{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:UMJVRUUXQRMVRWQF6A3TG27CRD","short_pith_number":"pith:UMJVRUUX","schema_version":"1.0","canonical_sha256":"a31358d297845958da05f037336be288d40082ddc68af410e7fd141266cc6391","source":{"kind":"arxiv","id":"1308.4130","version":2},"attestation_state":"computed","paper":{"title":"Composite Goldstone Dark Matter: Experimental Predictions from the Lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Ari Hietanen, Claudio Pica, Francesco Sannino, Randy Lewis","submitted_at":"2013-08-19T20:00:00Z","abstract_excerpt":"We study, via first principles lattice simulations, the nonperturbative dynamics of $SU(2)$ gauge theory with two fundamental Dirac flavors. The model can be used simultaneously as a template for composite Goldstone boson dark matter and for breaking the electroweak symmetry dynamically. We compute the form factor, allowing us to estimate the associated electromagnetic charge radius. Interestingly we observe that the form factor obeys vector meson dominance even for the two color theory. We finally compare the model predictions with dark matter direct detection experiments. We find that the co"},"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":"1308.4130","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-08-19T20:00:00Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"4e607f7780c2f3d291301cec8e08f4b7b4db6b78d9412262183f6fa7a957da62","abstract_canon_sha256":"4448bb538c27d0422ecdd5f021fb0a86e569e19fec7a8e342be814fede4c3eb3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:48:13.876734Z","signature_b64":"Q6szS53Xw9hZWot1bi0CJlD0+6JmeLUKEmTU81KdYBDoIMEhDsmqLX9XwR2P1mMipEmzHc2mRo80MBfsAH68Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a31358d297845958da05f037336be288d40082ddc68af410e7fd141266cc6391","last_reissued_at":"2026-05-18T01:48:13.876160Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:48:13.876160Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Composite Goldstone Dark Matter: Experimental Predictions from the Lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Ari Hietanen, Claudio Pica, Francesco Sannino, Randy Lewis","submitted_at":"2013-08-19T20:00:00Z","abstract_excerpt":"We study, via first principles lattice simulations, the nonperturbative dynamics of $SU(2)$ gauge theory with two fundamental Dirac flavors. The model can be used simultaneously as a template for composite Goldstone boson dark matter and for breaking the electroweak symmetry dynamically. We compute the form factor, allowing us to estimate the associated electromagnetic charge radius. Interestingly we observe that the form factor obeys vector meson dominance even for the two color theory. We finally compare the model predictions with dark matter direct detection experiments. We find that the co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.4130","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":""},"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":"1308.4130","created_at":"2026-05-18T01:48:13.876265+00:00"},{"alias_kind":"arxiv_version","alias_value":"1308.4130v2","created_at":"2026-05-18T01:48:13.876265+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.4130","created_at":"2026-05-18T01:48:13.876265+00:00"},{"alias_kind":"pith_short_12","alias_value":"UMJVRUUXQRMV","created_at":"2026-05-18T12:28:02.375192+00:00"},{"alias_kind":"pith_short_16","alias_value":"UMJVRUUXQRMVRWQF","created_at":"2026-05-18T12:28:02.375192+00:00"},{"alias_kind":"pith_short_8","alias_value":"UMJVRUUX","created_at":"2026-05-18T12:28:02.375192+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.19009","citing_title":"Finite-temperature Yang-Mills theories with the density of states method: towards the continuum limit","ref_index":45,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UMJVRUUXQRMVRWQF6A3TG27CRD","json":"https://pith.science/pith/UMJVRUUXQRMVRWQF6A3TG27CRD.json","graph_json":"https://pith.science/api/pith-number/UMJVRUUXQRMVRWQF6A3TG27CRD/graph.json","events_json":"https://pith.science/api/pith-number/UMJVRUUXQRMVRWQF6A3TG27CRD/events.json","paper":"https://pith.science/paper/UMJVRUUX"},"agent_actions":{"view_html":"https://pith.science/pith/UMJVRUUXQRMVRWQF6A3TG27CRD","download_json":"https://pith.science/pith/UMJVRUUXQRMVRWQF6A3TG27CRD.json","view_paper":"https://pith.science/paper/UMJVRUUX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1308.4130&json=true","fetch_graph":"https://pith.science/api/pith-number/UMJVRUUXQRMVRWQF6A3TG27CRD/graph.json","fetch_events":"https://pith.science/api/pith-number/UMJVRUUXQRMVRWQF6A3TG27CRD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UMJVRUUXQRMVRWQF6A3TG27CRD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UMJVRUUXQRMVRWQF6A3TG27CRD/action/storage_attestation","attest_author":"https://pith.science/pith/UMJVRUUXQRMVRWQF6A3TG27CRD/action/author_attestation","sign_citation":"https://pith.science/pith/UMJVRUUXQRMVRWQF6A3TG27CRD/action/citation_signature","submit_replication":"https://pith.science/pith/UMJVRUUXQRMVRWQF6A3TG27CRD/action/replication_record"}},"created_at":"2026-05-18T01:48:13.876265+00:00","updated_at":"2026-05-18T01:48:13.876265+00:00"}