{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:HFJSRJSR2S7H5PXYWQCTRHMJH3","short_pith_number":"pith:HFJSRJSR","canonical_record":{"source":{"id":"1812.01040","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-12-03T19:19:50Z","cross_cats_sorted":["cond-mat.str-el","gr-qc"],"title_canon_sha256":"5e8fae6ecca8ea334ca586dc85ecefc2839e95cb0aa0372c536a894c87b5f8e0","abstract_canon_sha256":"4d0866cc697572abed35cda86a1c28fe0f9de33abce813e9c840c6f2d37e17dd"},"schema_version":"1.0"},"canonical_sha256":"395328a651d4be7ebef8b405389d893ed1ee0e754dbf24c8c44edcc7e942cc78","source":{"kind":"arxiv","id":"1812.01040","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.01040","created_at":"2026-05-17T23:49:40Z"},{"alias_kind":"arxiv_version","alias_value":"1812.01040v2","created_at":"2026-05-17T23:49:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.01040","created_at":"2026-05-17T23:49:40Z"},{"alias_kind":"pith_short_12","alias_value":"HFJSRJSR2S7H","created_at":"2026-05-18T12:32:28Z"},{"alias_kind":"pith_short_16","alias_value":"HFJSRJSR2S7H5PXY","created_at":"2026-05-18T12:32:28Z"},{"alias_kind":"pith_short_8","alias_value":"HFJSRJSR","created_at":"2026-05-18T12:32:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:HFJSRJSR2S7H5PXYWQCTRHMJH3","target":"record","payload":{"canonical_record":{"source":{"id":"1812.01040","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-12-03T19:19:50Z","cross_cats_sorted":["cond-mat.str-el","gr-qc"],"title_canon_sha256":"5e8fae6ecca8ea334ca586dc85ecefc2839e95cb0aa0372c536a894c87b5f8e0","abstract_canon_sha256":"4d0866cc697572abed35cda86a1c28fe0f9de33abce813e9c840c6f2d37e17dd"},"schema_version":"1.0"},"canonical_sha256":"395328a651d4be7ebef8b405389d893ed1ee0e754dbf24c8c44edcc7e942cc78","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:49:40.261389Z","signature_b64":"uRGxSz44ABjMHuLgUGTzq1aOqYE9dlxX3KmVP9ytY9MyBEGMaVUsgZ3Oy0hc5/Y3laMX/sVhcg4wUnRbmqahBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"395328a651d4be7ebef8b405389d893ed1ee0e754dbf24c8c44edcc7e942cc78","last_reissued_at":"2026-05-17T23:49:40.260719Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:49:40.260719Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1812.01040","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:49:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iOCPIrS/cLcg3ecrm9Csh3PoZu8r0+gJN9PSZZVNL9VSuGnrLM71UHHiBaf+KOG9QzmWWskjw9wf+cYzzz+1Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T19:58:06.276357Z"},"content_sha256":"358ca9e37365fddf7f73f0cdcb97802e790512ce365eba0cbea00213fe4b65f6","schema_version":"1.0","event_id":"sha256:358ca9e37365fddf7f73f0cdcb97802e790512ce365eba0cbea00213fe4b65f6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:HFJSRJSR2S7H5PXYWQCTRHMJH3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Anomalous scalings of the cuprate strange metals from nonlinear electrodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","gr-qc"],"primary_cat":"hep-th","authors_text":"Anthony Hoover, Li Li, Sera Cremonini, Steven Waskie","submitted_at":"2018-12-03T19:19:50Z","abstract_excerpt":"We examine transport in a holographic model which describes, through a nonlinear gauge field sector, generic nonlinear interactions between the charge carriers. Scaling exponents are introduced by using geometries which are nonrelativistic and hyperscaling-violating in the infrared. In the dilute charge limit in which the gauge field sector does not backreact on the geometry, a particularly simple nonlinear theory reproduces the anomalous temperature dependence of the resistivity and Hall angle of the cuprate strange metals, $R \\sim T$ and $\\cot\\Theta_H \\sim T^2$ while also allowing for a line"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.01040","kind":"arxiv","version":2},"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":"2026-05-17T23:49:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ucwhnjh169ldVf3jZd9NCTre1mCEOGeWux1R56om4iIlDMyHgBXQIQbh/ojYLAMyvUoE6Gm+3VL/kG9EBWnYBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T19:58:06.277015Z"},"content_sha256":"bdcfef0bfcc68bed8da8a31f80b74c7c9593b68f6d6af09c5081e499175aac10","schema_version":"1.0","event_id":"sha256:bdcfef0bfcc68bed8da8a31f80b74c7c9593b68f6d6af09c5081e499175aac10"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HFJSRJSR2S7H5PXYWQCTRHMJH3/bundle.json","state_url":"https://pith.science/pith/HFJSRJSR2S7H5PXYWQCTRHMJH3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HFJSRJSR2S7H5PXYWQCTRHMJH3/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":"2026-05-29T19:58:06Z","links":{"resolver":"https://pith.science/pith/HFJSRJSR2S7H5PXYWQCTRHMJH3","bundle":"https://pith.science/pith/HFJSRJSR2S7H5PXYWQCTRHMJH3/bundle.json","state":"https://pith.science/pith/HFJSRJSR2S7H5PXYWQCTRHMJH3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HFJSRJSR2S7H5PXYWQCTRHMJH3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:HFJSRJSR2S7H5PXYWQCTRHMJH3","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":"4d0866cc697572abed35cda86a1c28fe0f9de33abce813e9c840c6f2d37e17dd","cross_cats_sorted":["cond-mat.str-el","gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-12-03T19:19:50Z","title_canon_sha256":"5e8fae6ecca8ea334ca586dc85ecefc2839e95cb0aa0372c536a894c87b5f8e0"},"schema_version":"1.0","source":{"id":"1812.01040","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.01040","created_at":"2026-05-17T23:49:40Z"},{"alias_kind":"arxiv_version","alias_value":"1812.01040v2","created_at":"2026-05-17T23:49:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.01040","created_at":"2026-05-17T23:49:40Z"},{"alias_kind":"pith_short_12","alias_value":"HFJSRJSR2S7H","created_at":"2026-05-18T12:32:28Z"},{"alias_kind":"pith_short_16","alias_value":"HFJSRJSR2S7H5PXY","created_at":"2026-05-18T12:32:28Z"},{"alias_kind":"pith_short_8","alias_value":"HFJSRJSR","created_at":"2026-05-18T12:32:28Z"}],"graph_snapshots":[{"event_id":"sha256:bdcfef0bfcc68bed8da8a31f80b74c7c9593b68f6d6af09c5081e499175aac10","target":"graph","created_at":"2026-05-17T23:49:40Z","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 examine transport in a holographic model which describes, through a nonlinear gauge field sector, generic nonlinear interactions between the charge carriers. Scaling exponents are introduced by using geometries which are nonrelativistic and hyperscaling-violating in the infrared. In the dilute charge limit in which the gauge field sector does not backreact on the geometry, a particularly simple nonlinear theory reproduces the anomalous temperature dependence of the resistivity and Hall angle of the cuprate strange metals, $R \\sim T$ and $\\cot\\Theta_H \\sim T^2$ while also allowing for a line","authors_text":"Anthony Hoover, Li Li, Sera Cremonini, Steven Waskie","cross_cats":["cond-mat.str-el","gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-12-03T19:19:50Z","title":"Anomalous scalings of the cuprate strange metals from nonlinear electrodynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.01040","kind":"arxiv","version":2},"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":"sha256:358ca9e37365fddf7f73f0cdcb97802e790512ce365eba0cbea00213fe4b65f6","target":"record","created_at":"2026-05-17T23:49:40Z","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":"4d0866cc697572abed35cda86a1c28fe0f9de33abce813e9c840c6f2d37e17dd","cross_cats_sorted":["cond-mat.str-el","gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-12-03T19:19:50Z","title_canon_sha256":"5e8fae6ecca8ea334ca586dc85ecefc2839e95cb0aa0372c536a894c87b5f8e0"},"schema_version":"1.0","source":{"id":"1812.01040","kind":"arxiv","version":2}},"canonical_sha256":"395328a651d4be7ebef8b405389d893ed1ee0e754dbf24c8c44edcc7e942cc78","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"395328a651d4be7ebef8b405389d893ed1ee0e754dbf24c8c44edcc7e942cc78","first_computed_at":"2026-05-17T23:49:40.260719Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:49:40.260719Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"uRGxSz44ABjMHuLgUGTzq1aOqYE9dlxX3KmVP9ytY9MyBEGMaVUsgZ3Oy0hc5/Y3laMX/sVhcg4wUnRbmqahBA==","signature_status":"signed_v1","signed_at":"2026-05-17T23:49:40.261389Z","signed_message":"canonical_sha256_bytes"},"source_id":"1812.01040","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:358ca9e37365fddf7f73f0cdcb97802e790512ce365eba0cbea00213fe4b65f6","sha256:bdcfef0bfcc68bed8da8a31f80b74c7c9593b68f6d6af09c5081e499175aac10"],"state_sha256":"84a787df13840cb0fd1cfda6a0d6c94a6d993481e21d7f630504515735bc7c2c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"a/+yUI5fAsG6A4VO6uKmwH31UfXeA03Lx4d+PStC7kep77CqC5emXt4D8hlItcmMPq5NgI1BHleaQvQ6GjiqAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T19:58:06.280422Z","bundle_sha256":"2f253b378383bd0d3b98a79ed601693543cd2d3da616950f47c7006109928e8f"}}