{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:CMUN6YKXDHSM54U5D6HEPOKJ34","short_pith_number":"pith:CMUN6YKX","schema_version":"1.0","canonical_sha256":"1328df615719e4cef29d1f8e47b949df05331344ec4db122f5a39db8336d0310","source":{"kind":"arxiv","id":"0807.0792","version":2},"attestation_state":"computed","paper":{"title":"Phase diagram of SU(2) with 2 flavors of dynamical adjoint quarks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-lat","authors_text":"Francesco Sannino, Joel Giedt, Joe Schneible, Simon Catterall","submitted_at":"2008-07-04T17:10:55Z","abstract_excerpt":"We report on numerical simulations of SU(2) lattice gauge theory with two flavors of light dynamical quarks in the adjoint of the gauge group. The dynamics of this theory is thought to be very different from QCD -- the theory exhibiting conformal or near conformal behavior in the infrared. We make a high resolution survey of the phase diagram of this model in the plane of the bare coupling and quark mass on lattices of size 8^3 \\times 16. Our simulations reveal a line of first order phase transitions extending from beta=0 to beta=beta_c \\sim 2.0. For beta > beta_c the phase boundary is no long"},"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":"0807.0792","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2008-07-04T17:10:55Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"ee26c1b118ab2e1406fddfb8efcbdfe4df43419f82d3d59c42e27e40f458160d","abstract_canon_sha256":"bb4653792215a5729a851ed136c2151a40cbaba07aa42ac07d9f3d3a7fb2b761"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:20:44.059946Z","signature_b64":"dB2OB2gGSUaw9mfLU5BH3fDVmPQmfeSRSbrScVUXtXBt96To2/m8+GjeXwrUKTWZk70l2JToXNkMvEgYYpSBAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1328df615719e4cef29d1f8e47b949df05331344ec4db122f5a39db8336d0310","last_reissued_at":"2026-07-04T17:20:44.059541Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:20:44.059541Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phase diagram of SU(2) with 2 flavors of dynamical adjoint quarks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-lat","authors_text":"Francesco Sannino, Joel Giedt, Joe Schneible, Simon Catterall","submitted_at":"2008-07-04T17:10:55Z","abstract_excerpt":"We report on numerical simulations of SU(2) lattice gauge theory with two flavors of light dynamical quarks in the adjoint of the gauge group. The dynamics of this theory is thought to be very different from QCD -- the theory exhibiting conformal or near conformal behavior in the infrared. We make a high resolution survey of the phase diagram of this model in the plane of the bare coupling and quark mass on lattices of size 8^3 \\times 16. Our simulations reveal a line of first order phase transitions extending from beta=0 to beta=beta_c \\sim 2.0. For beta > beta_c the phase boundary is no long"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0807.0792","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/0807.0792/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":"0807.0792","created_at":"2026-07-04T17:20:44.059610+00:00"},{"alias_kind":"arxiv_version","alias_value":"0807.0792v2","created_at":"2026-07-04T17:20:44.059610+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0807.0792","created_at":"2026-07-04T17:20:44.059610+00:00"},{"alias_kind":"pith_short_12","alias_value":"CMUN6YKXDHSM","created_at":"2026-07-04T17:20:44.059610+00:00"},{"alias_kind":"pith_short_16","alias_value":"CMUN6YKXDHSM54U5","created_at":"2026-07-04T17:20:44.059610+00:00"},{"alias_kind":"pith_short_8","alias_value":"CMUN6YKX","created_at":"2026-07-04T17:20:44.059610+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2408.00171","citing_title":"SU(2) gauge theory with one and two adjoint fermions towards the continuum limit","ref_index":40,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CMUN6YKXDHSM54U5D6HEPOKJ34","json":"https://pith.science/pith/CMUN6YKXDHSM54U5D6HEPOKJ34.json","graph_json":"https://pith.science/api/pith-number/CMUN6YKXDHSM54U5D6HEPOKJ34/graph.json","events_json":"https://pith.science/api/pith-number/CMUN6YKXDHSM54U5D6HEPOKJ34/events.json","paper":"https://pith.science/paper/CMUN6YKX"},"agent_actions":{"view_html":"https://pith.science/pith/CMUN6YKXDHSM54U5D6HEPOKJ34","download_json":"https://pith.science/pith/CMUN6YKXDHSM54U5D6HEPOKJ34.json","view_paper":"https://pith.science/paper/CMUN6YKX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0807.0792&json=true","fetch_graph":"https://pith.science/api/pith-number/CMUN6YKXDHSM54U5D6HEPOKJ34/graph.json","fetch_events":"https://pith.science/api/pith-number/CMUN6YKXDHSM54U5D6HEPOKJ34/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CMUN6YKXDHSM54U5D6HEPOKJ34/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CMUN6YKXDHSM54U5D6HEPOKJ34/action/storage_attestation","attest_author":"https://pith.science/pith/CMUN6YKXDHSM54U5D6HEPOKJ34/action/author_attestation","sign_citation":"https://pith.science/pith/CMUN6YKXDHSM54U5D6HEPOKJ34/action/citation_signature","submit_replication":"https://pith.science/pith/CMUN6YKXDHSM54U5D6HEPOKJ34/action/replication_record"}},"created_at":"2026-07-04T17:20:44.059610+00:00","updated_at":"2026-07-04T17:20:44.059610+00:00"}