{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:B77A5ZWMUEMCBTJT7QG7PEESDM","short_pith_number":"pith:B77A5ZWM","canonical_record":{"source":{"id":"1702.08470","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-02-27T19:02:00Z","cross_cats_sorted":[],"title_canon_sha256":"3b097bcdbe2035428d8676b6b74969f24418c891b8c65d9f00253d39d088c6dc","abstract_canon_sha256":"f0997135b9390b2912af43c849aae21302dcffe7d63c5e7cff847d0e53d1ad0c"},"schema_version":"1.0"},"canonical_sha256":"0ffe0ee6cca11820cd33fc0df790921b3c02cf86f38671e5b5957d39bbeab9d5","source":{"kind":"arxiv","id":"1702.08470","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.08470","created_at":"2026-05-18T00:10:19Z"},{"alias_kind":"arxiv_version","alias_value":"1702.08470v2","created_at":"2026-05-18T00:10:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.08470","created_at":"2026-05-18T00:10:19Z"},{"alias_kind":"pith_short_12","alias_value":"B77A5ZWMUEMC","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"B77A5ZWMUEMCBTJT","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"B77A5ZWM","created_at":"2026-05-18T12:31:08Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:B77A5ZWMUEMCBTJT7QG7PEESDM","target":"record","payload":{"canonical_record":{"source":{"id":"1702.08470","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-02-27T19:02:00Z","cross_cats_sorted":[],"title_canon_sha256":"3b097bcdbe2035428d8676b6b74969f24418c891b8c65d9f00253d39d088c6dc","abstract_canon_sha256":"f0997135b9390b2912af43c849aae21302dcffe7d63c5e7cff847d0e53d1ad0c"},"schema_version":"1.0"},"canonical_sha256":"0ffe0ee6cca11820cd33fc0df790921b3c02cf86f38671e5b5957d39bbeab9d5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:10:19.509618Z","signature_b64":"460GYvDSb3SXVDlv5mOeDNlor2ibo1d4X6pgFxKhrGM8rLDH99yWY7Xd17jl5S+tVUW7hAvsI4XL7G5S/PT5AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0ffe0ee6cca11820cd33fc0df790921b3c02cf86f38671e5b5957d39bbeab9d5","last_reissued_at":"2026-05-18T00:10:19.509116Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:10:19.509116Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1702.08470","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":"2026-05-18T00:10:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"10A6v0CWfQa0DbfEAPeukEPv2LOg2fMfES8F7TKvqGZ6OMtJ6tNOnEGdupe3pcjbU/7Ne3MH3dEP4wL2OzEfBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T23:10:46.970694Z"},"content_sha256":"733b13ab202f6622a218b32bd0c2e84b5f74178531a1565f8876561d7441c23d","schema_version":"1.0","event_id":"sha256:733b13ab202f6622a218b32bd0c2e84b5f74178531a1565f8876561d7441c23d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:B77A5ZWMUEMCBTJT7QG7PEESDM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Solvable models for neutral modes in fractional quantum Hall edges","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Chris Heinrich, Michael Levin","submitted_at":"2017-02-27T19:02:00Z","abstract_excerpt":"We describe solvable models that capture how impurity scattering in certain fractional quantum Hall edges can give rise to a neutral mode --- i.e. an edge mode that does not carry electric charge. These models consist of two counter-propagating chiral Luttinger liquids together with a collection of discrete impurity scatterers. Our main result is an exact solution of these models in the limit of infinitely strong impurity scattering. From this solution, we explicitly derive the existence of a neutral mode and we determine all of its microscopic properties including its velocity. We also study "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.08470","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":"2026-05-18T00:10:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zBIOV8arjTzRI6ZeQz+E8omoiP/Z/JoqtOi/+PEhoR/TvSVeqjy3+SVO/RFk+DLNSiJXu9NtKq7z4TGwJj2VCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T23:10:46.971348Z"},"content_sha256":"72a56eddc601644011b597b6dd33f2d6c33d213f8940d82fe02a31a4474bde3d","schema_version":"1.0","event_id":"sha256:72a56eddc601644011b597b6dd33f2d6c33d213f8940d82fe02a31a4474bde3d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/B77A5ZWMUEMCBTJT7QG7PEESDM/bundle.json","state_url":"https://pith.science/pith/B77A5ZWMUEMCBTJT7QG7PEESDM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/B77A5ZWMUEMCBTJT7QG7PEESDM/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":"2026-05-25T23:10:46Z","links":{"resolver":"https://pith.science/pith/B77A5ZWMUEMCBTJT7QG7PEESDM","bundle":"https://pith.science/pith/B77A5ZWMUEMCBTJT7QG7PEESDM/bundle.json","state":"https://pith.science/pith/B77A5ZWMUEMCBTJT7QG7PEESDM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/B77A5ZWMUEMCBTJT7QG7PEESDM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:B77A5ZWMUEMCBTJT7QG7PEESDM","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":"f0997135b9390b2912af43c849aae21302dcffe7d63c5e7cff847d0e53d1ad0c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-02-27T19:02:00Z","title_canon_sha256":"3b097bcdbe2035428d8676b6b74969f24418c891b8c65d9f00253d39d088c6dc"},"schema_version":"1.0","source":{"id":"1702.08470","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.08470","created_at":"2026-05-18T00:10:19Z"},{"alias_kind":"arxiv_version","alias_value":"1702.08470v2","created_at":"2026-05-18T00:10:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.08470","created_at":"2026-05-18T00:10:19Z"},{"alias_kind":"pith_short_12","alias_value":"B77A5ZWMUEMC","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"B77A5ZWMUEMCBTJT","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"B77A5ZWM","created_at":"2026-05-18T12:31:08Z"}],"graph_snapshots":[{"event_id":"sha256:72a56eddc601644011b597b6dd33f2d6c33d213f8940d82fe02a31a4474bde3d","target":"graph","created_at":"2026-05-18T00:10:19Z","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 describe solvable models that capture how impurity scattering in certain fractional quantum Hall edges can give rise to a neutral mode --- i.e. an edge mode that does not carry electric charge. These models consist of two counter-propagating chiral Luttinger liquids together with a collection of discrete impurity scatterers. Our main result is an exact solution of these models in the limit of infinitely strong impurity scattering. From this solution, we explicitly derive the existence of a neutral mode and we determine all of its microscopic properties including its velocity. We also study ","authors_text":"Chris Heinrich, Michael Levin","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-02-27T19:02:00Z","title":"Solvable models for neutral modes in fractional quantum Hall edges"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.08470","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":"sha256:733b13ab202f6622a218b32bd0c2e84b5f74178531a1565f8876561d7441c23d","target":"record","created_at":"2026-05-18T00:10:19Z","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":"f0997135b9390b2912af43c849aae21302dcffe7d63c5e7cff847d0e53d1ad0c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-02-27T19:02:00Z","title_canon_sha256":"3b097bcdbe2035428d8676b6b74969f24418c891b8c65d9f00253d39d088c6dc"},"schema_version":"1.0","source":{"id":"1702.08470","kind":"arxiv","version":2}},"canonical_sha256":"0ffe0ee6cca11820cd33fc0df790921b3c02cf86f38671e5b5957d39bbeab9d5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0ffe0ee6cca11820cd33fc0df790921b3c02cf86f38671e5b5957d39bbeab9d5","first_computed_at":"2026-05-18T00:10:19.509116Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:10:19.509116Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"460GYvDSb3SXVDlv5mOeDNlor2ibo1d4X6pgFxKhrGM8rLDH99yWY7Xd17jl5S+tVUW7hAvsI4XL7G5S/PT5AA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:10:19.509618Z","signed_message":"canonical_sha256_bytes"},"source_id":"1702.08470","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:733b13ab202f6622a218b32bd0c2e84b5f74178531a1565f8876561d7441c23d","sha256:72a56eddc601644011b597b6dd33f2d6c33d213f8940d82fe02a31a4474bde3d"],"state_sha256":"59161d063ef0e78ca26ec68848df0a9d952cc5872476325149d84a8e3f357ae8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nywbQ2gPILF3tEkZOzSglzGJvdF2uNeKy3CaMZ9g7UF7gkTeY8298vgMC9+6szlsKErdFmP+RPXj9pLlydM2AA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T23:10:46.974592Z","bundle_sha256":"bd67ae9bfb648f797b4d588330c0ccdcf906cec14eaaa1229bd06d0e7f0eaf44"}}