{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:SGFIW2GDL6TH3OTHV4IJDYMQJK","short_pith_number":"pith:SGFIW2GD","canonical_record":{"source":{"id":"2406.18649","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-06-26T18:00:02Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"99522088766355f2f6431b11df34185bd7f2df0ebe0f8a08ba07c1994152c851","abstract_canon_sha256":"70fd11295592c4c04c3be5e378f5d50160f45d8d6a7a510473baf0f368bd4574"},"schema_version":"1.0"},"canonical_sha256":"918a8b68c35fa67dba67af1091e1904aadcf1f88557784c6dd4e90caf8dd892b","source":{"kind":"arxiv","id":"2406.18649","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2406.18649","created_at":"2026-07-05T09:38:27Z"},{"alias_kind":"arxiv_version","alias_value":"2406.18649v2","created_at":"2026-07-05T09:38:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.18649","created_at":"2026-07-05T09:38:27Z"},{"alias_kind":"pith_short_12","alias_value":"SGFIW2GDL6TH","created_at":"2026-07-05T09:38:27Z"},{"alias_kind":"pith_short_16","alias_value":"SGFIW2GDL6TH3OTH","created_at":"2026-07-05T09:38:27Z"},{"alias_kind":"pith_short_8","alias_value":"SGFIW2GD","created_at":"2026-07-05T09:38:27Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:SGFIW2GDL6TH3OTHV4IJDYMQJK","target":"record","payload":{"canonical_record":{"source":{"id":"2406.18649","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-06-26T18:00:02Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"99522088766355f2f6431b11df34185bd7f2df0ebe0f8a08ba07c1994152c851","abstract_canon_sha256":"70fd11295592c4c04c3be5e378f5d50160f45d8d6a7a510473baf0f368bd4574"},"schema_version":"1.0"},"canonical_sha256":"918a8b68c35fa67dba67af1091e1904aadcf1f88557784c6dd4e90caf8dd892b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:38:27.589923Z","signature_b64":"zlQWGif/fxX5i+K94AUgmxzK62R3wruxLqYdzto2uJgH/QhVnbReQKLCZRdgCQLC/cIWMo9yFpUx6XxPMJWvBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"918a8b68c35fa67dba67af1091e1904aadcf1f88557784c6dd4e90caf8dd892b","last_reissued_at":"2026-07-05T09:38:27.589489Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:38:27.589489Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2406.18649","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":"2026-07-05T09:38:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1Fee+TsjPLiVU0ncjRE198/MdLw32DNZzxpOqbL1Ox4FnEjK/+oMh799SA9NKSLKVxU/YZCF7RaDV0dMj5YxCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T04:45:50.064307Z"},"content_sha256":"7c7b34a5a026b9fb0e00e1a5660cc194898300d568959591661deac419c82da5","schema_version":"1.0","event_id":"sha256:7c7b34a5a026b9fb0e00e1a5660cc194898300d568959591661deac419c82da5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:SGFIW2GDL6TH3OTHV4IJDYMQJK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"[111]-strained spin ice: Localization of thermodynamically deconfined monopoles","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"Chris R. Laumann, Jonathan N. Hall\\'en, Robin Sch\\\"afer, Zhongling Lu","submitted_at":"2024-06-26T18:00:02Z","abstract_excerpt":"We study classical spin ice under uniaxial strain along the $[111]$ crystallographic axis. Remarkably, such strain preserves the extensive ice degeneracy and the corresponding classical Coulomb phase. The emergent monopole excitations remain thermodynamically deconfined exactly as in the isotropic case. However, their motion under local heat bath dynamics depends qualitatively on the sign of the strain. In the low-temperature limit for negative strain, the monopoles diffuse, while for positive strain, they localize. Introducing additional ring exchange dynamics into the ice background transfor"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.18649","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2406.18649/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":"2026-07-05T09:38:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VEb50GK7fB+4Qr/a1ftarMLWAvCJOWqtxTdOjIL7iZlpf+5g0fRpu5O5ZoBKekbyEt62eQp9iF/o4RPYVflpBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T04:45:50.064905Z"},"content_sha256":"47be13344099e349befc744e5b65acf47868ecafd49df9f7b75e970c66facc1f","schema_version":"1.0","event_id":"sha256:47be13344099e349befc744e5b65acf47868ecafd49df9f7b75e970c66facc1f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SGFIW2GDL6TH3OTHV4IJDYMQJK/bundle.json","state_url":"https://pith.science/pith/SGFIW2GDL6TH3OTHV4IJDYMQJK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SGFIW2GDL6TH3OTHV4IJDYMQJK/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":"2026-08-13T04:45:50Z","links":{"resolver":"https://pith.science/pith/SGFIW2GDL6TH3OTHV4IJDYMQJK","bundle":"https://pith.science/pith/SGFIW2GDL6TH3OTHV4IJDYMQJK/bundle.json","state":"https://pith.science/pith/SGFIW2GDL6TH3OTHV4IJDYMQJK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SGFIW2GDL6TH3OTHV4IJDYMQJK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:SGFIW2GDL6TH3OTHV4IJDYMQJK","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":"70fd11295592c4c04c3be5e378f5d50160f45d8d6a7a510473baf0f368bd4574","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-06-26T18:00:02Z","title_canon_sha256":"99522088766355f2f6431b11df34185bd7f2df0ebe0f8a08ba07c1994152c851"},"schema_version":"1.0","source":{"id":"2406.18649","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2406.18649","created_at":"2026-07-05T09:38:27Z"},{"alias_kind":"arxiv_version","alias_value":"2406.18649v2","created_at":"2026-07-05T09:38:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.18649","created_at":"2026-07-05T09:38:27Z"},{"alias_kind":"pith_short_12","alias_value":"SGFIW2GDL6TH","created_at":"2026-07-05T09:38:27Z"},{"alias_kind":"pith_short_16","alias_value":"SGFIW2GDL6TH3OTH","created_at":"2026-07-05T09:38:27Z"},{"alias_kind":"pith_short_8","alias_value":"SGFIW2GD","created_at":"2026-07-05T09:38:27Z"}],"graph_snapshots":[{"event_id":"sha256:47be13344099e349befc744e5b65acf47868ecafd49df9f7b75e970c66facc1f","target":"graph","created_at":"2026-07-05T09:38:27Z","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/2406.18649/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study classical spin ice under uniaxial strain along the $[111]$ crystallographic axis. Remarkably, such strain preserves the extensive ice degeneracy and the corresponding classical Coulomb phase. The emergent monopole excitations remain thermodynamically deconfined exactly as in the isotropic case. However, their motion under local heat bath dynamics depends qualitatively on the sign of the strain. In the low-temperature limit for negative strain, the monopoles diffuse, while for positive strain, they localize. Introducing additional ring exchange dynamics into the ice background transfor","authors_text":"Chris R. Laumann, Jonathan N. Hall\\'en, Robin Sch\\\"afer, Zhongling Lu","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-06-26T18:00:02Z","title":"[111]-strained spin ice: Localization of thermodynamically deconfined monopoles"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.18649","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":"sha256:7c7b34a5a026b9fb0e00e1a5660cc194898300d568959591661deac419c82da5","target":"record","created_at":"2026-07-05T09:38:27Z","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":"70fd11295592c4c04c3be5e378f5d50160f45d8d6a7a510473baf0f368bd4574","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-06-26T18:00:02Z","title_canon_sha256":"99522088766355f2f6431b11df34185bd7f2df0ebe0f8a08ba07c1994152c851"},"schema_version":"1.0","source":{"id":"2406.18649","kind":"arxiv","version":2}},"canonical_sha256":"918a8b68c35fa67dba67af1091e1904aadcf1f88557784c6dd4e90caf8dd892b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"918a8b68c35fa67dba67af1091e1904aadcf1f88557784c6dd4e90caf8dd892b","first_computed_at":"2026-07-05T09:38:27.589489Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:38:27.589489Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"zlQWGif/fxX5i+K94AUgmxzK62R3wruxLqYdzto2uJgH/QhVnbReQKLCZRdgCQLC/cIWMo9yFpUx6XxPMJWvBw==","signature_status":"signed_v1","signed_at":"2026-07-05T09:38:27.589923Z","signed_message":"canonical_sha256_bytes"},"source_id":"2406.18649","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7c7b34a5a026b9fb0e00e1a5660cc194898300d568959591661deac419c82da5","sha256:47be13344099e349befc744e5b65acf47868ecafd49df9f7b75e970c66facc1f"],"state_sha256":"f88f2e126e3660b1de0706c3de1cd1f66689033bd8bdada127dfd26dd8f40df4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jOKcija9Vsw3yjmu45Vi+WX/EFCLy+WLy8q8w+v8VmMk7u2w5lpAeHaRqUJbJkjT3B49nfh2fY3hLu4WO/DbBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-13T04:45:50.069125Z","bundle_sha256":"66a3da2d3ef71b1c34e854a2736d062b5254d3e3f303c9ae5666731564a19277"}}