{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:RQTWF2MF3OV4Y3UXJ4N3RFVYSD","short_pith_number":"pith:RQTWF2MF","canonical_record":{"source":{"id":"2502.08537","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-02-12T16:21:12Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci","physics.optics"],"title_canon_sha256":"a878075fb40ef53a511f0618599069ddcea7545d7fd368b2281015bc57fc21d1","abstract_canon_sha256":"a01f306669d7fb3a5f460f7b8d0205f02de1baa328ca6a45cef6b9bbb5317cb7"},"schema_version":"1.0"},"canonical_sha256":"8c2762e985dbabcc6e974f1bb896b890d5761a64bb0810a94c19233cc6b79ab9","source":{"kind":"arxiv","id":"2502.08537","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2502.08537","created_at":"2026-07-05T10:59:49Z"},{"alias_kind":"arxiv_version","alias_value":"2502.08537v1","created_at":"2026-07-05T10:59:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.08537","created_at":"2026-07-05T10:59:49Z"},{"alias_kind":"pith_short_12","alias_value":"RQTWF2MF3OV4","created_at":"2026-07-05T10:59:49Z"},{"alias_kind":"pith_short_16","alias_value":"RQTWF2MF3OV4Y3UX","created_at":"2026-07-05T10:59:49Z"},{"alias_kind":"pith_short_8","alias_value":"RQTWF2MF","created_at":"2026-07-05T10:59:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:RQTWF2MF3OV4Y3UXJ4N3RFVYSD","target":"record","payload":{"canonical_record":{"source":{"id":"2502.08537","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-02-12T16:21:12Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci","physics.optics"],"title_canon_sha256":"a878075fb40ef53a511f0618599069ddcea7545d7fd368b2281015bc57fc21d1","abstract_canon_sha256":"a01f306669d7fb3a5f460f7b8d0205f02de1baa328ca6a45cef6b9bbb5317cb7"},"schema_version":"1.0"},"canonical_sha256":"8c2762e985dbabcc6e974f1bb896b890d5761a64bb0810a94c19233cc6b79ab9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:59:49.194312Z","signature_b64":"oBEU4O4mwMPYMFPWvtr65oXQHKIPzAJmQFID/Lrlsr+gTfMPDW+tM0f2/mgfd+XHRoakKATiZYZW6aYinWrRAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8c2762e985dbabcc6e974f1bb896b890d5761a64bb0810a94c19233cc6b79ab9","last_reissued_at":"2026-07-05T10:59:49.193827Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:59:49.193827Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2502.08537","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":"2026-07-05T10:59:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BcSrRF3ioKu1kKfb2MJ0grTv27S07BVL6HKnmdS51j+7u90dB47aZoPKBhObYMT1jJpKlw9e9+RkC1uJbDTLBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-06T18:42:07.778714Z"},"content_sha256":"ad4c80702bdd3404e531a0b08fd4ecf6a651ba147cb398673e490cc25c67936a","schema_version":"1.0","event_id":"sha256:ad4c80702bdd3404e531a0b08fd4ecf6a651ba147cb398673e490cc25c67936a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:RQTWF2MF3OV4Y3UXJ4N3RFVYSD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Broken symmetries associated with a Kagome chiral charge order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.mtrl-sci","physics.optics"],"primary_cat":"cond-mat.str-el","authors_text":"Byunghoon Kim, Guoqing Chang, Jia-Xin Yin, Jinjin Liu, Junyi Zhang, Luis Balicas, Maksim Litskevich, Md Shafayat Hossain, Mohammad Yahyavi, M. Zahid Hasan, Qi Zhang, Sen Shao, Tyler A. Cochran, Xian Yang, Yilin Zhao, Yongkai Li, Yugui Yao, Yu-Xiao Jiang, Zhiwei Wang, Zi-Jia Cheng","submitted_at":"2025-02-12T16:21:12Z","abstract_excerpt":"Chirality or handedness manifests in all fields of science, ranging from cell biology, molecular interaction, and catalysis to different branches of physics. In condensed matter physics, chirality is intrinsic to enigmatic quantum phases, such as chiral charge density waves and chiral superconductivity. Here, the underlying chiral response is subtle and leads to broken symmetries in the ground state. Detection of subtle broken symmetries is the key to understand these quantum states but they are extremely challenging to expose leading to debate and controversy. Here, using second-order optical"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.08537","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/2502.08537/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":"2026-07-05T10:59:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VxxWIDncYW4q4d/Yu0YtnOFC0piKs5f6k72rCGjVYLvPXYhv7vRSkW/+D996CIbr6DjuINiIPZAcZvk7fyESDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-06T18:42:07.779092Z"},"content_sha256":"2bd75b4a5411ba67c8716ce5fea20ee1852656f6a2a4214f0e4040883c670e4c","schema_version":"1.0","event_id":"sha256:2bd75b4a5411ba67c8716ce5fea20ee1852656f6a2a4214f0e4040883c670e4c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RQTWF2MF3OV4Y3UXJ4N3RFVYSD/bundle.json","state_url":"https://pith.science/pith/RQTWF2MF3OV4Y3UXJ4N3RFVYSD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RQTWF2MF3OV4Y3UXJ4N3RFVYSD/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":"2026-07-06T18:42:07Z","links":{"resolver":"https://pith.science/pith/RQTWF2MF3OV4Y3UXJ4N3RFVYSD","bundle":"https://pith.science/pith/RQTWF2MF3OV4Y3UXJ4N3RFVYSD/bundle.json","state":"https://pith.science/pith/RQTWF2MF3OV4Y3UXJ4N3RFVYSD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RQTWF2MF3OV4Y3UXJ4N3RFVYSD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:RQTWF2MF3OV4Y3UXJ4N3RFVYSD","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":"a01f306669d7fb3a5f460f7b8d0205f02de1baa328ca6a45cef6b9bbb5317cb7","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-02-12T16:21:12Z","title_canon_sha256":"a878075fb40ef53a511f0618599069ddcea7545d7fd368b2281015bc57fc21d1"},"schema_version":"1.0","source":{"id":"2502.08537","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2502.08537","created_at":"2026-07-05T10:59:49Z"},{"alias_kind":"arxiv_version","alias_value":"2502.08537v1","created_at":"2026-07-05T10:59:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.08537","created_at":"2026-07-05T10:59:49Z"},{"alias_kind":"pith_short_12","alias_value":"RQTWF2MF3OV4","created_at":"2026-07-05T10:59:49Z"},{"alias_kind":"pith_short_16","alias_value":"RQTWF2MF3OV4Y3UX","created_at":"2026-07-05T10:59:49Z"},{"alias_kind":"pith_short_8","alias_value":"RQTWF2MF","created_at":"2026-07-05T10:59:49Z"}],"graph_snapshots":[{"event_id":"sha256:2bd75b4a5411ba67c8716ce5fea20ee1852656f6a2a4214f0e4040883c670e4c","target":"graph","created_at":"2026-07-05T10:59:49Z","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/2502.08537/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Chirality or handedness manifests in all fields of science, ranging from cell biology, molecular interaction, and catalysis to different branches of physics. In condensed matter physics, chirality is intrinsic to enigmatic quantum phases, such as chiral charge density waves and chiral superconductivity. Here, the underlying chiral response is subtle and leads to broken symmetries in the ground state. Detection of subtle broken symmetries is the key to understand these quantum states but they are extremely challenging to expose leading to debate and controversy. Here, using second-order optical","authors_text":"Byunghoon Kim, Guoqing Chang, Jia-Xin Yin, Jinjin Liu, Junyi Zhang, Luis Balicas, Maksim Litskevich, Md Shafayat Hossain, Mohammad Yahyavi, M. Zahid Hasan, Qi Zhang, Sen Shao, Tyler A. Cochran, Xian Yang, Yilin Zhao, Yongkai Li, Yugui Yao, Yu-Xiao Jiang, Zhiwei Wang, Zi-Jia Cheng","cross_cats":["cond-mat.mes-hall","cond-mat.mtrl-sci","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-02-12T16:21:12Z","title":"Broken symmetries associated with a Kagome chiral charge order"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.08537","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:ad4c80702bdd3404e531a0b08fd4ecf6a651ba147cb398673e490cc25c67936a","target":"record","created_at":"2026-07-05T10:59:49Z","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":"a01f306669d7fb3a5f460f7b8d0205f02de1baa328ca6a45cef6b9bbb5317cb7","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-02-12T16:21:12Z","title_canon_sha256":"a878075fb40ef53a511f0618599069ddcea7545d7fd368b2281015bc57fc21d1"},"schema_version":"1.0","source":{"id":"2502.08537","kind":"arxiv","version":1}},"canonical_sha256":"8c2762e985dbabcc6e974f1bb896b890d5761a64bb0810a94c19233cc6b79ab9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8c2762e985dbabcc6e974f1bb896b890d5761a64bb0810a94c19233cc6b79ab9","first_computed_at":"2026-07-05T10:59:49.193827Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:59:49.193827Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"oBEU4O4mwMPYMFPWvtr65oXQHKIPzAJmQFID/Lrlsr+gTfMPDW+tM0f2/mgfd+XHRoakKATiZYZW6aYinWrRAA==","signature_status":"signed_v1","signed_at":"2026-07-05T10:59:49.194312Z","signed_message":"canonical_sha256_bytes"},"source_id":"2502.08537","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ad4c80702bdd3404e531a0b08fd4ecf6a651ba147cb398673e490cc25c67936a","sha256:2bd75b4a5411ba67c8716ce5fea20ee1852656f6a2a4214f0e4040883c670e4c"],"state_sha256":"f23b648962b6c7150a9cd493dc9d82388c04a51bbf05c26765f366b61fa2ab91"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sc+aye5huKxj2CF4vnYFGJrZTu2UTFm0kkRBSeEULDQOH4ZkTbJ7IQqxAEzlUb94rkycNelmLKsHxzizWBhzAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-06T18:42:07.781431Z","bundle_sha256":"1772981470d8268691d1feb787cf712443dc421cb27ce6ae06063546afc94b51"}}