{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:K5VFHW4EDHUWOSTHP2RP3DTBQR","short_pith_number":"pith:K5VFHW4E","schema_version":"1.0","canonical_sha256":"576a53db8419e9674a677ea2fd8e618478b7b91ce18e0479b0f051946cc8f147","source":{"kind":"arxiv","id":"1606.01902","version":3},"attestation_state":"computed","paper":{"title":"Emergent Dimensions and Braneworlds from Large-N Confinement","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"Aleksey Cherman, Erich Poppitz","submitted_at":"2016-06-06T20:00:07Z","abstract_excerpt":"$\\mathcal{N}=1$ $SU(N)$ super-Yang-Mills theory on $\\mathbb{R}^3\\times S^1$ is believed to have a smooth dependence on the circle size $L$. Making $L$ small leads to calculable non-perturbative color confinement, mass gap, and string tensions. For finite $N$, the small-$L$ low-energy dynamics is described by a three-dimensional effective theory. The large-$N$ limit, however, reveals surprises: the infrared dual description is in terms of a theory with an emergent fourth dimension, curiously reminiscent of T-duality in string theory. Here, however, the emergent dimension is a lattice, with mome"},"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":"1606.01902","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-06-06T20:00:07Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"26698b3f4874ec0139221b548e7836cfb33ffadd2bd590295428f7840d13b509","abstract_canon_sha256":"827c5b39924d20c8cb78ca269ae778e89771cd40f9b9b4409e17c45d494fa616"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:55:13.595088Z","signature_b64":"SdY8C5+d2s0ZlZKZZzvxljns1Ob4ndo5s1DlTMT4LYhr8HprwMQ9SD9I0h/Z0jaTE0epD1qBLPR6ONv+ILRNAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"576a53db8419e9674a677ea2fd8e618478b7b91ce18e0479b0f051946cc8f147","last_reissued_at":"2026-05-18T00:55:13.594662Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:55:13.594662Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Emergent Dimensions and Braneworlds from Large-N Confinement","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"Aleksey Cherman, Erich Poppitz","submitted_at":"2016-06-06T20:00:07Z","abstract_excerpt":"$\\mathcal{N}=1$ $SU(N)$ super-Yang-Mills theory on $\\mathbb{R}^3\\times S^1$ is believed to have a smooth dependence on the circle size $L$. Making $L$ small leads to calculable non-perturbative color confinement, mass gap, and string tensions. For finite $N$, the small-$L$ low-energy dynamics is described by a three-dimensional effective theory. The large-$N$ limit, however, reveals surprises: the infrared dual description is in terms of a theory with an emergent fourth dimension, curiously reminiscent of T-duality in string theory. Here, however, the emergent dimension is a lattice, with mome"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.01902","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1606.01902","created_at":"2026-05-18T00:55:13.594721+00:00"},{"alias_kind":"arxiv_version","alias_value":"1606.01902v3","created_at":"2026-05-18T00:55:13.594721+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.01902","created_at":"2026-05-18T00:55:13.594721+00:00"},{"alias_kind":"pith_short_12","alias_value":"K5VFHW4EDHUW","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_16","alias_value":"K5VFHW4EDHUWOSTH","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_8","alias_value":"K5VFHW4E","created_at":"2026-05-18T12:30:25.849896+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/K5VFHW4EDHUWOSTHP2RP3DTBQR","json":"https://pith.science/pith/K5VFHW4EDHUWOSTHP2RP3DTBQR.json","graph_json":"https://pith.science/api/pith-number/K5VFHW4EDHUWOSTHP2RP3DTBQR/graph.json","events_json":"https://pith.science/api/pith-number/K5VFHW4EDHUWOSTHP2RP3DTBQR/events.json","paper":"https://pith.science/paper/K5VFHW4E"},"agent_actions":{"view_html":"https://pith.science/pith/K5VFHW4EDHUWOSTHP2RP3DTBQR","download_json":"https://pith.science/pith/K5VFHW4EDHUWOSTHP2RP3DTBQR.json","view_paper":"https://pith.science/paper/K5VFHW4E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1606.01902&json=true","fetch_graph":"https://pith.science/api/pith-number/K5VFHW4EDHUWOSTHP2RP3DTBQR/graph.json","fetch_events":"https://pith.science/api/pith-number/K5VFHW4EDHUWOSTHP2RP3DTBQR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K5VFHW4EDHUWOSTHP2RP3DTBQR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K5VFHW4EDHUWOSTHP2RP3DTBQR/action/storage_attestation","attest_author":"https://pith.science/pith/K5VFHW4EDHUWOSTHP2RP3DTBQR/action/author_attestation","sign_citation":"https://pith.science/pith/K5VFHW4EDHUWOSTHP2RP3DTBQR/action/citation_signature","submit_replication":"https://pith.science/pith/K5VFHW4EDHUWOSTHP2RP3DTBQR/action/replication_record"}},"created_at":"2026-05-18T00:55:13.594721+00:00","updated_at":"2026-05-18T00:55:13.594721+00:00"}