{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:6HR23DXXZ4XZKWIP6F5LINUGIH","short_pith_number":"pith:6HR23DXX","canonical_record":{"source":{"id":"2508.16547","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-08-22T17:12:18Z","cross_cats_sorted":["cond-mat.str-el","math-ph","math.MP","quant-ph"],"title_canon_sha256":"bef9507f8f4f7932f449ec67bfea311cf07cf7c4ee7e4e8b4cc79e22a0340cbd","abstract_canon_sha256":"f4c0eafefae2b835710e4671a6f0fa0a727970fa06c3f3857204c3df28f5a927"},"schema_version":"1.0"},"canonical_sha256":"f1e3ad8ef7cf2f95590ff17ab4368641c0fb1039cd86f95ab408908ab18fa151","source":{"kind":"arxiv","id":"2508.16547","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2508.16547","created_at":"2026-07-05T11:57:50Z"},{"alias_kind":"arxiv_version","alias_value":"2508.16547v1","created_at":"2026-07-05T11:57:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.16547","created_at":"2026-07-05T11:57:50Z"},{"alias_kind":"pith_short_12","alias_value":"6HR23DXXZ4XZ","created_at":"2026-07-05T11:57:50Z"},{"alias_kind":"pith_short_16","alias_value":"6HR23DXXZ4XZKWIP","created_at":"2026-07-05T11:57:50Z"},{"alias_kind":"pith_short_8","alias_value":"6HR23DXX","created_at":"2026-07-05T11:57:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:6HR23DXXZ4XZKWIP6F5LINUGIH","target":"record","payload":{"canonical_record":{"source":{"id":"2508.16547","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-08-22T17:12:18Z","cross_cats_sorted":["cond-mat.str-el","math-ph","math.MP","quant-ph"],"title_canon_sha256":"bef9507f8f4f7932f449ec67bfea311cf07cf7c4ee7e4e8b4cc79e22a0340cbd","abstract_canon_sha256":"f4c0eafefae2b835710e4671a6f0fa0a727970fa06c3f3857204c3df28f5a927"},"schema_version":"1.0"},"canonical_sha256":"f1e3ad8ef7cf2f95590ff17ab4368641c0fb1039cd86f95ab408908ab18fa151","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:57:50.558285Z","signature_b64":"sMaUKPe8f1V2Fh2g4wex+omtbMgjinHFF9Zhve8dB8i0la2gQOK+NZ2KkNTZoBet8nabqPDYDIR/bHsQXRYKCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f1e3ad8ef7cf2f95590ff17ab4368641c0fb1039cd86f95ab408908ab18fa151","last_reissued_at":"2026-07-05T11:57:50.557796Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:57:50.557796Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2508.16547","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":"2026-07-05T11:57:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vS0DF8sUNA2CIYU1Is5Iq2hr5C9qCy6azs+Z71INwMg9Ny75YRFq1O5+24gcMbZHr23e/DLtsM7Eb9Iuy8uVDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T08:39:31.376476Z"},"content_sha256":"ef63562620130cacb0a03348765fe1677faee884a376d455be4dba3179c7b177","schema_version":"1.0","event_id":"sha256:ef63562620130cacb0a03348765fe1677faee884a376d455be4dba3179c7b177"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:6HR23DXXZ4XZKWIP6F5LINUGIH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Microscopic field theories of the quantum skyrmion Hall effect","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el","math-ph","math.MP","quant-ph"],"primary_cat":"hep-th","authors_text":"Archi Banerjee, Ashley M. Cook, Vinay Patil","submitted_at":"2025-08-22T17:12:18Z","abstract_excerpt":"We construct effective field theories of the quantum skyrmion Hall effect from matrix Chern-Simons theory for $N$ electrons, corresponding to matrix dimension $N$. We first consider a quantum Hall droplet within finite $N$ matrix Chern-Simons theory. Taking into account the differential geometry of the matrix Chern-Simons droplet for a partially-filled fuzzy two-sphere, we first generalize the quantization procedure by replacing the Poisson bracket, a classical Lie derivative, with a quantum counterpart, the Lie derivative for a deformed fuzzy sphere. This yields the topological invariant intr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.16547","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/2508.16547/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":"2026-07-05T11:57:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BREZvxFvDHKzP3qws0B+J9vR1rzVUS5WFb4T3LfJShFi10O0NCSDrrBNCQ77b5qmWCxlJhwjL3wm+GWBBqqdCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T08:39:31.377287Z"},"content_sha256":"da40e06ce6d3411ade675e761f7bbac144857d2728cd27f923fd3df4fe846999","schema_version":"1.0","event_id":"sha256:da40e06ce6d3411ade675e761f7bbac144857d2728cd27f923fd3df4fe846999"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6HR23DXXZ4XZKWIP6F5LINUGIH/bundle.json","state_url":"https://pith.science/pith/6HR23DXXZ4XZKWIP6F5LINUGIH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6HR23DXXZ4XZKWIP6F5LINUGIH/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":"2026-08-12T08:39:31Z","links":{"resolver":"https://pith.science/pith/6HR23DXXZ4XZKWIP6F5LINUGIH","bundle":"https://pith.science/pith/6HR23DXXZ4XZKWIP6F5LINUGIH/bundle.json","state":"https://pith.science/pith/6HR23DXXZ4XZKWIP6F5LINUGIH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6HR23DXXZ4XZKWIP6F5LINUGIH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:6HR23DXXZ4XZKWIP6F5LINUGIH","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":"f4c0eafefae2b835710e4671a6f0fa0a727970fa06c3f3857204c3df28f5a927","cross_cats_sorted":["cond-mat.str-el","math-ph","math.MP","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-08-22T17:12:18Z","title_canon_sha256":"bef9507f8f4f7932f449ec67bfea311cf07cf7c4ee7e4e8b4cc79e22a0340cbd"},"schema_version":"1.0","source":{"id":"2508.16547","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2508.16547","created_at":"2026-07-05T11:57:50Z"},{"alias_kind":"arxiv_version","alias_value":"2508.16547v1","created_at":"2026-07-05T11:57:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.16547","created_at":"2026-07-05T11:57:50Z"},{"alias_kind":"pith_short_12","alias_value":"6HR23DXXZ4XZ","created_at":"2026-07-05T11:57:50Z"},{"alias_kind":"pith_short_16","alias_value":"6HR23DXXZ4XZKWIP","created_at":"2026-07-05T11:57:50Z"},{"alias_kind":"pith_short_8","alias_value":"6HR23DXX","created_at":"2026-07-05T11:57:50Z"}],"graph_snapshots":[{"event_id":"sha256:da40e06ce6d3411ade675e761f7bbac144857d2728cd27f923fd3df4fe846999","target":"graph","created_at":"2026-07-05T11:57:50Z","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/2508.16547/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We construct effective field theories of the quantum skyrmion Hall effect from matrix Chern-Simons theory for $N$ electrons, corresponding to matrix dimension $N$. We first consider a quantum Hall droplet within finite $N$ matrix Chern-Simons theory. Taking into account the differential geometry of the matrix Chern-Simons droplet for a partially-filled fuzzy two-sphere, we first generalize the quantization procedure by replacing the Poisson bracket, a classical Lie derivative, with a quantum counterpart, the Lie derivative for a deformed fuzzy sphere. This yields the topological invariant intr","authors_text":"Archi Banerjee, Ashley M. Cook, Vinay Patil","cross_cats":["cond-mat.str-el","math-ph","math.MP","quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-08-22T17:12:18Z","title":"Microscopic field theories of the quantum skyrmion Hall effect"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.16547","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:ef63562620130cacb0a03348765fe1677faee884a376d455be4dba3179c7b177","target":"record","created_at":"2026-07-05T11:57:50Z","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":"f4c0eafefae2b835710e4671a6f0fa0a727970fa06c3f3857204c3df28f5a927","cross_cats_sorted":["cond-mat.str-el","math-ph","math.MP","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-08-22T17:12:18Z","title_canon_sha256":"bef9507f8f4f7932f449ec67bfea311cf07cf7c4ee7e4e8b4cc79e22a0340cbd"},"schema_version":"1.0","source":{"id":"2508.16547","kind":"arxiv","version":1}},"canonical_sha256":"f1e3ad8ef7cf2f95590ff17ab4368641c0fb1039cd86f95ab408908ab18fa151","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f1e3ad8ef7cf2f95590ff17ab4368641c0fb1039cd86f95ab408908ab18fa151","first_computed_at":"2026-07-05T11:57:50.557796Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:57:50.557796Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"sMaUKPe8f1V2Fh2g4wex+omtbMgjinHFF9Zhve8dB8i0la2gQOK+NZ2KkNTZoBet8nabqPDYDIR/bHsQXRYKCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T11:57:50.558285Z","signed_message":"canonical_sha256_bytes"},"source_id":"2508.16547","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ef63562620130cacb0a03348765fe1677faee884a376d455be4dba3179c7b177","sha256:da40e06ce6d3411ade675e761f7bbac144857d2728cd27f923fd3df4fe846999"],"state_sha256":"49ed1527c99b1b7f9d15f6dfa46e63854011d13dcc2a4559af7ba941da55242c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6IQ+9rV6VYAGgEg2S92hyeBIZtcI8YF5WD5m6bCxPbBMNNoxZCZDAgQH18rBuZrJmuSO7MoWAI4pDFBmtoP8Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-12T08:39:31.384400Z","bundle_sha256":"b330f391a5924210fb9047e4b8867359f8e3a247321a21f8845f5a5b3a17d06f"}}