{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:GS6I76EM6D54TOU7UPIG4QLQ7P","short_pith_number":"pith:GS6I76EM","canonical_record":{"source":{"id":"1509.00991","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-09-03T08:54:24Z","cross_cats_sorted":["cond-mat.supr-con","hep-th"],"title_canon_sha256":"3cffae50a54e8802835d2d08b9ea7b67ca336618355d6c07284d21dcc4665659","abstract_canon_sha256":"d2b9919506bde855e029bb25ce0c448de9deaf078ced3b930f5b445dcb312cb1"},"schema_version":"1.0"},"canonical_sha256":"34bc8ff88cf0fbc9ba9fa3d06e4170fbfa09bbebd84a608259513dddc7760519","source":{"kind":"arxiv","id":"1509.00991","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.00991","created_at":"2026-05-18T01:15:06Z"},{"alias_kind":"arxiv_version","alias_value":"1509.00991v3","created_at":"2026-05-18T01:15:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.00991","created_at":"2026-05-18T01:15:06Z"},{"alias_kind":"pith_short_12","alias_value":"GS6I76EM6D54","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_16","alias_value":"GS6I76EM6D54TOU7","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_8","alias_value":"GS6I76EM","created_at":"2026-05-18T12:29:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:GS6I76EM6D54TOU7UPIG4QLQ7P","target":"record","payload":{"canonical_record":{"source":{"id":"1509.00991","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-09-03T08:54:24Z","cross_cats_sorted":["cond-mat.supr-con","hep-th"],"title_canon_sha256":"3cffae50a54e8802835d2d08b9ea7b67ca336618355d6c07284d21dcc4665659","abstract_canon_sha256":"d2b9919506bde855e029bb25ce0c448de9deaf078ced3b930f5b445dcb312cb1"},"schema_version":"1.0"},"canonical_sha256":"34bc8ff88cf0fbc9ba9fa3d06e4170fbfa09bbebd84a608259513dddc7760519","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:15:06.754856Z","signature_b64":"nW+wm0ZpTtivOQveUDIGtf6yFNukUtzMZdiEJZnpDR5oSZ45QnVmbV2OnMkYhddVsajreAe6NwXfiTbtnWg1CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"34bc8ff88cf0fbc9ba9fa3d06e4170fbfa09bbebd84a608259513dddc7760519","last_reissued_at":"2026-05-18T01:15:06.754222Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:15:06.754222Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1509.00991","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":"2026-05-18T01:15:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cc6Kw+lJMBulEUHsSI8ULazIcVQl0X1cg+3uW80W8gOZMYuCCbPhMHl0ew2t+oI7jRUAy87aImKKfSlOWrs7Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T09:52:53.199479Z"},"content_sha256":"a40ee439d1e9bcaeee2f87d251fa7c1da73d40f5d03f91c2e90bf5e9ce9f4234","schema_version":"1.0","event_id":"sha256:a40ee439d1e9bcaeee2f87d251fa7c1da73d40f5d03f91c2e90bf5e9ce9f4234"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:GS6I76EM6D54TOU7UPIG4QLQ7P","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Strange Metals from Quantum Geometric Fluctuations of Interfaces","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Alexander V. Balatsky, A. R. Bishop, Jian-Huang She","submitted_at":"2015-09-03T08:54:24Z","abstract_excerpt":"Our current understanding of strongly correlated electron systems is based on a homogeneous framework. Here we take a step going beyond this paradigm by incorporating inhomogeneity from the beginning. Specifying to systems near the Mott metal-insulator transition, we propose a real space picture of itinerant electrons functioning in the fluctuating geometries bounded by interfaces between metallic and insulating regions. In 2+1-dimensions, the interfaces are closed bosonic strings, and we have a system of strings coupled to itinerant electrons. When the interface tension vanishes, the geometri"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.00991","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":"2026-05-18T01:15:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YWrn5I91+MiRbm0QeB71XUO8UJA4FP0N6iRHwXfQUMWWdNsaXlK0w0XRINoTGkEmtW1BVM6lYOyT/7cySS3yAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T09:52:53.199833Z"},"content_sha256":"002a2fd0f0cab53e1c849cc8207db6d2675676d0dd997a04d9cb522425fc952e","schema_version":"1.0","event_id":"sha256:002a2fd0f0cab53e1c849cc8207db6d2675676d0dd997a04d9cb522425fc952e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GS6I76EM6D54TOU7UPIG4QLQ7P/bundle.json","state_url":"https://pith.science/pith/GS6I76EM6D54TOU7UPIG4QLQ7P/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GS6I76EM6D54TOU7UPIG4QLQ7P/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":"2026-06-08T09:52:53Z","links":{"resolver":"https://pith.science/pith/GS6I76EM6D54TOU7UPIG4QLQ7P","bundle":"https://pith.science/pith/GS6I76EM6D54TOU7UPIG4QLQ7P/bundle.json","state":"https://pith.science/pith/GS6I76EM6D54TOU7UPIG4QLQ7P/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GS6I76EM6D54TOU7UPIG4QLQ7P/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:GS6I76EM6D54TOU7UPIG4QLQ7P","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":"d2b9919506bde855e029bb25ce0c448de9deaf078ced3b930f5b445dcb312cb1","cross_cats_sorted":["cond-mat.supr-con","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-09-03T08:54:24Z","title_canon_sha256":"3cffae50a54e8802835d2d08b9ea7b67ca336618355d6c07284d21dcc4665659"},"schema_version":"1.0","source":{"id":"1509.00991","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.00991","created_at":"2026-05-18T01:15:06Z"},{"alias_kind":"arxiv_version","alias_value":"1509.00991v3","created_at":"2026-05-18T01:15:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.00991","created_at":"2026-05-18T01:15:06Z"},{"alias_kind":"pith_short_12","alias_value":"GS6I76EM6D54","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_16","alias_value":"GS6I76EM6D54TOU7","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_8","alias_value":"GS6I76EM","created_at":"2026-05-18T12:29:22Z"}],"graph_snapshots":[{"event_id":"sha256:002a2fd0f0cab53e1c849cc8207db6d2675676d0dd997a04d9cb522425fc952e","target":"graph","created_at":"2026-05-18T01:15:06Z","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":"Our current understanding of strongly correlated electron systems is based on a homogeneous framework. Here we take a step going beyond this paradigm by incorporating inhomogeneity from the beginning. Specifying to systems near the Mott metal-insulator transition, we propose a real space picture of itinerant electrons functioning in the fluctuating geometries bounded by interfaces between metallic and insulating regions. In 2+1-dimensions, the interfaces are closed bosonic strings, and we have a system of strings coupled to itinerant electrons. When the interface tension vanishes, the geometri","authors_text":"Alexander V. Balatsky, A. R. Bishop, Jian-Huang She","cross_cats":["cond-mat.supr-con","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-09-03T08:54:24Z","title":"Strange Metals from Quantum Geometric Fluctuations of Interfaces"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.00991","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:a40ee439d1e9bcaeee2f87d251fa7c1da73d40f5d03f91c2e90bf5e9ce9f4234","target":"record","created_at":"2026-05-18T01:15:06Z","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":"d2b9919506bde855e029bb25ce0c448de9deaf078ced3b930f5b445dcb312cb1","cross_cats_sorted":["cond-mat.supr-con","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-09-03T08:54:24Z","title_canon_sha256":"3cffae50a54e8802835d2d08b9ea7b67ca336618355d6c07284d21dcc4665659"},"schema_version":"1.0","source":{"id":"1509.00991","kind":"arxiv","version":3}},"canonical_sha256":"34bc8ff88cf0fbc9ba9fa3d06e4170fbfa09bbebd84a608259513dddc7760519","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"34bc8ff88cf0fbc9ba9fa3d06e4170fbfa09bbebd84a608259513dddc7760519","first_computed_at":"2026-05-18T01:15:06.754222Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:15:06.754222Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nW+wm0ZpTtivOQveUDIGtf6yFNukUtzMZdiEJZnpDR5oSZ45QnVmbV2OnMkYhddVsajreAe6NwXfiTbtnWg1CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:15:06.754856Z","signed_message":"canonical_sha256_bytes"},"source_id":"1509.00991","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a40ee439d1e9bcaeee2f87d251fa7c1da73d40f5d03f91c2e90bf5e9ce9f4234","sha256:002a2fd0f0cab53e1c849cc8207db6d2675676d0dd997a04d9cb522425fc952e"],"state_sha256":"819200803bf0f8ca6386a2cb23706f324d264aaa0799cf1c01da541209f3a6c9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XHDtHIQhkOMH2rr8SezwWRVKKECsFcG3PpAkJgeBAG5vcF2XDA+R0kld7fEDHWxW9n0JtbUIl2V1Whus+TURDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T09:52:53.201811Z","bundle_sha256":"c6bd328c6c6ffb3cd5f55269a95c51d28630645f9cafb4169fe5a634cad93f90"}}