{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:EFXSD66EVT3XAR2PE7DLZYWGFU","short_pith_number":"pith:EFXSD66E","schema_version":"1.0","canonical_sha256":"216f21fbc4acf770474f27c6bce2c62d2b236bed97013a196d97abdfed7f5545","source":{"kind":"arxiv","id":"2210.13482","version":3},"attestation_state":"computed","paper":{"title":"Uncovering conformal symmetry in the $3D$ Ising transition: State-operator correspondence from a fuzzy sphere regularization","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-lat","hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Chao Han, Emilie Huffman, Johannes S. Hofmann, Wei Zhu, Yin-Chen He","submitted_at":"2022-10-24T18:00:02Z","abstract_excerpt":"The $3D$ Ising transition, the most celebrated and unsolved critical phenomenon in nature, has long been conjectured to have emergent conformal symmetry, similar to the case of the $2D$ Ising transition. Yet, the emergence of conformal invariance in the $3D$ Ising transition has rarely been explored directly, mainly due to unavoidable mathematical or conceptual obstructions. Here, we design an innovative way to study the quantum version of the $3D$ Ising phase transition on spherical geometry, using the \"fuzzy (non-commutative) sphere\" regularization. We accurately calculate and analyze the en"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2210.13482","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2022-10-24T18:00:02Z","cross_cats_sorted":["cond-mat.str-el","hep-lat","hep-th"],"title_canon_sha256":"d3a82863c675156bf3349ab387e547d6b4a39957b00a2edb9e493cde8359e999","abstract_canon_sha256":"3b3c4f2b166c95b9da7fe0c0789444ffd375844fa54f421ca69b127186f30813"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:06:20.834572Z","signature_b64":"qwtlgTJIk2hFYso6mGPeyYRA8+QGZjXLqNian+yrDz3RVhXAgcmCsBusOXfa5EJvGw3pWGGx+4JKFu6kRuK7Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"216f21fbc4acf770474f27c6bce2c62d2b236bed97013a196d97abdfed7f5545","last_reissued_at":"2026-07-05T07:06:20.834065Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:06:20.834065Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Uncovering conformal symmetry in the $3D$ Ising transition: State-operator correspondence from a fuzzy sphere regularization","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-lat","hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Chao Han, Emilie Huffman, Johannes S. Hofmann, Wei Zhu, Yin-Chen He","submitted_at":"2022-10-24T18:00:02Z","abstract_excerpt":"The $3D$ Ising transition, the most celebrated and unsolved critical phenomenon in nature, has long been conjectured to have emergent conformal symmetry, similar to the case of the $2D$ Ising transition. Yet, the emergence of conformal invariance in the $3D$ Ising transition has rarely been explored directly, mainly due to unavoidable mathematical or conceptual obstructions. Here, we design an innovative way to study the quantum version of the $3D$ Ising phase transition on spherical geometry, using the \"fuzzy (non-commutative) sphere\" regularization. We accurately calculate and analyze the en"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.13482","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2210.13482/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2210.13482","created_at":"2026-07-05T07:06:20.834131+00:00"},{"alias_kind":"arxiv_version","alias_value":"2210.13482v3","created_at":"2026-07-05T07:06:20.834131+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.13482","created_at":"2026-07-05T07:06:20.834131+00:00"},{"alias_kind":"pith_short_12","alias_value":"EFXSD66EVT3X","created_at":"2026-07-05T07:06:20.834131+00:00"},{"alias_kind":"pith_short_16","alias_value":"EFXSD66EVT3XAR2P","created_at":"2026-07-05T07:06:20.834131+00:00"},{"alias_kind":"pith_short_8","alias_value":"EFXSD66E","created_at":"2026-07-05T07:06:20.834131+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":14,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.19732","citing_title":"Quantum models with the Yang-Lee phase transition","ref_index":17,"is_internal_anchor":false},{"citing_arxiv_id":"2606.17167","citing_title":"Thermal One-point Functions and Asymptotic CFT Data: QFT in AdS","ref_index":44,"is_internal_anchor":false},{"citing_arxiv_id":"2606.12540","citing_title":"Toward Entanglement Bootstrap for Conformal Field Theory in Any Dimension","ref_index":65,"is_internal_anchor":false},{"citing_arxiv_id":"2606.11317","citing_title":"Lectures on Semiclassical Methods for Composite Operators","ref_index":35,"is_internal_anchor":false},{"citing_arxiv_id":"2606.09985","citing_title":"Bootstrap Cone of the Multicritical Deconfined Quantum Critical Point","ref_index":57,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06773","citing_title":"Direct Experimental Test of Conformal Invariance via Grazing Scattering: A Proposal for X-ray and Neutron Experiments","ref_index":16,"is_internal_anchor":false},{"citing_arxiv_id":"2604.24840","citing_title":"Quantum Rotors on the Fuzzy Sphere and the Cubic CFT","ref_index":3,"is_internal_anchor":false},{"citing_arxiv_id":"2605.00979","citing_title":"Universality of Quantum Gates in Particle and Symmetry Constrained Subspaces","ref_index":7,"is_internal_anchor":false},{"citing_arxiv_id":"2604.18686","citing_title":"Neural Spectral Bias and Conformal Correlators I: Introduction and Applications","ref_index":50,"is_internal_anchor":false},{"citing_arxiv_id":"2604.18673","citing_title":"Neural Networks Reveal a Universal Bias in Conformal Correlators","ref_index":35,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07554","citing_title":"Fortuitous Universality of Bose-Kondo Impurities","ref_index":30,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06773","citing_title":"Direct Experimental Test of Conformal Invariance via Grazing Scattering: A Proposal for X-ray and Neutron Experiments","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2604.14741","citing_title":"The OPE Approach to Renormalization: Operator Mixing","ref_index":40,"is_internal_anchor":false},{"citing_arxiv_id":"2604.18705","citing_title":"Conformal Data for the $O(2)$ Wilson-Fisher CFT in $(2+1)$-Dimensional Spacetime from Exact Diagonalization and Matrix Product States on the Fuzzy Sphere","ref_index":14,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EFXSD66EVT3XAR2PE7DLZYWGFU","json":"https://pith.science/pith/EFXSD66EVT3XAR2PE7DLZYWGFU.json","graph_json":"https://pith.science/api/pith-number/EFXSD66EVT3XAR2PE7DLZYWGFU/graph.json","events_json":"https://pith.science/api/pith-number/EFXSD66EVT3XAR2PE7DLZYWGFU/events.json","paper":"https://pith.science/paper/EFXSD66E"},"agent_actions":{"view_html":"https://pith.science/pith/EFXSD66EVT3XAR2PE7DLZYWGFU","download_json":"https://pith.science/pith/EFXSD66EVT3XAR2PE7DLZYWGFU.json","view_paper":"https://pith.science/paper/EFXSD66E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2210.13482&json=true","fetch_graph":"https://pith.science/api/pith-number/EFXSD66EVT3XAR2PE7DLZYWGFU/graph.json","fetch_events":"https://pith.science/api/pith-number/EFXSD66EVT3XAR2PE7DLZYWGFU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EFXSD66EVT3XAR2PE7DLZYWGFU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EFXSD66EVT3XAR2PE7DLZYWGFU/action/storage_attestation","attest_author":"https://pith.science/pith/EFXSD66EVT3XAR2PE7DLZYWGFU/action/author_attestation","sign_citation":"https://pith.science/pith/EFXSD66EVT3XAR2PE7DLZYWGFU/action/citation_signature","submit_replication":"https://pith.science/pith/EFXSD66EVT3XAR2PE7DLZYWGFU/action/replication_record"}},"created_at":"2026-07-05T07:06:20.834131+00:00","updated_at":"2026-07-05T07:06:20.834131+00:00"}