{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:XFP45SIPF26WR5UVNWJNOS5YYS","short_pith_number":"pith:XFP45SIP","canonical_record":{"source":{"id":"1210.4284","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-10-16T07:51:59Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"22e0e738f66616f37b4e9b91845aa67d08fa47075605f73acb07c759dd946855","abstract_canon_sha256":"21994d2f1b3fdab24a7c0a90eb2b01d4976aafd16164e14e0e8122cfbc4b90ec"},"schema_version":"1.0"},"canonical_sha256":"b95fcec90f2ebd68f6956d92d74bb8c49c6b459008846ec1fa3b6bbae1878dab","source":{"kind":"arxiv","id":"1210.4284","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.4284","created_at":"2026-05-18T03:31:16Z"},{"alias_kind":"arxiv_version","alias_value":"1210.4284v2","created_at":"2026-05-18T03:31:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.4284","created_at":"2026-05-18T03:31:16Z"},{"alias_kind":"pith_short_12","alias_value":"XFP45SIPF26W","created_at":"2026-05-18T12:27:27Z"},{"alias_kind":"pith_short_16","alias_value":"XFP45SIPF26WR5UV","created_at":"2026-05-18T12:27:27Z"},{"alias_kind":"pith_short_8","alias_value":"XFP45SIP","created_at":"2026-05-18T12:27:27Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:XFP45SIPF26WR5UVNWJNOS5YYS","target":"record","payload":{"canonical_record":{"source":{"id":"1210.4284","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-10-16T07:51:59Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"22e0e738f66616f37b4e9b91845aa67d08fa47075605f73acb07c759dd946855","abstract_canon_sha256":"21994d2f1b3fdab24a7c0a90eb2b01d4976aafd16164e14e0e8122cfbc4b90ec"},"schema_version":"1.0"},"canonical_sha256":"b95fcec90f2ebd68f6956d92d74bb8c49c6b459008846ec1fa3b6bbae1878dab","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:31:16.857578Z","signature_b64":"WwYI868QwoYFUkkj0Wc7h83b606eQknkW1DNfuT9MKwNIYHy5OK89XhTTSLshrONo/15805+2k3fX3WjPn0EBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b95fcec90f2ebd68f6956d92d74bb8c49c6b459008846ec1fa3b6bbae1878dab","last_reissued_at":"2026-05-18T03:31:16.856990Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:31:16.856990Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1210.4284","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":"2026-05-18T03:31:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kNKbDEA1ycgSqZ++2UGBWZ5HufxiztlH9QhhNOJQfjhT4MccSpz5V07iW3fc5bIyPbHwVm3s6dq/MsumXuhBCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T06:31:01.545333Z"},"content_sha256":"43d080caf97c19655205b1629383a6c25a90db75fefa0f303b6d674991050a32","schema_version":"1.0","event_id":"sha256:43d080caf97c19655205b1629383a6c25a90db75fefa0f303b6d674991050a32"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:XFP45SIPF26WR5UVNWJNOS5YYS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Phase with no mass gap in non-perturbatively gauge-fixed Yang--Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"Maarten Golterman, Yigal Shamir","submitted_at":"2012-10-16T07:51:59Z","abstract_excerpt":"An equivariantly gauge-fixed non-abelian gauge theory is a theory in which a coset of the gauge group, not containing the maximal abelian subgroup, is gauge fixed. Such theories are non-perturbatively well-defined. In a finite volume, the equivariant BRST symmetry guarantees that expectation values of gauge-invariant operators are equal to their values in the unfixed theory. However, turning on a small breaking of this symmetry, and turning it off after the thermodynamic limit has been taken, can in principle reveal new phases. In this paper we use a combination of strong-coupling and mean-fie"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.4284","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":""},"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":"2026-05-18T03:31:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"t3FMATuio+46UaRqQeX1uviZgR4HwrPuT2fsh7fxsdot6TH9nJg868U6utaoHuFgPpons5RbMsn/fzTPAf/LAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T06:31:01.545971Z"},"content_sha256":"1345623d0ec4e1bdc8be7b765429ed58379ae9077dcb8710bde081025b1e71df","schema_version":"1.0","event_id":"sha256:1345623d0ec4e1bdc8be7b765429ed58379ae9077dcb8710bde081025b1e71df"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XFP45SIPF26WR5UVNWJNOS5YYS/bundle.json","state_url":"https://pith.science/pith/XFP45SIPF26WR5UVNWJNOS5YYS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XFP45SIPF26WR5UVNWJNOS5YYS/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":"2026-05-24T06:31:01Z","links":{"resolver":"https://pith.science/pith/XFP45SIPF26WR5UVNWJNOS5YYS","bundle":"https://pith.science/pith/XFP45SIPF26WR5UVNWJNOS5YYS/bundle.json","state":"https://pith.science/pith/XFP45SIPF26WR5UVNWJNOS5YYS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XFP45SIPF26WR5UVNWJNOS5YYS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:XFP45SIPF26WR5UVNWJNOS5YYS","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":"21994d2f1b3fdab24a7c0a90eb2b01d4976aafd16164e14e0e8122cfbc4b90ec","cross_cats_sorted":["hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-10-16T07:51:59Z","title_canon_sha256":"22e0e738f66616f37b4e9b91845aa67d08fa47075605f73acb07c759dd946855"},"schema_version":"1.0","source":{"id":"1210.4284","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.4284","created_at":"2026-05-18T03:31:16Z"},{"alias_kind":"arxiv_version","alias_value":"1210.4284v2","created_at":"2026-05-18T03:31:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.4284","created_at":"2026-05-18T03:31:16Z"},{"alias_kind":"pith_short_12","alias_value":"XFP45SIPF26W","created_at":"2026-05-18T12:27:27Z"},{"alias_kind":"pith_short_16","alias_value":"XFP45SIPF26WR5UV","created_at":"2026-05-18T12:27:27Z"},{"alias_kind":"pith_short_8","alias_value":"XFP45SIP","created_at":"2026-05-18T12:27:27Z"}],"graph_snapshots":[{"event_id":"sha256:1345623d0ec4e1bdc8be7b765429ed58379ae9077dcb8710bde081025b1e71df","target":"graph","created_at":"2026-05-18T03:31:16Z","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"},"paper":{"abstract_excerpt":"An equivariantly gauge-fixed non-abelian gauge theory is a theory in which a coset of the gauge group, not containing the maximal abelian subgroup, is gauge fixed. Such theories are non-perturbatively well-defined. In a finite volume, the equivariant BRST symmetry guarantees that expectation values of gauge-invariant operators are equal to their values in the unfixed theory. However, turning on a small breaking of this symmetry, and turning it off after the thermodynamic limit has been taken, can in principle reveal new phases. In this paper we use a combination of strong-coupling and mean-fie","authors_text":"Maarten Golterman, Yigal Shamir","cross_cats":["hep-ph","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-10-16T07:51:59Z","title":"Phase with no mass gap in non-perturbatively gauge-fixed Yang--Mills theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.4284","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":"sha256:43d080caf97c19655205b1629383a6c25a90db75fefa0f303b6d674991050a32","target":"record","created_at":"2026-05-18T03:31:16Z","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":"21994d2f1b3fdab24a7c0a90eb2b01d4976aafd16164e14e0e8122cfbc4b90ec","cross_cats_sorted":["hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-10-16T07:51:59Z","title_canon_sha256":"22e0e738f66616f37b4e9b91845aa67d08fa47075605f73acb07c759dd946855"},"schema_version":"1.0","source":{"id":"1210.4284","kind":"arxiv","version":2}},"canonical_sha256":"b95fcec90f2ebd68f6956d92d74bb8c49c6b459008846ec1fa3b6bbae1878dab","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b95fcec90f2ebd68f6956d92d74bb8c49c6b459008846ec1fa3b6bbae1878dab","first_computed_at":"2026-05-18T03:31:16.856990Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:31:16.856990Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"WwYI868QwoYFUkkj0Wc7h83b606eQknkW1DNfuT9MKwNIYHy5OK89XhTTSLshrONo/15805+2k3fX3WjPn0EBw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:31:16.857578Z","signed_message":"canonical_sha256_bytes"},"source_id":"1210.4284","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:43d080caf97c19655205b1629383a6c25a90db75fefa0f303b6d674991050a32","sha256:1345623d0ec4e1bdc8be7b765429ed58379ae9077dcb8710bde081025b1e71df"],"state_sha256":"aae25c15d87e4848a90a10cd8371bb6c7193fccb0b70b71a57c273563b7dfa8b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ulHqv73wuLbH7ha3fpthVgMwH/NP4zZU/Uv+guVN8G3wQ2mhCqvqxmT3zMMtKaBYOS4yI/oU8F29giE17NXYAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-24T06:31:01.549279Z","bundle_sha256":"dbd64a637b23e949986f20e0937cb44118e2b6b1c0e0c4c2faf2cb349ebed79e"}}