<p>We investigate the impact of effective interactions of dimension-8 (dim-8) operators in the standard model effective field theory (SMEFT) on neutral meson mixing, focusing on the <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25789_Article_IEq1.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="66" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msup> <mi>K</mi> <mn>0</mn> </msup> <mo>−</mo> <msup> <mover accent="true"> <mi>K</mi> <mo stretchy="true">¯</mo> </mover> <mn>0</mn> </msup> </math></EquationSource> <EquationSource Format="TEX">\( {K}^0-{\overline{K}}^0 \)</EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25789_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="81" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msub> <mi>B</mi> <mrow> <mi>d</mi> <mo>,</mo> <mi>s</mi> </mrow> </msub> <mo>−</mo> <msub> <mover accent="true"> <mi>B</mi> <mo stretchy="true">¯</mo> </mover> <mrow> <mi>d</mi> <mo>,</mo> <mi>s</mi> </mrow> </msub> </math></EquationSource> <EquationSource Format="TEX">\( {B}_{d,s}-{\overline{B}}_{d,s} \)</EquationSource> </InlineEquation>, and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25789_Article_IEq3.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="64" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msup> <mi>D</mi> <mn>0</mn> </msup> <mo>−</mo> <msup> <mover accent="true"> <mi>D</mi> <mo stretchy="true">¯</mo> </mover> <mn>0</mn> </msup> </math></EquationSource> <EquationSource Format="TEX">\( {D}^0-{\overline{D}}^0 \)</EquationSource> </InlineEquation> systems. Within the framework of the low energy effective field theory (LEFT), each system is governed by eight dim-6 operators, with four originating at tree level from dim-6 SMEFT operators and the other four from dim-8 SMEFT operators. Notably, in certain UV complete models those dim-8 operators instead of the dim-6 ones are generated at the leading order. Our analysis focuses on those dim-8 operators and includes their one-loop QCD renormalization group running effects. By leveraging the LEFT master formula we impose stringent constraints on the effective scales associated with these dim-8 operators. We find that neutral meson mixing can probe an effective scale up to 80 TeV for some operators, surpassing the constraints imposed on other dim-8 operators by other observables. Lastly, we present a UV complete model capable of generating dim-8 operators at the leading order, thus offering a unique perspective on the interplay between different operator dimensions in probing new physics phenomena.</p>

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Probing dimension-8 SMEFT operators through neutral meson mixing

  • Yi Liao,
  • Xiao-Dong Ma,
  • Hao-Lin Wang

摘要

We investigate the impact of effective interactions of dimension-8 (dim-8) operators in the standard model effective field theory (SMEFT) on neutral meson mixing, focusing on the K 0 K ¯ 0 \( {K}^0-{\overline{K}}^0 \) , B d , s B ¯ d , s \( {B}_{d,s}-{\overline{B}}_{d,s} \) , and D 0 D ¯ 0 \( {D}^0-{\overline{D}}^0 \) systems. Within the framework of the low energy effective field theory (LEFT), each system is governed by eight dim-6 operators, with four originating at tree level from dim-6 SMEFT operators and the other four from dim-8 SMEFT operators. Notably, in certain UV complete models those dim-8 operators instead of the dim-6 ones are generated at the leading order. Our analysis focuses on those dim-8 operators and includes their one-loop QCD renormalization group running effects. By leveraging the LEFT master formula we impose stringent constraints on the effective scales associated with these dim-8 operators. We find that neutral meson mixing can probe an effective scale up to 80 TeV for some operators, surpassing the constraints imposed on other dim-8 operators by other observables. Lastly, we present a UV complete model capable of generating dim-8 operators at the leading order, thus offering a unique perspective on the interplay between different operator dimensions in probing new physics phenomena.