{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1998:IV2AH6MIBU2CGLD2ZXCTNTJRTK","short_pith_number":"pith:IV2AH6MI","canonical_record":{"source":{"id":"hep-lat/9806036","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1998-06-30T13:13:58Z","cross_cats_sorted":[],"title_canon_sha256":"8650ab179956744ab3246ca6bda23e496c6294e4e02c265e752e2ac5966ee401","abstract_canon_sha256":"e90cafead6d91b3a6bfa167dc029ed473dc7e6a0225906f35b115dc4186aea74"},"schema_version":"1.0"},"canonical_sha256":"457403f9880d34232c7acdc536cd319aa1619239f1c1845b35bd8baddb220861","source":{"kind":"arxiv","id":"hep-lat/9806036","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/9806036","created_at":"2026-05-18T01:08:06Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9806036v1","created_at":"2026-05-18T01:08:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9806036","created_at":"2026-05-18T01:08:06Z"},{"alias_kind":"pith_short_12","alias_value":"IV2AH6MIBU2C","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"IV2AH6MIBU2CGLD2","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"IV2AH6MI","created_at":"2026-05-18T12:25:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1998:IV2AH6MIBU2CGLD2ZXCTNTJRTK","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/9806036","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1998-06-30T13:13:58Z","cross_cats_sorted":[],"title_canon_sha256":"8650ab179956744ab3246ca6bda23e496c6294e4e02c265e752e2ac5966ee401","abstract_canon_sha256":"e90cafead6d91b3a6bfa167dc029ed473dc7e6a0225906f35b115dc4186aea74"},"schema_version":"1.0"},"canonical_sha256":"457403f9880d34232c7acdc536cd319aa1619239f1c1845b35bd8baddb220861","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:08:06.002215Z","signature_b64":"Ep+k4/ynMTYUAFxN1ZcJcCjY2q8G2WadnBLEHOK8F8Lw99hiahtUQau+15mhz+UchPebplM7TmGNPDDvakUIAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"457403f9880d34232c7acdc536cd319aa1619239f1c1845b35bd8baddb220861","last_reissued_at":"2026-05-18T01:08:06.001800Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:08:06.001800Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/9806036","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":"2026-05-18T01:08:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"10due0WkmHYkffTIMR5EHisMuVaT0Owx6dw8hq/HBgWEs5GKx/DuiuLj55GKv35nz6NMwhUJjYhWAHbCQnDMBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T02:30:12.024557Z"},"content_sha256":"e0f5075cf10b28d8b6898e12faf65a4d67f8077d52ddcc7efc5c5a7d9c0952f1","schema_version":"1.0","event_id":"sha256:e0f5075cf10b28d8b6898e12faf65a4d67f8077d52ddcc7efc5c5a7d9c0952f1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1998:IV2AH6MIBU2CGLD2ZXCTNTJRTK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Phase structure of U(1) lattice gauge theory with monopole term","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"G. Damm, W. Kerler","submitted_at":"1998-06-30T13:13:58Z","abstract_excerpt":"We investigate four-dimensional compact U(1) lattice gauge theory with a monopole term added to the Wilson action. First we consider the phase structure at negative $\\beta$, revealing some properties of a third phase region there, in particular the existence of a number of different states. Then our present studies concentrate on larger values of the monopole coupling $\\lambda$ where the confinement-Coulomb phase transition turns out to become of second order. Performing a finite-size analysis we find that the critical exponent $\\nu$ is close to, however, different from the gaussian value and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9806036","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":"2026-05-18T01:08:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"02II/btpYX2A452XTT/cAJiJ1OHmVsswzF7E7vobPXY4fxAU9x0Zg4F8QuCpQpUeieTM3Sddxg81208RWvk4BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T02:30:12.024908Z"},"content_sha256":"1669cae5d5991e362e30bb72cdc463750fd5e32bfbbcb9c726e0c207f02a7586","schema_version":"1.0","event_id":"sha256:1669cae5d5991e362e30bb72cdc463750fd5e32bfbbcb9c726e0c207f02a7586"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IV2AH6MIBU2CGLD2ZXCTNTJRTK/bundle.json","state_url":"https://pith.science/pith/IV2AH6MIBU2CGLD2ZXCTNTJRTK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IV2AH6MIBU2CGLD2ZXCTNTJRTK/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":"2026-06-03T02:30:12Z","links":{"resolver":"https://pith.science/pith/IV2AH6MIBU2CGLD2ZXCTNTJRTK","bundle":"https://pith.science/pith/IV2AH6MIBU2CGLD2ZXCTNTJRTK/bundle.json","state":"https://pith.science/pith/IV2AH6MIBU2CGLD2ZXCTNTJRTK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IV2AH6MIBU2CGLD2ZXCTNTJRTK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1998:IV2AH6MIBU2CGLD2ZXCTNTJRTK","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":"e90cafead6d91b3a6bfa167dc029ed473dc7e6a0225906f35b115dc4186aea74","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"1998-06-30T13:13:58Z","title_canon_sha256":"8650ab179956744ab3246ca6bda23e496c6294e4e02c265e752e2ac5966ee401"},"schema_version":"1.0","source":{"id":"hep-lat/9806036","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/9806036","created_at":"2026-05-18T01:08:06Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9806036v1","created_at":"2026-05-18T01:08:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9806036","created_at":"2026-05-18T01:08:06Z"},{"alias_kind":"pith_short_12","alias_value":"IV2AH6MIBU2C","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"IV2AH6MIBU2CGLD2","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"IV2AH6MI","created_at":"2026-05-18T12:25:49Z"}],"graph_snapshots":[{"event_id":"sha256:1669cae5d5991e362e30bb72cdc463750fd5e32bfbbcb9c726e0c207f02a7586","target":"graph","created_at":"2026-05-18T01:08:06Z","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 investigate four-dimensional compact U(1) lattice gauge theory with a monopole term added to the Wilson action. First we consider the phase structure at negative $\\beta$, revealing some properties of a third phase region there, in particular the existence of a number of different states. Then our present studies concentrate on larger values of the monopole coupling $\\lambda$ where the confinement-Coulomb phase transition turns out to become of second order. Performing a finite-size analysis we find that the critical exponent $\\nu$ is close to, however, different from the gaussian value and ","authors_text":"G. Damm, W. Kerler","cross_cats":[],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"1998-06-30T13:13:58Z","title":"Phase structure of U(1) lattice gauge theory with monopole term"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9806036","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:e0f5075cf10b28d8b6898e12faf65a4d67f8077d52ddcc7efc5c5a7d9c0952f1","target":"record","created_at":"2026-05-18T01:08:06Z","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":"e90cafead6d91b3a6bfa167dc029ed473dc7e6a0225906f35b115dc4186aea74","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"1998-06-30T13:13:58Z","title_canon_sha256":"8650ab179956744ab3246ca6bda23e496c6294e4e02c265e752e2ac5966ee401"},"schema_version":"1.0","source":{"id":"hep-lat/9806036","kind":"arxiv","version":1}},"canonical_sha256":"457403f9880d34232c7acdc536cd319aa1619239f1c1845b35bd8baddb220861","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"457403f9880d34232c7acdc536cd319aa1619239f1c1845b35bd8baddb220861","first_computed_at":"2026-05-18T01:08:06.001800Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:08:06.001800Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Ep+k4/ynMTYUAFxN1ZcJcCjY2q8G2WadnBLEHOK8F8Lw99hiahtUQau+15mhz+UchPebplM7TmGNPDDvakUIAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:08:06.002215Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/9806036","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e0f5075cf10b28d8b6898e12faf65a4d67f8077d52ddcc7efc5c5a7d9c0952f1","sha256:1669cae5d5991e362e30bb72cdc463750fd5e32bfbbcb9c726e0c207f02a7586"],"state_sha256":"920583d026d7b7c24b262210db2c1682e6dbfc3aa8de73d450b5528d6489e8bf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ul0wTCY7C19JmSNuhIcYNIko2JQZ2n8mcHLcF81Ad5zbF2va/Y1sJXpN0VqxpFkBZipP4Hdj9agh0KUKv7evCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T02:30:12.026886Z","bundle_sha256":"81285e743ec0eb11a6b32a5c43c180717af76841743cc6b012cd79c81e7a7f30"}}