{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1993:BZB5X7TNWHSVMWVQCTSO5ALPPQ","short_pith_number":"pith:BZB5X7TN","canonical_record":{"source":{"id":"hep-th/9305056","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1993-05-13T09:39:19Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"580958930985eb6f3f8c29ec1f48a3e070408b35d41382f8d602540f437b9b58","abstract_canon_sha256":"68a12bd15364d60089a582bc4f03ea05bd5a98255b2a4ccd7a3774c2f217c2dc"},"schema_version":"1.0"},"canonical_sha256":"0e43dbfe6db1e5565ab014e4ee816f7c34d94f8ef357ca0544011936d42c7b48","source":{"kind":"arxiv","id":"hep-th/9305056","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9305056","created_at":"2026-05-18T02:36:04Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9305056v1","created_at":"2026-05-18T02:36:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9305056","created_at":"2026-05-18T02:36:04Z"},{"alias_kind":"pith_short_12","alias_value":"BZB5X7TNWHSV","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"BZB5X7TNWHSVMWVQ","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"BZB5X7TN","created_at":"2026-05-18T12:25:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1993:BZB5X7TNWHSVMWVQCTSO5ALPPQ","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9305056","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1993-05-13T09:39:19Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"580958930985eb6f3f8c29ec1f48a3e070408b35d41382f8d602540f437b9b58","abstract_canon_sha256":"68a12bd15364d60089a582bc4f03ea05bd5a98255b2a4ccd7a3774c2f217c2dc"},"schema_version":"1.0"},"canonical_sha256":"0e43dbfe6db1e5565ab014e4ee816f7c34d94f8ef357ca0544011936d42c7b48","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:04.670272Z","signature_b64":"yJse/1Wp6IazcMh/nYl8siWYlxZAc7LolDCYGd5MPfB/4JmhWNsGLq6EUGHOxq8alWBuuMpwGqIqcyIWdFvFDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0e43dbfe6db1e5565ab014e4ee816f7c34d94f8ef357ca0544011936d42c7b48","last_reissued_at":"2026-05-18T02:36:04.669710Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:04.669710Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9305056","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":"2026-05-18T02:36:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1MxwYZ52ucRcG+8AdUG2rur5H9AC6Wrf5XehjAnjqTXG1kDLlfiPhNMFgGnFyW7iuom//fK2tBpS958W7BKaBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T22:27:21.507633Z"},"content_sha256":"22b057275a3e3e2ca68a08727e08a534163c7b89dd2b43f3ac26a73e1ce146b9","schema_version":"1.0","event_id":"sha256:22b057275a3e3e2ca68a08727e08a534163c7b89dd2b43f3ac26a73e1ce146b9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1993:BZB5X7TNWHSVMWVQCTSO5ALPPQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Body Fixed Frame, Rigid Gauge Rotations and Large N Random Fields in QCD","license":"","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"Shimon Levit","submitted_at":"1993-05-13T09:39:19Z","abstract_excerpt":"The \"body fixed frame\" with respect to local gauge transformations is introduced. Rigid gauge \"rotations\" in QCD and their \\Sch equation are studied for static and dynamic quarks. Possible choices of the rigid gauge field configuration corresponding to a nonvanishing static colormagnetic field in the \"body fixed\" frame are discussed. A gauge invariant variational equation is derived in this frame. For large number N of colors the rigid gauge field configuration is regarded as random with maximally random probability distribution under constraints on macroscopic--like quantities. For the unifor"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9305056","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":"2026-05-18T02:36:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VLvDIzd2d5VLGQ27RY6vQz9y9LpSApjIjFrQoukjPCyI2rLFLIzgCK8zn+yCb8X+yEDYYcpA0fxcy6c/b3x4Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T22:27:21.507993Z"},"content_sha256":"c8fc9e13c99716773731ca7be637e5cc2b1fee917ce9533af02b43937d497417","schema_version":"1.0","event_id":"sha256:c8fc9e13c99716773731ca7be637e5cc2b1fee917ce9533af02b43937d497417"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BZB5X7TNWHSVMWVQCTSO5ALPPQ/bundle.json","state_url":"https://pith.science/pith/BZB5X7TNWHSVMWVQCTSO5ALPPQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BZB5X7TNWHSVMWVQCTSO5ALPPQ/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":"2026-05-31T22:27:21Z","links":{"resolver":"https://pith.science/pith/BZB5X7TNWHSVMWVQCTSO5ALPPQ","bundle":"https://pith.science/pith/BZB5X7TNWHSVMWVQCTSO5ALPPQ/bundle.json","state":"https://pith.science/pith/BZB5X7TNWHSVMWVQCTSO5ALPPQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BZB5X7TNWHSVMWVQCTSO5ALPPQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1993:BZB5X7TNWHSVMWVQCTSO5ALPPQ","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":"68a12bd15364d60089a582bc4f03ea05bd5a98255b2a4ccd7a3774c2f217c2dc","cross_cats_sorted":["hep-ph","nucl-th"],"license":"","primary_cat":"hep-th","submitted_at":"1993-05-13T09:39:19Z","title_canon_sha256":"580958930985eb6f3f8c29ec1f48a3e070408b35d41382f8d602540f437b9b58"},"schema_version":"1.0","source":{"id":"hep-th/9305056","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9305056","created_at":"2026-05-18T02:36:04Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9305056v1","created_at":"2026-05-18T02:36:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9305056","created_at":"2026-05-18T02:36:04Z"},{"alias_kind":"pith_short_12","alias_value":"BZB5X7TNWHSV","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"BZB5X7TNWHSVMWVQ","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"BZB5X7TN","created_at":"2026-05-18T12:25:47Z"}],"graph_snapshots":[{"event_id":"sha256:c8fc9e13c99716773731ca7be637e5cc2b1fee917ce9533af02b43937d497417","target":"graph","created_at":"2026-05-18T02:36:04Z","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":"The \"body fixed frame\" with respect to local gauge transformations is introduced. Rigid gauge \"rotations\" in QCD and their \\Sch equation are studied for static and dynamic quarks. Possible choices of the rigid gauge field configuration corresponding to a nonvanishing static colormagnetic field in the \"body fixed\" frame are discussed. A gauge invariant variational equation is derived in this frame. For large number N of colors the rigid gauge field configuration is regarded as random with maximally random probability distribution under constraints on macroscopic--like quantities. For the unifor","authors_text":"Shimon Levit","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1993-05-13T09:39:19Z","title":"Body Fixed Frame, Rigid Gauge Rotations and Large N Random Fields in QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9305056","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":"sha256:22b057275a3e3e2ca68a08727e08a534163c7b89dd2b43f3ac26a73e1ce146b9","target":"record","created_at":"2026-05-18T02:36:04Z","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":"68a12bd15364d60089a582bc4f03ea05bd5a98255b2a4ccd7a3774c2f217c2dc","cross_cats_sorted":["hep-ph","nucl-th"],"license":"","primary_cat":"hep-th","submitted_at":"1993-05-13T09:39:19Z","title_canon_sha256":"580958930985eb6f3f8c29ec1f48a3e070408b35d41382f8d602540f437b9b58"},"schema_version":"1.0","source":{"id":"hep-th/9305056","kind":"arxiv","version":1}},"canonical_sha256":"0e43dbfe6db1e5565ab014e4ee816f7c34d94f8ef357ca0544011936d42c7b48","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0e43dbfe6db1e5565ab014e4ee816f7c34d94f8ef357ca0544011936d42c7b48","first_computed_at":"2026-05-18T02:36:04.669710Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:36:04.669710Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yJse/1Wp6IazcMh/nYl8siWYlxZAc7LolDCYGd5MPfB/4JmhWNsGLq6EUGHOxq8alWBuuMpwGqIqcyIWdFvFDw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:36:04.670272Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9305056","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:22b057275a3e3e2ca68a08727e08a534163c7b89dd2b43f3ac26a73e1ce146b9","sha256:c8fc9e13c99716773731ca7be637e5cc2b1fee917ce9533af02b43937d497417"],"state_sha256":"9d92565f56238ea16f441d8df8c8d7a0db85ff4d69f1804420baf73828cb097c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9faKDta4e+blg1d9Xht8XqrGqA1O1Q9KWwUt8NoPZotiNAm7Xs02tADKATK/aEvxn45fNZp4SEVT0VFMtjxcDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T22:27:21.510397Z","bundle_sha256":"726052784d91ef051115a7e956cbb9d6f1edc1ad0cfc195ac105dd65d20f0608"}}