{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:DMFF6BNBABJWNSTNEDJOXNER5I","short_pith_number":"pith:DMFF6BNB","canonical_record":{"source":{"id":"1504.02278","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-04-09T12:20:46Z","cross_cats_sorted":[],"title_canon_sha256":"86acaa54a867279ee1dfc23307c012d697ec46aebc477ad6a493e3c5e7d9bab9","abstract_canon_sha256":"294593ec5eb224b639a53da0fa4465bf0d5c5e4128bd41ddce39ffbbb90e7547"},"schema_version":"1.0"},"canonical_sha256":"1b0a5f05a1005366ca6d20d2ebb491ea0b4d99c098c505bdf4986cfe3636f07c","source":{"kind":"arxiv","id":"1504.02278","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1504.02278","created_at":"2026-05-18T01:26:31Z"},{"alias_kind":"arxiv_version","alias_value":"1504.02278v2","created_at":"2026-05-18T01:26:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.02278","created_at":"2026-05-18T01:26:31Z"},{"alias_kind":"pith_short_12","alias_value":"DMFF6BNBABJW","created_at":"2026-05-18T12:29:17Z"},{"alias_kind":"pith_short_16","alias_value":"DMFF6BNBABJWNSTN","created_at":"2026-05-18T12:29:17Z"},{"alias_kind":"pith_short_8","alias_value":"DMFF6BNB","created_at":"2026-05-18T12:29:17Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:DMFF6BNBABJWNSTNEDJOXNER5I","target":"record","payload":{"canonical_record":{"source":{"id":"1504.02278","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-04-09T12:20:46Z","cross_cats_sorted":[],"title_canon_sha256":"86acaa54a867279ee1dfc23307c012d697ec46aebc477ad6a493e3c5e7d9bab9","abstract_canon_sha256":"294593ec5eb224b639a53da0fa4465bf0d5c5e4128bd41ddce39ffbbb90e7547"},"schema_version":"1.0"},"canonical_sha256":"1b0a5f05a1005366ca6d20d2ebb491ea0b4d99c098c505bdf4986cfe3636f07c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:26:31.610085Z","signature_b64":"TCLPpK8fS9WI05YCMeksYcYCOI3qSI4sQYV8tt+nCpHwoxcEBuV5XFBNYzT7qOr6RrK5NOiJZd1tuUk01Lf2DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1b0a5f05a1005366ca6d20d2ebb491ea0b4d99c098c505bdf4986cfe3636f07c","last_reissued_at":"2026-05-18T01:26:31.609371Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:26:31.609371Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1504.02278","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":"2026-05-18T01:26:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FzNZ0Kt08hfp/e+nYyDqMpjjOu5opyoo+2lp6cFfholRzQVOyeqQcGluRvkHsct/WiwJGHyFGd/99cMmGKf+Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T13:01:34.663087Z"},"content_sha256":"6df4804ebf32efcae4e72b98ea218f55d9482bf348d5d82adb3119ce02f192f6","schema_version":"1.0","event_id":"sha256:6df4804ebf32efcae4e72b98ea218f55d9482bf348d5d82adb3119ce02f192f6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:DMFF6BNBABJWNSTNEDJOXNER5I","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Scaling dimensions of higher-charge monopoles at deconfined critical points","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"G J Sreejith, Stephen Powell","submitted_at":"2015-04-09T12:20:46Z","abstract_excerpt":"The classical cubic dimer model has a columnar ordering transition that is continuous and described by a critical Anderson--Higgs theory containing an SU(2)-symmetric complex field minimally coupled to a noncompact U(1) gauge theory. Defects in the dimer constraints correspond to monopoles of the gauge theory, with charge determined by the deviation from unity of the dimer occupancy. By introducing such defects into Monte Carlo simulations of the dimer model at its critical point, we determine the scaling dimensions $y_2 = 1.48\\pm0.07$ and $y_3 = 0.20 \\pm 0.03$ for the operators corresponding "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.02278","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":"2026-05-18T01:26:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Pb93KWJkjd7wp3Rn67nUDi8Rw+DOdyFdhf4totD65Ul337rrKIREgsdKAqX/aFP+PooXBxovfGsYUK/cXeutCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T13:01:34.663460Z"},"content_sha256":"56f78ea16783634eec99c62e7f05b77e1108e3f24fac6651074a675b2edc30fc","schema_version":"1.0","event_id":"sha256:56f78ea16783634eec99c62e7f05b77e1108e3f24fac6651074a675b2edc30fc"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DMFF6BNBABJWNSTNEDJOXNER5I/bundle.json","state_url":"https://pith.science/pith/DMFF6BNBABJWNSTNEDJOXNER5I/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DMFF6BNBABJWNSTNEDJOXNER5I/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":"2026-06-03T13:01:34Z","links":{"resolver":"https://pith.science/pith/DMFF6BNBABJWNSTNEDJOXNER5I","bundle":"https://pith.science/pith/DMFF6BNBABJWNSTNEDJOXNER5I/bundle.json","state":"https://pith.science/pith/DMFF6BNBABJWNSTNEDJOXNER5I/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DMFF6BNBABJWNSTNEDJOXNER5I/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:DMFF6BNBABJWNSTNEDJOXNER5I","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":"294593ec5eb224b639a53da0fa4465bf0d5c5e4128bd41ddce39ffbbb90e7547","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-04-09T12:20:46Z","title_canon_sha256":"86acaa54a867279ee1dfc23307c012d697ec46aebc477ad6a493e3c5e7d9bab9"},"schema_version":"1.0","source":{"id":"1504.02278","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1504.02278","created_at":"2026-05-18T01:26:31Z"},{"alias_kind":"arxiv_version","alias_value":"1504.02278v2","created_at":"2026-05-18T01:26:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.02278","created_at":"2026-05-18T01:26:31Z"},{"alias_kind":"pith_short_12","alias_value":"DMFF6BNBABJW","created_at":"2026-05-18T12:29:17Z"},{"alias_kind":"pith_short_16","alias_value":"DMFF6BNBABJWNSTN","created_at":"2026-05-18T12:29:17Z"},{"alias_kind":"pith_short_8","alias_value":"DMFF6BNB","created_at":"2026-05-18T12:29:17Z"}],"graph_snapshots":[{"event_id":"sha256:56f78ea16783634eec99c62e7f05b77e1108e3f24fac6651074a675b2edc30fc","target":"graph","created_at":"2026-05-18T01:26:31Z","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 classical cubic dimer model has a columnar ordering transition that is continuous and described by a critical Anderson--Higgs theory containing an SU(2)-symmetric complex field minimally coupled to a noncompact U(1) gauge theory. Defects in the dimer constraints correspond to monopoles of the gauge theory, with charge determined by the deviation from unity of the dimer occupancy. By introducing such defects into Monte Carlo simulations of the dimer model at its critical point, we determine the scaling dimensions $y_2 = 1.48\\pm0.07$ and $y_3 = 0.20 \\pm 0.03$ for the operators corresponding ","authors_text":"G J Sreejith, Stephen Powell","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-04-09T12:20:46Z","title":"Scaling dimensions of higher-charge monopoles at deconfined critical points"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.02278","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":"sha256:6df4804ebf32efcae4e72b98ea218f55d9482bf348d5d82adb3119ce02f192f6","target":"record","created_at":"2026-05-18T01:26:31Z","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":"294593ec5eb224b639a53da0fa4465bf0d5c5e4128bd41ddce39ffbbb90e7547","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-04-09T12:20:46Z","title_canon_sha256":"86acaa54a867279ee1dfc23307c012d697ec46aebc477ad6a493e3c5e7d9bab9"},"schema_version":"1.0","source":{"id":"1504.02278","kind":"arxiv","version":2}},"canonical_sha256":"1b0a5f05a1005366ca6d20d2ebb491ea0b4d99c098c505bdf4986cfe3636f07c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1b0a5f05a1005366ca6d20d2ebb491ea0b4d99c098c505bdf4986cfe3636f07c","first_computed_at":"2026-05-18T01:26:31.609371Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:26:31.609371Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TCLPpK8fS9WI05YCMeksYcYCOI3qSI4sQYV8tt+nCpHwoxcEBuV5XFBNYzT7qOr6RrK5NOiJZd1tuUk01Lf2DQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:26:31.610085Z","signed_message":"canonical_sha256_bytes"},"source_id":"1504.02278","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6df4804ebf32efcae4e72b98ea218f55d9482bf348d5d82adb3119ce02f192f6","sha256:56f78ea16783634eec99c62e7f05b77e1108e3f24fac6651074a675b2edc30fc"],"state_sha256":"645ad12f28e60765d05cd00d44fada541ef29a33d41b625dd0b754575f639c27"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bK3nTodXamnLeZKspC3KBKl95p70Y0vsG3EyqGgKXjhegN9NnD42SVsOfwn1jZb7ao3X78xsMNYQVsX3kUhRAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T13:01:34.665642Z","bundle_sha256":"9ac5d6b2a7a5dc0fcb130f7bf780767c0c9476a2b34611798acc8a4b086844a1"}}