<p>Precision observables are well known for constraining most of the beyond standard model (BSM) scenarios tightly, among which the electroweak precision observables (EWPO) play a significant role. Recent measurement of the <i>W</i> boson mass (<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12043_2025_2990_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(M_W\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>M</mi> <mi>W</mi> </msub> </math></EquationSource> </InlineEquation>) at CDF-II has put a renewed focus on the EWPO and its ensuing constraints. In this study, we look at the scenarios where these BSM effects are encoded primarily in ten dimension-6 standard model effective field theory (SMEFT) operators (in the Warsaw basis) which contribute to the EWPO at tree-level. After presenting the fitting procedure and testing it on the <i>S</i>, <i>T</i> and <i>V</i> parameters, we go on to fit various BSM scenarios consisting of different well-motivated subsets of the 10 operators of our interest. To constrain these scenarios further, we augment the EWPO with <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12043_2025_2990_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta _{\textrm{CKM}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Δ</mi> <mtext>CKM</mtext> </msub> </math></EquationSource> </InlineEquation> measurement using 1-loop matching of the low-energy effective field theory to SMEFT operators at the Z-pole. We show that the inclusion of the <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12043_2025_2990_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta _{\textrm{CKM}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Δ</mi> <mtext>CKM</mtext> </msub> </math></EquationSource> </InlineEquation> constraint indeed results in stronger bounds on our Wilson coefficients. One of our operator subsets caters to the models of vector-like leptons, where we find out that such a minimal extension is in tension with the forward–backward asymmetry in the <i>b</i>-sector (<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12043_2025_2990_Article_IEq6.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="30" /> </InlineMediaObject> <EquationSource Format="TEX">\(A_b^{\textrm{FB}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>A</mi> <mi>b</mi> <mtext>FB</mtext> </msubsup> </math></EquationSource> </InlineEquation>) and <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12043_2025_2990_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(M_W\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>M</mi> <mi>W</mi> </msub> </math></EquationSource> </InlineEquation>. Finally, we also include the LEP-II observables pertaining to the <i>WW</i> production, thereby lifting the two associated blind directions, helping us present the results for the full fit.</p>

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Constraining SMEFT BSM scenarios with EWPO and \(\Delta _{\textrm{CKM}}\)

  • Mathew Thomas Arun,
  • Kuldeep Deka,
  • Tripurari Srivastava

摘要

Precision observables are well known for constraining most of the beyond standard model (BSM) scenarios tightly, among which the electroweak precision observables (EWPO) play a significant role. Recent measurement of the W boson mass ( \(M_W\) M W ) at CDF-II has put a renewed focus on the EWPO and its ensuing constraints. In this study, we look at the scenarios where these BSM effects are encoded primarily in ten dimension-6 standard model effective field theory (SMEFT) operators (in the Warsaw basis) which contribute to the EWPO at tree-level. After presenting the fitting procedure and testing it on the S, T and V parameters, we go on to fit various BSM scenarios consisting of different well-motivated subsets of the 10 operators of our interest. To constrain these scenarios further, we augment the EWPO with \(\Delta _{\textrm{CKM}}\) Δ CKM measurement using 1-loop matching of the low-energy effective field theory to SMEFT operators at the Z-pole. We show that the inclusion of the \(\Delta _{\textrm{CKM}}\) Δ CKM constraint indeed results in stronger bounds on our Wilson coefficients. One of our operator subsets caters to the models of vector-like leptons, where we find out that such a minimal extension is in tension with the forward–backward asymmetry in the b-sector ( \(A_b^{\textrm{FB}}\) A b FB ) and \(M_W\) M W . Finally, we also include the LEP-II observables pertaining to the WW production, thereby lifting the two associated blind directions, helping us present the results for the full fit.