{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:JISGZ2OHGXXVJ55LIBLZT5TLXE","short_pith_number":"pith:JISGZ2OH","schema_version":"1.0","canonical_sha256":"4a246ce9c735ef54f7ab405799f66bb922863501d6a4d291d60ec3c1aa50fc6d","source":{"kind":"arxiv","id":"1003.4952","version":3},"attestation_state":"computed","paper":{"title":"First Results from Lattice Simulation of the PWMM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-th","authors_text":"Greg van Anders, Simon Catterall","submitted_at":"2010-03-25T17:00:55Z","abstract_excerpt":"We present results of lattice simulations of the Plane Wave Matrix Model (PWMM). The PWMM is a theory of supersymmetric quantum mechanics that has a well-defined canonical ensemble. We simulate this theory by applying rational hybrid Monte Carlo techniques to a naive lattice action. We examine the strong coupling behaviour of the model focussing on the deconfinement transition."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1003.4952","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-03-25T17:00:55Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"50ca9834de307ae5ac4af3d1795837c6678cb420dc530420213de72bacda10e0","abstract_canon_sha256":"8ba8d84dbbd50b1f845a524a263549c8c574e44c0fb20a14822464186648c00b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:34:27.649095Z","signature_b64":"uWMcigiMhKNBMW+5ApSzBKMGVf/U5MgNOe99rgZikCsiLJugXQBpZN6Fu9pyEGXL7Tyz1qhNkVdxazyOSdcUCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4a246ce9c735ef54f7ab405799f66bb922863501d6a4d291d60ec3c1aa50fc6d","last_reissued_at":"2026-05-18T04:34:27.648341Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:34:27.648341Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"First Results from Lattice Simulation of the PWMM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-th","authors_text":"Greg van Anders, Simon Catterall","submitted_at":"2010-03-25T17:00:55Z","abstract_excerpt":"We present results of lattice simulations of the Plane Wave Matrix Model (PWMM). The PWMM is a theory of supersymmetric quantum mechanics that has a well-defined canonical ensemble. We simulate this theory by applying rational hybrid Monte Carlo techniques to a naive lattice action. We examine the strong coupling behaviour of the model focussing on the deconfinement transition."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.4952","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1003.4952","created_at":"2026-05-18T04:34:27.648467+00:00"},{"alias_kind":"arxiv_version","alias_value":"1003.4952v3","created_at":"2026-05-18T04:34:27.648467+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.4952","created_at":"2026-05-18T04:34:27.648467+00:00"},{"alias_kind":"pith_short_12","alias_value":"JISGZ2OHGXXV","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_16","alias_value":"JISGZ2OHGXXVJ55L","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_8","alias_value":"JISGZ2OH","created_at":"2026-05-18T12:26:09.077623+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JISGZ2OHGXXVJ55LIBLZT5TLXE","json":"https://pith.science/pith/JISGZ2OHGXXVJ55LIBLZT5TLXE.json","graph_json":"https://pith.science/api/pith-number/JISGZ2OHGXXVJ55LIBLZT5TLXE/graph.json","events_json":"https://pith.science/api/pith-number/JISGZ2OHGXXVJ55LIBLZT5TLXE/events.json","paper":"https://pith.science/paper/JISGZ2OH"},"agent_actions":{"view_html":"https://pith.science/pith/JISGZ2OHGXXVJ55LIBLZT5TLXE","download_json":"https://pith.science/pith/JISGZ2OHGXXVJ55LIBLZT5TLXE.json","view_paper":"https://pith.science/paper/JISGZ2OH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1003.4952&json=true","fetch_graph":"https://pith.science/api/pith-number/JISGZ2OHGXXVJ55LIBLZT5TLXE/graph.json","fetch_events":"https://pith.science/api/pith-number/JISGZ2OHGXXVJ55LIBLZT5TLXE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JISGZ2OHGXXVJ55LIBLZT5TLXE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JISGZ2OHGXXVJ55LIBLZT5TLXE/action/storage_attestation","attest_author":"https://pith.science/pith/JISGZ2OHGXXVJ55LIBLZT5TLXE/action/author_attestation","sign_citation":"https://pith.science/pith/JISGZ2OHGXXVJ55LIBLZT5TLXE/action/citation_signature","submit_replication":"https://pith.science/pith/JISGZ2OHGXXVJ55LIBLZT5TLXE/action/replication_record"}},"created_at":"2026-05-18T04:34:27.648467+00:00","updated_at":"2026-05-18T04:34:27.648467+00:00"}