{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:6Z25M4M4U6BHPBYSNPHQCZ7RFG","short_pith_number":"pith:6Z25M4M4","canonical_record":{"source":{"id":"2305.10495","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-17T18:01:44Z","cross_cats_sorted":["cond-mat.quant-gas","hep-th","nlin.SI"],"title_canon_sha256":"baa435f60d271b8d69e0cdc86ca84fb89bcc75b2441237037cb4c2916408caad","abstract_canon_sha256":"09204338d36803a5523aa1a95137926a36e1a9b37afd2c9ee787ba31cb70c5f2"},"schema_version":"1.0"},"canonical_sha256":"f675d6719ca7827787126bcf0167f129a25f608bf0282367c6d4244f9a14b347","source":{"kind":"arxiv","id":"2305.10495","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2305.10495","created_at":"2026-07-05T07:29:26Z"},{"alias_kind":"arxiv_version","alias_value":"2305.10495v2","created_at":"2026-07-05T07:29:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.10495","created_at":"2026-07-05T07:29:26Z"},{"alias_kind":"pith_short_12","alias_value":"6Z25M4M4U6BH","created_at":"2026-07-05T07:29:26Z"},{"alias_kind":"pith_short_16","alias_value":"6Z25M4M4U6BHPBYS","created_at":"2026-07-05T07:29:26Z"},{"alias_kind":"pith_short_8","alias_value":"6Z25M4M4","created_at":"2026-07-05T07:29:26Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:6Z25M4M4U6BHPBYSNPHQCZ7RFG","target":"record","payload":{"canonical_record":{"source":{"id":"2305.10495","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-17T18:01:44Z","cross_cats_sorted":["cond-mat.quant-gas","hep-th","nlin.SI"],"title_canon_sha256":"baa435f60d271b8d69e0cdc86ca84fb89bcc75b2441237037cb4c2916408caad","abstract_canon_sha256":"09204338d36803a5523aa1a95137926a36e1a9b37afd2c9ee787ba31cb70c5f2"},"schema_version":"1.0"},"canonical_sha256":"f675d6719ca7827787126bcf0167f129a25f608bf0282367c6d4244f9a14b347","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:29:26.869149Z","signature_b64":"a15DBa/23c+S9+m53tnkfVamAbGPbbzLGZoQtozezZBq4F5d2WTt5cT5H6iJALt5w/xhVfDuUrwp6AyUZkQVBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f675d6719ca7827787126bcf0167f129a25f608bf0282367c6d4244f9a14b347","last_reissued_at":"2026-07-05T07:29:26.868642Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:29:26.868642Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2305.10495","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":"2026-07-05T07:29:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nRgaVQLjv2L4jDuinwUXVZjho20oyIaQP8HQ1pLI3Cf1f2xKxWFsoJfea6CJ9BWkHpjYBbWXQOScDJVd6MWqCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T22:11:34.869125Z"},"content_sha256":"b2f4f8b8098e0ac8f3e2fbe239af48bc96c4b5df5d81b9cab18a369d9b8b2a69","schema_version":"1.0","event_id":"sha256:b2f4f8b8098e0ac8f3e2fbe239af48bc96c4b5df5d81b9cab18a369d9b8b2a69"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:6Z25M4M4U6BHPBYSNPHQCZ7RFG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Exact large-scale fluctuations of the phase field in the sine-Gordon model","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.quant-gas","hep-th","nlin.SI"],"primary_cat":"cond-mat.stat-mech","authors_text":"Alvise Bastianello, Benjamin Doyon, Giuseppe Del Vecchio Del Vecchio, M\\'arton Kormos","submitted_at":"2023-05-17T18:01:44Z","abstract_excerpt":"We present the first exact theory and analytical formulas for the large-scale phase fluctuations in the sine-Gordon model, valid in all regimes of the field theory, for arbitrary temperatures and interaction strengths. Our result is based on the Ballistic Fluctuation Theory combined with Generalized Hydrodynamics, and can be seen as an exact ``dressing\" of the phenomenological soliton-gas picture first introduced by Sachdev and Young [S. Sachdev and A. P. Young, PRL 78, 2220 (1997)], to the modes of Generalised Hydrodynamics. The resulting physics of phase fluctuations in the sine-Gordon model"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.10495","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2305.10495/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T07:29:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1dE4rmV/ukTMDCOD+K1oUVVDuYtGM6bZKjApqlEYMM8tpZ6dQaICu0liFZGlkS+5Ry+HoBrCqJ0tsmsO6vFWDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T22:11:34.869735Z"},"content_sha256":"1cad2f691dd1674de37975d233690fbfe7f02124481bb3d5b5aadedd0a753340","schema_version":"1.0","event_id":"sha256:1cad2f691dd1674de37975d233690fbfe7f02124481bb3d5b5aadedd0a753340"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6Z25M4M4U6BHPBYSNPHQCZ7RFG/bundle.json","state_url":"https://pith.science/pith/6Z25M4M4U6BHPBYSNPHQCZ7RFG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6Z25M4M4U6BHPBYSNPHQCZ7RFG/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":"2026-08-04T22:11:34Z","links":{"resolver":"https://pith.science/pith/6Z25M4M4U6BHPBYSNPHQCZ7RFG","bundle":"https://pith.science/pith/6Z25M4M4U6BHPBYSNPHQCZ7RFG/bundle.json","state":"https://pith.science/pith/6Z25M4M4U6BHPBYSNPHQCZ7RFG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6Z25M4M4U6BHPBYSNPHQCZ7RFG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:6Z25M4M4U6BHPBYSNPHQCZ7RFG","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":"09204338d36803a5523aa1a95137926a36e1a9b37afd2c9ee787ba31cb70c5f2","cross_cats_sorted":["cond-mat.quant-gas","hep-th","nlin.SI"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-17T18:01:44Z","title_canon_sha256":"baa435f60d271b8d69e0cdc86ca84fb89bcc75b2441237037cb4c2916408caad"},"schema_version":"1.0","source":{"id":"2305.10495","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2305.10495","created_at":"2026-07-05T07:29:26Z"},{"alias_kind":"arxiv_version","alias_value":"2305.10495v2","created_at":"2026-07-05T07:29:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.10495","created_at":"2026-07-05T07:29:26Z"},{"alias_kind":"pith_short_12","alias_value":"6Z25M4M4U6BH","created_at":"2026-07-05T07:29:26Z"},{"alias_kind":"pith_short_16","alias_value":"6Z25M4M4U6BHPBYS","created_at":"2026-07-05T07:29:26Z"},{"alias_kind":"pith_short_8","alias_value":"6Z25M4M4","created_at":"2026-07-05T07:29:26Z"}],"graph_snapshots":[{"event_id":"sha256:1cad2f691dd1674de37975d233690fbfe7f02124481bb3d5b5aadedd0a753340","target":"graph","created_at":"2026-07-05T07:29:26Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2305.10495/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present the first exact theory and analytical formulas for the large-scale phase fluctuations in the sine-Gordon model, valid in all regimes of the field theory, for arbitrary temperatures and interaction strengths. Our result is based on the Ballistic Fluctuation Theory combined with Generalized Hydrodynamics, and can be seen as an exact ``dressing\" of the phenomenological soliton-gas picture first introduced by Sachdev and Young [S. Sachdev and A. P. Young, PRL 78, 2220 (1997)], to the modes of Generalised Hydrodynamics. The resulting physics of phase fluctuations in the sine-Gordon model","authors_text":"Alvise Bastianello, Benjamin Doyon, Giuseppe Del Vecchio Del Vecchio, M\\'arton Kormos","cross_cats":["cond-mat.quant-gas","hep-th","nlin.SI"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-17T18:01:44Z","title":"Exact large-scale fluctuations of the phase field in the sine-Gordon model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.10495","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:b2f4f8b8098e0ac8f3e2fbe239af48bc96c4b5df5d81b9cab18a369d9b8b2a69","target":"record","created_at":"2026-07-05T07:29:26Z","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":"09204338d36803a5523aa1a95137926a36e1a9b37afd2c9ee787ba31cb70c5f2","cross_cats_sorted":["cond-mat.quant-gas","hep-th","nlin.SI"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-17T18:01:44Z","title_canon_sha256":"baa435f60d271b8d69e0cdc86ca84fb89bcc75b2441237037cb4c2916408caad"},"schema_version":"1.0","source":{"id":"2305.10495","kind":"arxiv","version":2}},"canonical_sha256":"f675d6719ca7827787126bcf0167f129a25f608bf0282367c6d4244f9a14b347","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f675d6719ca7827787126bcf0167f129a25f608bf0282367c6d4244f9a14b347","first_computed_at":"2026-07-05T07:29:26.868642Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:29:26.868642Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"a15DBa/23c+S9+m53tnkfVamAbGPbbzLGZoQtozezZBq4F5d2WTt5cT5H6iJALt5w/xhVfDuUrwp6AyUZkQVBw==","signature_status":"signed_v1","signed_at":"2026-07-05T07:29:26.869149Z","signed_message":"canonical_sha256_bytes"},"source_id":"2305.10495","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b2f4f8b8098e0ac8f3e2fbe239af48bc96c4b5df5d81b9cab18a369d9b8b2a69","sha256:1cad2f691dd1674de37975d233690fbfe7f02124481bb3d5b5aadedd0a753340"],"state_sha256":"4b9da9f3c9fdc69491262e09c22b075d5af490c4a0fe59e75f148fb2fe9e5f47"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ac2EZY+1ALYAXMVrrWPePeYWA/3WmmiHQwO74zqtldp3YrPYLwcnZwi9CvwTUF2x9+KBpJP1JTnwrrbYuQOoBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T22:11:34.876943Z","bundle_sha256":"379cd0c86a24a17c5c8bf85dd73b7ee7b5d636563ce952d58d23412d384063bf"}}