{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:OTH3M3W4D72MCCNCARK2ZX7LSX","short_pith_number":"pith:OTH3M3W4","canonical_record":{"source":{"id":"1410.6398","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-10-23T15:29:52Z","cross_cats_sorted":[],"title_canon_sha256":"7870e92e468a19fefab4b52e6116e6ece43075c75dce4eb392c5f8b73beb0edf","abstract_canon_sha256":"2da3da2e4d0efcc75fb2fc5fd8caad8cc999268d6844a9f7b6bd1dd640acabd2"},"schema_version":"1.0"},"canonical_sha256":"74cfb66edc1ff4c109a20455acdfeb95d6ca94caa296ff11dfd2e84affa185d1","source":{"kind":"arxiv","id":"1410.6398","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.6398","created_at":"2026-05-18T02:17:33Z"},{"alias_kind":"arxiv_version","alias_value":"1410.6398v1","created_at":"2026-05-18T02:17:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.6398","created_at":"2026-05-18T02:17:33Z"},{"alias_kind":"pith_short_12","alias_value":"OTH3M3W4D72M","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_16","alias_value":"OTH3M3W4D72MCCNC","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_8","alias_value":"OTH3M3W4","created_at":"2026-05-18T12:28:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:OTH3M3W4D72MCCNCARK2ZX7LSX","target":"record","payload":{"canonical_record":{"source":{"id":"1410.6398","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-10-23T15:29:52Z","cross_cats_sorted":[],"title_canon_sha256":"7870e92e468a19fefab4b52e6116e6ece43075c75dce4eb392c5f8b73beb0edf","abstract_canon_sha256":"2da3da2e4d0efcc75fb2fc5fd8caad8cc999268d6844a9f7b6bd1dd640acabd2"},"schema_version":"1.0"},"canonical_sha256":"74cfb66edc1ff4c109a20455acdfeb95d6ca94caa296ff11dfd2e84affa185d1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:17:33.543654Z","signature_b64":"AY7bg5fHKiGjl9cDHi0gKW2QtdkCGFU/DHASdqkt4hBaAeS1+NLhqUMsREtkHUPr/huR4iWiI3y6WpX6J0h6AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"74cfb66edc1ff4c109a20455acdfeb95d6ca94caa296ff11dfd2e84affa185d1","last_reissued_at":"2026-05-18T02:17:33.542880Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:17:33.542880Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1410.6398","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":"2026-05-18T02:17:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ybmyR8Q59EF+ispGplBauv1WiSKeU+2qZhKnGIrh977oMwU3/bLFDHrYeKGQ1D3xPOPYtmHsU6vr5zR5iy0KCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T09:07:22.194992Z"},"content_sha256":"c1d6626f0e89f996dd83e0e16409f51c40be951e9f4ef3e99d63a0d0c130ce3d","schema_version":"1.0","event_id":"sha256:c1d6626f0e89f996dd83e0e16409f51c40be951e9f4ef3e99d63a0d0c130ce3d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:OTH3M3W4D72MCCNCARK2ZX7LSX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Chirality density wave of the 'hidden order' phase in URu$_2$Si$_2$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"E. D. Bauer, G. Blumberg, H.-H. Kung, J. A. Mydosh, K. Haule, R. E. Baumbach, V. K. Thorsm{\\o}lle, W.-L. Zhang","submitted_at":"2014-10-23T15:29:52Z","abstract_excerpt":"A second-order phase transition is associated with emergence of an \"order parameter\" and a spontaneous symmetry breaking. For the heavy fermion superconductor URu$_2$Si$_2$, the symmetry of the order parameter associated with its ordered phase below 17.5 K has remained ambiguous despite 30 years of research, and hence is called \"hidden order\" (HO). Here we use polarization resolved Raman spectroscopy to specify the symmetry of the low energy excitations above and below the HO transition. These excitations involve transitions between interacting heavy uranium 5f orbitals, responsible for the br"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.6398","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":""},"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":"2026-05-18T02:17:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"i2jDAMrmhgPpfsMPXgXDC+qaOgtQm6sYyFNoz3nb+Hu5tpaHnFvCmmkRwUVLxefeKcwanYiNBU4l+1eRmHovAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T09:07:22.195786Z"},"content_sha256":"cde649297c6c8afb2bfe166039a3912cae145572c3985b9f5c217d040840db8c","schema_version":"1.0","event_id":"sha256:cde649297c6c8afb2bfe166039a3912cae145572c3985b9f5c217d040840db8c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OTH3M3W4D72MCCNCARK2ZX7LSX/bundle.json","state_url":"https://pith.science/pith/OTH3M3W4D72MCCNCARK2ZX7LSX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OTH3M3W4D72MCCNCARK2ZX7LSX/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":"2026-05-27T09:07:22Z","links":{"resolver":"https://pith.science/pith/OTH3M3W4D72MCCNCARK2ZX7LSX","bundle":"https://pith.science/pith/OTH3M3W4D72MCCNCARK2ZX7LSX/bundle.json","state":"https://pith.science/pith/OTH3M3W4D72MCCNCARK2ZX7LSX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OTH3M3W4D72MCCNCARK2ZX7LSX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:OTH3M3W4D72MCCNCARK2ZX7LSX","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":"2da3da2e4d0efcc75fb2fc5fd8caad8cc999268d6844a9f7b6bd1dd640acabd2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-10-23T15:29:52Z","title_canon_sha256":"7870e92e468a19fefab4b52e6116e6ece43075c75dce4eb392c5f8b73beb0edf"},"schema_version":"1.0","source":{"id":"1410.6398","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.6398","created_at":"2026-05-18T02:17:33Z"},{"alias_kind":"arxiv_version","alias_value":"1410.6398v1","created_at":"2026-05-18T02:17:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.6398","created_at":"2026-05-18T02:17:33Z"},{"alias_kind":"pith_short_12","alias_value":"OTH3M3W4D72M","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_16","alias_value":"OTH3M3W4D72MCCNC","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_8","alias_value":"OTH3M3W4","created_at":"2026-05-18T12:28:43Z"}],"graph_snapshots":[{"event_id":"sha256:cde649297c6c8afb2bfe166039a3912cae145572c3985b9f5c217d040840db8c","target":"graph","created_at":"2026-05-18T02:17:33Z","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":"A second-order phase transition is associated with emergence of an \"order parameter\" and a spontaneous symmetry breaking. For the heavy fermion superconductor URu$_2$Si$_2$, the symmetry of the order parameter associated with its ordered phase below 17.5 K has remained ambiguous despite 30 years of research, and hence is called \"hidden order\" (HO). Here we use polarization resolved Raman spectroscopy to specify the symmetry of the low energy excitations above and below the HO transition. These excitations involve transitions between interacting heavy uranium 5f orbitals, responsible for the br","authors_text":"E. D. Bauer, G. Blumberg, H.-H. Kung, J. A. Mydosh, K. Haule, R. E. Baumbach, V. K. Thorsm{\\o}lle, W.-L. Zhang","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-10-23T15:29:52Z","title":"Chirality density wave of the 'hidden order' phase in URu$_2$Si$_2$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.6398","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:c1d6626f0e89f996dd83e0e16409f51c40be951e9f4ef3e99d63a0d0c130ce3d","target":"record","created_at":"2026-05-18T02:17:33Z","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":"2da3da2e4d0efcc75fb2fc5fd8caad8cc999268d6844a9f7b6bd1dd640acabd2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-10-23T15:29:52Z","title_canon_sha256":"7870e92e468a19fefab4b52e6116e6ece43075c75dce4eb392c5f8b73beb0edf"},"schema_version":"1.0","source":{"id":"1410.6398","kind":"arxiv","version":1}},"canonical_sha256":"74cfb66edc1ff4c109a20455acdfeb95d6ca94caa296ff11dfd2e84affa185d1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"74cfb66edc1ff4c109a20455acdfeb95d6ca94caa296ff11dfd2e84affa185d1","first_computed_at":"2026-05-18T02:17:33.542880Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:17:33.542880Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AY7bg5fHKiGjl9cDHi0gKW2QtdkCGFU/DHASdqkt4hBaAeS1+NLhqUMsREtkHUPr/huR4iWiI3y6WpX6J0h6AA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:17:33.543654Z","signed_message":"canonical_sha256_bytes"},"source_id":"1410.6398","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c1d6626f0e89f996dd83e0e16409f51c40be951e9f4ef3e99d63a0d0c130ce3d","sha256:cde649297c6c8afb2bfe166039a3912cae145572c3985b9f5c217d040840db8c"],"state_sha256":"aec585b42017fa1c0bcc3ad74b456b44156b293c130f60f041d662a4fe429ed7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/H9mFPymPw2r5Bd2psMc9Ksb63ixBbwYiZ96RCQDEJqfT/o9qplIF3KQr0tqB1B6ceTST1v/uW5Y5sTbYZ23DQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T09:07:22.199692Z","bundle_sha256":"7874a586c80608df37d5fe2d593114d7a282e7b5c4ab74efb53cb30687c8705d"}}