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Future prospects for the determination of the Wilson coefficient $C_{7\gamma}^\prime$
High Energy Physics - Phenomenology · Submitted 7 Jun 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim By studying different New Physics scenarios we show that the future measurement of conveniently defined observables in these decays could provide us with the full determination of $C_{7\gamma}$ and $C_{7\gamma}^\prime$.
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The abstract, sentence by sentence
We discuss the possibilities of assessing a non-zero $C_{7\gamma}^\prime$ from the direct and the indirect measurements of the photon polarization in the exclusive $b \to s\gamma^{(*)}$ decays. We focus on three methods and explore the following three decay modes: $B \to K^*(\to K_S\pi^0)\gamma$, $B \to K_1(\to K\pi\pi)\gamma$, and $B \to K^*(\to K\pi)\ell^+\ell^-$. By studying different New Physics scenarios we show that the future measurement of conveniently defined observables in these decays could provide us with the full determination of $C_{7\gamma}$ and $C_{7\gamma}^\prime$.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We discuss the possibilities of assessing a non-zero $C_{7\gamma}^\prime$ from the direct and the indirect measurements of the photon polarization in the exclusive $b \to s\gamma^{(*)}$ decays. | contribution 0.90 | 0.29 | 0.10 | hedged possibility 0.89 |
| s1 | We focus on three methods and explore the following three decay modes: $B \to K^*(\to K_S\pi^0)\gamma$, $B \to K_1(\to K\pi\pi)\gamma$, and $B \to K^*(\to K\pi)\ell^+\ell^-$. | method 0.55 | 0.46 | 0.04 | asserted 0.87 |
| s2 | By studying different New Physics scenarios we show that the future measurement of conveniently defined observables in these decays could provide us with the full determination of $C_{7\gamma}$ and $C_{7\gamma}^\prime$. | result 0.56 | 0.77 | 0.88 | hedged possibility 0.88 |
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The paper
Original abstract
We discuss the possibilities of assessing a non-zero $C_{7\gamma}^\prime$ from the direct and the indirect measurements of the photon polarization in the exclusive $b \to s\gamma^{(*)}$ decays. We focus on three methods and explore the following three decay modes: $B \to K^*(\to K_S\pi^0)\gamma$, $B \to K_1(\to K\pi\pi)\gamma$, and $B \to K^*(\to K\pi)\ell^+\ell^-$. By studying different New Physics scenarios we show that the future measurement of conveniently defined observables in these decays could provide us with the full determination of $C_{7\gamma}$ and $C_{7\gamma}^\prime$.
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References
How the literature uses it
22 arXiv papers cite this in 39 sentences
Papers citing it · 27 sentences without a confident label
Uses its method or tool 1 paper
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Here, following the discussion in [ref] , we study the three types of methods; i) The time-dependent $CP$-asymmetry of $B→K_Sπ^0γ$ ($S_K_Sπ^0γ$), ii) The angular distribution of the $B→K_1→Kππ$ decay ($λ_$), and iii) The angular analysis of $B→K^*(→Kπ)ℓ^+ℓ^-$ ($A_T^(2), A_T^(im)$).
Photon Polarization in the b->s gamma processes in the Left-Right Symmetric Model · Impacts of the future photon polarization measurement on the LRSM · 0.85
Uses its data or values 1 paper
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The superKEKB with an integrated luminosity of $75 ab^-1$ and the LHCb with $2 fb^-1$ might reach the 20 ($|λ_γ|=0.8 |λ_γ^SM|$) and $10%$ ($|λ_γ|=0.9 |λ_γ^SM|$) precision, respectively [ref] .
Search for new physics via photon polarization of $b \rightarrow s \gamma$ · Photon polarization in SUSY SU(5) with right-handed neutrino · 0.81
Cites it as support 1 paper
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While simple power counting leads to a relatively large possible range for this quantity [ref] , based on more refined parametric arguments implying the existence of a helicity suppression [ref] as well as on the above numerical estimates of the soft gluon charm loop contribution to $ΔC_7'$ from LCSR, we assume an uncertainty of $±0.4×10^-2$ on the real and imaginary parts of $ΔC_7'$ and consider this to be a conservative choice.
Constraints on new physics from radiative $B$ decays · Discussion of hadronic contributions · 0.97
Cites it as background 8 papers
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A wealth of model-independent combined analyses of $b→sγ$ and $b→sℓ^+ℓ^-$ decays have appeared recently in the literature [ref] .
New Physics constraints from optimized observables in B -> K*ll at large recoil · Status of $b→s ℓ^+ℓ^-$ decays · 0.88
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In addition to general global fits to radiative $B$-decays [ref] (see also Refs. [ref] ), there has been a growing literature aiming at determining the best set of observables with a reduced sensitivity to hadronic inputs, and the ability of these observables to find New Physics.
Optimizing the basis of B->K*ll observables in the full kinematic range · Comparison with other works · 0.97
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For works exploiting the suppression of $f_+$, see [ref] .
B -> K^* Form Factors from Flavor Data to QCD and Back · Maximum recoil · 0.90
What it cites · 57 sentences without a confident label
Contests 2 papers
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Contrary to Refs. [ref] we pointed out the complex hadronic structure of $K_1(1270)→Kππ$, that we studied in great detail in Ref. [ref] .
The strong decays of K1 resonances · GGPR and DDLR-inspired methods using $B→K_1(→Kππ)γ$ · contest 0.80
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Contrary to Refs. [ref] we pointed out the complex hadronic structure of $K_1(1270)→Kππ$, that we studied in great detail in Ref. [ref] .
Measuring the Photon Helicity in Radiative B Decays · GGPR and DDLR-inspired methods using $B→K_1(→Kππ)γ$ · contest 0.80
Uses the method or tool of 1 paper
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Using the anomalous dimension matrix from Ref. [ref] and running the coefficients $C_7γ^ (') ()$ from the SUSY scale $M_S$ (See Eq. [ref]) to the low scale $μ_b=m_b,pole$, in Fig. [ref] we show the potential constraints on the dominant $(δ_RL^d)_23$ MIA parameter for $m_≃m_=500$ GeV (plots on the left) and 1000 GeV (plots on the right) respectively.
Gluino Contribution to Radiative B Decays: Organization of QCD Corrections and Leading Order Results · SUSY models with large $(δ_RL^d)_23$ mass insertion · 0.98
Uses data or values from 11 papers
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The region outside the gray (dark gray) circle is excluded at $3σ$ ($1σ$) level by the current measurement [ref] , [equation] which we combined with the SM prediction given in Ref. [ref] .
Averages of b-hadron, c-hadron, and tau-lepton Properties · Current constraint on $_7γ$ by $(B→X_sγ)$ and $S_K_Sπ^0γ$ · 0.98
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The region outside the gray (dark gray) circle is excluded at $3σ$ ($1σ$) level by the current measurement [ref] , [equation] which we combined with the SM prediction given in Ref. [ref] .
QCD Anatomy of B -> X_s gamma Decays · Current constraint on $_7γ$ by $(B→X_sγ)$ and $S_K_Sπ^0γ$ · 0.98
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In our numerics we use $_7γ(μ_b)=-0.304$ [ref] .
Photonic penguins at two loops and m_t-dependence of BR[ B -> X_s l^+ l^-] · Photon polarization in the $b→sγ$ process · 1.00
Compares with 1 paper
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This is larger than the estimate made in Ref. [ref] (see Eq. [ref]).
Time-dependent CP Asymmetry in B->K* gamma as a (Quasi) Null Test of the Standard Model · Discussion of the $Ø_2$ contribution to the “wrong" helicity amplitude · 0.85
Cites as background 1 paper
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In this sense the content of this paper is a contribution to the broad effort in the particle physics community to search for NP through $b→s$ exclusive decays [ref] .
New Physics in b -> s mu+ mu-: CP-Conserving Observables · Introduction · 0.83
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