{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:AJG73O72IN2BFN6DCHLCID4JZW","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":"777a780b24fa657366095e955852eaedc9365ef04368c7ec94be53a3b5a4f3fc","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-05-22T08:30:46Z","title_canon_sha256":"0adc40819b01355bcdce3957d0f32ff1615d102f2b8282b17cc6b5624dc39ef5"},"schema_version":"1.0","source":{"id":"2505.16378","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2505.16378","created_at":"2026-07-23T01:24:15Z"},{"alias_kind":"arxiv_version","alias_value":"2505.16378v3","created_at":"2026-07-23T01:24:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.16378","created_at":"2026-07-23T01:24:15Z"},{"alias_kind":"pith_short_12","alias_value":"AJG73O72IN2B","created_at":"2026-07-23T01:24:15Z"},{"alias_kind":"pith_short_16","alias_value":"AJG73O72IN2BFN6D","created_at":"2026-07-23T01:24:15Z"},{"alias_kind":"pith_short_8","alias_value":"AJG73O72","created_at":"2026-07-23T01:24:15Z"}],"graph_snapshots":[{"event_id":"sha256:930d5a6a1e3427a089cbcbfaef36fe2c2f3196f208d0be394d1fbe56207e3035","target":"graph","created_at":"2026-07-23T01:24:15Z","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/2505.16378/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Interacting many-particle systems can self-organize into a rich variety of crystalline structures. While symmetry provides a powerful framework for predicting whether transitions between crystal states are continuous or discontinuous, collective lattice dynamics offer complementary insights into the microscopic mechanisms that drive these transitions. Trapped laser-cooled ions present a pristine and highly controllable few-body system for studying this interplay of symmetry and dynamics. Here, we use real-time fluorescence imaging while deforming the trap potential to observe a variety of stru","authors_text":"Akhil Ayyadevara, Anand Prakash, Arun Paramekanti, S. A. Rangwala, Shovan Dutta","cross_cats":["cond-mat.mes-hall","cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-05-22T08:30:46Z","title":"Observing the dynamics of octupolar structural transitions in trapped-ion clusters"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.16378","kind":"arxiv","version":3},"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:eadb53fca94751bba68a09bb1ae71c8c4ef24a3d58be67ab641eb95edc53cc8b","target":"record","created_at":"2026-07-23T01:24:15Z","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":"777a780b24fa657366095e955852eaedc9365ef04368c7ec94be53a3b5a4f3fc","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-05-22T08:30:46Z","title_canon_sha256":"0adc40819b01355bcdce3957d0f32ff1615d102f2b8282b17cc6b5624dc39ef5"},"schema_version":"1.0","source":{"id":"2505.16378","kind":"arxiv","version":3}},"canonical_sha256":"024dfdbbfa437412b7c311d6240f89cd9675967dd4392ba60ffe0453c55027d7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"024dfdbbfa437412b7c311d6240f89cd9675967dd4392ba60ffe0453c55027d7","first_computed_at":"2026-07-23T01:24:15.485200Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-23T01:24:15.485200Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"VbWCOiu9IM+lx2MmN4PtuecdmYIW21VXvn41WJXZlXnunT92U7hL+pzSAXPncJ/GjUXyTqks8OGNpp7iJ44BAQ==","signature_status":"signed_v1","signed_at":"2026-07-23T01:24:15.486387Z","signed_message":"canonical_sha256_bytes"},"source_id":"2505.16378","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:eadb53fca94751bba68a09bb1ae71c8c4ef24a3d58be67ab641eb95edc53cc8b","sha256:930d5a6a1e3427a089cbcbfaef36fe2c2f3196f208d0be394d1fbe56207e3035"],"state_sha256":"928d36afe6ef79d48b0c76e75332e5e6fe2ea8dbfb9ae9e71ceae4c8c0302d77"}