{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:6A6C5PGKBYKICKNZJHLRFWA4JX","short_pith_number":"pith:6A6C5PGK","canonical_record":{"source":{"id":"1511.06515","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-11-20T08:01:55Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"47a43f05c249514c00c9d89325d518355799310994c71f00544496a514be3744","abstract_canon_sha256":"04ef804efcab7c4445355c77c99247c270d865f7a2cf1faeca33d70871c6c3b0"},"schema_version":"1.0"},"canonical_sha256":"f03c2ebcca0e148129b949d712d81c4ddca26cbff09a03c0bf981010e47fcc9f","source":{"kind":"arxiv","id":"1511.06515","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1511.06515","created_at":"2026-05-18T01:18:14Z"},{"alias_kind":"arxiv_version","alias_value":"1511.06515v2","created_at":"2026-05-18T01:18:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.06515","created_at":"2026-05-18T01:18:14Z"},{"alias_kind":"pith_short_12","alias_value":"6A6C5PGKBYKI","created_at":"2026-05-18T12:29:07Z"},{"alias_kind":"pith_short_16","alias_value":"6A6C5PGKBYKICKNZ","created_at":"2026-05-18T12:29:07Z"},{"alias_kind":"pith_short_8","alias_value":"6A6C5PGK","created_at":"2026-05-18T12:29:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:6A6C5PGKBYKICKNZJHLRFWA4JX","target":"record","payload":{"canonical_record":{"source":{"id":"1511.06515","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-11-20T08:01:55Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"47a43f05c249514c00c9d89325d518355799310994c71f00544496a514be3744","abstract_canon_sha256":"04ef804efcab7c4445355c77c99247c270d865f7a2cf1faeca33d70871c6c3b0"},"schema_version":"1.0"},"canonical_sha256":"f03c2ebcca0e148129b949d712d81c4ddca26cbff09a03c0bf981010e47fcc9f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:18:14.088857Z","signature_b64":"hU2AQ7bDk+nUWslPWGvP3CBN1cgX7kCZDLRhmCW7hHAw1usKZjLb2ShgNlNm/R+Lji9lLieJCpjV5RZNto4FBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f03c2ebcca0e148129b949d712d81c4ddca26cbff09a03c0bf981010e47fcc9f","last_reissued_at":"2026-05-18T01:18:14.088217Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:18:14.088217Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1511.06515","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":"2026-05-18T01:18:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"of0nAF4h3sxyflsA2/esU8yVsqmHR1yVK7vPOXDkPzo88zAftCso5x0VBvibplxEm6nBdavRO9d+nyugnhqlDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T22:08:28.307645Z"},"content_sha256":"de97a7928e4a3d10bf36b6c936599e61becc75141a3d58f59ee9d9eed28f51ca","schema_version":"1.0","event_id":"sha256:de97a7928e4a3d10bf36b6c936599e61becc75141a3d58f59ee9d9eed28f51ca"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:6A6C5PGKBYKICKNZJHLRFWA4JX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum solitons with emergent interactions in a model of cold atoms on the triangular lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"Hiroaki T. Ueda, Nic Shannon, Yutaka Akagi","submitted_at":"2015-11-20T08:01:55Z","abstract_excerpt":"Cold atoms bring new opportunities to study quantum magnetism, and in particular, to simulate quantum magnets with symmetry greater than $SU(2)$. Here we explore the topological excitations which arise in a model of cold atoms on the triangular lattice with $SU(3)$ symmetry. Using a combination of homotopy analysis and analytic field-theory we identify a new family of solitonic wave functions characterised by integer charge ${\\bf Q} = (Q_A, Q_B, Q_C)$, with $Q_A + Q_B + Q_C = 0$. We use a numerical approach, based on a variational wave function, to explore the stability of these solitons on a "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.06515","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":"2026-05-18T01:18:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cdV5s2XvdtdhmKBSxnpLGpRTn6p4c/bG2S8dxx0aCS4hJZbZafdQrN5YmW7yB4BOxZRkPo7SsNcb+VZh5uJFAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T22:08:28.307985Z"},"content_sha256":"f1b782a3cea7aaac1f46b0fda2d8efe764383f5e8a23cdffbaa5fb9c3517bc52","schema_version":"1.0","event_id":"sha256:f1b782a3cea7aaac1f46b0fda2d8efe764383f5e8a23cdffbaa5fb9c3517bc52"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6A6C5PGKBYKICKNZJHLRFWA4JX/bundle.json","state_url":"https://pith.science/pith/6A6C5PGKBYKICKNZJHLRFWA4JX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6A6C5PGKBYKICKNZJHLRFWA4JX/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":"2026-06-03T22:08:28Z","links":{"resolver":"https://pith.science/pith/6A6C5PGKBYKICKNZJHLRFWA4JX","bundle":"https://pith.science/pith/6A6C5PGKBYKICKNZJHLRFWA4JX/bundle.json","state":"https://pith.science/pith/6A6C5PGKBYKICKNZJHLRFWA4JX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6A6C5PGKBYKICKNZJHLRFWA4JX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:6A6C5PGKBYKICKNZJHLRFWA4JX","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":"04ef804efcab7c4445355c77c99247c270d865f7a2cf1faeca33d70871c6c3b0","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-11-20T08:01:55Z","title_canon_sha256":"47a43f05c249514c00c9d89325d518355799310994c71f00544496a514be3744"},"schema_version":"1.0","source":{"id":"1511.06515","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1511.06515","created_at":"2026-05-18T01:18:14Z"},{"alias_kind":"arxiv_version","alias_value":"1511.06515v2","created_at":"2026-05-18T01:18:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.06515","created_at":"2026-05-18T01:18:14Z"},{"alias_kind":"pith_short_12","alias_value":"6A6C5PGKBYKI","created_at":"2026-05-18T12:29:07Z"},{"alias_kind":"pith_short_16","alias_value":"6A6C5PGKBYKICKNZ","created_at":"2026-05-18T12:29:07Z"},{"alias_kind":"pith_short_8","alias_value":"6A6C5PGK","created_at":"2026-05-18T12:29:07Z"}],"graph_snapshots":[{"event_id":"sha256:f1b782a3cea7aaac1f46b0fda2d8efe764383f5e8a23cdffbaa5fb9c3517bc52","target":"graph","created_at":"2026-05-18T01:18:14Z","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":"Cold atoms bring new opportunities to study quantum magnetism, and in particular, to simulate quantum magnets with symmetry greater than $SU(2)$. Here we explore the topological excitations which arise in a model of cold atoms on the triangular lattice with $SU(3)$ symmetry. Using a combination of homotopy analysis and analytic field-theory we identify a new family of solitonic wave functions characterised by integer charge ${\\bf Q} = (Q_A, Q_B, Q_C)$, with $Q_A + Q_B + Q_C = 0$. We use a numerical approach, based on a variational wave function, to explore the stability of these solitons on a ","authors_text":"Hiroaki T. Ueda, Nic Shannon, Yutaka Akagi","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-11-20T08:01:55Z","title":"Quantum solitons with emergent interactions in a model of cold atoms on the triangular lattice"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.06515","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:de97a7928e4a3d10bf36b6c936599e61becc75141a3d58f59ee9d9eed28f51ca","target":"record","created_at":"2026-05-18T01:18:14Z","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":"04ef804efcab7c4445355c77c99247c270d865f7a2cf1faeca33d70871c6c3b0","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-11-20T08:01:55Z","title_canon_sha256":"47a43f05c249514c00c9d89325d518355799310994c71f00544496a514be3744"},"schema_version":"1.0","source":{"id":"1511.06515","kind":"arxiv","version":2}},"canonical_sha256":"f03c2ebcca0e148129b949d712d81c4ddca26cbff09a03c0bf981010e47fcc9f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f03c2ebcca0e148129b949d712d81c4ddca26cbff09a03c0bf981010e47fcc9f","first_computed_at":"2026-05-18T01:18:14.088217Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:18:14.088217Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hU2AQ7bDk+nUWslPWGvP3CBN1cgX7kCZDLRhmCW7hHAw1usKZjLb2ShgNlNm/R+Lji9lLieJCpjV5RZNto4FBw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:18:14.088857Z","signed_message":"canonical_sha256_bytes"},"source_id":"1511.06515","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:de97a7928e4a3d10bf36b6c936599e61becc75141a3d58f59ee9d9eed28f51ca","sha256:f1b782a3cea7aaac1f46b0fda2d8efe764383f5e8a23cdffbaa5fb9c3517bc52"],"state_sha256":"64cdbd27fe4ea19fff2f737741f7a223842771aa8c9dbea8fca69115146e080c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UYo1cczK1t7UwDSqjOQGTCneiztuGcw13t7gY/y6OFq/mPIL8XqYI6nT66GmPx9988193AMuR4ob+RCmlx0TDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T22:08:28.309941Z","bundle_sha256":"5dc951eda465efe0d4b91f85b137814243464bcd86d3000489937ecddb96dee9"}}