{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:GER2SRSJENNSLR4EK2V4VHS4CB","short_pith_number":"pith:GER2SRSJ","canonical_record":{"source":{"id":"1112.3403","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-15T01:08:42Z","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","math.QA"],"title_canon_sha256":"8c12428d9bc29e300c252545053ad3f504bb81a687413e23ac70e35adb1e30a9","abstract_canon_sha256":"c7fe03081cb65a10af567d21582746e5135f5416e9cc49bae4ec319eb6899749"},"schema_version":"1.0"},"canonical_sha256":"3123a94649235b25c78456abca9e5c1053360d4ab5bf64980566c28194409dcf","source":{"kind":"arxiv","id":"1112.3403","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.3403","created_at":"2026-05-18T03:29:39Z"},{"alias_kind":"arxiv_version","alias_value":"1112.3403v3","created_at":"2026-05-18T03:29:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.3403","created_at":"2026-05-18T03:29:39Z"},{"alias_kind":"pith_short_12","alias_value":"GER2SRSJENNS","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_16","alias_value":"GER2SRSJENNSLR4E","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_8","alias_value":"GER2SRSJ","created_at":"2026-05-18T12:26:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:GER2SRSJENNSLR4EK2V4VHS4CB","target":"record","payload":{"canonical_record":{"source":{"id":"1112.3403","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-15T01:08:42Z","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","math.QA"],"title_canon_sha256":"8c12428d9bc29e300c252545053ad3f504bb81a687413e23ac70e35adb1e30a9","abstract_canon_sha256":"c7fe03081cb65a10af567d21582746e5135f5416e9cc49bae4ec319eb6899749"},"schema_version":"1.0"},"canonical_sha256":"3123a94649235b25c78456abca9e5c1053360d4ab5bf64980566c28194409dcf","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:29:39.212178Z","signature_b64":"paDYQTUBbxhoZBpJGm6XVOiLmf14wS/z2P83mRC1Li+L4xPCt8bnJr4lx7RpAcwKpizKCTc1EFI+MWN97J8lBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3123a94649235b25c78456abca9e5c1053360d4ab5bf64980566c28194409dcf","last_reissued_at":"2026-05-18T03:29:39.211709Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:29:39.211709Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1112.3403","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":"2026-05-18T03:29:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jpiIFwBHp7/remnhGqCD7QKzjLpaAGi4ifeNVVj2pMmrkCZmRpUnDcuT7PdqiDxeXJbbVSoSngDurj9C2bzbCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:16:13.471186Z"},"content_sha256":"30521499eb57aed96009567ed0350c015e429d1f283f2c8bb63b0b8019be05d4","schema_version":"1.0","event_id":"sha256:30521499eb57aed96009567ed0350c015e429d1f283f2c8bb63b0b8019be05d4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:GER2SRSJENNSLR4EK2V4VHS4CB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Continuum limit and symmetries of the periodic gl(1|1) spin chain","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","math-ph","math.MP","math.QA"],"primary_cat":"hep-th","authors_text":"A. M. Gainutdinov, H. Saleur, N. Read","submitted_at":"2011-12-15T01:08:42Z","abstract_excerpt":"This paper is the first in a series devoted to the study of logarithmic conformal field theories (LCFT) in the bulk. Building on earlier work in the boundary case, our general strategy consists in analyzing the algebraic properties of lattice regularizations (quantum spin chains) of these theories. In the boundary case, a crucial step was the identification of the space of states as a bimodule over the Temperley Lieb (TL) algebra and the quantum group U_q sl(2). The extension of this analysis in the bulk case involves considerable difficulties, since the U_q sl(2) symmetry is partly lost, whil"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.3403","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":"2026-05-18T03:29:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Xaf4Tz40jJquOnbTJMHwnu6rr13F/M7CBehxX9UFwUuXxp0BsY8uKuV9DQTXe0PLWSdlMTX5zcc3wIMMi0GNCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:16:13.471893Z"},"content_sha256":"65aeff2f698f4db7ac85fa615f28bf92f45af6a45096735fa1e4554987d9d632","schema_version":"1.0","event_id":"sha256:65aeff2f698f4db7ac85fa615f28bf92f45af6a45096735fa1e4554987d9d632"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GER2SRSJENNSLR4EK2V4VHS4CB/bundle.json","state_url":"https://pith.science/pith/GER2SRSJENNSLR4EK2V4VHS4CB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GER2SRSJENNSLR4EK2V4VHS4CB/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":"2026-05-25T21:16:13Z","links":{"resolver":"https://pith.science/pith/GER2SRSJENNSLR4EK2V4VHS4CB","bundle":"https://pith.science/pith/GER2SRSJENNSLR4EK2V4VHS4CB/bundle.json","state":"https://pith.science/pith/GER2SRSJENNSLR4EK2V4VHS4CB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GER2SRSJENNSLR4EK2V4VHS4CB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:GER2SRSJENNSLR4EK2V4VHS4CB","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":"c7fe03081cb65a10af567d21582746e5135f5416e9cc49bae4ec319eb6899749","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","math.QA"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-15T01:08:42Z","title_canon_sha256":"8c12428d9bc29e300c252545053ad3f504bb81a687413e23ac70e35adb1e30a9"},"schema_version":"1.0","source":{"id":"1112.3403","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.3403","created_at":"2026-05-18T03:29:39Z"},{"alias_kind":"arxiv_version","alias_value":"1112.3403v3","created_at":"2026-05-18T03:29:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.3403","created_at":"2026-05-18T03:29:39Z"},{"alias_kind":"pith_short_12","alias_value":"GER2SRSJENNS","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_16","alias_value":"GER2SRSJENNSLR4E","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_8","alias_value":"GER2SRSJ","created_at":"2026-05-18T12:26:28Z"}],"graph_snapshots":[{"event_id":"sha256:65aeff2f698f4db7ac85fa615f28bf92f45af6a45096735fa1e4554987d9d632","target":"graph","created_at":"2026-05-18T03:29:39Z","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":"This paper is the first in a series devoted to the study of logarithmic conformal field theories (LCFT) in the bulk. Building on earlier work in the boundary case, our general strategy consists in analyzing the algebraic properties of lattice regularizations (quantum spin chains) of these theories. In the boundary case, a crucial step was the identification of the space of states as a bimodule over the Temperley Lieb (TL) algebra and the quantum group U_q sl(2). The extension of this analysis in the bulk case involves considerable difficulties, since the U_q sl(2) symmetry is partly lost, whil","authors_text":"A. M. Gainutdinov, H. Saleur, N. Read","cross_cats":["cond-mat.stat-mech","math-ph","math.MP","math.QA"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-15T01:08:42Z","title":"Continuum limit and symmetries of the periodic gl(1|1) spin chain"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.3403","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":"sha256:30521499eb57aed96009567ed0350c015e429d1f283f2c8bb63b0b8019be05d4","target":"record","created_at":"2026-05-18T03:29:39Z","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":"c7fe03081cb65a10af567d21582746e5135f5416e9cc49bae4ec319eb6899749","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","math.QA"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-15T01:08:42Z","title_canon_sha256":"8c12428d9bc29e300c252545053ad3f504bb81a687413e23ac70e35adb1e30a9"},"schema_version":"1.0","source":{"id":"1112.3403","kind":"arxiv","version":3}},"canonical_sha256":"3123a94649235b25c78456abca9e5c1053360d4ab5bf64980566c28194409dcf","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3123a94649235b25c78456abca9e5c1053360d4ab5bf64980566c28194409dcf","first_computed_at":"2026-05-18T03:29:39.211709Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:29:39.211709Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"paDYQTUBbxhoZBpJGm6XVOiLmf14wS/z2P83mRC1Li+L4xPCt8bnJr4lx7RpAcwKpizKCTc1EFI+MWN97J8lBw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:29:39.212178Z","signed_message":"canonical_sha256_bytes"},"source_id":"1112.3403","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:30521499eb57aed96009567ed0350c015e429d1f283f2c8bb63b0b8019be05d4","sha256:65aeff2f698f4db7ac85fa615f28bf92f45af6a45096735fa1e4554987d9d632"],"state_sha256":"186ccda83180bfed250fb4c5802d2f7593bca083beb688a3c621631c46efb406"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TVSwkFwvD4OdRERDAEdGHPaGQy7Y49K7S5qd+5eJY0Ro/tHhL3o4nBqdyrfRIv/NBzqDnuhmjmmfwF1/irqrAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T21:16:13.475039Z","bundle_sha256":"d4de42e85ab8a5a46294f5de0233bd03e80f98286680323299d33d4315acd689"}}