{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:HXVLWUMJUWXJWMH2TXEJJWDQ33","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":"5529d90ecab9b5bb74d1fe00bd96b8c0b878b80a8c1a701972cc130a0c17cc72","cross_cats_sorted":["cond-mat.str-el","nucl-th","physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-07-13T15:45:07Z","title_canon_sha256":"3d318cbd11459746c6c6e4a304fa5349765a6602f6cf05e7d26e9dc1d7d60018"},"schema_version":"1.0","source":{"id":"1707.04182","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.04182","created_at":"2026-05-17T23:47:44Z"},{"alias_kind":"arxiv_version","alias_value":"1707.04182v3","created_at":"2026-05-17T23:47:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.04182","created_at":"2026-05-17T23:47:44Z"},{"alias_kind":"pith_short_12","alias_value":"HXVLWUMJUWXJ","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"HXVLWUMJUWXJWMH2","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"HXVLWUMJ","created_at":"2026-05-18T12:31:21Z"}],"graph_snapshots":[{"event_id":"sha256:26f8bf81c1693bdc59e13df647ef2dd3844d1cfee0de44a1f91c97009f7b7ff6","target":"graph","created_at":"2026-05-17T23:47:44Z","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"},"paper":{"abstract_excerpt":"We begin the exploration of holographic duals to theories with generalised global (higher-form) symmetries. In particular, we focus on the case of magnetohydrodynamics (MHD) in strongly coupled plasmas by constructing and analysing a holographic dual to a recent, generalised global symmetry-based formulation of dissipative MHD. The simplest holographic dual to the effective theory of MHD that was proposed as a description of plasmas with any equation of state and transport coefficients contains dynamical graviton and two-form gauge field fluctuations in a magnetised black brane background. The","authors_text":"Napat Poovuttikul, Sa\\v{s}o Grozdanov","cross_cats":["cond-mat.str-el","nucl-th","physics.plasm-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-07-13T15:45:07Z","title":"Generalised global symmetries in holography: magnetohydrodynamic waves in a strongly interacting plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.04182","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:f591761a9f362a2b8f783e2d468cc613552f17f95fa55e20fc66f67f8827dffe","target":"record","created_at":"2026-05-17T23:47:44Z","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":"5529d90ecab9b5bb74d1fe00bd96b8c0b878b80a8c1a701972cc130a0c17cc72","cross_cats_sorted":["cond-mat.str-el","nucl-th","physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-07-13T15:45:07Z","title_canon_sha256":"3d318cbd11459746c6c6e4a304fa5349765a6602f6cf05e7d26e9dc1d7d60018"},"schema_version":"1.0","source":{"id":"1707.04182","kind":"arxiv","version":3}},"canonical_sha256":"3deabb5189a5ae9b30fa9dc894d870dece9a09fbd46874f7ceb460c0fbcb9249","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3deabb5189a5ae9b30fa9dc894d870dece9a09fbd46874f7ceb460c0fbcb9249","first_computed_at":"2026-05-17T23:47:44.525718Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:47:44.525718Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"F6JPwZGXGnhsE0rALP9fskzXwcTogg8COh/gw1D6LLTjKrvtUQBt0XRo+HghvsxmldHjGOx058l1gIPuPSvtDw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:47:44.526272Z","signed_message":"canonical_sha256_bytes"},"source_id":"1707.04182","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f591761a9f362a2b8f783e2d468cc613552f17f95fa55e20fc66f67f8827dffe","sha256:26f8bf81c1693bdc59e13df647ef2dd3844d1cfee0de44a1f91c97009f7b7ff6"],"state_sha256":"84fc984efd46f961653fe6bd5124c21329bdcc50f7b941ae79a9e76d0c7e9a48"}