph","created_at":"2026-07-05T04:45:59Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2205.11339/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study quantum chromodynamics including the two-index symmetric or anti-symmetric quark (QCD(Sym/ASym)) on small $\\mathbb{R}^2\\times T^2$ with a suitable magnetic flux. We first discuss the 't Hooft anomaly of these theories and claim that discrete chiral symmetry should be spontaneously broken completely to satisfy the anomaly matching condition. The $T^2$ compactification with the magnetic flux preserves the 't Hooft anomaly, and the $2$d effective theory is constrained by the same anomaly of $4$d QCD(Sym/ASym). We demonstrate the spontaneous breakdown of chiral symmetry using the dilute g","authors_text":"Mithat \\\"Unsal, Yuya Tanizaki","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-05-23T14:32:39Z","title":"Semiclassics with 't Hooft flux background for QCD with $2$-index quarks"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2205.11339","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":"sha256:0ab22607d0227f007112459fc1284ac7b5189c857cc69ba855d18bcd30c75168","target":"record","created_at":"2026-07-05T04:45:59Z","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":"39e2cc7a2ec2b5ad800eb76f1d8a42982dd473986fcdf5d411248d4750baa90f","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-05-23T14:32:39Z","title_canon_sha256":"dce49f460131329c6e329baf2f608176e0582da2f094e9c79844fc71befd11ce"},"schema_version":"1.0","source":{"id":"2205.11339","kind":"arxiv","version":3}},"canonical_sha256":"4bd2b7c91733bda4d1a6c613a3ff3911256a9790da98a6d9d54c1c4045ab405f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4bd2b7c91733bda4d1a6c613a3ff3911256a9790da98a6d9d54c1c4045ab405f","first_computed_at":"2026-07-05T04:45:59.793064Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:45:59.793064Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"COvF/xMFZNjjYczRw3JpT17xaf6gfQNr7sIVBJTqnRgV5YmaIaS3svOH1Kc2xjvM4h+HFeGkZKF9rTq/j7LuAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T04:45:59.793589Z","signed_message":"canonical_sha256_bytes"},"source_id":"2205.11339","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0ab22607d0227f007112459fc1284ac7b5189c857cc69ba855d18bcd30c75168","sha256:2101c23e45b02a66e4fe44c4c1451a5be5eb0cc4ee3ea840a8a26be0dd571a61"],"state_sha256":"163df2bdc9c1c35dd8e00c83c076e6c4f3eca27c7e78b36f2831cfc49c7863de"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"10eGpgan5HdlQIEpQ1PQtHwk+eMbxEaxD0YPv3Nv6EhP8Bpvtyuwy1AKQKrVkBvbTKGfdBxz7SCEDOhEq4L4Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-18T10:12:24.571743Z","bundle_sha256":"d4770fb9a5eb27789b5b6100c29cc9cf3c7885f9d208fdcb73ef18f2489beca3"}}