{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:GY2R3N46ESBSMQHZX5IC3EYQJ5","short_pith_number":"pith:GY2R3N46","canonical_record":{"source":{"id":"1406.2727","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-06-10T21:33:04Z","cross_cats_sorted":[],"title_canon_sha256":"cd2b54099147dd4202c7ca40fccd59b0565d363f3d5638dd1f62670bc9186281","abstract_canon_sha256":"5c7072049c2a73f0d09fb3e71441f2ab2d36b43d0970cb94e213773abe332673"},"schema_version":"1.0"},"canonical_sha256":"36351db79e24832640f9bf502d93104f6d7db1914f2481bbb46d35b503fd0fb6","source":{"kind":"arxiv","id":"1406.2727","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1406.2727","created_at":"2026-05-18T01:42:58Z"},{"alias_kind":"arxiv_version","alias_value":"1406.2727v1","created_at":"2026-05-18T01:42:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.2727","created_at":"2026-05-18T01:42:58Z"},{"alias_kind":"pith_short_12","alias_value":"GY2R3N46ESBS","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_16","alias_value":"GY2R3N46ESBSMQHZ","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_8","alias_value":"GY2R3N46","created_at":"2026-05-18T12:28:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:GY2R3N46ESBSMQHZX5IC3EYQJ5","target":"record","payload":{"canonical_record":{"source":{"id":"1406.2727","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-06-10T21:33:04Z","cross_cats_sorted":[],"title_canon_sha256":"cd2b54099147dd4202c7ca40fccd59b0565d363f3d5638dd1f62670bc9186281","abstract_canon_sha256":"5c7072049c2a73f0d09fb3e71441f2ab2d36b43d0970cb94e213773abe332673"},"schema_version":"1.0"},"canonical_sha256":"36351db79e24832640f9bf502d93104f6d7db1914f2481bbb46d35b503fd0fb6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:42:58.674125Z","signature_b64":"IaaHHOq3UaGe/rH3DP3WeyiR3vXDstcJJQCCK3eJ1uaMJCiszVTzKPqLO+dn3e1JM1e6iuYqwh1VZYhIYV06CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"36351db79e24832640f9bf502d93104f6d7db1914f2481bbb46d35b503fd0fb6","last_reissued_at":"2026-05-18T01:42:58.673389Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:42:58.673389Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1406.2727","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":"2026-05-18T01:42:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6os0a1xx9c7fvULtN+/pw8D6Iq8c080fxyCUFlOsaw7enh/B3jctg1JEsbtFZt7/WEMphfdm+DJDWrDTBmPCBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T06:45:14.490880Z"},"content_sha256":"15406f4474f8b18124b11f4418aa56cd22315b88a04034647f22995db50e15c9","schema_version":"1.0","event_id":"sha256:15406f4474f8b18124b11f4418aa56cd22315b88a04034647f22995db50e15c9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:GY2R3N46ESBSMQHZX5IC3EYQJ5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Topological self-dual vacua of deformed gauge theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Julio Oliva, Mauricio Valenzuela","submitted_at":"2014-06-10T21:33:04Z","abstract_excerpt":"We propose a deformation principle of gauge theories in three dimensions that can describe topologically stable self-dual gauge fields, i.e., vacua configurations that in spite of their masses do not deform the background geometry and are locally undetected by charged particles. We interpret these systems as describing boundary degrees of freedom of a self-dual Yang-Mills field in $2+2$ dimensions with mixed boundary conditions. Some of these fields correspond to Abrikosov-like vortices with an exponential damping in the direction penetrating into the bulk. We also propose generalizations of t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.2727","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":""},"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":"2026-05-18T01:42:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NXbNLk+rRKBYCupDpd8f3KhqdSIBYxyPuTpCMct3g3qHkhhE3VRDNI9o/FKzLmspCXVZiYYiIzNXsN9GNtlWCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T06:45:14.491225Z"},"content_sha256":"4a5345e1130cf5c7d877db21b23c55f21c332963f1f0f662a5abffce38f95820","schema_version":"1.0","event_id":"sha256:4a5345e1130cf5c7d877db21b23c55f21c332963f1f0f662a5abffce38f95820"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GY2R3N46ESBSMQHZX5IC3EYQJ5/bundle.json","state_url":"https://pith.science/pith/GY2R3N46ESBSMQHZX5IC3EYQJ5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GY2R3N46ESBSMQHZX5IC3EYQJ5/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":"2026-06-25T06:45:14Z","links":{"resolver":"https://pith.science/pith/GY2R3N46ESBSMQHZX5IC3EYQJ5","bundle":"https://pith.science/pith/GY2R3N46ESBSMQHZX5IC3EYQJ5/bundle.json","state":"https://pith.science/pith/GY2R3N46ESBSMQHZX5IC3EYQJ5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GY2R3N46ESBSMQHZX5IC3EYQJ5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:GY2R3N46ESBSMQHZX5IC3EYQJ5","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":"5c7072049c2a73f0d09fb3e71441f2ab2d36b43d0970cb94e213773abe332673","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-06-10T21:33:04Z","title_canon_sha256":"cd2b54099147dd4202c7ca40fccd59b0565d363f3d5638dd1f62670bc9186281"},"schema_version":"1.0","source":{"id":"1406.2727","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1406.2727","created_at":"2026-05-18T01:42:58Z"},{"alias_kind":"arxiv_version","alias_value":"1406.2727v1","created_at":"2026-05-18T01:42:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.2727","created_at":"2026-05-18T01:42:58Z"},{"alias_kind":"pith_short_12","alias_value":"GY2R3N46ESBS","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_16","alias_value":"GY2R3N46ESBSMQHZ","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_8","alias_value":"GY2R3N46","created_at":"2026-05-18T12:28:30Z"}],"graph_snapshots":[{"event_id":"sha256:4a5345e1130cf5c7d877db21b23c55f21c332963f1f0f662a5abffce38f95820","target":"graph","created_at":"2026-05-18T01:42:58Z","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":"We propose a deformation principle of gauge theories in three dimensions that can describe topologically stable self-dual gauge fields, i.e., vacua configurations that in spite of their masses do not deform the background geometry and are locally undetected by charged particles. We interpret these systems as describing boundary degrees of freedom of a self-dual Yang-Mills field in $2+2$ dimensions with mixed boundary conditions. Some of these fields correspond to Abrikosov-like vortices with an exponential damping in the direction penetrating into the bulk. We also propose generalizations of t","authors_text":"Julio Oliva, Mauricio Valenzuela","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-06-10T21:33:04Z","title":"Topological self-dual vacua of deformed gauge theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.2727","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":"sha256:15406f4474f8b18124b11f4418aa56cd22315b88a04034647f22995db50e15c9","target":"record","created_at":"2026-05-18T01:42:58Z","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":"5c7072049c2a73f0d09fb3e71441f2ab2d36b43d0970cb94e213773abe332673","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-06-10T21:33:04Z","title_canon_sha256":"cd2b54099147dd4202c7ca40fccd59b0565d363f3d5638dd1f62670bc9186281"},"schema_version":"1.0","source":{"id":"1406.2727","kind":"arxiv","version":1}},"canonical_sha256":"36351db79e24832640f9bf502d93104f6d7db1914f2481bbb46d35b503fd0fb6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"36351db79e24832640f9bf502d93104f6d7db1914f2481bbb46d35b503fd0fb6","first_computed_at":"2026-05-18T01:42:58.673389Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:42:58.673389Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IaaHHOq3UaGe/rH3DP3WeyiR3vXDstcJJQCCK3eJ1uaMJCiszVTzKPqLO+dn3e1JM1e6iuYqwh1VZYhIYV06CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:42:58.674125Z","signed_message":"canonical_sha256_bytes"},"source_id":"1406.2727","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:15406f4474f8b18124b11f4418aa56cd22315b88a04034647f22995db50e15c9","sha256:4a5345e1130cf5c7d877db21b23c55f21c332963f1f0f662a5abffce38f95820"],"state_sha256":"f7517273abdef19fd5adf5619e1fe514c4ec2ebd0150461b834ce385efa2d9fe"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rA6aB3vmq6jCrQx+5Xuz514D9VcNyKuPcZfdMP3oKtf8J92EA0oxzwdcGpTA4VbjO+YOg67dL033MWTHpnucCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-25T06:45:14.493175Z","bundle_sha256":"18fdc823ff730134b6fbbbae884fd09315183dc36490815d7eabb0d082b9a8e5"}}