{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:P5OFZAXXPJ5UMW62U5GMJYGLHR","short_pith_number":"pith:P5OFZAXX","canonical_record":{"source":{"id":"1211.0712","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-11-04T18:51:12Z","cross_cats_sorted":[],"title_canon_sha256":"19d01f0c42e96c1916a4d6a51f8af2351f7eab45ed6f82f42f1c2a992f36ad04","abstract_canon_sha256":"c7b8d5ff61ea779bbe92459f0f213811d90b602ccaf87f27bf6f56f4daf97b23"},"schema_version":"1.0"},"canonical_sha256":"7f5c5c82f77a7b465bdaa74cc4e0cb3c6377070522b74fb434ccef6e9acbb068","source":{"kind":"arxiv","id":"1211.0712","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.0712","created_at":"2026-05-18T03:41:32Z"},{"alias_kind":"arxiv_version","alias_value":"1211.0712v1","created_at":"2026-05-18T03:41:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.0712","created_at":"2026-05-18T03:41:32Z"},{"alias_kind":"pith_short_12","alias_value":"P5OFZAXXPJ5U","created_at":"2026-05-18T12:27:18Z"},{"alias_kind":"pith_short_16","alias_value":"P5OFZAXXPJ5UMW62","created_at":"2026-05-18T12:27:18Z"},{"alias_kind":"pith_short_8","alias_value":"P5OFZAXX","created_at":"2026-05-18T12:27:18Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:P5OFZAXXPJ5UMW62U5GMJYGLHR","target":"record","payload":{"canonical_record":{"source":{"id":"1211.0712","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-11-04T18:51:12Z","cross_cats_sorted":[],"title_canon_sha256":"19d01f0c42e96c1916a4d6a51f8af2351f7eab45ed6f82f42f1c2a992f36ad04","abstract_canon_sha256":"c7b8d5ff61ea779bbe92459f0f213811d90b602ccaf87f27bf6f56f4daf97b23"},"schema_version":"1.0"},"canonical_sha256":"7f5c5c82f77a7b465bdaa74cc4e0cb3c6377070522b74fb434ccef6e9acbb068","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:41:32.638103Z","signature_b64":"cThK8DXxXrc1wnMmcSZ2XXip9KPZwOTAmVGLRmKMXGGGPx3LvjBLYaAZCOHK9gc9R8236gHt06OLslj4L5vLBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7f5c5c82f77a7b465bdaa74cc4e0cb3c6377070522b74fb434ccef6e9acbb068","last_reissued_at":"2026-05-18T03:41:32.637575Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:41:32.637575Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1211.0712","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":"2026-05-18T03:41:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qX9JgN+VSpluNbjpfZ56jI8l3AN7jcHue0fQSwvCEHAbMOtkea5cS8EXCJxclQZ8ZUVk4F79x2JVCi8ouEfqBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T01:00:19.951142Z"},"content_sha256":"b11f0477bcd9a815070f84c5bfa1e2c95248754f6030b4381ee9116495c74e14","schema_version":"1.0","event_id":"sha256:b11f0477bcd9a815070f84c5bfa1e2c95248754f6030b4381ee9116495c74e14"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:P5OFZAXXPJ5UMW62U5GMJYGLHR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"QCD with colour-sextet quarks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"D. K. Sinclair, J. B. Kogut","submitted_at":"2012-11-04T18:51:12Z","abstract_excerpt":"We study QCD with 2 colour-sextet quarks as a model for walking Technicolor, using lattice gauge theory simulations (RHMC) at finite temperature. Our goal is to determine if the massless theory is QCD-like (confining, with spontaneously-broken chiral symmetry) with a slowly varying coupling (walks) or if it is a conformal field theory. We do this by simulating the theory at finite temperature and observing how the coupling at the chiral-symmetry restoration temperature depends on the temporal extent $N_t$ of the lattice (in lattice units). If the theory is QCD-like, this coupling should approa"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.0712","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":"2026-05-18T03:41:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vee9Ctcno8hIeqkp1L4H3ObrjhLmgfh/PnaRPXybCz/LtQUXqnJC1hZhD4B9/YXnY0FTypB83wbBqiYIC1ACAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T01:00:19.951529Z"},"content_sha256":"5fe0b68741d99eb12ece73a3250cfddcda30cbb025ef7a3c627e81516c930aed","schema_version":"1.0","event_id":"sha256:5fe0b68741d99eb12ece73a3250cfddcda30cbb025ef7a3c627e81516c930aed"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/P5OFZAXXPJ5UMW62U5GMJYGLHR/bundle.json","state_url":"https://pith.science/pith/P5OFZAXXPJ5UMW62U5GMJYGLHR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/P5OFZAXXPJ5UMW62U5GMJYGLHR/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":"2026-06-07T01:00:19Z","links":{"resolver":"https://pith.science/pith/P5OFZAXXPJ5UMW62U5GMJYGLHR","bundle":"https://pith.science/pith/P5OFZAXXPJ5UMW62U5GMJYGLHR/bundle.json","state":"https://pith.science/pith/P5OFZAXXPJ5UMW62U5GMJYGLHR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/P5OFZAXXPJ5UMW62U5GMJYGLHR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:P5OFZAXXPJ5UMW62U5GMJYGLHR","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":"c7b8d5ff61ea779bbe92459f0f213811d90b602ccaf87f27bf6f56f4daf97b23","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-11-04T18:51:12Z","title_canon_sha256":"19d01f0c42e96c1916a4d6a51f8af2351f7eab45ed6f82f42f1c2a992f36ad04"},"schema_version":"1.0","source":{"id":"1211.0712","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.0712","created_at":"2026-05-18T03:41:32Z"},{"alias_kind":"arxiv_version","alias_value":"1211.0712v1","created_at":"2026-05-18T03:41:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.0712","created_at":"2026-05-18T03:41:32Z"},{"alias_kind":"pith_short_12","alias_value":"P5OFZAXXPJ5U","created_at":"2026-05-18T12:27:18Z"},{"alias_kind":"pith_short_16","alias_value":"P5OFZAXXPJ5UMW62","created_at":"2026-05-18T12:27:18Z"},{"alias_kind":"pith_short_8","alias_value":"P5OFZAXX","created_at":"2026-05-18T12:27:18Z"}],"graph_snapshots":[{"event_id":"sha256:5fe0b68741d99eb12ece73a3250cfddcda30cbb025ef7a3c627e81516c930aed","target":"graph","created_at":"2026-05-18T03:41:32Z","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 study QCD with 2 colour-sextet quarks as a model for walking Technicolor, using lattice gauge theory simulations (RHMC) at finite temperature. Our goal is to determine if the massless theory is QCD-like (confining, with spontaneously-broken chiral symmetry) with a slowly varying coupling (walks) or if it is a conformal field theory. We do this by simulating the theory at finite temperature and observing how the coupling at the chiral-symmetry restoration temperature depends on the temporal extent $N_t$ of the lattice (in lattice units). If the theory is QCD-like, this coupling should approa","authors_text":"D. K. Sinclair, J. B. Kogut","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-11-04T18:51:12Z","title":"QCD with colour-sextet quarks"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.0712","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:b11f0477bcd9a815070f84c5bfa1e2c95248754f6030b4381ee9116495c74e14","target":"record","created_at":"2026-05-18T03:41:32Z","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":"c7b8d5ff61ea779bbe92459f0f213811d90b602ccaf87f27bf6f56f4daf97b23","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-11-04T18:51:12Z","title_canon_sha256":"19d01f0c42e96c1916a4d6a51f8af2351f7eab45ed6f82f42f1c2a992f36ad04"},"schema_version":"1.0","source":{"id":"1211.0712","kind":"arxiv","version":1}},"canonical_sha256":"7f5c5c82f77a7b465bdaa74cc4e0cb3c6377070522b74fb434ccef6e9acbb068","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7f5c5c82f77a7b465bdaa74cc4e0cb3c6377070522b74fb434ccef6e9acbb068","first_computed_at":"2026-05-18T03:41:32.637575Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:41:32.637575Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"cThK8DXxXrc1wnMmcSZ2XXip9KPZwOTAmVGLRmKMXGGGPx3LvjBLYaAZCOHK9gc9R8236gHt06OLslj4L5vLBg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:41:32.638103Z","signed_message":"canonical_sha256_bytes"},"source_id":"1211.0712","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b11f0477bcd9a815070f84c5bfa1e2c95248754f6030b4381ee9116495c74e14","sha256:5fe0b68741d99eb12ece73a3250cfddcda30cbb025ef7a3c627e81516c930aed"],"state_sha256":"712eedb0ff8253f35e45beb99dd1a3941c7064a5f3a0b6bf34fa93cbb0e90d52"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4Cl+DMO4bRQxua27PJUFso2zJooK0kzBno4gxOR9wdMM2jfUQoDWpY81/QPSXNJLTUl39Hqw5AsAGcUGlWEaBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T01:00:19.953887Z","bundle_sha256":"dc0db2dae3b54057f33e894823dfc50d4ca822a4d97f5098437452c59fee96a1"}}