{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:ALGKLUTENHNKJISB7E76J3YLAH","short_pith_number":"pith:ALGKLUTE","canonical_record":{"source":{"id":"1507.08946","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-07-31T17:01:28Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.str-el","physics.flu-dyn"],"title_canon_sha256":"6be966a152423883b807c7a7ea670bfba276018469a6745ea1f9f6b459002a00","abstract_canon_sha256":"c072c1b9dfafc72653a7bc5271639deb93a2a9ce7ef5ed561bfd505523ace7a2"},"schema_version":"1.0"},"canonical_sha256":"02cca5d26469daa4a241f93fe4ef0b01e90aaa566e7b5d67d4b6c2cc54e99040","source":{"kind":"arxiv","id":"1507.08946","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1507.08946","created_at":"2026-05-18T01:32:28Z"},{"alias_kind":"arxiv_version","alias_value":"1507.08946v1","created_at":"2026-05-18T01:32:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.08946","created_at":"2026-05-18T01:32:28Z"},{"alias_kind":"pith_short_12","alias_value":"ALGKLUTENHNK","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_16","alias_value":"ALGKLUTENHNKJISB","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_8","alias_value":"ALGKLUTE","created_at":"2026-05-18T12:29:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:ALGKLUTENHNKJISB7E76J3YLAH","target":"record","payload":{"canonical_record":{"source":{"id":"1507.08946","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-07-31T17:01:28Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.str-el","physics.flu-dyn"],"title_canon_sha256":"6be966a152423883b807c7a7ea670bfba276018469a6745ea1f9f6b459002a00","abstract_canon_sha256":"c072c1b9dfafc72653a7bc5271639deb93a2a9ce7ef5ed561bfd505523ace7a2"},"schema_version":"1.0"},"canonical_sha256":"02cca5d26469daa4a241f93fe4ef0b01e90aaa566e7b5d67d4b6c2cc54e99040","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:32:28.451728Z","signature_b64":"cWReIMg6zR8WklTKulEhU/LCO/f6dJSieNQXdkAIyCe4jNpkgnNxJIaLMDApc8DxAWMT7x/e5A4Ew87XdDHEBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"02cca5d26469daa4a241f93fe4ef0b01e90aaa566e7b5d67d4b6c2cc54e99040","last_reissued_at":"2026-05-18T01:32:28.450981Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:32:28.450981Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1507.08946","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:32:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"n0T0IDAiWYvYT91T1DMdUv877Z8tZZMzET8zT5t/3IqYyiSsyA/w60nLaphBVDeh4TnrFIV5XlmMFhRxTtirDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T16:56:06.803813Z"},"content_sha256":"524b31885e278b34dfc1e7ca4d6309565b079cf510efb2be01db314d6ecb462a","schema_version":"1.0","event_id":"sha256:524b31885e278b34dfc1e7ca4d6309565b079cf510efb2be01db314d6ecb462a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:ALGKLUTENHNKJISB7E76J3YLAH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Collision-dominated nonlinear hydrodynamics in graphene","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.str-el","physics.flu-dyn"],"primary_cat":"cond-mat.mes-hall","authors_text":"A.D. Mirlin, B.N. Narozhny, I.V. Gornyi, M. Sch\\\"utt, M. Titov, U. Briskot","submitted_at":"2015-07-31T17:01:28Z","abstract_excerpt":"We present an effective hydrodynamic theory of electronic transport in graphene in the interaction-dominated regime. We derive the emergent hydrodynamic description from the microscopic Boltzmann kinetic equation taking into account dissipation due to Coulomb interaction and find the viscosity of Dirac fermions in graphene for arbitrary densities. The viscous terms have a dramatic effect on transport coefficients in clean samples at high temperatures. Within linear response, we show that viscosity manifests itself in the nonlocal conductivity as well as dispersion of hydrodynamic plasmons. Bey"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.08946","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":""},"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":"2026-05-18T01:32:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2id8n5iHMZfuOWzvl47J2RgNeC49wnz9NeXO7y64gIcMa1yq2Ya0eHYcimfDuBu1gzhb3jqk3slfQLR12Uw6Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T16:56:06.804151Z"},"content_sha256":"b75c1b33a12126cb0cf011bc030c70e266adf421fa89cab3f771489d943d8237","schema_version":"1.0","event_id":"sha256:b75c1b33a12126cb0cf011bc030c70e266adf421fa89cab3f771489d943d8237"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ALGKLUTENHNKJISB7E76J3YLAH/bundle.json","state_url":"https://pith.science/pith/ALGKLUTENHNKJISB7E76J3YLAH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ALGKLUTENHNKJISB7E76J3YLAH/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":"2026-06-01T16:56:06Z","links":{"resolver":"https://pith.science/pith/ALGKLUTENHNKJISB7E76J3YLAH","bundle":"https://pith.science/pith/ALGKLUTENHNKJISB7E76J3YLAH/bundle.json","state":"https://pith.science/pith/ALGKLUTENHNKJISB7E76J3YLAH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ALGKLUTENHNKJISB7E76J3YLAH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:ALGKLUTENHNKJISB7E76J3YLAH","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":"c072c1b9dfafc72653a7bc5271639deb93a2a9ce7ef5ed561bfd505523ace7a2","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.str-el","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-07-31T17:01:28Z","title_canon_sha256":"6be966a152423883b807c7a7ea670bfba276018469a6745ea1f9f6b459002a00"},"schema_version":"1.0","source":{"id":"1507.08946","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1507.08946","created_at":"2026-05-18T01:32:28Z"},{"alias_kind":"arxiv_version","alias_value":"1507.08946v1","created_at":"2026-05-18T01:32:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.08946","created_at":"2026-05-18T01:32:28Z"},{"alias_kind":"pith_short_12","alias_value":"ALGKLUTENHNK","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_16","alias_value":"ALGKLUTENHNKJISB","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_8","alias_value":"ALGKLUTE","created_at":"2026-05-18T12:29:10Z"}],"graph_snapshots":[{"event_id":"sha256:b75c1b33a12126cb0cf011bc030c70e266adf421fa89cab3f771489d943d8237","target":"graph","created_at":"2026-05-18T01:32:28Z","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 present an effective hydrodynamic theory of electronic transport in graphene in the interaction-dominated regime. We derive the emergent hydrodynamic description from the microscopic Boltzmann kinetic equation taking into account dissipation due to Coulomb interaction and find the viscosity of Dirac fermions in graphene for arbitrary densities. The viscous terms have a dramatic effect on transport coefficients in clean samples at high temperatures. Within linear response, we show that viscosity manifests itself in the nonlocal conductivity as well as dispersion of hydrodynamic plasmons. Bey","authors_text":"A.D. Mirlin, B.N. Narozhny, I.V. Gornyi, M. Sch\\\"utt, M. Titov, U. Briskot","cross_cats":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.str-el","physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-07-31T17:01:28Z","title":"Collision-dominated nonlinear hydrodynamics in graphene"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.08946","kind":"arxiv","version":1},"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":"sha256:524b31885e278b34dfc1e7ca4d6309565b079cf510efb2be01db314d6ecb462a","target":"record","created_at":"2026-05-18T01:32:28Z","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":"c072c1b9dfafc72653a7bc5271639deb93a2a9ce7ef5ed561bfd505523ace7a2","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.str-el","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-07-31T17:01:28Z","title_canon_sha256":"6be966a152423883b807c7a7ea670bfba276018469a6745ea1f9f6b459002a00"},"schema_version":"1.0","source":{"id":"1507.08946","kind":"arxiv","version":1}},"canonical_sha256":"02cca5d26469daa4a241f93fe4ef0b01e90aaa566e7b5d67d4b6c2cc54e99040","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"02cca5d26469daa4a241f93fe4ef0b01e90aaa566e7b5d67d4b6c2cc54e99040","first_computed_at":"2026-05-18T01:32:28.450981Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:32:28.450981Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"cWReIMg6zR8WklTKulEhU/LCO/f6dJSieNQXdkAIyCe4jNpkgnNxJIaLMDApc8DxAWMT7x/e5A4Ew87XdDHEBA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:32:28.451728Z","signed_message":"canonical_sha256_bytes"},"source_id":"1507.08946","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:524b31885e278b34dfc1e7ca4d6309565b079cf510efb2be01db314d6ecb462a","sha256:b75c1b33a12126cb0cf011bc030c70e266adf421fa89cab3f771489d943d8237"],"state_sha256":"252ab291b496abebca000ae26bede19fa56ff35e4614d7ae5396aba58cb92fec"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gJ1GZTbcUxOPBB+d/TaaA4MHQ7RgMXOWgb2b+W1+KM0oEcBpxvc15OWk6BQ6GVK+wsHI5P2kzQZk2uNaZCY+Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T16:56:06.805999Z","bundle_sha256":"5ded67912201f05164611874eb52579e769c1935c32969c2c960b48fd2c06b34"}}