{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:HAM3URWBI5KSWCVQBK22XYZVTR","short_pith_number":"pith:HAM3URWB","schema_version":"1.0","canonical_sha256":"3819ba46c147552b0ab00ab5abe3359c7d17b5663e8891feb5a513df82b6379e","source":{"kind":"arxiv","id":"1511.05097","version":1},"attestation_state":"computed","paper":{"title":"Lattice simulations of technicolour theories with adjoint fermions and supersymmetric Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Georg Bergner, Gernot M\\\"unster, Istvan Montvay, Pietro Giudice, Stefano Piemonte","submitted_at":"2015-11-16T19:32:01Z","abstract_excerpt":"Theories with fermions in the adjoint representation have several interesting applications in extensions of the standard model. The conformal window for these theories is of particular interest for technicolour extensions. We present here our newest results for the spectrum of $N_f=2$ adjoint QCD and compare them with the predictions for a conformal behaviour. The comparison with supersymmetric Yang-Mills theory, investigated with the same methods, will help to distinguish more clearly the conformal and the confining scenario. The spectrum includes additional fermionic states that are not pres"},"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":"1511.05097","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-11-16T19:32:01Z","cross_cats_sorted":[],"title_canon_sha256":"46f9ace3dec8e8888fd02c99a248680a0281d19cf16c507c475a403deb651aad","abstract_canon_sha256":"4d3ba1da9ce9d114dd0f9015792f488772e0d493489e897951266620f27175e2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:26:50.880143Z","signature_b64":"j4CAfbhzq6dDlit5rtYEakl0LRSswCTTJ0Dq28EYsfOjwJSh1EG57qn7Ne2gDI/VWmaZY4dZdJmuGyjq3nclCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3819ba46c147552b0ab00ab5abe3359c7d17b5663e8891feb5a513df82b6379e","last_reissued_at":"2026-05-18T01:26:50.879480Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:26:50.879480Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Lattice simulations of technicolour theories with adjoint fermions and supersymmetric Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Georg Bergner, Gernot M\\\"unster, Istvan Montvay, Pietro Giudice, Stefano Piemonte","submitted_at":"2015-11-16T19:32:01Z","abstract_excerpt":"Theories with fermions in the adjoint representation have several interesting applications in extensions of the standard model. The conformal window for these theories is of particular interest for technicolour extensions. We present here our newest results for the spectrum of $N_f=2$ adjoint QCD and compare them with the predictions for a conformal behaviour. The comparison with supersymmetric Yang-Mills theory, investigated with the same methods, will help to distinguish more clearly the conformal and the confining scenario. The spectrum includes additional fermionic states that are not pres"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.05097","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1511.05097","created_at":"2026-05-18T01:26:50.879605+00:00"},{"alias_kind":"arxiv_version","alias_value":"1511.05097v1","created_at":"2026-05-18T01:26:50.879605+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.05097","created_at":"2026-05-18T01:26:50.879605+00:00"},{"alias_kind":"pith_short_12","alias_value":"HAM3URWBI5KS","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_16","alias_value":"HAM3URWBI5KSWCVQ","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_8","alias_value":"HAM3URWB","created_at":"2026-05-18T12:29:22.688609+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/HAM3URWBI5KSWCVQBK22XYZVTR","json":"https://pith.science/pith/HAM3URWBI5KSWCVQBK22XYZVTR.json","graph_json":"https://pith.science/api/pith-number/HAM3URWBI5KSWCVQBK22XYZVTR/graph.json","events_json":"https://pith.science/api/pith-number/HAM3URWBI5KSWCVQBK22XYZVTR/events.json","paper":"https://pith.science/paper/HAM3URWB"},"agent_actions":{"view_html":"https://pith.science/pith/HAM3URWBI5KSWCVQBK22XYZVTR","download_json":"https://pith.science/pith/HAM3URWBI5KSWCVQBK22XYZVTR.json","view_paper":"https://pith.science/paper/HAM3URWB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1511.05097&json=true","fetch_graph":"https://pith.science/api/pith-number/HAM3URWBI5KSWCVQBK22XYZVTR/graph.json","fetch_events":"https://pith.science/api/pith-number/HAM3URWBI5KSWCVQBK22XYZVTR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HAM3URWBI5KSWCVQBK22XYZVTR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HAM3URWBI5KSWCVQBK22XYZVTR/action/storage_attestation","attest_author":"https://pith.science/pith/HAM3URWBI5KSWCVQBK22XYZVTR/action/author_attestation","sign_citation":"https://pith.science/pith/HAM3URWBI5KSWCVQBK22XYZVTR/action/citation_signature","submit_replication":"https://pith.science/pith/HAM3URWBI5KSWCVQBK22XYZVTR/action/replication_record"}},"created_at":"2026-05-18T01:26:50.879605+00:00","updated_at":"2026-05-18T01:26:50.879605+00:00"}