{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:4UJU3ZIZP2JJNQNGKC5Z2G55YR","short_pith_number":"pith:4UJU3ZIZ","canonical_record":{"source":{"id":"1706.02322","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-06-07T18:07:37Z","cross_cats_sorted":["cond-mat.stat-mech","cond-mat.str-el"],"title_canon_sha256":"d652de0e6721893200126b1ffae1b7df368615b2e9dab1ec7fbb2dfe3571d393","abstract_canon_sha256":"46192ba035ba5cf8796c4f2c154e1fffc6e83ca189033a436cdb4b4f57cbffcc"},"schema_version":"1.0"},"canonical_sha256":"e5134de5197e9296c1a650bb9d1bbdc4721798e565fc0a9aeea991645cc1e690","source":{"kind":"arxiv","id":"1706.02322","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.02322","created_at":"2026-05-18T00:25:57Z"},{"alias_kind":"arxiv_version","alias_value":"1706.02322v2","created_at":"2026-05-18T00:25:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.02322","created_at":"2026-05-18T00:25:57Z"},{"alias_kind":"pith_short_12","alias_value":"4UJU3ZIZP2JJ","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_16","alias_value":"4UJU3ZIZP2JJNQNG","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_8","alias_value":"4UJU3ZIZ","created_at":"2026-05-18T12:31:00Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:4UJU3ZIZP2JJNQNGKC5Z2G55YR","target":"record","payload":{"canonical_record":{"source":{"id":"1706.02322","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-06-07T18:07:37Z","cross_cats_sorted":["cond-mat.stat-mech","cond-mat.str-el"],"title_canon_sha256":"d652de0e6721893200126b1ffae1b7df368615b2e9dab1ec7fbb2dfe3571d393","abstract_canon_sha256":"46192ba035ba5cf8796c4f2c154e1fffc6e83ca189033a436cdb4b4f57cbffcc"},"schema_version":"1.0"},"canonical_sha256":"e5134de5197e9296c1a650bb9d1bbdc4721798e565fc0a9aeea991645cc1e690","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:25:57.376626Z","signature_b64":"evOsSvH1ID+cSt9mkAJcfmspwTJcoRLt70HO66mj3DmqppaJ9RO+KzwvnQ9S+Mh6N8SSqUKq2Ztmg/D4DLYjAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e5134de5197e9296c1a650bb9d1bbdc4721798e565fc0a9aeea991645cc1e690","last_reissued_at":"2026-05-18T00:25:57.375902Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:25:57.375902Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1706.02322","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":"2026-05-18T00:25:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EcZGpP0KwQPUT4Yw4COFJLKeWNMYeKf3Y1vrQNI0pzYjDsszmIVkbcbEANKLWrAYPy5LPqjj2lp4yZx+A/u5Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T01:14:50.504085Z"},"content_sha256":"28a202f9a200e2537e02de9915869975a90fc77c69abeb88c6a7359424e68fe9","schema_version":"1.0","event_id":"sha256:28a202f9a200e2537e02de9915869975a90fc77c69abeb88c6a7359424e68fe9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:4UJU3ZIZP2JJNQNGKC5Z2G55YR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"An exactly solvable quench protocol for integrable spin models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Dami\\'an A. Galante, Diptarka Das, Krishnendu Sengupta, Robert C. Myers, Sumit R. Das","submitted_at":"2017-06-07T18:07:37Z","abstract_excerpt":"Quantum quenches in continuum field theory across critical points are known to display different scaling behaviours in different regimes of the quench rate. We extend these results to integrable lattice models such as the transverse field Ising model on a one-dimensional chain and the Kitaev model on a two-dimensional honeycomb lattice using a nonlinear quench protocol which allows for exact analytical solutions of the dynamics. Our quench protocol starts with a finite mass gap at early times and crosses a critical point or a critical region, and we study the behaviour of one point functions o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.02322","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":"2026-05-18T00:25:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"P8BfdrAvpue/FJfzikftgADMNJXt5+8h0X65u6O3ypXUOVG1kjj3nMAded82Y58ht3NMNoaBD4p7Uks+BmAiCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T01:14:50.504483Z"},"content_sha256":"976a53517e5d075e1c03d24495b8b230d77d37ded5a7f9073adb1dc553efd6d5","schema_version":"1.0","event_id":"sha256:976a53517e5d075e1c03d24495b8b230d77d37ded5a7f9073adb1dc553efd6d5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4UJU3ZIZP2JJNQNGKC5Z2G55YR/bundle.json","state_url":"https://pith.science/pith/4UJU3ZIZP2JJNQNGKC5Z2G55YR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4UJU3ZIZP2JJNQNGKC5Z2G55YR/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":"2026-05-26T01:14:50Z","links":{"resolver":"https://pith.science/pith/4UJU3ZIZP2JJNQNGKC5Z2G55YR","bundle":"https://pith.science/pith/4UJU3ZIZP2JJNQNGKC5Z2G55YR/bundle.json","state":"https://pith.science/pith/4UJU3ZIZP2JJNQNGKC5Z2G55YR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4UJU3ZIZP2JJNQNGKC5Z2G55YR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:4UJU3ZIZP2JJNQNGKC5Z2G55YR","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":"46192ba035ba5cf8796c4f2c154e1fffc6e83ca189033a436cdb4b4f57cbffcc","cross_cats_sorted":["cond-mat.stat-mech","cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-06-07T18:07:37Z","title_canon_sha256":"d652de0e6721893200126b1ffae1b7df368615b2e9dab1ec7fbb2dfe3571d393"},"schema_version":"1.0","source":{"id":"1706.02322","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.02322","created_at":"2026-05-18T00:25:57Z"},{"alias_kind":"arxiv_version","alias_value":"1706.02322v2","created_at":"2026-05-18T00:25:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.02322","created_at":"2026-05-18T00:25:57Z"},{"alias_kind":"pith_short_12","alias_value":"4UJU3ZIZP2JJ","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_16","alias_value":"4UJU3ZIZP2JJNQNG","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_8","alias_value":"4UJU3ZIZ","created_at":"2026-05-18T12:31:00Z"}],"graph_snapshots":[{"event_id":"sha256:976a53517e5d075e1c03d24495b8b230d77d37ded5a7f9073adb1dc553efd6d5","target":"graph","created_at":"2026-05-18T00:25:57Z","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":"Quantum quenches in continuum field theory across critical points are known to display different scaling behaviours in different regimes of the quench rate. We extend these results to integrable lattice models such as the transverse field Ising model on a one-dimensional chain and the Kitaev model on a two-dimensional honeycomb lattice using a nonlinear quench protocol which allows for exact analytical solutions of the dynamics. Our quench protocol starts with a finite mass gap at early times and crosses a critical point or a critical region, and we study the behaviour of one point functions o","authors_text":"Dami\\'an A. Galante, Diptarka Das, Krishnendu Sengupta, Robert C. Myers, Sumit R. Das","cross_cats":["cond-mat.stat-mech","cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-06-07T18:07:37Z","title":"An exactly solvable quench protocol for integrable spin models"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.02322","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":"sha256:28a202f9a200e2537e02de9915869975a90fc77c69abeb88c6a7359424e68fe9","target":"record","created_at":"2026-05-18T00:25:57Z","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":"46192ba035ba5cf8796c4f2c154e1fffc6e83ca189033a436cdb4b4f57cbffcc","cross_cats_sorted":["cond-mat.stat-mech","cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-06-07T18:07:37Z","title_canon_sha256":"d652de0e6721893200126b1ffae1b7df368615b2e9dab1ec7fbb2dfe3571d393"},"schema_version":"1.0","source":{"id":"1706.02322","kind":"arxiv","version":2}},"canonical_sha256":"e5134de5197e9296c1a650bb9d1bbdc4721798e565fc0a9aeea991645cc1e690","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e5134de5197e9296c1a650bb9d1bbdc4721798e565fc0a9aeea991645cc1e690","first_computed_at":"2026-05-18T00:25:57.375902Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:25:57.375902Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"evOsSvH1ID+cSt9mkAJcfmspwTJcoRLt70HO66mj3DmqppaJ9RO+KzwvnQ9S+Mh6N8SSqUKq2Ztmg/D4DLYjAg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:25:57.376626Z","signed_message":"canonical_sha256_bytes"},"source_id":"1706.02322","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:28a202f9a200e2537e02de9915869975a90fc77c69abeb88c6a7359424e68fe9","sha256:976a53517e5d075e1c03d24495b8b230d77d37ded5a7f9073adb1dc553efd6d5"],"state_sha256":"178eba543477a0ce675ed845a255ced9881ef3ca7520d38a94a96f5d9652cb69"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VOVtgNawEQGZflIJcBwSnr0jvTER+1RZ1OUu6RVnYNYB3KTynnHSgZsHTuhdu/X9jfes56tgZZZD0tzLDkPtAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T01:14:50.507355Z","bundle_sha256":"c5d2704df0eed343b9c9a985a1d4e6ca12f01ab09ed94901efe310e68e60f192"}}