{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:JUHYEKG42FUA4THRDFSEFOSH22","short_pith_number":"pith:JUHYEKG4","schema_version":"1.0","canonical_sha256":"4d0f8228dcd1680e4cf1196442ba47d6a2dfb8338bbf58300a8166c38bd160f0","source":{"kind":"arxiv","id":"2411.05582","version":2},"attestation_state":"computed","paper":{"title":"Condensation and prescaling in spatial Polyakov loop correlations far from equilibrium","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Daniel Spitz, Kirill Boguslavski, Thimo Preis","submitted_at":"2024-11-08T14:10:38Z","abstract_excerpt":"The far-from-equilibrium dynamics of spatial Polyakov loop correlations, which provide gauge-invariant observables akin to effective particle numbers for gluon plasmas, are investigated within real-time $\\mathrm{SU}(N_c)$ lattice gauge theory at weak couplings and large gluon occupations. The momentum zero mode of these correlations reveals the dynamic formation of a condensate, while at nonzero momenta, energy is transported toward the ultraviolet. We demonstrate that the non-zero momentum dynamics is well described by a direct cascade in terms of gauge-invariant Polyakov loop excitations, ex"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2411.05582","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-11-08T14:10:38Z","cross_cats_sorted":["cond-mat.quant-gas","hep-lat","nucl-th"],"title_canon_sha256":"fb93a1535f2bc962d7c3fba385ba70fb8ed7b469733f84ee187cbd86cde5fc53","abstract_canon_sha256":"558bf231c01312e331e4bf007774d00f9df5cb547ca78db11ad3e8c96e787c45"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:08:12.852503Z","signature_b64":"/+AQwtr40KsdqswylbhU8lm7vpDJWP0DusbocoqS4Xjxkt95wEmav+7OXYs1cU1p3nxSnDdhYYpZpZD1aC0nBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4d0f8228dcd1680e4cf1196442ba47d6a2dfb8338bbf58300a8166c38bd160f0","last_reissued_at":"2026-07-05T11:08:12.851942Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:08:12.851942Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Condensation and prescaling in spatial Polyakov loop correlations far from equilibrium","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Daniel Spitz, Kirill Boguslavski, Thimo Preis","submitted_at":"2024-11-08T14:10:38Z","abstract_excerpt":"The far-from-equilibrium dynamics of spatial Polyakov loop correlations, which provide gauge-invariant observables akin to effective particle numbers for gluon plasmas, are investigated within real-time $\\mathrm{SU}(N_c)$ lattice gauge theory at weak couplings and large gluon occupations. The momentum zero mode of these correlations reveals the dynamic formation of a condensate, while at nonzero momenta, energy is transported toward the ultraviolet. We demonstrate that the non-zero momentum dynamics is well described by a direct cascade in terms of gauge-invariant Polyakov loop excitations, ex"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.05582","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/2411.05582/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2411.05582","created_at":"2026-07-05T11:08:12.852007+00:00"},{"alias_kind":"arxiv_version","alias_value":"2411.05582v2","created_at":"2026-07-05T11:08:12.852007+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.05582","created_at":"2026-07-05T11:08:12.852007+00:00"},{"alias_kind":"pith_short_12","alias_value":"JUHYEKG42FUA","created_at":"2026-07-05T11:08:12.852007+00:00"},{"alias_kind":"pith_short_16","alias_value":"JUHYEKG42FUA4THR","created_at":"2026-07-05T11:08:12.852007+00:00"},{"alias_kind":"pith_short_8","alias_value":"JUHYEKG4","created_at":"2026-07-05T11:08:12.852007+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JUHYEKG42FUA4THRDFSEFOSH22","json":"https://pith.science/pith/JUHYEKG42FUA4THRDFSEFOSH22.json","graph_json":"https://pith.science/api/pith-number/JUHYEKG42FUA4THRDFSEFOSH22/graph.json","events_json":"https://pith.science/api/pith-number/JUHYEKG42FUA4THRDFSEFOSH22/events.json","paper":"https://pith.science/paper/JUHYEKG4"},"agent_actions":{"view_html":"https://pith.science/pith/JUHYEKG42FUA4THRDFSEFOSH22","download_json":"https://pith.science/pith/JUHYEKG42FUA4THRDFSEFOSH22.json","view_paper":"https://pith.science/paper/JUHYEKG4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2411.05582&json=true","fetch_graph":"https://pith.science/api/pith-number/JUHYEKG42FUA4THRDFSEFOSH22/graph.json","fetch_events":"https://pith.science/api/pith-number/JUHYEKG42FUA4THRDFSEFOSH22/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JUHYEKG42FUA4THRDFSEFOSH22/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JUHYEKG42FUA4THRDFSEFOSH22/action/storage_attestation","attest_author":"https://pith.science/pith/JUHYEKG42FUA4THRDFSEFOSH22/action/author_attestation","sign_citation":"https://pith.science/pith/JUHYEKG42FUA4THRDFSEFOSH22/action/citation_signature","submit_replication":"https://pith.science/pith/JUHYEKG42FUA4THRDFSEFOSH22/action/replication_record"}},"created_at":"2026-07-05T11:08:12.852007+00:00","updated_at":"2026-07-05T11:08:12.852007+00:00"}