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Two-loop matching of the dipole operators for $b \to s \gamma$ and $b \to s gluon$
High Energy Physics - Phenomenology · Submitted 18 Mar 1997
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Our results are in complete agreement with those in ref. [1].
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The abstract, sentence by sentence
The order $\alpha_s$ corrections to the Wilson coefficients of the dipole operators ($O_7,O_8$) at the matching scale $\mu =m_W$ are a crucial ingredient for a complete next- to-leading logarithmic calculation of the branching ratio for $b \to s \gamma$. Given the phenomenological relevance and the fact that this two-loop calculation has been done so far only by one group [1], we present a detailed re-calculation using a different method. Our results are in complete agreement with those in ref. [1].
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The order $\alpha_s$ corrections to the Wilson coefficients of the dipole operators ($O_7,O_8$) at the matching scale $\mu =m_W$ are a crucial ingredient for a complete next- to-leading logarithmic calculation of the branching ratio for $b \to s \gamma$. | background 1.00 | 0.06 | 0.07 | asserted 1.00 |
| s1 | Given the phenomenological relevance and the fact that this two-loop calculation has been done so far only by one group [1], we present a detailed re-calculation using a different method. | contribution 0.85 | 0.54 | 0.06 | asserted 0.99 |
| s2 | Our results are in complete agreement with those in ref. [1]. | result 0.98 | 0.87 | 0.58 | asserted 1.00 |
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The paper
Original abstract
The order $\alpha_s$ corrections to the Wilson coefficients of the dipole operators ($O_7,O_8$) at the matching scale $\mu =m_W$ are a crucial ingredient for a complete next- to-leading logarithmic calculation of the branching ratio for $b \to s \gamma$. Given the phenomenological relevance and the fact that this two-loop calculation has been done so far only by one group [1], we present a detailed re-calculation using a different method. Our results are in complete agreement with those in ref. [1].
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How the literature uses it
6 arXiv papers cite this in 7 sentences
Papers citing it · 5 sentences without a confident label
Compares with it 1 paper
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Denoting $Γ_virt,mix^i (i=γ,Z)$ as contributions to partial decay widths from the sum of Fig. [ref](b)-(g) and the corresponding counter terms, we obtain [equation] where $C_0$ and the renormalization constants $δZ_gγ$ and $δZ_gZ$ are given below: [equation] We can see that $Γ_virt,mix^γ$ and $δZ_gγ$ are consistent with Eqs. (4.8) and (4.10) in Ref. [ref] , up to a factor of $1/3$, which is absorbed into $Q_f$ in our formula.
Next-to-leading order QCD corrections to the top quark decay via the Flavor-Changing Neutral-Current operators with mixing effects · Contributions to $t→q+γ$ and $t→q+Z$ from FCNC operator mixing · 1.00
Cites it as background 1 paper
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We refer in particular to [ref] and more recent reviews [ref] .
Climbing NLO and NNLO Summits of Weak Decays: 1988-2023 · $B→X_sγ$ at NNLO · 0.94
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