{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:APRKLZ5IBZ5JQCVESXJH53OVPN","short_pith_number":"pith:APRKLZ5I","canonical_record":{"source":{"id":"2305.15561","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-24T20:49:39Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"17cf247c0057ca6a171a53062067070a8f7eb530d77da99f3a3a2fba52a2a10b","abstract_canon_sha256":"fc7995a4806a0e4c62856d66f0679d3d3e1eadb91f56998c0d65a94c6954eab8"},"schema_version":"1.0"},"canonical_sha256":"03e2a5e7a80e7a980aa495d27eedd57b642b8ff6ff224c7b1f4c1bfdf6c1cbea","source":{"kind":"arxiv","id":"2305.15561","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2305.15561","created_at":"2026-05-17T23:39:18Z"},{"alias_kind":"arxiv_version","alias_value":"2305.15561v1","created_at":"2026-05-17T23:39:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.15561","created_at":"2026-05-17T23:39:18Z"},{"alias_kind":"pith_short_12","alias_value":"APRKLZ5IBZ5J","created_at":"2026-05-18T12:33:33Z"},{"alias_kind":"pith_short_16","alias_value":"APRKLZ5IBZ5JQCVE","created_at":"2026-05-18T12:33:33Z"},{"alias_kind":"pith_short_8","alias_value":"APRKLZ5I","created_at":"2026-05-18T12:33:33Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:APRKLZ5IBZ5JQCVESXJH53OVPN","target":"record","payload":{"canonical_record":{"source":{"id":"2305.15561","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-24T20:49:39Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"17cf247c0057ca6a171a53062067070a8f7eb530d77da99f3a3a2fba52a2a10b","abstract_canon_sha256":"fc7995a4806a0e4c62856d66f0679d3d3e1eadb91f56998c0d65a94c6954eab8"},"schema_version":"1.0"},"canonical_sha256":"03e2a5e7a80e7a980aa495d27eedd57b642b8ff6ff224c7b1f4c1bfdf6c1cbea","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:39:18.528344Z","signature_b64":"cZ46FdRprPEhVOv8Z3Tc8LxRjPSx9Vc6mSHmjYU0YI2Uv3E1D9T0esLbH7qs5reXyVkpC3wPZS0l8RFP/B+tDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"03e2a5e7a80e7a980aa495d27eedd57b642b8ff6ff224c7b1f4c1bfdf6c1cbea","last_reissued_at":"2026-05-17T23:39:18.527679Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:39:18.527679Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2305.15561","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":"2026-05-17T23:39:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"y9+YFY1d5oIZSk1IFhwPmHA+4k97gwu/LpvA2YoMDz2AsVsO5D13QVHi4zJ8/CGRhRTKqGc0eUV/kdMhY9NkAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T17:16:58.720259Z"},"content_sha256":"f6bf1cd525d9e7cc5edf2beb9e7ddd72768266137dfff015f5a39652aa8a1f7b","schema_version":"1.0","event_id":"sha256:f6bf1cd525d9e7cc5edf2beb9e7ddd72768266137dfff015f5a39652aa8a1f7b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:APRKLZ5IBZ5JQCVESXJH53OVPN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum-field multiloop calculations in critical dynamics","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Ella Ivanova, Georgii Kalagov, Marina Komarova, Mikhail Nalimov","submitted_at":"2023-05-24T20:49:39Z","abstract_excerpt":"The quantum-field renormalization group method is one of the most efficient and powerful tools for studying critical and scaling phenomena in interacting many-particle systems. The multiloop Feynman diagrams underpin the specific implementation of the renormalization group program. In recent years, multiloop computation has had a significant breakthrough in both static and dynamic models of critical behavior. In the paper, we focus on the state-of-the-art computational techniques for critical dynamic diagrams and the results obtained with their help. The generic nature of the evaluated physica"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.15561","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":"2026-05-17T23:39:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xDIZP781n2O9C2vcAVSulqRdVhDVdEJonDVO7B7VRyX0kYQ5EXIyBjTV5GKVt/dnaCfIyrw/s34xqL3nhlwWAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T17:16:58.721015Z"},"content_sha256":"7cc3e8b952a365561894e1ad38560c466e4ccbbb976b5f04f30d7e34407203e4","schema_version":"1.0","event_id":"sha256:7cc3e8b952a365561894e1ad38560c466e4ccbbb976b5f04f30d7e34407203e4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/APRKLZ5IBZ5JQCVESXJH53OVPN/bundle.json","state_url":"https://pith.science/pith/APRKLZ5IBZ5JQCVESXJH53OVPN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/APRKLZ5IBZ5JQCVESXJH53OVPN/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":"2026-05-24T17:16:58Z","links":{"resolver":"https://pith.science/pith/APRKLZ5IBZ5JQCVESXJH53OVPN","bundle":"https://pith.science/pith/APRKLZ5IBZ5JQCVESXJH53OVPN/bundle.json","state":"https://pith.science/pith/APRKLZ5IBZ5JQCVESXJH53OVPN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/APRKLZ5IBZ5JQCVESXJH53OVPN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:APRKLZ5IBZ5JQCVESXJH53OVPN","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":"fc7995a4806a0e4c62856d66f0679d3d3e1eadb91f56998c0d65a94c6954eab8","cross_cats_sorted":["hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-24T20:49:39Z","title_canon_sha256":"17cf247c0057ca6a171a53062067070a8f7eb530d77da99f3a3a2fba52a2a10b"},"schema_version":"1.0","source":{"id":"2305.15561","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2305.15561","created_at":"2026-05-17T23:39:18Z"},{"alias_kind":"arxiv_version","alias_value":"2305.15561v1","created_at":"2026-05-17T23:39:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.15561","created_at":"2026-05-17T23:39:18Z"},{"alias_kind":"pith_short_12","alias_value":"APRKLZ5IBZ5J","created_at":"2026-05-18T12:33:33Z"},{"alias_kind":"pith_short_16","alias_value":"APRKLZ5IBZ5JQCVE","created_at":"2026-05-18T12:33:33Z"},{"alias_kind":"pith_short_8","alias_value":"APRKLZ5I","created_at":"2026-05-18T12:33:33Z"}],"graph_snapshots":[{"event_id":"sha256:7cc3e8b952a365561894e1ad38560c466e4ccbbb976b5f04f30d7e34407203e4","target":"graph","created_at":"2026-05-17T23:39:18Z","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":"The quantum-field renormalization group method is one of the most efficient and powerful tools for studying critical and scaling phenomena in interacting many-particle systems. The multiloop Feynman diagrams underpin the specific implementation of the renormalization group program. In recent years, multiloop computation has had a significant breakthrough in both static and dynamic models of critical behavior. In the paper, we focus on the state-of-the-art computational techniques for critical dynamic diagrams and the results obtained with their help. The generic nature of the evaluated physica","authors_text":"Ella Ivanova, Georgii Kalagov, Marina Komarova, Mikhail Nalimov","cross_cats":["hep-th"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-24T20:49:39Z","title":"Quantum-field multiloop calculations in critical dynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.15561","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:f6bf1cd525d9e7cc5edf2beb9e7ddd72768266137dfff015f5a39652aa8a1f7b","target":"record","created_at":"2026-05-17T23:39:18Z","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":"fc7995a4806a0e4c62856d66f0679d3d3e1eadb91f56998c0d65a94c6954eab8","cross_cats_sorted":["hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-24T20:49:39Z","title_canon_sha256":"17cf247c0057ca6a171a53062067070a8f7eb530d77da99f3a3a2fba52a2a10b"},"schema_version":"1.0","source":{"id":"2305.15561","kind":"arxiv","version":1}},"canonical_sha256":"03e2a5e7a80e7a980aa495d27eedd57b642b8ff6ff224c7b1f4c1bfdf6c1cbea","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"03e2a5e7a80e7a980aa495d27eedd57b642b8ff6ff224c7b1f4c1bfdf6c1cbea","first_computed_at":"2026-05-17T23:39:18.527679Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:39:18.527679Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"cZ46FdRprPEhVOv8Z3Tc8LxRjPSx9Vc6mSHmjYU0YI2Uv3E1D9T0esLbH7qs5reXyVkpC3wPZS0l8RFP/B+tDw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:39:18.528344Z","signed_message":"canonical_sha256_bytes"},"source_id":"2305.15561","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f6bf1cd525d9e7cc5edf2beb9e7ddd72768266137dfff015f5a39652aa8a1f7b","sha256:7cc3e8b952a365561894e1ad38560c466e4ccbbb976b5f04f30d7e34407203e4"],"state_sha256":"940d6c2089037da666d100cdd73322a45cdfdedf5b544e84813205539f9aced9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nLy9BOybnfyBwN/ao6OFfV69M6ulSh7TSbN1Bmi7OHNzcsrb1Eaw6F5im30kF6ccgolN2sF1YNOj6wuiJpebBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-24T17:16:58.723983Z","bundle_sha256":"893965148424c23abd815557ab813bf54c563a80316b39c2100f76fa16cb68f9"}}