{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:NJW5232TRGR7LFS6JYVJQI2BKJ","short_pith_number":"pith:NJW5232T","schema_version":"1.0","canonical_sha256":"6a6ddd6f5389a3f5965e4e2a982341527e7f2ed0a4822a0d5ffa2f9b70ff25fe","source":{"kind":"arxiv","id":"1801.09084","version":3},"attestation_state":"computed","paper":{"title":"Incoherent transport for phases that spontaneously break translations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Aristomenis Donos, Jerome P. Gauntlett, Tom Griffin, Vaios Ziogas","submitted_at":"2018-01-27T12:44:00Z","abstract_excerpt":"We consider phases of matter at finite charge density which spontaneously break spatial translations. Without taking a hydrodynamic limit we identify a boost invariant incoherent current operator. We also derive expressions for the small frequency behaviour of the thermoelectric conductivities generalising those that have been derived in a translationally invariant context. Within holographic constructions we show that the DC conductivity for the incoherent current can be obtained from a solution to a Stokes flow for an auxiliary fluid on the black hole horizon combined with specific thermodyn"},"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":"1801.09084","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-01-27T12:44:00Z","cross_cats_sorted":[],"title_canon_sha256":"543b5161bf05108e537ec5f5aa8ec6ed16273f7b16bef9ebb87774c64cc3049e","abstract_canon_sha256":"1b0e67789a009dbdf16b705c987da675aff93f1d5ac689e5ae0f1de10f673a47"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:16:26.802094Z","signature_b64":"IPs67sleBc/OnUU4W6+N4fCJGz8CNjbJmu6Y3tlvNgg9/RYLBU7e0tzCgzUwrnP8w+EnwlXzfN6O5i+8NZNoDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6a6ddd6f5389a3f5965e4e2a982341527e7f2ed0a4822a0d5ffa2f9b70ff25fe","last_reissued_at":"2026-05-18T00:16:26.801608Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:16:26.801608Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Incoherent transport for phases that spontaneously break translations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Aristomenis Donos, Jerome P. Gauntlett, Tom Griffin, Vaios Ziogas","submitted_at":"2018-01-27T12:44:00Z","abstract_excerpt":"We consider phases of matter at finite charge density which spontaneously break spatial translations. Without taking a hydrodynamic limit we identify a boost invariant incoherent current operator. We also derive expressions for the small frequency behaviour of the thermoelectric conductivities generalising those that have been derived in a translationally invariant context. Within holographic constructions we show that the DC conductivity for the incoherent current can be obtained from a solution to a Stokes flow for an auxiliary fluid on the black hole horizon combined with specific thermodyn"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.09084","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1801.09084","created_at":"2026-05-18T00:16:26.801683+00:00"},{"alias_kind":"arxiv_version","alias_value":"1801.09084v3","created_at":"2026-05-18T00:16:26.801683+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.09084","created_at":"2026-05-18T00:16:26.801683+00:00"},{"alias_kind":"pith_short_12","alias_value":"NJW5232TRGR7","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_16","alias_value":"NJW5232TRGR7LFS6","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_8","alias_value":"NJW5232T","created_at":"2026-05-18T12:32:40.477152+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.19694","citing_title":"Linear response beyond hydrodynamic poles","ref_index":9,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NJW5232TRGR7LFS6JYVJQI2BKJ","json":"https://pith.science/pith/NJW5232TRGR7LFS6JYVJQI2BKJ.json","graph_json":"https://pith.science/api/pith-number/NJW5232TRGR7LFS6JYVJQI2BKJ/graph.json","events_json":"https://pith.science/api/pith-number/NJW5232TRGR7LFS6JYVJQI2BKJ/events.json","paper":"https://pith.science/paper/NJW5232T"},"agent_actions":{"view_html":"https://pith.science/pith/NJW5232TRGR7LFS6JYVJQI2BKJ","download_json":"https://pith.science/pith/NJW5232TRGR7LFS6JYVJQI2BKJ.json","view_paper":"https://pith.science/paper/NJW5232T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1801.09084&json=true","fetch_graph":"https://pith.science/api/pith-number/NJW5232TRGR7LFS6JYVJQI2BKJ/graph.json","fetch_events":"https://pith.science/api/pith-number/NJW5232TRGR7LFS6JYVJQI2BKJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NJW5232TRGR7LFS6JYVJQI2BKJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NJW5232TRGR7LFS6JYVJQI2BKJ/action/storage_attestation","attest_author":"https://pith.science/pith/NJW5232TRGR7LFS6JYVJQI2BKJ/action/author_attestation","sign_citation":"https://pith.science/pith/NJW5232TRGR7LFS6JYVJQI2BKJ/action/citation_signature","submit_replication":"https://pith.science/pith/NJW5232TRGR7LFS6JYVJQI2BKJ/action/replication_record"}},"created_at":"2026-05-18T00:16:26.801683+00:00","updated_at":"2026-05-18T00:16:26.801683+00:00"}