{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:CCA7ZXLDQHARZFKWEG5TWNAREB","short_pith_number":"pith:CCA7ZXLD","schema_version":"1.0","canonical_sha256":"1081fcdd6381c11c955621bb3b3411204ec2a30edd3a8dc1251d31944ba604d5","source":{"kind":"arxiv","id":"2602.22016","version":1},"attestation_state":"computed","paper":{"title":"Nonequilibrium steady states in driven holographic Weyl semi-metals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"James Stokes, Matteo Baggioli, Sebastian Grieninger","submitted_at":"2026-02-25T15:30:42Z","abstract_excerpt":"Three-dimensional Weyl materials provide a controlled setting for exploring Floquet dynamics in open quantum systems, including nonequilibrium steady states (NESS). Motivated by the desire for a strongly-coupled description, we employ holography to analyze the formation and stability of a NESS in a Weyl semi-metal induced by an external circularly polarized electric field. A time-periodic steady-state solution is constructed and its stability is determined from the spectrum of out-of-equilibrium quasinormal modes (Floquet exponents). A stable region in the drive parameter space is identified; "},"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":"2602.22016","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-02-25T15:30:42Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"a832a65539a5e41919ed6d8e0a7b87e94a0ee03156ed7e2dde98fae477d4a5f2","abstract_canon_sha256":"00af5ed535acfdde42f7f34ed2ab7427253a987ce5f63483d0f669a8db81bafb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-21T02:21:32.061363Z","signature_b64":"K85q2nKbt4/lMJEkrEou3A4zeWtqK+SwcYCCEIMq0zEB5s70D+87y2lUWnwXpjCvrPVHhwxwnQYgtZtCnVv8Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1081fcdd6381c11c955621bb3b3411204ec2a30edd3a8dc1251d31944ba604d5","last_reissued_at":"2026-07-21T02:21:32.060448Z","signature_status":"signed_v1","first_computed_at":"2026-07-21T02:21:32.060448Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonequilibrium steady states in driven holographic Weyl semi-metals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"James Stokes, Matteo Baggioli, Sebastian Grieninger","submitted_at":"2026-02-25T15:30:42Z","abstract_excerpt":"Three-dimensional Weyl materials provide a controlled setting for exploring Floquet dynamics in open quantum systems, including nonequilibrium steady states (NESS). Motivated by the desire for a strongly-coupled description, we employ holography to analyze the formation and stability of a NESS in a Weyl semi-metal induced by an external circularly polarized electric field. A time-periodic steady-state solution is constructed and its stability is determined from the spectrum of out-of-equilibrium quasinormal modes (Floquet exponents). A stable region in the drive parameter space is identified; "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2602.22016","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/2602.22016/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":"2602.22016","created_at":"2026-07-21T02:21:32.060870+00:00"},{"alias_kind":"arxiv_version","alias_value":"2602.22016v1","created_at":"2026-07-21T02:21:32.060870+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2602.22016","created_at":"2026-07-21T02:21:32.060870+00:00"},{"alias_kind":"pith_short_12","alias_value":"CCA7ZXLDQHAR","created_at":"2026-07-21T02:21:32.060870+00:00"},{"alias_kind":"pith_short_16","alias_value":"CCA7ZXLDQHARZFKW","created_at":"2026-07-21T02:21:32.060870+00:00"},{"alias_kind":"pith_short_8","alias_value":"CCA7ZXLD","created_at":"2026-07-21T02:21:32.060870+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.10689","citing_title":"Chiral Plasma under Strong Magnetic Fields: A Holographic Analysis of Transport Phenomena","ref_index":31,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CCA7ZXLDQHARZFKWEG5TWNAREB","json":"https://pith.science/pith/CCA7ZXLDQHARZFKWEG5TWNAREB.json","graph_json":"https://pith.science/api/pith-number/CCA7ZXLDQHARZFKWEG5TWNAREB/graph.json","events_json":"https://pith.science/api/pith-number/CCA7ZXLDQHARZFKWEG5TWNAREB/events.json","paper":"https://pith.science/paper/CCA7ZXLD"},"agent_actions":{"view_html":"https://pith.science/pith/CCA7ZXLDQHARZFKWEG5TWNAREB","download_json":"https://pith.science/pith/CCA7ZXLDQHARZFKWEG5TWNAREB.json","view_paper":"https://pith.science/paper/CCA7ZXLD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2602.22016&json=true","fetch_graph":"https://pith.science/api/pith-number/CCA7ZXLDQHARZFKWEG5TWNAREB/graph.json","fetch_events":"https://pith.science/api/pith-number/CCA7ZXLDQHARZFKWEG5TWNAREB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CCA7ZXLDQHARZFKWEG5TWNAREB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CCA7ZXLDQHARZFKWEG5TWNAREB/action/storage_attestation","attest_author":"https://pith.science/pith/CCA7ZXLDQHARZFKWEG5TWNAREB/action/author_attestation","sign_citation":"https://pith.science/pith/CCA7ZXLDQHARZFKWEG5TWNAREB/action/citation_signature","submit_replication":"https://pith.science/pith/CCA7ZXLDQHARZFKWEG5TWNAREB/action/replication_record"}},"created_at":"2026-07-21T02:21:32.060870+00:00","updated_at":"2026-07-21T02:21:32.060870+00:00"}