{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:HXVLWUMJUWXJWMH2TXEJJWDQ33","short_pith_number":"pith:HXVLWUMJ","canonical_record":{"source":{"id":"1707.04182","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-07-13T15:45:07Z","cross_cats_sorted":["cond-mat.str-el","nucl-th","physics.plasm-ph"],"title_canon_sha256":"3d318cbd11459746c6c6e4a304fa5349765a6602f6cf05e7d26e9dc1d7d60018","abstract_canon_sha256":"5529d90ecab9b5bb74d1fe00bd96b8c0b878b80a8c1a701972cc130a0c17cc72"},"schema_version":"1.0"},"canonical_sha256":"3deabb5189a5ae9b30fa9dc894d870dece9a09fbd46874f7ceb460c0fbcb9249","source":{"kind":"arxiv","id":"1707.04182","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"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:HXVLWUMJUWXJWMH2TXEJJWDQ33","target":"record","payload":{"canonical_record":{"source":{"id":"1707.04182","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-07-13T15:45:07Z","cross_cats_sorted":["cond-mat.str-el","nucl-th","physics.plasm-ph"],"title_canon_sha256":"3d318cbd11459746c6c6e4a304fa5349765a6602f6cf05e7d26e9dc1d7d60018","abstract_canon_sha256":"5529d90ecab9b5bb74d1fe00bd96b8c0b878b80a8c1a701972cc130a0c17cc72"},"schema_version":"1.0"},"canonical_sha256":"3deabb5189a5ae9b30fa9dc894d870dece9a09fbd46874f7ceb460c0fbcb9249","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:47:44.526272Z","signature_b64":"F6JPwZGXGnhsE0rALP9fskzXwcTogg8COh/gw1D6LLTjKrvtUQBt0XRo+HghvsxmldHjGOx058l1gIPuPSvtDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3deabb5189a5ae9b30fa9dc894d870dece9a09fbd46874f7ceb460c0fbcb9249","last_reissued_at":"2026-05-17T23:47:44.525718Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:47:44.525718Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1707.04182","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:47:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Wdq74v6kYChZf48jEVS5JtV/7D/Zu0NGZ7Q67tIWXrNd6KKTBVqbRkb3z5g7sPp8CWBOfSmi4QpCbaiexXoFCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T10:07:37.553593Z"},"content_sha256":"f591761a9f362a2b8f783e2d468cc613552f17f95fa55e20fc66f67f8827dffe","schema_version":"1.0","event_id":"sha256:f591761a9f362a2b8f783e2d468cc613552f17f95fa55e20fc66f67f8827dffe"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:HXVLWUMJUWXJWMH2TXEJJWDQ33","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Generalised global symmetries in holography: magnetohydrodynamic waves in a strongly interacting plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","nucl-th","physics.plasm-ph"],"primary_cat":"hep-th","authors_text":"Napat Poovuttikul, Sa\\v{s}o Grozdanov","submitted_at":"2017-07-13T15:45:07Z","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"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.04182","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"2026-05-17T23:47:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MRcOE7s6mpjiiwC1vAktbEPhI1WRVuvrLT5O8Yngvw/fG5vGolU/eZ6GfEeJKt3QdajRyblTqU6c4Ths1dNrDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T10:07:37.554328Z"},"content_sha256":"26f8bf81c1693bdc59e13df647ef2dd3844d1cfee0de44a1f91c97009f7b7ff6","schema_version":"1.0","event_id":"sha256:26f8bf81c1693bdc59e13df647ef2dd3844d1cfee0de44a1f91c97009f7b7ff6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HXVLWUMJUWXJWMH2TXEJJWDQ33/bundle.json","state_url":"https://pith.science/pith/HXVLWUMJUWXJWMH2TXEJJWDQ33/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HXVLWUMJUWXJWMH2TXEJJWDQ33/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":"2026-05-26T10:07:37Z","links":{"resolver":"https://pith.science/pith/HXVLWUMJUWXJWMH2TXEJJWDQ33","bundle":"https://pith.science/pith/HXVLWUMJUWXJWMH2TXEJJWDQ33/bundle.json","state":"https://pith.science/pith/HXVLWUMJUWXJWMH2TXEJJWDQ33/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HXVLWUMJUWXJWMH2TXEJJWDQ33/bundle.json"},"state":{"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"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QAqm/OpBE+u9BTq15BUEh8akN+/SFKiUzus1WkFjjjRhkZEex+IYGp28eE1WNeat4HvPvg009D/eEB9emLfACw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T10:07:37.558213Z","bundle_sha256":"b4fa8ba8f46450579549caf228e2a4c7bce74d46fff5232b50bdbb72a905b93e"}}