{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:VRTLIJPCCPMIZNML3RBWSDVQM2","short_pith_number":"pith:VRTLIJPC","canonical_record":{"source":{"id":"1502.06756","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2015-02-24T10:44:48Z","cross_cats_sorted":["cond-mat.stat-mech","math.MP","nlin.CD"],"title_canon_sha256":"17a8f22feeae8e2bce7ffd9fc19c7d32ff86505507c96d868184ac8863c0daa9","abstract_canon_sha256":"4301a86d4d653c259266a9e81b0c20dde14d90b693e77cd4ed7124a7b731efd7"},"schema_version":"1.0"},"canonical_sha256":"ac66b425e213d88cb58bdc43690eb066b7fcb41e08c075e1ee1def8b79400846","source":{"kind":"arxiv","id":"1502.06756","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1502.06756","created_at":"2026-05-18T01:37:49Z"},{"alias_kind":"arxiv_version","alias_value":"1502.06756v4","created_at":"2026-05-18T01:37:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.06756","created_at":"2026-05-18T01:37:49Z"},{"alias_kind":"pith_short_12","alias_value":"VRTLIJPCCPMI","created_at":"2026-05-18T12:29:47Z"},{"alias_kind":"pith_short_16","alias_value":"VRTLIJPCCPMIZNML","created_at":"2026-05-18T12:29:47Z"},{"alias_kind":"pith_short_8","alias_value":"VRTLIJPC","created_at":"2026-05-18T12:29:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:VRTLIJPCCPMIZNML3RBWSDVQM2","target":"record","payload":{"canonical_record":{"source":{"id":"1502.06756","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2015-02-24T10:44:48Z","cross_cats_sorted":["cond-mat.stat-mech","math.MP","nlin.CD"],"title_canon_sha256":"17a8f22feeae8e2bce7ffd9fc19c7d32ff86505507c96d868184ac8863c0daa9","abstract_canon_sha256":"4301a86d4d653c259266a9e81b0c20dde14d90b693e77cd4ed7124a7b731efd7"},"schema_version":"1.0"},"canonical_sha256":"ac66b425e213d88cb58bdc43690eb066b7fcb41e08c075e1ee1def8b79400846","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:37:49.034887Z","signature_b64":"zyk2a9fTDApJHAxwyeUePwUM4gOeZDUx5W9MsO1zqXhV0q/JxE2jJzy+Fra8tUmJLrjJNw3USlk0McS39L2jBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ac66b425e213d88cb58bdc43690eb066b7fcb41e08c075e1ee1def8b79400846","last_reissued_at":"2026-05-18T01:37:49.034224Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:37:49.034224Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1502.06756","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:37:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"x17So7+A5FObqkOy59qShorLogOsze/NsxDoOm+b8s2mT0gRPkfklxOxD1uFZmaccJ/Apnn4ayqJv2c7hqfWBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T05:35:21.011705Z"},"content_sha256":"82f836a6d9b629e719daff7090860e3545f8e3c8eded40d3d7edfa80a68e59db","schema_version":"1.0","event_id":"sha256:82f836a6d9b629e719daff7090860e3545f8e3c8eded40d3d7edfa80a68e59db"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:VRTLIJPCCPMIZNML3RBWSDVQM2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fluctuations in the two-dimensional one-component plasma and associated fourth-order phase transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","math.MP","nlin.CD"],"primary_cat":"math-ph","authors_text":"Anna Maltsev, Fabio Deelan Cunden, Francesco Mezzadri","submitted_at":"2015-02-24T10:44:48Z","abstract_excerpt":"We study the distribution of the mean radial displacement of charges of a 2D one-component plasma in the thermodynamic limit $N\\to\\infty$ at finite temperature $\\beta>0$. We compute explicitly the large deviation functions showing the emergence of a fourth-order phase transition as a consequence of a change of topology in the plasma distribution. This weak phase transition occurs exactly at the ground state of the plasma. These results have been compared with the integrable case (finite $N$) of plasma parameter $\\beta q^2=2$. In this case the problem can be mapped to the stationary properties "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.06756","kind":"arxiv","version":4},"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":"2026-05-18T01:37:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HKRZqgoUSkHSE2bzpupy4/xpU7iD60qqSGLqPdva0mGbJcFtayygb0phn+ZqihSiyau8UOBofUUQZRllZY1fCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T05:35:21.012047Z"},"content_sha256":"857b339ff3c57b2c89d724e2241fadf00ee9ccac4c82b9ba31b6922e796fa840","schema_version":"1.0","event_id":"sha256:857b339ff3c57b2c89d724e2241fadf00ee9ccac4c82b9ba31b6922e796fa840"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VRTLIJPCCPMIZNML3RBWSDVQM2/bundle.json","state_url":"https://pith.science/pith/VRTLIJPCCPMIZNML3RBWSDVQM2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VRTLIJPCCPMIZNML3RBWSDVQM2/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":"2026-06-03T05:35:21Z","links":{"resolver":"https://pith.science/pith/VRTLIJPCCPMIZNML3RBWSDVQM2","bundle":"https://pith.science/pith/VRTLIJPCCPMIZNML3RBWSDVQM2/bundle.json","state":"https://pith.science/pith/VRTLIJPCCPMIZNML3RBWSDVQM2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VRTLIJPCCPMIZNML3RBWSDVQM2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:VRTLIJPCCPMIZNML3RBWSDVQM2","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":"4301a86d4d653c259266a9e81b0c20dde14d90b693e77cd4ed7124a7b731efd7","cross_cats_sorted":["cond-mat.stat-mech","math.MP","nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2015-02-24T10:44:48Z","title_canon_sha256":"17a8f22feeae8e2bce7ffd9fc19c7d32ff86505507c96d868184ac8863c0daa9"},"schema_version":"1.0","source":{"id":"1502.06756","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1502.06756","created_at":"2026-05-18T01:37:49Z"},{"alias_kind":"arxiv_version","alias_value":"1502.06756v4","created_at":"2026-05-18T01:37:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.06756","created_at":"2026-05-18T01:37:49Z"},{"alias_kind":"pith_short_12","alias_value":"VRTLIJPCCPMI","created_at":"2026-05-18T12:29:47Z"},{"alias_kind":"pith_short_16","alias_value":"VRTLIJPCCPMIZNML","created_at":"2026-05-18T12:29:47Z"},{"alias_kind":"pith_short_8","alias_value":"VRTLIJPC","created_at":"2026-05-18T12:29:47Z"}],"graph_snapshots":[{"event_id":"sha256:857b339ff3c57b2c89d724e2241fadf00ee9ccac4c82b9ba31b6922e796fa840","target":"graph","created_at":"2026-05-18T01:37:49Z","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 study the distribution of the mean radial displacement of charges of a 2D one-component plasma in the thermodynamic limit $N\\to\\infty$ at finite temperature $\\beta>0$. We compute explicitly the large deviation functions showing the emergence of a fourth-order phase transition as a consequence of a change of topology in the plasma distribution. This weak phase transition occurs exactly at the ground state of the plasma. These results have been compared with the integrable case (finite $N$) of plasma parameter $\\beta q^2=2$. In this case the problem can be mapped to the stationary properties ","authors_text":"Anna Maltsev, Fabio Deelan Cunden, Francesco Mezzadri","cross_cats":["cond-mat.stat-mech","math.MP","nlin.CD"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2015-02-24T10:44:48Z","title":"Fluctuations in the two-dimensional one-component plasma and associated fourth-order phase transition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.06756","kind":"arxiv","version":4},"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":"sha256:82f836a6d9b629e719daff7090860e3545f8e3c8eded40d3d7edfa80a68e59db","target":"record","created_at":"2026-05-18T01:37:49Z","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":"4301a86d4d653c259266a9e81b0c20dde14d90b693e77cd4ed7124a7b731efd7","cross_cats_sorted":["cond-mat.stat-mech","math.MP","nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2015-02-24T10:44:48Z","title_canon_sha256":"17a8f22feeae8e2bce7ffd9fc19c7d32ff86505507c96d868184ac8863c0daa9"},"schema_version":"1.0","source":{"id":"1502.06756","kind":"arxiv","version":4}},"canonical_sha256":"ac66b425e213d88cb58bdc43690eb066b7fcb41e08c075e1ee1def8b79400846","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ac66b425e213d88cb58bdc43690eb066b7fcb41e08c075e1ee1def8b79400846","first_computed_at":"2026-05-18T01:37:49.034224Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:37:49.034224Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"zyk2a9fTDApJHAxwyeUePwUM4gOeZDUx5W9MsO1zqXhV0q/JxE2jJzy+Fra8tUmJLrjJNw3USlk0McS39L2jBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:37:49.034887Z","signed_message":"canonical_sha256_bytes"},"source_id":"1502.06756","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:82f836a6d9b629e719daff7090860e3545f8e3c8eded40d3d7edfa80a68e59db","sha256:857b339ff3c57b2c89d724e2241fadf00ee9ccac4c82b9ba31b6922e796fa840"],"state_sha256":"962c717d2bf07aea7153f78906de0c5aaefe2d04a830c0d17f736ebc1cdb5c97"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"X8UVu7DHDbz8PUj5DF+4rh9MUTcv2sKXontSlQm7FoCgOhyeOvz5WEPc7KWgAazL5XqedRLFk880A6NEAjGKDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T05:35:21.014037Z","bundle_sha256":"8d61cc3325ac277d590a460a0bfea4be2e346a3ff79238fbf51fd0749fc69327"}}