{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:MOMYG7IRGUPFZMVEWJCE3DMX7V","short_pith_number":"pith:MOMYG7IR","canonical_record":{"source":{"id":"1609.03220","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-09-11T21:59:14Z","cross_cats_sorted":["cond-mat.str-el","hep-lat","hep-th","math-ph","math.MP"],"title_canon_sha256":"d3830330a3cc857395d94c5f40cdffad315b7685a60c1f39779421ec23526c90","abstract_canon_sha256":"37004f9d04cf0a1d36cd85552fcb5f0fb2133c6f10d5329b801bec3b975bfcf6"},"schema_version":"1.0"},"canonical_sha256":"6399837d11351e5cb2a4b2444d8d97fd6da3f91be64cff42800d7620287c1271","source":{"kind":"arxiv","id":"1609.03220","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.03220","created_at":"2026-05-18T00:48:27Z"},{"alias_kind":"arxiv_version","alias_value":"1609.03220v3","created_at":"2026-05-18T00:48:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.03220","created_at":"2026-05-18T00:48:27Z"},{"alias_kind":"pith_short_12","alias_value":"MOMYG7IRGUPF","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"MOMYG7IRGUPFZMVE","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"MOMYG7IR","created_at":"2026-05-18T12:30:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:MOMYG7IRGUPFZMVEWJCE3DMX7V","target":"record","payload":{"canonical_record":{"source":{"id":"1609.03220","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-09-11T21:59:14Z","cross_cats_sorted":["cond-mat.str-el","hep-lat","hep-th","math-ph","math.MP"],"title_canon_sha256":"d3830330a3cc857395d94c5f40cdffad315b7685a60c1f39779421ec23526c90","abstract_canon_sha256":"37004f9d04cf0a1d36cd85552fcb5f0fb2133c6f10d5329b801bec3b975bfcf6"},"schema_version":"1.0"},"canonical_sha256":"6399837d11351e5cb2a4b2444d8d97fd6da3f91be64cff42800d7620287c1271","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:48:27.424949Z","signature_b64":"nVhLM8XCAdVLX5qBGFlOtZmA4rcQ3vZIrrAQYBNXe8SOVbIvT7YIheivKmsIEKGqNMtQYp3mk8rMCp1+lXz7Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6399837d11351e5cb2a4b2444d8d97fd6da3f91be64cff42800d7620287c1271","last_reissued_at":"2026-05-18T00:48:27.424070Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:48:27.424070Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1609.03220","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:48:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"znHRh+AOHskM0zCpc96SYk+Jf5XDM3VigFcockvtM8S3NtHdtyVceFt0hGZSIUIku8jpWRJI1lTzX02dB5khDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T13:28:47.217382Z"},"content_sha256":"a009ec5db7adb5ffa9e7d7a0f70cad9559298460e8573978d69e2b05bd391a0b","schema_version":"1.0","event_id":"sha256:a009ec5db7adb5ffa9e7d7a0f70cad9559298460e8573978d69e2b05bd391a0b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:MOMYG7IRGUPFZMVEWJCE3DMX7V","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quasilocal charges and progress towards the complete GGE for field theories with non-diagonal scattering","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-lat","hep-th","math-ph","math.MP"],"primary_cat":"cond-mat.stat-mech","authors_text":"Axel Cort\\'es Cubero, Eric Vernier","submitted_at":"2016-09-11T21:59:14Z","abstract_excerpt":"It has recently been shown that some integrable spin chains possess a set of quasilocal conserved charges, with the classic example being the spin-$\\frac{1}{2}$ XXZ Heisenberg chain. These charges have been proven to be essential for properly describing stationary states after a quantum quench, and must be included in the generalized Gibbs ensemble (GGE). We find that similar charges are also necessary for the GGE description of integrable quantum field theories with non-diagonal scattering. A stationary state in a non-diagonal scattering theory is completely specified by fixing the mode-ocupp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.03220","kind":"arxiv","version":3},"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":"2026-05-18T00:48:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LghrRVPtiEN1VdpYs5Dyyrt4C4Hkhy6gf2ei5RYqZfXY9FTyHGj5voRTqyp9Dngc8lgfJF3avGKLpVlnNJWZCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T13:28:47.218179Z"},"content_sha256":"41cd76b71dfe2572419ae015e1408323ba2332d12a18812a568e7e17ca4ecad8","schema_version":"1.0","event_id":"sha256:41cd76b71dfe2572419ae015e1408323ba2332d12a18812a568e7e17ca4ecad8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MOMYG7IRGUPFZMVEWJCE3DMX7V/bundle.json","state_url":"https://pith.science/pith/MOMYG7IRGUPFZMVEWJCE3DMX7V/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MOMYG7IRGUPFZMVEWJCE3DMX7V/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":"2026-05-31T13:28:47Z","links":{"resolver":"https://pith.science/pith/MOMYG7IRGUPFZMVEWJCE3DMX7V","bundle":"https://pith.science/pith/MOMYG7IRGUPFZMVEWJCE3DMX7V/bundle.json","state":"https://pith.science/pith/MOMYG7IRGUPFZMVEWJCE3DMX7V/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MOMYG7IRGUPFZMVEWJCE3DMX7V/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:MOMYG7IRGUPFZMVEWJCE3DMX7V","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":"37004f9d04cf0a1d36cd85552fcb5f0fb2133c6f10d5329b801bec3b975bfcf6","cross_cats_sorted":["cond-mat.str-el","hep-lat","hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-09-11T21:59:14Z","title_canon_sha256":"d3830330a3cc857395d94c5f40cdffad315b7685a60c1f39779421ec23526c90"},"schema_version":"1.0","source":{"id":"1609.03220","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.03220","created_at":"2026-05-18T00:48:27Z"},{"alias_kind":"arxiv_version","alias_value":"1609.03220v3","created_at":"2026-05-18T00:48:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.03220","created_at":"2026-05-18T00:48:27Z"},{"alias_kind":"pith_short_12","alias_value":"MOMYG7IRGUPF","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"MOMYG7IRGUPFZMVE","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"MOMYG7IR","created_at":"2026-05-18T12:30:32Z"}],"graph_snapshots":[{"event_id":"sha256:41cd76b71dfe2572419ae015e1408323ba2332d12a18812a568e7e17ca4ecad8","target":"graph","created_at":"2026-05-18T00:48:27Z","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":"It has recently been shown that some integrable spin chains possess a set of quasilocal conserved charges, with the classic example being the spin-$\\frac{1}{2}$ XXZ Heisenberg chain. These charges have been proven to be essential for properly describing stationary states after a quantum quench, and must be included in the generalized Gibbs ensemble (GGE). We find that similar charges are also necessary for the GGE description of integrable quantum field theories with non-diagonal scattering. A stationary state in a non-diagonal scattering theory is completely specified by fixing the mode-ocupp","authors_text":"Axel Cort\\'es Cubero, Eric Vernier","cross_cats":["cond-mat.str-el","hep-lat","hep-th","math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-09-11T21:59:14Z","title":"Quasilocal charges and progress towards the complete GGE for field theories with non-diagonal scattering"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.03220","kind":"arxiv","version":3},"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:a009ec5db7adb5ffa9e7d7a0f70cad9559298460e8573978d69e2b05bd391a0b","target":"record","created_at":"2026-05-18T00:48:27Z","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":"37004f9d04cf0a1d36cd85552fcb5f0fb2133c6f10d5329b801bec3b975bfcf6","cross_cats_sorted":["cond-mat.str-el","hep-lat","hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-09-11T21:59:14Z","title_canon_sha256":"d3830330a3cc857395d94c5f40cdffad315b7685a60c1f39779421ec23526c90"},"schema_version":"1.0","source":{"id":"1609.03220","kind":"arxiv","version":3}},"canonical_sha256":"6399837d11351e5cb2a4b2444d8d97fd6da3f91be64cff42800d7620287c1271","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6399837d11351e5cb2a4b2444d8d97fd6da3f91be64cff42800d7620287c1271","first_computed_at":"2026-05-18T00:48:27.424070Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:48:27.424070Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nVhLM8XCAdVLX5qBGFlOtZmA4rcQ3vZIrrAQYBNXe8SOVbIvT7YIheivKmsIEKGqNMtQYp3mk8rMCp1+lXz7Aw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:48:27.424949Z","signed_message":"canonical_sha256_bytes"},"source_id":"1609.03220","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a009ec5db7adb5ffa9e7d7a0f70cad9559298460e8573978d69e2b05bd391a0b","sha256:41cd76b71dfe2572419ae015e1408323ba2332d12a18812a568e7e17ca4ecad8"],"state_sha256":"b1cdce7edc828f0fd287e85639231277d908602f8d72d4625209f6e8c694d09c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qtSm4s0PBXgCkiqbQ88XaULc+OIB873MfgaBJusPGxWS3xm0nJrI5lpHWEzsLkQyBwmwos6aXmrc908q7O37Bg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T13:28:47.222627Z","bundle_sha256":"12141897f7fc8a737cdb539a7a264474ef0a39a0e9509a11c06f1aabe9969a3b"}}