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Short-distance QCD corrections to $K^0\bar{K}^0$ mixing at next-to-leading order in Left-Right models
High Energy Physics - Phenomenology · Submitted 2 Dec 2015
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We conclude by providing next-to-leading-order estimates for $cc$, $ct$ and $tt$ boxes in LR models.
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The abstract, sentence by sentence
Left-Right (LR) models are extensions of the Standard Model where left-right symmetry is restored at high energies, and which are strongly constrained by kaon mixing described in the framework of the $|\Delta S|=2$ effective Hamiltonian. We consider the short-distance QCD corrections to this Hamiltonian both in the Standard Model (SM) and in LR models. The leading logarithms occurring in these short-distance corrections can be resummed within a rigourous Effective Field Theory (EFT) approach integrating out heavy degrees of freedom progressively, or using an approximate simpler method of regions identifying the ranges of loop momentum generating large logarithms in the relevant two-loop diagrams. We compare the two approaches in the SM at next-to-leading order, finding a very good agreement when one scale dominates the problem, but only a fair agreement in the presence of a large logarithm at leading order. We compute the short-distance QCD corrections for LR models at next-to-leading order using the method of regions, and we compare the results with the EFT approach for the $WW'$ box with two charm quarks (together with additional diagrams forming a gauge-invariant combination), where a large logarithm occurs already at leading order. We conclude by providing next-to-leading-order estimates for $cc$, $ct$ and $tt$ boxes in LR models.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Left-Right (LR) models are extensions of the Standard Model where left-right symmetry is restored at high energies, and which are strongly constrained by kaon mixing described in the framework of the $|\Delta S|=2$ effective Hamiltonian. | background 1.00 | 0.05 | 0.02 | asserted 1.00 |
| s1 | We consider the short-distance QCD corrections to this Hamiltonian both in the Standard Model (SM) and in LR models. | contribution 0.99 | 0.86 | 0.03 | asserted 0.89 |
| s2 | The leading logarithms occurring in these short-distance corrections can be resummed within a rigourous Effective Field Theory (EFT) approach integrating out heavy degrees of freedom progressively, or using an approximate simpler method of regions identifying the ranges of loop momentum generating large logarithms in the relevant two-loop diagrams. | method 0.83 | 0.12 | 0.04 | asserted 0.94 |
| s3 | We compare the two approaches in the SM at next-to-leading order, finding a very good agreement when one scale dominates the problem, but only a fair agreement in the presence of a large logarithm at leading order. | result 0.92 | 0.96 | 0.13 | asserted 1.00 |
| s4 | We compute the short-distance QCD corrections for LR models at next-to-leading order using the method of regions, and we compare the results with the EFT approach for the $WW'$ box with two charm quarks (together with additional diagrams forming a gauge-invariant combination), where a large logarithm occurs already at leading order. | contribution 0.86 | 0.96 | 0.12 | asserted 1.00 |
| s5 | We conclude by providing next-to-leading-order estimates for $cc$, $ct$ and $tt$ boxes in LR models. | result 0.76 | 0.95 | 0.69 | asserted 0.90 |
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The paper
Original abstract
Left-Right (LR) models are extensions of the Standard Model where left-right symmetry is restored at high energies, and which are strongly constrained by kaon mixing described in the framework of the $|\Delta S|=2$ effective Hamiltonian. We consider the short-distance QCD corrections to this Hamiltonian both in the Standard Model (SM) and in LR models. The leading logarithms occurring in these short-distance corrections can be resummed within a rigourous Effective Field Theory (EFT) approach integrating out heavy degrees of freedom progressively, or using an approximate simpler method of regions identifying the ranges of loop momentum generating large logarithms in the relevant two-loop diagrams. We compare the two approaches in the SM at next-to-leading order, finding a very good agreement when one scale dominates the problem, but only a fair agreement in the presence of a large logarithm at leading order. We compute the short-distance QCD corrections for LR models at next-to-leading order using the method of regions, and we compare the results with the EFT approach for the $WW'$ box with two charm quarks (together with additional diagrams forming a gauge-invariant combination), where a large logarithm occurs already at leading order. We conclude by providing next-to-leading-order estimates for $cc$, $ct$ and $tt$ boxes in LR models.
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References
How the literature uses it
10 arXiv papers cite this in 13 sentences
Papers citing it · 9 sentences without a confident label
Cites it as background 3 papers
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In most of the cases, the LR symmetry breaking scale is low and the phenomenology has been discussed involving not only the extra scalars and the extra gauge bosons induced by the $SU(2)_R$ symmetry [ref] .
Flavor physics in the multi-Higgs doublet models induced by the left-right symmetry · Summary and Discussion · 1.00
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Such matrices can be constrained by flavour observables [ref] , such as $K^0$-$K^0$ neutral meson mixing [ref] , that exceed the scope of the present work.
Direct bounds on Left-Right gauge boson masses at LHC Run 2 · Introduction · 0.93
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In the model under consideration the additional Higgs doublet couples to all fermions, a setup which appears in many UV models, such as the left-right model [ref] and even in the TeV scale Pati-Salam model to break the symmetry with a bi-doublet field [ref] .
Towards ruling out the charged Higgs interpretation of the $R_{D^{(*)}}$ anomaly · Model and parameters · 0.83
What it cites · 17 sentences without a confident label
Uses data or values from 2 papers
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This led to an evaluation of these contributions at NNLO, leading to a significant positive shift compared to NLO for $η_cc=1.87±0.76$ [ref] and a $7 %$ increase for $η_ct=0.496±0.047$ [ref] ($η_tt$ remaining almost unchanged).
Epsilon_K at Next-to-Next-to-Leading Order: The Charm-Top-Quark Contribution · EFT computation: specific issues · 0.92
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This led to an evaluation of these contributions at NNLO, leading to a significant positive shift compared to NLO for $η_cc=1.87±0.76$ [ref] and a $7 %$ increase for $η_ct=0.496±0.047$ [ref] ($η_tt$ remaining almost unchanged).
Next-to-Next-to-Leading-Order Charm-Quark Contribution to the CP Violation Parameter epsilon_K and Delta M_K · EFT computation: specific issues · 0.92
Compares with 1 paper
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The LO results are in fairly good agreement with the calculation of Ref. [ref] .
Present and Future K and B Meson Mixing Constraints on TeV Scale Left-Right Symmetry · Method of regions · 1.00
Cites as support 2 papers
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The short-distance corrections $η̅_1,UV$ are at least an order of magnitude smaller than $η̅_2,UV$ and will not be considered further, in agreement with Refs. [ref] .
Delta F = 2 observables and B -> X_q gamma decays in the Left-Right Model: Higgs particles striking back · Method of regions · 0.96
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The short-distance corrections $η̅_1,UV$ are at least an order of magnitude smaller than $η̅_2,UV$ and will not be considered further, in agreement with Refs. [ref] .
Present and Future K and B Meson Mixing Constraints on TeV Scale Left-Right Symmetry · Method of regions · 0.96
Cites as background 1 paper
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This extension induces the presence of heavy spin-1 $W'$ and $Z'$ bosons predominantly coupling to right-handed fermions, introducing a new CKM-like matrix for right-handed quarks, as well as charged and neutral heavy Higgs bosons with an interesting pattern of flavour-changing currents [ref] .
General CP Violation in Minimal Left-Right Symmetric Model and Constraints on the Right-Handed Scale · Introduction · 0.91
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