{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:XFKU66FJBYINSHJOBLTIS36ZL2","short_pith_number":"pith:XFKU66FJ","canonical_record":{"source":{"id":"1801.06132","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-01-18T17:14:29Z","cross_cats_sorted":[],"title_canon_sha256":"9965728216f95118773f31329be804569dec8b549de582176220370afcf6b0f0","abstract_canon_sha256":"a954c9b344079fe03e8dfb07d41165ce98df3338671d37762a4db70457e7b0aa"},"schema_version":"1.0"},"canonical_sha256":"b9554f78a90e10d91d2e0ae6896fd95eb68a7625a593e3d2a3fee1b37056497c","source":{"kind":"arxiv","id":"1801.06132","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.06132","created_at":"2026-05-18T00:18:11Z"},{"alias_kind":"arxiv_version","alias_value":"1801.06132v2","created_at":"2026-05-18T00:18:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.06132","created_at":"2026-05-18T00:18:11Z"},{"alias_kind":"pith_short_12","alias_value":"XFKU66FJBYIN","created_at":"2026-05-18T12:33:01Z"},{"alias_kind":"pith_short_16","alias_value":"XFKU66FJBYINSHJO","created_at":"2026-05-18T12:33:01Z"},{"alias_kind":"pith_short_8","alias_value":"XFKU66FJ","created_at":"2026-05-18T12:33:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:XFKU66FJBYINSHJOBLTIS36ZL2","target":"record","payload":{"canonical_record":{"source":{"id":"1801.06132","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-01-18T17:14:29Z","cross_cats_sorted":[],"title_canon_sha256":"9965728216f95118773f31329be804569dec8b549de582176220370afcf6b0f0","abstract_canon_sha256":"a954c9b344079fe03e8dfb07d41165ce98df3338671d37762a4db70457e7b0aa"},"schema_version":"1.0"},"canonical_sha256":"b9554f78a90e10d91d2e0ae6896fd95eb68a7625a593e3d2a3fee1b37056497c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:18:11.625784Z","signature_b64":"92+92fMQc0/EiO1H4eJoYZj1LsDYJAg9213XPTPZr8eeqBGtcy+2NIDzLZXvNUZC+Wh7NDfyFFifbTaacOt1AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b9554f78a90e10d91d2e0ae6896fd95eb68a7625a593e3d2a3fee1b37056497c","last_reissued_at":"2026-05-18T00:18:11.625161Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:18:11.625161Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1801.06132","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":"2026-05-18T00:18:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9bqFtA1k/l9nQ8vF35bZxOJTRmnUHOVASfztrGsTdJ6KOqEGes8sk8GbXv0iDEe5PLSeNSV9658aIGzICp1YAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T00:01:23.648952Z"},"content_sha256":"27d7c37881b8dd3543db614380e24747c71a30684ec88a195fb2861f9427ce87","schema_version":"1.0","event_id":"sha256:27d7c37881b8dd3543db614380e24747c71a30684ec88a195fb2861f9427ce87"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:XFKU66FJBYINSHJOBLTIS36ZL2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Scaling properties of multiscale equilibration","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Michael G. Endres, William Detmold","submitted_at":"2018-01-18T17:14:29Z","abstract_excerpt":"We investigate the lattice spacing dependence of the equilibration time for a recently proposed multiscale thermalization algorithm for Markov chain Monte Carlo simulations. The algorithm uses a renormalization-group matched coarse lattice action and prolongation operation to rapidly thermalize decorrelated initial configurations for evolution using a corresponding target lattice action defined at a finer scale. Focusing on non-topological long-distance observables in pure SU(3) gauge theory, we provide quantitative evidence that the slow modes of the Markov process, which provide the dominant"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.06132","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":"2026-05-18T00:18:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"u3Zl3cbXWFZUzeBCFAaCizm+P4WKvmQEfxj8X+lw3pkO6U6lddqgLGhUAa9Razt3npkPha2dsiL/ju7cMVfjDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T00:01:23.649684Z"},"content_sha256":"d10d675582fc21eb0843c40aa1c841d511ae17c31d162f567f3f3b82699e69fe","schema_version":"1.0","event_id":"sha256:d10d675582fc21eb0843c40aa1c841d511ae17c31d162f567f3f3b82699e69fe"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XFKU66FJBYINSHJOBLTIS36ZL2/bundle.json","state_url":"https://pith.science/pith/XFKU66FJBYINSHJOBLTIS36ZL2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XFKU66FJBYINSHJOBLTIS36ZL2/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":"2026-05-26T00:01:23Z","links":{"resolver":"https://pith.science/pith/XFKU66FJBYINSHJOBLTIS36ZL2","bundle":"https://pith.science/pith/XFKU66FJBYINSHJOBLTIS36ZL2/bundle.json","state":"https://pith.science/pith/XFKU66FJBYINSHJOBLTIS36ZL2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XFKU66FJBYINSHJOBLTIS36ZL2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:XFKU66FJBYINSHJOBLTIS36ZL2","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":"a954c9b344079fe03e8dfb07d41165ce98df3338671d37762a4db70457e7b0aa","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-01-18T17:14:29Z","title_canon_sha256":"9965728216f95118773f31329be804569dec8b549de582176220370afcf6b0f0"},"schema_version":"1.0","source":{"id":"1801.06132","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.06132","created_at":"2026-05-18T00:18:11Z"},{"alias_kind":"arxiv_version","alias_value":"1801.06132v2","created_at":"2026-05-18T00:18:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.06132","created_at":"2026-05-18T00:18:11Z"},{"alias_kind":"pith_short_12","alias_value":"XFKU66FJBYIN","created_at":"2026-05-18T12:33:01Z"},{"alias_kind":"pith_short_16","alias_value":"XFKU66FJBYINSHJO","created_at":"2026-05-18T12:33:01Z"},{"alias_kind":"pith_short_8","alias_value":"XFKU66FJ","created_at":"2026-05-18T12:33:01Z"}],"graph_snapshots":[{"event_id":"sha256:d10d675582fc21eb0843c40aa1c841d511ae17c31d162f567f3f3b82699e69fe","target":"graph","created_at":"2026-05-18T00:18:11Z","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 investigate the lattice spacing dependence of the equilibration time for a recently proposed multiscale thermalization algorithm for Markov chain Monte Carlo simulations. The algorithm uses a renormalization-group matched coarse lattice action and prolongation operation to rapidly thermalize decorrelated initial configurations for evolution using a corresponding target lattice action defined at a finer scale. Focusing on non-topological long-distance observables in pure SU(3) gauge theory, we provide quantitative evidence that the slow modes of the Markov process, which provide the dominant","authors_text":"Michael G. Endres, William Detmold","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-01-18T17:14:29Z","title":"Scaling properties of multiscale equilibration"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.06132","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":"sha256:27d7c37881b8dd3543db614380e24747c71a30684ec88a195fb2861f9427ce87","target":"record","created_at":"2026-05-18T00:18:11Z","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":"a954c9b344079fe03e8dfb07d41165ce98df3338671d37762a4db70457e7b0aa","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-01-18T17:14:29Z","title_canon_sha256":"9965728216f95118773f31329be804569dec8b549de582176220370afcf6b0f0"},"schema_version":"1.0","source":{"id":"1801.06132","kind":"arxiv","version":2}},"canonical_sha256":"b9554f78a90e10d91d2e0ae6896fd95eb68a7625a593e3d2a3fee1b37056497c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b9554f78a90e10d91d2e0ae6896fd95eb68a7625a593e3d2a3fee1b37056497c","first_computed_at":"2026-05-18T00:18:11.625161Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:18:11.625161Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"92+92fMQc0/EiO1H4eJoYZj1LsDYJAg9213XPTPZr8eeqBGtcy+2NIDzLZXvNUZC+Wh7NDfyFFifbTaacOt1AQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:18:11.625784Z","signed_message":"canonical_sha256_bytes"},"source_id":"1801.06132","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:27d7c37881b8dd3543db614380e24747c71a30684ec88a195fb2861f9427ce87","sha256:d10d675582fc21eb0843c40aa1c841d511ae17c31d162f567f3f3b82699e69fe"],"state_sha256":"7ad8bb73450cb34ee3f24a09141c84fd706789f13818b128e34d51310691038c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"w37ZxuGdo/y68UDL4Sl+8jhhmAE+7T7el7swJFNmEB11ekHETac2N4whhZgxrbPng+Js4rmnAMpGqmcfBEHvAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T00:01:23.652529Z","bundle_sha256":"7168e807b76a6d29c492339f35a596099cb8f821908a1a4008bc8a7bfb701056"}}