{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:VOJP4H3KAEPJBHTQ3XQFIFKLZT","short_pith_number":"pith:VOJP4H3K","schema_version":"1.0","canonical_sha256":"ab92fe1f6a011e909e70dde054154bcce2e069b1c68a01d0592eecf2c5c92e40","source":{"kind":"arxiv","id":"0706.3517","version":2},"attestation_state":"computed","paper":{"title":"Phase structure of matrix quantum mechanics at finite temperature","license":"","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-th","authors_text":"Jun Nishimura (KEK, Naoyuki Kawahara (KEK), Shingo Takeuchi (SOKENDAI), SOKENDAI)","submitted_at":"2007-06-25T14:45:57Z","abstract_excerpt":"We study matrix quantum mechanics at finite temperature by Monte Carlo simulation. The model is obtained by dimensionally reducing 10d U(N) pure Yang-Mills theory to 1d. Following Aharony et al., one can view the same model as describing the high temperature regime of (1+1)d U(N) super Yang-Mills theory on a circle. In this interpretation an analog of the deconfinement transition was conjectured to be a continuation of the black-hole/black-string transition in the dual gravity theory. Our detailed analysis in the critical regime up to N=32 suggests the existence of the non-uniform phase, in wh"},"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":"0706.3517","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2007-06-25T14:45:57Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"dad201eb101fe27620ae1e9f29f2e4c996c9c660a628b750436772052d3f0981","abstract_canon_sha256":"212b76fd0ec1718bd896ce881c9e88ccdb62bafa3c879abb1c3f969ea8adb574"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:21:17.781386Z","signature_b64":"pBMYQq06ET7FzoYekR97IjPcjUYQf/i0Yu+zUjY15iFjVNtSZyfBSJ8mam+v/lgDkP7RVK0hslusptWAODM8DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ab92fe1f6a011e909e70dde054154bcce2e069b1c68a01d0592eecf2c5c92e40","last_reissued_at":"2026-07-04T15:21:17.780973Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:21:17.780973Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phase structure of matrix quantum mechanics at finite temperature","license":"","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-th","authors_text":"Jun Nishimura (KEK, Naoyuki Kawahara (KEK), Shingo Takeuchi (SOKENDAI), SOKENDAI)","submitted_at":"2007-06-25T14:45:57Z","abstract_excerpt":"We study matrix quantum mechanics at finite temperature by Monte Carlo simulation. The model is obtained by dimensionally reducing 10d U(N) pure Yang-Mills theory to 1d. Following Aharony et al., one can view the same model as describing the high temperature regime of (1+1)d U(N) super Yang-Mills theory on a circle. In this interpretation an analog of the deconfinement transition was conjectured to be a continuation of the black-hole/black-string transition in the dual gravity theory. Our detailed analysis in the critical regime up to N=32 suggests the existence of the non-uniform phase, in wh"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0706.3517","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0706.3517/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"0706.3517","created_at":"2026-07-04T15:21:17.781040+00:00"},{"alias_kind":"arxiv_version","alias_value":"0706.3517v2","created_at":"2026-07-04T15:21:17.781040+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0706.3517","created_at":"2026-07-04T15:21:17.781040+00:00"},{"alias_kind":"pith_short_12","alias_value":"VOJP4H3KAEPJ","created_at":"2026-07-04T15:21:17.781040+00:00"},{"alias_kind":"pith_short_16","alias_value":"VOJP4H3KAEPJBHTQ","created_at":"2026-07-04T15:21:17.781040+00:00"},{"alias_kind":"pith_short_8","alias_value":"VOJP4H3K","created_at":"2026-07-04T15:21:17.781040+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2607.08481","citing_title":"Gram--Wishart--Stiefel formulation of the $N=2$, large--$d$ gauge theory in 1D","ref_index":46,"is_internal_anchor":true},{"citing_arxiv_id":"2605.25647","citing_title":"Endpoint formulation and Molien--Weyl structure for the \\(N=2\\), large--\\(d\\) BFSS/BMN models","ref_index":46,"is_internal_anchor":true},{"citing_arxiv_id":"2606.17758","citing_title":"A Double--Scaling Large--\\(d\\) Saddle of BFSS/BMN Matrix Quantum Mechanics","ref_index":57,"is_internal_anchor":true},{"citing_arxiv_id":"2605.04621","citing_title":"Molien--Weyl Singlet Counting and BFSS$_2$--Factorization in Gaussian Matrix QM","ref_index":49,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06985","citing_title":"Real-Time Quantum Dynamics on the Fuzzy Sphere: Chaos and Entanglement","ref_index":21,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VOJP4H3KAEPJBHTQ3XQFIFKLZT","json":"https://pith.science/pith/VOJP4H3KAEPJBHTQ3XQFIFKLZT.json","graph_json":"https://pith.science/api/pith-number/VOJP4H3KAEPJBHTQ3XQFIFKLZT/graph.json","events_json":"https://pith.science/api/pith-number/VOJP4H3KAEPJBHTQ3XQFIFKLZT/events.json","paper":"https://pith.science/paper/VOJP4H3K"},"agent_actions":{"view_html":"https://pith.science/pith/VOJP4H3KAEPJBHTQ3XQFIFKLZT","download_json":"https://pith.science/pith/VOJP4H3KAEPJBHTQ3XQFIFKLZT.json","view_paper":"https://pith.science/paper/VOJP4H3K","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0706.3517&json=true","fetch_graph":"https://pith.science/api/pith-number/VOJP4H3KAEPJBHTQ3XQFIFKLZT/graph.json","fetch_events":"https://pith.science/api/pith-number/VOJP4H3KAEPJBHTQ3XQFIFKLZT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VOJP4H3KAEPJBHTQ3XQFIFKLZT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VOJP4H3KAEPJBHTQ3XQFIFKLZT/action/storage_attestation","attest_author":"https://pith.science/pith/VOJP4H3KAEPJBHTQ3XQFIFKLZT/action/author_attestation","sign_citation":"https://pith.science/pith/VOJP4H3KAEPJBHTQ3XQFIFKLZT/action/citation_signature","submit_replication":"https://pith.science/pith/VOJP4H3KAEPJBHTQ3XQFIFKLZT/action/replication_record"}},"created_at":"2026-07-04T15:21:17.781040+00:00","updated_at":"2026-07-04T15:21:17.781040+00:00"}