{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:KDC7D56GJFR6R433MRJCSFOFTY","short_pith_number":"pith:KDC7D56G","canonical_record":{"source":{"id":"1801.05444","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-01-16T19:00:33Z","cross_cats_sorted":[],"title_canon_sha256":"db1e843e94d1c2b5d149ecf4467e4de204299177af5ac8df3a86560a90113470","abstract_canon_sha256":"3c69282cf468d5a3473929083f05fe3ca05caf82ce5e1c72c7709e50432320c7"},"schema_version":"1.0"},"canonical_sha256":"50c5f1f7c64963e8f37b64522915c59e21e8d24c399f7a1280c861340652ef57","source":{"kind":"arxiv","id":"1801.05444","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.05444","created_at":"2026-05-18T00:16:36Z"},{"alias_kind":"arxiv_version","alias_value":"1801.05444v2","created_at":"2026-05-18T00:16:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.05444","created_at":"2026-05-18T00:16:36Z"},{"alias_kind":"pith_short_12","alias_value":"KDC7D56GJFR6","created_at":"2026-05-18T12:32:33Z"},{"alias_kind":"pith_short_16","alias_value":"KDC7D56GJFR6R433","created_at":"2026-05-18T12:32:33Z"},{"alias_kind":"pith_short_8","alias_value":"KDC7D56G","created_at":"2026-05-18T12:32:33Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:KDC7D56GJFR6R433MRJCSFOFTY","target":"record","payload":{"canonical_record":{"source":{"id":"1801.05444","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-01-16T19:00:33Z","cross_cats_sorted":[],"title_canon_sha256":"db1e843e94d1c2b5d149ecf4467e4de204299177af5ac8df3a86560a90113470","abstract_canon_sha256":"3c69282cf468d5a3473929083f05fe3ca05caf82ce5e1c72c7709e50432320c7"},"schema_version":"1.0"},"canonical_sha256":"50c5f1f7c64963e8f37b64522915c59e21e8d24c399f7a1280c861340652ef57","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:16:36.462657Z","signature_b64":"eNZbka6GdkGdVzji8I4QkJ4mREFpRgqNqkbEMCFhzUcM1ebGKXAcuw2M1ESLjFxoLkSHf4/CQ28GG0Qu1u/NDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"50c5f1f7c64963e8f37b64522915c59e21e8d24c399f7a1280c861340652ef57","last_reissued_at":"2026-05-18T00:16:36.462053Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:16:36.462053Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1801.05444","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:16:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6kFOq0hYJVoJ8OCij9C5uzkDxXKRhFLXvXyzSlgdF39o3cEMO+uFv9Z9PGObKB1fde2+XY1Jw2fcrra8J5weAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T22:14:49.978176Z"},"content_sha256":"ea4bf399374d3a1efd1b948158b13198e8fdea299ca402f04b48261cf536ff91","schema_version":"1.0","event_id":"sha256:ea4bf399374d3a1efd1b948158b13198e8fdea299ca402f04b48261cf536ff91"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:KDC7D56GJFR6R433MRJCSFOFTY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Classification of NLO operators for composite Higgs models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F.Sannino, G.Cacciapaglia, N.Bizot, T.Alanne","submitted_at":"2018-01-16T19:00:33Z","abstract_excerpt":"We provide a general classification of template operators, up to next-to-leading order, that appear in chiral perturbation theories based on the two flavour patterns of spontaneous symmetry breaking SU($N_F$)/Sp($N_F$) and SU($N_F$)/SO($N_F$). All possible explicit-breaking sources parametrised by spurions transforming in the fundamental and in the two-index representations of the flavour symmetry are included. While our general framework can be applied to any model of strong dynamics, we specialise to composite-Higgs models, where the main explicit breaking sources are a current mass, the gau"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.05444","kind":"arxiv","version":2},"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":"2026-05-18T00:16:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zIwGQUXohkU6gO2qJqySt1KtY12baLm2TCGmZte+TfZbAy0JpoI4COd2RlpMMr9ruWnfXJboJBliN4gotOVCBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T22:14:49.978934Z"},"content_sha256":"8065695cbf6681430e7476ad2229e5a4508bbe0a9f2dc3bbe3b430ab89c5b63c","schema_version":"1.0","event_id":"sha256:8065695cbf6681430e7476ad2229e5a4508bbe0a9f2dc3bbe3b430ab89c5b63c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KDC7D56GJFR6R433MRJCSFOFTY/bundle.json","state_url":"https://pith.science/pith/KDC7D56GJFR6R433MRJCSFOFTY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KDC7D56GJFR6R433MRJCSFOFTY/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":"2026-05-31T22:14:49Z","links":{"resolver":"https://pith.science/pith/KDC7D56GJFR6R433MRJCSFOFTY","bundle":"https://pith.science/pith/KDC7D56GJFR6R433MRJCSFOFTY/bundle.json","state":"https://pith.science/pith/KDC7D56GJFR6R433MRJCSFOFTY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KDC7D56GJFR6R433MRJCSFOFTY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:KDC7D56GJFR6R433MRJCSFOFTY","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":"3c69282cf468d5a3473929083f05fe3ca05caf82ce5e1c72c7709e50432320c7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-01-16T19:00:33Z","title_canon_sha256":"db1e843e94d1c2b5d149ecf4467e4de204299177af5ac8df3a86560a90113470"},"schema_version":"1.0","source":{"id":"1801.05444","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.05444","created_at":"2026-05-18T00:16:36Z"},{"alias_kind":"arxiv_version","alias_value":"1801.05444v2","created_at":"2026-05-18T00:16:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.05444","created_at":"2026-05-18T00:16:36Z"},{"alias_kind":"pith_short_12","alias_value":"KDC7D56GJFR6","created_at":"2026-05-18T12:32:33Z"},{"alias_kind":"pith_short_16","alias_value":"KDC7D56GJFR6R433","created_at":"2026-05-18T12:32:33Z"},{"alias_kind":"pith_short_8","alias_value":"KDC7D56G","created_at":"2026-05-18T12:32:33Z"}],"graph_snapshots":[{"event_id":"sha256:8065695cbf6681430e7476ad2229e5a4508bbe0a9f2dc3bbe3b430ab89c5b63c","target":"graph","created_at":"2026-05-18T00:16:36Z","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 general classification of template operators, up to next-to-leading order, that appear in chiral perturbation theories based on the two flavour patterns of spontaneous symmetry breaking SU($N_F$)/Sp($N_F$) and SU($N_F$)/SO($N_F$). All possible explicit-breaking sources parametrised by spurions transforming in the fundamental and in the two-index representations of the flavour symmetry are included. While our general framework can be applied to any model of strong dynamics, we specialise to composite-Higgs models, where the main explicit breaking sources are a current mass, the gau","authors_text":"F.Sannino, G.Cacciapaglia, N.Bizot, T.Alanne","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-01-16T19:00:33Z","title":"Classification of NLO operators for composite Higgs models"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.05444","kind":"arxiv","version":2},"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:ea4bf399374d3a1efd1b948158b13198e8fdea299ca402f04b48261cf536ff91","target":"record","created_at":"2026-05-18T00:16:36Z","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":"3c69282cf468d5a3473929083f05fe3ca05caf82ce5e1c72c7709e50432320c7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-01-16T19:00:33Z","title_canon_sha256":"db1e843e94d1c2b5d149ecf4467e4de204299177af5ac8df3a86560a90113470"},"schema_version":"1.0","source":{"id":"1801.05444","kind":"arxiv","version":2}},"canonical_sha256":"50c5f1f7c64963e8f37b64522915c59e21e8d24c399f7a1280c861340652ef57","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"50c5f1f7c64963e8f37b64522915c59e21e8d24c399f7a1280c861340652ef57","first_computed_at":"2026-05-18T00:16:36.462053Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:16:36.462053Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"eNZbka6GdkGdVzji8I4QkJ4mREFpRgqNqkbEMCFhzUcM1ebGKXAcuw2M1ESLjFxoLkSHf4/CQ28GG0Qu1u/NDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:16:36.462657Z","signed_message":"canonical_sha256_bytes"},"source_id":"1801.05444","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ea4bf399374d3a1efd1b948158b13198e8fdea299ca402f04b48261cf536ff91","sha256:8065695cbf6681430e7476ad2229e5a4508bbe0a9f2dc3bbe3b430ab89c5b63c"],"state_sha256":"b3c73f52e75812530663fd84371b8f169f328d821667f51b31148cb5c2cae71b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IB4d7SAElBtNNesxdWETs7G+Oi9ttKxXIKdr1PEtOlEObS9Fjm9YMWTJIWlpuQYaJiXJEOT3mGiCSnez3hdMDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T22:14:49.982835Z","bundle_sha256":"b9a933bfdf8881868101e868b1fda8cdc76dbfd1a6624d02271c9d77ccbb18ca"}}