{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:T26CYKRZPQYKRNKDV4JTJUEZWZ","short_pith_number":"pith:T26CYKRZ","canonical_record":{"source":{"id":"1407.3816","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-14T21:07:37Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"5bf0843e2a99f55518fe847e45da51c6284624669859b01fda7397a6da0dc821","abstract_canon_sha256":"d03f0c6909cd5d374cc673480ceef22de054784ceb4316ccd2cb04a9e8b0d260"},"schema_version":"1.0"},"canonical_sha256":"9ebc2c2a397c30a8b543af1334d099b6547ca18f97a976db7dd21b33aea7e872","source":{"kind":"arxiv","id":"1407.3816","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.3816","created_at":"2026-05-18T02:47:32Z"},{"alias_kind":"arxiv_version","alias_value":"1407.3816v1","created_at":"2026-05-18T02:47:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.3816","created_at":"2026-05-18T02:47:32Z"},{"alias_kind":"pith_short_12","alias_value":"T26CYKRZPQYK","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"T26CYKRZPQYKRNKD","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"T26CYKRZ","created_at":"2026-05-18T12:28:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:T26CYKRZPQYKRNKDV4JTJUEZWZ","target":"record","payload":{"canonical_record":{"source":{"id":"1407.3816","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-14T21:07:37Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"5bf0843e2a99f55518fe847e45da51c6284624669859b01fda7397a6da0dc821","abstract_canon_sha256":"d03f0c6909cd5d374cc673480ceef22de054784ceb4316ccd2cb04a9e8b0d260"},"schema_version":"1.0"},"canonical_sha256":"9ebc2c2a397c30a8b543af1334d099b6547ca18f97a976db7dd21b33aea7e872","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:47:32.559202Z","signature_b64":"Sy+toDqnj5SVZG8vCjtf39kWF81zZt3Q5JkwWuODNyBeYtW/dGvTXjgCeNrCPFtgi/3O4sCONM/h5WCYH7SrBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9ebc2c2a397c30a8b543af1334d099b6547ca18f97a976db7dd21b33aea7e872","last_reissued_at":"2026-05-18T02:47:32.558710Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:47:32.558710Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.3816","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":"2026-05-18T02:47:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l41+c8MR+/CKHlpIkkd8//EA5xsdfyBxfOYCG/Qt/DNgS4hmKq2cCX7/7nV6LXUKLHQky+G05OFj2iAT1OchBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T09:15:04.157632Z"},"content_sha256":"6691427104b4a90e22ad1b89388108ada7efd0e556f32355a35bdbafd201f72f","schema_version":"1.0","event_id":"sha256:6691427104b4a90e22ad1b89388108ada7efd0e556f32355a35bdbafd201f72f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:T26CYKRZPQYKRNKDV4JTJUEZWZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"nPI Resummation in 3D SU(N) Higgs Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Guy D. Moore, Mark C. Abraao York","submitted_at":"2014-07-14T21:07:37Z","abstract_excerpt":"We test the utility of the nPI formalism for solving nonperturbative dynamics of gauge theories by applying it to study the phase diagram of SU(N) Higgs theory in 3 Euclidean spacetime dimensions. Solutions reveal standard signatures of a first order phase transition with a critical endpoint leading to a crossover regime, in qualitative agreement with lattice studies. The location of the critical endpoint, x sim 0.14 for SU(2) with a fundamental Higgs, is in rough but not tight quantitative agreement with the lattice. We end by commenting on the overall effectiveness and limitations of an nPI "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.3816","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":"2026-05-18T02:47:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iW7TrstxaBwDa0an4y/+0KNTL711kspt5ELcqXyVumCEVTE0bMu6k89H5edzie5B0YmWp88fjDrL3V9pg4K+AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T09:15:04.158406Z"},"content_sha256":"58ac20f91b234ffffac8ee97d427726b472bac5cdde029833500aa21949ca9a1","schema_version":"1.0","event_id":"sha256:58ac20f91b234ffffac8ee97d427726b472bac5cdde029833500aa21949ca9a1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/T26CYKRZPQYKRNKDV4JTJUEZWZ/bundle.json","state_url":"https://pith.science/pith/T26CYKRZPQYKRNKDV4JTJUEZWZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/T26CYKRZPQYKRNKDV4JTJUEZWZ/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":"2026-05-31T09:15:04Z","links":{"resolver":"https://pith.science/pith/T26CYKRZPQYKRNKDV4JTJUEZWZ","bundle":"https://pith.science/pith/T26CYKRZPQYKRNKDV4JTJUEZWZ/bundle.json","state":"https://pith.science/pith/T26CYKRZPQYKRNKDV4JTJUEZWZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/T26CYKRZPQYKRNKDV4JTJUEZWZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:T26CYKRZPQYKRNKDV4JTJUEZWZ","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":"d03f0c6909cd5d374cc673480ceef22de054784ceb4316ccd2cb04a9e8b0d260","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-14T21:07:37Z","title_canon_sha256":"5bf0843e2a99f55518fe847e45da51c6284624669859b01fda7397a6da0dc821"},"schema_version":"1.0","source":{"id":"1407.3816","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.3816","created_at":"2026-05-18T02:47:32Z"},{"alias_kind":"arxiv_version","alias_value":"1407.3816v1","created_at":"2026-05-18T02:47:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.3816","created_at":"2026-05-18T02:47:32Z"},{"alias_kind":"pith_short_12","alias_value":"T26CYKRZPQYK","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"T26CYKRZPQYKRNKD","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"T26CYKRZ","created_at":"2026-05-18T12:28:49Z"}],"graph_snapshots":[{"event_id":"sha256:58ac20f91b234ffffac8ee97d427726b472bac5cdde029833500aa21949ca9a1","target":"graph","created_at":"2026-05-18T02:47:32Z","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 test the utility of the nPI formalism for solving nonperturbative dynamics of gauge theories by applying it to study the phase diagram of SU(N) Higgs theory in 3 Euclidean spacetime dimensions. Solutions reveal standard signatures of a first order phase transition with a critical endpoint leading to a crossover regime, in qualitative agreement with lattice studies. The location of the critical endpoint, x sim 0.14 for SU(2) with a fundamental Higgs, is in rough but not tight quantitative agreement with the lattice. We end by commenting on the overall effectiveness and limitations of an nPI ","authors_text":"Guy D. Moore, Mark C. Abraao York","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-14T21:07:37Z","title":"nPI Resummation in 3D SU(N) Higgs Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.3816","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":"sha256:6691427104b4a90e22ad1b89388108ada7efd0e556f32355a35bdbafd201f72f","target":"record","created_at":"2026-05-18T02:47:32Z","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":"d03f0c6909cd5d374cc673480ceef22de054784ceb4316ccd2cb04a9e8b0d260","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-14T21:07:37Z","title_canon_sha256":"5bf0843e2a99f55518fe847e45da51c6284624669859b01fda7397a6da0dc821"},"schema_version":"1.0","source":{"id":"1407.3816","kind":"arxiv","version":1}},"canonical_sha256":"9ebc2c2a397c30a8b543af1334d099b6547ca18f97a976db7dd21b33aea7e872","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9ebc2c2a397c30a8b543af1334d099b6547ca18f97a976db7dd21b33aea7e872","first_computed_at":"2026-05-18T02:47:32.558710Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:47:32.558710Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Sy+toDqnj5SVZG8vCjtf39kWF81zZt3Q5JkwWuODNyBeYtW/dGvTXjgCeNrCPFtgi/3O4sCONM/h5WCYH7SrBw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:47:32.559202Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.3816","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6691427104b4a90e22ad1b89388108ada7efd0e556f32355a35bdbafd201f72f","sha256:58ac20f91b234ffffac8ee97d427726b472bac5cdde029833500aa21949ca9a1"],"state_sha256":"7bc1b71cd06e79b269725adae82b1563cdf3c7149eb06c251f5d3e6892ac4a8a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Rxr0qgWpY5O/mbCtTRRua1chNZ0WX7mK7sGk2uC/NC97VjUTOTbb8GKXfcpT/s5XtxVeukhL/IRseCft4/SqBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T09:15:04.163062Z","bundle_sha256":"8e4ed40210919e241749069fda181370bfc601796590f4f6a20b7198d5a58c95"}}