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The two-loop and three-loop results are not appreciably different from each other. The two-loop and three-loop radiative corrections have led to an improvement of Higgs boson mass and the value of the scalar coupling. For the value $m_{t}=170$ GeV at the energy scale $\\mu\\approx 5.68\\times10^2$GeV, we get $m_{H2-loop}\\approx 125."},"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":"1605.08923","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-05-28T18:28:54Z","cross_cats_sorted":[],"title_canon_sha256":"0341913d3d5dba282eed7225f3bc663ce9e93a1dd30fc92307a21d0b1ab25e7c","abstract_canon_sha256":"8cb7c961aa96f01e50ab8cd307a9ee9b1f1c7d6663e79276a0fa32e46e3443db"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:13:22.609377Z","signature_b64":"x0aZ4z9ldrbUiB81bJcixvPwlf0Dn4LUesKfYyak8jamo/xgPfajW1wvL5IXOpYebOzKghvEir0B2d8od3uvDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"060d43928c209bebb884ba66f915e93f458a37237c1b5e5f84a3c5d57508003b","last_reissued_at":"2026-05-18T01:13:22.608669Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:13:22.608669Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Higgs Boson Mass from Three-loop Effective Potential of Massless Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"H. 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