{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:JWDOBM6DJHGDYZ2V2XGM7RIMBU","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":"a9a818af14be0cba1f6a09cf3889d41e40986830775bae6fde4b786c62be42a0","cross_cats_sorted":["cond-mat.stat-mech","physics.atom-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2021-04-22T16:29:56Z","title_canon_sha256":"35b2645b7c5f552b93daf6ef0fea4a2cf2033097190a431f4dbdde3c37ef95bb"},"schema_version":"1.0","source":{"id":"2104.11160","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2104.11160","created_at":"2026-07-05T04:42:30Z"},{"alias_kind":"arxiv_version","alias_value":"2104.11160v3","created_at":"2026-07-05T04:42:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2104.11160","created_at":"2026-07-05T04:42:30Z"},{"alias_kind":"pith_short_12","alias_value":"JWDOBM6DJHGD","created_at":"2026-07-05T04:42:30Z"},{"alias_kind":"pith_short_16","alias_value":"JWDOBM6DJHGDYZ2V","created_at":"2026-07-05T04:42:30Z"},{"alias_kind":"pith_short_8","alias_value":"JWDOBM6D","created_at":"2026-07-05T04:42:30Z"}],"graph_snapshots":[{"event_id":"sha256:d090f88bad4f42ede17524eff3f5d706c3aa6c4b909e8cd5a35619ce142c7d60","target":"graph","created_at":"2026-07-05T04:42:30Z","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/2104.11160/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study the dynamics of a one-dimensional Rydberg lattice gas under facilitation (anti-blockade) conditions which implements a so-called kinetically constrained spin system. Here an atom can only be excited to a Rydberg state when one of its neighbors is already excited. Once two or more atoms are simultaneously excited mechanical forces emerge, which couple the internal electronic dynamics of this many-body system to external vibrational degrees of freedom in the lattice. This electron-phonon coupling results in a so-called phonon dressing of many-body states which in turn impacts on the fac","authors_text":"Igor Lesanovsky, Matteo Magoni, Paolo P. Mazza","cross_cats":["cond-mat.stat-mech","physics.atom-ph","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2021-04-22T16:29:56Z","title":"Phonon dressing of a facilitated one-dimensional Rydberg lattice gas"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2104.11160","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":"sha256:1c88817fea019545d4e842ffabc699464d1cb98d3d2533b02a3846d1249ae86a","target":"record","created_at":"2026-07-05T04:42:30Z","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":"a9a818af14be0cba1f6a09cf3889d41e40986830775bae6fde4b786c62be42a0","cross_cats_sorted":["cond-mat.stat-mech","physics.atom-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2021-04-22T16:29:56Z","title_canon_sha256":"35b2645b7c5f552b93daf6ef0fea4a2cf2033097190a431f4dbdde3c37ef95bb"},"schema_version":"1.0","source":{"id":"2104.11160","kind":"arxiv","version":3}},"canonical_sha256":"4d86e0b3c349cc3c6755d5cccfc50c0d2e176dcdb5b1ee552321a4f91feefa1d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4d86e0b3c349cc3c6755d5cccfc50c0d2e176dcdb5b1ee552321a4f91feefa1d","first_computed_at":"2026-07-05T04:42:30.569484Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:42:30.569484Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nszTJgYS38V/ehcFLOIggJNZcwV8G060RV/Cd/ojZXXAY7aQmEvcQmjX6+QOqbiE7ybjZQ/9/grm0DnUnefiAA==","signature_status":"signed_v1","signed_at":"2026-07-05T04:42:30.570042Z","signed_message":"canonical_sha256_bytes"},"source_id":"2104.11160","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1c88817fea019545d4e842ffabc699464d1cb98d3d2533b02a3846d1249ae86a","sha256:d090f88bad4f42ede17524eff3f5d706c3aa6c4b909e8cd5a35619ce142c7d60"],"state_sha256":"3341c55cc906ef61a1aafe3164c0e5af76d6c3c76545addbef33032ae57c0ab5"}