{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:4M4VJZZSYG3454RCOYSA67DPKE","short_pith_number":"pith:4M4VJZZS","canonical_record":{"source":{"id":"2608.07242","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-08-07T14:00:12Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.stat-mech","physics.optics"],"title_canon_sha256":"5c76304f03e6f1e0b44b8452ffd42db4c1731044fb7ce116f1926bd95d862636","abstract_canon_sha256":"025b17104efdf6123de95ba628f480a67c282c72848ae31c157b0e8d92bf4a04"},"schema_version":"1.0"},"canonical_sha256":"e33954e732c1b7cef22276240f7c6f51289f1dd729ddd2d282f6f8c813418fbf","source":{"kind":"arxiv","id":"2608.07242","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2608.07242","created_at":"2026-08-10T01:14:44Z"},{"alias_kind":"arxiv_version","alias_value":"2608.07242v1","created_at":"2026-08-10T01:14:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.07242","created_at":"2026-08-10T01:14:44Z"},{"alias_kind":"pith_short_12","alias_value":"4M4VJZZSYG34","created_at":"2026-08-10T01:14:44Z"},{"alias_kind":"pith_short_16","alias_value":"4M4VJZZSYG3454RC","created_at":"2026-08-10T01:14:44Z"},{"alias_kind":"pith_short_8","alias_value":"4M4VJZZS","created_at":"2026-08-10T01:14:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:4M4VJZZSYG3454RCOYSA67DPKE","target":"record","payload":{"canonical_record":{"source":{"id":"2608.07242","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-08-07T14:00:12Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.stat-mech","physics.optics"],"title_canon_sha256":"5c76304f03e6f1e0b44b8452ffd42db4c1731044fb7ce116f1926bd95d862636","abstract_canon_sha256":"025b17104efdf6123de95ba628f480a67c282c72848ae31c157b0e8d92bf4a04"},"schema_version":"1.0"},"canonical_sha256":"e33954e732c1b7cef22276240f7c6f51289f1dd729ddd2d282f6f8c813418fbf","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-10T01:14:44.182628Z","signature_b64":"SZRvnEMxJxSHHfo4DhPYlCH4Rqba3qdV9QuTnqpHOzsirbqbuuFj1e6tdvQu9z0fJZ4Sm+bpK5iIj3yD9IPeAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e33954e732c1b7cef22276240f7c6f51289f1dd729ddd2d282f6f8c813418fbf","last_reissued_at":"2026-08-10T01:14:44.180160Z","signature_status":"signed_v1","first_computed_at":"2026-08-10T01:14:44.180160Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2608.07242","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":"2026-08-10T01:14:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"s3mX8y92BNt2o1JuScLrT6rGKeGDdwEkBXocVAtR45tpVfnCHp27/EtjhEDrq/ZhS7mTuotbAsUSgkzmLxCNBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T10:49:56.501035Z"},"content_sha256":"977c2f8ceb7a14fb1a3feee9d7ebf13c6572bf81dc9194693f9abaa2469f9703","schema_version":"1.0","event_id":"sha256:977c2f8ceb7a14fb1a3feee9d7ebf13c6572bf81dc9194693f9abaa2469f9703"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:4M4VJZZSYG3454RCOYSA67DPKE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Crossing over universal scaling laws in two-dimensional driven dissipative condensates","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.stat-mech","physics.optics"],"primary_cat":"cond-mat.quant-gas","authors_text":"A. Lema\\^{i}tre, A. Minguzzi, D. Pinto Dias, F. Helluin, J. Bloch, L. Canet, M. Escalera, M. Morassi, M. Wouters, Q. Fontaine, S. Ravets","submitted_at":"2026-08-07T14:00:12Z","abstract_excerpt":"In low dimensional systems, fluctuations are enhanced and prevent the spontaneous breaking of continuous symmetries. As a result, spatial and temporal correlation functions decay at large distances and long times. A well established example is given by two-dimensional bosonic condensates at equilibrium, which do not display long-range order of the coherence but algebraic decay belonging to the Berezinski-Kosterlitz-Thouless universality class. In contrast, the universal behaviors of non-equilibrium bosonic condensates are more diverse and many open questions remain. Here, we explore the spatio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.07242","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2608.07242/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":"2026-08-10T01:14:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vBos44/73EoVAX6dR4kRvnvAvnMS2LnP8ApytSO8HMBhwHV7xalNiWBnyb79WKOn5OtF1tERZuKOpz2Fx+uYDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T10:49:56.501873Z"},"content_sha256":"69bec94f4c9419390089095a1d6f9a11344563c856a550b9626b608687f34682","schema_version":"1.0","event_id":"sha256:69bec94f4c9419390089095a1d6f9a11344563c856a550b9626b608687f34682"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4M4VJZZSYG3454RCOYSA67DPKE/bundle.json","state_url":"https://pith.science/pith/4M4VJZZSYG3454RCOYSA67DPKE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4M4VJZZSYG3454RCOYSA67DPKE/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":"2026-08-12T10:49:56Z","links":{"resolver":"https://pith.science/pith/4M4VJZZSYG3454RCOYSA67DPKE","bundle":"https://pith.science/pith/4M4VJZZSYG3454RCOYSA67DPKE/bundle.json","state":"https://pith.science/pith/4M4VJZZSYG3454RCOYSA67DPKE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4M4VJZZSYG3454RCOYSA67DPKE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:4M4VJZZSYG3454RCOYSA67DPKE","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":"025b17104efdf6123de95ba628f480a67c282c72848ae31c157b0e8d92bf4a04","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.stat-mech","physics.optics"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-08-07T14:00:12Z","title_canon_sha256":"5c76304f03e6f1e0b44b8452ffd42db4c1731044fb7ce116f1926bd95d862636"},"schema_version":"1.0","source":{"id":"2608.07242","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2608.07242","created_at":"2026-08-10T01:14:44Z"},{"alias_kind":"arxiv_version","alias_value":"2608.07242v1","created_at":"2026-08-10T01:14:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.07242","created_at":"2026-08-10T01:14:44Z"},{"alias_kind":"pith_short_12","alias_value":"4M4VJZZSYG34","created_at":"2026-08-10T01:14:44Z"},{"alias_kind":"pith_short_16","alias_value":"4M4VJZZSYG3454RC","created_at":"2026-08-10T01:14:44Z"},{"alias_kind":"pith_short_8","alias_value":"4M4VJZZS","created_at":"2026-08-10T01:14:44Z"}],"graph_snapshots":[{"event_id":"sha256:69bec94f4c9419390089095a1d6f9a11344563c856a550b9626b608687f34682","target":"graph","created_at":"2026-08-10T01:14:44Z","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/2608.07242/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In low dimensional systems, fluctuations are enhanced and prevent the spontaneous breaking of continuous symmetries. As a result, spatial and temporal correlation functions decay at large distances and long times. A well established example is given by two-dimensional bosonic condensates at equilibrium, which do not display long-range order of the coherence but algebraic decay belonging to the Berezinski-Kosterlitz-Thouless universality class. In contrast, the universal behaviors of non-equilibrium bosonic condensates are more diverse and many open questions remain. Here, we explore the spatio","authors_text":"A. Lema\\^{i}tre, A. Minguzzi, D. Pinto Dias, F. Helluin, J. Bloch, L. Canet, M. Escalera, M. Morassi, M. Wouters, Q. Fontaine, S. Ravets","cross_cats":["cond-mat.mes-hall","cond-mat.stat-mech","physics.optics"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-08-07T14:00:12Z","title":"Crossing over universal scaling laws in two-dimensional driven dissipative condensates"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.07242","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":"sha256:977c2f8ceb7a14fb1a3feee9d7ebf13c6572bf81dc9194693f9abaa2469f9703","target":"record","created_at":"2026-08-10T01:14:44Z","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":"025b17104efdf6123de95ba628f480a67c282c72848ae31c157b0e8d92bf4a04","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.stat-mech","physics.optics"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-08-07T14:00:12Z","title_canon_sha256":"5c76304f03e6f1e0b44b8452ffd42db4c1731044fb7ce116f1926bd95d862636"},"schema_version":"1.0","source":{"id":"2608.07242","kind":"arxiv","version":1}},"canonical_sha256":"e33954e732c1b7cef22276240f7c6f51289f1dd729ddd2d282f6f8c813418fbf","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e33954e732c1b7cef22276240f7c6f51289f1dd729ddd2d282f6f8c813418fbf","first_computed_at":"2026-08-10T01:14:44.180160Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-08-10T01:14:44.180160Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"SZRvnEMxJxSHHfo4DhPYlCH4Rqba3qdV9QuTnqpHOzsirbqbuuFj1e6tdvQu9z0fJZ4Sm+bpK5iIj3yD9IPeAA==","signature_status":"signed_v1","signed_at":"2026-08-10T01:14:44.182628Z","signed_message":"canonical_sha256_bytes"},"source_id":"2608.07242","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:977c2f8ceb7a14fb1a3feee9d7ebf13c6572bf81dc9194693f9abaa2469f9703","sha256:69bec94f4c9419390089095a1d6f9a11344563c856a550b9626b608687f34682"],"state_sha256":"9ac3c2c381589eed94c9c5127fc7e582d1920564d84110f86d29e6978e5bd1c6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3Gxkia34mMIhabuBNoKW2bjeXanw8UUpua9ntadhphph1lT3EVtWqEErEjyRvJDfD+Sm2CQR414KuHLKC87JAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-12T10:49:56.506212Z","bundle_sha256":"35972238a6e1295fcf1356fe07973a3538bdb10350a4b70fadb1ad4f6e333569"}}