{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:SNC67DAXT4NRWXGLDRCWZ2QYLJ","short_pith_number":"pith:SNC67DAX","canonical_record":{"source":{"id":"2404.14152","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-04-22T13:01:52Z","cross_cats_sorted":[],"title_canon_sha256":"b422c2b551c052edd91a70475a387cd6e40f141960ecf6421a6ba51189a8f975","abstract_canon_sha256":"a569707fef51f3fdf94c5b6f31c7387533f3568077aac5786ec0bbeb5d092366"},"schema_version":"1.0"},"canonical_sha256":"9345ef8c179f1b1b5ccb1c456cea185a6c2d29e2cd3c1bb4f427b054820931d6","source":{"kind":"arxiv","id":"2404.14152","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2404.14152","created_at":"2026-07-05T08:10:42Z"},{"alias_kind":"arxiv_version","alias_value":"2404.14152v1","created_at":"2026-07-05T08:10:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.14152","created_at":"2026-07-05T08:10:42Z"},{"alias_kind":"pith_short_12","alias_value":"SNC67DAXT4NR","created_at":"2026-07-05T08:10:42Z"},{"alias_kind":"pith_short_16","alias_value":"SNC67DAXT4NRWXGL","created_at":"2026-07-05T08:10:42Z"},{"alias_kind":"pith_short_8","alias_value":"SNC67DAX","created_at":"2026-07-05T08:10:42Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:SNC67DAXT4NRWXGLDRCWZ2QYLJ","target":"record","payload":{"canonical_record":{"source":{"id":"2404.14152","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-04-22T13:01:52Z","cross_cats_sorted":[],"title_canon_sha256":"b422c2b551c052edd91a70475a387cd6e40f141960ecf6421a6ba51189a8f975","abstract_canon_sha256":"a569707fef51f3fdf94c5b6f31c7387533f3568077aac5786ec0bbeb5d092366"},"schema_version":"1.0"},"canonical_sha256":"9345ef8c179f1b1b5ccb1c456cea185a6c2d29e2cd3c1bb4f427b054820931d6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:10:42.680234Z","signature_b64":"ipqQVOqDciHi41iTVirCirBI9dh53IEdZXyiYX01nW5EyNN0gNafg0ncQyEiYCQwucqu5n3Zg962FtlF2KW2Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9345ef8c179f1b1b5ccb1c456cea185a6c2d29e2cd3c1bb4f427b054820931d6","last_reissued_at":"2026-07-05T08:10:42.679756Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:10:42.679756Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2404.14152","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":"2026-07-05T08:10:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"87kavRPFJDyi7NaCJeID+1FcrR0eG5/yZjVlerpCEwNuQHWHdGH4G+Scn9d9+3Yg7iCTRtEQjNyh81SBKug4Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T10:53:53.132934Z"},"content_sha256":"a959a56a3bcb8b34c62ddbeeb88270975fc8c3d8bb8f70c3c7e4182994aad947","schema_version":"1.0","event_id":"sha256:a959a56a3bcb8b34c62ddbeeb88270975fc8c3d8bb8f70c3c7e4182994aad947"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:SNC67DAXT4NRWXGLDRCWZ2QYLJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Complete $CP$ Eigen-bases of Mesonic Chiral Lagrangian up to $p^8$-order","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Feng-Jie Tang, Hao Sun, Jiang-Hao Yu, Xuan-He Li","submitted_at":"2024-04-22T13:01:52Z","abstract_excerpt":"Chiral perturbation theory systematically describes the low energy dynamics of meson and baryons using nonlinear Nambu-Goldstone fields. Using the Young tensor technique, we construct the pure mesonic effective operators up to $p^8$-order, one-to-one corresponding to contact amplitudes with the on-shell Adler zero condition. The off-shell external sources, non-vanishing under equation-of-motion conditions, are also added to the operator bases. We also show the invariant tensor bases using the Young tableau is equivalent to the trace bases with Cayley-Hamilton relations. Separated into differen"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.14152","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2404.14152/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":"2026-07-05T08:10:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ykhJJX8R/CkRxvaTyzWLuUZvtxshGObCprSbc4sOw6vXNHw/VoUOusjoRuD4nPnOIAruo1ewH2vZcNSr8y9WBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T10:53:53.133419Z"},"content_sha256":"fc2a63d31c796a609fa7d1798684ddb340441c293dc67da8abe570ff32f6f42e","schema_version":"1.0","event_id":"sha256:fc2a63d31c796a609fa7d1798684ddb340441c293dc67da8abe570ff32f6f42e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SNC67DAXT4NRWXGLDRCWZ2QYLJ/bundle.json","state_url":"https://pith.science/pith/SNC67DAXT4NRWXGLDRCWZ2QYLJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SNC67DAXT4NRWXGLDRCWZ2QYLJ/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":"2026-08-07T10:53:53Z","links":{"resolver":"https://pith.science/pith/SNC67DAXT4NRWXGLDRCWZ2QYLJ","bundle":"https://pith.science/pith/SNC67DAXT4NRWXGLDRCWZ2QYLJ/bundle.json","state":"https://pith.science/pith/SNC67DAXT4NRWXGLDRCWZ2QYLJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SNC67DAXT4NRWXGLDRCWZ2QYLJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:SNC67DAXT4NRWXGLDRCWZ2QYLJ","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":"a569707fef51f3fdf94c5b6f31c7387533f3568077aac5786ec0bbeb5d092366","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-04-22T13:01:52Z","title_canon_sha256":"b422c2b551c052edd91a70475a387cd6e40f141960ecf6421a6ba51189a8f975"},"schema_version":"1.0","source":{"id":"2404.14152","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2404.14152","created_at":"2026-07-05T08:10:42Z"},{"alias_kind":"arxiv_version","alias_value":"2404.14152v1","created_at":"2026-07-05T08:10:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.14152","created_at":"2026-07-05T08:10:42Z"},{"alias_kind":"pith_short_12","alias_value":"SNC67DAXT4NR","created_at":"2026-07-05T08:10:42Z"},{"alias_kind":"pith_short_16","alias_value":"SNC67DAXT4NRWXGL","created_at":"2026-07-05T08:10:42Z"},{"alias_kind":"pith_short_8","alias_value":"SNC67DAX","created_at":"2026-07-05T08:10:42Z"}],"graph_snapshots":[{"event_id":"sha256:fc2a63d31c796a609fa7d1798684ddb340441c293dc67da8abe570ff32f6f42e","target":"graph","created_at":"2026-07-05T08:10:42Z","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/2404.14152/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Chiral perturbation theory systematically describes the low energy dynamics of meson and baryons using nonlinear Nambu-Goldstone fields. Using the Young tensor technique, we construct the pure mesonic effective operators up to $p^8$-order, one-to-one corresponding to contact amplitudes with the on-shell Adler zero condition. The off-shell external sources, non-vanishing under equation-of-motion conditions, are also added to the operator bases. We also show the invariant tensor bases using the Young tableau is equivalent to the trace bases with Cayley-Hamilton relations. Separated into differen","authors_text":"Feng-Jie Tang, Hao Sun, Jiang-Hao Yu, Xuan-He Li","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-04-22T13:01:52Z","title":"Complete $CP$ Eigen-bases of Mesonic Chiral Lagrangian up to $p^8$-order"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.14152","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:a959a56a3bcb8b34c62ddbeeb88270975fc8c3d8bb8f70c3c7e4182994aad947","target":"record","created_at":"2026-07-05T08:10:42Z","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":"a569707fef51f3fdf94c5b6f31c7387533f3568077aac5786ec0bbeb5d092366","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-04-22T13:01:52Z","title_canon_sha256":"b422c2b551c052edd91a70475a387cd6e40f141960ecf6421a6ba51189a8f975"},"schema_version":"1.0","source":{"id":"2404.14152","kind":"arxiv","version":1}},"canonical_sha256":"9345ef8c179f1b1b5ccb1c456cea185a6c2d29e2cd3c1bb4f427b054820931d6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9345ef8c179f1b1b5ccb1c456cea185a6c2d29e2cd3c1bb4f427b054820931d6","first_computed_at":"2026-07-05T08:10:42.679756Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:10:42.679756Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ipqQVOqDciHi41iTVirCirBI9dh53IEdZXyiYX01nW5EyNN0gNafg0ncQyEiYCQwucqu5n3Zg962FtlF2KW2Dw==","signature_status":"signed_v1","signed_at":"2026-07-05T08:10:42.680234Z","signed_message":"canonical_sha256_bytes"},"source_id":"2404.14152","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a959a56a3bcb8b34c62ddbeeb88270975fc8c3d8bb8f70c3c7e4182994aad947","sha256:fc2a63d31c796a609fa7d1798684ddb340441c293dc67da8abe570ff32f6f42e"],"state_sha256":"fe363b0c3245d184a58b454b92c21039ea11f948cf217549bce66349f40fab4e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7QuyISkV2V2djAj4O17njhdwxZXZDUjaphIIh5JbhuRF6+CIUJV2s2W8euxffoUlpGphQZ3+2c3ZbYOgJqShAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-07T10:53:53.137266Z","bundle_sha256":"d6b69c0dbc9c0a8fabe5b77b6dc37b8c43055f3f007e9ee19f4b07eacbb6e887"}}