{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:DDFLRYAULLKHOP37Z4X72ZOIU6","short_pith_number":"pith:DDFLRYAU","canonical_record":{"source":{"id":"1308.4333","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2013-08-20T15:52:31Z","cross_cats_sorted":["cond-mat.stat-mech","hep-th","math-ph","math.MP"],"title_canon_sha256":"416a670a4b5479e5b4accfb35cc2f5306934cf59d9268498135e72d9df3ff191","abstract_canon_sha256":"53f8713825d213de42246ef895026d3cfc0512042f559b2dde7d894059cfcbbd"},"schema_version":"1.0"},"canonical_sha256":"18cab8e0145ad4773f7fcf2ffd65c8a7928a120951c6af767fcfa41bca5c6408","source":{"kind":"arxiv","id":"1308.4333","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1308.4333","created_at":"2026-05-18T02:54:54Z"},{"alias_kind":"arxiv_version","alias_value":"1308.4333v2","created_at":"2026-05-18T02:54:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.4333","created_at":"2026-05-18T02:54:54Z"},{"alias_kind":"pith_short_12","alias_value":"DDFLRYAULLKH","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_16","alias_value":"DDFLRYAULLKHOP37","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_8","alias_value":"DDFLRYAU","created_at":"2026-05-18T12:27:40Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:DDFLRYAULLKHOP37Z4X72ZOIU6","target":"record","payload":{"canonical_record":{"source":{"id":"1308.4333","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2013-08-20T15:52:31Z","cross_cats_sorted":["cond-mat.stat-mech","hep-th","math-ph","math.MP"],"title_canon_sha256":"416a670a4b5479e5b4accfb35cc2f5306934cf59d9268498135e72d9df3ff191","abstract_canon_sha256":"53f8713825d213de42246ef895026d3cfc0512042f559b2dde7d894059cfcbbd"},"schema_version":"1.0"},"canonical_sha256":"18cab8e0145ad4773f7fcf2ffd65c8a7928a120951c6af767fcfa41bca5c6408","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:54:54.405069Z","signature_b64":"G/r7aAYB/LBd7zyhqaAPuNdka1MfB0vP7s8wVo7OzVcl8hhe9UnpILanPCJi3HuTkhDajo6woRH/+dRNVFt9Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"18cab8e0145ad4773f7fcf2ffd65c8a7928a120951c6af767fcfa41bca5c6408","last_reissued_at":"2026-05-18T02:54:54.404656Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:54:54.404656Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1308.4333","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":"2026-05-18T02:54:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1gBcA6RbjAnrZ7c4XkG+xZF0pk09uenvbWdGmeeLaejvkbDaHivXvmjEteJ8sHt4ldzmu/Bm7BcAjbA7MY14CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T20:13:34.311515Z"},"content_sha256":"a5a0053a79f5a422135be4175e5148f7bf2c7bfaa961843baa38f08c5d7b0c73","schema_version":"1.0","event_id":"sha256:a5a0053a79f5a422135be4175e5148f7bf2c7bfaa961843baa38f08c5d7b0c73"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:DDFLRYAULLKHOP37Z4X72ZOIU6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Phase diagram and the strong-coupling fixed point in the disordered O(n) loop model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","hep-th","math-ph","math.MP"],"primary_cat":"cond-mat.dis-nn","authors_text":"Hirohiko Shimada, Jesper Lykke Jacobsen, Yoshitomo Kamiya","submitted_at":"2013-08-20T15:52:31Z","abstract_excerpt":"We numerically study the phase diagram and critical properties of the two-dimensional disordered O(n) loop model by using the transfer matrix and the worm Monte Carlo methods. The renormalization group flow is extracted from the landscape of the effective central charge obtained by the transfer matrix method based on the Zamolodchikov's C-theorem. We find a line of random fixed points (FPs) for $n_c < n <1$, with $n_c \\sim 0.5$, for which the central charge and critical exponents agree well with the results of the $1-n$ perturbative expansion. Furthermore, for $n> n_c$, we find a line of multi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.4333","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":"2026-05-18T02:54:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FK0zv2XwecDEGY/FxoPEx5XgXT95cHfJwvjRhFPEiEnoQbbcrZ+nAhAQGPvltfzr5msooAbR98tG+akkTkreDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T20:13:34.312223Z"},"content_sha256":"278ad23c7ff81e843786561ce2a15b123a8ff34c0bc9a2843fd357f2584e3dca","schema_version":"1.0","event_id":"sha256:278ad23c7ff81e843786561ce2a15b123a8ff34c0bc9a2843fd357f2584e3dca"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DDFLRYAULLKHOP37Z4X72ZOIU6/bundle.json","state_url":"https://pith.science/pith/DDFLRYAULLKHOP37Z4X72ZOIU6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DDFLRYAULLKHOP37Z4X72ZOIU6/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":"2026-05-31T20:13:34Z","links":{"resolver":"https://pith.science/pith/DDFLRYAULLKHOP37Z4X72ZOIU6","bundle":"https://pith.science/pith/DDFLRYAULLKHOP37Z4X72ZOIU6/bundle.json","state":"https://pith.science/pith/DDFLRYAULLKHOP37Z4X72ZOIU6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DDFLRYAULLKHOP37Z4X72ZOIU6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:DDFLRYAULLKHOP37Z4X72ZOIU6","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":"53f8713825d213de42246ef895026d3cfc0512042f559b2dde7d894059cfcbbd","cross_cats_sorted":["cond-mat.stat-mech","hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2013-08-20T15:52:31Z","title_canon_sha256":"416a670a4b5479e5b4accfb35cc2f5306934cf59d9268498135e72d9df3ff191"},"schema_version":"1.0","source":{"id":"1308.4333","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1308.4333","created_at":"2026-05-18T02:54:54Z"},{"alias_kind":"arxiv_version","alias_value":"1308.4333v2","created_at":"2026-05-18T02:54:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.4333","created_at":"2026-05-18T02:54:54Z"},{"alias_kind":"pith_short_12","alias_value":"DDFLRYAULLKH","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_16","alias_value":"DDFLRYAULLKHOP37","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_8","alias_value":"DDFLRYAU","created_at":"2026-05-18T12:27:40Z"}],"graph_snapshots":[{"event_id":"sha256:278ad23c7ff81e843786561ce2a15b123a8ff34c0bc9a2843fd357f2584e3dca","target":"graph","created_at":"2026-05-18T02:54:54Z","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 numerically study the phase diagram and critical properties of the two-dimensional disordered O(n) loop model by using the transfer matrix and the worm Monte Carlo methods. The renormalization group flow is extracted from the landscape of the effective central charge obtained by the transfer matrix method based on the Zamolodchikov's C-theorem. We find a line of random fixed points (FPs) for $n_c < n <1$, with $n_c \\sim 0.5$, for which the central charge and critical exponents agree well with the results of the $1-n$ perturbative expansion. Furthermore, for $n> n_c$, we find a line of multi","authors_text":"Hirohiko Shimada, Jesper Lykke Jacobsen, Yoshitomo Kamiya","cross_cats":["cond-mat.stat-mech","hep-th","math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2013-08-20T15:52:31Z","title":"Phase diagram and the strong-coupling fixed point in the disordered O(n) loop model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.4333","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:a5a0053a79f5a422135be4175e5148f7bf2c7bfaa961843baa38f08c5d7b0c73","target":"record","created_at":"2026-05-18T02:54:54Z","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":"53f8713825d213de42246ef895026d3cfc0512042f559b2dde7d894059cfcbbd","cross_cats_sorted":["cond-mat.stat-mech","hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2013-08-20T15:52:31Z","title_canon_sha256":"416a670a4b5479e5b4accfb35cc2f5306934cf59d9268498135e72d9df3ff191"},"schema_version":"1.0","source":{"id":"1308.4333","kind":"arxiv","version":2}},"canonical_sha256":"18cab8e0145ad4773f7fcf2ffd65c8a7928a120951c6af767fcfa41bca5c6408","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"18cab8e0145ad4773f7fcf2ffd65c8a7928a120951c6af767fcfa41bca5c6408","first_computed_at":"2026-05-18T02:54:54.404656Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:54:54.404656Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"G/r7aAYB/LBd7zyhqaAPuNdka1MfB0vP7s8wVo7OzVcl8hhe9UnpILanPCJi3HuTkhDajo6woRH/+dRNVFt9Cg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:54:54.405069Z","signed_message":"canonical_sha256_bytes"},"source_id":"1308.4333","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a5a0053a79f5a422135be4175e5148f7bf2c7bfaa961843baa38f08c5d7b0c73","sha256:278ad23c7ff81e843786561ce2a15b123a8ff34c0bc9a2843fd357f2584e3dca"],"state_sha256":"c567e893d65eae8ca917d0b52a0cd434460c7e50777fe9ec5df6dd124cc25af8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bJ6BWjoPqhCpCl6qVKVIZBO0/u77gj43WzT2dBdpUQT6LKwz7vnDeq+wi+D1XVuMsAkECRkK+AhRShpwi2FFBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T20:13:34.315438Z","bundle_sha256":"8efddb1936a7a84819fc9be54f1c21e2930ac08ed33167c917d0d7a4da127ded"}}