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To that end, we apply the pionless effective field theory to experimental data and numerical lattice calculations which simulate QCD at pion masses of 450~MeV and 806~MeV.\n  At the physical pion mass, we postdict the magnetic moment of helium-3, $\\mu_{^3He}=-2.13~$nNM, and the magnetic polarizability of deuterium, $\\beta_D=7.33~10^{-2}~$fm$^3$. Magnetic polarizabilities of helium-3, $\\beta_{^3He}=9.7~10^{-4}~$fm$^3$, and the triton, $\\beta_{^3H}=8.2~10^{-4}~$fm$^3$, are predictions.\n  Postdictio"},"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":"1702.07268","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-02-23T15:57:39Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"ca1d2cbb16caab2a5205b0fac29a095dd54630ce5158a27c924432d37b99c465","abstract_canon_sha256":"b64609759af240bf939bdcb5546d645283c56a0363ea29d39b56ca88d4d6f995"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:28.341536Z","signature_b64":"cWbGLIS0efKyKPMHkF8HcmSMBJKSQqq8auihFUWOx0SwleYDwbXQ1soqO6gV0RvPTo7ROZWo4NJeOhOa7to0Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7a2c385cb537bf9b8364f711073792eb2d47e38fb9009eb0ccc90ea2c9a81543","last_reissued_at":"2026-05-18T00:38:28.340892Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:28.340892Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electromagnetic characteristics of $A \\leq 3$ physical and lattice nuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"nucl-th","authors_text":"Ehoud Pazy, Johannes Kirscher, Jonathan Drachman, Nir Barnea","submitted_at":"2017-02-23T15:57:39Z","abstract_excerpt":"We analyze the quark-mass dependence of electromagnetic properties of two and three-nucleon states. 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Magnetic polarizabilities of helium-3, $\\beta_{^3He}=9.7~10^{-4}~$fm$^3$, and the triton, $\\beta_{^3H}=8.2~10^{-4}~$fm$^3$, are predictions.\n  Postdictio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.07268","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":"1702.07268","created_at":"2026-05-18T00:38:28.340983+00:00"},{"alias_kind":"arxiv_version","alias_value":"1702.07268v1","created_at":"2026-05-18T00:38:28.340983+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.07268","created_at":"2026-05-18T00:38:28.340983+00:00"},{"alias_kind":"pith_short_12","alias_value":"PIWDQXFVG67Z","created_at":"2026-05-18T12:31:37.085036+00:00"},{"alias_kind":"pith_short_16","alias_value":"PIWDQXFVG67ZXA3E","created_at":"2026-05-18T12:31:37.085036+00:00"},{"alias_kind":"pith_short_8","alias_value":"PIWDQXFV","created_at":"2026-05-18T12:31:37.085036+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.19062","citing_title":"Coulomb Corrections to Three-Nucleon Moments","ref_index":33,"is_internal_anchor":true},{"citing_arxiv_id":"2604.25221","citing_title":"Coulomb Effects and Wigner-SU(4) Symmetry in He-3 Charge and Magnetic Properties","ref_index":37,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PIWDQXFVG67ZXA3E64IQON4S5M","json":"https://pith.science/pith/PIWDQXFVG67ZXA3E64IQON4S5M.json","graph_json":"https://pith.science/api/pith-number/PIWDQXFVG67ZXA3E64IQON4S5M/graph.json","events_json":"https://pith.science/api/pith-number/PIWDQXFVG67ZXA3E64IQON4S5M/events.json","paper":"https://pith.science/paper/PIWDQXFV"},"agent_actions":{"view_html":"https://pith.science/pith/PIWDQXFVG67ZXA3E64IQON4S5M","download_json":"https://pith.science/pith/PIWDQXFVG67ZXA3E64IQON4S5M.json","view_paper":"https://pith.science/paper/PIWDQXFV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1702.07268&json=true","fetch_graph":"https://pith.science/api/pith-number/PIWDQXFVG67ZXA3E64IQON4S5M/graph.json","fetch_events":"https://pith.science/api/pith-number/PIWDQXFVG67ZXA3E64IQON4S5M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PIWDQXFVG67ZXA3E64IQON4S5M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PIWDQXFVG67ZXA3E64IQON4S5M/action/storage_attestation","attest_author":"https://pith.science/pith/PIWDQXFVG67ZXA3E64IQON4S5M/action/author_attestation","sign_citation":"https://pith.science/pith/PIWDQXFVG67ZXA3E64IQON4S5M/action/citation_signature","submit_replication":"https://pith.science/pith/PIWDQXFVG67ZXA3E64IQON4S5M/action/replication_record"}},"created_at":"2026-05-18T00:38:28.340983+00:00","updated_at":"2026-05-18T00:38:28.340983+00:00"}