{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2021:5AK6WJ5H55KPIAOSVDJS2JVJZD","short_pith_number":"pith:5AK6WJ5H","canonical_record":{"source":{"id":"2103.04163","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-03-06T17:45:03Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"f771858d3173f8f5f2634ffd7eb98612cc1ba15b41a97a0fe43df8c1e668bcbe","abstract_canon_sha256":"234e7b90aad01445eaa14cb76f5009700c41af62d150265695300768cebda9e8"},"schema_version":"1.0"},"canonical_sha256":"e815eb27a7ef54f401d2a8d32d26a9c8e6d7c5c25ff553d788d9a0387e237018","source":{"kind":"arxiv","id":"2103.04163","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2103.04163","created_at":"2026-07-05T02:45:24Z"},{"alias_kind":"arxiv_version","alias_value":"2103.04163v1","created_at":"2026-07-05T02:45:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.04163","created_at":"2026-07-05T02:45:24Z"},{"alias_kind":"pith_short_12","alias_value":"5AK6WJ5H55KP","created_at":"2026-07-05T02:45:24Z"},{"alias_kind":"pith_short_16","alias_value":"5AK6WJ5H55KPIAOS","created_at":"2026-07-05T02:45:24Z"},{"alias_kind":"pith_short_8","alias_value":"5AK6WJ5H","created_at":"2026-07-05T02:45:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2021:5AK6WJ5H55KPIAOSVDJS2JVJZD","target":"record","payload":{"canonical_record":{"source":{"id":"2103.04163","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-03-06T17:45:03Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"f771858d3173f8f5f2634ffd7eb98612cc1ba15b41a97a0fe43df8c1e668bcbe","abstract_canon_sha256":"234e7b90aad01445eaa14cb76f5009700c41af62d150265695300768cebda9e8"},"schema_version":"1.0"},"canonical_sha256":"e815eb27a7ef54f401d2a8d32d26a9c8e6d7c5c25ff553d788d9a0387e237018","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:45:24.649241Z","signature_b64":"m0iU+6AS02/5OdpoxhKvMw9EZ5dZ7bkKPwaZa4okJ8tEe8QWyENLIGIX4zKwqcUf2TphWhok/nO9Yzdw1iDkAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e815eb27a7ef54f401d2a8d32d26a9c8e6d7c5c25ff553d788d9a0387e237018","last_reissued_at":"2026-07-05T02:45:24.648795Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:45:24.648795Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2103.04163","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":"2026-07-05T02:45:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qJeInPfSihD+1PstiNZ9BWrNHJJZKFNwl+m3vt8aYCyZWYeKt3oAfDXSRPjT1HHJi3nO/LJssxubcSf3+60oAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-25T04:47:45.442185Z"},"content_sha256":"b8f0104b07c80a8ba7060855d84df7d4118f830457eacae8e90561627699a27b","schema_version":"1.0","event_id":"sha256:b8f0104b07c80a8ba7060855d84df7d4118f830457eacae8e90561627699a27b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2021:5AK6WJ5H55KPIAOSVDJS2JVJZD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"W-infinity Symmetry in the Quantum Hall Effect Beyond the Edge","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Andrea Cappelli, Lorenzo Maffi","submitted_at":"2021-03-06T17:45:03Z","abstract_excerpt":"The description of chiral quantum incompressible fluids by the W-infinity symmetry can be extended from the edge, where it encompasses the conformal field theory approach, to the non-conformal bulk. The two regimes are characterized by excitations with different sizes, energies and momenta within the disk geometry. In particular, the bulk quantities have a finite limit for large droplets. We obtain analytic results for the radial shape of excitations, the edge reconstruction phenomenon and the energy spectrum of density fluctuations in Laughlin states."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.04163","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2103.04163/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T02:45:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tQCXypa+cAHiJNfqqhJpV+WzR5MCyT2YICkuHGIuBmouqma+hJN81tvTkEBh8o3gSLEm9QAJF9MOPsMf6dllBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-25T04:47:45.442562Z"},"content_sha256":"eb74dbe16d0eb60705a98dd6d1577f128ff2685f7dba8f2236f87d6205b30682","schema_version":"1.0","event_id":"sha256:eb74dbe16d0eb60705a98dd6d1577f128ff2685f7dba8f2236f87d6205b30682"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5AK6WJ5H55KPIAOSVDJS2JVJZD/bundle.json","state_url":"https://pith.science/pith/5AK6WJ5H55KPIAOSVDJS2JVJZD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5AK6WJ5H55KPIAOSVDJS2JVJZD/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":"2026-07-25T04:47:45Z","links":{"resolver":"https://pith.science/pith/5AK6WJ5H55KPIAOSVDJS2JVJZD","bundle":"https://pith.science/pith/5AK6WJ5H55KPIAOSVDJS2JVJZD/bundle.json","state":"https://pith.science/pith/5AK6WJ5H55KPIAOSVDJS2JVJZD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5AK6WJ5H55KPIAOSVDJS2JVJZD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:5AK6WJ5H55KPIAOSVDJS2JVJZD","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":"234e7b90aad01445eaa14cb76f5009700c41af62d150265695300768cebda9e8","cross_cats_sorted":["cond-mat.str-el"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-03-06T17:45:03Z","title_canon_sha256":"f771858d3173f8f5f2634ffd7eb98612cc1ba15b41a97a0fe43df8c1e668bcbe"},"schema_version":"1.0","source":{"id":"2103.04163","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2103.04163","created_at":"2026-07-05T02:45:24Z"},{"alias_kind":"arxiv_version","alias_value":"2103.04163v1","created_at":"2026-07-05T02:45:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.04163","created_at":"2026-07-05T02:45:24Z"},{"alias_kind":"pith_short_12","alias_value":"5AK6WJ5H55KP","created_at":"2026-07-05T02:45:24Z"},{"alias_kind":"pith_short_16","alias_value":"5AK6WJ5H55KPIAOS","created_at":"2026-07-05T02:45:24Z"},{"alias_kind":"pith_short_8","alias_value":"5AK6WJ5H","created_at":"2026-07-05T02:45:24Z"}],"graph_snapshots":[{"event_id":"sha256:eb74dbe16d0eb60705a98dd6d1577f128ff2685f7dba8f2236f87d6205b30682","target":"graph","created_at":"2026-07-05T02:45:24Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2103.04163/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The description of chiral quantum incompressible fluids by the W-infinity symmetry can be extended from the edge, where it encompasses the conformal field theory approach, to the non-conformal bulk. The two regimes are characterized by excitations with different sizes, energies and momenta within the disk geometry. In particular, the bulk quantities have a finite limit for large droplets. We obtain analytic results for the radial shape of excitations, the edge reconstruction phenomenon and the energy spectrum of density fluctuations in Laughlin states.","authors_text":"Andrea Cappelli, Lorenzo Maffi","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-03-06T17:45:03Z","title":"W-infinity Symmetry in the Quantum Hall Effect Beyond the Edge"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.04163","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:b8f0104b07c80a8ba7060855d84df7d4118f830457eacae8e90561627699a27b","target":"record","created_at":"2026-07-05T02:45:24Z","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":"234e7b90aad01445eaa14cb76f5009700c41af62d150265695300768cebda9e8","cross_cats_sorted":["cond-mat.str-el"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-03-06T17:45:03Z","title_canon_sha256":"f771858d3173f8f5f2634ffd7eb98612cc1ba15b41a97a0fe43df8c1e668bcbe"},"schema_version":"1.0","source":{"id":"2103.04163","kind":"arxiv","version":1}},"canonical_sha256":"e815eb27a7ef54f401d2a8d32d26a9c8e6d7c5c25ff553d788d9a0387e237018","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e815eb27a7ef54f401d2a8d32d26a9c8e6d7c5c25ff553d788d9a0387e237018","first_computed_at":"2026-07-05T02:45:24.648795Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T02:45:24.648795Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"m0iU+6AS02/5OdpoxhKvMw9EZ5dZ7bkKPwaZa4okJ8tEe8QWyENLIGIX4zKwqcUf2TphWhok/nO9Yzdw1iDkAg==","signature_status":"signed_v1","signed_at":"2026-07-05T02:45:24.649241Z","signed_message":"canonical_sha256_bytes"},"source_id":"2103.04163","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b8f0104b07c80a8ba7060855d84df7d4118f830457eacae8e90561627699a27b","sha256:eb74dbe16d0eb60705a98dd6d1577f128ff2685f7dba8f2236f87d6205b30682"],"state_sha256":"6651705541a2f6d2c3c77fa36994576c23b407d809e8664d0c7505e5ac6c1032"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QXCxO8QoaldCHDDQgA1mtUFnYMTk6t/azYi/I0vhxFaF1eqV90iNLjIH+F+5U/7SGN4uPlB3AiyontQ+99j6Dw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-25T04:47:45.444947Z","bundle_sha256":"b0d7ccf22edaa069e74081546d70a7adddc841a19040cd5518fce60117efb532"}}