{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2021:FVJ2G72O6Y23HM4BUS73S54KWQ","short_pith_number":"pith:FVJ2G72O","canonical_record":{"source":{"id":"2105.03921","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-05-09T12:33:14Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"4c2df8aca832dcbac81db684cdcc1b2ff8d8a086b0da414302f98bc94377f231","abstract_canon_sha256":"0d141ff162287a87060916c91e21f331c8eae890128e00f1a297691890e8b122"},"schema_version":"1.0"},"canonical_sha256":"2d53a37f4ef635b3b381a4bfb9778ab40b6aa1dfa34d99ac184cbcc09ce925fb","source":{"kind":"arxiv","id":"2105.03921","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2105.03921","created_at":"2026-07-05T03:10:08Z"},{"alias_kind":"arxiv_version","alias_value":"2105.03921v3","created_at":"2026-07-05T03:10:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2105.03921","created_at":"2026-07-05T03:10:08Z"},{"alias_kind":"pith_short_12","alias_value":"FVJ2G72O6Y23","created_at":"2026-07-05T03:10:08Z"},{"alias_kind":"pith_short_16","alias_value":"FVJ2G72O6Y23HM4B","created_at":"2026-07-05T03:10:08Z"},{"alias_kind":"pith_short_8","alias_value":"FVJ2G72O","created_at":"2026-07-05T03:10:08Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2021:FVJ2G72O6Y23HM4BUS73S54KWQ","target":"record","payload":{"canonical_record":{"source":{"id":"2105.03921","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-05-09T12:33:14Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"4c2df8aca832dcbac81db684cdcc1b2ff8d8a086b0da414302f98bc94377f231","abstract_canon_sha256":"0d141ff162287a87060916c91e21f331c8eae890128e00f1a297691890e8b122"},"schema_version":"1.0"},"canonical_sha256":"2d53a37f4ef635b3b381a4bfb9778ab40b6aa1dfa34d99ac184cbcc09ce925fb","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:10:08.209818Z","signature_b64":"xvMjlqBr78OpaPmvmfWwKO+9rUWAsVHi5AjZaTZhHOPWUNNEDYW3fjLuuNWcKke+8J6eaRqe6B3vGpcBeGOLDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2d53a37f4ef635b3b381a4bfb9778ab40b6aa1dfa34d99ac184cbcc09ce925fb","last_reissued_at":"2026-07-05T03:10:08.209409Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:10:08.209409Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2105.03921","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":"2026-07-05T03:10:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VmNCAhDzA+1g8TKTmCLm0IYv0keRaN/6rD5HbXGj1cxUhUKnSVDytISST3hLBaiZV/FIpVG81gPcl+y6NymcCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-24T00:25:34.653989Z"},"content_sha256":"4b1553599185bb8a7adf14e652e65835ec0c707b01692423a04b458459b363e0","schema_version":"1.0","event_id":"sha256:4b1553599185bb8a7adf14e652e65835ec0c707b01692423a04b458459b363e0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2021:FVJ2G72O6Y23HM4BUS73S54KWQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Strong anomaly and phases of chiral gauge theories","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"Andrea Luzio, Kenichi Konishi, Stefano Bolognesi","submitted_at":"2021-05-09T12:33:14Z","abstract_excerpt":"We present a simple argument which seems to favor, when applied to a large class of strongly-coupled chiral gauge theories, a dynamical-Higgs-phase scenario, characterized by certain bifermion condensates. Flavor symmetric confining vacua described in the infrared by a set of baryonlike massless composite fermions saturating the conventional 't Hooft anomaly matching equations, appear instead disfavored. Our basic criterion is that it should be possible to write a strong-anomaly effective action, analogous to the one used in QCD to describe the solution of the $U(1)_A$ problem in the low-energ"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2105.03921","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/2105.03921/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":"2026-07-05T03:10:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZOmDxKN9FIpQbROGSXzU7kfU6RngV722rS8xHB9GlYfBGpdy712FdvdhVMysdljJ7X6fCUESscseDYOB38soAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-24T00:25:34.654671Z"},"content_sha256":"cd5775fcf52c0ec34c1ad983f094f3c25cee9be5546e3eb6fc5b277c65bd668c","schema_version":"1.0","event_id":"sha256:cd5775fcf52c0ec34c1ad983f094f3c25cee9be5546e3eb6fc5b277c65bd668c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FVJ2G72O6Y23HM4BUS73S54KWQ/bundle.json","state_url":"https://pith.science/pith/FVJ2G72O6Y23HM4BUS73S54KWQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FVJ2G72O6Y23HM4BUS73S54KWQ/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":"2026-08-24T00:25:34Z","links":{"resolver":"https://pith.science/pith/FVJ2G72O6Y23HM4BUS73S54KWQ","bundle":"https://pith.science/pith/FVJ2G72O6Y23HM4BUS73S54KWQ/bundle.json","state":"https://pith.science/pith/FVJ2G72O6Y23HM4BUS73S54KWQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FVJ2G72O6Y23HM4BUS73S54KWQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:FVJ2G72O6Y23HM4BUS73S54KWQ","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":"0d141ff162287a87060916c91e21f331c8eae890128e00f1a297691890e8b122","cross_cats_sorted":["hep-lat","hep-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-05-09T12:33:14Z","title_canon_sha256":"4c2df8aca832dcbac81db684cdcc1b2ff8d8a086b0da414302f98bc94377f231"},"schema_version":"1.0","source":{"id":"2105.03921","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2105.03921","created_at":"2026-07-05T03:10:08Z"},{"alias_kind":"arxiv_version","alias_value":"2105.03921v3","created_at":"2026-07-05T03:10:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2105.03921","created_at":"2026-07-05T03:10:08Z"},{"alias_kind":"pith_short_12","alias_value":"FVJ2G72O6Y23","created_at":"2026-07-05T03:10:08Z"},{"alias_kind":"pith_short_16","alias_value":"FVJ2G72O6Y23HM4B","created_at":"2026-07-05T03:10:08Z"},{"alias_kind":"pith_short_8","alias_value":"FVJ2G72O","created_at":"2026-07-05T03:10:08Z"}],"graph_snapshots":[{"event_id":"sha256:cd5775fcf52c0ec34c1ad983f094f3c25cee9be5546e3eb6fc5b277c65bd668c","target":"graph","created_at":"2026-07-05T03:10:08Z","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/2105.03921/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present a simple argument which seems to favor, when applied to a large class of strongly-coupled chiral gauge theories, a dynamical-Higgs-phase scenario, characterized by certain bifermion condensates. Flavor symmetric confining vacua described in the infrared by a set of baryonlike massless composite fermions saturating the conventional 't Hooft anomaly matching equations, appear instead disfavored. Our basic criterion is that it should be possible to write a strong-anomaly effective action, analogous to the one used in QCD to describe the solution of the $U(1)_A$ problem in the low-energ","authors_text":"Andrea Luzio, Kenichi Konishi, Stefano Bolognesi","cross_cats":["hep-lat","hep-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-05-09T12:33:14Z","title":"Strong anomaly and phases of chiral gauge theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2105.03921","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":"sha256:4b1553599185bb8a7adf14e652e65835ec0c707b01692423a04b458459b363e0","target":"record","created_at":"2026-07-05T03:10:08Z","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":"0d141ff162287a87060916c91e21f331c8eae890128e00f1a297691890e8b122","cross_cats_sorted":["hep-lat","hep-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-05-09T12:33:14Z","title_canon_sha256":"4c2df8aca832dcbac81db684cdcc1b2ff8d8a086b0da414302f98bc94377f231"},"schema_version":"1.0","source":{"id":"2105.03921","kind":"arxiv","version":3}},"canonical_sha256":"2d53a37f4ef635b3b381a4bfb9778ab40b6aa1dfa34d99ac184cbcc09ce925fb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2d53a37f4ef635b3b381a4bfb9778ab40b6aa1dfa34d99ac184cbcc09ce925fb","first_computed_at":"2026-07-05T03:10:08.209409Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T03:10:08.209409Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xvMjlqBr78OpaPmvmfWwKO+9rUWAsVHi5AjZaTZhHOPWUNNEDYW3fjLuuNWcKke+8J6eaRqe6B3vGpcBeGOLDw==","signature_status":"signed_v1","signed_at":"2026-07-05T03:10:08.209818Z","signed_message":"canonical_sha256_bytes"},"source_id":"2105.03921","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4b1553599185bb8a7adf14e652e65835ec0c707b01692423a04b458459b363e0","sha256:cd5775fcf52c0ec34c1ad983f094f3c25cee9be5546e3eb6fc5b277c65bd668c"],"state_sha256":"62d5575d24f41689b905b28f50e36f1e8d99b494fba8e38b3756f9654360da66"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Wq+QyGuGx3G2bng9Y+XYwcxcOAMkIYa0uMUVKz342NtXlXc/jLRNnxitTmM/9bat5UCYuKLfF9SOM032J9eKAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-24T00:25:34.659752Z","bundle_sha256":"6eec794cbefa3a196208a7568005fd22296477f56ebbe096848e29463be53c63"}}