{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:HR4GI5ZJQJOS3ZLPHAA7ER44KF","short_pith_number":"pith:HR4GI5ZJ","canonical_record":{"source":{"id":"1406.2617","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-06-10T16:24:49Z","cross_cats_sorted":[],"title_canon_sha256":"327f347b5492e3791b4df9d595882c0de8f562c7036d51137c98c022b267a51c","abstract_canon_sha256":"a1b22f45d0f1822af2a2b5f9a6093ea7e159f5855d0399fb4a7ef6436fc65f93"},"schema_version":"1.0"},"canonical_sha256":"3c78647729825d2de56f3801f2479c515b9135c362a933f4244c659b368156f5","source":{"kind":"arxiv","id":"1406.2617","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1406.2617","created_at":"2026-05-18T02:50:01Z"},{"alias_kind":"arxiv_version","alias_value":"1406.2617v1","created_at":"2026-05-18T02:50:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.2617","created_at":"2026-05-18T02:50:01Z"},{"alias_kind":"pith_short_12","alias_value":"HR4GI5ZJQJOS","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_16","alias_value":"HR4GI5ZJQJOS3ZLP","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_8","alias_value":"HR4GI5ZJ","created_at":"2026-05-18T12:28:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:HR4GI5ZJQJOS3ZLPHAA7ER44KF","target":"record","payload":{"canonical_record":{"source":{"id":"1406.2617","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-06-10T16:24:49Z","cross_cats_sorted":[],"title_canon_sha256":"327f347b5492e3791b4df9d595882c0de8f562c7036d51137c98c022b267a51c","abstract_canon_sha256":"a1b22f45d0f1822af2a2b5f9a6093ea7e159f5855d0399fb4a7ef6436fc65f93"},"schema_version":"1.0"},"canonical_sha256":"3c78647729825d2de56f3801f2479c515b9135c362a933f4244c659b368156f5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:50:01.332556Z","signature_b64":"h0PFqDNcVpU2M3N4a6kAX3Vf8DR0R7HSHyA5RM53XdzM0Tg9GzXEsrbg3VvvN3tH9Z+Pxaxwpvwsm3VCNcjkCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3c78647729825d2de56f3801f2479c515b9135c362a933f4244c659b368156f5","last_reissued_at":"2026-05-18T02:50:01.331967Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:50:01.331967Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1406.2617","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":"2026-05-18T02:50:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YpdV3OuD0kz1WDZ5AXoo8jaTKGpuOClN9CaJmU+RZiuTAZoLO8BXOKI+ljVgBeXOO1GsinUUMXcvoKzXUBhiAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T14:29:29.810348Z"},"content_sha256":"ff24383887a7607234f6e5d848bff957b6d831694cb37539203d8da186475106","schema_version":"1.0","event_id":"sha256:ff24383887a7607234f6e5d848bff957b6d831694cb37539203d8da186475106"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:HR4GI5ZJQJOS3ZLPHAA7ER44KF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Spontaneous chiral symmetry breaking on a fully polarized frustrated magnet at finite temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Hiroaki T. Ueda","submitted_at":"2014-06-10T16:24:49Z","abstract_excerpt":"Frustration can introduce more-than-two minima in a spin dispersion relation even in a fully polarized magnet under high magnetic field. We generally discuss, on the fully polarized phase, the possibility of the chiral symmetry breaking where the number of magnons pumped by finite temperature deviates to one side of minima. We study this phase by constructing the Ginzburg-Landau energy which is controlled by the external magnetic field and interactions between magnons near the dispersion minima. This chirality breaking phase accompanies, not a magnetization perpendicular to the external field,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.2617","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":"2026-05-18T02:50:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"swApjFdxYRc9GLYlsiSqVUhpIjd3xV9bhOcMaWg3dTxv3ZLv8bJBEc9RYsgdcfsxI1aXV2kODhvaC3TMzKDXDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T14:29:29.810696Z"},"content_sha256":"34cc482d3ec318fb703880a672235e29a1fbcd943c717d5bb60564952c6f61da","schema_version":"1.0","event_id":"sha256:34cc482d3ec318fb703880a672235e29a1fbcd943c717d5bb60564952c6f61da"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HR4GI5ZJQJOS3ZLPHAA7ER44KF/bundle.json","state_url":"https://pith.science/pith/HR4GI5ZJQJOS3ZLPHAA7ER44KF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HR4GI5ZJQJOS3ZLPHAA7ER44KF/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":"2026-06-03T14:29:29Z","links":{"resolver":"https://pith.science/pith/HR4GI5ZJQJOS3ZLPHAA7ER44KF","bundle":"https://pith.science/pith/HR4GI5ZJQJOS3ZLPHAA7ER44KF/bundle.json","state":"https://pith.science/pith/HR4GI5ZJQJOS3ZLPHAA7ER44KF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HR4GI5ZJQJOS3ZLPHAA7ER44KF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:HR4GI5ZJQJOS3ZLPHAA7ER44KF","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":"a1b22f45d0f1822af2a2b5f9a6093ea7e159f5855d0399fb4a7ef6436fc65f93","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-06-10T16:24:49Z","title_canon_sha256":"327f347b5492e3791b4df9d595882c0de8f562c7036d51137c98c022b267a51c"},"schema_version":"1.0","source":{"id":"1406.2617","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1406.2617","created_at":"2026-05-18T02:50:01Z"},{"alias_kind":"arxiv_version","alias_value":"1406.2617v1","created_at":"2026-05-18T02:50:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.2617","created_at":"2026-05-18T02:50:01Z"},{"alias_kind":"pith_short_12","alias_value":"HR4GI5ZJQJOS","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_16","alias_value":"HR4GI5ZJQJOS3ZLP","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_8","alias_value":"HR4GI5ZJ","created_at":"2026-05-18T12:28:30Z"}],"graph_snapshots":[{"event_id":"sha256:34cc482d3ec318fb703880a672235e29a1fbcd943c717d5bb60564952c6f61da","target":"graph","created_at":"2026-05-18T02:50:01Z","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":"Frustration can introduce more-than-two minima in a spin dispersion relation even in a fully polarized magnet under high magnetic field. We generally discuss, on the fully polarized phase, the possibility of the chiral symmetry breaking where the number of magnons pumped by finite temperature deviates to one side of minima. We study this phase by constructing the Ginzburg-Landau energy which is controlled by the external magnetic field and interactions between magnons near the dispersion minima. This chirality breaking phase accompanies, not a magnetization perpendicular to the external field,","authors_text":"Hiroaki T. Ueda","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-06-10T16:24:49Z","title":"Spontaneous chiral symmetry breaking on a fully polarized frustrated magnet at finite temperature"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.2617","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:ff24383887a7607234f6e5d848bff957b6d831694cb37539203d8da186475106","target":"record","created_at":"2026-05-18T02:50:01Z","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":"a1b22f45d0f1822af2a2b5f9a6093ea7e159f5855d0399fb4a7ef6436fc65f93","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-06-10T16:24:49Z","title_canon_sha256":"327f347b5492e3791b4df9d595882c0de8f562c7036d51137c98c022b267a51c"},"schema_version":"1.0","source":{"id":"1406.2617","kind":"arxiv","version":1}},"canonical_sha256":"3c78647729825d2de56f3801f2479c515b9135c362a933f4244c659b368156f5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3c78647729825d2de56f3801f2479c515b9135c362a933f4244c659b368156f5","first_computed_at":"2026-05-18T02:50:01.331967Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:50:01.331967Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"h0PFqDNcVpU2M3N4a6kAX3Vf8DR0R7HSHyA5RM53XdzM0Tg9GzXEsrbg3VvvN3tH9Z+Pxaxwpvwsm3VCNcjkCA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:50:01.332556Z","signed_message":"canonical_sha256_bytes"},"source_id":"1406.2617","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ff24383887a7607234f6e5d848bff957b6d831694cb37539203d8da186475106","sha256:34cc482d3ec318fb703880a672235e29a1fbcd943c717d5bb60564952c6f61da"],"state_sha256":"9c8330dbfdf74a6ab9cea967497a586d92f72553c4b03e892bec29be0c24be33"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VurfEWb+hza8NR6CVBwuRKwI0DRYAeOJCcGwzWLZiWhZm825uikE35lv90FBw4J19fYu1K7zgSzS476HHMJZDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T14:29:29.812606Z","bundle_sha256":"e88589413fe395e247e31bd014092812a06f8820410680822d810b2ab981d44d"}}