{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:XL6ZQU5IFBMUK7YBSIT64MHJEF","short_pith_number":"pith:XL6ZQU5I","canonical_record":{"source":{"id":"2411.13436","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-11-20T16:22:14Z","cross_cats_sorted":[],"title_canon_sha256":"562edbe076be3eb4b414818d888e70679c0065050678701ad9a35f78e6be988c","abstract_canon_sha256":"c57f896385a7da6cff4cfa964d0d4816b429366b5f798a19137c01b741a6ff45"},"schema_version":"1.0"},"canonical_sha256":"bafd9853a82859457f019227ee30e92164258a687d6fef0d5f67d7fffcf38e96","source":{"kind":"arxiv","id":"2411.13436","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.13436","created_at":"2026-07-05T10:22:10Z"},{"alias_kind":"arxiv_version","alias_value":"2411.13436v2","created_at":"2026-07-05T10:22:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.13436","created_at":"2026-07-05T10:22:10Z"},{"alias_kind":"pith_short_12","alias_value":"XL6ZQU5IFBMU","created_at":"2026-07-05T10:22:10Z"},{"alias_kind":"pith_short_16","alias_value":"XL6ZQU5IFBMUK7YB","created_at":"2026-07-05T10:22:10Z"},{"alias_kind":"pith_short_8","alias_value":"XL6ZQU5I","created_at":"2026-07-05T10:22:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:XL6ZQU5IFBMUK7YBSIT64MHJEF","target":"record","payload":{"canonical_record":{"source":{"id":"2411.13436","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-11-20T16:22:14Z","cross_cats_sorted":[],"title_canon_sha256":"562edbe076be3eb4b414818d888e70679c0065050678701ad9a35f78e6be988c","abstract_canon_sha256":"c57f896385a7da6cff4cfa964d0d4816b429366b5f798a19137c01b741a6ff45"},"schema_version":"1.0"},"canonical_sha256":"bafd9853a82859457f019227ee30e92164258a687d6fef0d5f67d7fffcf38e96","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:22:10.134505Z","signature_b64":"S/hzvIoj/b99ZP41SCfOit2Yg6aI5PGcR27vphN6YWkppCDlPqRJ0KJZX7unocXphuV+f9wH2J4DzVzYviKTBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bafd9853a82859457f019227ee30e92164258a687d6fef0d5f67d7fffcf38e96","last_reissued_at":"2026-07-05T10:22:10.133940Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:22:10.133940Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2411.13436","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":"2026-07-05T10:22:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SzFQk8eEl3se8tQiiCzuRnLBcNDjXVVBZAw1KO1TuCF/Xm7RJl19FDiMvJEaTR2X75fczQ0wnh4ShiN5h7ZfDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-18T05:16:32.767331Z"},"content_sha256":"a6e03b30f3605c98c808d784babcb92ec50fe3eb07d423541f3c22663589e1ce","schema_version":"1.0","event_id":"sha256:a6e03b30f3605c98c808d784babcb92ec50fe3eb07d423541f3c22663589e1ce"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:XL6ZQU5IFBMUK7YBSIT64MHJEF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On Emergent Directions in Weakly Coupled, Large N$_c$ $\\mathcal{N}=1$ SYM","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Aditya Dhumuntarao, Baiyang Zhang","submitted_at":"2024-11-20T16:22:14Z","abstract_excerpt":"The $SU(N)$ Yang-Mills theory compactified on $\\mathbb{R}^3 \\times S^1_L$ with small $L$ has many merits, for example the long range effective theory is weakly coupled and adopts rich topological structures, making it semi-classically solvable. Due to the $SU(N) \\to U(1)^{N-1}$ symmetry breaking by gauge holonomy, the low-energy effective theory can be described in terms of unbroken $U(1)$ photons and gauge holonomy. With the addition of $N_f$ adjoint light fermions, the center symmetry breaking phase transition can be studied using the twisted partition function, i.e., fermions with periodic "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.13436","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2411.13436/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":"2026-07-05T10:22:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"44MvZBq0/2tNFuf31xdAxSvJSiIZLhVvqXvCr+PEwA/Is0TDLYj8ja5zFVSU0A3ZHZE1MjOYUSXhbylO71vPBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-18T05:16:32.767865Z"},"content_sha256":"fe699b829b2de536cb5690d7e6af97eade5eb6d059af876f903732d034d99352","schema_version":"1.0","event_id":"sha256:fe699b829b2de536cb5690d7e6af97eade5eb6d059af876f903732d034d99352"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XL6ZQU5IFBMUK7YBSIT64MHJEF/bundle.json","state_url":"https://pith.science/pith/XL6ZQU5IFBMUK7YBSIT64MHJEF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XL6ZQU5IFBMUK7YBSIT64MHJEF/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":"2026-08-18T05:16:32Z","links":{"resolver":"https://pith.science/pith/XL6ZQU5IFBMUK7YBSIT64MHJEF","bundle":"https://pith.science/pith/XL6ZQU5IFBMUK7YBSIT64MHJEF/bundle.json","state":"https://pith.science/pith/XL6ZQU5IFBMUK7YBSIT64MHJEF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XL6ZQU5IFBMUK7YBSIT64MHJEF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:XL6ZQU5IFBMUK7YBSIT64MHJEF","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":"c57f896385a7da6cff4cfa964d0d4816b429366b5f798a19137c01b741a6ff45","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-11-20T16:22:14Z","title_canon_sha256":"562edbe076be3eb4b414818d888e70679c0065050678701ad9a35f78e6be988c"},"schema_version":"1.0","source":{"id":"2411.13436","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.13436","created_at":"2026-07-05T10:22:10Z"},{"alias_kind":"arxiv_version","alias_value":"2411.13436v2","created_at":"2026-07-05T10:22:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.13436","created_at":"2026-07-05T10:22:10Z"},{"alias_kind":"pith_short_12","alias_value":"XL6ZQU5IFBMU","created_at":"2026-07-05T10:22:10Z"},{"alias_kind":"pith_short_16","alias_value":"XL6ZQU5IFBMUK7YB","created_at":"2026-07-05T10:22:10Z"},{"alias_kind":"pith_short_8","alias_value":"XL6ZQU5I","created_at":"2026-07-05T10:22:10Z"}],"graph_snapshots":[{"event_id":"sha256:fe699b829b2de536cb5690d7e6af97eade5eb6d059af876f903732d034d99352","target":"graph","created_at":"2026-07-05T10:22:10Z","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/2411.13436/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The $SU(N)$ Yang-Mills theory compactified on $\\mathbb{R}^3 \\times S^1_L$ with small $L$ has many merits, for example the long range effective theory is weakly coupled and adopts rich topological structures, making it semi-classically solvable. Due to the $SU(N) \\to U(1)^{N-1}$ symmetry breaking by gauge holonomy, the low-energy effective theory can be described in terms of unbroken $U(1)$ photons and gauge holonomy. With the addition of $N_f$ adjoint light fermions, the center symmetry breaking phase transition can be studied using the twisted partition function, i.e., fermions with periodic ","authors_text":"Aditya Dhumuntarao, Baiyang Zhang","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-11-20T16:22:14Z","title":"On Emergent Directions in Weakly Coupled, Large N$_c$ $\\mathcal{N}=1$ SYM"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.13436","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:a6e03b30f3605c98c808d784babcb92ec50fe3eb07d423541f3c22663589e1ce","target":"record","created_at":"2026-07-05T10:22:10Z","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":"c57f896385a7da6cff4cfa964d0d4816b429366b5f798a19137c01b741a6ff45","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-11-20T16:22:14Z","title_canon_sha256":"562edbe076be3eb4b414818d888e70679c0065050678701ad9a35f78e6be988c"},"schema_version":"1.0","source":{"id":"2411.13436","kind":"arxiv","version":2}},"canonical_sha256":"bafd9853a82859457f019227ee30e92164258a687d6fef0d5f67d7fffcf38e96","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bafd9853a82859457f019227ee30e92164258a687d6fef0d5f67d7fffcf38e96","first_computed_at":"2026-07-05T10:22:10.133940Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:22:10.133940Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"S/hzvIoj/b99ZP41SCfOit2Yg6aI5PGcR27vphN6YWkppCDlPqRJ0KJZX7unocXphuV+f9wH2J4DzVzYviKTBQ==","signature_status":"signed_v1","signed_at":"2026-07-05T10:22:10.134505Z","signed_message":"canonical_sha256_bytes"},"source_id":"2411.13436","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a6e03b30f3605c98c808d784babcb92ec50fe3eb07d423541f3c22663589e1ce","sha256:fe699b829b2de536cb5690d7e6af97eade5eb6d059af876f903732d034d99352"],"state_sha256":"1240aaa17ff1b9f33a3c491245976a3a2a49dff624d54b88b83c390c2732629e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oBHrf5djnlOjEBanDgtvsHf3M32Mv08uMa1+uETuGDCbY5oIbYbBZoJN+D9+X87xBMGdk8ch+gdmfeoeGZ2+Aw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-18T05:16:32.773627Z","bundle_sha256":"792e1740f0227862c532ef2f45893436e11ad4395013b59ca6e8faee594b274e"}}