{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:6DVBQOFIJYG2NIJC2YGNONGNDC","short_pith_number":"pith:6DVBQOFI","canonical_record":{"source":{"id":"1412.8494","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-29T21:45:45Z","cross_cats_sorted":[],"title_canon_sha256":"201209815d52e4eb0092d68d98fea9ea570550447efbe62ae8876ea9e782436f","abstract_canon_sha256":"45713cf306171e0c957094640e1c6861af7f716b741144eb65a010bf4a7d2604"},"schema_version":"1.0"},"canonical_sha256":"f0ea1838a84e0da6a122d60cd734cd1886c83506196289a6a393e2952bf8b0b6","source":{"kind":"arxiv","id":"1412.8494","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.8494","created_at":"2026-05-18T00:30:50Z"},{"alias_kind":"arxiv_version","alias_value":"1412.8494v1","created_at":"2026-05-18T00:30:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.8494","created_at":"2026-05-18T00:30:50Z"},{"alias_kind":"pith_short_12","alias_value":"6DVBQOFIJYG2","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6DVBQOFIJYG2NIJC","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6DVBQOFI","created_at":"2026-05-18T12:28:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:6DVBQOFIJYG2NIJC2YGNONGNDC","target":"record","payload":{"canonical_record":{"source":{"id":"1412.8494","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-29T21:45:45Z","cross_cats_sorted":[],"title_canon_sha256":"201209815d52e4eb0092d68d98fea9ea570550447efbe62ae8876ea9e782436f","abstract_canon_sha256":"45713cf306171e0c957094640e1c6861af7f716b741144eb65a010bf4a7d2604"},"schema_version":"1.0"},"canonical_sha256":"f0ea1838a84e0da6a122d60cd734cd1886c83506196289a6a393e2952bf8b0b6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:30:50.923208Z","signature_b64":"d8PZp0UmSdm+ILCWe/UJEhwvOYJ1Vl5ujgAm9FI5SkV5cXLSdnU9iqpJTyL81JtOG38G41L4KqV3eIhbv2IcAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f0ea1838a84e0da6a122d60cd734cd1886c83506196289a6a393e2952bf8b0b6","last_reissued_at":"2026-05-18T00:30:50.922750Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:30:50.922750Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1412.8494","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:30:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OR0YUQdAjMuIANHt2OXrLPUC+hnQ5Ex8JbceLXjbGxdG26aHpmqEMEkXKzf5V/b4ugpBl5dO8nlq/x8pDSz5Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T23:55:21.401349Z"},"content_sha256":"26e1398fe1cbc0be8c14d20bad4be9f3d51575527305e1f958228ce42bf3c062","schema_version":"1.0","event_id":"sha256:26e1398fe1cbc0be8c14d20bad4be9f3d51575527305e1f958228ce42bf3c062"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:6DVBQOFIJYG2NIJC2YGNONGNDC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Finite-Volume Spectra of the Lee-Yang Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Omar el Deeb, Paul A. Pearce, Zoltan Bajnok","submitted_at":"2014-12-29T21:45:45Z","abstract_excerpt":"We consider the non-unitary Lee-Yang minimal model ${\\cal M}(2,5)$ in three different finite geometries: (i) on the interval with integrable boundary conditions labelled by the Kac labels $(r,s)=(1,1),(1,2)$, (ii) on the circle with periodic boundary conditions and (iii) on the periodic circle including an integrable purely transmitting defect. We apply $\\varphi_{1,3}$ integrable perturbations on the boundary and on the defect and describe the flow of the spectrum. Adding a $\\Phi_{1,3}$ integrable perturbation to move off-criticality in the bulk, we determine the finite size spectrum of the ma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.8494","kind":"arxiv","version":1},"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":"2026-05-18T00:30:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WL8+Kkc20CmPHUwlJy1kO3WOEPjjMoa182XYfqGqrucAYlOowMD+XZDkvT0fKco5fvs7F3b+d0V4PpmfPbiqAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T23:55:21.402317Z"},"content_sha256":"68e744cd80c1a819ffe97b733186208070c8d63ac8704c6421e23391011cd07f","schema_version":"1.0","event_id":"sha256:68e744cd80c1a819ffe97b733186208070c8d63ac8704c6421e23391011cd07f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6DVBQOFIJYG2NIJC2YGNONGNDC/bundle.json","state_url":"https://pith.science/pith/6DVBQOFIJYG2NIJC2YGNONGNDC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6DVBQOFIJYG2NIJC2YGNONGNDC/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":"2026-08-04T23:55:21Z","links":{"resolver":"https://pith.science/pith/6DVBQOFIJYG2NIJC2YGNONGNDC","bundle":"https://pith.science/pith/6DVBQOFIJYG2NIJC2YGNONGNDC/bundle.json","state":"https://pith.science/pith/6DVBQOFIJYG2NIJC2YGNONGNDC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6DVBQOFIJYG2NIJC2YGNONGNDC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:6DVBQOFIJYG2NIJC2YGNONGNDC","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":"45713cf306171e0c957094640e1c6861af7f716b741144eb65a010bf4a7d2604","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-29T21:45:45Z","title_canon_sha256":"201209815d52e4eb0092d68d98fea9ea570550447efbe62ae8876ea9e782436f"},"schema_version":"1.0","source":{"id":"1412.8494","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.8494","created_at":"2026-05-18T00:30:50Z"},{"alias_kind":"arxiv_version","alias_value":"1412.8494v1","created_at":"2026-05-18T00:30:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.8494","created_at":"2026-05-18T00:30:50Z"},{"alias_kind":"pith_short_12","alias_value":"6DVBQOFIJYG2","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6DVBQOFIJYG2NIJC","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6DVBQOFI","created_at":"2026-05-18T12:28:16Z"}],"graph_snapshots":[{"event_id":"sha256:68e744cd80c1a819ffe97b733186208070c8d63ac8704c6421e23391011cd07f","target":"graph","created_at":"2026-05-18T00:30:50Z","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 consider the non-unitary Lee-Yang minimal model ${\\cal M}(2,5)$ in three different finite geometries: (i) on the interval with integrable boundary conditions labelled by the Kac labels $(r,s)=(1,1),(1,2)$, (ii) on the circle with periodic boundary conditions and (iii) on the periodic circle including an integrable purely transmitting defect. We apply $\\varphi_{1,3}$ integrable perturbations on the boundary and on the defect and describe the flow of the spectrum. Adding a $\\Phi_{1,3}$ integrable perturbation to move off-criticality in the bulk, we determine the finite size spectrum of the ma","authors_text":"Omar el Deeb, Paul A. Pearce, Zoltan Bajnok","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-29T21:45:45Z","title":"Finite-Volume Spectra of the Lee-Yang Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.8494","kind":"arxiv","version":1},"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":"sha256:26e1398fe1cbc0be8c14d20bad4be9f3d51575527305e1f958228ce42bf3c062","target":"record","created_at":"2026-05-18T00:30:50Z","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":"45713cf306171e0c957094640e1c6861af7f716b741144eb65a010bf4a7d2604","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-29T21:45:45Z","title_canon_sha256":"201209815d52e4eb0092d68d98fea9ea570550447efbe62ae8876ea9e782436f"},"schema_version":"1.0","source":{"id":"1412.8494","kind":"arxiv","version":1}},"canonical_sha256":"f0ea1838a84e0da6a122d60cd734cd1886c83506196289a6a393e2952bf8b0b6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f0ea1838a84e0da6a122d60cd734cd1886c83506196289a6a393e2952bf8b0b6","first_computed_at":"2026-05-18T00:30:50.922750Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:30:50.922750Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"d8PZp0UmSdm+ILCWe/UJEhwvOYJ1Vl5ujgAm9FI5SkV5cXLSdnU9iqpJTyL81JtOG38G41L4KqV3eIhbv2IcAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:30:50.923208Z","signed_message":"canonical_sha256_bytes"},"source_id":"1412.8494","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:26e1398fe1cbc0be8c14d20bad4be9f3d51575527305e1f958228ce42bf3c062","sha256:68e744cd80c1a819ffe97b733186208070c8d63ac8704c6421e23391011cd07f"],"state_sha256":"e6ca6bb27c0d6e34417bec5e0658e0a44aab83b05bde36b638af4d429eec3447"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cp+FNYlh9+XifnB/AtTyc8RlqE5KCl3mAopuXLx/022iull2emLUd3juKAx0P9czXfZ2Cy1fcT9P2QvJzHh8Dw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T23:55:21.407196Z","bundle_sha256":"cf2c8d5dd06901a065c5de899df09e31fb66c270bfc481dc09fd0ae373cbeb67"}}